Kitabın içinden
67 sonuçtan 1-3 arası sonuçlar
Sayfa 91
In what follows , we deal with various vectors in the tensor product V®2n , along
with those obtained by permuting the tensor ... By $ 2 , 2 , 1 , 1 we do not mean a
vector in V2 V2 ØVi Ví . Note that , in this notation , s } = - s ' e Vio Ví . Sometimes
...
In what follows , we deal with various vectors in the tensor product V®2n , along
with those obtained by permuting the tensor ... By $ 2 , 2 , 1 , 1 we do not mean a
vector in V2 V2 ØVi Ví . Note that , in this notation , s } = - s ' e Vio Ví . Sometimes
...
Sayfa 410
The components Aj of the vector - valued ( magnetic ) potential ... 3 ) is absolutely
continuous if ( at least ) one of the following conditions is satisfied : 1 ) n = 2 ,
V E L ' ( K ) , 9 > 2 , and the vector - valued potential A E L ( R2 ; R2 ) satisfies ( 0 .
The components Aj of the vector - valued ( magnetic ) potential ... 3 ) is absolutely
continuous if ( at least ) one of the following conditions is satisfied : 1 ) n = 2 ,
V E L ' ( K ) , 9 > 2 , and the vector - valued potential A E L ( R2 ; R2 ) satisfies ( 0 .
Sayfa 411
For n > 3 , the results of ( 12 ) were based on Sobolev ' s paper [ 17 ] , where the
absolute continuity of the spectrum was proved for the Schrödinger operator with
a periodic vector - valued potential A E C2n + 3 ( R " ; R ” ) . The latter condition ...
For n > 3 , the results of ( 12 ) were based on Sobolev ' s paper [ 17 ] , where the
absolute continuity of the spectrum was proved for the Schrödinger operator with
a periodic vector - valued potential A E C2n + 3 ( R " ; R ” ) . The latter condition ...
Kullanıcılar ne diyor? - Eleştiri yazın
Her zamanki yerlerde hiçbir eleştiri bulamadık.
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 | |
6 diğer bölüm gösterilmiyor
Diğer baskılar - Tümünü görüntüle
Sık kullanılan terimler ve kelime öbekleri
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