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Energy-Dependent Noncommutative Quantum Mechanics

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Energy-Dependent Noncommutative Quantum Mechanics Eur. Phys. J. C (2019) 79:300 https://doi.org/10.1140/epjc/s10052-019-6794-4 Regular Article - Theoretical Physics Energy-dependent noncommutative quantum mechanics Tiberiu Harko1,2,3,a, Shi-Dong Liang1,4,b 1 School of Physics, Sun Yat-Sen University, Guangzhou 510275, People’s Republic of China 2 Department of Physics, Babes-Bolyai University, Kogalniceanu Street, 400084 Cluj-Napoca, Romania 3 Department of Mathematics, University College London, Gower Street, London WC1E 6BT, UK 4 State Key Laboratory of Optoelectronic Material and Technology, and Guangdong Province Key Laboratory of Display Material and Technology, Sun Yat-Sen University, Guangzhou 510275, People’s Republic of China Received: 15 January 2019 / Accepted: 15 March 2019 / Published online: 3 April 2019 © The Author(s) 2019 Abstract We propose a model of dynamical noncommu- 3.1 Probability current and density in the energy- tative quantum mechanics in which the noncommutative dependent potential ............... 7 strengths, describing the properties of the commutation rela- 3.2 The free particle ................. 8 tions of the coordinate and momenta, respectively, are arbi- 3.3 The harmonic oscillator ............. 8 trary energy-dependent functions. The Schrödinger equation 4 Physical mechanisms generating energy-dependent in the energy-dependent noncommutative algebra is derived noncommutative algebras, and their implications .. 9 for a two-dimensional system for an arbitrary potential. The 4.1 The noncommutative algebra of the spacetime resulting equation reduces in the small energy limit to the quantum fluctuations (SQF) model ....... 9 standard quantum mechanical one, while for large energies 4.2 The noncommutative algebra of the energy cou- the effects of the noncommutativity become important. We pling (EC) model ................ 10 investigate in detail three cases, in which the noncommu- 4.3 The noncommutative algebra of the energy oper- tative strengths are determined by an independent energy ator (EO) model ................. 10 scale, related to the vacuum quantum fluctuations, by the 5 Quantum evolution in the spacetime quantum fluctuation particle energy, and by a quantum operator representation, (SQF) energy-dependent noncommutative model ..... 11 respectively. Specifically, in our study we assume an arbi- 5.1 Quantum mechanics of the free particle in the trary power-law energy dependence of the noncommutative SQF model ................... 11 strength parameters, and of their algebra. In this case, in the 5.2 The harmonic oscillator ............. 12 quantum operator representation, the Schrö dinger equation 6 Quantum dynamics in the energy coupling model .. 12 can be formulated mathematically as a fractional differential 6.1 Quantum evolution: the Schrödinger equation .12 equation. For all our three models we analyze the quantum 6.2 Quantum evolution: wave function and energy levels .... 13 evolution of the free particle, and of the harmonic oscillator, 6.3 The case of the free particle ........... 14 respectively. The general solutions of the noncommutative 6.4 The harmonic oscillator ............. 15 Schrödinger equation as well as the expressions of the energy 7 Quantum evolution in the energy operator (EO) levels are explicitly obtained. energy-dependent noncommutative geometry .... 16 7.1 Fractional calculus: a brief review ....... 16 7.2 The fractional Schrödinger equation ...... 17 α = Contents 7.3 The free particle: the case 1 ........ 18 8 Discussions and final remarks ............ 18 1 Introduction ..................... 1 References ........................ 21 2 Energy-dependent noncommutative geometry and algebra ... 5 3 The Schrödinger equation in the energy-dependent noncommutative geometry .............. 7 1 Introduction It is generally believed today that the description of the space- a e-mail: [email protected] time as a manifold M, locally modeled as a flat Minkowski b 3 e-mail: [email protected] space M0 = R × R , may break down at very short dis- 123 300 Page 2 of 22 Eur. Phys. J. C (2019) 79 :300 3 2 tances of the order of the Planck length lP = Gh¯ /c ≈ a − xμ,xν = i Lμν, (2) 1.6 × 10 33 cm, where G, h¯ and c are the gravitational con- h¯ stant, Planck’s constant, and the speed of light, respectively [1]. This assumption is substantiated by a number of argu- where a is a basic length unit, and Lμν are the generators ments, following from quantum mechanical and general rela- of the Lorentz group. In this approach, Lorentz covariance tivistic considerations, which point towards the impossibility is maintained, but the translational invariance is lost. A rig- of an arbitrarily precise location of a physical particle in terms orous mathematical approach to noncommutative geometry of points in spacetime. was introduced in [8–11], by generalizing the notion of a ∗ One of the basic principles of quantum mechanics, Heisen- differential structure to arbitrary C algebras, as well as to berg’s uncertainty principle, requires that a localization x quantum groups and matrix pseudo-groups. This approach in spacetime can be reached by a momentum transfer of the led to an operator algebraic description of noncommutative order of p = h¯ /x, and an energy of the order of E = spacetimes, based entirely on algebras of functions. hc¯ /x [2–4]. On the other hand, the energy E must contain Since at the quantum level noncommutative spacetimes amassm, which, according to Einstein’s general theory do appear naturally when gravitational effects are taken into of relativity, generates a gravitational field. If this gravita- account, their existence must also follow from string theory. tional field is so strong that it can completely screen out from In [12] it was shown that if open strings have allowed end- observations some regions of spacetime, then its size must points on D-branes in a constant B-field background, then be of the order of its Schwarzschild radius R ≈ Gm/c2. the endpoints live on a noncommutative space with the com- Hence we easily find R ≈ GE/c4 = Gh¯ /c3x,giving mutation relations Rx ≈ Gh¯ /c3. Thus the Planck length appears to give the [μ,ν]= θ μν, lower quantum mechanically limit of the accuracy of position x x i (3) measurements [5]. Therefore the combination of the Heisen- θ μν berg uncertainty principle with Einstein’s theory of general where is an antisymmetric constant matrix, with com- −2 relativity leads to the conclusion that at short distances the ponents c-numbers with the dimensionality (length) .More standard concept of space and time may lose any operational generally, a similar relation can also be imposed on the par- meaning. ticle momenta, which generates a noncommutative algebra On the other hand, the very existence of the Planck length in the momentum space of the form requires that the mathematical concepts for high-energy , = η , (short distance) physics have to be modified. This follows pμ pν i μν (4) from the fact that classical geometrical notions and con- η cepts may not be well suited for the description of physical where μν are constants. In [13] noncommutative field phenomena at very short distances. Moreover, some drastic theories with commutator of the coordinates of the form μ, ν = μν ω changes are expected in the physics near the Planck scale, [x x ] i ωx have been studied. By considering a with one important and intriguing effect being the emer- Lorentz tensor, explicit Lorentz invariance is maintained, a gence of the noncommutative structure of the spacetime. The free quantum field theory is not affected. On the other hand, basic idea behind spacetime noncommutativity is very much since invariance under translations is broken, the conserva- inspired by quantum mechanics. A quantum phase space is tion of energy–momentum tensor is violated, and a new law defined by replacing canonical position and momentum vari- expressed by a Poincaré-invariant equation is obtained. The λφ4 ables xμ, pν with Hermitian operators that obey the Heisen- quantum field theory was also considered. It turns out berg commutation relations, that the usual UV divergent terms are still present in this model. Moreover, new type of terms also emerge that are μ ν μν [x , p ]=ih¯ δ . (1) IR divergent, violates momentum conservation and lead to corrections to the dispersion relations. Hence the phase space becomes smeared out, and the The physical implications and the mathematical proper- notion of a point is replaced with that of a Planck cell. The ties of the noncommutative geometry have been extensively , = generalization of commutation relations for the canonical investigated in [14–42]. In the case when pi p j 0, the operators (coordinate-momentum or creation-annihilation noncommutative quantum mechanics goes into the usual one, operators) to non-trivial commutation relations for the coor- described by the non-relativistic Schrödinger equation, dinate operators was performed in [6,7], where it was first ( ˜, ) ψ ( ˜) = ψ ( ˜) , suggested that the coordinates xμ may be noncommutating H x p x E x (5) operators, with the six commutators being given by 123 Eur. Phys. J. C (2019) 79 :300 Page 3 of 22 300 μ μ μν where x˜ = x − (1/2)θ pν [43]. In the presence of a properties of systems with dynamic noncommutativity were constant magnetic field B and an arbitrary central potential considered in [51–58]. V (r), with Hamiltonian A quantum mechanical system on a noncommutative space for which the structure constant is explicitly time- p2 dependent was investigated in [59], in a two-dimensional H = + V (r), (6) 2m space with nonvanishing commutators for the coordinates X, Y and momenta Px , Py given by the operators p, x obey the commutation relations [43] [ , ]= θ( ), , = ( ), X Y i t Px Py i t (11a) 1 2 μ μ e x ,x = iθ, x , pν = ih¯ δν , [p1, p2] = i B. (7) θ(t)(t) c [X, Px ] = Y, Py = ih¯ + i . (11b) 4h¯ Several other types of noncommutativity, extending the Any autonomous Hamiltonian on such a space acquires a canonical one, have also been proposed.
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