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60 sonuçtan 1-3 arası sonuçlar
Sayfa 115
To prove the claim , we bound the integrand by a certain integrable function of
the form n - 1 ( B.8 ) e - cu uk Rk ( U1 , ... , Uni 12 , ... , An ) , k = - ( n - 1 ) where c
is a positive constant . First , consider the rational part Pa , B . We have inequality
...
To prove the claim , we bound the integrand by a certain integrable function of
the form n - 1 ( B.8 ) e - cu uk Rk ( U1 , ... , Uni 12 , ... , An ) , k = - ( n - 1 ) where c
is a positive constant . First , consider the rational part Pa , B . We have inequality
...
Sayfa 540
Since the proof of inequality ( 4.5 ) is independent of the mutual location of the
points x and y , this proof remains valid under the assumption that the event S
happens . Multiplying ( 4.5 ) by ( n − 1 ) ( n − 2 ) ( u ) y ( v ) dum ( B ( u , x ) ) dy (
B ( v ...
Since the proof of inequality ( 4.5 ) is independent of the mutual location of the
points x and y , this proof remains valid under the assumption that the event S
happens . Multiplying ( 4.5 ) by ( n − 1 ) ( n − 2 ) ( u ) y ( v ) dum ( B ( u , x ) ) dy (
B ( v ...
Sayfa 547
This proves inequalities ( 5.14 ) . In a similar way we ... To prove ( 1.17 ) in this
case , we substitute the value ( 5.6 ) of the B - statentropy into inequality ( 1.17 ) ,
obtaining an equivalent inequality : ( 5.16 ) 9 ( 23 ) < 29 ( 8 ) . This is equivalent to
...
This proves inequalities ( 5.14 ) . In a similar way we ... To prove ( 1.17 ) in this
case , we substitute the value ( 5.6 ) of the B - statentropy into inequality ( 1.17 ) ,
obtaining an equivalent inequality : ( 5.16 ) 9 ( 23 ) < 29 ( 8 ) . This is equivalent to
...
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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