2013
DOI: 10.1088/1751-8113/46/8/085204
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Spectral triplets, statistical mechanics and emergent geometry in non-commutative quantum mechanics

Abstract: We show that when non-commutative quantum mechanics is formulated on the Hilbert space of Hilbert-Schmidt operators acting on a classical configuration space, spectral triplets as introduced by Connes in the context of non-commutative geometry arise naturally. A distance function as defined by Connes can therefore also be introduced. We proceed to give a simple algorithm to compute this function in generic situations. Using this we compute the distance between pure and mixed states on quantum Hilbert space and… Show more

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Cited by 14 publications
(58 citation statements)
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“…Since statistical mechanics plays an important role in understanding a system consisting of large number of particles, it is reasonable to assume that a study of statistical mechanics of these compact systems in the background of a non-commutative spacetime will be a viable option to understand the Planck scale physics. The effect of Planck scale physics, especially due to the presence of minimal length, in statistical mechanics has been reported by many in the literature [2][3][4][5][6][7][8][9]. Compact stars appears to be a potential source to study the effects of non-commutativity on statistical mechanics, due to its accessibility for observation.…”
Section: Introductionmentioning
confidence: 95%
See 1 more Smart Citation
“…Since statistical mechanics plays an important role in understanding a system consisting of large number of particles, it is reasonable to assume that a study of statistical mechanics of these compact systems in the background of a non-commutative spacetime will be a viable option to understand the Planck scale physics. The effect of Planck scale physics, especially due to the presence of minimal length, in statistical mechanics has been reported by many in the literature [2][3][4][5][6][7][8][9]. Compact stars appears to be a potential source to study the effects of non-commutativity on statistical mechanics, due to its accessibility for observation.…”
Section: Introductionmentioning
confidence: 95%
“…, which has the correct dimension and reduces to ÿ in the commutative limit a 0  . The possibility of such a modification was studied in [7].…”
Section: Degeneracy Pressure and Hydrostatic Equilibrium In κ-Spacetimentioning
confidence: 99%
“…This non-Voros state will be useful if we are interested in computing Connes' spectral distance between a pair of such "points " i.e. pure states (see for example [11] and references there-in). However, since our interest is to compute the thermal correlation function between a pair of identical particles in Voros states, we shall not be concerned with such states in the rest of the paper.…”
Section: Computation Of Variance Matrix In the Non-commutative Casmentioning
confidence: 99%
“…In particular the Voros basis turns out to be a coherent state |z) representing a maximally localized state in the non-commutative plane. Indeed, it has been shown recently [11] that one can compute the spectral distance, a la Connes [12] between a pair of neighboring states |z) V and |z + dz) V to get a Euclidean geometry: d 2 (|z), |z + dz)) = 2θ 3 dzdz. But such a distance function cannot be assigned between the pair of neighboring states | x) M and | x + d x) M corresponding to the Moyal basis.…”
Section: Introductionmentioning
confidence: 99%
“…Here we have introduced the density matrix ρ z ∈ H q , as viewed from H c and can be associated with the pure state ω ρz corresponding to the * -algebra H q = A M and defined as a linear functional on A M : ω ρz (a) ∈ C of norm one. As explained in detail in [13], here too we shall be working with normal states, so that the states can be represented by density matrices : ω ρz (a) = Tr Hc (ρ z a). For brevity, therefore, the states will be denoted just by density matrices themselves as ρ(a) = Tr (ρa).…”
Section: Introductionmentioning
confidence: 99%