Linear Operators: Spectral theory |
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Page 977
G ( u , v ) = lim R + - 2n Jo f ( r ) rdr Jo By substituting O ' for 0 - 9 + ( / 2 ) and
simplifying , it is seen that PR G ( u , v ) = Glu , v ) - ke - i ay sim Soporar jo ika - si
in evapo . ( r ) rdr e i ( ne ' - ( rs sin 0 ' ) ) JA ' . 21 ? ) " lim R f JO JO Now the
Bessel ...
G ( u , v ) = lim R + - 2n Jo f ( r ) rdr Jo By substituting O ' for 0 - 9 + ( / 2 ) and
simplifying , it is seen that PR G ( u , v ) = Glu , v ) - ke - i ay sim Soporar jo ika - si
in evapo . ( r ) rdr e i ( ne ' - ( rs sin 0 ' ) ) JA ' . 21 ? ) " lim R f JO JO Now the
Bessel ...
Page 1154
Since it is clear that ( 2 ) = Ex£ , what will be proved then , is that 2 ( 2 ) ( E ) = c (
2x2 ) ( E ) , Ee L ( 2 ) , for some constant c independent of E . This condition ( i ) ,
as is seen from Corollary III . 11 . 6 , is a consequence of the assertion that 2 ( 2 )
...
Since it is clear that ( 2 ) = Ex£ , what will be proved then , is that 2 ( 2 ) ( E ) = c (
2x2 ) ( E ) , Ee L ( 2 ) , for some constant c independent of E . This condition ( i ) ,
as is seen from Corollary III . 11 . 6 , is a consequence of the assertion that 2 ( 2 )
...
Page 1324
Nelson Dunford, Jacob T. Schwartz, William G. Bade, Robert G. Bartle. it is seen
from Lemma 4 ( c ) that the jump equations are equivalent to the relation un 10 ) =
349P 4 . 000 – £240F 44 , 45 ) , 16c + ( ) . an - 1 j = 1 Define a ; = ki , i = 1 , . . .
Nelson Dunford, Jacob T. Schwartz, William G. Bade, Robert G. Bartle. it is seen
from Lemma 4 ( c ) that the jump equations are equivalent to the relation un 10 ) =
349P 4 . 000 – £240F 44 , 45 ) , 16c + ( ) . an - 1 j = 1 Define a ; = ki , i = 1 , . . .
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Contents
IX | 859 |
Eigenvalues and Eigenvectors | 903 |
Spectral Representation | 911 |
Copyright | |
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