2021
DOI: 10.1038/s41586-021-03582-4
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Quantum phases of matter on a 256-atom programmable quantum simulator

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Cited by 737 publications
(562 citation statements)
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References 63 publications
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“…For comparison we also show the corresponding spectrum for the critical antiferromagnetic transverse-field Ising model, which realizes the noninteracting limit of the Ising CFT with u = 0 [Eq. (10)]. As described in the text, the slight reduction in the Rydberg energies near the middle of the plot suggests that the critical Rydberg chain at V 2 = 0 retains weak four-fermion interactions with u < 0.…”
Section: Four-fermion Interactions At Ising Criticalitymentioning
confidence: 70%
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“…For comparison we also show the corresponding spectrum for the critical antiferromagnetic transverse-field Ising model, which realizes the noninteracting limit of the Ising CFT with u = 0 [Eq. (10)]. As described in the text, the slight reduction in the Rydberg energies near the middle of the plot suggests that the critical Rydberg chain at V 2 = 0 retains weak four-fermion interactions with u < 0.…”
Section: Four-fermion Interactions At Ising Criticalitymentioning
confidence: 70%
“…Fermion velocity v in the low-energy Ising CFT Hamiltonian [Eq. (10)] versus V 2 for a critical Rydberg chain. The velocity is calculated from the slope of the lines near the |σ state in Fig.…”
Section: Four-fermion Interactions At Ising Criticalitymentioning
confidence: 99%
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“…Over the past few years, tweezer atom arrays have emerged as a very versatile platform for quantum science, with applications ranging from quantum simulation of many-body systems [2] to quantum metrology [3,4] and quantum computing [5,6]. Large arrays with up to approximately 200 atoms are now used for quantum simulation of spin systems [7,8]. They are assembled atom by atom, using moving optical tweezers, from an initially disordered configuration.…”
Section: Introductionmentioning
confidence: 99%
“…Despite their impressive success and accuracy in many scenarios, the com-plete understanding of several phenomena, e.g. the low-energy properties of Hubbard-like Hamiltonians for interacting fermions or the behavior of spin systems with frustrating interactions, is still debated, especially in two or three spatial dimensions [13][14][15][16][17][18][19][20], where current and near-future experimental setups require benchmarking tools capable of simulating large quantum many-body systems [21][22][23][24].…”
mentioning
confidence: 99%