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2016 | OriginalPaper | Buchkapitel

A Star Product for the Volume Form Nambu-Poisson Structure on a Kähler Manifold

verfasst von : Baran Serajelahi

Erschienen in: Lie Theory and Its Applications in Physics

Verlag: Springer Singapore

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Abstract

Every symplectic (1-plectic) manifold \((M,\omega )\) of dimension 2n may be regarded as a \((2n-1)\)-plectic manifold by wedging together n copies of the symplectic 2-form to get the Liouville volume form. This volume form defines a Nambu-Poisson structure \(\{.,\dots ,.\}_{NP}\) of order 2n on \(C^{\infty }(M)\). When the manifold is Kähler, the Kähler structure can be used to define a star product (known as the Berezin-Toeplitz star product) for the Poisson algebra \(C^{\infty }(M)\). For a Kähler manifold \((M,\omega )\) we define a higher order analogue of the Berezin-Toeplitz star product on the Nambu-Poisson algebra \((C^{\infty }(M),\{.,\dots ,.\}_{NP})\).

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Fußnoten
1
These properties are known as the axioms of quantization, the exact axioms that are chosen depend somewhat on the mathematical setting. For a discussion of the reasons behind this and of the axioms that are used in the Kähler setting see [3].
 
2
\(const(\hbar )\) denotes a constant that depends on \(\hbar \).
 
3
Because of the role played by the operators on the Hilbert space \(\mathscr {H}\).
 
4
If the bracket \({\{f,g\}}_t\) converges for all t and for all \(f,g\in C^{\infty }(M)\) we would be in the most ideal situation, of course this will depend on the details of the definition of the \(C_i\).
 
5
in the sense of [5].
 
6
This principal says that the classical theory should be recovered in the limit \(t\rightarrow 0\).
 
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Metadaten
Titel
A Star Product for the Volume Form Nambu-Poisson Structure on a Kähler Manifold
verfasst von
Baran Serajelahi
Copyright-Jahr
2016
Verlag
Springer Singapore
DOI
https://doi.org/10.1007/978-981-10-2636-2_49