Manuscript IV@1 · IV.tex · section · 351cb2d7

Front matter

Front matter · lines 169–202

{}1.2

Model	Operator class	Cutoffs in the theorem	$λ = 0$
Finite TT plane	ESA quadratic	Edge $ε$ removable; plane fixed	Exact
Dense TT	Bounded $A_{R, M}$	$R, M$ named; $R \to \infty$ at fixed $M$	Exact
$k = 0$ stress form	Bounded $A_{Λ, M}$	$Λ, M$ named	Exact

Classical sourced $j$ exists. It is not an argument of $A^{(1)}$ or $A^{(2)}$ , and it is not the cubic $S_{t_{0}} (j) ϕ$ .

Nearby in this section