diff b34550f..b1f9bc4 hard_sphere_boltzmann_fluctuations_v2.txt
diff --git a/hard_sphere_boltzmann_fluctuations_v2.txt b/hard_sphere_boltzmann_fluctuations_v2.txt
index 1e7629c..fb0f602 100644
--- a/hard_sphere_boltzmann_fluctuations_v2.txt
+++ b/hard_sphere_boltzmann_fluctuations_v2.txt
@@ -3,7 +3,7 @@
A gas of billiard balls. A large box holds identical hard spheres,
like a three-dimensional break of pool: they fly in straight lines and
bounce elastically on contact. The diameter $ε$ is tiny and the density
-is $\mu=ε^{-2}$ spheres per unit volume, so the gas is dilute yet the
+is $mu=ε^{-2}$ spheres per unit volume, so the gas is dilute yet the
number of spheres is enormous.
The average. The expected number of spheres per unit volume of
@@ -11,14 +11,14 @@ position-velocity space, the one-particle density, solves the Boltzmann
equation as $ε↓0$. That is Lanford's kinetic limit.
The wobble. The random gas equals this deterministic density plus
-a small error. Scaling the error by $\sqrt\mu$ gives the fluctuation field
-$\zeta^ε_t$; the question is its law as $ε↓0$.
+a small error. Scaling the error by $sqrtmu$ gives the fluctuation field
+$zeta^ε_t$; the question is its law as $ε↓0$.
The answer. The scaled error is asymptotically Gaussian, with a
covariance governed by the fluctuating Boltzmann equation: the linearized
Boltzmann drift plus a Gaussian noise whose strength is the collision rate,
$$
-d \zeta_t(\phi)=\zeta_t(A_t\phi) d t+ d W_t(\phi),
+d zeta_t(phi)=zeta_t(A_tphi) d t+ d W_t(phi),
$$
where $A_t$ is the linearized generator and $W$ is a noise of covariance
$C_t$, both fixed below. This is a finite-dimensional, multi-time central
@@ -56,47 +56,47 @@ equilibrium.
Two new difficulties. First, size: the $h$-th factorial cumulant,
the connected $h$-point correlation, must be pinned at the sharp scale
-$\mu^{1-h}$, far below a crude bound. A change of relative translations of
+$mu^{1-h}$, far below a crude bound. A change of relative translations of
collision clusters extracts one $ε^2$ per merging collision and does it.
Second, centering: the gas is centered by its true microscopic mean, which
differs from the Boltzmann mean already at order $ε$, since hard spheres
-cannot overlap; at the scale $\sqrt\mu=ε^{-1}$ that difference survives,
+cannot overlap; at the scale $sqrtmu=ε^{-1}$ that difference survives,
so the model dynamics must match the gas with probability better than
$O(ε)$.
Notation is fixed once and used without variation.
-$N$ : number of spheres; $N/\mu$ stays near the mass $\int f_0 d z$.
+$N$ : number of spheres; $N/mu$ stays near the mass $int f_0 d z$.
$f_0(z)$, $f_t(z)$ : initial one-particle density and the regular Boltzmann
solution, both in $z=(x,v)$; regularity on $[0,T]$ is
the kinetic assumption.
-$\|\cdot\|_{Bol,\beta}$ : sup norm with a Gaussian velocity weight
-$e^{\beta|v|^2}$, summed over unit spatial cells so mass is controlled.
+$|cdot|_{Bol,beta}$ : sup norm with a Gaussian velocity weight
+$e^{beta|v|^2}$, summed over unit spatial cells so mass is controlled.
-$B$, $\Delta\phi$ : collision kernel $[(v-v_*)\cdot\omega]_+$ and the change
-$\Delta\phi$ of a test across one collision.
+$B$, $Deltaphi$ : collision kernel $[(v-v_*)cdotomega]_+$ and the change
+$Deltaphi$ of a test across one collision.
$A_t$, $C_t$ : linearized Boltzmann drift and collision-noise covariance:
the two coefficients of the fluctuating equation.
-$\zeta_t^ε$, $\zeta_t$ : the centered, $\sqrt\mu$-scaled fluctuation
+$zeta_t^ε$, $zeta_t$ : the centered, $sqrtmu$-scaled fluctuation
(microscopic) and its Gaussian limit.
-$W$ : the Gaussian noise driving $\zeta_t$, with independent increments.
+$W$ : the Gaussian noise driving $zeta_t$, with independent increments.
-$g_i$, $f_{i\tau}$ : one-root mean at interface $i$ (the independent input)
-and the Boltzmann density $f_{i\tau}$ at the same time.
+$g_i$, $f_{itau}$ : one-root mean at interface $i$ (the independent input)
+and the Boltzmann density $f_{itau}$ at the same time.
-$H_i,Λ_i,\Gamma$ : collision bookkeeping of the Deng--Hani--Ma
+$H_i,Λ_i,Gamma$ : collision bookkeeping of the Deng--Hani--Ma
machinery: root count, particle-size cap, and cluster-excess cap.
-$L, \tau=T/L$, $K$, $\rho$ : number of slabs, slab length, the complexity
+$L, tau=T/L$, $K$, $rho$ : number of slabs, slab length, the complexity
cutoff, and the complexity of a history.
$c_h^ε$ : the $h$-th factorial cumulant density; its target size is the
-sharp scale $\mu^{1-h}$.
+sharp scale $mu^{1-h}$.
Why one collision costs $ε^2$. Two groups of spheres that
evolved independently can join one connected history only if, at the
@@ -105,9 +105,9 @@ around the other group. Their relative motion is a straight line, and a line
meets that tiny sphere in a window whose cross section is a disk of area of
order $ε^2$, hit during a sliding time interval. This is the source of the
factor $ε^2$ per merging collision, the merger Jacobian
-$ε^2[(v-v_*)\cdot\omega] d t d \omega$. The gas carries activity
-$\mu=ε^{-2}$ per particle, so a connected diagram with $h$ marked
-particles and $m$ lines weighs $\mu^{m-h}$, and each merger pays one $ε^2$:
+$ε^2[(v-v_*)cdotomega] d t d omega$. The gas carries activity
+$mu=ε^{-2}$ per particle, so a connected diagram with $h$ marked
+particles and $m$ lines weighs $mu^{m-h}$, and each merger pays one $ε^2$:
the two powers of $ε$ cancel line by line. The initial excluded-volume link
is a ball, not a sphere, so it costs $ε^3$, the only place where the
static problem is even smaller than the dynamical one.
@@ -121,112 +121,112 @@ the collision rate, exactly $C_t$. The body of the argument proves the gas is
close enough to this picture for it to hold throughout the regular lifespan
and on the whole space.
-Phase space is $R_x^3\times R_v^3$ and $z=(x,v)$. For a rate $\beta>0$
+Phase space is $R_x^3times R_v^3$ and $z=(x,v)$. For a rate $beta>0$
define the weighted sup norm
-$$\|g\|_{Bol,\beta}
-:=\sum_{a\in Z^3} \sup_{\substack{|x-a|\le1\\v\in R^3}}
-e^{\beta|v|^2} |g(x,v)|$$
+$$|g|_{Bol,beta}
+:=sum_{ain Z^3} sup_{substack{|x-a|le1vin R^3}}
+e^{beta|v|^2} |g(x,v)|$$
It is a supremum with a Gaussian velocity weight, summed over unit spatial
cells so that it also controls the total mass. Hard-sphere collisions use
the kernel and scattering
-$$B(v-v_*,\omega) =[(v-v_*)\cdot\omega]_+, \omega\in\mathbb S^2$$
+$$B(v-v_*,omega) =[(v-v_*)cdotomega]_+, omegainmathbb S^2$$bbS^2$$
-$$v' =v-[(v-v_*)\cdot\omega]\omega,
-v_*' =v_*+[(v-v_*)\cdot\omega]\omega$$
+$$v' =v-[(v-v_*)cdotomega]omega,
+v_*' =v_*+[(v-v_*)cdotomega]omega$$
-with $[a]_+=\max\{a,0\}$ and $ d \omega$ the unnormalized surface measure.
+with $[a]_+=max{a,0}$ and $ d omega$ the unnormalized surface measure.
The Boltzmann equation reads
-$$(∂_t+v\cdot\nabla_x)f=Q(f,f),
-Q(f,f)=\int_{R^3\times\mathbb S^2}B(f'f_*'-ff_*) d v_* d \omega$$
+$$(∂_t+vcdotnabla_x)f=Q(f,f),
+Q(f,f)=int_{R^3timesmathbb S^2}bbS^2B(f'f_*'-ff_*) d v_* d omega$$
all densities evaluated at the same $x$.
Fix the sphere diameter $ε>0$ and set the mean density
-$\mu=ε^{-2}$. The grand-canonical initial law, including $N=0$, is
+$mu=ε^{-2}$. The grand-canonical initial law, including $N=0$, is
$$P_ε(N, d Z_N)
-=\mathcal Z_ε^{-1}(\mu^N)/(N!)
-1 _{\mathcal D_N^ε}(Z_N)\prod_{i=1}^N f_0(z_i) d z_i$$
+=mathcal Z_ε^calZ_ε^{-1}(mu^N)/(N!)
+1 _{mathcal D_N^ε}calD_N^ε(Z_N)prod_{i=1}^N f_0(z_i) d z_i$$
with the non-overlap set
-$\mathcal D_N^ε=\{(z_i):|x_i-x_j|>ε, i\ne j\}$ and
-$1\le\mathcal Z_ε\le e^\mu$. Given the configuration, spheres move by
+$mathcal D_N^ε=calD_N^ε={(z_i):|x_i-x_j|>ε, ine j}$ and
+$1lemathcal Z_εcalZ_εle e^mu$. Given the configuration, spheres move by
free flight and deterministic elastic collisions, defined almost surely
by Deng--Hani--Ma, Proposition 1.2. There is no random collision rule and no
resampling: the only randomness is the initial configuration.
-Assumption. $f_0\ge0$ is a smooth probability density with
-$\|f_0\|_{Bol,2\beta}+\|\nabla_xf_0\|_{Bol,2\beta}<∞$ for some
-$\beta>0$. There is a nonnegative classical solution $f$ of
+Assumption. $f_0ge0$ is a smooth probability density with
+$|f_0|_{Bol,2beta}+|nabla_xf_0|_{Bol,2beta}<∞$ for some
+$beta>0$. There is a nonnegative classical solution $f$ of
the Boltzmann equation on a prescribed interval $[0,T]$ with
-$$M:=\sup_{0\le t\le T}\sup_{x,v}e^{2\beta|v|^2}f(t,x,v)<∞$$
+$$M:=sup_{0le tle T}sup_{x,v}e^{2beta|v|^2}f(t,x,v)<∞$$
Throughout, $[0,T]$ is one fixed regular kinetic interval; nothing
below asserts that $T$ can be taken infinite.
-For real $\phi\in C_c^∞(R^6)$ put
+For real $phiin C_c^∞(R^6)$ put
-$$\pi_t^ε(\phi)=\mu^{-1}\sum_{i=1}^N\phi(z_i(t)),
+$$pi_t^ε(phi)=mu^{-1}sum_{i=1}^Nphi(z_i(t)),
-\zeta_t^ε(\phi)=\sqrt\mu [\pi_t^ε(\phi)-E_ε\pi_t^ε(\phi)]$$
+zeta_t^ε(phi)=sqrtmu [pi_t^ε(phi)-E_εpi_t^ε(phi)]$$
The expectation is the exact microscopic one. This is essential; see
the centering remark.
Define the pair difference and the two limiting operators
-$$\Delta\phi =\phi(x,v')+\phi(x,v_*')-\phi(x,v)-\phi(x,v_*)$$
+$$Deltaphi =phi(x,v')+phi(x,v_*')-phi(x,v)-phi(x,v_*)$$
-$$(A_t\phi)(x,v)
-=v\cdot\nabla_x\phi
-+\int_{R^3\times\mathbb S^2}B(v-v_*,\omega)f_t(x,v_*)\Delta\phi
-d v_* d \omega$$
+$$(A_tphi)(x,v)
+=vcdotnabla_xphi
++int_{R^3timesmathbb S^2}bbS^2B(v-v_*,omega)f_t(x,v_*)Deltaphi
+d v_* d omega$$
-$$C_t(\phi,\psi)
-=\tfrac12\int_{R^3\times R^3\times R^3\times\mathbb S^2}
-B(v-v_*,\omega)f_t(x,v)f_t(x,v_*)\Delta\phi \Delta\psi
-d x d v d v_* d \omega$$
+$$C_t(phi,psi)
+=tfrac12int_{R^3times R^3times R^3timesmathbb S^2}bbS^2
+B(v-v_*,omega)f_t(x,v)f_t(x,v_*)Deltaphi Deltapsi
+d x d v d v_* d omega$$
$A_t$ is the linearized Boltzmann generator; the collision part carries
no extra factor $1/2$ because of the pre/post substitution together with
-$\omega\mapsto-\omega$ (the collision normalization, below). The quadratic form
-$C_t$ is the collision noise, nonnegative because $f_t\ge0$.
+$omegamapsto-omega$ (the collision normalization, below). The quadratic form
+$C_t$ is the collision noise, nonnegative because $f_tge0$.
-Theorem (Finite-dimensional fluctuation limit). Under the kinetic assumption, the centered Gaussian field $\zeta$ solving the
+Theorem (Finite-dimensional fluctuation limit). Under the kinetic assumption, the centered Gaussian field $zeta$ solving the
weak fluctuating Boltzmann equation
-$$d \zeta_t(\phi)=\zeta_t(A_t\phi) d t+ d W_t(\phi)$$
+$$d zeta_t(phi)=zeta_t(A_tphi) d t+ d W_t(phi)$$
in backward-mild form is well defined on test scales of small Gaussian
growth. Its initial field is independent of $W$, and
-$$E[\zeta_0(\phi)\zeta_0(\psi)] =\int_{R^6}f_0 \phi\psi d z$$
+$$E[zeta_0(phi)zeta_0(psi)] =int_{R^6}f_0 phipsi d z$$
-$$E[W_t(\phi)W_s(\psi)] =\int_0^{t\wedge s}C_r(\phi,\psi) d r$$
+$$E[W_t(phi)W_s(psi)] =int_0^{twedge s}C_r(phi,psi) d r$$
-with $W$ of independent increments. For every $m\ge1$, all $t_1,...,t_m
-\in[0,T]$, and real $\phi_1,...,\phi_m\in C_c^∞(R^6)$,
+with $W$ of independent increments. For every $mge1$, all $t_1,...,t_m
+in[0,T]$, and real $phi_1,...,phi_min C_c^∞(R^6)$,
-$$(\zeta_{t_1}^ε(\phi_1),...,\zeta_{t_m}^ε(\phi_m))
-⇒\
-(\zeta_{t_1}(\phi_1),...,\zeta_{t_m}(\phi_m))
+$$(zeta_{t_1}^ε(phi_1),...,zeta_{t_m}^ε(phi_m))
+⇒
+(zeta_{t_1}(phi_1),...,zeta_{t_m}(phi_m))
(ε↓0)$$
Remark (The initial covariance). The initial covariance has no subtraction of
-$(\int f_0\phi)(\int f_0\psi)$: the particle number is random. More
+$(int f_0phi)(int f_0psi)$: the particle number is random. More
importantly, microscopic centering is not the same as centering by the
-Boltzmann mean. With $ρ_0(x)=\int f_0(x,v) d v$,
+Boltzmann mean. With $ρ_0(x)=int f_0(x,v) d v$,
$$
-\lim_{ε\to0}\sqrt\mu(E\pi_0^ε(\phi)-\int f_0\phi)
-=-(4\pi)/(3)\int f_0(x,v)\phi(x,v)ρ_0(x) d x d v .
+lim_{εto0}sqrtmu(Epi_0^ε(phi)-int f_0phi)
+=-(4pi)/(3)int f_0(x,v)phi(x,v)ρ_0(x) d x d v .
$$
So exclusion shifts the mean by order $ε$, which survives the factor
-$\sqrt\mu=ε^{-1}$. Centering by the Boltzmann density alone would
+$sqrtmu=ε^{-1}$. Centering by the Boltzmann density alone would
leave a nonzero deterministic drift already at time zero. This is why
the proof must compare exact expectations, not merely laws.
@@ -248,12 +248,12 @@ keeping finitely many observation records. Large complexity is dropped
by the Deng--Hani--Ma package.
3. Sharp correlation bounds (the sharp bounds, below,
-the sharp connected bounds). The $h$-th cumulant is $O(\mu^{1-h})$,
+the sharp connected bounds). The $h$-th cumulant is $O(mu^{1-h})$,
with the leading $h=1,2$ terms identified as signed sums of trees
-weighted by $f_{i\tau}$, contact flux, and $\pm1$ signs. This is proved
+weighted by $f_{itau}$, contact flux, and $pm1$ signs. This is proved
by chronological merger coordinates: each collision that merges two
-clusters contributes $ε^2[(v-v_*)\cdot\omega]_+$, and summing all
-clusters costs $CT/\sqrt L<1$.
+clusters contributes $ε^2[(v-v_*)cdotomega]_+$, and summing all
+clusters costs $CT/sqrt L<1$.
4. Gaussian limit for the model dynamics
(the Gaussian limit of the model dynamics, below). A mark that accumulates observations turns
@@ -263,14 +263,14 @@ vanish, giving the Gaussian law with the correct covariance.
5. Accuracy of the model dynamics (the cutoff comparison, below,
the pasted accuracy bound). The pasted and true dynamics agree with
-probability $O(ε^{1+\eta})$, $\eta=1/20$. This is a positive
+probability $O(ε^{1+eta})$, $eta=1/20$. This is a positive
geometric estimate on terminal witnesses, carried out with local
gains, a common birth-energy bound, and a causal time-order sum free of
per-vertex logarithms.
6. Exact centering transfer (the centering transfer, below). The
-discrepancy estimate, the fixed moments of $N/\mu$, and H\"older's
-inequality show that expectations agree to $o(\mu^{-1/2})$, which is
+discrepancy estimate, the fixed moments of $N/mu$, and H"older's
+inequality show that expectations agree to $o(mu^{-1/2})$, which is
what transfers the limit with exact centering.
This stage is independent of the dynamics. It does two things: prove the
@@ -280,24 +280,24 @@ that the fluctuation limit theorem claims to be the limit. It also records the i
correlation bounds that later parts use.
Let $F_{h,0}^{ε}$ be the density of the ordered factorial measure
-divided by $\mu^h$:
+divided by $mu^h$:
-$$\int F_{h,0}^{ε}(Z_h)\Phi(Z_h) d Z_h
-=\mu^{-h}E\sum_{i_1,...,i_h distinct}\Phi(z_{i_1},...,z_{i_h})$$
+$$int F_{h,0}^{ε}(Z_h)Phi(Z_h) d Z_h
+=mu^{-h}Esum_{i_1,...,i_h distinct}Phi(z_{i_1},...,z_{i_h})$$
-Write $[h]=\{1,...,h\}$, $Z_B=(z_j)_{j\in B}$, and let $\mathcal P(V)$
+Write $[h]={1,...,h}$, $Z_B=(z_j)_{jin B}$, and let $mathcal P(V)$calP(V)$
be the set of set-partitions of $V$. The factorial cumulant
(connected) densities $c_{h,0}^{ε}$ are defined by the cumulant
inversion of the factorial hierarchy,
$$F_{h,0}^{ε}(Z_h)
-=\sum_{\pi\in\mathcal P([h])}\prod_{B\in\pi}c_{|B|,0}^{ε}(Z_B)$$
+=sum_{piinmathcal P([h])}calP([h])prod_{Binpi}c_{|B|,0}^{ε}(Z_B)$$
The one-point function is $g_0=c_{1,0}^{ε}=F_{1,0}^{ε}$. Set
$$
-ρ_0(x)=\int f_0(x,v) d v,
-b_ε=(4\pi)/(3)\|ρ_0\|_∞ε^3,
-d_ε=\mu b_ε=O(ε),
+ρ_0(x)=int f_0(x,v) d v,
+b_ε=(4pi)/(3)|ρ_0|_∞ε^3,
+d_ε=mu b_ε=O(ε),
$$
and let $(N)_p=N...(N-p+1)$ denote the falling factorial.
@@ -308,74 +308,74 @@ collision costs $ε^2$; excluded volume makes it $ε^3$.
Proposition (Initial ensemble). For all sufficiently small $ε$:
-(i) $0\le F_{h,0}^{ε}\le\prod_{j=1}^hf_0(z_j)$ and
-$(1-Cε)f_0\le g_0\le f_0$. Hence
-$\|g_0-f_0\|_{Bol,2\beta}=O(ε)$ and, for every fixed $p\ge1$,
+(i) $0le F_{h,0}^{ε}leprod_{j=1}^hf_0(z_j)$ and
+$(1-Cε)f_0le g_0le f_0$. Hence
+$|g_0-f_0|_{Bol,2beta}=O(ε)$ and, for every fixed $pge1$,
-$$E(N)_p\le\mu^p, \sup_{0<ε\leε_0}E(N/\mu)^p<∞$$
+$$E(N)_plemu^p, sup_{0<εleε_0}E(N/mu)^p<∞$$
-(ii) With $υ=1/81$, for every $h\ge2$ and a constant $C$ independent
+(ii) With $υ=1/81$, for every $hge2$ and a constant $C$ independent
of $h$,
-$$|c_{h,0}^{ε}(Z_h)|\le(Ch)^{Ch}\prod_{j=1}^hf_0(z_j)
-\sum_{\mathcal T}\prod_{\{i,j\}\in\mathcal T}
-( 1 _{|x_i-x_j|\leε}+ε^υ)$$
+$$|c_{h,0}^{ε}(Z_h)|le(Ch)^{Ch}prod_{j=1}^hf_0(z_j)
+sum_{mathcal T}calTprod_{{i,j}inmathcal T}calT
+( 1 _{|x_i-x_j|leε}+ε^υ)$$
-the sum over trees $\mathcal T$ on $[h]$. For fixed $h\ge2$ and any
+the sum over trees $mathcal T$calT$ on $[h]$. For fixed $hge2$ and any
$D>0$ there is $C_{D,h}$ with
-$$|c_{h,0}^{ε}(Z_h)|\le C_{D,h}\prod_{j=1}^hf_0(z_j)
-\sum_{\mathcal T}\prod_{\{i,j\}\in\mathcal T}
-( 1 _{|x_i-x_j|\le C_{D,h}ε}+ε^D)$$
+$$|c_{h,0}^{ε}(Z_h)|le C_{D,h}prod_{j=1}^hf_0(z_j)
+sum_{mathcal T}calTprod_{{i,j}inmathcal T}calT
+( 1 _{|x_i-x_j|le C_{D,h}ε}+ε^D)$$
and
-$$\|c_{h,0}^{ε}\|_{L^1}\le C_hε^{3(h-1)} (h\ge2)$$
+$$|c_{h,0}^{ε}|_{L^1}le C_hε^{3(h-1)} (hge2)$$
(iii) For every finite list of bounded real tests, the exact-centered
initial fluctuations converge jointly to a centered Gaussian vector with
-covariance $\int f_0\phi\psi$. For smooth compactly supported real
-$\phi$,
+covariance $int f_0phipsi$. For smooth compactly supported real
+$phi$,
-$$\lim_{ε\to0}\sqrt\mu(E\pi_0^ε(\phi)-\int f_0\phi)
-=-(4\pi)/(3)\int_{R^6}f_0\phi ρ_0 d z$$
+$$lim_{εto0}sqrtmu(Epi_0^ε(phi)-int f_0phi)
+=-(4pi)/(3)int_{R^6}f_0phi ρ_0 d z$$
Proof.
(i) Factorial bound and moments. For fixed $Z_h$, let
-$\mathcal Z_ε[Z_h]$ be the partition function of the remaining
+$mathcal Z_ε[Z_h]$calZ_ε[Z_h]$ be the partition function of the remaining
particles, still mutually excluding and additionally avoiding the balls
$B(x_j,ε)$. Directly from the grand-canonical law,
-$$F_{h,0}^{ε}(Z_h)= 1 _{\mathcal D_h^ε}(Z_h)\prod_{j=1}^hf_0(z_j)
-(\mathcal Z_ε[Z_h])/(\mathcal Z_ε)$$
+$$F_{h,0}^{ε}(Z_h)= 1 _{mathcal D_h^ε}calD_h^ε(Z_h)prod_{j=1}^hf_0(z_j)
+(mathcal Z_ε[Z_h])/(calZ_ε[Z_h])/(mathcal Z_ε)$$calZ_ε)$$
-The ratio is $\le1$, giving the factorial upper bound. For $h=1$ it is
+The ratio is $le1$, giving the factorial upper bound. For $h=1$ it is
the probability that $B(x_1,ε)$ is empty of particle centers; by the
factorial upper bound with one particle and the union bound this is
-$\ge1-\mu b_ε=1-O(ε)$, giving $(1-Cε)f_0\le g_0\le f_0$.
-Integrating the factorial bound gives $E(N)_p\le\mu^p$; writing $N^p$
+$ge1-mu b_ε=1-O(ε)$, giving $(1-Cε)f_0le g_0le f_0$.
+Integrating the factorial bound gives $E(N)_plemu^p$; writing $N^p$
as a positive combination of $(N)_j$ gives the moment bounds.
-(ii) The Penrose tree bound. Write $\chi_{ij}= 1 _{|x_i-x_j|\le
+(ii) The Penrose tree bound. Write $chi_{ij}= 1 _{|x_i-x_j|le
ε}$ and set
$$
-\mathcal U_1=1,
-\mathcal U_n(Z_n)=\sum_{H conn. on [n]}\prod_{\{i,j\}\in H}(-\chi_{ij}) (n\ge2).
+mathcal U_1=1,calU_1=1,
+mathcal U_n(Z_n)=calU_n(Z_n)=sum_{H conn. on [n]}prod_{{i,j}in H}(-chi_{ij}) (nge2).
$$
The tree bound is
-$$|\mathcal U_n(Z_n)|\le\sum_{\mathcal T tree}\prod_{\{i,j\}\in\mathcal T}\chi_{ij}$$
+$$|mathcal U_n(Z_n)|calU_n(Z_n)|lesum_{mathcal TcalT tree}prod_{{i,j}inmathcal T}calTchi_{ij}$$
This is the Penrose forest scheme. Root a connected labelled graph at
vertex $1$, assign graph-distance levels, and let the parent of each
vertex be its least-labelled neighbour in the preceding level. For a
-fixed resulting tree $\mathcal T$, the graphs giving it are exactly
-$\mathcal T⊆ H⊆ R(\mathcal T)$, where $R(\mathcal T)$
+fixed resulting tree $mathcal T$,calT$, the graphs giving it are exactly
+$mathcal T⊆calT⊆ H⊆ R(mathcal T)$,calT)$, where $R(mathcal T)$calT)$
adds all same-level edges and every edge to a preceding-level vertex with
-label $\ge$ that of the chosen parent. These intervals partition all
+label $ge$ that of the chosen parent. These intervals partition all
connected graphs, and summing one interval gives
$$
-\prod_{e\in\mathcal T}(-\chi_e)\prod_{e\in R(\mathcal T)∖\mathcal T}(1-\chi_e),
+prod_{einmathcal T}calT(-chi_e)prod_{ein R(mathcal T)∖calT)∖mathcal T}calT(1-chi_e),
$$
whose second factor lies in $[0,1]$, proving the tree bound.
@@ -387,46 +387,46 @@ classical systems, in Statistical Mechanics (Benjamin, 1967).
Integrating a tree from its leaves, keeping one free vertex, gives
-$$\int f_0^{ ⊗ n}|\mathcal U_n|\le n^{n-2}b_ε^{n-1} (n\ge2)$$
+$$int f_0^{ ⊗ n}|mathcal U_n|calU_n|le n^{n-2}b_ε^{n-1} (nge2)$$
Hence the connected-graph (Mayer) series is absolutely convergent when
-$e\mu b_ε\|a\|_∞<1$, and by exponentiation/analytic continuation
+$emu b_ε|a|_∞<1$, and by exponentiation/analytic continuation
-$$\log\mathcal Z_ε[a]=\sum_{n\ge1}(\mu^n)/(n!)\int\mathcal U_n(Z_n)
-\prod_{j=1}^nf_0(z_j)a(z_j) d Z_n$$
+$$logmathcal Z_ε[a]=calZ_ε[a]=sum_{nge1}(mu^n)/(n!)intmathcal U_n(Z_n)calU_n(Z_n)
+prod_{j=1}^nf_0(z_j)a(z_j) d Z_n$$
From the partition function to the cumulants. Apply
the logarithmic partition formula with $a=1+u$. The log of
-$E\prod_i(1+u(z_i))$ has coefficients $\mu^hc_{h,0}^{ε}/h!$, so
+$Eprod_i(1+u(z_i))$ has coefficients $mu^hc_{h,0}^{ε}/h!$, so
differentiation gives the rooted Mayer series
-$$c_{h,0}^{ε}(Z_h)=\prod_{j=1}^hf_0(z_j)
-\sum_{n\ge0}(\mu^n)/(n!)\int f_0^{ ⊗ n}(Z_{h+1:h+n})
-\mathcal U_{h+n}(Z_{h+n}) d Z_{h+1:h+n}$$
+$$c_{h,0}^{ε}(Z_h)=prod_{j=1}^hf_0(z_j)
+sum_{nge0}(mu^n)/(n!)int f_0^{ ⊗ n}(Z_{h+1:h+n})
+mathcal U_calU_{h+n}(Z_{h+n}) d Z_{h+1:h+n}$$
For bounds uniform in $h$: delete $h-1$ edges of a tree on $h+n$ vertices
so each component contains one fixed root (possible by repeatedly cutting
an edge on a path between two roots). Dropping the deleted constraints and
integrating the auxiliary leaves costs at most $b_ε^n$. With
-$n!\ge(n/e)^n$, $(1+h/n)^n\le e^h$, $(h+n)^h\le h^he^n$,
+$n!ge(n/e)^n$, $(1+h/n)^nle e^h$, $(h+n)^hle h^he^n$,
-$$\frac{(h+n)^{h+n-2}}{n!}\le(eh)^he^{2n}$$
+$$frac{(h+n)^{h+n-2}}{n!}le(eh)^he^{2n}$$
-and the $n=0$ count is $\le(Ch)^{Ch}$. Thus the rooted Mayer series
-converges absolutely for $ε\leε_0$ with $ε_0$ independent of
+and the $n=0$ count is $le(Ch)^{Ch}$. Thus the rooted Mayer series
+converges absolutely for $εleε_0$ with $ε_0$ independent of
$h$.
Coarse link bound. Let $q$ be the number of connected components
-of the graph on the $h$ roots with edges $|x_i-x_j|\leε$. If $q\ge2$,
+of the graph on the $h$ roots with edges $|x_i-x_j|leε$. If $qge2$,
every contributing tree must attach each such component to an auxiliary
vertex. One auxiliary vertex touches at most $27$ root components: pick
one adjacent root from each; their mutual distances exceed $ε$, and
their disjoint balls of radius $ε/2$ lie in a ball of radius
-$3ε/2$. Hence $q\le27n$ for a contributing tree with $n$ auxiliary
+$3ε/2$. Hence $qle27n$ for a contributing tree with $n$ auxiliary
vertices. Using the counting inequality and $d_ε=O(ε)$,
$$
-\frac{|c_{h,0}^{ε}(Z_h)|}{\prod_jf_0(z_j)}
-\le(Ch)^{Ch}ε^{q/27}\le(Ch)^{Ch}ε^{(q-1)/81} (q\ge2),
+frac{|c_{h,0}^{ε}(Z_h)|}{prod_jf_0(z_j)}
+le(Ch)^{Ch}ε^{q/27}le(Ch)^{Ch}ε^{(q-1)/81} (qge2),
$$
and for $q=1$ the same argument without the restriction on $n$ gives
$(Ch)^{Ch}$. A tree of the roots using intra-component and $q-1$
@@ -434,179 +434,179 @@ inter-component edges has weight at least $ε^{(q-1)/81}$ in
the factorial bound. This proves the factorial lower bound.
Sharp link bound. For fixed $h,D$, truncate
-the rooted Mayer series at $n_0+1\ge D(h-1)$. The tail is
-$C_{D,h}ε^{D(h-1)}\prod_jf_0(z_j)$. In any term with $n\le n_0$, all
-roots are connected by paths of $\le h+n_0-1$ links of length $\leε$,
-so their diameter is $\le(h+n_0)ε$; on that set the sharp link bound
+the rooted Mayer series at $n_0+1ge D(h-1)$. The tail is
+$C_{D,h}ε^{D(h-1)}prod_jf_0(z_j)$. In any term with $nle n_0$, all
+roots are connected by paths of $le h+n_0-1$ links of length $leε$,
+so their diameter is $le(h+n_0)ε$; on that set the sharp link bound
holds with $C_{D,h}$ chosen large. This proves the sharp link bound.
Integrating the rooted Mayer series and using the rooted tree integral bound
instead gives
$$
-\|c_{h,0}^{ε}\|_1\le b_ε^{h-1}\sum_{n\ge0}\frac{(h+n)^{h+n-2}}{n!}d_ε^n
-\le C_hε^{3(h-1)},
+|c_{h,0}^{ε}|_1le b_ε^{h-1}sum_{nge0}frac{(h+n)^{h+n-2}}{n!}d_ε^n
+le C_hε^{3(h-1)},
$$
which is the L1 bound.
-(iii) Initial CLT and the shift. For real bounded $\phi$ put
-$S_\phi=\sum_i\phi(z_i)$ and let $\kappa_k$ denote ordinary cumulants.
-Substituting $a=e^{u\phi}$ in the logarithmic partition formula and
+(iii) Initial CLT and the shift. For real bounded $phi$ put
+$S_phi=sum_iphi(z_i)$ and let $kappa_k$ denote ordinary cumulants.
+Substituting $a=e^{uphi}$ in the logarithmic partition formula and
differentiating $k$ times at $u=0$,
$$
-\kappa_k(S_\phi)=\sum_{n\ge1}(\mu^n)/(n!)\int f_0^{ ⊗ n}\mathcal U_n
-(\sum_{j=1}^n\phi(z_j))^k,
+kappa_k(S_phi)=sum_{nge1}(mu^n)/(n!)int f_0^{ ⊗ n}mathcal U_ncalU_n
+(sum_{j=1}^nphi(z_j))^k,
$$
-and the rooted tree integral bound gives $\kappa_k(S_\phi)=\mu\int f_0\phi^k+
-O_{k,\phi}(\muε)$. After exact centering and division by $\sqrt\mu$,
-the second cumulant tends to $\int f_0\phi^2$ and every higher one to
+and the rooted tree integral bound gives $kappa_k(S_phi)=muint f_0phi^k+
+O_{k,phi}(muε)$. After exact centering and division by $sqrtmu$,
+the second cumulant tends to $int f_0phi^2$ and every higher one to
zero. The moment-cumulant identity then gives every Gaussian moment; for
scalar convergence compare characteristic functions of the normalized
-variable and the Gaussian of variance $\sigma^2=\int f_0\phi^2$ using
+variable and the Gaussian of variance $sigma^2=int f_0phi^2$ using
Taylor polynomials of degree $2n-1$, whose combined remainder after
-$limsup$ is at most $2|u|^{2n}\sigma^{2n}/(2^n n!)\to0$. Joint
+$limsup$ is at most $2|u|^{2n}sigma^{2n}/(2^n n!)to0$. Joint
convergence follows on each linear combination. This includes zero
variance.
For the shift, the $n=1$ term of the rooted Mayer series with $h=1$
gives, uniformly in $z$,
$$
-g_0(z)=f_0(z)[1-\mu\int_{|x-x_*|\leε}ρ_0(x_*) d x_*+O(ε^2)].
+g_0(z)=f_0(z)[1-muint_{|x-x_*|leε}ρ_0(x_*) d x_*+O(ε^2)].
$$
The bounded gradient of $ρ_0$ gives
-$\int_{|x-x_*|\leε}ρ_0=(4\pi)/(3)ε^3ρ_0(x)+O(ε^4)$,
-and $\sqrt\mu=ε^{-1}$ converts this into the centering shift.
+$int_{|x-x_*|leε}ρ_0=(4pi)/(3)ε^3ρ_0(x)+O(ε^4)$,
+and $sqrtmu=ε^{-1}$ converts this into the centering shift.
Remark (The centering shift). The shift is generally nonzero, so exact
microscopic centering is essential already at time zero. Meanwhile
-$\mu\|c_{2,0}^{ε}\|_1=O(ε)$, so the limiting initial covariance has
-only the same-particle term $\int f_0\phi\psi$.
+$mu|c_{2,0}^{ε}|_1=O(ε)$, so the limiting initial covariance has
+only the same-particle term $int f_0phipsi$.
-Write $M=\sup_{t\le T,x,v}e^{2\beta|v|^2}f_t(x,v)$. The noise form needs global velocity integrability, which does not
+Write $M=sup_{tle T,x,v}e^{2beta|v|^2}f_t(x,v)$. The noise form needs global velocity integrability, which does not
follow from a spatially uniform bound alone.
-Lemma (Global weighted integrability). For every $0<q<2\beta$,
+Lemma (Global weighted integrability). For every $0<q<2beta$,
-$$\sup_{0\le t\le T}\int_{R^6}f_t(x,v)e^{q|v|^2} d x d v<∞$$
+$$sup_{0le tle T}int_{R^6}f_t(x,v)e^{q|v|^2} d x d v<∞$$
Proof.
Let $Q^+$ be the gain part of $Q$ and $P_tg=Q^+(g,f_t)$ with the second
-factor fixed. With $\mathsf T_tg(x,v)=g(x-tv,v)$ and
-$(\mathcal Vg)_t=\int_0^t\mathsf T_{t-s}P_sg_s d s$, positivity and the
+factor fixed. With $mathsf T_tg(x,v)=g(x-tv,v)$sfT_tg(x,v)=g(x-tv,v)$ and
+$(mathcal Vg)_t=calVg)_t=int_0^tmathsf T_sfT_{t-s}P_sg_s d s$, positivity and the
transport Duhamel formula give
-$f_t\le\sum_{j<n}(\mathcal V^j\mathsf T_\cdot f_0)_t+(\mathcal V^nf)_t$.
-On the Gaussian decay spaces $Y_a$ with $\|g\|_{Y_a}=\sup e^{a|v|^2}|g|$,
-energy conservation gives for $0<b<a\le2\beta$
+$f_tlesum_{j<n}(mathcal V^jcalV^jmathsf T_sfT_cdot f_0)_t+(mathcal V^nf)_t$.calV^nf)_t$.
+On the Gaussian decay spaces $Y_a$ with $|g|_{Y_a}=sup e^{a|v|^2}|g|$,
+energy conservation gives for $0<b<ale2beta$
$$
-|P_tg|\le CM\|g\|_{Y_a}(1+|v|)e^{-a|v|^2},
-\|P_tg\|_{Y_b}\le CM(1+(a-b)^{-1/2})\|g\|_{Y_a}.
+|P_tg|le CM|g|_{Y_a}(1+|v|)e^{-a|v|^2},
+|P_tg|_{Y_b}le CM(1+(a-b)^{-1/2})|g|_{Y_a}.
$$
-Distributing the exponent from $\beta$ to $\beta/2$ over $n$ factors and
+Distributing the exponent from $beta$ to $beta/2$ over $n$ factors and
using that the time simplex has volume $T^n/n!$,
-$\sup_{t\le T}\|(\mathcal V^nf)_t\|_{Y_{\beta/2}}\le M(CT)^n/n!(1+
-√(2n/\beta))^n\to0$, so $f$ is dominated pointwise by the positive
+$sup_{tle T}|(mathcal V^nf)_tcalV^nf)_t|_{Y_{beta/2}}le M(CT)^n/n!(1+
+√(2n/beta))^nto0$, so $f$ is dominated pointwise by the positive
gain series.
Let $X_q=L^1(e^{q|v|^2} d x d v)$. The pre/post substitution with
-$e^{q|v'|^2}\le e^{q|v|^2+q|v_*|^2}$ and the bound on $f_t$ give
-$\|P_tg\|_{X_q}\le CM(1+\delta^{-1/2})\|g\|_{X_{q+\delta}}$ uniformly for
-exponents in a compact subinterval of $(0,2\beta)$. Since $f_0\in X_{q_0}$
-for $q_0<2\beta$, distributing the exponent over the gain series and using
-$n^{n/2}/n!$ bounds its $X_q$ norm uniformly for $t\le T$; integrating the
+$e^{q|v'|^2}le e^{q|v|^2+q|v_*|^2}$ and the bound on $f_t$ give
+$|P_tg|_{X_q}le CM(1+delta^{-1/2})|g|_{X_{q+delta}}$ uniformly for
+exponents in a compact subinterval of $(0,2beta)$. Since $f_0in X_{q_0}$
+for $q_0<2beta$, distributing the exponent over the gain series and using
+$n^{n/2}/n!$ bounds its $X_q$ norm uniformly for $tle T$; integrating the
pointwise majorant proves the velocity moment bound.
-For $a\ge0$ define the test spaces
+For $age0$ define the test spaces
-$$E_a^0=\{h\in C(R^6):e^{-a|v|^2}h\in C_0(R^6)\},
-\|h\|_a=\sup e^{-a|v|^2}|h|$$
+$$E_a^0={hin C(R^6):e^{-a|v|^2}hin C_0(R^6)},
+|h|_a=sup e^{-a|v|^2}|h|$$
on which smooth compactly supported tests are dense. Let
-$\mathsf S_uh(x,v)=h(x+uv,v)$ be free test transport and
-$K_t=A_t-v\cdot\nabla_x$.
+$mathsf S_uh(x,v)=h(x+uv,v)$sfS_uh(x,v)=h(x+uv,v)$ be free test transport and
+$K_t=A_t-vcdotnabla_x$.
-Lemma (Backward evolution). For $0\le a<b<2\beta$ and $0\le r\le t\le T$ there is a bounded backward
-propagator $U(r,t):E_a^0\to E_b^0$ solving
+Lemma (Backward evolution). For $0le a<b<2beta$ and $0le rle tle T$ there is a bounded backward
+propagator $U(r,t):E_a^0to E_b^0$ solving
-$$U(r,t)h=\mathsf S_{t-r}h+\int_r^t\mathsf S_{s-r}K_sU(s,t)h d s$$
+$$U(r,t)h=mathsf S_sfS_{t-r}h+int_r^tmathsf S_sfS_{s-r}K_sU(s,t)h d s$$
with the composition law at intermediate exponents and uniqueness as a
-mild propagator in these scales. For $\phi\in C_c^∞$,
+mild propagator in these scales. For $phiin C_c^∞$,
-$$U(r,t)\phi-\phi=\int_r^tU(r,s)A_s\phi d s$$
+$$U(r,t)phi-phi=int_r^tU(r,s)A_sphi d s$$
Proof.
-For $a$ in a compact subinterval of $[0,2\beta)$, energy conservation and
+For $a$ in a compact subinterval of $[0,2beta)$, energy conservation and
the Gaussian bound give
-$$|K_th|\le CM\|h\|_a(1+|v|)e^{a|v|^2},
-\|K_th\|_b\le CM(1+(b-a)^{-1/2})\|h\|_a$$
+$$|K_th|le CM|h|_a(1+|v|)e^{a|v|^2},
+|K_th|_ble CM(1+(b-a)^{-1/2})|h|_a$$
-using $|\Delta_h|\le4\|h\|_ae^{a(|v|^2+|v_*|^2)}$ and
-$\int B d \omega=\pi|v-v_*|$. Spatial tails vanish by replacing $\|h\|_a$
-with $\eta_h(x)=\sup_ve^{-a|v|^2}|h|$, and $K_th$ is continuous in
+using $|Delta_h|le4|h|_ae^{a(|v|^2+|v_*|^2)}$ and
+$int B d omega=pi|v-v_*|$. Spatial tails vanish by replacing $|h|_a$
+with $eta_h(x)=sup_ve^{-a|v|^2}|h|$, and $K_th$ is continuous in
$E_b^0$. Iterating the backward mild equation bounds the $n$-th
time-ordered term by
-$$((CM(t-r))^n)/(n!)(1+√(n/(b-a)))^n\|h\|_a$$
+$$((CM(t-r))^n)/(n!)(1+√(n/(b-a)))^n|h|_a$$
so the series converges for every finite $T$. Splitting a time simplex at
an intermediate time gives composition, and the same estimate on an
iterated remainder gives uniqueness with a positive exponent allowance.
-For compactly supported smooth $\phi$, differentiability of the series at
-its upper end (its final transport gives $U(r,t)(v\cdot\nabla_x\phi)$;
-the simplex faces give $U(r,t)K_t\phi$) converges with the Dyson bound,
-giving $∂_tU(r,t)\phi=U(r,t)A_t\phi$ and hence the upper-end identity.
+For compactly supported smooth $phi$, differentiability of the series at
+its upper end (its final transport gives $U(r,t)(vcdotnabla_xphi)$;
+the simplex faces give $U(r,t)K_tphi$) converges with the Dyson bound,
+giving $∂_tU(r,t)phi=U(r,t)A_tphi$ and hence the upper-end identity.
Proposition (Gaussian target). The fluctuating equation has a centered Gaussian solution on each
-test scale $E_a^0$, $0\le a<\beta$, mapping continuously and linearly into
+test scale $E_a^0$, $0le a<beta$, mapping continuously and linearly into
$L^2$ uniformly on $[0,T]$, with covariance
-$$E[\zeta_t(\phi)\zeta_s(\psi)]
-={} \int f_0 U(0,t)\phi U(0,s)\psi d z$$
+$$E[zeta_t(phi)zeta_s(psi)]
+={} int f_0 U(0,t)phi U(0,s)psi d z$$
-$$+\int_0^{\min(s,t)}C_r(U(r,t)\phi,U(r,s)\psi) d r$$
+$$+int_0^{min(s,t)}C_r(U(r,t)phi,U(r,s)psi) d r$$
It is unique in the class of solutions extending to these scales with
uniformly bounded second-moment norms. Thus the law in the fluctuation limit theorem
is well defined.
Proof.
-For $b<\beta$, energy conservation and the weighted integrability bound give
+For $b<beta$, energy conservation and the weighted integrability bound give
-$$|C_t(h,k)|\le CM\|h\|_b\|k\|_b\int f_t(1+|v|)e^{2b|v|^2} d x d v\le C_b\|h\|_b\|k\|_b$$
+$$|C_t(h,k)|le CM|h|_b|k|_bint f_t(1+|v|)e^{2b|v|^2} d x d vle C_b|h|_b|k|_b$$
choosing the moment exponent slightly above $2b$ to absorb $1+|v|$. The
initial form has the corresponding bound.
Let $I_0,I$ be independent isonormal Gaussians on $L^2(f_0 d z)$ and
-$L^2(\nu)$ with
-$ d \nu=\tfrac12B(v-v_*,\omega)f_r(x,v)f_r(x,v_*) d r d x d v d v_* d \omega$.
+$L^2(nu)$ with
+$ d nu=tfrac12B(v-v_*,omega)f_r(x,v)f_r(x,v_*) d r d x d v d v_* d omega$.
Define
-$$\zeta_t(h)=I_0(U(0,t)h)+I( 1 _{r\le t}\Delta_{U(r,t)h}),
-W_t(h)=I( 1 _{r\le t}\Delta_h)$$
+$$zeta_t(h)=I_0(U(0,t)h)+I( 1 _{rle t}Delta_{U(r,t)h}),
+W_t(h)=I( 1 _{rle t}Delta_h)$$
-For $h\in E_a^0$ propagate to $b\in(a,\beta)$ and apply
+For $hin E_a^0$ propagate to $bin(a,beta)$ and apply
the isonormal construction: the maps are well defined and
-$$\sup_{t\le T}\|\zeta_t(h)\|_{L^2}\le C_a\|h\|_a$$
+$$sup_{tle T}|zeta_t(h)|_{L^2}le C_a|h|_a$$
They are jointly Gaussian and linear with covariance the target covariance;
-orthogonality of disjoint time intervals in $L^2(\nu)$ gives independent
-increments of $W$, and $I_0\perp I$ gives initial independence.
+orthogonality of disjoint time intervals in $L^2(nu)$ gives independent
+increments of $W$, and $I_0perp I$ gives initial independence.
-Weak equation. For $\phi\in C_c^∞$, using the upper-end identity
+Weak equation. For $phiin C_c^∞$, using the upper-end identity
and boundedness of the isonormal maps against Bochner integrals,
-$\int_0^t\zeta_s(A_s\phi) d s=I_0(U(0,t)\phi-\phi)+
-I( 1 _{r\le t}\Delta_{U(r,t)\phi-\phi})$, which together with
-the isonormal construction is $\zeta_t(\phi)=\zeta_0(\phi)+\int_0^t\zeta_s(A_s\phi)
-d s+W_t(\phi)$.
+$int_0^tzeta_s(A_sphi) d s=I_0(U(0,t)phi-phi)+
+I( 1 _{rle t}Delta_{U(r,t)phi-phi})$, which together with
+the isonormal construction is $zeta_t(phi)=zeta_0(phi)+int_0^tzeta_s(A_sphi)
+d s+W_t(phi)$.
Uniqueness. On any candidate's probability space, construct the
backward mild field from its own initial field and noise. The difference
$D_t$ has zero initial field and noise, mean-square continuity, and the
-transport mild identity $D_t(\phi)=\int_0^tD_s(K_s\mathsf S_{t-s}\phi) d s$
-(finite-support Riemann sums with $\mathsf S_{t-s}\phi$). Iterating $n$
-times with $0\le a<b<\beta$ bounds its $L^2$ norm by
-$C_b\|\phi\|_a(CT)^n/n!(1+√(n/(b-a)))^n\to0$, proving uniqueness in
+transport mild identity $D_t(phi)=int_0^tD_s(K_smathsf S_sfS_{t-s}phi) d s$
+(finite-support Riemann sums with $mathsf S_sfS_{t-s}phi$). Iterating $n$
+times with $0le a<b<beta$ bounds its $L^2$ norm by
+$C_b|phi|_a(CT)^n/n!(1+√(n/(b-a)))^nto0$, proving uniqueness in
the class and uniqueness in law.
This is a Gaussian generalized field in the mean-square sense of
@@ -625,28 +625,28 @@ bound. Everything is either a definition that is needed or a
statement quoted from Deng--Hani--Ma with its source location. This is the only
place where an unproved external input enters.
-Fix $υ=3^{-4}=1/81$. Choose the excess bound $\Gamma$ as a large
+Fix $υ=3^{-4}=1/81$. Choose the excess bound $Gamma$ as a large
dimensional constant before the number of slabs $L$. Put
-$\tau=T/L$ and, with harmless integer roundings,
+$tau=T/L$ and, with harmless integer roundings,
-$$A_L=|\logε|, Λ_i=A_i^{30}, A_{i-1}=Λ_i^{30}$$
+$$A_L=|logε|, Λ_i=A_i^{30}, A_{i-1}=Λ_i^{30}$$
and for the analytic induction
-$$\beta_i=(1-(i)/(10L))\frac\beta2,
-\widetilde\beta_i=\frac{\beta_{i-1}+\beta_i}{2},
-\theta_i=(1-(i)/(10L))3^{-11}$$
+$$beta_i=(1-(i)/(10L))fracbeta2,
+widetildebeta_i=frac{beta_{i-1}+beta_i}{2},
+theta_i=(1-(i)/(10L))3^{-11}$$
Constants written $C$ inside an exponential factor $C^b$ are independent
of $L$; constants $C_*$ and $c_*>0$ may depend on $L$ and the kinetic
bounds but not on $ε$. Crucially, no moment order enters the choice of
-$\Gamma$ or $L$.
+$Gamma$ or $L$.
Restarted truncated dynamics. Work slab by slab. Within slab $i$,
restart the collision prehistory. At an incoming contact, accept the
elastic collision iff adding it to the current collision graph of
-that component keeps the component's particle count $\leΛ_i$ and its
-excess $\le\Gamma$; otherwise both particles continue straight. The
+that component keeps the component's particle count $leΛ_i$ and its
+excess $leGamma$; otherwise both particles continue straight. The
excess of a graph with $b$ edges, $n$ vertices, $k$ components is
$r=b-n+k$ (repeated edges counted with multiplicity); an internal contact
adds $1$, a merging contact adds the two excesses. Grazing, simultaneous,
@@ -659,12 +659,12 @@ the cutoff comparison, below.
Lemma (Kinetic envelopes). Under the kinetic assumption,
-$$\sup_{0\le t\le T}(\|f_t\|_{Bol,\beta}+\|\nabla_xf_t\|_{Bol,\beta})<∞$$
+$$sup_{0le tle T}(|f_t|_{Bol,beta}+|nabla_xf_t|_{Bol,beta})<∞$$
Proof.
Apply Deng--Hani--Ma, Proposition A.1 with decreasing exponent
-$\beta_*(t)=2\beta-\beta t/T$. Its hypothesis is the initial Gaussian bound, and its two initial summable spatial norms are that same initial bound;
-since $\beta_*(t)\ge\beta$, its conclusion gives the propagated envelope.
+$beta_*(t)=2beta-beta t/T$. Its hypothesis is the initial Gaussian bound, and its two initial summable spatial norms are that same initial bound;
+since $beta_*(t)gebeta$, its conclusion gives the propagated envelope.
This is Deng--Hani--Ma, Eq. (1.29).
Definition (Layered C/O history). A history consists of finitely many oriented particle lines and binary
@@ -689,12 +689,12 @@ designated roots if $i$ is the top slab), and $H_0$ the lines incident to
an initial link, where initial links join pairs of lines born at zero with
weight
-$$\ell_ε(x,x')= 1 _{|x-x'|\leε}+ε^υ 1 _{|x-x'|>ε}$$
+$$ell_ε(x,x')= 1 _{|x-x'|leε}+ε^υ 1 _{|x-x'|>ε}$$
An admissible dependent history satisfies:
-(i) $|H_i|\le A_i$; every C-cluster has $\leΛ_i$ lines and excess
-$\le\Gamma$; every layer component has $<Λ_i$ C-clusters.
+(i) $|H_i|le A_i$; every C-cluster has $leΛ_i$ lines and excess
+$leGamma$; every layer component has $<Λ_i$ C-clusters.
(ii) The cluster graph in each slab is a forest and every layer component
contains a root of its slab; every unrooted line is connected in its slab
@@ -702,7 +702,7 @@ to a rooted line.
(iii) The initial links form a forest.
-(iv) For $i\ge2$, each line in $H_i$ is connected within slab $i$ to a
+(iv) For $ige2$, each line in $H_i$ is connected within slab $i$ to a
different line of $H_i$, or to a line of $H_{i-1}$, or itself lies in
$H_{i-1}$ (replace $H_{i-1}$ by $H_0$ when $i=1$).
@@ -710,99 +710,99 @@ Connection in a slab means sharing a component of its atom graph; the last
alternative of (iv) covers a straight line with no atom there. These are
Deng--Hani--Ma, Definition 3.20(1). The complexity is
-$$\rho=|H_0|+\sum_i(|H_i|+r(\mathcal M_i))$$
+$$rho=|H_0|+sum_i(|H_i|+r(mathcal M_i))$$calM_i))$$
-with $r(\mathcal M_i)$ the cycle excess in slab $i$; since the O-graph is
+with $r(mathcal M_i)$calM_i)$ the cycle excess in slab $i$; since the O-graph is
a forest this is the sum of C-cluster excesses. $b$ denotes the number of
atoms.
Integral convention. Give each bond $e$ a vector $z_e=(x_e,v_e)$
with position $X_e(t)=x_e+tv_e$; give atom $a$ a time $t_a$. Its incoming
edges are $1,2$ and serial outgoing edges $1',2'$. On the contact surface
-put $u=v_1-v_2$, $\omega=(X_1(t_a)-X_2(t_a))/ε$, and
-$\mathfrak b=[-u\cdot\omega]_+$. Define
+put $u=v_1-v_2$, $omega=(X_1(t_a)-X_2(t_a))/ε$, and
+$mathfrak b=[-ufrakb=[-ucdotomega]_+$. Define
-$$\Delta_a^{\mathrm C}
-=\delta(|X_1-X_2|-ε)\mathfrak b
-\prod_{j=1}^2\delta(X_{j'}(t_a)-X_j(t_a))
-\delta(v_{1'}-v_1+(u\cdot\omega)\omega)\delta(v_{2'}-v_2-(u\cdot\omega)\omega)$$
+$$Delta_a^{mathrm C}rmC
+=delta(|X_1-X_2|-ε)mathfrak bfrakb
+prod_{j=1}^2delta(X_{j'}(t_a)-X_j(t_a))
+delta(v_{1'}-v_1+(ucdotomega)omega)delta(v_{2'}-v_2-(ucdotomega)omega)$$
-$$\Delta_a^{\mathrm O}
-=\delta(|X_1-X_2|-ε)\mathfrak b
-\prod_{j=1}^2\delta(x_{j'}-x_j)\delta(v_{j'}-v_j)$$
+$$Delta_a^{mathrm O}rmO
+=delta(|X_1-X_2|-ε)mathfrak bfrakb
+prod_{j=1}^2delta(x_{j'}-x_j)delta(v_{j'}-v_j)$$
-Reverse $\omega$ to match the scattering convention; surface measure is
+Reverse $omega$ to match the scattering convention; surface measure is
unnormalized. With a set $E_*$ of integrated bonds and free ends, the
positive measure of a cut history $M$ with kernel $Q$ is
$$I_M(Q)(z_{fixed})
-:=\mu^{|E_*|-2b}\int_{\mathcal D_M}\int Q(z_E,t_M)
-\prod_{a\in M}\Delta_a\prod_{e\in E_*} d z_e\prod_{a\in M} d t_a$$
+:=mu^{|E_*|-2b}int_{mathcal D_M}calD_Mint Q(z_E,t_M)
+prod_{ain M}Delta_aprod_{ein E_*} d z_eprod_{ain M} d t_a$$
-where $\mathcal D_M$ enforces the slab and strictly increasing times along
+where $mathcal D_M$calD_M$ enforces the slab and strictly increasing times along
each line. For a full history $|E|-2b=n=$ number of lines, and with $h$
roots the normalized integral is
-$$\mathcal J_M(Q)=\mu^{-h}I_M(Q):$$
+$$mathcal J_M(Q)=calJ_M(Q)=mu^{-h}I_M(Q):$$
-each birth carries activity $\mu$, each root a normalization $\mu^{-1}$,
+each birth carries activity $mu$, each root a normalization $mu^{-1}$,
each contact surface a factor $ε^2$ Deng--Hani--Ma, Proposition 7.5, Eq. (7.7).
To keep a root endpoint $(x,v)$ at time $t$ free, make its top end a fixed
end evaluated at $(x-tv,v)$, removing the root activity.
-The one-slab class $\mathcal T_i$ consists of connected histories with one
+The one-slab class $mathcal T_i$calT_i$ consists of connected histories with one
top root, conditions (i)--(ii) only, no continuation or initial-link
-requirement; it may have up to $\simΛ_i^2$ lines.
-$\mathcal T_i^{err}$ inserts one extra O-atom into a member of
-$\mathcal T_i$. The one-root signed tree sum contains every one-root
+requirement; it may have up to $simΛ_i^2$ lines.
+$mathcal T_i^calT_i^{err}$ inserts one extra O-atom into a member of
+$mathcal T_i$.calT_i$. The one-root signed tree sum contains every one-root
particle-line tree of size $<Λ_i/3$, with C/O choices and sign
-$(-1)^{\#\mathrm O}$.
+$(-1)^{#mathrm O}rmO$.
Theorem (Deng--Hani--Ma analytic package). Assume the kinetic assumption, the cutoff hierarchy, the exponent hierarchy, and a common Gaussian $Bol$ bound on all birth
inputs. For $L$ sufficiently large (fixed) and $ε$ sufficiently small:
(a) For admissible dependent histories with prescribed labeled roots,
-fixed $b$, and complexity $\rho$, the normalized positive integral sums
+fixed $b$, and complexity $rho$, the normalized positive integral sums
to at most
-$$C^b\tau^{b/10}ε^{c_*\rho}|\logε|^{C_*\rho}$$
+$$C^btau^{b/10}ε^{c_*rho}|logε|^{C_*rho}$$
The sum includes graph enumeration and admissibility restrictions;
bounded observable multipliers cost their supremum. Birth inputs need
only satisfy the common Gaussian $Bol$ envelope.
(b) If the independent input $g$ in slab $i$ has
-$\|g-f_{(i-1)\tau}\|_{Bol,\beta_{i-1}}\leε^{\theta_{i-1}}$, then the
-signed tree sum $\mathsf T_i^ε[g]$ satisfies
+$|g-f_{(i-1)tau}|_{Bol,beta_{i-1}}leε^{theta_{i-1}}$, then the
+signed tree sum $mathsf T_i^ε[g]$sfT_i^ε[g]$ satisfies
-$$\|\mathsf T_i^ε[g]-f_{i\tau}\|_{Bol,\beta_i}\le\tfrac12ε^{\theta_i}$$
+$$|mathsf T_i^ε[g]-f_sfT_i^ε[g]-f_{itau}|_{Bol,beta_i}letfrac12ε^{theta_i}$$
-In the fixed-top-endpoint norm $Bol,\widetilde\beta_i$, the summed
-absolute contributions of cyclic $\mathcal T_i$, of
-$\mathcal T_i^{err}$, and of $\mathcal T_i$ with $\geΛ_i/3$
-lines are $o(ε^{\theta_i})$. Fixed cutoff powers and a fixed
+In the fixed-top-endpoint norm $Bol,widetildebeta_i$, the summed
+absolute contributions of cyclic $mathcal T_i$,calT_i$, of
+$mathcal T_i^calT_i^{err}$, and of $mathcal T_i$calT_i$ with $geΛ_i/3$
+lines are $o(ε^{theta_i})$. Fixed cutoff powers and a fixed
exponential-atom factor can be included, the latter absorbed by large
$L$.
-Part (b) holds uniformly for a slab truncated at any $0\le\sigma\le\tau$,
-with target $f_{(i-1)\tau+\sigma}$; at $\sigma=0$ the map is the identity.
+Part (b) holds uniformly for a slab truncated at any $0lesigmaletau$,
+with target $f_{(i-1)tau+sigma}$; at $sigma=0$ the map is the identity.
Proof (Source and envelope adaptations).
For (a): Deng--Hani--Ma, Proposition 7.2 counts root-labeled unlabeled histories by
-$C^b|\logε|^{C_*\rho}$; Deng--Hani--Ma, Proposition 9.7 and Eq. (9.51) retain a
-positive gain $\propto\rho$; after regular cutting, Deng--Hani--Ma, Eq. (9.53)
+$C^b|logε|^{C_*rho}$; Deng--Hani--Ma, Proposition 9.7 and Eq. (9.51) retain a
+positive gain $proptorho$; after regular cutting, Deng--Hani--Ma, Eq. (9.53)
bounds each full edge integral by
-$\tau^{b/9}ε^{-2h+2υ/5+c_*\rho}|\logε|^{C_*\rho}$.
-Multiplication by $\mu^{-h}=ε^{2h}$ cancels the root power; weakening
-$1/9\to1/10$ and discarding the extra positive power gives
+$tau^{b/9}ε^{-2h+2υ/5+c_*rho}|logε|^{C_*rho}$.
+Multiplication by $mu^{-h}=ε^{2h}$ cancels the root power; weakening
+$1/9to1/10$ and discarding the extra positive power gives
the coarse bound. These are the estimates inside the proof of Deng--Hani--Ma, Proposition 6.2, Section 9.2, not only its displayed conclusion.
The only use of a birth density is the envelope decomposition Deng--Hani--Ma, Eqs. (9.58)--(9.63): from (1) choose a summable
sequence $(m_a)$ bounding the weighted supremum on unit balls; bounded
-overlap and $\sum_am_a<∞$ dominate $|g|$ by
-$C\sum_am_a 1 _{|x-a|\le1}e^{-\beta'|v|^2}$, and the positive source
+overlap and $sum_am_a<∞$ dominate $|g|$ by
+$Csum_am_a 1 _{|x-a|le1}e^{-beta'|v|^2}$, and the positive source
estimates applied to each envelope product sum by
-$\sum_am_a<∞$. This extends (a) to arbitrary bounded inputs,
+$sum_am_a<∞$. This extends (a) to arbitrary bounded inputs,
including absolute values of signed inputs. Multipliers in $[0,1]$ are
kept or dropped only when taking a positive upper bound.
@@ -810,35 +810,35 @@ For (b): the one-root integral is a function of a fixed endpoint
Deng--Hani--Ma, Eq. (14.2); the C/O involution Deng--Hani--Ma, Proposition 14.2 cancels
noncausal trees; the causal remainder satisfies the Gaussian $Bol$
estimate Deng--Hani--Ma, Proposition 14.3, Eq. (14.8); comparison to the short-time
-Boltzmann expansion, using the kinetic envelope bound, is Deng--Hani--Ma, Proposition 6.1, Section 14. To pass from $f_{(i-1)\tau}$ to $g$, expand each birth factor as
-$f_{(i-1)\tau}+(g-f_{(i-1)\tau})$; each residual costs
-$ε^{\theta_{i-1}}$ by hypothesis, and the multilinear tree bound sums
-all choices; since $\theta_{i-1}>\theta_i$ the residuals are
-$o(ε^{\theta_i})$. For the positive subleading terms the bound is
-Deng--Hani--Ma, Eq. (14.28) in $Bol,\widetilde\beta_i$ with a time power per atom
-and gain $ε^{υ/3+c_*\rho}$ in cyclic and extra-encounter
+Boltzmann expansion, using the kinetic envelope bound, is Deng--Hani--Ma, Proposition 6.1, Section 14. To pass from $f_{(i-1)tau}$ to $g$, expand each birth factor as
+$f_{(i-1)tau}+(g-f_{(i-1)tau})$; each residual costs
+$ε^{theta_{i-1}}$ by hypothesis, and the multilinear tree bound sums
+all choices; since $theta_{i-1}>theta_i$ the residuals are
+$o(ε^{theta_i})$. For the positive subleading terms the bound is
+Deng--Hani--Ma, Eq. (14.28) in $Bol,widetildebeta_i$ with a time power per atom
+and gain $ε^{υ/3+c_*rho}$ in cyclic and extra-encounter
classes; Section 14.3 Points 1--2 keep the Gaussian weight at the fixed root and
the spatial $Bol$ sum, Point 4 regularizes an O-atom adjacent to the root
without changing its integral. The tree-tail branch of Point 5 uses only
-that the atom number is of cutoff order, so $Λ_i\toΛ_i/3$
+that the atom number is of cutoff order, so $Λ_itoΛ_i/3$
leaves an exponentially small tail. Graph enumeration, the bounded
selected-edge choices, and fixed exponential factors are absorbed by
taking $L$ large. For the partial slab, restrict contact times to
-$((i-1)\tau,(i-1)\tau+\sigma)$ and repeat the fixed-root Gaussian and
-spatial localization at endpoint $(x-\sigma v,v)$; all shifts are $\le\tau$
+$((i-1)tau,(i-1)tau+sigma)$ and repeat the fixed-root Gaussian and
+spatial localization at endpoint $(x-sigma v,v)$; all shifts are $letau$
so the exponent margin survives. The signed involution preserves the
-restriction and the upper majorants keep their full-$\tau$ bounds. At
-$\sigma=0$ only the zero-atom tree remains, i.e. $g$, and
-$\theta_{i-1}>\theta_i$ gives the bound.
+restriction and the upper majorants keep their full-$tau$ bounds. At
+$sigma=0$ only the zero-atom tree remains, i.e. $g$, and
+$theta_{i-1}>theta_i$ gives the bound.
Lemma (Coarse boundary modifications). The positive coarse bound tolerates:
(i) dropping continuation condition (iv) in the top slab with $h$ roots,
at the cost of a loss $ε^{-C_*h}$;
-(ii) a connected pure-C terminal component with $\le3Λ_i$ lines and
-excess $\le2\Gamma$, meeting a lower continuation but with no designated
-root, at cost $\mu$ (add one artificial root);
+(ii) a connected pure-C terminal component with $le3Λ_i$ lines and
+excess $le2Gamma$, meeting a lower continuation but with no designated
+root, at cost $mu$ (add one artificial root);
(iii) supplying initial-link continuations to a fixed number $q$ of
specified lines, at cost $ε^{-qυ}$ (add $q$ dummy straight
@@ -848,28 +848,28 @@ Bounded records carried by these lines are kept.
Proof (Source and construction).
(i): use the error form of the cutting inequality Deng--Hani--Ma, Eq. (9.51)
-retaining its deficit $\propto h$. The finale Deng--Hani--Ma, Section 13.5, p. 169 splits
-into a bounded-$\rho$ case, where the UP algorithm makes $\le h$ free-
-component ``bad pieces'' paid by the root deficit, and a large-$\rho$ case
+retaining its deficit $propto h$. The finale Deng--Hani--Ma, Section 13.5, p. 169 splits
+into a bounded-$rho$ case, where the UP algorithm makes $le h$ free-
+component ``bad pieces'' paid by the root deficit, and a large-$rho$ case
using the dependent cutting argument with the continuation condition of a
strictly lower layer still available; the resulting positive integration
gives the loss $ε^{-C_*h}$ of Deng--Hani--Ma, Eq. (9.82). Terminal size is used
only later and absorbed by the time power.
(ii): take one line of the terminal component as root; its normalization
-costs $\mu^{-1}$ and multiplication by $\mu$ restores the integral.
-Splitting into $\leΛ_i$ lines and $\le\Gamma$ excess (ordinary
+costs $mu^{-1}$ and multiplication by $mu$ restores the integral.
+Splitting into $leΛ_i$ lines and $leGamma$ excess (ordinary
admissible) versus the enlarged terminal class of Deng--Hani--Ma, Definition 3.20(4), the same root operation is Deng--Hani--Ma, Eq. (15.4); summing over the
choice of line costs a cutoff polynomial.
-(iii): fix nonnegative $q_0$ with $\int q_0=1$ and finite Gaussian $Bol$
+(iii): fix nonnegative $q_0$ with $int q_0=1$ and finite Gaussian $Bol$
norm; for every $x$,
$$
-\int q_0(x',v')\ell_ε(x,x') d x' d v'\geε^υ .
+int q_0(x',v')ell_ε(x,x') d x' d v'geε^υ .
$$
Insert once
-per continuation: the dummy activity $\mu$ cancels the extra root factor
-$\mu^{-1}$, its straight line satisfies continuation in every slab, and
+per continuation: the dummy activity $mu$ cancels the extra root factor
+$mu^{-1}$, its straight line satisfies continuation in every slab, and
the new links are pendant so the initial forest is preserved. This is a
positive kernel inequality, valid even where $f_0$ vanishes; the envelope
extension of the analytic package admits $q_0$, and records are
@@ -887,11 +887,11 @@ process, not a factorization assumption.
Put
-$$M_i=\lfloorΛ_i/2\rfloor$$
+$$M_i=lfloorΛ_i/2rfloor$$
the expansion cluster cap. It differs from the dynamics caps
-$Λ_i,\Gamma$ and belongs only to the expansion; take $ε$ small so
-$M_i\ge2$ for all $i$.
+$Λ_i,Gamma$ and belongs only to the expansion; take $ε$ small so
+$M_ige2$ for all $i$.
Idea. Run each subset of particles on its own, with the truncated
collision rule. The full truncated history is then a union of ``autonomous
@@ -903,25 +903,25 @@ Fix a slab (suppress its index). Let $V$ be a finite labelled particle set.
A particle state may carry previously observed test values, or their
running sum, as extra coordinates called records; the acceptance rule uses
only positions, velocities, and the prehistory on this slab. For
-$C⊆ V$, $\Psi_C$ is the autonomous truncated evolution of $C$
-(including its observation updates), and $\kappa_C$ is the indicator that
-its accepted collision graph is connected (singletons $\kappa_\bullet=1$;
-$|C|>Λ⇒\kappa_C=0$). For disjoint $C,D$, $a(C,D)$
+$C⊆ V$, $Psi_C$ is the autonomous truncated evolution of $C$
+(including its observation updates), and $kappa_C$ is the indicator that
+its accepted collision graph is connected (singletons $kappa_bullet=1$;
+$|C|>Λ⇒kappa_C=0$). For disjoint $C,D$, $a(C,D)$
indicates an incoming cross-contact that would be accepted with
-their respective prefix prehistories, and $\chi(C,D)=1-a(C,D)$. These are
+their respective prefix prehistories, and $chi(C,D)=1-a(C,D)$. These are
indicators, not counts. All identities are on the common full-measure set
where all finite subsystems are defined.
Lemma (Autonomous partition). For finite $V$,
-$$\sum_{\mathcal C\in\mathcal P(V)}\prod_{C\in\mathcal C}\kappa_C
-\prod_{\{C,D\}⊆\mathcal C}\chi(C,D)=1$$
+$$sum_{mathcal CcalCinmathcal P(V)}calP(V)prod_{Cinmathcal C}calCkappa_C
+prod_{{C,D}⊆mathcal C}calCchi(C,D)=1$$
For $S⊆ V$ and a root test $H$,
-$$H(\Psi_V|_S)=\sum_{\mathcal C\in\mathcal P(V)}
-\prod_{C\in\mathcal C}\kappa_C\prod_{\{C,D\}⊆\mathcal C}\chi(C,D)
-H(\Psi_{\mathcal C}|_S)$$
+$$H(Psi_V|_S)=sum_{mathcal CcalCinmathcal P(V)}calP(V)
+prod_{Cinmathcal C}calCkappa_Cprod_{{C,D}⊆mathcal C}calCchi(C,D)
+H(Psi_{mathcal C}calC|_S)$$
Proof.
The collision components of the full truncated history give one summand
@@ -929,31 +929,31 @@ $=1$; its restrictions are autonomous because no accepted collision joins
components and the rule is prefix-local. Conversely, if all factors of a
summand equal one, juxtapose the autonomous histories and scan incoming
contacts in time order: internal accepted contacts obey the rule, every
-cross-contact fails it by $\chi=1$, so the juxtaposition is the full
+cross-contact fails it by $chi=1$, so the juxtaposition is the full
truncated history, and uniqueness identifies its components with
-$\mathcal C$.
+$mathcal C$.calC$.
The next lemma is finite algebra; its vertices will be autonomous clusters.
-Lemma (Rooted forest stopping). Let $W$ be finite, $R⊆ W$ nonempty, $a_e\in\{0,1\}$ for each pair,
-$M\ge2$, and
+Lemma (Rooted forest stopping). Let $W$ be finite, $R⊆ W$ nonempty, $a_ein{0,1}$ for each pair,
+$Mge2$, and
-$$u(B)=\sum_{\substack{G connected\\V(G)=B}}\prod_{e\in E(G)}(-a_e),
-u(\{w\})=1$$
+$$u(B)=sum_{substack{G connectedV(G)=B}}prod_{ein E(G)}(-a_e),
+u({w})=1$$
-There is a finite signed remainder $\mathcal R$ with
+There is a finite signed remainder $mathcal R$calR$ with
-$$\prod_{e⊆ W}(1-a_e)
-=\sum_{R⊆ I⊆ W}
-\sum_{\substack{\mathcal B\in\mathcal P(I)\ B\cap R\ne∅, |B|<M (B\in\mathcal B)}}
-\prod_{B\in\mathcal B}u(B)\prod_{e⊆ W∖ I}(1-a_e)+\mathcal R$$
+$$prod_{e⊆ W}(1-a_e)
+=sum_{R⊆ I⊆ W}
+sum_{substack{mathcal BcalBinmathcal P(I)calP(I) Bcap Rne∅, |B|<M (Binmathcal B)}calB)}
+prod_{Binmathcal B}calBu(B)prod_{e⊆ W∖ I}(1-a_e)+mathcal R$$calR$$
-$|\mathcal R|$ is bounded by a sum of rooted forests, each with exactly one
+$|mathcal R|$calR|$ is bounded by a sum of rooted forests, each with exactly one
component of size in $[M,2M-2]$ and all other components smaller than $M$,
all meeting $R$, vertices off the forest keeping their mutual compatibility
-product, each selected forest with coefficient $\le1$. Moreover
+product, each selected forest with coefficient $le1$. Moreover
-$$|u(B)|\le\sum_{T spanning tree}\prod_{e\in E(T)}a_e$$
+$$|u(B)|lesum_{T spanning tree}prod_{ein E(T)}a_e$$
Proof.
Order the pairs. Grow the empty forest: at each step take the first
@@ -970,8 +970,8 @@ $u(B)$ with survivors keeping their compatibility product, giving the main
term; stopped branches give the forest bound. For the tree inequality, fix
a total edge order on $B$, assign each connected graph its minimum spanning
tree $T$, let $Q(T)$ be the edges later than the whole $T$-path; then
-connected graphs on $B$ are exactly $T⊆ G⊆ T\cup Q(T)$, so
-$u(B)=(-1)^{|B|-1}\sum_T\prod_{e\in T}a_e\prod_{e\in Q(T)}(1-a_e)$; since
+connected graphs on $B$ are exactly $T⊆ G⊆ Tcup Q(T)$, so
+$u(B)=(-1)^{|B|-1}sum_Tprod_{ein T}a_eprod_{ein Q(T)}(1-a_e)$; since
the second product lies in $[0,1]$, dropping it proves
the autonomous partition.
@@ -980,76 +980,76 @@ single linear operator on the factorial hierarchy. Its ``retained'' part
keeps bounded rooted blocks; its ``stopped'' part bounds the remainder by
a positive forest integral.
-Write $F_s$ for ordered factorial measures normalized by $\mu^s$ (records
+Write $F_s$ for ordered factorial measures normalized by $mu^s$ (records
allowed on a specified subset of the $s$ labels). Using symmetric Janossy
-measures $p_n$ ($\sum_n p_n(E^n)/n!=1$, $p_n/n!$ the law restricted to
+measures $p_n$ ($sum_n p_n(E^n)/n!=1$, $p_n/n!$ the law restricted to
$N=n$),
-$$F_s=\mu^{-s}\sum_{n\ge s}(1)/((n-s)!)(pr_{[s]})_\#p_n$$
+$$F_s=mu^{-s}sum_{nge s}(1)/((n-s)!)(pr_{[s]})_#p_n$$
For $S=[s]$, $V=[s+j]$, define the signed root-output kernel
-$$\mathcal K_{S,V}(X, d X'_S)
-=\sum_{\mathcal C\in\mathcal P(V)}\prod_{C\in\mathcal C}\kappa_C(X)
-\sum_{\substack{\mathcal B\in\mathcal P(\mathcal C)\\
-(∪_{C\in B}C)\cap S\ne∅, |B|<M}}
-\prod_{B\in\mathcal B}u(B;X) \delta_{\Psi_{\mathcal C}(X)|_S}( d X'_S)$$
+$$mathcal K_calK_{S,V}(X, d X'_S)
+=sum_{mathcal CcalCinmathcal P(V)}calP(V)prod_{Cinmathcal C}calCkappa_C(X)
+sum_{substack{mathcal BcalBinmathcal P(calP(mathcal C)calC)
+(∪_{Cin B}C)cap Sne∅, |B|<M}}
+prod_{Binmathcal B}calBu(B;X) delta_{Psi_{mathcal C}calC(X)|_S}( d X'_S)$$
and the retained operator
-$$(\mathcal L_sF)( d X'_S)
-=\sum_{j=0}^{s(M-1)Λ-s}(\mu^j)/(j!)
-\int F_{s+j}( d X_V) \mathcal K_{S,V}(X, d X'_S)$$
+$$(mathcal L_sF)(calL_sF)( d X'_S)
+=sum_{j=0}^{s(M-1)Λ-s}(mu^j)/(j!)
+int F_{s+j}( d X_V) mathcal K_calK_{S,V}(X, d X'_S)$$
(An empty restriction is zero; at most $s$ retained blocks, so the bound on
$j$ follows from the caps.) The stopped kernel replaces the inner
block sum by
-$\sum_{F\in\mathfrak F^{stop}_S(\mathcal C)}\prod_{e\in E(F)}a_e(X)$,
-where $\mathfrak F^{stop}_S(\mathcal C)$ are forests spanning
-$\mathcal C$ with every component meeting $S$, exactly one of size
+$sum_{Finmathfrak F^frakF^{stop}_S(mathcal C)}calC)prod_{ein E(F)}a_e(X)$,
+where $mathfrak F^frakF^{stop}_S(mathcal C)$calC)$ are forests spanning
+$mathcal C$calC$ with every component meeting $S$, exactly one of size
$[M,2M-2]$, the rest smaller, no unrooted isolated cluster; keep
-$\prod_C\kappa_C$ and the root-output map. Define $\mathcal E_sF$ by
+$prod_Ckappa_C$ and the root-output map. Define $mathcal E_sF$calE_sF$ by
the retained operator with this kernel and $j$ up to
-$$j\le(s+1)(M-1)Λ-s$$
+$$jle(s+1)(M-1)Λ-s$$
Lemma (One-slab identity and variation remainder). For a positive input law with factorial hierarchy $F$, let $F'$ be its
hierarchy after the truncated slab. If factorial measures up to
the fresh-label bound are finite, then
-$$F'_s=\mathcal L_sF+R_s, |R_s|\le\mathcal E_sF$$
+$$F'_s=mathcal L_sF+R_s,calL_sF+R_s, |R_s|lemathcal E_sF$$calE_sF$$
-The record version holds, and $\mathcal E_sF$ is a positive domination of
+The record version holds, and $mathcal E_sF$calE_sF$ is a positive domination of
$R_s$, not a claim that $R_s$ has this local kernel.
Proof.
Insert the one-slab identity and the rooted forest stopping lemma into
the branch recursion. On a completed branch, fix the reached labels
-$V\supset S$, $|V|=s+j$; the unreached cluster partitions sum to one
+$Vsupset S$, $|V|=s+j$; the unreached cluster partitions sum to one
pointwise by the stopped bound, using no independence of the
input, and
-$\frac1{(n-s)!}\binom{n-s}{j}=\frac1{j!(n-s-j)!}$ turns the remaining sum
-into $\mu^{s+j}F_{s+j}$; the output normalization $\mu^{-s}$ leaves
-$\mu^j/j!$. Stopped terms keep only the unreached compatibility product and
+$frac1{(n-s)!}binom{n-s}{j}=frac1{j!(n-s-j)!}$ turns the remaining sum
+into $mu^{s+j}F_{s+j}$; the output normalization $mu^{-s}$ leaves
+$mu^j/j!$. Stopped terms keep only the unreached compatibility product and
drop the rest, so positivity of the input and the multiplicity bound give
-$|R_s(H)|\le(\mathcal E_sF)(|H|)$; there are $\le s$ rooted components and
+$|R_s(H)|le(mathcal E_sF)(|H|)$;calE_sF)(|H|)$; there are $le s$ rooted components and
only one of size up to $2M-2$ clusters, giving
the fresh-label bound. Records are untouched by the spectator
summation and travel with the root-output map.
-For a signed family $\Delta$ (uniformly in records and $s\le A_i/2$),
+For a signed family $Delta$ (uniformly in records and $sle A_i/2$),
-$$\|\mathcal L_{i,s}\Delta\|_{TV}+\|\mathcal E_{i,s}|\Delta|\|_{TV}
-\le e^{C_*A_iΛ_i^2\log(1/ε)}\max_{q\le A_{i-1}/2}\|\Delta_q\|_{TV}$$
+$$|mathcal L_calL_{i,s}Delta|_{TV}+|mathcal E_calE_{i,s}|Delta||_{TV}
+le e^{C_*A_iΛ_i^2log(1/ε)}max_{qle A_{i-1}/2}|Delta_q|_{TV}$$
-Indeed relevant $q\le(s+1)Λ_i^2/2<A_{i-1}/2$, with at most $q^q$
-particle and $q^q$ cluster partitions, spanning/forest sum $\le q^{2q}$,
-activity $\le\mu^q$, and at most $A_iΛ_i^2$ values of $q$; take logs.
+Indeed relevant $qle(s+1)Λ_i^2/2<A_{i-1}/2$, with at most $q^q$
+particle and $q^q$ cluster partitions, spanning/forest sum $le q^{2q}$,
+activity $lemu^q$, and at most $A_iΛ_i^2$ values of $q$; take logs.
Define the unmarked one-root measures recursively by
-$$g_i=\mathcal U_i(g_{i-1}),
-\mathcal U_i(g):=\mathcal L_{i,1}((g^{ ⊗ q})_{q\ge0})$$
+$$g_i=mathcal U_i(g_calU_i(g_{i-1}),
+mathcal U_i(g):=calU_i(g):=mathcal L_calL_{i,1}((g^{ ⊗ q})_{qge0})$$
a finite signed measure using the full retained one-root block. It
approximates the Boltzmann density:
@@ -1057,46 +1057,46 @@ approximates the Boltzmann density:
Proposition (Independent factors). $g_i$ has a Gaussian $Bol$-bounded density representative and, with the
exponents of the analytic package,
-$$\|g_i-f_{i\tau}\|_{Bol,\beta_i}\leε^{\theta_i},
-\sup_{0\le i\le L}\|g_i\|_{Bol,\beta_i}\le C$$
+$$|g_i-f_{itau}|_{Bol,beta_i}leε^{theta_i},
+sup_{0le ile L}|g_i|_{Bol,beta_i}le C$$
with the same bounds for the one-root map run through any partial slab
-$\sigma\in[0,\tau]$, target $f_{(i-1)\tau+\sigma}$.
+$sigmain[0,tau]$, target $f_{(i-1)tau+sigma}$.
The bridge from the retained block to the unrestricted tree sum is the
following; it is where ``retained'' and ``DHM signed trees'' are shown to
differ only by error classes.
-Lemma (Modified one-root bridge). The difference between $\mathcal U_i(g)$ and the signed unrestricted
+Lemma (Modified one-root bridge). The difference between $mathcal U_i(g)$calU_i(g)$ and the signed unrestricted
one-root particle-tree sum with $n<Λ_i/3$ is dominated, with inputs
replaced by $|g|$, by the positive integrals of
-(i) retained one-root molecules with cycle excess $r\ge1$;
+(i) retained one-root molecules with cycle excess $rge1$;
-(ii) retained one-root molecules with $n\geΛ_i/3$;
+(ii) retained one-root molecules with $ngeΛ_i/3$;
(iii) small unrestricted trees with one extra incoming O-atom inserted
between two flight segments.
Families (i)--(ii) are subsets of the DHM one-root class; (iii) is its
additional-overlap class. Coefficients carry only a fixed cutoff power, and
-the leading tree coefficient is exactly $(-1)^{\#\mathrm O}$ with the
-labelled factorial $\mu^{n-1}/(n-1)!$.
+the leading tree coefficient is exactly $(-1)^{#mathrm O}rmO$ with the
+labelled factorial $mu^{n-1}/(n-1)!$.
Proof.
Apply the autonomous partition to the single retained block and refine
each autonomous C-cluster by its ordered accepted collisions; the internal
indicator is at most the prescribed-C-contact indicator. Each chosen
cluster-tree edge demands a prospective accepted encounter between two
-isolated histories. A cluster of $q$ particles has $\le q-1+\Gamma$
-collisions, so each pair of straight segments has $\le1$ incoming contact;
+isolated histories. A cluster of $q$ particles has $le q-1+Gamma$
+collisions, so each pair of straight segments has $le1$ incoming contact;
partition the encounter event by the first admissible segment pair, giving
disjoint encounter indicators with weights in $[0,1]$. Ordering these along
lines gives particle-line molecules. C-clusters plus the O forest determine
-the connected block with sign $(-1)^{\#\mathrm O}$ and global excess equal
-to the sum of C-cluster excesses, so cyclic terms and $n\geΛ_i/3$
+the connected block with sign $(-1)^{#mathrm O}rmO$ and global excess equal
+to the sum of C-cluster excesses, so cyclic terms and $ngeΛ_i/3$
terms are exactly (i)--(ii), inside the DHM caps $Λ_i<∞$,
-$\Gamma$. A remaining tree molecule with no other encounters has autonomous
+$Gamma$. A remaining tree molecule with no other encounters has autonomous
C-clusters equal to the displayed ones, every O contact the unique selected
one, and unused factors equal to one; otherwise the first undesignated
accepted contact (or a discarded compatibility factor, or a nonfirst
@@ -1105,12 +1105,12 @@ cluster-pair contact) inserts an O-atom that changes no velocity, giving
is admitted with the displayed sign, so no symmetry factor is dropped.
Proof of the independent-factor construction.
-the initial ensemble gives $\|g_0-f_0\|_{Bol,\beta_0}\le Cε$, which is
-the initial smallness for $\theta_0<1$. Assume the bound at the preceding
+the initial ensemble gives $|g_0-f_0|_{Bol,beta_0}le Cε$, which is
+the initial smallness for $theta_0<1$. Assume the bound at the preceding
interface. the one-root bridge plus the fixed-endpoint part of
the analytic package bounds the three error families and compares the
-signed small-tree sum with $f_{i\tau}$, under the preceding
-$Bol,\beta_{i-1}$ error, to $o(ε^{\theta_i})$, giving the induction and
+signed small-tree sum with $f_{itau}$, under the preceding
+$Bol,beta_{i-1}$ error, to $o(ε^{theta_i})$, giving the induction and
the uniform $Bol$ bound. The estimate is a fixed-endpoint $Bol$ one, not
an integrated $L^1$ inference, so it also gives density representatives;
restricting contact times gives the uniform partial-slab version.
@@ -1119,21 +1119,21 @@ Fix finitely many observation pulses. Let $m$ bound both the number of
pulses and of record-carrying labels; record coordinates lie in a fixed
bounded interval. For a root set $S$ and required records on $R⊆ S$,
let $F^R_{i,S}$ be the pasted factorial measure at interface $i$ with record
-coordinates on $R$. The operators $\mathcal L_i$ append the slab
+coordinates on $R$. The operators $mathcal L_i$calL_i$ append the slab
observations on the same labels; compatibility is record-independent. The
retained hierarchy is the finite composition
-$$\widehat F^R_i=\mathcal L_i\mathcal L_{i-1}...\mathcal L_1F^R_0$$
+$$widehatwidehat F^R_i=F^R_i=mathcal L_icalL_imathcal L_calL_{i-1}...mathcal L_1F^R_0$$calL_1F^R_0$$
well defined order by order (finitely many previous orders per output).
Lemma (Resummation with records). There is an exact finite expansion
-$$\widehat F^R_{i,S}=\sum_{R⊆ H⊆ S}E^R_{i,H} ⊗ g_i^{ ⊗ (S∖ H)}$$
+$$widehatwidehat F^R_F^R_{i,S}=sum_{R⊆ H⊆ S}E^R_{i,H} ⊗ g_i^{ ⊗ (S∖ H)}$$
The $E^R_{i,H}$ are represented by layered diagrams: every retained block
in slab $i$ contains a root of the interface above; a block is retained if
-it has $\ge2$ such roots or meets a dependent input label below; all other
+it has $ge2$ such roots or meets a dependent input label below; all other
blocks resum to the independent factor $g_i$ on their single root; every
record-bearing line continues to time zero. Forgetting a record commutes
with the projection identity.
@@ -1150,92 +1150,92 @@ keep the rest and call their new root set $H$. This gives
the dependent-subset expansion and the rule; record labels stay in $H_-$ at
every step, so their lines continue. Fresh labels on distinct blocks are
disjoint with multinomial coefficients, and
-$\frac1{(j_1+j_2)!}\binom{j_1+j_2}{j_1}=\frac1{j_1!j_2!}$ permits the
+$frac1{(j_1+j_2)!}binom{j_1+j_2}{j_1}=frac1{j_1!j_2!}$ permits the
separate sums; everything is finite. Record forgetting commutes with the
root-output kernel the root-output kernel (record-free weight) and with
the initial updates, so it commutes with the composition.
Regard each nontrivial initial cumulant block as a connection. A block on
-$k$ labels is dominated by $\prod f_0$, $(Ck)^{Ck}$, and a root tree with
+$k$ labels is dominated by $prod f_0$, $(Ck)^{Ck}$, and a root tree with
edge kernel the edge kernel; the sharper kernel
-$ 1 _{|x-x'|\le C_{D,k}ε}+ε^D$ holds for bounded $k$. These dominate
+$ 1 _{|x-x'|le C_{D,k}ε}+ε^D$ holds for bounded $k$. These dominate
the exact blocks; artificial links for marked lines are not connections.
Lemma (Labels and connected components). The retained expansion factors over global components. If $D^R_{i,B}$ is
the sum of diagrams connected on roots $B$, then
-$$\widehat F^R_{i,S}=\sum_{\pi\in\mathcal P(S)}⊗_{B\in\pi}D^{R\cap B}_{i,B}$$
+$$widehatwidehat F^R_F^R_{i,S}=sum_{piinmathcal P(S)}calP(S)⊗_{Binpi}D^{Rcap B}_{i,B}$$
Hence factorial-cumulant inversion keeps exactly the connected diagrams,
even after resumming into $g_i$. At fixed root order $h=|S|$ and bounded
-complexity $\rho\le K$, with $n_i$ lines and $j_i$ fresh labels in slab $i$,
+complexity $rhole K$, with $n_i$ lines and $j_i$ fresh labels in slab $i$,
$$n_i-j_i=O_{K,h,m,L}(1),
-\prod_i\frac1{j_i!}\le\frac{(1+\sum_in_i)^{C_{K,h,m,L}}}{\prod_in_i!}$$
+prod_ifrac1{j_i!}lefrac{(1+sum_in_i)^{C_{K,h,m,L}}}{prod_in_i!}$$
Apart from ordinary contact pair/order choices, all distinguished-label,
gluing, initial-block, and record-placement multiplicities are bounded by a
fixed polynomial in total size times $C^b$, with base $C$ independent of $K$
and the moment order; in the coarse regime the same choices cost a cutoff
-power with exponent $O(\rho)$.
+power with exponent $O(rho)$.
Proof.
Expand each $g_i$ to time zero (algebraically only). Weights are label-local;
size and excess caps are componentwise; every global component contains a
designated root (each slab block meets a root above). Distributing $j$ fresh
labels with sizes $j_1,...,j_q$ gives coefficient
-$\frac1{j!}(j!)/(j_1!... j_q!)=\prod_a\frac1{j_a!}$, so everything
+$frac1{j!}(j!)/(j_1!... j_q!)=prod_afrac1{j_a!}$, so everything
factors; group components to get the component expansion, and finite
partition inversion gives the cumulant statement. A one-root resummation
contracts a history attached through one line and cannot split or merge
components. For counting, the only non-fresh labels in a slab are
boundedly many roots/continued labels, giving the first part of
-the crossing-factorial bound and then, via $n!/(n-d)!\le n^d$, the second.
+the crossing-factorial bound and then, via $n!/(n-d)!le n^d$, the second.
There are $2^b$ C/O choices; once the ordered C/O graph is fixed its
C-components are the clusters and its O-forest the blocks, so no extra
partition enters; the exploration has one branch per selected forest.
Bounded distinguished choices cost fixed powers of total size, with
exponent controlled by crossings and initial links.
-Lemma (Stopped variation errors). For $L$ large in terms of the fixed data and $\Gamma$, any fixed record
-bound, and $|S|\le A_i/2$, there are $c_i>0$ with
+Lemma (Stopped variation errors). For $L$ large in terms of the fixed data and $Gamma$, any fixed record
+bound, and $|S|le A_i/2$, there are $c_i>0$ with
-$$\|F^R_{i,S}-\widehat F^R_{i,S}\|_{TV}\le e^{-c_iΛ_i}$$
+$$|F^R_{i,S}-widehatwidehat F^R_F^R_{i,S}|_{TV}le e^{-c_iΛ_i}$$
uniformly for a partial final slab (no velocity weight claimed).
Proof.
-Write $\Delta_i=F_i-\widehat F_i$. Then
-$\Delta_i=R_i+\mathcal L_i\Delta_{i-1}$, $|R_i|\le\mathcal E_iF_{i-1}$,
-$\Delta_0=0$. Substitute $F_{i-1}=\widehat F_{i-1}+\Delta_{i-1}$ in the
+Write $Delta_i=F_i-widehatwidehat F_i$.F_i$. Then
+$Delta_i=R_i+mathcal L_icalL_iDelta_{i-1}$, $|R_i|lemathcal E_iF_calE_iF_{i-1}$,
+$Delta_0=0$. Substitute $F_{i-1}=widehatwidehat F_F_{i-1}+Delta_{i-1}$ in the
positive stopped bound and expand the retained part as in
the resummation with records; refining autonomous histories into C graphs
and picking one incoming contact per incompatibility gives exactly the
positive C/O histories of the coarse package with previous-interface
continuations. The only top-slab difference, a stopped component with
-$M_i\le\cdot<2M_i-2<Λ_i$ clusters, is in the same coarse family with
-atom count $\ge M_i-1$. Bookkeeping: the lower independent inputs are
+$M_ilecdot<2M_i-2<Λ_i$ clusters, is in the same coarse family with
+atom count $ge M_i-1$. Bookkeeping: the lower independent inputs are
already resummed into $g$; the top stopped forest is not resummed. Top
components failing continuation are paid by the coarse boundary modifications, part (i)
($ε^{-C_*|S|}$), and bottom continuation of a record line with no
initial link uses the coarse boundary modifications, part (ii)--(iii) (add a unit-mass Gaussian
-Bol dummy and an initial link $\geε^υ$, cost $ε^{-υ}$,
+Bol dummy and an initial link $geε^υ$, cost $ε^{-υ}$,
bounded many). Remaining label and initial-block factors are the cutoff
powers of the label bookkeeping. Choosing $L$ so
-$C\tau^{c_0}<1$ and using $Λ_i=A_i^{30}$, $A_i\ge|\logε|$ makes the
+$Ctau^{c_0}<1$ and using $Λ_i=A_i^{30}$, $A_ige|logε|$ makes the
top loss absorb into the exponential size gain,
-$$\|\mathcal E_i\widehat F_{i-1}\|_{TV}\le
-ε^{-C_*|S|-C_m}\sum_{b\ge M_i-1}(C\tau^{c_0})^b
-\sum_{\rho\ge0}|\logε|^{C_*\rho}ε^{c_*\rho}\le e^{-cΛ_i}$$
+$$|mathcal E_icalE_iwidehatwidehat F_F_{i-1}|_{TV}le
+ε^{-C_*|S|-C_m}sum_{bge M_i-1}(Ctau^{c_0})^b
+sum_{rhoge0}|logε|^{C_*rho}ε^{c_*rho}le e^{-cΛ_i}$$
Input orders are at most $(|S|+1)Λ_i^2/2$, which is below
-$A_{i-1}/2$; the $\Delta_{i-1}$
+$A_{i-1}/2$; the $Delta_{i-1}$
terms are bounded by the stopped input bound, and
-$A_iΛ_i^2\log(1/ε)=o(Λ_{i-1})=Λ_i^{30}$ absorbs them.
+$A_iΛ_i^2log(1/ε)=o(Λ_{i-1})=Λ_i^{30}$ absorbs them.
This is the induction; restricting the last slab preserves every bound.
-Theorem (Marked component expansion). Choose $\Gamma$ then $L$ as above, independent of the moment order and the
+Theorem (Marked component expansion). Choose $Gamma$ then $L$ as above, independent of the moment order and the
observation list. On this single pasted dynamics:
(i) The factorial hierarchy with any fixed finite record list has the
@@ -1246,33 +1246,33 @@ projections are those of the resummation with records, the label bookkeeping.
(ii) At fixed final order $h$, the actual normalized marked cumulant
$c_h^ε$ is the sum of retained globally connected diagrams plus an
-error of total variation $\le C_he^{-cΛ_L}$. Nontrivial initial
+error of total variation $le C_he^{-cΛ_L}$. Nontrivial initial
blocks count as connections; dummy links do not.
(iii) For any accuracy power $P$, one can choose $K$ (after the record list
-and $h$) so that all retained diagrams with $\rho>K$ have summed absolute
-variation $\leε^P$; at $\rho\le K$ the crossing-factorial bound holds.
+and $h$) so that all retained diagrams with $rho>K$ have summed absolute
+variation $leε^P$; at $rhole K$ the crossing-factorial bound holds.
Increasing $K$ or $h$ never changes the exponential base per ordinary atom.
Proof.
(i) combines the preceding results. For (ii), invert both the actual and the
retained hierarchies: the component expansion gives the connected sum for
the retained one, and every term in the difference of the two finite
-partition polynomials carries a factor $\Delta_{L,B}$. The actual
-normalized factorial measures have mass $\le1$ (initially by the insertion
+partition polynomials carries a factor $Delta_{L,B}$. The actual
+normalized factorial measures have mass $le1$ (initially by the insertion
bound of the initial ensemble, and conserved since $N$ is preserved), and
-the retained ones have variation $\le1+e^{-cΛ_L}$ at fixed orders by
+the retained ones have variation $le1+e^{-cΛ_L}$ at fixed orders by
the stopped variation bound. For (iii) apply the coarse bound to each
resummed core with the same fixed record and top-root losses; independent
top singletons are bounded by the independent-factor construction; for small $ε$,
-$|\logε|^{C_*\rho}ε^{c_*\rho}\leε^{c_*\rho/2}$, so after summing
-the geometric atom factor the $\rho>K$ part is
-$\le C_{h,m}ε^{-C_*h-C_m}ε^{c_*K/2}$; raise $K$ to make it
-$\leε^P$. Dummy lines change complexity by a fixed amount and are
+$|logε|^{C_*rho}ε^{c_*rho}leε^{c_*rho/2}$, so after summing
+the geometric atom factor the $rho>K$ part is
+$le C_{h,m}ε^{-C_*h-C_m}ε^{c_*K/2}$; raise $K$ to make it
+$leε^P$. Dummy lines change complexity by a fixed amount and are
removed before low-complexity asymptotics. All root-order and observation
dependence sits in cutoff powers or fixed polynomial factors of
the crossing-factorial bound; the exponential atom base depends only on the
-fixed graph counting, the $Bol$ bounds, and $\Gamma$, so the chosen $L$
+fixed graph counting, the $Bol$ bounds, and $Gamma$, so the chosen $L$
works for every subsequently fixed order.
The comparison with the true flow (the cutoff comparison, below) needs a positive
@@ -1280,52 +1280,52 @@ version with a connected final collision witness instead of observed
outputs, and without any bound on the cutoff probability.
Corollary (Terminal-witness expansion). In slab $i$ let a terminal witness be a connected true C history on
-$n\le3Λ_i$ incoming labels, excess $\le2\Gamma$, stopped at a contact
+$nle3Λ_i$ incoming labels, excess $le2Gamma$, stopped at a contact
in that slab, with arbitrary further nonnegative realizability
restrictions. Its activity-normalized functional
-$$\sum_n(\mu^n)/(n!)\int F_{i-1,n}( d Z_n) 1 _{terminal witness}(Z_n)$$
+$$sum_n(mu^n)/(n!)int F_{i-1,n}( d Z_n) 1 _{terminal witness}(Z_n)$$
has the retained layer expansion with independent $g$ inputs and initial
blocks. All lower C/O components attach through particle lines to the
witness. The preceding variation error is smaller than every fixed power of
-$ε$. After the artificial-top-root normalization $\mu$, the coarse part
-with $\rho>K$ is also $<$ any assigned power for large $K$; the remaining
+$ε$. After the artificial-top-root normalization $mu$, the coarse part
+with $rho>K$ is also $<$ any assigned power for large $K$; the remaining
low-complexity witness integrals keep their realizability restrictions.
Proof.
-Since $n\le3Λ_i<A_{i-1}/2$, insert the preceding expansion from
+Since $nle3Λ_i<A_{i-1}/2$, insert the preceding expansion from
the marked component expansion into the terminal-witness functional.
Every lower component has a root leading above and the final roots enter
the connected witness (attachment before discarding any initial link). The
variation error contributes at most
-$\sum_{n\le3Λ_i}\mu^n/n! e^{-cΛ_{i-1}}\le
-e^{CΛ_i\log(1/ε)-cΛ_{i-1}}$, which is super-polynomially
+$sum_{nle3Λ_i}mu^n/n! e^{-cΛ_{i-1}}le
+e^{CΛ_ilog(1/ε)-cΛ_{i-1}}$, which is super-polynomially
small. Designating an artificial top root places the dependent diagrams in
-the terminal class at cost $\mu$; with no dependent continuation the
+the terminal class at cost $mu$; with no dependent continuation the
diagram lives in the terminal slab with independent inputs and complexity
-$\le1+2\Gamma$. The same geometric complexity summation, with this fixed
+$le1+2Gamma$. The same geometric complexity summation, with this fixed
power, proves the last assertion. For $i=1$ there is no preceding variation
error and the argument starts from the initial cumulant expansion. No
comparison of true and pasted evolutions is made.
This is the central new estimate. The Deng--Hani--Ma package already removed large
complexity (the marked component expansion, part (iii)); the remaining issue is what
-survives at the sharp fluctuation scale $\mu^{1-h}$ for the $h$-th
+survives at the sharp fluctuation scale $mu^{1-h}$ for the $h$-th
factorial cumulant. The mechanism is a change of relative
translations: every collision that merges two clusters of particles
adjusts one relative position by the collision geometry, producing a
-factor $ε^2[(v-v_*)\cdot\omega]_+ d t d \omega$. After accounting
-for the activity $\mu$ per birth line, a connected diagram with $p$
-physical initial links scales like $\mu^{1-h}ε^p$, which is exactly the
+factor $ε^2[(v-v_*)cdotomega]_+ d t d omega$. After accounting
+for the activity $mu$ per birth line, a connected diagram with $p$
+physical initial links scales like $mu^{1-h}ε^p$, which is exactly the
size sought; cycles and nontrivial initial correlations are smaller by a
positive power (proved via a null-set/dominated-convergence argument). The
sum over all cluster structures converges because each cluster slab has a
-life time $\tau=T/L$ and the base $CT/\sqrt L<1$ for large $L$.
+life time $tau=T/L$ and the base $CT/sqrt L<1$ for large $L$.
Fix finitely many observation times and bounded continuous observation
functions. When observations are accumulated in a mark, update
-$y\mapsto y+\phi_j(x,v)$, so $|y|\le M$ with $M$ independent of the
+$ymapsto y+phi_j(x,v)$, so $|y|le M$ with $M$ independent of the
number of particles. More generally one may retain finitely many phase
points along each designated trajectory. A record is kept only along a
line on which it is required; forgetting part of a record means pushing
@@ -1336,37 +1336,37 @@ the marked component expansion.
Let $c_h^ε$ be the ordered normalized factorial cumulant measure of the
pasted process, with records on its $h$ designated particles; thus $c_1^ε$
is the one-particle measure and the normalization at order $h$ is
-$\mu^{-h}$. Constants $C_K$ may depend on a fixed complexity bound $K$, on
+$mu^{-h}$. Constants $C_K$ may depend on a fixed complexity bound $K$, on
the fixed observations, and on $L$; the exponential base $C^n$ never does.
The independent factors of the independent-factor construction satisfy, for some $b>0$ and
$B_0<∞$,
-$$\sup_{0<ε\leε_0, i}\|g_i\|_{Bol,b}\le B_0,
-\|g_i-f_{i\tau}\|_{Bol,b}→0$$
+$$sup_{0<εleε_0, i}|g_i|_{Bol,b}le B_0,
+|g_i-f_{itau}|_{Bol,b}→0$$
The exponent $b$ is decreased a fixed number of times when reserving Gaussian weights;
this does not change the microscopic dynamics.
-Theorem (Sharp connected bounds). Choose $\Gamma,L$ as in the marked component expansion, increasing $L$ if
+Theorem (Sharp connected bounds). Choose $Gamma,L$ as in the marked component expansion, increasing $L$ if
necessary by an amount depending only on the Boltzmann bounds and on $T$.
This single choice works for every fixed factorial order $h$ and every
fixed bounded observation list. For each fixed $h$,
-$$\|c_h^ε\|_{TV}\le C_h\mu^{1-h}$$
+$$|c_h^ε|_{TV}le C_hmu^{1-h}$$
-For $h=1,2$, the measures $\mu^{h-1}c_h^ε$ converge against bounded
+For $h=1,2$, the measures $mu^{h-1}c_h^ε$ converge against bounded
continuous record tests to the signed sums of retained global trees with
trivial initial cumulants, with contact weight
-$[(v-v_*)\cdot\omega]_+ d t d \omega$ (scattering $+1$,
-non-scattering $-1$) and independent birth factors $f_{i\tau}$. The sums
+$[(v-v_*)cdotomega]_+ d t d omega$ (scattering $+1$,
+non-scattering $-1$) and independent birth factors $f_{itau}$. The sums
of absolute retained diagram measures, after multiplication by
-$\mu^{h-1}$, are bounded uniformly with a small Gaussian weight in their
+$mu^{h-1}$, are bounded uniformly with a small Gaussian weight in their
designated endpoint velocities; the same holds for the limiting tree
measures and for Gaussian weights in finitely many record velocities after
decreasing the exponent. Among retained connected diagrams, the sum of the
absolute measures having a nontrivial initial cumulant or a global cycle
-is $o(\mu^{1-h})$. These weighted assertions concern retained diagrams and
+is $o(mu^{1-h})$. These weighted assertions concern retained diagrams and
their limits, not the microscopic expansion remainder.
A global tree is a tree on the particle lines with contacts as
@@ -1374,12 +1374,12 @@ edges; continuing one line through an interface does not create a vertex,
while newly integrated particles do. This convention is essential for
counting translations and activity factors.
-Work with a term of complexity $\le K$. Replace each initial cumulant by
+Work with a term of complexity $le K$. Replace each initial cumulant by
its bound from the initial ensemble,
-$$C_K\sum_{\mathcal L forest}\prod_{(p,q)\in\mathcal L}
-( 1 _{|x_p(0)-x_q(0)|\le R_{K,D}ε}+ε^D)
-\prod_pf_0(z_p(0))$$
+$$C_Ksum_{mathcal LcalL forest}prod_{(p,q)inmathcal L}calL
+( 1 _{|x_p(0)-x_q(0)|le R_{K,D}ε}+ε^D)
+prod_pf_0(z_p(0))$$
only for absolute bounds (not to sign an initial link). Expand the
parentheses and suppose first that all chosen links are physical.
@@ -1391,24 +1391,24 @@ contact is a merger if its two lines lie in different components
just before it, else redundant. With $a_i$ mergers in slab $i$ and
$r$ redundant contacts,
-$$\sum_ia_i=m-c-p, r=\sum_ie_i+p-m+c$$
+$$sum_ia_i=m-c-p, r=sum_ie_i+p-m+c$$
the second being the global cycle excess. With $n_i$ lines present in slab
$i$ (including contact-free lines) and $q$ interface crossings,
-$$\sum_in_i=m+q, \sum_i(n_i-a_i)=q+c+p$$
+$$sum_in_i=m+q, sum_i(n_i-a_i)=q+c+p$$
-Merger edges in one slab form a forest on its $n_i$ lines, so $a_i\le n_i$.
+Merger edges in one slab form a forest on its $n_i$ lines, so $a_ile n_i$.
All of $q,p,c,r$ and $n_i-a_i$ are bounded by $K$: glue layer graphs along
interfaces to see $r$ (total excess grows by at most the number of
-gluings, all in $\rho$); each layer component meets a root so its count is
+gluings, all in $rho$); each layer component meets a root so its count is
bounded; erasing boundedly many initial links changes this boundedly.
Each birth line has one independent input velocity and position; a
continued line has neither. The cancellation of activity at interfaces
leaves, in the normalized factorial expansion,
-$$\mu^{m-h}$$
+$$mu^{m-h}$$
A birth at an interface of a $g_i$-supplied line is an independent phase
variable; the passage of a recorded line is a continuation of its old
@@ -1418,10 +1418,10 @@ Lemma (Chronological merger coordinates). Fix a finite line graph, the C/O choic
which contacts are redundant. Away from nontransversal and simultaneous
events, its history integral has coordinates: the birth velocities, one
absolute translation per global component, a vector in a ball of radius
-$R_{K,D}ε$ per physical initial merger, and $(t,\omega)\in R\times
+$R_{K,D}ε$ per physical initial merger, and $(t,omega)in Rtimes
S^2$ per dynamic merger. The positional Jacobian per dynamic merger is
-$$ε^2[(v-v_*)\cdot\omega]_+ d t d \omega$$
+$$ε^2[(v-v_*)cdotomega]_+ d t d omega$$
A specified redundant contact has no free continuous parameter. The
coordinate map has multiplicity at most one on each incoming transversal
@@ -1436,19 +1436,19 @@ the forest toward one representative per group has determinant one.
Proceed in increasing contact time. Within each group the histories are
known up to a common translation. A merger of groups with translations
$X,X_*$ on the indicated straight segments satisfies
-$X-X_*=-d(t)-ε\omega$ with $d(t)$ the known relative displacement,
-$\dot d=v-v_*$, and $\omega$ opposite the outward normal, so the incoming
-condition is $(v-v_*)\cdot\omega>0$. The determinant of
-$(t,\omega)\mapsto X-X_*$ on the sphere is
-$ε^2|(v-v_*)\cdot\omega|$, and the incoming convention selects the sign
+$X-X_*=-d(t)-εomega$ with $d(t)$ the known relative displacement,
+$dot d=v-v_*$, and $omega$ opposite the outward normal, so the incoming
+condition is $(v-v_*)cdotomega>0$. The determinant of
+$(t,omega)mapsto X-X_*$ on the sphere is
+$ε^2|(v-v_*)cdotomega|$, and the incoming convention selects the sign
in the coordinate formula. A scattering reflection or O-continuation
updates velocities; the two groups now share one translation.
If the next specified contact is redundant, its relative displacement and
velocities are already fixed. A straight relative flight $r(t)=d+tu$ has
at most one incoming crossing, and
-$\int_I\delta(|r|-ε)[-u\cdot r/ε]_+ d t= 1 _{\{incoming
-crossing in I\}}$, since the flux cancels the absolute derivative of
+$int_Idelta(|r|-ε)[-ucdot r/ε]_+ d t= 1 _{{incoming
+crossing in I}}$, since the flux cancels the absolute derivative of
$|r|-ε$; the outgoing deltas then make a deterministic substitution.
If the crossing is absent the branch has weight zero. Segments starting
inside the sphere have an exit, not an incoming crossing.
@@ -1467,23 +1467,23 @@ subsets of transversal branches and exhaust.
Multiplying the activity bookkeeping factor by the merger Jacobians and the
physical-link volumes,
-$$\mu^{m-h}ε^{2(m-c-p)}ε^{3p}=\mu^{c-h}ε^{p}$$
+$$mu^{m-h}ε^{2(m-c-p)}ε^{3p}=mu^{c-h}ε^{p}$$
All acceptance indicators can be carried through the change of variables;
for an upper bound they may be dropped, except that a redundant scattering
determines its branch velocities when it occurs (extend by zero where it
does not). For a connected diagram $c=1$, and a physical initial block has
-$p\ge1$ so gains a factor $ε$. A term of the sharp scaling
-using a tail factor: erase that link; erasing $\le K$ links raises $c$ by
-$\le K$ and costs $\leε^{-2K}$ in the activity counting; choosing
-$D>2K+M$ makes such terms $O(ε^M\mu^{1-h})$, with $M$ arbitrary and
+$pge1$ so gains a factor $ε$. A term of the sharp scaling
+using a tail factor: erase that link; erasing $le K$ links raises $c$ by
+$le K$ and costs $leε^{-2K}$ in the activity counting; choosing
+$D>2K+M$ makes such terms $O(ε^Mmu^{1-h})$, with $M$ arbitrary and
chosen after the moment order.
-Lemma (Fresh-label factorials). For complexity $\le K$, the absolute sum with slab sizes $(n_1,...,n_L)$
+Lemma (Fresh-label factorials). For complexity $le K$, the absolute sum with slab sizes $(n_1,...,n_L)$
is bounded by a sum over chronologically ordered merger pair lists with
-denominator $\prod_in_i!$, times
+denominator $prod_in_i!$, times
-$$C_K(1+n)^{d_K}C^{\sum_ia_i}, n=\sum_in_i$$
+$$C_K(1+n)^{d_K}C^{sum_ia_i}, n=sum_in_i$$
with base $C$ independent of $K$ (the merger pairs themselves are not
counted).
@@ -1491,89 +1491,89 @@ counted).
Proof.
In slab $i$, $s_i$ labels arrive as roots from above (the final roots in
the top slab) and $j_i=n_i-s_i$ are fresh, integrated with coefficient
-$1/j_i!$. Since $s_i\le K$,
-$\frac1{j_i!}=(n_i!)/((n_i-s_i)!)\frac1{n_i!}\le
-\frac{(1+n_i)^{s_i}}{n_i!}$. Continued labels, dependent subsets, and
+$1/j_i!$. Since $s_ile K$,
+$frac1{j_i!}=(n_i!)/((n_i-s_i)!)frac1{n_i!}le
+frac{(1+n_i)^{s_i}}{n_i!}$. Continued labels, dependent subsets, and
initial-link labels are boundedly many, costing a fixed power of $1+n$.
The rooted compatibility expansion represents connected coefficients by
spanning forests whose deterministic exploration has one branch per
selected forest; after selecting one incoming encounter per forest edge
the C-components are the collision clusters and the O-forest the blocks,
so no extra partition enters, and the fresh-label denominator survives.
-There are $r\le C_K$ redundant contacts costing $(1+n)^{2r}$ choices and
+There are $rle C_K$ redundant contacts costing $(1+n)^{2r}$ choices and
$(1+n+r)^r$ insertions; C/O flags give an absolute exponential base; a
chronological order already fixes the line order so has no extra
permutation factor.
Lemma (Uniform summability). For fixed $K$, the sum of absolute connected diagram measures with slab
-sizes $(n_i)$, after removing $\mu^{1-h}$, is bounded by
+sizes $(n_i)$, after removing $mu^{1-h}$, is bounded by
-$$C_K(1+n)^{d_K}(C\tau\sqrt L)^n$$
+$$C_K(1+n)^{d_K}(Ctausqrt L)^n$$
-The same bound (with the corresponding $\mu^{c-h}$) holds after erasing
+The same bound (with the corresponding $mu^{c-h}$) holds after erasing
boundedly many initial links, after prescribing the absolute position of
one observation per component, or after inserting a small Gaussian weight
in the designated velocities.
Proof.
Energy and time are bounded jointly to avoid a logarithmic loss per vertex.
-Let $E_0=\sum_{p=1}^m|v_p^{birth}|^2$. Elastic collisions conserve
+Let $E_0=sum_{p=1}^m|v_p^{birth}|^2$. Elastic collisions conserve
every colliding-pair energy, O-contacts do not change it, a line ending at
an interface discards its energy, and a birth adds energy already in
-$E_0$. Hence the sum of squared velocities active at any time is $\le E_0$.
+$E_0$. Hence the sum of squared velocities active at any time is $le E_0$.
-On the bin $E_0\in[P/2,P]$ (with $E_0<1$ by $P=1$), summing the incoming
+On the bin $E_0in[P/2,P]$ (with $E_0<1$ by $P=1$), summing the incoming
speed over all merger-pair choices in slab $i$ gives
-$$\sum_{p<q}|v_p-v_q|\le(n_i-1)\sum_p|v_p|\le n_i^{3/2}\sqrt P$$
+$$sum_{p<q}|v_p-v_q|le(n_i-1)sum_p|v_p|le n_i^{3/2}sqrt P$$
Applied to a discrete tree of successive pair choices at fixed merger
times, normals, and birth velocities, where earlier velocities and
intervening specified redundant contacts are already determined by
the merger coordinates, induction bounds the product of fluxes by
-$$\prod_i(n_i^{3/2}\sqrt P)^{a_i}$$
+$$prod_i(n_i^{3/2}sqrt P)^{a_i}$$
-Integrating normals adds $C^{\sum_ia_i}$; merger times are globally ordered
-within a slab, leaving $\prod_i\tau^{a_i}/a_i!$.
+Integrating normals adds $C^{sum_ia_i}$; merger times are globally ordered
+within a slab, leaving $prod_itau^{a_i}/a_i!$.
A common translation remains per component. For fixed birth velocities and
merger coordinates, write the input spatial arguments as $X+d_p$,
integrate one chosen input in $X$, and use the spatial supremum of the
-others; the Gaussian suppression gives $\le C^m\exp(-bE_0)$ uniformly
+others; the Gaussian suppression gives $le C^mexp(-bE_0)$ uniformly
in the displacements. To prescribe an observation position, solve
$X=x-d_{obs}$ with Jacobian one, same bound uniformly in $x$.
For the velocity volume, reserve half the Gaussian: with $b_1>0$,
-$ 1 _{E_0\in[P/2,P]}e^{-2b_1E_0}\le e^{-b_1P/2}e^{-b_1E_0}$, whose last
-factor integrates over $3m$ birth velocities to $(\pi/b_1)^{3m/2}$ (the
-lowest bin uses $P^{a/2}=1$ and costs only $C^m$). With $a=\sum_ia_i$,
+$ 1 _{E_0in[P/2,P]}e^{-2b_1E_0}le e^{-b_1P/2}e^{-b_1E_0}$, whose last
+factor integrates over $3m$ birth velocities to $(pi/b_1)^{3m/2}$ (the
+lowest bin uses $P^{a/2}=1$ and costs only $C^m$). With $a=sum_ia_i$,
-$$\sum_{P=1,2,4,...}e^{-b_1P/2}P^{a/2}\le C^{a+1}(1+a)^{a/2}$$
+$$sum_{P=1,2,4,...}e^{-b_1P/2}P^{a/2}le C^{a+1}(1+a)^{a/2}$$
-by comparison with $\int e^{-b_1u/4}(1+u)^{a/2}$ and Stirling.
+by comparison with $int e^{-b_1u/4}(1+u)^{a/2}$ and Stirling.
Combining with the fresh-label factorials, the remainder is a fixed polynomial
in $1+n$ times
-$$C^{n+a}\tau^a(1+a)^{a/2}\prod_i\frac{n_i^{3a_i/2}}{a_i!n_i!}$$
+$$C^{n+a}tau^a(1+a)^{a/2}prod_ifrac{n_i^{3a_i/2}}{a_i!n_i!}$$
-With $\delta_i=n_i-a_i\ge0$ and $\sum_i\delta_i\le C_K$, and
-$n_i!/a_i!\le(1+n_i)^{\delta_i}$, $n_i!\ge(n_i/e)^{n_i}$,
+With $delta_i=n_i-a_ige0$ and $sum_idelta_ile C_K$, and
+$n_i!/a_i!le(1+n_i)^{delta_i}$, $n_i!ge(n_i/e)^{n_i}$,
$$
-\frac{n_i^{3a_i/2}}{a_i!n_i!}\le e^{2n_i}(1+n_i)^{\delta_i}n_i^{-n_i/2}.
+frac{n_i^{3a_i/2}}{a_i!n_i!}le e^{2n_i}(1+n_i)^{delta_i}n_i^{-n_i/2}.
$$
-Also $\tau^a\le\tau^n\max(1,\tau^{-1})^{C_K}$ and
-$(1+a)^{a/2}\le C(1+n)^{C_K}n^{n/2}$, and convexity of $u\log u$ gives
+Also $tau^aletau^nmax(1,tau^{-1})^{C_K}$ and
+$(1+a)^{a/2}le C(1+n)^{C_K}n^{n/2}$, and convexity of $ulog u$ gives
-$$\prod_in_i^{n_i}\ge(n/L)^n$$
+$$prod_in_i^{n_i}ge(n/L)^n$$
Substitution proves the Stirling bound. For weights: the sum of
-squared designated velocities is $\le E_0$ at a fixed time and
-$\le q_0E_0$ at $q_0$ record times, so a weight exponent below
-$b_1/(2\max(1,q_0))$ is absorbed by the reserved Gaussian fraction; the
+squared designated velocities is $le E_0$ at a fixed time and
+$le q_0E_0$ at $q_0$ record times, so a weight exponent below
+$b_1/(2max(1,q_0))$ is absorbed by the reserved Gaussian fraction; the
exponent shrinks with the record list but the exponential base does not.
-Since $\tau=T/L$, the base in the Stirling bound is $CT/\sqrt L$;
+Since $tau=T/L$, the base in the Stirling bound is $CT/sqrt L$;
increase $L$ once so it is $<1$. There are polynomially many vectors
$(n_i)$ of total size $n$ (fixed $L$), so the Stirling bound gives
uniform summability and vanishing size tails, with polynomial degrees that
@@ -1610,14 +1610,14 @@ zero polynomial has a null zero set (grazing/ineffective reflections
extend analytically). For two lines on a common time interval, write the
relative displacement $d+tu$; a coincidence requires the collinearity
-$$d\times u=0$$
+$$dtimes u=0$$
If the lines lie in different forest components, vary their free relative
translation. Otherwise, with ineffective reflections, a non-neighbor path
-$p_0,...,p_k$, $k\ge2$, with edge times $s_1,...,s_k$ gives an endpoint
+$p_0,...,p_k$, $kge2$, with edge times $s_1,...,s_k$ gives an endpoint
displacement built from $(v_{p_{j-1}}-v_{p_j})s_j$; the intermediate
-velocity $v_{p_j}$ ($1\le j<k$) occurs with coefficient
-$s_{j+1}-s_j\ne0$, so varying it off the endpoint velocity direction
+velocity $v_{p_j}$ ($1le j<k$) occurs with coefficient
+$s_{j+1}-s_jne0$, so varying it off the endpoint velocity direction
disproves the null-set conclusion.
Neighbors meeting at time $a$: after $a$ with no later velocity change the
@@ -1625,8 +1625,8 @@ relative flight is the single separating flight, which has no second
incoming crossing (an O-contact passes out once). If an endpoint scatters
at $b>a$, the third particle is distinct; choose its velocity and the
normal so the pair's relative velocity jumps from $u_1$ to $u_2$
-nonparallel (e.g. endpoint velocity $e_1\to e_2$, third particle $-e_1$,
-normal $(e_1-e_2)/\sqrt2$), then the displacement contains
+nonparallel (e.g. endpoint velocity $e_1to e_2$, third particle $-e_1$,
+normal $(e_1-e_2)/sqrt2$), then the displacement contains
$(b-a)u_1+(t-b)u_2$ with nonzero cross product against $u_2$. Before the
meeting, an intervening scattering $b<a$ with the same jump forces a
displacement $(t-b)e_1-(a-b)e_2$ not parallel to $e_1$.
@@ -1663,22 +1663,22 @@ once $ε$ is small; by the no-extra-contact lemma almost every merger parameter
set has only prescribed incoming contacts for all small $ε$. Thus every
acceptance restriction holds, counting an encounter or its existence is the
same, and the connected compatibility coefficient equals its tree sign
-$(-1)^{\#\mathrm O}$. Replacing $g_i$ by $f_{i\tau}$ in a fixed-size term is
+$(-1)^{#mathrm O}rmO$. Replacing $g_i$ by $f_{itau}$ in a fixed-size term is
justified by a telescoping product and the Gaussian suppression, with
the uniform summability bound (one factor replaced by its $Bol$-difference)
giving convergence to zero. Dominated convergence in space (checked first
on bounded velocities/size, then removing truncations with
the Stirling bound) defines the limiting signed tree measures.
-Lemma (Spatial traces of tree measures). Let $\mathcal T$ be one of the summable tree measures above, with a line
+Lemma (Spatial traces of tree measures). Let $mathcal T$calT$ be one of the summable tree measures above, with a line
and a time at which its position is required. It has a disintegration
-$$\mathcal T= d x \mathcal T_x$$
+$$mathcal T=calT= d x mathcal T_x$$calT_x$$
-with Gaussian-weighted variation of $\mathcal T_x$ bounded uniformly in $x$
+with Gaussian-weighted variation of $mathcal T_x$calT_x$ bounded uniformly in $x$
and finite integral over $x$. For every bounded continuous test of the
other coordinates (and continuous tests of smaller Gaussian growth),
-$x\mapsto\mathcal T_x(\Phi)$ is continuous. If two tree components are
+$xmapstomathcal T_x(calT_x(Phi)$ is continuous. If two tree components are
joined at their designated positions, the product of their conditional
measures at a common position, integrated against incoming flux, is an
absolutely defined measure; it equals imposing the joining position in
@@ -1697,7 +1697,7 @@ is continuous in $x$ with a uniform integrable majorant, and the tails
converge uniformly in $x$ by the fixed-position estimate; a stronger
reserved Gaussian handles Gaussian growth. For two components with
positions $x,x_*$, setting $x_*=x$ gives the conditional product, whose
-variation is finite by $B(v-v_*,\omega)\le|v|+|v_*|$ (one component
+variation is finite by $B(v-v_*,omega)le|v|+|v_*|$ (one component
conditional, the other integrated); the same bound dominates a compactly
supported approximate identity in $x-x_*$ uniformly, and on bounded
velocity sets conditional weak continuity gives convergence against
@@ -1705,7 +1705,7 @@ product tests, extended by the variation bounds.
Lemma (Completeness of the tree class). For fixed roots, required records, and $L$, all global trees with trivial
initial cumulants in the regrouped retained expansion have complexity
-$\le K_0$, independent of their number of ordinary vertices. Undoing and
+$le K_0$, independent of their number of ordinary vertices. Undoing and
reapplying an unmarked one-root regrouping preserves their weights and
record projections.
@@ -1715,7 +1715,7 @@ initial cumulants. In its highest occupied slab a one-root component is a
single connected block; if all lower inputs are independent it is a term of
$g_i$ and regroups away. If a lower dependent component attaches through
two lines, the upper and lower connections form a global cycle; so for a
-global tree each lower dependent component attaches through $\le1$ line,
+global tree each lower dependent component attaches through $le1$ line,
and at least one must exist for the upper component to stay dependent.
Following it down repeats the argument; at time zero a dependent
nonsingleton needs a nontrivial initial cumulant. Downward induction proves
@@ -1723,12 +1723,12 @@ the claim; required records are the only cause to expand an independent
singleton further.
Cut a global forest at an interface and contract upper components to
-vertices. With $u$ such, a lower component with $k\ge2$ attachments meets
+vertices. With $u$ such, a lower component with $kge2$ attachments meets
distinct upper components (else a cycle), so the bipartite incidence graph
-is a forest; with $v$ lower vertices of degree $\ge2$ and $d$ incidences,
-$d\le u+v-1$ and $2v\le d$, giving
+is a forest; with $v$ lower vertices of degree $ge2$ and $d$ incidences,
+$dle u+v-1$ and $2vle d$, giving
-$$d\le2u$$
+$$dle2u$$
A lower component attached at one line is either absorbed (first
paragraph) or continues a required record, contributing at most the fixed
@@ -1767,10 +1767,10 @@ plus their edge form a tree whose highest block meets the original root;
inverse regroupings restore the retained representation. Coefficients:
choosing an extra incident particle among $j$ fresh labels changes $1/j!$
to $1/(j-1)!$, and
-$\binom{j_1+j_2}{j_1}\frac1{(j_1+j_2)!}=\frac1{j_1!j_2!}$ splits the
+$binom{j_1+j_2}{j_1}frac1{(j_1+j_2)!}=frac1{j_1!j_2!}$ splits the
remaining labels; a contact between two designated particles uses one
unordered pair, no fresh label; the deleted contact contributes its C/O
-sign, other signs multiply. Letting $N\to∞$ passes through deletion
+sign, other signs multiply. Letting $Nto∞$ passes through deletion
and joining by the uniform summability bound, the spatial-trace construction, the uniform
conditional Gaussian bound controlling the joining flux with a fixed
exponent loss; records project because record forgetting commutes.
@@ -1780,8 +1780,8 @@ Weighted high-complexity tail. Take the birth exponent $b>0$ of
the Gaussian suppression independent of $L$, and $L$ large enough for
the coarse package at the smaller exponent $3b/4$. For a fixed record list
let $J$ count designated endpoint and record velocity slots; on every
-retained history the sum of their squared velocities is $\le JE_0$. Choose
-$\alpha>0$ with $\alpha J\le b/4$; the weight is dominated by
+retained history the sum of their squared velocities is $le JE_0$. Choose
+$alpha>0$ with $alpha Jle b/4$; the weight is dominated by
$e^{bE_0/4}$, absorbed by tilting every birth input to
$|g_i(x,v)|e^{b|v|^2/4}$ (and $f_0$ likewise), which has a common
$Bol,3b/4$ bound. The positive coarse bound the analytic package(a)
@@ -1794,11 +1794,11 @@ independent of $J,h,K$.
Assembling the scale. Use the marked component expansion at accuracy
$ε^M$, $M>2(h-1)$, with $K$ large enough for that accuracy and for
the tree-class completeness. The expansion error and the high-complexity
-tail are negligible after multiplication by $\mu^{h-1}$ (they need only the
+tail are negligible after multiplication by $mu^{h-1}$ (they need only the
unweighted variation bound, since observation tests are bounded).
For the remaining connected diagrams, the activity bookkeeping and
-the uniform summability bound prove the uniform bound at scale $\mu^{1-h}$.
+the uniform summability bound prove the uniform bound at scale $mu^{1-h}$.
Physical initial links gain $ε$; nonphysical initial tails gain any
power after choosing $D$; cycles are negligible by the no-extra-contact lemma plus
finite-size dominated convergence and the uniform tails; the survivors are
@@ -1808,11 +1808,11 @@ summable majorant yields the asserted Gaussian variation bounds for their
retained sums and limits, including the one-root and two-root limits of the
following stage. All exponential bases are independent of $K$ and $h$; those
quantities enter only through front constants and polynomial degrees, so
-the $\Gamma,L$ choice remains the single choice made before the moment
+the $Gamma,L$ choice remains the single choice made before the moment
order.
The central limit theorem is now run on the single pasted dynamics fixed by
-the marked component expansion, the sharp connected bounds. Its $\Gamma,L$ do not
+the marked component expansion, the sharp connected bounds. Its $Gamma,L$ do not
depend on the observation list or the moment order. The method: attach a
mark that accumulates test values along each particle, so that any
fixed multitime linear combination becomes one scalar. Its ordinary
@@ -1823,29 +1823,29 @@ deferred to the next stage; exact centering is restored at the end.
Give every particle a scalar mark, initially $0$, and at time $t_j$ update
-$$(x,v,y)⟼Θ_j(x,v,y)=(x,v,y+\phi_j(x,v))$$
+$$(x,v,y)⟼Θ_j(x,v,y)=(x,v,y+phi_j(x,v))$$
Collisions preserve the mark of each particle. Write
-$M_{obs}=\sum_j\|\phi_j\|_∞$, $\xi=(x,v,y)$, $|y|\le
+$M_{obs}=sum_j|phi_j|_∞$, $xi=(x,v,y)$, $|y|le
M_{obs}$. The mark only records deterministic trajectories; it adds
no randomness. On either dynamics,
-$$\sum_{i=1}^Ny_i(T)=\sum_j\sum_{i=1}^N\phi_j(z_i(t_j))$$
+$$sum_{i=1}^Ny_i(T)=sum_jsum_{i=1}^Nphi_j(z_i(t_j))$$
Use a superscript $ε$ for the normalized factorial cumulants of the
pasted marked process. At any observation-free time the sharp connected bounds
provides limits
-$$c_1^ε→ F_t, \mu c_2^ε→ J_t$$
+$$c_1^ε→ F_t, mu c_2^ε→ J_t$$
against bounded continuous tests of the records; $F_t$ is a one-root
measure and $J_t$ a symmetric signed two-root measure, both with the
Gaussian variation bounds of the sharp connected bounds. Before the updates
at time zero, the initial ensemble gives
-$$F_0=f_0(x,v) d x d v \delta_0( d y), J_0=0$$
+$$F_0=f_0(x,v) d x d v delta_0( d y), J_0=0$$
-(since $\mu\|c_{2,0}^ε\|_1=O(ε)$). Forgetting records in the finite
+(since $mu|c_{2,0}^ε|_1=O(ε)$). Forgetting records in the finite
marked hierarchy commutes with the one-root regroupings; by
the marked component expansion, the independent-factor construction, the tree-class completeness, the
$(x,v)$ marginal of $F_t$ is $f_t(x,v) d x d v$ (also inside a slab, via
@@ -1860,38 +1860,38 @@ sense (a.e. $x$ by globality, then both sides weakly continuous). To form
collision products, use the conditional measure of a factor at its
designated position, multiply the two component measures at a common
position, integrate that position, and include
-$B(v-v_*,\omega) d \omega$ when the incident variables collide. These are
+$B(v-v_*,omega) d omega$ when the incident variables collide. These are
absolutely defined; a conditional Gaussian bound for one component and the
-integrated one for the other, with $B\le|v|+|v_*|$, give an integrable
+integrated one for the other, with $Ble|v|+|v_*|$, give an integrable
majorant, equivalently replacing equality by a smooth approximate identity
and passing to width zero.
-At a collision, with $\xi=(x,v,y)$, $\xi_*=(x,v_*,y_*)$,
-$\xi'=(x,v',y)$, $\xi_*'=(x,v_*',y_*)$, put
+At a collision, with $xi=(x,v,y)$, $xi_*=(x,v_*,y_*)$,
+$xi'=(x,v',y)$, $xi_*'=(x,v_*',y_*)$, put
$$
-\Delta\Phi=\Phi(\xi')+\Phi(\xi_*')-\Phi(\xi)-\Phi(\xi_*),
-D\Phi=v\cdot\nabla_x\Phi,
+DeltaPhi=Phi(xi')+Phi(xi_*')-Phi(xi)-Phi(xi_*),
+DPhi=vcdotnabla_xPhi,
$$
and
-$$(H_t\Phi)(\xi)=\int_{R^3\times[-M_{obs},M_{obs}]\times\mathbb S^2}
-B(v-v_*,\omega)\Delta\Phi F_t(x, d v_* d y_*) d \omega$$
+$$(H_tPhi)(xi)=int_{R^3times[-M_{obs},M_{obs}]timesmathbb S^2}bbS^2
+B(v-v_*,omega)DeltaPhi F_t(x, d v_* d y_*) d omega$$
-In the formulas below, $\int BFF_*(...)$ is the simultaneous position
-integral, with $ d x d \omega$.
+In the formulas below, $int BFF_*(...)$ is the simultaneous position
+integral, with $ d x d omega$.
Proposition (Evolution of the marked tree laws). Between updates,
-$$∂_tF_t(\Phi) =F_t(D\Phi)+\tfrac12\int BF_tF_{t,*}\Delta\Phi$$
+$$∂_tF_t(Phi) =F_t(DPhi)+tfrac12int BF_tF_{t,*}DeltaPhi$$
-$$∂_tJ_t(\Phi ⊗ \Psi) =J_t((D+H_t)\Phi ⊗ \Psi+\Phi ⊗ (D+H_t)\Psi)$$
+$$∂_tJ_t(Phi ⊗ Psi) =J_t((D+H_t)Phi ⊗ Psi+Phi ⊗ (D+H_t)Psi)$$
-$$ +\int BF_tF_{t,*}(\Phi(\xi')\Psi(\xi_*')-\Phi(\xi)\Psi(\xi_*))$$
+$$ +int BF_tF_{t,*}(Phi(xi')Psi(xi_*')-Phi(xi)Psi(xi_*))$$
These hold in transport mild form, hence in weak differential form for
smooth tests for which the integrals exist. At an update,
-$$F_{t_j+}=(Θ_j)_\#F_{t_j-}, J_{t_j+}=(Θ_j ⊗ Θ_j)_\#J_{t_j-}$$
+$$F_{t_j+}=(Θ_j)_#F_{t_j-}, J_{t_j+}=(Θ_j ⊗ Θ_j)_#J_{t_j-}$$
Proof.
Derive the identities from the tree integrals after the limit. Start with
@@ -1908,18 +1908,18 @@ joining and its fresh-label coefficients.
Three counts enter. (a) One root: the partner chosen among $j$ fresh labels changes $1/j!$
to $1/(j-1)!$ and splitting remaining labels uses
-$\frac1{(j_1+j_2)!}\binom{j_1+j_2}{j_1}=\frac1{j_1!j_2!}$, giving
-$\int BFF_*(\Phi(\xi')-\Phi(\xi))$, symmetrized by particle interchange
-(including $\omega\mapsto-\omega$) into the collision term of
+$frac1{(j_1+j_2)!}binom{j_1+j_2}{j_1}=frac1{j_1!j_2!}$, giving
+$int BFF_*(Phi(xi')-Phi(xi))$, symmetrized by particle interchange
+(including $omegamapsto-omega$) into the collision term of
the pushforward identity.
(b) Two roots: a contact between them is one
unordered pair and no fresh label; deleting it gives two one-root means and
the last integral of the pushforward identity with no factor $1/2$.
(c) A contact between the first root and a new partner: the second original root
lies with the first (contribution $J$ on it, $F$ on the partner, change
-$\Phi(\xi')-\Phi(\xi)$) or with the partner (interchange; the $J$ component
-carries $\Phi(\xi_*')-\Phi(\xi_*)$), summing to $J(H_t\Phi ⊗ \Psi)$,
-and the same at the second root gives $J(\Phi ⊗ H_t\Psi)$. Records
+$Phi(xi')-Phi(xi)$) or with the partner (interchange; the $J$ component
+carries $Phi(xi_*')-Phi(xi_*)$), summing to $J(H_tPhi ⊗ Psi)$,
+and the same at the second root gives $J(Phi ⊗ H_tPsi)$. Records
project when a partner has no record in the integrand. Free flight gives
$D$; a transport-mild version avoids differentiating a sum (freely
transport the test to the last-contact time $s$; no-contact term plus
@@ -1931,104 +1931,104 @@ concatenation is the empty-top-slab no-contact term, preserved by the
absolutely convergent tree sums. Updates are deterministic pushforwards,
giving the pushforward identity.
-The pre/post substitution with $\omega\mapsto-\omega$ preserves
-$B(v-v_*,\omega) d v d v_* d \omega$, as does particle interchange with
+The pre/post substitution with $omegamapsto-omega$ preserves
+$B(v-v_*,omega) d v d v_* d omega$, as does particle interchange with
the normal reversed. Hence the normalization in the Boltzmann equation gives
-$$\int Q(f,f)\phi=\tfrac12\int Bff_*\Delta\phi,
-\int[Q(g,f)+Q(f,g)]\phi=\int g K_t\phi$$
+$$int Q(f,f)phi=tfrac12int Bff_*Deltaphi,
+int[Q(g,f)+Q(f,g)]phi=int g K_tphi$$
with background $f=f_t$. So the collision part of the linearized weak drift
has no extra $1/2$.
Restore the same-particle term by defining
-$$G_t(\Phi,\Psi)=J_t(\Phi ⊗ \Psi)+F_t(\Phi\Psi)$$
+$$G_t(Phi,Psi)=J_t(Phi ⊗ Psi)+F_t(PhiPsi)$$
Then the tree-law evolution gives
-$$∂_tG_t(\Phi,\Psi)=G_t((D+H_t)\Phi,\Psi)+G_t(\Phi,(D+H_t)\Psi)
-+\tfrac12\int BF_tF_{t,*}\Delta\Phi \Delta\Psi$$
+$$∂_tG_t(Phi,Psi)=G_t((D+H_t)Phi,Psi)+G_t(Phi,(D+H_t)Psi)
++tfrac12int BF_tF_{t,*}DeltaPhi DeltaPsi$$
-Direct check of the source: with $P=\Phi+\Phi_*$, $R=\Psi+\Psi_*$, the
+Direct check of the source: with $P=Phi+Phi_*$, $R=Psi+Psi_*$, the
collision change of the diagonal products from the $F$ equation plus the
-$J$ source, symmetrized, is $\tfrac12\int BFF_*\Delta(PR)$; the diagonal
-drifts contribute $\tfrac12\int BFF_*(R\Delta P+P\Delta R)$; the difference
+$J$ source, symmetrized, is $tfrac12int BFF_*Delta(PR)$; the diagonal
+drifts contribute $tfrac12int BFF_*(RDelta P+PDelta R)$; the difference
is the last term of the G evolution since
-$\Delta(PR)=R\Delta P+P\Delta R+\Delta P \Delta R$. This uses neither
+$Delta(PR)=RDelta P+PDelta R+Delta P Delta R$. This uses neither
detailed balance nor equilibrium. The source is positive semidefinite
-($F_t\ge0$). Initially, before updates,
+($F_tge0$). Initially, before updates,
-$$G_0(\Phi,\Psi)=\int f_0(z)\Phi(z,0)\Psi(z,0) d z$$
+$$G_0(Phi,Psi)=int f_0(z)Phi(z,0)Psi(z,0) d z$$
and at an update $G$ pushes forward in both slots.
the G evolution is needed on the spaces
$$
-\mathcal V_a=\{\Phi=c y+h:c\in R, h\in E_a^0\},
-\|\Phi\|_{\mathcal V_a}=|c|+\|h\|_a .
+mathcal V_a=calV_a={Phi=c y+h:cin R, hin E_a^0},
+|Phi|_{mathcal V_a}calV_a=|c|+|h|_a .
$$
-Let $\alpha>0$ be a common exponent in the integrated and conditional
-Gaussian variation bounds for $F,J$, and choose $0<a<b<\beta$ with
-$2b<\alpha$ (a positive margin for the flux; the factor $2$ also controls
+Let $alpha>0$ be a common exponent in the integrated and conditional
+Gaussian variation bounds for $F,J$, and choose $0<a<b<beta$ with
+$2b<alpha$ (a positive margin for the flux; the factor $2$ also controls
the diagonal $F_t(hk)$). The mark is constant on a particle between updates
and conserved at a collision, so the marginal statement after
the collision-position integral gives
$$(D+H_t)(c y+h)=A_th,
-\tfrac12\int BF_tF_{t,*}\Delta(c y+h)\Delta(d y+k)=C_t(h,k)$$
+tfrac12int BF_tF_{t,*}Delta(c y+h)Delta(d y+k)=C_t(h,k)$$
-At pulse $t_j$, backward substitution sends $c y+h$ to $c y+h+c\phi_j$.
+At pulse $t_j$, backward substitution sends $c y+h$ to $c y+h+cphi_j$.
Use the backward propagator in this possibly nonsmooth class: the Gaussian
variation bounds make $G_t$ a uniformly bounded bilinear form on
-$\mathcal V_b$, and the transport mild identity extends from smooth tests
+$mathcal V_b$,calV_b$, and the transport mild identity extends from smooth tests
by local uniform approximation with a small Gaussian margin; the unmarked
collision operator is $K_t$, so the linearized operator estimate applies. Iterating
the bilinear mild identity chooses one of two slots per collision factor;
an $n$-fold remainder is bounded by
-$((CT)^n)/(n!)(1+√(n/\delta))^n$ for fixed allowance
-$\delta=b-a>0$ (the $2^n$ slot choices absorbed in $C^n$), which vanishes.
+$((CT)^n)/(n!)(1+√(n/delta))^n$ for fixed allowance
+$delta=b-a>0$ (the $2^n$ slot choices absorbed in $C^n$), which vanishes.
Source iterations obey the same bound, justifying dual propagation by the
convergent mild series with no spatial/velocity differentiability of
-$U(r,t)\phi$.
+$U(r,t)phi$.
Starting from the test $y$ after the last observation, the backward test at
$r$ away from pulses is $y+h_r$ with
-$$h_r=\sum_{j: t_j\ge r}U(r,t_j)\phi_j$$
+$$h_r=sum_{j: t_jge r}U(r,t_j)phi_j$$
(The convention at $r=0$ includes observations at time zero; values at
positive pulse times do not affect a time integral.) Combining dual
propagation, the backward pulse test, and the pulse substitutions,
-$$G_T(y,y)=\int f_0h_0^2+\int_0^TC_r(h_r,h_r) d r$$
+$$G_T(y,y)=int f_0h_0^2+int_0^TC_r(h_r,h_r) d r$$
After the last pulse the unmarked backward part is zero, so the last
observation time may replace $T$. By the explicit construction
-the isonormal construction, $\sum_j\zeta_{t_j}(\phi_j)=I_0(h_0)+I(\Delta h_r)$,
+the isonormal construction, $sum_jzeta_{t_j}(phi_j)=I_0(h_0)+I(Delta h_r)$,
whose variance is exactly the variance formula, which by expanding
-$h_r=\sum_{j:t_j\ge r}U(r,t_j)\phi_j$ equals the target covariance. This
+$h_r=sum_{j:t_jge r}U(r,t_j)phi_j$ equals the target covariance. This
identifies all multi-time and repeated-observation correlations.
Proposition (Gaussian limit on the pasted dynamics). For the single pasted dynamics fixed above and every fixed observation list,
$$
-(\sum_iy_i(T)-E\sum_iy_i(T))/(\sqrt\mu) ⇒\
-\sum_j\zeta_{t_j}(\phi_j),
+(sum_iy_i(T)-Esum_iy_i(T))/(sqrtmu) ⇒
+sum_jzeta_{t_j}(phi_j),
$$
and all centered moments converge to the Gaussian ones.
Proof.
-Put $S^ε=\sum_iy_i(T)$. Since $|S^ε|\le M_{obs}N$ and
-$\mathcal Z_ε\le e^\mu$, $S^ε$ has exponential moments for each fixed
+Put $S^ε=sum_iy_i(T)$. Since $|S^ε|le M_{obs}N$ and
+$mathcal Z_εcalZ_εle e^mu$, $S^ε$ has exponential moments for each fixed
$ε$. The exact factorial-to-ordinary identity at the final marked time is
-$$\kappa_k(S^ε)=\sum_{\pi\in\mathcal P([k])}\mu^{|\pi|}
-\int c_{|\pi|}^ε( d \xi_1... d \xi_{|\pi|})\prod_{B\in\pi}y_B^{|B|}$$
+$$kappa_k(S^ε)=sum_{piinmathcal P([k])}calP([k])mu^{|pi|}
+int c_{|pi|}^ε( d xi_1... d xi_{|pi|})prod_{Binpi}y_B^{|B|}$$
Directly: write
-$\exp(\lambda S^ε)=\prod_i[1+(\exp(\lambda y_i)-1)]$, insert the factorial
-series, and take the logarithm; each $\exp(\lambda y)-1$ must receive a
+$exp(lambda S^ε)=prod_i[1+(exp(lambda y_i)-1)]$, insert the factorial
+series, and take the logarithm; each $exp(lambda y)-1$ must receive a
nonempty set of the $k$ derivatives, and distributing those sets gives
exactly the partitions of the factorial-to-ordinary identity, whose ordering
cancels the factorial denominator. This is a finite formal identity through
@@ -2036,53 +2036,53 @@ degree $k$.
All $y$-powers are bounded on the mark interval (extend to bounded
continuous functions on the mark line). By the sharp connected bounds every
-term on the right is $O_k(\mu)$. For
-$X^ε=(S^ε-E S^ε)/\sqrt\mu$, the first cumulant vanishes and
+term on the right is $O_k(mu)$. For
+$X^ε=(S^ε-E S^ε)/sqrtmu$, the first cumulant vanishes and
$$
-\kappa_2(X^ε)=c_1^ε(y^2)+\mu c_2^ε(y ⊗ y)→
+kappa_2(X^ε)=c_1^ε(y^2)+mu c_2^ε(y ⊗ y)→
F_T(y^2)+J_T(y ⊗ y)=G_T(y,y),
$$
-while for $k>2$, $\kappa_k(X^ε)=O_k(\mu^{1-k/2})\to0$. That these hold on
-one dynamics is essential: the bases fixing $\Gamma,L$ in
+while for $k>2$, $kappa_k(X^ε)=O_k(mu^{1-k/2})to0$. That these hold on
+one dynamics is essential: the bases fixing $Gamma,L$ in
the marked component expansion, the sharp connected bounds are independent of the fixed
order; enlarging the auxiliary complexity cutoff or $D$ only changes the
error representation, not the random variable $X^ε$.
The finite moment-cumulant identities give every centered Gaussian moment
-with variance $\sigma^2=G_T(y,y)$. For scalar convergence, truncate the
+with variance $sigma^2=G_T(y,y)$. For scalar convergence, truncate the
characteristic functions of $X^ε$ and of a centered Gaussian $Z$ at
degree $2n-1$; Taylor's integral remainder is bounded by
$|ux|^{2n}/(2n)!$, so
$$
-limsup_{ε\to0}|E e^{iuX^ε}-E e^{iuZ}|
-\le\frac{2|u|^{2n}E Z^{2n}}{(2n)!}
-=\frac{2|u|^{2n}\sigma^{2n}}{2^nn!},
+limsup_{εto0}|E e^{iuX^ε}-E e^{iuZ}|
+lefrac{2|u|^{2n}E Z^{2n}}{(2n)!}
+=frac{2|u|^{2n}sigma^{2n}}{2^nn!},
$$
-and $n\to∞$ proves convergence for every real $u$, including
-$\sigma=0$. This gives weak convergence with variance
+and $nto∞$ proves convergence for every real $u$, including
+$sigma=0$. This gives weak convergence with variance
the variance formula.
The pasted dynamics recolors every restarted slab, resets the collision
prehistory at each interface, and truncates components above the caps
-$Λ_i,\Gamma$. The true hard-sphere flow does none of this. It must be
+$Λ_i,Gamma$. The true hard-sphere flow does none of this. It must be
shown that the two trajectories coincide up to time $T$ with probability
-$1-O(ε^{1+\eta})$, $\eta>0$, better than $O(ε)$. The reason:
-the fluctuation scale is $\sqrt\mu=ε^{-1}$, and the mean of the pasted
+$1-O(ε^{1+eta})$, $eta>0$, better than $O(ε)$. The reason:
+the fluctuation scale is $sqrtmu=ε^{-1}$, and the mean of the pasted
process differs from the exact microscopic mean by a deterministic
$O(ε)$ amount; an error of probability $O(ε)$ alone would compete
with that shift after multiplication by $ε^{-1}$, and exact centering
would fail. The sharper bound is proved.
-Proposition (Accuracy of the pasted dynamics). There is a large dimensional integer $\Gamma_0$ with the following
-property. Fix $\Gamma\ge\Gamma_0$. There is
-$L_0=L_0(\Gamma,f_0,f,T,\beta)$ such that for every fixed $L\ge L_0$, the
+Proposition (Accuracy of the pasted dynamics). There is a large dimensional integer $Gamma_0$ with the following
+property. Fix $GammageGamma_0$. There is
+$L_0=L_0(Gamma,f_0,f,T,beta)$ such that for every fixed $Lge L_0$, the
true and pasted dynamics of the marked component expansion, coupled from the
same initial configuration, satisfy
-$$P\{the two trajectories differ at some time in [0,T]\}\le
-Cε^{1+\eta}$$
+$$P{the two trajectories differ at some time in [0,T]}le
+Cε^{1+eta}$$
-for all small $ε$, with $\eta=1/20$. The size cutoffs are the
+for all small $ε$, with $eta=1/20$. The size cutoffs are the
$A_i,Λ_i$ of the analytic package; $C$ and the upper bound on $ε$
may depend on the displayed fixed data.
@@ -2099,24 +2099,24 @@ $ε$ by the Deng--Hani--Ma package---this fixes $K$ large.
3. On the low-complexity fine regime, localize energy, then combine a
local gain at every good cutting piece with a global energy
and causal time-order bound, gaining enough powers of $ε$ to beat
-$1+\eta$.
+$1+eta$.
Distinguish the geometric cycle excess $r(M)$ of a graph from its
-multislab complexity $\rho(M)$. For a graph with $b$ binary-contact
+multislab complexity $rho(M)$. For a graph with $b$ binary-contact
vertices, $n$ particle lines, and $c$ connected components, when each line
has at least one vertex,
$$r(M)=b-n+c$$
equivalently, with contacts as vertices and segments as bonds,
-$r=\#\{bonds\}-b+c$. The graph's directed order is the order
+$r=#{bonds}-b+c$. The graph's directed order is the order
increasing in time along each particle line; orders on disjoint lines need
not be comparable.
Lemma (First disagreement). For every initial configuration the indicator that the true and pasted
trajectories first disagree in slab $i$ is at most the number of its
terminal witnesses: connected true C histories $M$ on incoming labels, with
-no designated root, excess $r(M)\le2\Gamma$, an internal realizability
+no designated root, excess $r(M)le2Gamma$, an internal realizability
restriction, meeting a label born at or after the previous interface,
ending at a terminal contact, and with an occupied replica at the terminal
contact.
@@ -2126,32 +2126,32 @@ Compare the two evolutions in chronological order; they agree up to the
first disagreement, which therefore is a contact accepted by the true rule
but rejected by the pasted one (or vice versa). On agreement so far the
pasted state is the true state; the collision component in the true history
-just before that contact has excess $\le2\Gamma$ (it was accepted), and the
-rejection is exactly ``component size $>Λ_i$ or excess added $>\Gamma$''
+just before that contact has excess $le2Gamma$ (it was accepted), and the
+rejection is exactly ``component size $>Λ_i$ or excess added $>Gamma$''
within this block. Summing over possible blocks, each such rejection is
charged to a distinct terminal witness; summing charges gives the bound.
Insert the terminal-witness functional
and apply the terminal-witness expansion. Begin with the previous pasted
-factorial measure at interface $i-1$. Since $n\le3Λ_i<A_{i-1}/2$, the
+factorial measure at interface $i-1$. Since $nle3Λ_i<A_{i-1}/2$, the
variation error is below every power. The connected terminal witness is
itself a block at the top of the pasted hierarchy and enters through its
positive layer expansion. Its lower dependent and rooted components attach
through particle lines to the terminal component. Keep $M$'s realizability
-restriction throughout. A rooted lower component with $k\ge2$ attachments
+restriction throughout. A rooted lower component with $kge2$ attachments
cannot touch the same upper component twice (that would create a cycle);
-with $u$ upper and $v$ lower vertices of degree $\ge2$ and $d$ incidence
-edges, the bipartite incidence forest has $d\le u+v-1$ per nonempty part
-and $2v\le d$, so $d\le2u$. A lower component attached at a single line is
+with $u$ upper and $v$ lower vertices of degree $ge2$ and $d$ incidence
+edges, the bipartite incidence forest has $dle u+v-1$ per nonempty part
+and $2vle d$, so $dle2u$. A lower component attached at a single line is
either absorbed into an independent $g$ input, or continues a required
record; the latter are boundedly many (the records through this interface,
including continued empty lines).
Choose a complexity threshold $K$ after $L$ is fixed. By
the terminal-witness expansion, the analytic package, the sum of positive majorants
-with $\rho>K$, including the activity cost of an artificial top root when
+with $rho>K$, including the activity cost of an artificial top root when
required, is $O(ε^3)$ for $K$ large enough. The terms left to estimate
-have $\rho\le K$. Their interface crossings, initial-link vertices,
+have $rhole K$. Their interface crossings, initial-link vertices,
within-slab cycles, and total geometric excess are bounded. Discard the
initial-link restrictions in these positive majorants; the trajectory
attachments to the terminal component persist.
@@ -2159,30 +2159,30 @@ attachments to the terminal component persist.
Henceforth all graphs are connected low-complexity witnesses,
summarized by a polylogarithmic exponent bound $B_ε$ on the total number
of atoms in the top-slab terminal component, with
-$B_ε\le C_*|\logε|$ ($C_*$ may depend on $K,L$). A connected witness
+$B_εle C_*|logε|$ ($C_*$ may depend on $K,L$). A connected witness
of low complexity has its top-slab component of bounded excess, and a
-connected graph with $b$ atoms and excess $\le2\Gamma$ can be produced
+connected graph with $b$ atoms and excess $le2Gamma$ can be produced
without new crossings and within the same realization family by
-$\le C^b$ choices of the initial labelled $M$ and its geometric data.
+$le C^b$ choices of the initial labelled $M$ and its geometric data.
The number of scattered velocities in any witness is at most $B_ε$, and
-initial data carry only $\le2\beta$ Gaussian under the kinetic assumption; a
+initial data carry only $le2beta$ Gaussian under the kinetic assumption; a
terminal witness has controllable total birth energy with Gaussian
cost $e^{-cP}$ for total energy $P$.
-Lemma (Energy tail). Fix $\Gamma$ and then choose $L$ once, larger when needed. For witnesses
-with $n$ true input lines carry total birth energy $E_0=\frac12\sum_j|v_j|^2$,
+Lemma (Energy tail). Fix $Gamma$ and then choose $L$ once, larger when needed. For witnesses
+with $n$ true input lines carry total birth energy $E_0=frac12sum_j|v_j|^2$,
put
-$$P_ε=(C_*B_ε)^{1/2}(1+B_ε|\logε|^{1/2}),
-\gamma_ε=ε^{B_ε^2}$$
+$$P_ε=(C_*B_ε)^{1/2}(1+B_ε|logε|^{1/2}),
+gamma_ε=ε^{B_ε^2}$$
-For a witness with $n\le B_ε$ terminal lines, once energy is
+For a witness with $nle B_ε$ terminal lines, once energy is
$>P_ε$ the
-$$integral\le C^{B_ε}e^{-cB_ε P_ε}\leε^{cB_ε^2}$$
+$$integralle C^{B_ε}e^{-cB_ε P_ε}leε^{cB_ε^2}$$
-smaller than every fixed power. On the low-energy regime $E_0\le P_ε$
+smaller than every fixed power. On the low-energy regime $E_0le P_ε$
the terminal terminals are localized to a ball of radius $R=C_*(1+B_ε P_ε^{1/2})$.
Proof.
@@ -2195,47 +2195,47 @@ an indicator; births at later interfaces are inserted at their times.
Dropping encounter restrictions and initial links, a graph with $n$ births
has mass at most
$$
-\mu^n\int\prod_{j=1}^nh_j(x_j,v_j) 1 _{\{\sum_j|v_j|^2>P_ε\}}
-\prod_j d x_j d v_j\le\mu^nC^ne^{-cP_ε},
+mu^nintprod_{j=1}^nh_j(x_j,v_j) 1 _{{sum_j|v_j|^2>P_ε}}
+prod_j d x_j d v_jlemu^nC^ne^{-cP_ε},
$$
using half of the uniform birth Gaussian for the tail and the number of
-births $\le B_ε$; summing a finite count and $\mu^n=ε^{-2n}$ gives
-$e^{2B_ε|\logε|-cP_ε}$ times a prefactor; choosing $P_ε$ a
-fixed large multiple of $B_ε|\logε|$ makes this below any fixed
-power. With no exponential growth $M_{top}\to1$.
+births $le B_ε$; summing a finite count and $mu^n=ε^{-2n}$ gives
+$e^{2B_ε|logε|-cP_ε}$ times a prefactor; choosing $P_ε$ a
+fixed large multiple of $B_ε|logε|$ makes this below any fixed
+power. With no exponential growth $M_{top}to1$.
Lemma (Causal order and relative speeds). In a slab with $q_i$ ordinary atoms, retain the partial order induced by the
full graph (including chains through exceptional atoms), and let
-$\mathcal T_i$ be its time-order region. On the original support with total
-birth energy $\le P$, an empty slab contributing one,
+$mathcal T_i$calT_i$ be its time-order region. On the original support with total
+birth energy $le P$, an empty slab contributing one,
-$$|\mathcal T_i|\sup\prod_{a ordinary in i}|v_a-v_{*a}|
-\le\frac{\tau^{q_i}(2q_iP)^{q_i/2}}{q_i!}$$
+$$|mathcal T_i|calT_i|supprod_{a ordinary in i}|v_a-v_{*a}|
+lefrac{tau^{q_i}(2q_iP)^{q_i/2}}{q_i!}$$
Proof.
-With $e_i$ the number of linear extensions, $|\mathcal T_i|=e_i\tau^{q_i}/q_i!$.
+With $e_i$ the number of linear extensions, $|mathcal T_i|=e_icalT_i|=e_itau^{q_i}/q_i!$.
An antichain of ordinary vertices occupies disjoint incoming pairs on a
common causal slice: place all strict ancestors first in a total extension;
no two vertices share a line; energy conservation bounds the sum of their
pair energies by $P$, including interfaces via inactive coordinates. For
-$a_v=|v_v-v_{*v}|$, every antichain has $\sum_{A}a_v\le√(2q_iP)$.
+$a_v=|v_v-v_{*v}|$, every antichain has $sum_{A}a_vle√(2q_iP)$.
Summing the products of weights over the recursive enumeration of linear
extensions (available minimal vertices form an antichain) gives
-$e_i\prod_va_v\le(2q_iP)^{q_i/2}$ for every feasible assignment, hence the
+$e_iprod_va_vle(2q_iP)^{q_i/2}$ for every feasible assignment, hence the
supremum.
Lemma (Free-parameter extraction). Consider a finite ordered composition of positive cut kernels. At an
-ordinary step the free variables are $θ_j=(t_j,\omega_j,w_j)$ with
-measure $a_j d t_j d \omega_j d w_j$, followed by a deterministic update.
-Suppose every exceptional kernel $K_\ell(h, d z)$ has mass at most
-$H_\ell$, uniformly in earlier-cut data (every restriction needed for that
+ordinary step the free variables are $θ_j=(t_j,omega_j,w_j)$ with
+measure $a_j d t_j d omega_j d w_j$, followed by a deterministic update.
+Suppose every exceptional kernel $K_ell(h, d z)$ has mass at most
+$H_ell$, uniformly in earlier-cut data (every restriction needed for that
bound included, zero outside the admissibility domain). Remove the $a_j$
-from the ordinary measures to get a positive measure $\nu$. If $E$ is a set
-of complete histories and $\mathcal D$ a measurable set containing its
+from the ordinary measures to get a positive measure $nu$. If $E$ is a set
+of complete histories and $mathcal D$calD$ a measurable set containing its
projection onto $θ$, then
-$$\nu(E)\le(\prod_\ell H_\ell)
-\int_{\mathcal D}\prod_{j=1}^q d t_j d \omega_j d w_j$$
+$$nu(E)le(prod_ell H_ell)
+int_{mathcal D}calDprod_{j=1}^q d t_j d omega_j d w_j$$
The same holds if the density after division by $a_j$ is merely bounded by
one.
@@ -2244,11 +2244,11 @@ Proof.
First put all ordinary variables in bounded boxes and fix their vector
$θ$. The exceptional kernels stay in place with $θ$
exterior; integrating them backwards from the last exceptional step bounds
-the surviving mass by $\prod_\ell H_\ell$, and intervening deterministic
+the surviving mass by $prod_ell H_ell$, and intervening deterministic
substitutions have norm at most one on bounded functions. Nonnegative
-Fubini represents $\nu$ as the product in $θ$ times these
+Fubini represents $nu$ as the product in $θ$ times these
kernels, and majorizing the indicator of $E$ by
-$ 1 _{\mathcal D}(θ)$ proves the extraction inequality.
+$ 1 _{mathcal D}calD(θ)$ proves the extraction inequality.
Exhaustion removes the boxes. Equivalently, restrict ordinary relative
speeds away from zero and bound a rectangle by its product volume; cover a
compact containing set by products of rectangles and take the infimum;
@@ -2262,116 +2262,116 @@ A cut exposes a set of contact variables. Its shared lines become
fixed phase-space data for the unexposed graph. The available degree of an
atom is its number of nonfixed edges; a history is regular if at every
O-atom each fixed end is serial with a free end. A one-atom piece of type
-$\{2\}$ has two nonfixed ends with the two fixed ends on the same time side
-(C) or nonserial (O); types $\{3\}$ and $\{4\}$ have respectively one and
-zero fixed ends. A $\{33\}$ piece has two degree-three atoms joined by one
-bond; it is type A if one atom cuts as a type $\{3\}$ singleton and the
-other becomes an allowed $\{2\}$ piece, type B otherwise. A $\{44\}$ piece
+${2}$ has two nonfixed ends with the two fixed ends on the same time side
+(C) or nonserial (O); types ${3}$ and ${4}$ have respectively one and
+zero fixed ends. A ${33}$ piece has two degree-three atoms joined by one
+bond; it is type A if one atom cuts as a type ${3}$ singleton and the
+other becomes an allowed ${2}$ piece, type B otherwise. A ${44}$ piece
has two degree-four atoms joined by one bond
(Deng--Hani--Ma, Definitions 8.2, 8.11). The kernels compose
-$I_M=I_A\circ I_{M∖ A}$ with repeated boundary variables identified
+$I_M=I_Acirc I_{M∖ A}$ with repeated boundary variables identified
(Deng--Hani--Ma, Proposition 8.14); this is how a later kernel is estimated
with earlier variables fixed. The uniform bound on the number of collisions in
semi-dispersing billiards behind these counting estimates is due to Burago,
Ferleger and Kononenko; Deng--Hani--Ma adapt it to the extended dynamics.
-Lemma (Local kernels). Let $R$ bound velocities and localized radii; the time length is $\le T$.
+Lemma (Local kernels). Let $R$ bound velocities and localized radii; the time length is $le T$.
For a singleton with two fixed ends in a free kernel:
-(i) If all incident free edges have relative speeds $\geε^υ$, the
-mass is $\le C R^Cε^{2+υ/3}$.
+(i) If all incident free edges have relative speeds $geε^υ$, the
+mass is $le C R^Cε^{2+υ/3}$.
(ii) If it is a scattering contact and the strong restrictions
($|s-s_*|$, $|x-x_*|$ and exterior $x_*$ below $ε^{1-υ}$ on both
-edges) hold, the mass is $\leε^{2+υ/3}$. The bound is uniform in
+edges) hold, the mass is $leε^{2+υ/3}$. The bound is uniform in
the exterior parameters $t_*,x_*$.
-(iii) For a type-B $\{33\}$ piece, both atoms C, with $|t_1-t_2|\geε^υ$
-and every incident pair having $|v_e-v_{e'}|\geε^υ$, the mass is
-$\leε^υ|\logε|^{C_*}$ uniformly in the two fixed ends.
+(iii) For a type-B ${33}$ piece, both atoms C, with $|t_1-t_2|geε^υ$
+and every incident pair having $|v_e-v_{e'}|geε^υ$, the mass is
+$leε^υ|logε|^{C_*}$ uniformly in the two fixed ends.
Multiplying any such kernel by a bounded factor on its support costs its
supremum; no independent Gaussian distribution of a fixed-end velocity is
assumed. This is (Deng--Hani--Ma, Lemmas 8.15, 8.20, 8.23). A
uniformly good singleton or type-B pair is one of these restricted
-kernels with conditional mass $ε^υ|\logε|^{C_*}$; all
+kernels with conditional mass $ε^υ|logε|^{C_*}$; all
gain-producing restrictions are part of the kernel.
Proposition (Pure-collision cutting alternatives). Let $M$ be a connected full realizable graph with only scattering contacts.
-A transversal set $A\subset M$ satisfies
-$M∖ A=A^-\sqcup A^+$ with no directed bond from $A^+$ to
-$A\cup A^-$, nor from $A$ to $A^-$. Let $X_0(A)$ be vertices outside $A$
+A transversal set $Asubset M$ satisfies
+$M∖ A=A^-sqcup A^+$ with no directed bond from $A^+$ to
+$Acup A^-$, nor from $A$ to $A^-$. Let $X_0(A)$ be vertices outside $A$
with two bonds to $A$, and $X(A)$ its closure obtained by repeatedly adding
vertices with two bonds to the grown set. Then:
(i) There is a chain of connected transversal sets $A_1,...,A_m=M$, $A_1$ a
-tree, $X_0(A_j)\ne∅$ for $j<m$,
-$A_j\cup X(A_j)\subset A_{j+1}$,
-$r(A_{j+1})=r(A_j\cup X(A_j))$, $r(A_{j+1})-r(A_j)\le10|X(A_j)|$. The
+tree, $X_0(A_j)ne∅$ for $j<m$,
+$A_jcup X(A_j)subset A_{j+1}$,
+$r(A_{j+1})=r(A_jcup X(A_j))$, $r(A_{j+1})-r(A_j)le10|X(A_j)|$. The
intermediate growth adds one bond per new vertex. For $D$ transitions there
-is a cutting sequence of $M$ with one type $\{4\}$, no type $\{44\}$ or
-type-B pair, and $\ge D$ type-A pairs.
+is a cutting sequence of $M$ with one type ${4}$, no type ${44}$ or
+type-B pair, and $ge D$ type-A pairs.
-(ii) One can choose $A^\pm$ so each component of $A^+$ is attached to $A$; then
-$X^\pm(A)=X(A)\cap A^\pm$ are convex along particle lines, and with $m_\pm$
-the bonds from $A$ to $X^\pm(A)$,
-$|X^\pm(A)|\le G(m_\pm)$, $G(q)=(2q+1)\binom q2(32q^{3/2})^{q^2}$.
+(ii) One can choose $A^pm$ so each component of $A^+$ is attached to $A$; then
+$X^pm(A)=X(A)cap A^pm$ are convex along particle lines, and with $m_pm$
+the bonds from $A$ to $X^pm(A)$,
+$|X^pm(A)|le G(m_pm)$, $G(q)=(2q+1)binom q2(32q^{3/2})^{q^2}$.
-(iii) Put $z=|X_0^\pm(A)|$, $a=r(A)$; there is a cutting sequence with one type
-$\{4\}$, no type $\{44\}$ or type-B pair, and $\ge z/2-a-1$ type-A pairs.
+(iii) Put $z=|X_0^pm(A)|$, $a=r(A)$; there is a cutting sequence with one type
+${4}$, no type ${44}$ or type-B pair, and $ge z/2-a-1$ type-A pairs.
(iv) For this side there is a finite Borel partition of the contact-parameter
-domain, with a subcase integer $y\ge0$ and two available sequences:
-a sequence with one type $\{4\}$, no type $\{44\}$ or type-B pair, and
-$\ge y/10-3(a+1)$ uniformly good singletons; or a sequence with no type
-$\{44\}$, $\le S=a+z+y$ type $\{4\}$ singletons, all type-B pairs uniformly
-good, and $\ge(m_\pm-10^5S)/10$ type-A or type-B pairs.
+domain, with a subcase integer $yge0$ and two available sequences:
+a sequence with one type ${4}$, no type ${44}$ or type-B pair, and
+$ge y/10-3(a+1)$ uniformly good singletons; or a sequence with no type
+${44}$, $le S=a+z+y$ type ${4}$ singletons, all type-B pairs uniformly
+good, and $ge(m_pm-10^5S)/10$ type-A or type-B pairs.
Neutral pieces keep their neutral kernels; partitions and operation
-sequences have $\le C^b|\logε|^{C_*}$ subcases with $C$ independent of
+sequences have $le C^b|logε|^{C_*}$ subcases with $C$ independent of
$L$. These are (Deng--Hani--Ma, Definition 15.3; Propositions 15.1, 15.2, 15.4, 15.6, 15.10).
-Lemma (Adjacent scattering contacts). Let $R\ge2$ bound velocities and localized radii, and length $\le T$. A pair
+Lemma (Adjacent scattering contacts). Let $Rge2$ bound velocities and localized radii, and length $le T$. A pair
of adjacent contacts with one bond is primitive if there is no other
directed chain between them; a double bond between two consecutive
scattering contacts is impossible. For $e_1,e_2$ the prospective fixed
edges of a type-A pair with contact times $t_1,t_2$ and
$$
-strongly close: |t_2-t_1|\leε^{9/10},
-|v_{e_2}-v_{e_1}|\leε^{4/5},
+strongly close: |t_2-t_1|leε^{9/10},
+|v_{e_2}-v_{e_1}|leε^{4/5},
$$
(i) a primitive strongly close pair cut freely as one piece has mass at most
-$$CR^C\muε^{9/10+3\cdot4/5}=CR^Cε^{13/10};$$
+$$CR^Cmuε^{9/10+3cdot4/5}=CR^Cε^{13/10};$$
(ii) without any strongly close primitive pair, each type-A pair used by a
-sequence has conditional mass $\le CR^Cε^{1/20}$, or splits into a
+sequence has conditional mass $le CR^Cε^{1/20}$, or splits into a
neutral type-two piece and a singleton with the same bound.
The bounds are uniform in previously exposed lines and times. This is
(Deng--Hani--Ma, Lemma 15.12).
-Fix $\delta=\tfrac12\min\{υ,1/20\}>0$; every retained local gain is
-at least $ε^\delta$ up to a fixed polylogarithmic factor.
+Fix $delta=tfrac12min{υ,1/20}>0$; every retained local gain is
+at least $ε^delta$ up to a fixed polylogarithmic factor.
-Lemma (Amplified pure-collision cut). For large dimensional $\Gamma_0$, every connected realizable full scattering
-graph with $\Gamma<r(M)\le2\Gamma$, $\Gamma\ge\Gamma_0$, decomposes into cut
+Lemma (Amplified pure-collision cut). For large dimensional $Gamma_0$, every connected realizable full scattering
+graph with $Gamma<r(M)le2Gamma$, $GammageGamma_0$, decomposes into cut
sequences such that either it contains a freely cut pair estimated by
the gain balance with no other activity loss, or its retained
improved pieces $g$ and free singletons $s_4$ satisfy
-$$\delta g-2s_4\ge6/5$$
+$$delta g-2s_4ge6/5$$
-There are $\le C^b|\logε|^{C_*}$ subcases; the number of non-ordinary
-pieces is bounded in terms of $\Gamma$ and fixed choices. This is
+There are $le C^b|logε|^{C_*}$ subcases; the number of non-ordinary
+pieces is bounded in terms of $Gamma$ and fixed choices. This is
(Deng--Hani--Ma, Proposition 15.11).
The local powers must survive simultaneous integration without a
per-vertex logarithmic loss. Call a neutral type-three singleton
ordinary; all other pieces exceptional. Counting both vertices
of an exceptional pair, their number is bounded by a constant depending on
-$K,\Gamma$; the terminal part is the amplified cut, below it
+$K,Gamma$; the terminal part is the amplified cut, below it
the local kernels; the degree count
$s_2+p_{33}=r(M)+s_4+p_{44}-1$ on the complete graph (or its version with
boundedly many crossing ends fixed) bounds the extra type-two pieces. With
@@ -2380,11 +2380,11 @@ $b$ the total atoms and $q$ the ordinary ones, $q=b-O_K(1)$.
Lemma (Total birth energy bounds the velocity domain). Fix a cutoff $E_{cut}=P_ε$ and, as in
the energy tail, use the local kernels at the scopes where
the cutting alternatives and the amplified cut retain them. Then
-for a witness with ordinary projection within the containing set $\mathcal D$
-(energy $\le P_ε$), there is a compact measurable set inside
-$\mathcal D$, of volume
+for a witness with ordinary projection within the containing set $mathcal D$calD$
+(energy $le P_ε$), there is a compact measurable set inside
+$mathcal D$,calD$, of volume
-$$\le\prod_i(C(L)/(q_i))^{q_i}(1+P_ε/q_i)^{3q_i/2}$$
+$$leprod_i(C(L)/(q_i))^{q_i}(1+P_ε/q_i)^{3q_i/2}$$
that contains every admissible ordinary velocity vector.
@@ -2395,26 +2395,26 @@ nonscattering contact applies the identity. At an exceptional atom erase the
dependence of the two outgoing coordinates and insert prescribed values;
inaugurated coordinates can be inactive from the start. The part linear in
the birth vector $u$ propagates by orthogonal matrices and projections, norm
-$\le1$ at each time. Each ordinary $w_j$ is a physical edge velocity
+$le1$ at each time. Each ordinary $w_j$ is a physical edge velocity
immediately before or after its contact (including the outgoing side when
cut backwards), so
-$$W=A(\omega)u+d(\omega,a), \|A(\omega)\|_{HS}^2\le3q$$
+$$W=A(omega)u+d(omega,a), |A(omega)|_{HS}^2le3q$$
Rows need not be orthogonal; only the sum of squared norms is used, and the
maps do not depend on contact times. Take a Euclidean net of $a$ of mesh
-$c_s(1+q)^{-1/2}$, cardinality $\le C_s\{(1+P_ε)(1+q)\}^{C_s}$; a change
-$\zeta$ in $a$ changes one chronological velocity by $\le\sqrt s\zeta$ and
-the observations by $\le C√(qs)\zeta$. Choose $c_s$ so simultaneous
-error is $\le1$. The allowed $W$ lie in $∪_{a_0}
-(d(\omega,a_0)+A(\omega)B_{3n}(√(P_ε))+B_{3q}(1))$, and the Minkowski
-sum is in $\sqrt2(P_ε AA^{\mathsf T}+Id_m)^{1/2}B_m(1)$ for $m=3q$
-(support function: $√(P_ε)|A^{\mathsf T}\xi|+|\xi|\le
-\sqrt{2(P_ε|A^{\mathsf T}\xi|^2+|\xi|^2)}$). Combining the trace bound
-with AM-GM on eigenvalues and $vol(B_m(1))\le(C/\sqrt m)^m$,
+$c_s(1+q)^{-1/2}$, cardinality $le C_s{(1+P_ε)(1+q)}^{C_s}$; a change
+$zeta$ in $a$ changes one chronological velocity by $lesqrt szeta$ and
+the observations by $le C√(qs)zeta$. Choose $c_s$ so simultaneous
+error is $le1$. The allowed $W$ lie in $∪_{a_0}
+(d(omega,a_0)+A(omega)B_{3n}(√(P_ε))+B_{3q}(1))$, and the Minkowski
+sum is in $sqrt2(P_ε AA^{mathsf T}sfT+Id_m)^{1/2}B_m(1)$ for $m=3q$
+(support function: $√(P_ε)|A^{mathsf T}sfTxi|+|xi|le
+sqrt{2(P_ε|A^{mathsf T}sfTxi|^2+|xi|^2)}$). Combining the trace bound
+with AM-GM on eigenvalues and $vol(B_m(1))le(C/sqrt m)^m$,
$$
-2^{m/2}vol(B_m(1))\det(Id_m+P_ε AA^{\mathsf T})^{1/2}
-\le(C√((1+P_ε)/q))^{3q}.
+2^{m/2}vol(B_m(1))det(Id_m+P_ε AA^{mathsf T}sfT)^{1/2}
+le(C√((1+P_ε)/q))^{3q}.
$$
The identity enlargement handles small singular values without an inverse
Jacobian; a finite union of continuous images of compact parameter sets
@@ -2422,10 +2422,10 @@ gives the compact containing set for the extraction lemma.
Lemma (Summation with finitely many exceptional pieces). Suppose a cut sequence has $q=b-O_K(1)$ ordinary atoms and boundedly many
exceptional pieces whose conditional mass bounds have product
-$ε^\alpha|\logε|^{C_*}$. After summing spatial cells and energy bins in
+$ε^alpha|logε|^{C_*}$. After summing spatial cells and energy bins in
a polylogarithmic energy region, its integral is at most
-$$ε^\alpha|\logε|^{C_*}(C\tau\sqrt L)^q$$
+$$ε^alpha|logε|^{C_*}(Ctausqrt L)^q$$
The base $C$ depends on the fixed kinetic envelopes and dimension, not on
$K,L$. This is (Deng--Hani--Ma, Lemma 16.2).
@@ -2434,29 +2434,29 @@ Proof of the pasted accuracy bound.
Start from the first-disagreement bound, the terminal-witness expansion, and fix the
complexity cutoff $K$ large enough that the coarse part is $<ε^3$
(the marked component expansion, part (iii) after the terminal-witness expansion):
-$\rho>K$ is discarded. The remaining witnesses are connected, full, realizable
-graphs with $\rho\le K$, hence bounded crossing/initial/cycle counts, and
-$r(M)\le2\Gamma$. Localize by the energy tail: outside the
+$rho>K$ is discarded. The remaining witnesses are connected, full, realizable
+graphs with $rhole K$, hence bounded crossing/initial/cycle counts, and
+$r(M)le2Gamma$. Localize by the energy tail: outside the
polylogarithmic energy region the sum is smaller than any power.
On the low-energy region, apply the cutting alternatives, the amplified cut
to the top-slab graph. The freely cut primitive pair (if any) gives
-the gain balance, product $ε^{13/10}|\logε|^{C_*}$. Otherwise
+the gain balance, product $ε^{13/10}|logε|^{C_*}$. Otherwise
the summation bound holds: the retained improved pieces number $g$
-with a fixed bound except for the bounded seed, and gain $ε^{\delta g}$,
-while each free type-four seed costs $\mu=ε^{-2}$; so the exceptional
-product is at most $ε^{6/5}|\logε|^{C_*}$ (using
-$\delta g-2s_4\ge6/5$ in both the $ε^{13/10}$ and the $ε^{6/5}$
+with a fixed bound except for the bounded seed, and gain $ε^{delta g}$,
+while each free type-four seed costs $mu=ε^{-2}$; so the exceptional
+product is at most $ε^{6/5}|logε|^{C_*}$ (using
+$delta g-2s_4ge6/5$ in both the $ε^{13/10}$ and the $ε^{6/5}$
branches). All the extra variables inside the containing set are then
removed by the coarea and time-order bounds: the causal-order bound
-gives $\prod_i\tau^{q_i}(2q_iP_ε)^{q_i/2}/q_i!$, and the ordinary
+gives $prod_itau^{q_i}(2q_iP_ε)^{q_i/2}/q_i!$, and the ordinary
velocity box by the birth-energy bound. Combining
the exceptional-piece summation, the extraction lemma, the low-complexity sum is
bounded by
$$
-ε^{6/5}|\logε|^{C_*}(C\tau\sqrt L)^{b-O_K(1)} .
+ε^{6/5}|logε|^{C_*}(Ctausqrt L)^{b-O_K(1)} .
$$
-Choose $L$ so large that $C\tau\sqrt L=C T/\sqrt L<1/2$, absorbing
+Choose $L$ so large that $Ctausqrt L=C T/sqrt L<1/2$, absorbing
constants depending on $K,L$ into the fixed prefactor. The exponential atom
counting ($C_1^b$ with $C_1$ independent of $K,L$, per
the marked component expansion, part (iii) and the terminal-witness expansion) together
@@ -2465,18 +2465,18 @@ costs only a fixed-degree polynomial; the resulting sum over $b$ is a
convergent geometric series, with the $Λ_i$ cutoff removing the large-$b$
part. Thus the total sum is at most
-$$Cε^{6/5}|\logε|^{C_*}$$
+$$Cε^{6/5}|logε|^{C_*}$$
Since $(6)/(5)=1.2>1+(1)/(20)=1.05$, this is
-$\le Cε^{1+1/20}$, proving the discrepancy bound. (The witnesses
+$le Cε^{1+1/20}$, proving the discrepancy bound. (The witnesses
with terminal component larger than $Λ_i$ are smaller than any power
by the energy tail, the analytic package, via the activity cost
-$\mu=ε^{-2}$ versus the Gaussian gain over $Λ_i\ge|\logε|^{30}$
+$mu=ε^{-2}$ versus the Gaussian gain over $Λ_ige|logε|^{30}$
births, summing geometrically as in the coarse step.)
-Remark (Order of choices). The local exponent $\delta$ and the finite hierarchy of
-the amplified cut fix $\Gamma_0$ from dimensional constants. Then
-choose $\Gamma$, then $L$ for the imported estimates and the common
+Remark (Order of choices). The local exponent $delta$ and the finite hierarchy of
+the amplified cut fix $Gamma_0$ from dimensional constants. Then
+choose $Gamma$, then $L$ for the imported estimates and the common
exponential base; only afterward choose $K$, the localization powers, and the
small upper bound on $ε$. No observation number or moment order enters the
first two choices. This is what allows a single pasted dynamics to be fixed in
@@ -2485,86 +2485,86 @@ the Gaussian limit of the model dynamics, below.
The pasted process of the pasted Gaussian limit is centered by its own
microscopic mean. The real gas is centered by a slightly different mean,
since the pasted and true laws charge the discrepancy event (probability
-$\le Cε^{1+\eta}$, the pasted accuracy bound) with different mass. At the
-fluctuation scale $\sqrt\mu=ε^{-1}$ this difference of means must go to
+$le Cε^{1+eta}$, the pasted accuracy bound) with different mass. At the
+fluctuation scale $sqrtmu=ε^{-1}$ this difference of means must go to
zero, and that is exactly the sharp estimate of the pasted accuracy bound. This is made
quantitative, then the fluctuation limit theorem is assembled.
Lemma (Discrepancy and centering). Couple the true and pasted dynamics from the same initial configuration.
-For every fixed time $t$ and bounded continuous test $\phi$, with
-$\|N/\mu\|_{L^2}\le C$,
+For every fixed time $t$ and bounded continuous test $phi$, with
+$|N/mu|_{L^2}le C$,
-$$\sqrt\mu |E_{true}\pi_t^ε(\phi)
--E_{pasted}\pi_t^ε(\phi)|
-\le C_\phi ε^{(\eta-1)/2}→0$$
+$$sqrtmu |E_{true}pi_t^ε(phi)
+-E_{pasted}pi_t^ε(phi)|
+le C_phi ε^{(eta-1)/2}→0$$
and moreover
-$$\zeta_t^{ε,true}(\phi)
-=\zeta_t^{ε,pasted}(\phi)+o_{L^1}(1)$$
+$$zeta_t^{ε,true}(phi)
+=zeta_t^{ε,pasted}(phi)+o_{L^1}(1)$$
Proof.
-Let $A=\{the two trajectories agree on [0,T]\}$, so
-$P(A^c)\le Cε^{1+\eta}$, and both $N$ and $N/\mu$ have bounded second
+Let $A={the two trajectories agree on [0,T]}$, so
+$P(A^c)le Cε^{1+eta}$, and both $N$ and $N/mu$ have bounded second
moments (the initial ensemble). On $A$ the empirical measures agree for every
-$t$, hence so do $\pi_t^ε(\phi)$ and the running records. Write
-$\pi=(1/\mu)\sum_i\phi$. Off $A$, $|\pi|\le\|\phi\|_∞ N/\mu$ on either
-side, so $|\pi^{true}-\pi^{pasted}|
-\le2\|\phi\|_∞ (N/\mu) 1 _{A^c}$. By Cauchy--Schwarz,
+$t$, hence so do $pi_t^ε(phi)$ and the running records. Write
+$pi=(1/mu)sum_iphi$. Off $A$, $|pi|le|phi|_∞ N/mu$ on either
+side, so $|pi^{true}-pi^{pasted}|
+le2|phi|_∞ (N/mu) 1 _{A^c}$. By Cauchy--Schwarz,
$$
-|E_{true}\pi-E_{pasted}\pi|
-\le2\|\phi\|_∞\|N/\mu\|_{L^2} P(A^c)^{1/2}
-\le C_\phi ε^{(1+\eta)/2},
+|E_{true}pi-E_{pasted}pi|
+le2|phi|_∞|N/mu|_{L^2} P(A^c)^{1/2}
+le C_phi ε^{(1+eta)/2},
$$
-and multiplying by $\sqrt\mu=ε^{-1}$ gives
-$ε^{(\eta-1)/2}\to0$, proving the mean comparison.
+and multiplying by $sqrtmu=ε^{-1}$ gives
+$ε^{(eta-1)/2}to0$, proving the mean comparison.
For the centered-difference estimate, insert the centered definitions:
-$\zeta^{true}-\zeta^{pasted}
-=\sqrt\mu[(\pi^{true}-\pi^{pasted})
--(E_{true}\pi-E_{pasted}\pi)]$.
+$zeta^{true}-zeta^{pasted}
+=sqrtmu[(pi^{true}-pi^{pasted})
+-(E_{true}pi-E_{pasted}pi)]$.
The second bracket is bounded by the mean comparison. For the first,
using the $A^c$ indicator,
$$
-E\sqrt\mu |\pi^{true}-\pi^{pasted}|
-\le2\|\phi\|_∞\sqrt\mu E[(N/\mu) 1 _{A^c}]
-\le2\|\phi\|_∞\|N/\mu\|_{L^2}\sqrt\mu P(A^c)^{1/2},
+Esqrtmu |pi^{true}-pi^{pasted}|
+le2|phi|_∞sqrtmu E[(N/mu) 1 _{A^c}]
+le2|phi|_∞|N/mu|_{L^2}sqrtmu P(A^c)^{1/2},
$$
-and $\sqrt\mu ε^{(1+\eta)/2}=ε^{-1}ε^{(1+\eta)/2}
-=ε^{(\eta-1)/2}\to0$. So the $L^1$ norm of the difference of the
+and $sqrtmu ε^{(1+eta)/2}=ε^{-1}ε^{(1+eta)/2}
+=ε^{(eta-1)/2}to0$. So the $L^1$ norm of the difference of the
centered fields tends to zero.
Proof of the fluctuation limit theorem.
Existence and uniqueness of the target. the Gaussian target
-constructs the centered generalized Gaussian field $\zeta$ with covariance
-the target covariance, initial field $\zeta_0$ of covariance
+constructs the centered generalized Gaussian field $zeta$ with covariance
+the target covariance, initial field $zeta_0$ of covariance
the initial covariance independent of the noise $W$, and weak equation
the fluctuating equation; uniqueness in law holds in the class of
$L^2$-continuous fields there.
Initial fluctuation limit. the initial ensemble, part (iii) gives, for any
fixed list of tests, joint convergence of
-$(\zeta_0^ε(\phi_1),...,\zeta_0^ε(\phi_m))$ to the centered Gaussian
-vector with covariance $\int f_0\phi_i\phi_j$.
+$(zeta_0^ε(phi_1),...,zeta_0^ε(phi_m))$ to the centered Gaussian
+vector with covariance $int f_0phi_iphi_j$.
Dynamical limit on the pasted dynamics. Fix a single pasted
-dynamics as in the Gaussian limit of the model dynamics, below ($\Gamma,L$ independent of the
+dynamics as in the Gaussian limit of the model dynamics, below ($Gamma,L$ independent of the
observation list and order). the pasted Gaussian limit gives, for every fixed
list of times and tests, convergence of the centered combination
-$ε\sum_i y_i(T)$ to $\sum_j\zeta_{t_j}(\phi_j)$, with convergence of all
+$εsum_i y_i(T)$ to $sum_jzeta_{t_j}(phi_j)$, with convergence of all
centered moments. By the factorial-to-ordinary identity and
the sharp connected bounds, this is the finite-dimensional Gaussian limit
with the multi-time covariance the target covariance.
Transfer to the true flow. By the discrepancy and centering bound,
-$\zeta_t^{ε,true}(\phi)-\zeta_t^{ε,pasted}(\phi)
+$zeta_t^{ε,true}(phi)-zeta_t^{ε,pasted}(phi)
=o_{L^1}(1)$, while
-$|\zeta_t^ε(\phi)|\le\|\phi\|_∞(ε N+ε E N)$ has uniformly
-bounded moments because $E(N/\mu)^p<∞$ (the initial ensemble). Hence the
+$|zeta_t^ε(phi)|le|phi|_∞(ε N+ε E N)$ has uniformly
+bounded moments because $E(N/mu)^p<∞$ (the initial ensemble). Hence the
$p$-moments of the difference vanish for every fixed $p$ by interpolation of
the $L^1$ bound with the uniform $L^{p+1}$ bound, and, for any bounded
continuous functional of a fixed finite collection
-$(\zeta_{t_1}^ε(\phi_1),...,\zeta_{t_m}^ε(\phi_m))$,
+$(zeta_{t_1}^ε(phi_1),...,zeta_{t_m}^ε(phi_m))$,
$$
E_{true}F-E_{pasted}F→0
$$
@@ -2573,7 +2573,7 @@ one, then the moment control of the difference off the compact). Therefore
the true centered fields converge in distribution to the same Gaussian
vector. Sending the finite list over a countable dense family and using the
variance bound the field bound upgrades this to the map
-$t\mapsto\zeta_t(\phi)$ in joint law.
+$tmapstozeta_t(phi)$ in joint law.
Weak equation. The limiting field inherits the fluctuating equation from the
isonormal construction, so its law is the one prescribed. The