Linear Operators: Spectral theory |
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Page 1241
Nelson Dunford, Jacob T. Schwartz, William G. Bade, Robert G. Bartle. then ,
letting 2n = Xn - Yn , we have limn _ 02n = 0 and limm . n - > 2m 2n | + = 0 .
Consequently there is a number M such that Izml + SM , m = 1 , 2 , . . . . Moreover
, given ε ...
Nelson Dunford, Jacob T. Schwartz, William G. Bade, Robert G. Bartle. then ,
letting 2n = Xn - Yn , we have limn _ 02n = 0 and limm . n - > 2m 2n | + = 0 .
Consequently there is a number M such that Izml + SM , m = 1 , 2 , . . . . Moreover
, given ε ...
Page 1383
With boundary conditions A , the eigenvalues are consequently to be determined
from the equation sin vā = 0 . Consequently , in Case A , the eigenvalues , are the
numbers of the form ( na ) , n 21 ; in Case C , the numbers { ( n + ) } ? , n 20 .
With boundary conditions A , the eigenvalues are consequently to be determined
from the equation sin vā = 0 . Consequently , in Case A , the eigenvalues , are the
numbers of the form ( na ) , n 21 ; in Case C , the numbers { ( n + ) } ? , n 20 .
Page 1387
Consequently , by Theorem 3 . 16 , the resolvent R ( 2 ; T ) is an integral operator
with the kernel In > O , Il > 0 , 1 sin văs ( cos Vīt + i sin Vīt ) 1 sat , V sin Vāt ( cos
Vīsti sin Văs ) < s , va sin Văs ( cos vă - i sin Vāt ) - s < t , V sin Vāt ( cos Vās i sin ...
Consequently , by Theorem 3 . 16 , the resolvent R ( 2 ; T ) is an integral operator
with the kernel In > O , Il > 0 , 1 sin văs ( cos Vīt + i sin Vīt ) 1 sat , V sin Vāt ( cos
Vīsti sin Văs ) < s , va sin Văs ( cos vă - i sin Vāt ) - s < t , V sin Vāt ( cos Vās i sin ...
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Contents
IX | 859 |
Eigenvalues and Eigenvectors | 903 |
Spectral Representation | 911 |
Copyright | |
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