Seminar talk, 18 May 2022: Difference between revisions

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| abstract = We consider quantum mechanics on the noncommutative spaces characterized by the commutation relations
| abstract = We consider quantum mechanics on the noncommutative spaces characterized by the commutation relations


<math> [x_a, x_b] \ =\ i\theta f_{abc} x_c\,,</math>
&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;<math> [x_a, x_b] \ =\ i\theta f_{abc} x_c\,,</math>


where <math>f_{abc}</math> are the structure constants of a Lie algebra. We note that this problem can be reformulated as an ordinary quantum problem in a commuting {\it momentum} space. The coordinates are then represented as linear differential operators <math>\hat x_a = -i \hat D_a = -iR_{ab} (p)\, \partial /\partial p_b </math>. Generically, the matrix <math>R_{ab}(p)</math> represents a certain infinite series over the deformation parameter <math>\theta</math>: <math>R_{ab} = \delta_{ab} + \ldots</math>. The deformed Hamiltonian, <math>\hat H \ =\ - \frac 12  \hat D_a^2\,, </math> describes the motion along the corresponding group manifolds with the characteristic size of order <math>\theta^{-1}</math>. Their metrics are also expressed into  certain infinite series in <math>\theta</math>.
where <math>f_{abc}</math> 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 <math>\hat x_a = -i \hat D_a = -iR_{ab} (p)\, \partial /\partial p_b </math>. Generically, the matrix <math>R_{ab}(p)</math> represents a certain infinite series over the deformation parameter <math>\theta</math>: <math>R_{ab} = \delta_{ab} + \ldots</math>. The deformed Hamiltonian, <math>\hat H \ =\ - \frac 12  \hat D_a^2\,, </math> describes the motion along the corresponding group manifolds with the characteristic size of order <math>\theta^{-1}</math>. Their metrics are also expressed into  certain infinite series in <math>\theta</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>.
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 =  
| video = https://video.gdeq.org/GDEq-zoom-seminar-20220518-Andrei_Smilga.mp4
| slides =  
| slides =  
| references = {{arXiv|2204.08705}}
| references = {{arXiv|2204.08705}}
| 79YY-MM-DD = 7977-94-81
| 79YY-MM-DD = 7977-94-81
}}
}}

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