diff 56bc728..6fbd3ac three_manifold_no_conjugate_v2.txt
diff --git a/three_manifold_no_conjugate_v2.txt b/three_manifold_no_conjugate_v2.txt
index 39717b3..fc5ae59 100644
--- a/three_manifold_no_conjugate_v2.txt
+++ b/three_manifold_no_conjugate_v2.txt
@@ -1802,7 +1802,7 @@ The right-hand side depends only on the "end-to-end displacement"
V. Because the field V^gauge has infinitely many degrees of freedom,
we cannot try to make (8.43) hold by minimization over shape: we
must SHOW it whenever V satisfies our gauge. That is the content
-of Part 9: the inequality (8.43) is proved for EVERY smooth field V
+of Part 9: the ineuality (8.43) is proved for EVERY smooth field V
along the passage [0, L], not merely the minimizer. The condition
"q_V affine" only enters via (8.41), which converts ∫|q_V'|²
into the "cheap" term (p^T Δz)^2/L.
@@ -1813,7 +1813,7 @@ PART 9. THE RETURNING PASSAGE ESTIMATE
================================================================
By Lemma 8.5, all passages except case (H) of 8.6 are already handled.
-This part treats case (H). Recall from 8.6 the required inequality:
+This part treats case (H). Recall from 8.6 the required ineuality:
E_[0,L](V) + (κ v_0/2)(z_1(0)^2 + z_1(L)^2) >= (p^T Δz)^2 / L, (9.0)
@@ -1908,8 +1908,8 @@ requires a more explicit value than β < 1; only the numeric quantity
9.2 The bilinear form S and the Hilbert-space duality
-In this subsection we turn the inequality (9.0) into a 2x2 matrix
-inequality. The mechanism is Hilbert-space Cauchy-Schwarz.
+In this subsection we turn the ineuality (9.0) into a 2x2 matrix
+ineuality. The mechanism is Hilbert-space Cauchy-Schwarz.
Setup. Fix a returning passage [0, L] as in 9.1. Its geodesic
gamma = (t, x) is fixed; the field V = (w, z) varies. Recall the
@@ -2032,7 +2032,7 @@ frame) and p the passage's conserved momentum:
Proof. We use the explicit structure (9.9) and the cometric bounds
(Lemma 6.4).
-Preliminary: D-norm inequality. For every w ∈ D and every
+Preliminary: D-norm ineuality. For every w ∈ D and every
-∞ <= s_1 < s_2 <= +∞,
∫_{s_1}^{s_2} sqrt(-F''(t(s))) |w(s)| ds <= sqrt(2(s_2 - s_1)) ||w||_D. (9.12)
@@ -2222,7 +2222,7 @@ This is (ii). ∎
LEMMA 9.7 (Turning estimate). There exists δ_2 ∈ (0, δ_1] such that,
for every 0 < δ <= δ_2, every returning passage [0, L] with t_* > 1/4
and every smooth field V = (w, z) with w(0) = w(L) = 0 satisfies the
-key inequality (9.0):
+key ineuality (9.0):
E_[0,L](V) + (κ v_0/2)(z_1(0)² + z_1(L)²) >= (p^T Δz)²/L. (9.0) again
@@ -2234,7 +2234,7 @@ ranging over R²:
(c^T X)² <= S(c,c) · E_[0,L](V) for every c ∈ R².
This is equivalent (standard 2x2 Cauchy-Schwarz) to the matrix
-inequality
+ineuality
X^T S^{-1} X <= E_[0,L](V). (9.21)
@@ -2300,8 +2300,8 @@ The specific threshold r_0 and constant δ_2 are chosen once and for
all, depending only on (C_m, C_e, β, a(0)), and independent of δ, of
B_1, B_2, and of the particular passage.
-CONCLUSION. With δ <= δ_2, the inequality (target) holds, hence by
-Lemma 9.6 the matrix inequality X^T M X <= L E (equivalently,
+CONCLUSION. With δ <= δ_2, the ineuality (target) holds, hence by
+Lemma 9.6 the matrix ineuality X^T M X <= L E (equivalently,
(p^T Δz)² <= L E + Lμ (e^T Δz)²) holds. Since
(κv_0/2)(z_1(0)² + z_1(L)²) >= (κv_0/4)(Δz_1)² = μ(e^T Δz)² (using
2(z_1(0)² + z_1(L)²) >= (Δz_1)²), this gives (9.0). ∎
@@ -2342,7 +2342,7 @@ of Lemma 8.3.
by Lemma 9.7. And I_J(V) = I_J^⊥(V) + ∫_J |q_V'|² >= I_J^⊥(V) >= 0.
-So both inequalities hold in every case. ∎
+So both ineualities hold in every case. ∎
================================================================