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88 sonuçtan 1-3 arası sonuçlar
Sayfa 188
Cube solution ( 2 ) . RS ? ( 1 / 3 2 . B - split . Cube solution ( ? ) : RSA ij 131
21111 : 1 / 3 , 1 / 2 2 = u 2 – 1 = ( 1 - 3 . 32 ) P ( 21 – a ) 3z1 p ( 21 – b ) ( 21 – t ) (
21 – c ) 2 ( 21 - 1 ) ' ( 21 - c ) 2 ( 21 – 1 ) ? ( 2s + 1 ) 3 P = ( 38 + 1 ) 2 ( 1 – 382 ) 2 ”
a ...
Cube solution ( 2 ) . RS ? ( 1 / 3 2 . B - split . Cube solution ( ? ) : RSA ij 131
21111 : 1 / 3 , 1 / 2 2 = u 2 – 1 = ( 1 - 3 . 32 ) P ( 21 – a ) 3z1 p ( 21 – b ) ( 21 – t ) (
21 – c ) 2 ( 21 - 1 ) ' ( 21 - c ) 2 ( 21 – 1 ) ? ( 2s + 1 ) 3 P = ( 38 + 1 ) 2 ( 1 – 382 ) 2 ”
a ...
Sayfa 191
The solution corresponding to the second RS - transformation ( 3 . 2 ) is a
renormalization of the function z ( zı ) : = = 3 ( M - 1 ( 51 ) ) , 81 = M ( 31 ) = = 931 ,
i = M ( t ) , ỵ = M ( g ) . Redenoting back t Ht and ✓ Hy , we get t = _ ( 28 – 1 ) ? y (
t ) ...
The solution corresponding to the second RS - transformation ( 3 . 2 ) is a
renormalization of the function z ( zı ) : = = 3 ( M - 1 ( 51 ) ) , 81 = M ( 31 ) = = 931 ,
i = M ( t ) , ỵ = M ( g ) . Redenoting back t Ht and ✓ Hy , we get t = _ ( 28 – 1 ) ? y (
t ) ...
Sayfa 194
The corresponding solution found with the help of Theorem 2 . 1 looks like this :
2893 ( s2 – 5 ) = ( s – 1 ) 5 ( 8 + 3 ) 3 ( 52 – 48 – 1 ) ' 2652 yl ) = ( s – 1 ) ( 8 + 3 ) (
82 + 3 ) ( 82 – 48 – 1 ) ' ôo = = 04 = 8c = By the Okamoto transformation ( see ...
The corresponding solution found with the help of Theorem 2 . 1 looks like this :
2893 ( s2 – 5 ) = ( s – 1 ) 5 ( 8 + 3 ) 3 ( 52 – 48 – 1 ) ' 2652 yl ) = ( s – 1 ) ( 8 + 3 ) (
82 + 3 ) ( 82 – 48 – 1 ) ' ôo = = 04 = 8c = By the Okamoto transformation ( see ...
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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 | |
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