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Sayfa 2
The integral was constructed explicitly in terms of modular forms as the Rankin -
Selberg convolution . After the results of Colin de Verdière and Mueller , it must
be remembered that on a general Riemannian manifold with cusps the Laplace ...
The integral was constructed explicitly in terms of modular forms as the Rankin -
Selberg convolution . After the results of Colin de Verdière and Mueller , it must
be remembered that on a general Riemannian manifold with cusps the Laplace ...
Sayfa 114
Thus , the integral in ( B . 3 ) takes the form n - 1 n - 1 n - 1 ( 8 . 4 ) . dan , [ edium +
/ . I do , I do + / sth I turn U n - 1 hus LI We treat the limit of these three parts
separately . Consider the first integral in ( B . 4 ) . After the change Un H Un + / 1 ,
the ...
Thus , the integral in ( B . 3 ) takes the form n - 1 n - 1 n - 1 ( 8 . 4 ) . dan , [ edium +
/ . I do , I do + / sth I turn U n - 1 hus LI We treat the limit of these three parts
separately . Consider the first integral in ( B . 4 ) . After the change Un H Un + / 1 ,
the ...
Sayfa 453
3 , Pages 453 – 463 S 1061 - 0022 ( 06 ) 00914 - 9 Article electronically
published on March 9 , 2006 INTEGRAL MEANS SPECTRUM AND THE
MODIFIED BESSEL FUNCTION OF ZERO ORDER I . R . KAYUMOV ABSTRACT
. A new ...
3 , Pages 453 – 463 S 1061 - 0022 ( 06 ) 00914 - 9 Article electronically
published on March 9 , 2006 INTEGRAL MEANS SPECTRUM AND THE
MODIFIED BESSEL FUNCTION OF ZERO ORDER I . R . KAYUMOV ABSTRACT
. A new ...
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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 | |
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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