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77 sonuçtan 1-3 arası sonuçlar
Sayfa 53
In the resulting difference system it is natural to assume that the variable u lives at
the points of the cubic lattice ( EZ ) 3 ; the variables a , b , c live on the edges of
the lattice adjacent to the point ( x , y , z ) in the r- , yand z - direction , respectively
...
In the resulting difference system it is natural to assume that the variable u lives at
the points of the cubic lattice ( EZ ) 3 ; the variables a , b , c live on the edges of
the lattice adjacent to the point ( x , y , z ) in the r- , yand z - direction , respectively
...
Sayfa 290
... ( 88,56 , ) .x8 , ( b ) ui , where vi ( respectively , ui ) is a product of elements of
the form Xa ( d ) , d E A , a E R( respectively , a E R + ) and a # -81 ( respectively ,
a # 81 ) , and where c , b E A ( this follows from Chevalley's commutator formula )
.
... ( 88,56 , ) .x8 , ( b ) ui , where vi ( respectively , ui ) is a product of elements of
the form Xa ( d ) , d E A , a E R( respectively , a E R + ) and a # -81 ( respectively ,
a # 81 ) , and where c , b E A ( this follows from Chevalley's commutator formula )
.
Sayfa 352
Then Y = Tor ( Ă ) is a nonsingular threefold , and Y Tor ( A ' ) , YO " = Tor ( A " )
are surfaces isomorphic ( respectively ) to p2 and P2 with a blown - up point ,
where A ' = conv { ( 0,0,0 ) , ( p , 0 , 0 ) , ( 0 , p , 0 ) } , A ” = conv { ( P , 0,0 ) , ( 0 , p ,
0 ) ...
Then Y = Tor ( Ă ) is a nonsingular threefold , and Y Tor ( A ' ) , YO " = Tor ( A " )
are surfaces isomorphic ( respectively ) to p2 and P2 with a blown - up point ,
where A ' = conv { ( 0,0,0 ) , ( p , 0 , 0 ) , ( 0 , p , 0 ) } , A ” = conv { ( P , 0,0 ) , ( 0 , p ,
0 ) ...
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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