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75 sonuçtan 1-3 arası sonuçlar
Sayfa 467
Next , we denote by X either the Sobolev spaces H ] ( 12 ) if Bu = u , or H1 ( 12 )
in the case of the Neumann condition or ... ( x ) dx + o ( s ) u ( s ) v ( s ) ds JΩ 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 ] ( 12 ) if Bu = u , or H1 ( 12 )
in the case of the Neumann condition or ... ( x ) dx + o ( s ) u ( s ) v ( s ) ds JΩ 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 Tzo = { 0 } .
In fact , the proof of necessity given in ( PY1 ] allows one to obtain a more general
result : if 0 is an arbitrary very badly approximable function in ( HR + C ) ( Mm ...
Obviously , this necessary condition is equivalent to the condition Ker Tzo = { 0 } .
In fact , the proof of necessity given in ( PY1 ] allows one to obtain a more general
result : if 0 is an arbitrary very badly approximable function in ( HR + C ) ( Mm ...
Sayfa 506
9 ) , then lim ; S ; ( HR ) = 0 , and so Hộ is compact . 86 . 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 .
9 ) , then lim ; S ; ( HR ) = 0 , and so Hộ is compact . 86 . 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 .
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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 | |
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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