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Landau's Fermi-liquid (FL) theory has been successful at the phenomenological description of the normal phase of many different Fermi systems. Using a dilute atomic Fermi fluid with tunable interactions, we investigate the microscopic basis of Landau's theory with a system describable from first principles. We study transport properties of an interacting Fermi gas by measuring its density response to a periodic external perturbation. In an ideal Fermi gas, we measure for the first time the celebrated Lindhard function. As the system is brought from the collisionless to the hydrodynamic regime, we observe the emergence of sound, and find that the experimental observations are quantitatively understood with a first-principle transport equation for the FL. When the system is more strongly interacting, we find deviations from such predictions. Finally, we observe the shape of the quasiparticle excitations directly from momentum-space tomography and see how it evolves from the collisionless to the collisional regime. Our study establishes this system as a clean platform for studying Landau's theory of the FL and paves the way for extending the theory to more exotic conditions, such as nonlinear dynamics and FLs with strong correlations in versatile settings.

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In this work, building on state-of-the-art quantum Monte Carlo simulations, we perform systematic finite-size scaling of both entanglement and participation entropies for long-range Heisenberg chain with unfrustrated power-law decaying interactions. We find distinctive scaling behaviors for both quantum entropies in the various regimes explored by tuning the decay exponent $\alpha$, thus capturing non-trivial features through logarithmic terms, beyond the case of linear Nambu-Goldstone modes. Our systematic analysis reveals that the quantum entanglement information, hidden in the scaling of the two studied entropies, can be obtained to the same level of order parameters and other usual finite-size observables of quantum many-body lattice models. The analysis and results obtained here can readily apply to more quantum criticalities in 1D and 2D systems.

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While gauge symmetry is a well-established requirement for representing topological orders in projected entangled-pair state (PEPS), its impact on the properties of low-lying excited states remains relatively unexplored. Here we perform PEPS simulations of low-energy dynamics in the Kitaev honeycomb model, which supports fractionalized gauge flux (vison) excitations. We identify gauge symmetry emerging upon optimizing an unbiased PEPS ground state. Using the PEPS adapted local mode approximation, we further classify the low-lying excited states by discerning different vison sectors. Our simulations of spin and spin-dimer dynamical correlations establish close connections with experimental observations. Notably, the selection rule imposed by the locally conserved visons results in nearly flat dispersions in momentum space for excited states belonging to the 2-vison or 4-vison sectors.

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Using a high-accuracy variational Monte Carlo approach based on group-convolutional neural networks, we obtain the symmetry-resolved low-energy spectrum of the spin-1/2 Heisenberg model on several highly symmetric fullerene geometries, including the famous C60 buckminsterfullerene. We argue that as the degree of frustration is lowered in large fullerenes, they display characteristic features of incipient magnetic ordering: Correlation functions show high-intensity Bragg peaks consistent with Néel-like ordering, while the low-energy spectrum is organized into a tower of states. Competition with frustration, however, turns the simple Néel order into a noncoplanar one. Remarkably, we find and predict chiral incipient ordering in a large number of fullerene structures.

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Quantum electrodynamics in <math display="inline"><mn>2</mn><mo>+</mo><mn>1</mn></math> dimensions (<math display="inline"><mrow><msub><mrow><mi>QED</mi></mrow><mrow><mn>3</mn></mrow></msub></mrow></math>) has been proposed as a critical field theory describing the low-energy effective theory of a putative algebraic Dirac spin liquid or of quantum phase transitions in two-dimensional frustrated magnets. We provide compelling evidence that the intricate spectrum of excitations of the elementary but strongly frustrated <math display="inline"><mrow><msub><mrow><mi>J</mi></mrow><mrow><mn>1</mn></mrow></msub><mtext>-</mtext><msub><mrow><mi>J</mi></mrow><mrow><mn>2</mn></mrow></msub></mrow></math> Heisenberg model on the triangular lattice is in one-to-one correspondence to a zoo of excitations from <math display="inline"><mrow><msub><mrow><mi>QED</mi></mrow><mrow><mn>3</mn></mrow></msub></mrow></math>, in the quantum spin liquid regime. This evidence includes a large manifold of explicitly constructed monopole and bilinear excitations of <math display="inline"><mrow><msub><mrow><mi>QED</mi></mrow><mrow><mn>3</mn></mrow></msub></mrow></math>, which is thus shown to serve as an organizing principle of phases of matter in triangular lattice antiferromagnets and their low-lying excitations. Moreover, we observe signatures of emergent valence-bond solid (VBS) correlations, which can be interpreted either as evidence of critical VBS fluctuations of an emergent Dirac spin liquid or as a transition from the 120° Néel order to a VBS whose quantum critical point is described by <math display="inline"><mrow><msub><mrow><mi>QED</mi></mrow><mrow><mn>3</mn></mrow></msub></mrow></math>. Our results are obtained by comparing ansatz wave functions from a parton construction to exact eigenstates obtained using large-scale exact diagonalization up to <math display="inline"><mi>N</mi><mo>=</mo><mn>48</mn></math> sites.

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Sujets

FOS Physical sciences T-J model Variational quantum Monte Carlo 7510Kt Tensor networks Correlation 6470Tg Entanglement quantum Spin Dimeres Théorie de la matière condensée Champ magnétique 7540Mg 7127+a Valence bond crystals Quantum dimer models t-J model Arrays of Josephson junctions Superconductivity cond-matsupr-con 7540Cx Méthodes numériques Quantum physics Boson Low dimension Liquid Antiferromagnétisme Aimants quantiques Quantum dimer models t-J model superconductivity magnetism Ground state Condensed Matter Electronic Properties Classical spin liquid Strongly Correlated Electrons Chaînes des jonctions Anti-ferromagnetism Advanced numerical methods Network Collective modes Low-dimensional systems 0270Ss Confinement Dirac spin liquid 7130+h Atom Strongly Correlated Electrons cond-matstr-el Numerical methods Monte-Carlo quantique Anyons Dimension Strongly correlated systems Bose glass Spin chain Chaines de spin1/2 Quasiparticle Color High-Tc Apprentissage automatique Magnetism Electronic structure and strongly correlated systems Quantum information Condensed matter physics Thermodynamical Spin liquids Antiferromagnetic conductors Plateaux d'aimantation Réseaux de tenseurs Strong interaction Entanglement Kagome lattice Chaines de spin Condensed Matter Bosons de coeur dur Physique de la matière condensée 7510Jm Polaron Disorder Excited state Variational Monte Carlo Deconfinement Many-body problem Superconductivity Benchmark Magnétisme quantique Collinear Solids Condensed matter theory Antiferromagnetism Condensed matter Électrons fortement corrélés Critical phenomena Supraconductivité Gas Frustration Atomic Physics physicsatom-ph Magnetic quantum oscillations Systèmes fortement corrélés Quantum magnetism Physique quantique Quantum Gases cond-matquant-gas Heisenberg model Basse dimension

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