Valery G. Rousseau
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Research Interests
Valery G. Rousseau has a total of 63 co-authors. Here are the top co-authors by number of shared publications:
R. T. Scalettar
Physics Department, University of California, Davis, California 95616, USA
20 shared publications- Ghassan George Batrouni
Université Côte d'Azur
19 shared publications F. Hébert
Institut de Physique de Nice, Université Côte d'Azur, CNRS, Nice, France
9 shared publications- Juana Moreno
Department of Physics and Astronomy, Louisiana State University 1 , Baton Rouge, Louisiana 70803, USA
8 shared publications G. G. Batrouni
INLN, Université de Nice-Sophia Antipolis, CNRS; 1361 route des Lucioles, 06560 Valbonne, France
6 shared publications- Marcos Rigol
Pennsylvania State University
5 shared publications
Latest Publications
- 22 July 2025
- Published by IOP Publishing in Physics Education
- Vol. 60 (5) , 055014
Einstein’s cat: a thought experiment on the universality of time dilation
The universality of time dilation is sometimes misunderstood, with claims that it applies exclusively to light clocks and not to mechanical clocks or other material objects, including biological entities. This leads to incorrect interpretations of experiments like the Hafele–Keating experiment, which actually confirm relativistic effects through the use of atomic clocks. To address this issue, we propose a thought experiment, inspired by Schrödinger’s cat, involving a ‘Sync-or-Die clock’, a device that combines a light clock and a mechanical stopwatch, with the life of Einstein’s cat, Tiger, depending on their synchronization. A straightforward analysis shows that both clocks experience time dilation equally, reinforcing the fact that time dilation is not limited to clocks based on light propagation but is a universal feature of Special Relativity.
- 22 July 2025
- Published by IOP Publishing in Physics Education
- Vol. 60 (5) , 055014
Einstein’s cat: a thought experiment on the universality of time dilation
The universality of time dilation is sometimes misunderstood, with claims that it applies exclusively to light clocks and not to mechanical clocks or other material objects, including biological entities. This leads to incorrect interpretations of experiments like the Hafele–Keating experiment, which actually confirm relativistic effects through the use of atomic clocks. To address this issue, we propose a thought experiment, inspired by Schrödinger’s cat, involving a ‘Sync-or-Die clock’, a device that combines a light clock and a mechanical stopwatch, with the life of Einstein’s cat, Tiger, depending on their synchronization. A straightforward analysis shows that both clocks experience time dilation equally, reinforcing the fact that time dilation is not limited to clocks based on light propagation but is a universal feature of Special Relativity.
- 21 June 2022
- Published by American Physical Society (APS) in Physical Review A
- Vol. 105 (6) , 063320
Quantum membrane phases in synthetic lattices of cold molecules or Rydberg atoms
We calculate properties of dipolar interacting ultracold molecules or Rydberg atoms in a semisynthetic three-dimensional configuration—one synthetic dimension plus a two-dimensional real-space optical lattice or periodic microtrap array—using the stochastic Green's function quantum Monte Carlo method. Through a calculation of thermodynamic quantities and appropriate correlation functions, along with their finite-size scalings, we show that there is a second-order transition to a low-temperature phase in which two-dimensional “sheets” form in the synthetic dimension of internal rotational or electronic states of the molecules or Rydberg atoms, respectively. Simulations for different values of the interaction , which acts between atoms or molecules that are adjacent both in real and synthetic space, allow us to compute a phase diagram. We find a finite-temperature transition at sufficiently large as well as a quantum phase transition—a critical value below which the transition temperature vanishes.- 21 June 2022
- Published by American Physical Society (APS) in Physical Review A
- Vol. 105 (6) , 063320
Quantum membrane phases in synthetic lattices of cold molecules or Rydberg atoms
We calculate properties of dipolar interacting ultracold molecules or Rydberg atoms in a semisynthetic three-dimensional configuration—one synthetic dimension plus a two-dimensional real-space optical lattice or periodic microtrap array—using the stochastic Green's function quantum Monte Carlo method. Through a calculation of thermodynamic quantities and appropriate correlation functions, along with their finite-size scalings, we show that there is a second-order transition to a low-temperature phase in which two-dimensional “sheets” form in the synthetic dimension of internal rotational or electronic states of the molecules or Rydberg atoms, respectively. Simulations for different values of the interaction , which acts between atoms or molecules that are adjacent both in real and synthetic space, allow us to compute a phase diagram. We find a finite-temperature transition at sufficiently large as well as a quantum phase transition—a critical value below which the transition temperature vanishes.- 4 December 2019
- Published by American Physical Society (APS) in Physical Review A
- Vol. 100 (6) , 063608
Scaling properties of Tan's contact: Embedding pairs and correlation effect in the Tonks-Girardeau limit
We study Tan's contact of a one-dimensional quantum gas of repulsive identical bosons confined in a harmonic trap at finite temperature. This canonical ensemble framework corresponds to the experimental conditions, with the number of particles being fixed for each experimental sequence. We show that in the strongly interacting regime, the contact rescaled by the contact at the Tonks-Girardeau limit is a universal function of two parameters: the rescaled interaction strength and temperature. This means that all pair and correlation effects in Tan's contact are embedded in Tan's contact in the Tonks-Girardeau limit.- 4 December 2019
- Published by American Physical Society (APS) in Physical Review A
- Vol. 100 (6) , 063608
Scaling properties of Tan's contact: Embedding pairs and correlation effect in the Tonks-Girardeau limit
We study Tan's contact of a one-dimensional quantum gas of repulsive identical bosons confined in a harmonic trap at finite temperature. This canonical ensemble framework corresponds to the experimental conditions, with the number of particles being fixed for each experimental sequence. We show that in the strongly interacting regime, the contact rescaled by the contact at the Tonks-Girardeau limit is a universal function of two parameters: the rescaled interaction strength and temperature. This means that all pair and correlation effects in Tan's contact are embedded in Tan's contact in the Tonks-Girardeau limit.- Open Access
- 10 December 2015
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 115 (24) , 240402
Cooling Atomic Gases With Disorder
Cold atomic gases have proven capable of emulating a number of fundamental condensed matter phenomena including Bose-Einstein condensation, the Mott transition, Fulde-Ferrell-Larkin-Ovchinnikov pairing, and the quantum Hall effect. Cooling to a low enough temperature to explore magnetism and exotic superconductivity in lattices of fermionic atoms remains a challenge. We propose a method to produce a low temperature gas by preparing it in a disordered potential and following a constant entropy trajectory to deliver the gas into a nondisordered state which exhibits these incompletely understood phases. We show, using quantum Monte Carlo simulations, that we can approach the Néel temperature of the three-dimensional Hubbard model for experimentally achievable parameters. Recent experimental estimates suggest the randomness required lies in a regime where atom transport and equilibration are still robust.
- 10 December 2015
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 115 (24) , 240402
Open AccessCooling Atomic Gases With Disorder
Cold atomic gases have proven capable of emulating a number of fundamental condensed matter phenomena including Bose-Einstein condensation, the Mott transition, Fulde-Ferrell-Larkin-Ovchinnikov pairing, and the quantum Hall effect. Cooling to a low enough temperature to explore magnetism and exotic superconductivity in lattices of fermionic atoms remains a challenge. We propose a method to produce a low temperature gas by preparing it in a disordered potential and following a constant entropy trajectory to deliver the gas into a nondisordered state which exhibits these incompletely understood phases. We show, using quantum Monte Carlo simulations, that we can approach the Néel temperature of the three-dimensional Hubbard model for experimentally achievable parameters. Recent experimental estimates suggest the randomness required lies in a regime where atom transport and equilibration are still robust.
- Open Access
- 28 September 2015
- Published by IOP Publishing in Journal of Physics: Conference Series
- Vol. 640 (1) , 012042
Competition between the Haldane insulator, superfluid and supersolid phases in the one-dimensional Bosonic Hubbard Model
Diverse solid and supersolid phases of bosons in a triangular lattice
- 28 September 2015
- Published by IOP Publishing in Journal of Physics: Conference Series
- Vol. 640 (1) , 012042
Open AccessCompetition between the Haldane insulator, superfluid and supersolid phases in the one-dimensional Bosonic Hubbard Model
Diverse solid and supersolid phases of bosons in a triangular lattice
- Open Access
- 12 August 2015
- Published by American Physical Society (APS) in Physical Review B
- Vol. 92 (5)
Competing exotic quantum phases of spin-ultracold lattice bosons with extended spin interactionsAdvances in pure optical trapping techniques now allow the creation of degenerate Bose gases with internal degrees of freedom. Systems such as , or in the hyperfine state offer an ideal platform for studying the interplay of superfluidity and quantum magnetism. Motivated by the experimental developments, we study ground-state phases of a two-component Bose gas loaded on an optical lattice. The system is described effectively by the Bose-Hubbard Hamiltonian with on-site and near-neighbor spin-spin interactions. An important feature of our investigation is the inclusion of interconversion (spin-flip) terms between the two species, which has been observed in optical lattice experiments. Using mean-field theory and quantum Monte Carlo simulations, we map out the phase diagram of the system. A rich variety of phases is identified, including antiferromagnetic (AF) Mott insulators and ferromagnetic and AF superfluids.- 12 August 2015
- Published by American Physical Society (APS) in Physical Review B
- Vol. 92 (5)
Open AccessCompeting exotic quantum phases of spin-ultracold lattice bosons with extended spin interactionsAdvances in pure optical trapping techniques now allow the creation of degenerate Bose gases with internal degrees of freedom. Systems such as , or in the hyperfine state offer an ideal platform for studying the interplay of superfluidity and quantum magnetism. Motivated by the experimental developments, we study ground-state phases of a two-component Bose gas loaded on an optical lattice. The system is described effectively by the Bose-Hubbard Hamiltonian with on-site and near-neighbor spin-spin interactions. An important feature of our investigation is the inclusion of interconversion (spin-flip) terms between the two species, which has been observed in optical lattice experiments. Using mean-field theory and quantum Monte Carlo simulations, we map out the phase diagram of the system. A rich variety of phases is identified, including antiferromagnetic (AF) Mott insulators and ferromagnetic and AF superfluids. - Open Access
- 1 July 2015
- Published by American Physical Society (APS) in Physical Review B
- Vol. 92 (3) , 035101
Bosonic Kondo-Hubbard model
We study, using quantum Monte Carlo simulations, the bosonic Kondo-Hubbard model in a two-dimensional square lattice. We explore the phase diagram and analyze the mobility of particles and magnetic properties. At unit filling, the transition from a paramagnetic Mott insulator to a ferromagnetic superfluid appears continuous, contrary to what was predicted with mean field. For double occupation per site, both the Mott insulating and superfluid phases are ferromagnetic and the transition is still continuous. Multiband tight-binding Hamiltonians can be realized in optical lattice experiments, which offer not only the possibility of tuning the different energy scales over wide ranges, but also the option of loading the system with either fermionic or bosonic atoms.
- 1 July 2015
- Published by American Physical Society (APS) in Physical Review B
- Vol. 92 (3) , 035101
Open AccessBosonic Kondo-Hubbard model
We study, using quantum Monte Carlo simulations, the bosonic Kondo-Hubbard model in a two-dimensional square lattice. We explore the phase diagram and analyze the mobility of particles and magnetic properties. At unit filling, the transition from a paramagnetic Mott insulator to a ferromagnetic superfluid appears continuous, contrary to what was predicted with mean field. For double occupation per site, both the Mott insulating and superfluid phases are ferromagnetic and the transition is still continuous. Multiband tight-binding Hamiltonians can be realized in optical lattice experiments, which offer not only the possibility of tuning the different energy scales over wide ranges, but also the option of loading the system with either fermionic or bosonic atoms.
- 11 May 2015
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 114 (19) , 195302
Feshbach-Stabilized Insulator of Bosons in Optical Lattices
Feshbach resonances—namely, resonances between an unbound two-body (atomic) state and a bound (molecular) state, differing in magnetic moment—are a unique tool to tune the interaction properties of ultracold atoms. Here we show that the spin-changing interactions, coherently coupling the atomic and molecular states, can act as a novel mechanism to stabilize an insulating phase—the Feshbach insulator—for bosons in an optical lattice close to a narrow Feshbach resonance. Making use of quantum Monte Carlo simulations and mean-field theory, we show that the Feshbach insulator appears around the resonance, preventing the system from collapsing when the effective atomic scattering length becomes negative. On the atomic side of the resonance, the transition from condensate to Feshbach insulator has a characteristic first-order nature, due to the simultaneous loss of coherence in the atomic and molecular components. These features appear clearly in the ground-state phase diagram of, e.g., around its 414 G resonance, and they are therefore directly amenable to experimental observation.- 11 May 2015
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 114 (19) , 195302
Feshbach-Stabilized Insulator of Bosons in Optical Lattices
Feshbach resonances—namely, resonances between an unbound two-body (atomic) state and a bound (molecular) state, differing in magnetic moment—are a unique tool to tune the interaction properties of ultracold atoms. Here we show that the spin-changing interactions, coherently coupling the atomic and molecular states, can act as a novel mechanism to stabilize an insulating phase—the Feshbach insulator—for bosons in an optical lattice close to a narrow Feshbach resonance. Making use of quantum Monte Carlo simulations and mean-field theory, we show that the Feshbach insulator appears around the resonance, preventing the system from collapsing when the effective atomic scattering length becomes negative. On the atomic side of the resonance, the transition from condensate to Feshbach insulator has a characteristic first-order nature, due to the simultaneous loss of coherence in the atomic and molecular components. These features appear clearly in the ground-state phase diagram of, e.g., around its 414 G resonance, and they are therefore directly amenable to experimental observation.- Open Access
- 17 November 2014
- Published by American Physical Society (APS) in Physical Review B
- Vol. 90 (20) , 205123
Competing phases, phase separation, and coexistence in the extended one-dimensional bosonic Hubbard model
We study the phase diagram of the one-dimensional bosonic Hubbard model with contact and near neighbor interactions focusing on the gapped Haldane insulating (HI) phase which is characterized by an exotic nonlocal order parameter. The parameter regime , and where this phase exists and how it competes with other phases, such as the supersolid (SS) phase, is incompletely understood. We use the stochastic Green function quantum Monte Carlo algorithm as well as the density matrix renormalization group to map out the phase diagram. Our main conclusions are that the HI exists only at , the SS phase exists for a very wide range of parameters (including commensurate fillings), and displays power law decay in the one-body Green function. In addition, we show that at fixed integer density, the system exhibits phase separation in the plane.- 17 November 2014
- Published by American Physical Society (APS) in Physical Review B
- Vol. 90 (20) , 205123
Open AccessCompeting phases, phase separation, and coexistence in the extended one-dimensional bosonic Hubbard model
We study the phase diagram of the one-dimensional bosonic Hubbard model with contact and near neighbor interactions focusing on the gapped Haldane insulating (HI) phase which is characterized by an exotic nonlocal order parameter. The parameter regime , and where this phase exists and how it competes with other phases, such as the supersolid (SS) phase, is incompletely understood. We use the stochastic Green function quantum Monte Carlo algorithm as well as the density matrix renormalization group to map out the phase diagram. Our main conclusions are that the HI exists only at , the SS phase exists for a very wide range of parameters (including commensurate fillings), and displays power law decay in the one-body Green function. In addition, we show that at fixed integer density, the system exhibits phase separation in the plane. - 4 November 2014
- Published by American Physical Society (APS) in Physical Review B
- Vol. 90 (20) , 205104
Ferromagnetic phase in the polarized two-species bosonic Hubbard model
We recently studied a doped two-dimensional bosonic Hubbard model with two hard-core species, with different masses, using quantum Monte Carlo simulations [Hettiarachchilage, Phys. Rev. B 88, 161101(R) (2013)]. Upon doping away from half filling, we find several distinct phases, including a phase-separated ferromagnet with Mott behavior for the heavy species and both Mott-insulating and superfluid behaviors for the light species. Introducing polarization, i.e., an imbalance in the population between species, we find a fully phase-separated ferromagnet. This phase exists for a broad range of temperatures and polarizations. By using finite-size scaling of the susceptibility, we find a critical exponent which is consistent with the two-dimensional Ising universality class. Significantly, since the global entropy of this phase is higher than that of the ferromagnetic phase with single species, its experimental observation in cold atoms may be feasible.
- 4 November 2014
- Published by American Physical Society (APS) in Physical Review B
- Vol. 90 (20) , 205104
Ferromagnetic phase in the polarized two-species bosonic Hubbard model
We recently studied a doped two-dimensional bosonic Hubbard model with two hard-core species, with different masses, using quantum Monte Carlo simulations [Hettiarachchilage, Phys. Rev. B 88, 161101(R) (2013)]. Upon doping away from half filling, we find several distinct phases, including a phase-separated ferromagnet with Mott behavior for the heavy species and both Mott-insulating and superfluid behaviors for the light species. Introducing polarization, i.e., an imbalance in the population between species, we find a fully phase-separated ferromagnet. This phase exists for a broad range of temperatures and polarizations. By using finite-size scaling of the susceptibility, we find a critical exponent which is consistent with the two-dimensional Ising universality class. Significantly, since the global entropy of this phase is higher than that of the ferromagnetic phase with single species, its experimental observation in cold atoms may be feasible.