Repulsively Bound Hadrons in a $\mathbb{Z}_2$ Lattice Gauge Theory

Fuente: arXiv
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Autori principali: Roy, Sayak Guha, Sharma, Vaibhav, Xu, Kaidi, Borla, Umberto, Halimeh, Jad C., Hazzard, Kaden R. A.
Natura: Preprint
Pubblicazione: 2025
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author Roy, Sayak Guha
Sharma, Vaibhav
Xu, Kaidi
Borla, Umberto
Halimeh, Jad C.
Hazzard, Kaden R. A.
author_facet Roy, Sayak Guha
Sharma, Vaibhav
Xu, Kaidi
Borla, Umberto
Halimeh, Jad C.
Hazzard, Kaden R. A.
contents The $\mathbb{Z}_2$ lattice gauge theory is a paradigmatic model that exhibits gauge-field-mediated-confinement of pairs of particles into mesons, drawing connections to quantum chromodynamics. In the absence of any additional attractive interactions between particles, mesons are not known to bind in this model. Here, we show that resonant pair-production terms give rise to two separate mechanisms to form stable ``hadron'' bound states of two mesons: either induced by an effective attractive interaction, or a new dynamical binding mechanism induced by an effective repulsion. The repulsively bound hadron is a high-energy state stabilized by being energetically separated from the two-meson continuum through quantum fluctuations of the gauge fields. We study the dynamical formation of this bound state starting from local excitations. We use matrix product state techniques based on the time-evolving block decimation algorithm to perform our numerical simulations and analyze the effect of model parameters on hadron formation. Furthermore, we derive an effective model that explains its formation. Our findings are amenable to experimental observation on modern quantum hardware such as superconducting qubits, trapped ions, and Rydberg atom arrays.
format Preprint
id arxiv_https___arxiv_org_abs_2510_23618
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Repulsively Bound Hadrons in a $\mathbb{Z}_2$ Lattice Gauge Theory
Roy, Sayak Guha
Sharma, Vaibhav
Xu, Kaidi
Borla, Umberto
Halimeh, Jad C.
Hazzard, Kaden R. A.
High Energy Physics - Lattice
Quantum Gases
High Energy Physics - Phenomenology
Quantum Physics
The $\mathbb{Z}_2$ lattice gauge theory is a paradigmatic model that exhibits gauge-field-mediated-confinement of pairs of particles into mesons, drawing connections to quantum chromodynamics. In the absence of any additional attractive interactions between particles, mesons are not known to bind in this model. Here, we show that resonant pair-production terms give rise to two separate mechanisms to form stable ``hadron'' bound states of two mesons: either induced by an effective attractive interaction, or a new dynamical binding mechanism induced by an effective repulsion. The repulsively bound hadron is a high-energy state stabilized by being energetically separated from the two-meson continuum through quantum fluctuations of the gauge fields. We study the dynamical formation of this bound state starting from local excitations. We use matrix product state techniques based on the time-evolving block decimation algorithm to perform our numerical simulations and analyze the effect of model parameters on hadron formation. Furthermore, we derive an effective model that explains its formation. Our findings are amenable to experimental observation on modern quantum hardware such as superconducting qubits, trapped ions, and Rydberg atom arrays.
title Repulsively Bound Hadrons in a $\mathbb{Z}_2$ Lattice Gauge Theory
topic High Energy Physics - Lattice
Quantum Gases
High Energy Physics - Phenomenology
Quantum Physics
url https://arxiv.org/abs/2510.23618