Kitabın içinden
80 sonuçtan 1-3 arası sonuçlar
Sayfa 91
Note that , in this notation , ( 1 ) ( 1 ) = -81.1 E Vio Vi . Sometimes , we need to
construct a vector in Vi ØV2 Ø V2 Vi starting with one in Vi Vi and one in V2 Vž .
Suppose f , gEVOV . Then f1,1 E VIVī , and 92,2 E V2 Ø Vž . We write f1,192 , ż for
...
Note that , in this notation , ( 1 ) ( 1 ) = -81.1 E Vio Vi . Sometimes , we need to
construct a vector in Vi ØV2 Ø V2 Vi starting with one in Vi Vi and one in V2 Vž .
Suppose f , gEVOV . Then f1,1 E VIVī , and 92,2 E V2 Ø Vž . We write f1,192 , ż for
...
Sayfa 190
This dessin gives rise to a function z ( 21 ) of the type R ( 4 + 1 + 12 + 2 + 2 3 + 2
+ 1 ) . It is of interest to note that , as a function of y , it has three branches . Only
two of them can be obtained as B - splits of the reduced cube . The third branch is
...
This dessin gives rise to a function z ( 21 ) of the type R ( 4 + 1 + 12 + 2 + 2 3 + 2
+ 1 ) . It is of interest to note that , as a function of y , it has three branches . Only
two of them can be obtained as B - splits of the reduced cube . The third branch is
...
Sayfa 447
We note that each line L of the generalized quadrangle ( a ) intersects A at 0 or 2
points . Indeed , if c E LnA , then M = ( LU { a } ) – { c } is a line in ( c ) , and , by the
definition of a generalized quadrangle , [ b ] contains a unique point d in M.
We note that each line L of the generalized quadrangle ( a ) intersects A at 0 or 2
points . Indeed , if c E LnA , then M = ( LU { a } ) – { c } is a line in ( c ) , and , by the
definition of a generalized quadrangle , [ b ] contains a unique point d in M.
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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 | |
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