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This preprint introduces "polymer quantum mechanics," a quantization scheme derived from loop quantum gravity that utilizes a discrete topology for configuration spaces rather than the conventional Schrödinger representation. The authors explicitly derive exact energy eigenvalues for particles on compact domains like rings and boxes, demonstrating how these discrete states converge to standard continuum counterparts in the limit. For researchers in foundational quantum physics, this work offers a rigorous mathematical framework for exploring alternative Hilbert space constructions on finite graphs.
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Polymer quantum mechanics on compact configuration spaces

arXiv2 min read

arXiv:2606.06019v1 Announce Type: new Abstract: "Polymer quantum mechanics" is the name given to a quantization scheme inspired by loop quantum gravity in which the configuration space of the theory is chosen to have a discrete topology. Polymer quantization yields a representation of the canonical commutation relations that is genuinely distinct from the conventional "Schr\"odinger" representation. In this paper, we summarize the main features of polymer quantum mechanics and investigate in detail the polymer quantization of systems with configuration spaces that are classically compact. We show explicitly how using the standard construction of polymer states leads to a Hilbert space of states defined on a finite graph of points. By way of example, we find the exact energy eigenvalues and eigenfunctions for a particle on a ring and a particle in a box defined on such lattices, and discuss similarities and differences from standard Schr\"odinger quantum mechanics. We also explore the continuum limit of states in these systems, and demonstrate in detail how the exact eigenfunctions in the position representation approach their continuum counterparts.

Abstract:"Polymer quantum mechanics" is the name given to a quantization scheme inspired by loop quantum gravity in which the configuration space of the theory is chosen to have a discrete topology. Polymer quantization yields a representation of the canonical commutation relations that is genuinely distinct from the conventional "Schrödinger" representation. In this paper, we summarize the main features of polymer quantum mechanics and investigate in detail the polymer quantization of systems with configuration spaces that are classically compact. We show explicitly how using the standard construction of polymer states leads to a Hilbert space of states defined on a finite graph of points. By way of example, we find the exact energy eigenvalues and eigenfunctions for a particle on a ring and a particle in a box defined on such lattices, and discuss similarities and differences from standard Schrödinger quantum mechanics. We also explore the continuum limit of states in these systems, and demonstrate in detail how the exact eigenfunctions in the position representation approach their continuum counterparts.

arXiv:2606.06019 [quant-ph]

(or arXiv:2606.06019v1 [quant-ph] for this version)

https://doi.org/10.48550/arXiv.2606.06019 Focus to learn more arXiv-issued DOI via DataCite (pending registration)

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Full text under the publisher's open licence · 259 words

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