Abstract:A particle system with a (2+1)D exotic Newton-Hooke symmetry is constructed by the method of nonlinear realization. It has three essentially different phases depending on the values of the two central charges. The subcritical and supercritical phases (describing 2D isotropic ordinary and exotic oscillators) are separated by the critical phase (one-mode oscillator), and are related by a duality transformation. In the flat limit, the system transforms into a free Galilean exotic particle on the noncommutative pl… Show more
“…The system displays three different phases depending on the values of the parameters [11]. The reduced phase space description reveals a symplectic structure similar to that of Landau problem in the non-commutative plane [12,13].…”
Section: Motivation and Resultsmentioning
confidence: 90%
“…In the non-relativistic limit X a ± → X a ± /ω, µ ± → ω 2 µ ± , the Lagrangian takes the NewtonHooke form [11] up to a divergent total derivative, and the equations of motion (18) become those of two harmonic oscillators.…”
We consider the dynamics of a particle of mass M and spin J in AdS 3 . The study reveals the presence of different dynamical sectors depending on the relative values of M , J and the
“…The system displays three different phases depending on the values of the parameters [11]. The reduced phase space description reveals a symplectic structure similar to that of Landau problem in the non-commutative plane [12,13].…”
Section: Motivation and Resultsmentioning
confidence: 90%
“…In the non-relativistic limit X a ± → X a ± /ω, µ ± → ω 2 µ ± , the Lagrangian takes the NewtonHooke form [11] up to a divergent total derivative, and the equations of motion (18) become those of two harmonic oscillators.…”
We consider the dynamics of a particle of mass M and spin J in AdS 3 . The study reveals the presence of different dynamical sectors depending on the relative values of M , J and the
“…This is due to the fact that the Newton-Hooke group can be obtained from the (A)dS groups as the non-relativistic limit with the velocity of light c going to infinity and the cosmological constant Λ going to zero while keeping c 2 Λ finite, see e.g. [23] and for recent work [24]. The conformal invariance of the relativistic action (23) independently of the power p may be interesting in the search of black hole solutions.…”
In this paper two things are done. We first prove that an arbitrary power p of the Schrödinger Lagrangian in arbitrary dimension always enjoys the non-relativistic conformal symmetry. The implementation of this symmetry on the dynamical field involves a phase term as well as a conformal factor that depends on the dimension and on the exponent. This non-relativistic conformal symmetry is shown to have its origin on the conformal isometry of the power p of the Klein-Gordon Lagrangian in one higher dimension which is related to the phase of the complex scalar field.
“…In recent years noncommutative geometry [1,2,3,4,5,6,7,8,9,10] has received much attention due to the fact that spacetime may be noncommutative at very small length scale. For detail study on noncommutative space see the list of Refs.…”
Isotropic oscillator on a plane is discussed where both the coordinate and momentum space are considered to be noncommutative. We also discuss the symmetry properties of the oscillator for three separate cases when both the noncommutative parameters Θ and Θ satisfy specific relations. We compare the Landau problem with the isotropic oscillator on noncommutative space and obtain a relation between the two noncommutative parameters with the magnetic field of the Landau problem.
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