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Sayfa 24
Then for the set of primitive representations we have the partition ( 1.18 ) pbQ.A =
pbQ.A ( I + ) + J + ( summation is over all proper classes J + of matrices with
determinant ( 1.8 ) ; thus , the partition is finite ) . $ 2 . THE ORBITS OF PRIMITIVE
...
Then for the set of primitive representations we have the partition ( 1.18 ) pbQ.A =
pbQ.A ( I + ) + J + ( summation is over all proper classes J + of matrices with
determinant ( 1.8 ) ; thus , the partition is finite ) . $ 2 . THE ORBITS OF PRIMITIVE
...
Sayfa 25
If we fix a class I + = { G } + and trace the relationship between the
representations b in ( 1.4 ) and the block C of the matrix QB , we may obtain a
finer partition of the representations pb ( I + ) associated with the class It . 2.1 . Let
Bbg be the ...
If we fix a class I + = { G } + and trace the relationship between the
representations b in ( 1.4 ) and the block C of the matrix QB , we may obtain a
finer partition of the representations pb ( I + ) associated with the class It . 2.1 . Let
Bbg be the ...
Sayfa 35
By analogy with ( 1.18 ) , we have the following finite partition : ( 4.18 ) EbQ , A ( 1
, ' , M , { G } + ) ; Arto M A { G } + here { G } + ranges over all classes of matrices G
with determinant | G | = a -md / [ A1 ] , where a , is the level of A1 = A [ M- ' ) ( cf.
By analogy with ( 1.18 ) , we have the following finite partition : ( 4.18 ) EbQ , A ( 1
, ' , M , { G } + ) ; Arto M A { G } + here { G } + ranges over all classes of matrices G
with determinant | G | = a -md / [ A1 ] , where a , is the level of A1 = A [ M- ' ) ( cf.
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İçindekiler
REPRESENTATION OF A FORM | 17 |
10 The automorphism groups of discriminant forms | 59 |
12 A general formula for the weight of representations | 65 |
Telif Hakkı | |
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apply arbitrary assume assumptions asymptotics bases basis belongs boundary bounded classical coefficients coincides compact complex condition Consequently consider constant construction contains continuous convex corresponding curve decomposition defined definition denote depends described determined differential dimension direct discrete domain eigenfunctions eigenvalues elements English equal equation estimate example exists factor field finite fixed formula function given gives graph implies independent inequality integral introduce invariant lattice Lemma limit linear manifolds Math Mathematical matrix measure method Moreover observe obtain operator orbits particular periodic perturbation Phys positive potential present problem Proof properties Proposition prove quantum relation Remark representations respect restriction result satisfies similar smooth solutions space spectral spectrum statement Subsection sufficiently surface symbol Theorem theory transformation transl unique values vector