By S. L. Sobolev
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Extra info for Applications of Functional Analysis in Mathematical Physics (Translations of Mathematical Monographs, Vol 7)
Example text
Lehrbueh der Mathematischen Physik. 3. R. Germany We p r e s e n t a g e o m e t r i c proof of a s y m p t o t i c c o m p l e t e n e s s ing systems which follows w i t h m a t h e m a t i c a l rigor the physical tion of the s p a c e - t i m e b e h a v i o r of a state. , sup t>0 scattering H = [3]. HP(H) • Hc°nt(H) spectral subspaces of + V, H O plication-or intui- As an example we will short-range potential The H i l b e r t space is H = L 2 ( ~ ) . for scatter- = -(i/2m) A, V a multiO (velocity d e p e n d e n t force) operator.
Follows A,B (i0) be b o u n d e d , fying IAul ~ B lu I for all class and Tr A $ Tr B We r e m a r k natively, that one By the arbitrary fields. cussed [i0]. in 3. S p e c t r a l (8) Lemma IAu~ As 2 Other Let A,B a = 0 ingredient Lemma 3 in the the be b o u n d e d u this . If is w e l l class (it) then (i) [53] that All sequence [58, there bounds A is t r a c e suitable the VI . Alter- in a box. (field-independent) quantum free energy and c l a s s i c a l limits compactness criterion following operators B known on L2(M,d~) is c o m p a c t , then is c o m p a c t and easy domination and points for to prove.
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