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Time-Space Noncommutativity: Quantised Evolutions
Author(s) -
A. P. Balachandran,
T. R. Govindarajan,
Andrey Gomes Martins,
Paulo Teotonio-Sobrinho
Publication year - 2004
Publication title -
journal of high energy physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.998
H-Index - 261
eISSN - 1126-6708
pISSN - 1029-8479
DOI - 10.1088/1126-6708/2004/11/068
Subject(s) - noncommutative geometry , observable , physics , hamiltonian (control theory) , mathematical physics , noncommutative quantum field theory , quantum field theory , quantum mechanics , scattering , space time , modulo , lattice (music) , scattering theory , quantum , classical mechanics , mathematics , discrete mathematics , mathematical optimization , chemical engineering , acoustics , engineering
In previous work, we developed quantum physics on the Moyal plane withtime-space noncommutativity, basing ourselves on the work of Doplicher et al..Here we extend it to certain noncommutative versions of the cylinder,$\mathbb{R}^{3}$ and $\mathbb{R}\times S^{3}$. In all these models, onlydiscrete time translations are possible, a result known before in the first twocases. One striking consequence of quantised time translations is that eventhough a time independent Hamiltonian is an observable, in scatteringprocesses, it is conserved only modulo $\frac{2\pi}{\theta}$, where $\theta$ isthe noncommutative parameter. (In contrast, on a one-dimensional periodiclattice of lattice spacing $a$ and length $L=Na$, only momentum mod$\frac{2\pi}{L}$ is observable (and can be conserved).) Suggestions for furtherstudy of this effect are made. Scattering theory is formulated and an approachto quantum field theory is outlined.Comment: 25 pages, LaTex; minor corrections, references correcte

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