## Linear Operators, Part 2 |

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Page 1290

Then the leading

while if n is odd , an is pure imaginary . ... 2 ( –196 ) az ( t ) ace ) ( 12 ) ( ) ' [ 6 ) 640

) +0,01 ( 4 ) ] ( ) [ ( n - 1 ) / 2 ] dii +1 Σ j = 0 where the

real .

Then the leading

**coefficient**in q * is ( -1 ) " ān ; thus , if n is even , an is real ,while if n is odd , an is pure imaginary . ... 2 ( –196 ) az ( t ) ace ) ( 12 ) ( ) ' [ 6 ) 640

) +0,01 ( 4 ) ] ( ) [ ( n - 1 ) / 2 ] dii +1 Σ j = 0 where the

**coefficients**a ; and b ; arereal .

Page 1486

Nelson Dunford, Jacob T. Schwartz, William G. Bade, Robert G. Bartle. Equations

with periodic

theory of solid crystals ) have a number of interesting and important properties .

Nelson Dunford, Jacob T. Schwartz, William G. Bade, Robert G. Bartle. Equations

with periodic

**coefficients**( which are fundamental in the quantum - mechanicaltheory of solid crystals ) have a number of interesting and important properties .

Page 1730

For partial differential operators in R with

may state the following analogue of the Gårding inequality , Lemma 10. As to its

proof , we need only remark that since , as has been pointed out above , only the

...

For partial differential operators in R with

**coefficients**belonging to C ( R ) , wemay state the following analogue of the Gårding inequality , Lemma 10. As to its

proof , we need only remark that since , as has been pointed out above , only the

...

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### Contents

BAlgebras | 859 |

Bounded Normal Operators in Hilbert Space | 887 |

Miscellaneous Applications | 937 |

Copyright | |

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