Publications (97)435.88 Total impact

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ABSTRACT: We study attractively interacting fermions on a square lattice with dispersion relations exhibiting strong spindependent anisotropy. The resulting Fermi surface mismatch suppresses the swave BCStype instability, clearing the way for unconventional types of order. Unbiased sampling of the Feynman diagrammatic series using diagrammatic Monte Carlo methods reveals a rich phase diagram in the regime of intermediate coupling strength. Instead of a proposed Cooperpair Bose metal phase [A. E. Feiguin and M. P. A. Fisher, Phys. Rev. Lett. 103, 025303 (2009).Physical Review Letters 11/2014; 113(19):195301. · 7.73 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: We argue that the three key phenomena recently observed in solid $^4$Hemass supertransport, anomalous isochoric compressibility (syringe effect), and giant plasticityare closely linked to each other through the physics of an interconnected network of tilted quantumrough dislocations. As immediate implications of this connection several predictions follow: In the absence of $^3$He impurities, the syringe effect and giant plasticity persist down to $T=0$; the dynamical lowfrequency syringe and giantplasticity responses are dispersionless; and similarly to giant plasticity but without direct relationship to the supertransport along the dislocation cores, $^3$He impurities should suppress the syringe effect partially or completely at appropriately low temperatures.09/2014;  [Show abstract] [Hide abstract]
ABSTRACT: We study the ground state phase diagram of a onedimensional hardcore bosonic model with nearestneighbor interactions (XXZ model) where every site is coupled Ohmically to an independent but identical reservoir, hereby generalizing spinboson models to interacting spinboson systems. %The coupling with the bath is taken to be Ohmic ($s=1)$. We show that a bathinduced Bose metal phase can occur in the ground state phase diagram away from half filling. This phase is compressible, gapless, and conducting but not superfluid. At haffilling, only a Luttinger liquid and a charge density wave are found. The phase transition between them is of KosterlitzThouless type where the Luttinger parameter takes a nonuniversal value.The applied quantum Monte Carlo method can be used for all open bosonic and unfrustrated spin systems, regardless of their dimension, filling factor and spectrum of the dissipation as long as the quantum system couples to the bath via the density operators.08/2014;  [Show abstract] [Hide abstract]
ABSTRACT: We study attractively interacting fermions on a square lattice with dispersion relations exhibiting strong spindependent anisotropy. The resulting Fermi surface mismatch suppresses the swave BCStype instability, clearing the way for unconventional types of order. Unbiased sampling of the Feynman diagrammatic series using Diagrammatic Monte Carlo methods reveals a rich phase diagram in the regime of intermediate coupling strength. Instead of a proposed Cooperpair Bose metal phase [A. E. Feiguin and M. P. A. Fisher, Phys. Rev. Lett. 103, 025303 (2009)] we find an incommensurate density wave at strong anisotropy and two different pwave superfluid states with unconventional symmetry at intermediate anisotropy.08/2014; 
Article: Thermalization of strongly interacting bosons after spontaneous emissions in optical lattices
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ABSTRACT: We study the outofequilibrium dynamics of bosonic atoms in a 1D optical lattice, after the groundstate is excited by a single spontaneous emission event, i.e. after an absorption and reemission of a lattice photon. This is an important fundamental source of decoherence for current experiments, and understanding the resulting dynamics and changes in the manybody state is important for controlling heating in quantum simulators. Previously it was found that in the superfluid regime, simple observables relax to values that can be described by a thermal distribution on experimental timescales, and that this breaks down for strong interactions (in the Mott insulator regime). Here we expand on this result, investigating the relaxation of the momentum distribution as a function of time, and discussing the relationship to eigenstate thermalization. For the strongly interacting limit, we provide an analytical analysis for the behavior of the system, based on an effective lowenergy Hamiltonian in which the dynamics can be understood based on correlated doublonholon pairs.08/2014;  [Show abstract] [Hide abstract]
ABSTRACT: The ground state of ^{4}He confined in a system with the topology of cylinder can display properties of solid, superfluid, and liquid crystal. This phase, which we call a compactified supersolid (CSS), originates from wrapping the basal planes of the bulk hcp solid into concentric cylindrical shells, with several central shells exhibiting superfluidity along the axial direction. Its main feature is the presence of a topological defect which can be viewed as a disclination with Frank index n=1 observed in liquid crystals, and which, in addition, has a superfluid core. The CSS as well as its transition to an insulating compactified solid with a very wide hysteresis loop are found by ab initio Monte Carlo simulations. A simple analytical model captures qualitatively correctly the main property of the CSSa gradual decrease of the superfluid response with increasing pressure.Physical Review Letters 07/2014; 113(4):045301. · 7.73 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: The ground state of solid $^4$He in a cylindrical nanopore hosts a topological linear defect which can be viewed as a nematictype Frank's disclination. The associated singular strain (or, rather, splay) may cause partial melting around the line to create a superfluid core of the disclination. The resulting phase, compactified supersolid (CSS), is studied by ab initio Monte Carlo simulations and by a simple model explaining its main feature  a gradual decrease of the superfluid response with pressure observed in vycor. The CSS is found to transform into insulating compactified solid (CS) by a first order transition with very wide hysteresis.03/2014;  [Show abstract] [Hide abstract]
ABSTRACT: We analyze the groundstate properties of mixtures consisting of scalar bosons and spin1/2 fermions using a meanfield treatment of the local bosonfermion interaction on a simple cubic lattice. In the deep superfluid limit of the boson sector and the BCS regime of the fermion sector, we derive BCStype equations to determine the phase diagram of the system. We find a competition between a charge density wave and a superconducting phase. In the opposite limit, we study the Mottinsulatortosuperfluid transition of the boson sector in the presence of a staggered densityinduced alternating potential provided by the fermions, and determine the meanfield transition line. In the twosuperfluids phase of the mixture, we restrict to nearestneighborinduced interactions between the fermions and consider the extended Hubbard model. We perform a meanfield analysis of the critical temperature for the formation of bosonassisted s, extended s, d, and pwave pairs at fermionic halffilling. We compare our results with a recent dynamical meanfield study [P. Anders et al., Phys. Rev. Lett. 109, 206401 (2012), 10.1103/PhysRevLett.109.206401].02/2014; 89(9). 
Article: Groundstate phase diagram of the twodimensional BoseHubbard model with anisotropic hopping
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ABSTRACT: We compute the groundstate phase diagram of the twodimensional (2D) BoseHubbard model with anisotropic hopping using quantum Monte Carlo simulations, connecting the onedimensional (1D) to the 2D system. We find that the tip of the lobe lies on a curve controlled by the 1D limit over the full anisotropy range, while the universality class is always the same as in the isotropic 2D system. This behavior can be derived analytically from the lowest renormalizationgroup equations and has a shape typical for the underlying KosterlitzThouless transition in one dimension. We also compute the phase boundary of the Mott lobe at unit density for strong anisotropy and compare it to the 1D system. Our calculations shed light on recent cold gas experiments monitoring the dynamics of an expanding cloud.01/2014; 89(2). 
Article: Universal Conductivity in a TwoDimensional SuperfluidtoInsulator Quantum Critical System.
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ABSTRACT: We compute the universal conductivity of the (2+1)dimensional XY universality class, which is realized for a superfluidtoMott insulator quantum phase transition at constant density. Based on largescale Monte Carlo simulations of the classical (2+1)dimensional Jcurrent model and the twodimensional BoseHubbard model, we can precisely determine the conductivity on the quantum critical plateau, σ(∞)=0.359(4)σ_{Q} with σ_{Q} the conductivity quantum. The universal conductivity curve is the standard example with the lowest number of components where the bottomsup AdS/CFT correspondence from string theory can be tested and made to use [R. C. Myers, S. Sachdev, and A. Singh, Phys. Rev. D 83, 066017 (2011)]. For the first time, the shape of the σ(iω_{n})σ(∞) function in the Matsubara representation is accurate enough for a conclusive comparison and establishes the particlelike nature of charge transport. We find that the holographic gaugegravity duality theory for transport properties can be made compatible with the data if temperature of the horizon of the black brane is different from the temperature of the conformal field theory. The requirements for measuring the universal conductivity in a cold gas experiment are also determined by our calculation.Physical Review Letters 01/2014; 112(3):030402. · 7.73 Impact Factor 
Article: Asymptotically Exact Scenario of StrongDisorder Criticality in OneDimensional Superfluids
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ABSTRACT: We present a controlled rareweaklink theory of the superfluidtoBose/Mott glass transition in onedimensional disordered systems. The transition has KosterlitzThouless critical properties but may occur at an arbitrary large value of the Luttinger parameter $K$. In contrast to the scenario by Altman {\it et al.} [Phys. Rev. B {\bf 81}, 174528 (2010)], the hydrodynamic description is valid under the correlation radius and defines criticality via the renormalization of microscopically weak links, along the lines of Kane and Fisher [Phys. Rev. Lett. {\bf 68}, 1220 (1992)]. The hallmark of the theory is the relation $K^{(c)}=1/\zeta$ between the critical value of the Luttinger parameter at macroscopic scales and the microscopic (irrenormalizable) exponent $\zeta$ describing the scaling $\propto 1/N^{1\zeta}$ for the strength of the weakest link among the $N/L \gg 1$ disorder realizations in a system of fixed mesoscopic size $L$.11/2013; 89(5). 
Dataset: Observation of Correlated ParticleHole Pairs and String Order in LowDimensional Mott Insulators
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ABSTRACT: Quantum phases of matter are characterized by the underlying correlations of the manybody system. Although this is typically captured by a local order parameter, it has been shown that a broad class of manybody systems possesses a hidden nonlocal order. In the case of bosonic Mott insulators, the ground state properties are governed by quantum fluctuations in the form of correlated particlehole pairs that lead to the emergence of a nonlocal string order in one dimension. By using highresolution imaging of lowdimensional quantum gases in an optical lattice, we directly detect these pairs with singlesite and singleparticle sensitivity and observe string order in the onedimensional case.  [Show abstract] [Hide abstract]
ABSTRACT: We compute the ground state phase diagram of the 2d BoseHubbard model with anisotropic hopping using quantum Monte Carlo simulations, connecting the 1d to the 2d system. We find that the tip of the lobe lies on a curve controlled by the 1d limit over the full anisotropy range while the universality class is always the same as in the isotropic 2d system. This behavior can be derived analytically from the lowest RG equations and has a form typical for the underlying KosterlitzThouless transition in 1d. We also compute the phase boundary of the Mott lobe for strong anisotropy and compare it to the 1d system. Our calculations shed light on recent cold gas experiments monitoring the dynamics of an expanding cloud.08/2013;  [Show abstract] [Hide abstract]
ABSTRACT: Correlation functions play an important role for the theoretical and experimental characterization of manybody systems. In solidstate systems, they are usually determined through scattering experiments, whereas in cold gases systems, timeofflight, and in situ absorption imaging are the standard observation techniques. However, none of these methods allow the in situ detection of spatially resolved correlation functions at the singleparticle level. Here, we give a more detailed account of recent advances in the detection of correlation functions using in situ fluorescence imaging of ultracold bosonic atoms in an optical lattice. This method yields singlesite and singleatomresolved images of the lattice gas in a single experimental run, thus gaining direct access to fluctuations in the manybody system. As a consequence, the detection of correlation functions between an arbitrary set of lattice sites is possible. This enables not only the detection of twosite correlation functions but also the evaluation of nonlocal correlations, which originate from an extended region of the system and are used for the characterization of quantum phases that do not possess (quasi)longrange order in the traditional sense.Applied Physics B 08/2013; · 1.78 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: We review the physics of the BoseHubbard model with disorder in the chemical potential focusing on recently published analytical arguments in combination with quantum Monte Carlo simulations. Apart from the superfluid and Mott insulator phases that can occur in this system without disorder, disorder allows for an additional phase, called the Bose glass phase. The topology of the phase diagram is subject to strong theorems proving that the Bose Glass phase must intervene between the superfluid and the Mott insulator and implying a Griffiths transition between the Mott insulator and the Bose glass. The full phase diagrams in 3d and 2d are discussed, and we zoom in on the insensitivity of the transition line between the superfluid and the Bose glass in the close vicinity of the tip of the Mott insulator lobe. We briefly comment on the established and remaining questions in the 1d case, and give a short overview of numerical work on related models.Comptes Rendus Physique 07/2013; 14(8). · 1.82 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: The droplet crystal phase of a symmetric binary mixture of Rydbergblockaded dipolar Bose gases is studied by computer simulation. At high temperature each droplet comprises on average equal numbers of particles of either component, but the two components demix below the supersolid transition temperature, i.e., droplets mostly consist of particles of one component. Droplets consisting of the same component will also favor clustering. Demixing is driven by quantum tunnelling of particles across droplets over the system, and does not take place in a nonsuperfluid crystal. This effect should be easily detectable in a cold gas experiment.Physical Review A 06/2013; 88(3). · 3.04 Impact Factor  [Show abstract] [Hide abstract]
ABSTRACT: We study the thermalization of excitations generated by spontaneous emission events for cold bosons in an optical lattice. Computing the dynamics described by the manybody master equa tion, we characterize equilibration timescales in different parameter regimes. For simple observables, we find regimes in which the system relaxes rapidly to values in agreement with a thermal distribu tion, and others where thermalization does not occur on typical experimental timescales. Because spontaneous emissions lead effectively to a local quantum quench, this behavior is strongly depen dent on the lowenergy spectrum of the Hamiltonian, and undergoes a qualitative change at the Mott Insulatorsuperfluid transition point. These results have important implications for the un derstanding of thermalization after localized quenches in isolated quantum gases, as well as the characterization of heating in experiments.05/2013;  [Show abstract] [Hide abstract]
ABSTRACT: We present spectral functions for the magnitude squared of the order parameter in the scaling limit of the twodimensional superfluid to Mott insulator quantum phase transition at constant density, which has emergent particlehole symmetry and Lorentz invariance. The universal functions for the superfluid, Mott insulator, and normal liquid phases reveal a lowfrequency resonance which is relatively sharp and is followed by a damped oscillation (in the first two phases only) before saturating to the quantum critical plateau. The counterintuitive resonance feature in the insulating and normal phases calls for deeper understanding of collective modes in the strongly coupled (2+1)dimensional relativistic field theory. Our results are derived from analytically continued correlation functions obtained from pathintegral Monte Carlo simulations of the BoseHubbard model.Physical Review Letters 04/2013; 110(17):170403. · 7.73 Impact Factor 
Article: Phase diagram of 4He on graphene
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ABSTRACT: The lowtemperature phase diagram of 4He adsorbed on a single graphene sheet is studied by computer simulations of a system consisting of nearly a thousand helium atoms. In the first layer, two commensurate solid phases are observed with fillings 1/3 and 7/16, respectively, separated by a domain wall phase, as well as an incommensurate crystal at a higher coverage. No evidence of a thermodynamically stable superfluid phase is found for the first adlayer. Secondlayer promotion occurs at a coverage of 0.111(4) Å−2. In the second layer, two phases are observed, namely a superfluid and an incommensurate solid, with no commensurate solid intervening between these two phases. The computed phase diagram closely resembles that predicted for helium on graphite.Physical review. B, Condensed matter 03/2013; 87(9). · 3.77 Impact Factor
Publication Stats
2k  Citations  
435.88  Total Impact Points  
Top Journals
Institutions

2013–2014

LudwigMaximilianUniversity of Munich
 Department of Physics
München, Bavaria, Germany


2008–2013

University of Massachusetts Amherst
 Department of Physics
Amherst Center, Massachusetts, United States 
UPMC
Pittsburgh, Pennsylvania, United States


2006–2012

ETH Zurich
 • Institute for Theoretical Physics
 • Department of Physics
Zürich, ZH, Switzerland


2011

Max Planck Institute of Quantum Optics
Arching, Bavaria, Germany 
GeorgAugustUniversität Göttingen
 Institute for Theoretical Physics
Göttingen, Lower Saxony, Germany 
Adam Mickiewicz University
 Faculty of Physics
Posen, Greater Poland Voivodeship, Poland


2003–2011

Ghent University
 Center for Molecular Modeling
Gand, Flanders, Belgium


2009–2010

Harvard University
 Department of Physics
Cambridge, MA, United States 
Università degli Studi di Trento
 Department of Physics
Trient, TrentinoAlto Adige, Italy 
University of California, Berkeley
 Pitzer Center for Theoretical Chemistry
Berkeley, CA, United States


2007

University of NiceSophia Antipolis
Nice, ProvenceAlpesCôte d'Azur, France 
Hochschule für Technik Zürich
Zürich, Zurich, Switzerland


2006–2007

University of Alberta
 Department of Physics
Edmonton, Alberta, Canada
