Physics - Mathematics Department - California Institute of Technology
Physics - Mathematics Department - California Institute of Technology
Physics - Mathematics Department - California Institute of Technology
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640 E. H. Lieb, I. M. Sigal, B. Simon and W. Thirring<br />
where G α is given by (3.3). The symmetry condition (1) is obvious, and (3) holds<br />
since φ(y)= 1 if y^l.<br />
F a Φ0 implies that 1*1^1-2^ \x a \ ^(1 -ε^lxU, and<br />
Σ<br />
bfa<br />
since φ(y) Φ 0 implies \y| ^ 1 — 2ε. Since \x — y\~* ^ G α (x,j/), we have proven (4).<br />
That leaves the key conditions (5') and (2').<br />
For (2'), we use Theorem 3.2. This guarantees us that there is an a where the<br />
last two factors in F a are 1, and so there is an a with F a(x) =