Pith. sign in

Propagators in Polymer Quantum Mechanics

1 Pith paper cite this work. Polarity classification is still indexing.

1 Pith paper citing it
abstract

Polymer Quantum Mechanics is based on some of the techniques used in the loop quantization of gravity that are adapted to describe systems possessing a finite number of degrees of freedom. It has been used in two ways: on one hand it has been used to represent some aspects of the loop quantization in a simpler context, and, on the other, it has been applied to each of the infinite mechanical modes of other systems. Indeed, this polymer approach was recently implemented for the free scalar field propagator. In this work we compute the polymer propagators of the free particle and a particle in a box; amusingly, just as in the non polymeric case, the one of the particle in a box may be computed also from that of the free particle using the method of images. We verify the propagators hereby obtained satisfy standard properties such as: consistency with initial conditions, composition and Green's function character. Furthermore they are also shown to reduce to the usual Schr\"odinger propagators in the limit of small parameter $\mu_0$, the length scale introduced in the polymer dynamics and which plays a role analog of that of Planck length in Quantum Gravity.

citation-role summary

background 1

citation-polarity summary

fields

gr-qc 1

years

2024 1

verdicts

CONDITIONAL 1

roles

background 1

polarities

background 1

representative citing papers

Unitary evolution and cosmic acceleration in Loop Quantum Cosmology

gr-qc · 2024-12-10 · conditional · novelty 5.0

For any weight parameter in the improved-dynamics LQC Hamiltonian, negative weights give essentially self-adjoint operators, while positive weights require U(1)-labeled self-adjoint extensions, which the paper implements in a propagator.

citing papers explorer

Showing 1 of 1 citing paper.

  • Unitary evolution and cosmic acceleration in Loop Quantum Cosmology gr-qc · 2024-12-10 · conditional · none · ref 37 · internal anchor

    For any weight parameter in the improved-dynamics LQC Hamiltonian, negative weights give essentially self-adjoint operators, while positive weights require U(1)-labeled self-adjoint extensions, which the paper implements in a propagator.