By André Unterberger

ISBN-10: 3540779108

ISBN-13: 9783540779100

ISBN-10: 3540779116

ISBN-13: 9783540779117

This quantity introduces a completely new pseudodifferential research at the line, the competition of which to the standard (Weyl-type) research may be stated to mirror that, in illustration concept, among the representations from the discrete and from the (full, non-unitary) sequence, or that among modular kinds of the holomorphic and alternative for the standard Moyal-type brackets. This pseudodifferential research depends on the one-dimensional case of the lately brought anaplectic illustration and research, a competitor of the metaplectic illustration and traditional analysis.

Besides researchers and graduate scholars drawn to pseudodifferential research and in modular types, the e-book can also entice analysts and physicists, for its innovations making attainable the transformation of creation-annihilation operators into automorphisms, concurrently altering the standard scalar product into an indefinite yet nonetheless non-degenerate one.

**Read Online or Download Alternative Pseudodifferential Analysis: With an Application to Modular Forms PDF**

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**Extra resources for Alternative Pseudodifferential Analysis: With an Application to Modular Forms**

**Example text**

57) when ε = 0, this is a representation taken from the complementary series of SL(2, R); when ε = 1, it is a signed version, non unitarizable, of the same. More details can be found in [38, Sect. 2], with the same notation. 12. Under the map u → ((Q u)0 , (Q u)1 ), the anaplectic representation transfers to the representation (πˆ− 1 ,0 , πˆ 1 ,1 ). 2 2 Proof. Though it is contained in the above given reference, let us at least give a short indication about one of the possible proofs of the proposition.

6 should continue to hold. 4 is still valid. Let us set (the first item is just a notational convenience) δ0m+1 = 1 ∂ , π ∂z δ1m+1 = 1 ∂ (z + m + 1). 36) 44 3 The One-Dimensional Alternative Pseudodifferential Analysis What we want to do is to define B = Opasc (i w) ¯ α 1 ∂ π ∂w β fm−α −β as B = [Q, [Q, . . [P, [P, . . , Opasc m−α −β ( f m−α −β )] . . ] . . 37) where the number of Q ’s is α and the number of P ’s is β . 6, this equation is correct in the case when fm−α −β ∈ Sm (R2 ). 34), setting χm−α −β +1 = Θm−α −β hm−α −β and considering an arbitrary sequence (ε1 , .

Finding a symbolic 2 calculus of operators, covariant under the anaplectic representation, quite appropriately started from the consideration of a calculus of operators based on the use of Hi as a temporary phase space. The corresponding quantization program, including a study of the sharp composition of symbols, was implemented in [34]; the quantizing map, in that case, had independently been obtained in [22]. In the present investigations, special consideration is attached to the discrete part only of the decomposition of L2 (Hi ).

### Alternative Pseudodifferential Analysis: With an Application to Modular Forms by André Unterberger

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