Seminar talk, 18 May 2022: Difference between revisions
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For the algebras <math>su(2)</math> and <math>u(2)</math>, it has been possible to represent the operators <math>\hat x_a</math> in a simple finite form. A byproduct of our study are new nonstandard formulas for the metrics on <math>SU(2) \equiv S^3</math> and on <math>SO(3)</math>. | For the algebras <math>su(2)</math> and <math>u(2)</math>, it has been possible to represent the operators <math>\hat x_a</math> in a simple finite form. A byproduct of our study are new nonstandard formulas for the metrics on <math>SU(2) \equiv S^3</math> and on <math>SO(3)</math>. | ||
| video = https://video.gdeq. | | video = https://video.gdeq.org/GDEq-zoom-seminar-20220518-Andrei_Smilga.mp4 | ||
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| references = {{arXiv|2204.08705}} | | references = {{arXiv|2204.08705}} | ||
| 79YY-MM-DD = 7977-94-81 | | 79YY-MM-DD = 7977-94-81 | ||
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Latest revision as of 08:40, 4 January 2025
Speaker: Andrei Smilga
Title: Noncommutative quantum mechanical systems associated with Lie algebras
Abstract:
We consider quantum mechanics on the noncommutative spaces characterized by the commutation relations
where are the structure constants of a Lie algebra. We note that this problem can be reformulated as an ordinary quantum problem in a commuting momentum space. The coordinates are then represented as linear differential operators . Generically, the matrix represents a certain infinite series over the deformation parameter : . The deformed Hamiltonian, describes the motion along the corresponding group manifolds with the characteristic size of order . Their metrics are also expressed into certain infinite series in .
For the algebras and , it has been possible to represent the operators in a simple finite form. A byproduct of our study are new nonstandard formulas for the metrics on and on .
Video
References:
arXiv:2204.08705