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SUMMARY:Andrei Smilga
DTSTART:20220518T162000Z
DTEND:20220518T180000Z
DTSTAMP:20260423T024831Z
UID:GDEq/66
DESCRIPTION:Title: <a href="https://researchseminars.org/talk/GDEq/66/">No
 ncommutative quantum mechanical systems associated with Lie algebras</a>\n
 by Andrei Smilga as part of Geometry of differential equations seminar\n\n
 \nAbstract\nWe consider quantum mechanics on the noncommutative spaces cha
 racterized by the commutation relations\n$$ [x_a\, x_b] \\ =\\ i\\theta f_
 {abc} x_c\\\,\, $$\nwhere $f_{abc}$ are the structure constants of a Lie a
 lgebra. We note that this problem can be reformulated as an ordinary quant
 um problem in a commuting {\\it momentum} space. The coordinates are then 
 represented as linear differential operators $\\hat x_a = -i \\hat D_a = -
 iR_{ab} (p)\\\, \\partial /\\partial p_b $. Generically\, the matrix $R_{a
 b}(p)$ represents a certain infinite series over the deformation parameter
  $\\theta$: $R_{ab} = \\delta_{ab} + \\ldots$. The deformed Hamiltonian\, 
 $\\hat H \\ =\\ - \\frac 12  \\hat D_a^2\\\,\, $ describes the motion alon
 g the corresponding group manifolds with the characteristic size of order 
 $\\theta^{-1}$. Their metrics are also expressed into  certain infinite se
 ries in $\\theta$.\n\nFor the algebras $su(2)$ and $u(2)$\, it has been po
 ssible to represent the operators $\\hat x_a$ in a simple finite form. A b
 yproduct of our study are new nonstandard formulas for the metrics on $SU(
 2) \\equiv S^3$ and on $SO(3)$.\n
LOCATION:https://researchseminars.org/talk/GDEq/66/
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