Kitabın içinden
75 sonuçtan 1-3 arası sonuçlar
Sayfa 467
Next , we denote by X either the Sobolev spaces H ! ( 1 ) if Bu = u , or H1 ( 12 ) in
the case of the Neumann condition or ... ( s ) u ( s ) ds ( Lu , v ) x uz i , j = 1 for any
u , v E X , where o ( x ) = 0 for the Dirichlet and Neumann boundary conditions .
Next , we denote by X either the Sobolev spaces H ! ( 1 ) if Bu = u , or H1 ( 12 ) in
the case of the Neumann condition or ... ( s ) u ( s ) ds ( Lu , v ) x uz i , j = 1 for any
u , v E X , where o ( x ) = 0 for the Dirichlet and Neumann boundary conditions .
Sayfa 496
Obviously , this necessary condition is equivalent to the condition Ker Tzd : = { 0 }
. In fact , the proof of necessity given in ( PY1 ] allows one to obtain a more
general result : if • is an arbitrary very badly approximable function in ( H® + C ) (
Mm ...
Obviously , this necessary condition is equivalent to the condition Ker Tzd : = { 0 }
. In fact , the proof of necessity given in ( PY1 ] allows one to obtain a more
general result : if • is an arbitrary very badly approximable function in ( H® + C ) (
Mm ...
Sayfa 506
VERY BADLY APPROXIMABLE FUNCTIONS In this section we obtain a
necessary and sufficient condition for an admissible infinite matrix function to be
very badly approximable . Let Me Lo ( B ( l2 ) ) . Put ta ( 9 ) = lim t ; ( 0 ) . 3 + 00 As
in the ...
VERY BADLY APPROXIMABLE FUNCTIONS In this section we obtain a
necessary and sufficient condition for an admissible infinite matrix function to be
very badly approximable . Let Me Lo ( B ( l2 ) ) . Put ta ( 9 ) = lim t ; ( 0 ) . 3 + 00 As
in the ...
Kullanıcılar ne diyor? - Eleştiri yazın
Her zamanki yerlerde hiçbir eleştiri bulamadık.
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