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73 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 f ( x1 , 71 ; 72 , 72 )
.
... 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 f ( x1 , 71 ; 72 , 72 )
.
Sayfa 115
vanishes in the limit u + + 0 . For this , we decompose D2 as follows . Set U ) = { +
Im u ; > u / 3 } n D2 for k = 1 , . . . , n - 1 . Then D2 = U ( UK ) UU ( K ) ) . We prove
that the integral over each set U x { £e + iyl – 4 / 3 SY SM / 3 } vanishes in the ...
vanishes in the limit u + + 0 . For this , we decompose D2 as follows . Set U ) = { +
Im u ; > u / 3 } n D2 for k = 1 , . . . , n - 1 . Then D2 = U ( UK ) UU ( K ) ) . We prove
that the integral over each set U x { £e + iyl – 4 / 3 SY SM / 3 } vanishes in the ...
Sayfa 402
We remark that the technique described above applies in the limit as 1 → as well
. In this limit , assuming that Ř + 1 = lim – + - R ( 1 ) exists , the YB equation ( 10 )
turns into ( 69 ) Ř 2 Ř23 Ř12 = Ř23 Ř12 Ř23 . Denote d ; = limi - toori ( 1 ) , so ...
We remark that the technique described above applies in the limit as 1 → as well
. In this limit , assuming that Ř + 1 = lim – + - R ( 1 ) exists , the YB equation ( 10 )
turns into ( 69 ) Ř 2 Ř23 Ř12 = Ř23 Ř12 Ř23 . Denote d ; = limi - toori ( 1 ) , so ...
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İçindekiler
A Antipov and A I Generalov The Yoneda algebras of symmetric special | 377 |
A G Bytsko On higher spin U sl2invariant Rmatrices | 393 |
Dirac operator | 409 |
Telif Hakkı | |
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algebraic analytic apply approximation arbitrary argument assume asymptotic bounded called closed coefficients coincides complete condition connected Consequently consider consists constant construction contains continuous corresponding curves defined definition denote depend determined differential dimension discrete edges element equal equation equivalent estimate example exists fact finite fixed formula function given Goursat problem graph hyperbolic identity implies inequality integral introduce invariant lattice Lemma limit linear locally Math Mathematical matrix functions means measure metric Moreover Note obtain operator parameter particular periodic 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 sufficiently Suppose Theorem theory transformation unique values vector vertices zero