Mutual response of the candidate coupling

Generalized force densities in N/m³, not electric current densities.

Theory · CANDIDATE MODELEquation version 1.0.0

Based on the final manuscript · Chapter 3

\mathbf f_L^{\rm nl}=-g_{LT}\nabla|\boldsymbol\Omega_T|^2,\quad\mathbf f_T^{\rm nl}=-2g_{LT}\nabla\times(\eta\boldsymbol\Omega_T)

Generalized force densities in N/m³, not electric current densities.
Chapter reference: Final collected manuscript · Chapter 3, equations (3.76) · ASD-BOOK-ddbade997b45

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Final collected manuscript · Chapter 3, equations (3.76)

Generalized force densities in N/m³, not electric current densities.

Conditions retained in this adoption

Vanishing boundary variations; constant g_LT, K_L and λ_T.
K_L>0 and λ_T≥2g_LT²/K_L
Minimize over η at fixed transverse intensity.

Specific unresolved source issues

Full gradient energy, microscopic parameters, long-range sources and stable configurations remain research tasks.

Source locators: p1240 · p1241 · p1243 · p1244 · p1245 · p1246 · p1249 · p1250 · p1251 · p1252 · p1284 · 最终合订稿 · 第三章式 (3.76)

Manuscript SHA-256: ddbade997b45913248e588953b1d27ccb9c7c206c3c8d992d3aef2364a64836e

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EM-f06476f55cae · 第三章 / Chapter 3 · (3.76), PDF p. 17

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