Manuscript Psy02-B@2 · Psy02-B-v2.tex · section · cfd06e2e

A fully specified parameterized Euler interface

Track B foundations: density weighting, response, and roots › A fully specified parameterized Euler interface · lines 1485–1501

Let $γ_{I}$ be the finitely many components of a symmetric metric perturbation. Fix a local cubic density

ℓ_{3} (γ, \partial γ, \partial^{2} γ)

with symmetric second-derivative jet convention. Its exact coefficients are input data. Define

V_{3, D} = \int σ_{ε} ℓ_{3} d^{4} x, J_{3, I} = EL_{I} (ℓ_{3}) .

Displayed formulas in this passage

unlabeled · line 1490
$ℓ_{3} (γ, \partial γ, \partial^{2} γ)$
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$V_{3, D} = \int σ_{ε} ℓ_{3} d^{4} x, J_{3, I} = EL_{I} (ℓ_{3}) .$