Kitabın içinden
70 sonuçtan 1-3 arası sonuçlar
Sayfa 74
... important asymptotic representations for the Green function can be deduced .
In the limit corresponding to zero temperature and to infinite size of the domain
occupied by the Bose gas , we can come to the asymptotics of I ( x1 , T1 : X2 , T2 )
.
... important asymptotic representations for the Green function can be deduced .
In the limit corresponding to zero temperature and to infinite size of the domain
occupied by the Bose gas , we can come to the asymptotics of I ( x1 , T1 : X2 , T2 )
.
Sayfa 115
vanishes in the limit + too . For this , we decompose D2 as follows . Set Uk ) = { #
Im u ; > u / 3 } n D2 for k = 1 , ... , n - 1. Then D2 = UK ( U ) UU ( k ) ) . We prove
that the integral over each set Uk ) x { te + iyl – 4/3 Sy SM / 3 } vanishes in the limit
.
vanishes in the limit + too . For this , we decompose D2 as follows . Set Uk ) = { #
Im u ; > u / 3 } n D2 for k = 1 , ... , n - 1. Then D2 = UK ( U ) UU ( k ) ) . We prove
that the integral over each set Uk ) x { te + iyl – 4/3 Sy SM / 3 } vanishes in the limit
.
Sayfa 402
We remark that the technique described above applies in the limit as I – o as well
. In this limit , assuming that Ř + 1 = lim – to R ( ) exists , the YB equation ( 10 )
turns into ( 69 ) Ř , 2Ř23 Ř , 2 = Ř23 Ř Ř23 . Denote d ; = limx - toorj ( 1 ) , so that
...
We remark that the technique described above applies in the limit as I – o as well
. In this limit , assuming that Ř + 1 = lim – to R ( ) exists , the YB equation ( 10 )
turns into ( 69 ) Ř , 2Ř23 Ř , 2 = Ř23 Ř Ř23 . Denote d ; = limx - toorj ( 1 ) , so that
...
Kullanıcılar ne diyor? - Eleştiri yazın
Her zamanki yerlerde hiçbir eleştiri bulamadık.
İçindekiler
Данилов Л И Об отсутствии собственных значений в спектре | 47 |
A Antipov and A I Generalov The Yoneda algebras of symmetric special | 377 |
A G Bytsko On higher spin U sl2invariant Rmatrices | 393 |
Telif Hakkı | |
7 diğer bölüm gösterilmiyor
Diğer baskılar - Tümünü görüntüle
Sık kullanılan terimler ve kelime öbekleri
algebraic analytic apply approximation arbitrary argument assume bounded called closed coefficients coincides complete condition connected Consequently consider constant construction contains continuous corresponding covering curves defined definition deformation denote depend determined dimension discrete edges element English equation equivalent estimate exists fact finite fixed formula function given Goursat problem graph identity implies inequality integral introduce invariant lattice Lemma limit linear locally Math Mathematical matrix means measure metric Moreover Note obtain operator parameters particular periodic Phys points polynomial positive potential problem Proof proof of Theorem Proposition prove quantum rational reduced regular relation Remark respectively result satisfies sequence side singular solution space spectrum statement Subsection suffices Suppose Theorem theory transformation unique values vector vertex vertices zero