AI summary · arXiv: 2207.12930v1 · cond-mat.quant-gas

Continuous Symmetry Breaking in a Two-dimensional Rydberg Array

Cheng Chen, Guillaume Bornet, Marcus Bintz, Gabriel Emperauger, Lucas Leclerc, Vincent S. Liu, Pascal Scholl, Daniel Barredo,

and 8 more authorsJohannes Hauschild, Shubhayu Chatterjee, Michael Schuler, Andreas M. Laeuchli, Michael P. Zaletel, Thierry Lahaye, Norman Y. Yao, Antoine Browaeys

Original paper · DOI Submitted to arXiv on 26 Jul. 2022 18 pages, 3 figures in main text, 9 figures in supplemental methods License: NONEXCLUSIVE-DISTRIB 1.0

The essentials

  • Spontaneous symmetry breaking is a fundamental concept in the classification of phases of matter and their transitions
  • It occurs when a system with many interacting components aligns its behavior across large scales, resulting in the emergence of new properties
  • The nature of the underlying symmetry being broken determines the qualitative characteristics of the phase
  • This study focuses on continuous symmetry breaking, which is governed by Goldstone's theorem
  • Continuous symmetry breaking predicts the existence of gapless modes that mediate power-law correlations
  • The researchers utilize a two-dimensional dipolar XY model implemented in a Rydberg quantum simulator to investigate this phenomenon
  • They demonstrate adiabatic preparation of correlated low-temperature states for both the XY ferromagnet and XY antiferromagnet within this system
  • Long-range XY order in ferromagnetic systems is characterized, made possible due to the long-range dipolar interaction present
  • This research complements recent studies utilizing Rydberg-blockade mechanism for Ising-type interactions with discrete spin rotation symmetries
  • By utilizing a programmable quantum simulator, this work opens up avenues for exploring many-body physics associated with XY interactions.

Key points written by AI: they may contain errors, check them against the paper.

AI-generated keywords: Spontaneous Symmetry Breaking Goldstone's Theorem Rydberg Quantum Simulator XY Interactions Programmable Quantum Simulation

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  • Original abstract
Spontaneous symmetry breaking is a fundamental concept in the classification of phases of matter and their transitions. It occurs when a system with many interacting components aligns its behavior across large scales, resulting in the emergence of new properties. The nature of the underlying symmetry being broken determines the qualitative characteristics of the phase. This study focuses on continuous symmetry breaking, which is governed by Goldstone's theorem. Unlike discrete symmetry breaking, continuous symmetry breaking predicts the existence of gapless modes that mediate power-law correlations. To investigate this phenomenon, the researchers utilize a two-dimensional dipolar XY model implemented in a Rydberg quantum simulator. The team demonstrates the adiabatic preparation of correlated low-temperature states for both the XY ferromagnet and XY antiferromagnet within this system. In particular, they characterize the presence of long-range XY order in the ferromagnetic case, which is only possible due to the long-range dipolar interaction present. This work complements recent studies that have utilized the Rydberg-blockade mechanism to realize Ising-type interactions with discrete spin rotation symmetries. By utilizing a programmable quantum simulator, this research opens up avenues for exploring the many-body physics associated with XY interactions. In conclusion, this study investigates spontaneous continuous symmetry breaking using a two-dimensional dipolar XY model implemented in a Rydberg quantum simulator. The researchers demonstrate adiabatic preparation of correlated low-temperature states and characterize long-range XY order in ferromagnetic systems. This work contributes to our understanding of many-body physics and provides insights into programmable quantum simulation techniques.

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