Independent stretch candidate

Its energy kernel differs from displacement divergence; keeping both requires constraints or scale separation.

Theory · CANDIDATE MODELEquation version 1.0.0

Based on the final manuscript · Chapters 4 and 5

\mathcal L_\varphi=\tfrac12Z_\varphi[(\partial_t\varphi)^2-c^2|\nabla\varphi|^2]+\varphi\mathcal J_g[\Theta,\nabla\Theta]

Its energy kernel differs from displacement divergence; keeping both requires constraints or scale separation.
Chapter reference: Ch. 5 (5.6.16) · ASD-BOOK-ddbade997b45

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Ch. 5 (5.6.16)

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Its energy kernel differs from displacement divergence; keeping both requires constraints or scale separation.

Source locators: p2254–2257

Manuscript SHA-256: ddbade997b45913248e588953b1d27ccb9c7c206c3c8d992d3aef2364a64836e

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SD-51779505a476 · Ch. 5 (5.6.16)

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