Arxiv:2003.08945V2 [Cond-Mat.Quant-Gas] 30 Aug 2020
Observation of gauge invariance in a 71-site Bose-Hubbard quantum simulator Bing Yang,1, 2, 3, ∗ Hui Sun,1, 2, 3 Robert Ott,4 Han-Yi Wang,1, 2, 3 Torsten V. Zache,4 Jad C. Halimeh,5, 6, 4 Zhen-Sheng Yuan,1, 2, 3, y Philipp Hauke,5, 6, 4, z and Jian-Wei Pan1, 2, 3, x 1Hefei National Laboratory for Physical Sciences at Microscale and Department of Modern Physics, University of Science and Technology of China, Hefei, Anhui 230026, China 2Physikalisches Institut, Ruprecht-Karls-Universit¨atHeidelberg, Im Neuenheimer Feld 226, 69120 Heidelberg, Germany 3CAS Centre for Excellence and Synergetic Innovation Centre in Quantum Information and Quantum Physics, University of Science and Technology of China, Hefei, Anhui 230026, China 4Institute for Theoretical Physics, Ruprecht-Karls-Universit¨atHeidelberg, Philosophenweg 16, 69120 Heidelberg, Germany 5Department of Physics, University of Trento, Via Sommarive 14, 38123 Povo (TN), Italy 6Kirchhoff-Institute for Physics, Ruprecht-Karls-Universit¨atHeidelberg, Im Neuenheimer Feld 227, 69120 Heidelberg, Germany The modern description of elementary parti- Gauge invariance in QED|described as a local U(1) cles, as formulated in the Standard Model of par- symmetry of the Hamiltonian|ties electric fields E~ and ticle physics, is built on gauge theories [1]. Gauge charges ρ to each other through Gauss's law, r · E~ = ρ. theories implement fundamental laws of physics This basic principle of gauge invariance has stood model by local symmetry constraints. For example, for the Standard Model of particle physics, including, in quantum electrodynamics, Gauss's law intro- e.g., quantum chromodynamics. However, despite im- duces an intrinsic local relation between charged pressive feats [17, 18], it remains extremely difficult for matter and electromagnetic fields, which protects classical computers to solve the dynamics of gauge the- many salient physical properties including mass- ories [3{6].
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