Manuscript X-I-ST@1 · X-I-ST.tex · section · 9745fd40

Why a covariant density does not erase all switching terms

The finite lift and its explicit next residual › Why a covariant density does not erase all switching terms · lines 1336–1345

Let

V_{1} = \frac{1}{4 !} \int \frac{1}{2} tr_{η} (h + r) a ϕ^{4} d^{4} x .

This is the first volume-density correction to the compact potential.

Displayed formulas in this passage

unlabeled · line 1339
$V_{1} = \frac{1}{4 !} \int \frac{1}{2} tr_{η} (h + r) a ϕ^{4} d^{4} x .$