Characterizing the phase diagram of finite-size dipolar Bose-Hubbard systems

Physical Review A American Physical Society 101 (2020) 013616

P Rosson, J Mur Petit, M Kiffner, D Jaksch

We use state-of-the-art density matrix renormalization group calculations in the canonical ensemble to determine the phase diagram of the dipolar Bose-Hubbard model on a finite cylinder. We consider several observables that are accessible in typical optical lattice setups and assess how well these quantities perform as order parameters. We find that, especially for small systems, the occupation imbalance is less susceptible to boundary effects than the structure factor in uncovering the presence of a periodic density modulation. By analyzing the nonlocal correlations, we find that the appearance of supersolid order is very sensitive to boundary effects, which may render it difficult to observe in quantum gas lattice experiments with a few tens of particles. Finally, we show that density measurements readily obtainable on a quantum gas microscope allow distinguishing between superfluid and solid phases using unsupervised machine-learning techniques.

Efficient microwave-to-optical conversion using Rydberg atoms

PHYSICAL REVIEW A 99 (2019) ARTN 023832

T Vogt, C Gross, J Han, SB Pal, M Lam, M Kiffner, W Li

Mott polaritons in cavity-coupled quantum materials

New Journal of Physics IOP Publishing (2019)

M Kiffner, J Coulthard, F Schlawin, A Ardavan, D Jaksch

Quantum impurity models coupled to Markovian and non-Markovian baths.

The Journal of chemical physics 151 (2019) 044102-044102

M Schiro, O Scarlatella

We develop a method to study quantum impurity models, small interacting quantum systems bilinearly coupled to an environment, in the presence of an additional Markovian quantum bath, with a generic nonlinear coupling to the impurity. We aim at computing the evolution operator of the reduced density matrix of the impurity, obtained after tracing out all the environmental degrees of freedom. First, we derive an exact real-time hybridization expansion for this quantity, which generalizes the result obtained in the absence of the additional Markovian dissipation and which could be amenable to stochastic sampling through diagrammatic Monte Carlo. Then, we obtain a Dyson equation for this quantity and we evaluate its self-energy with a resummation technique known as the noncrossing approximation. We apply this novel approach to a simple fermionic impurity coupled to a zero temperature fermionic bath and in the presence of Markovian pump, losses, and dephasing.

Spectral functions and negative density of states of a driven-dissipative nonlinear quantum resonator


O Scarlatella, AA Clerk, M Schiro

Emergent finite frequency criticality of driven-dissipative correlated lattice bosons

PHYSICAL REVIEW B 99 (2019) ARTN 064511

O Scarlatella, R Fazio, M Schiro

Heating-Induced Long-Range η Pairing in the Hubbard Model

Physical Review Letters American Physical Society 123 (2019) 030603

J Tindall, B Buča, J Coulthard, D Jaksch

We show how, upon heating the spin degrees of freedom of the Hubbard model to infinite temperature, the symmetries of the system allow the creation of steady states with long-range correlations between η pairs. We induce this heating with either dissipation or periodic driving and evolve the system towards a nonequilibrium steady state, a process which melts all spin order in the system. The steady state is identical in both cases and displays distance-invariant off-diagonal η correlations. These correlations were first recognized in the superconducting eigenstates described in Yang’s seminal Letter [Phys. Rev. Lett. 63, 2144 (1989)], which are a subset of our steady states. We show that our results are a consequence of symmetry properties and entirely independent of the microscopic details of the model and the heating mechanism.

Ultracold molecules for quantum simulation: rotational coherences in CaF and RbCs

Quantum Science and Technology IOP Publishing 4 (2018) 014010

JA Blackmore, L Caldwell, PD Gregory, EM Bridge, R Sawant, J Mur Petit, J Aldegunde, D Jaksch, JM Hutson, BE Sauer, SL Cornish

Polar molecules offer a new platform for quantum simulation of systems with long-range interactions, based on the electrostatic interaction between their electric dipole moments. Here, we report the development of coherent quantum state control using microwave fields in $^{40}$Ca$^{19}$F and $^{87}$Rb$^{133}$Cs molecules, a crucial ingredient for many quantum simulation applications. We perform Ramsey interferometry measurements with fringe spacings of $\sim 1~\rm kHz$ and investigate the dephasing time of a superposition of $N=0$ and $N=1$ rotational states when the molecules are confined. For both molecules, we show that a judicious choice of molecular hyperfine states minimises the impact of spatially varying transition-frequency shifts across the trap. For magnetically trapped $^{40}$Ca$^{19}$F we use a magnetically insensitive transition and observe a coherence time of 0.61(3)~ms. For optically trapped $^{87}$Rb$^{133}$Cs we exploit an avoided crossing in the AC Stark shifts and observe a maximum coherence time of 0.75(6)~ms.

Bosonic fractional quantum hall states on a finite cylinder

Physical Review A American Physical Society 99 (2019) 033603-

P Rosson, M Lubasch, M Kiffner, D Jaksch

We investigate the ground-state properties of a bosonic Harper-Hofstadter model with local interactions on a finite cylindrical lattice with filling fraction ν = 1/2. We find that our system supports topologically ordered states by calculating the topological entanglement entropy, and its value is in good agreement with the theoretical value for the ν = 1/2 Laughlin state. By exploring the behavior of the density profiles, edge currents, and singleparticle correlation functions, we find that the ground state on the cylinder shows all signatures of a fractional quantum Hall state even for large values of the magnetic flux density. Furthermore, we determine the dependence of the correlation functions and edge currents on the interaction strength. We find that depending on the magnetic flux density, the transition toward Laughlin-like behavior can be either smooth or it can happen abruptly for some critical interaction strength

Complex coherent quantum many-body dynamics through dissipation

Nature Communications Springer Nature 10 (2019) 1730

B Buca, D Jaksch, J Tindall

The assumption that physical systems relax to a stationary state in the long-time limit underpins statistical physics and much of our intuitive understanding of scientific phenomena. For isolated systems this follows from the eigenstate thermalization hypothesis. When an environment is present the expectation is that all of phase space is explored, eventually leading to stationarity. Notable exceptions are decoherence-free subspaces that have important implications for quantum technologies. These have been studied for systems with a few degrees of freedom only. Here we identify simple and generic conditions for dissipation to prevent a quantum many-body system from ever reaching a stationary state. We go beyond dissipative quantum state engineering approaches towards controllable long-time non-stationary dynamics typically associated with macroscopic complex systems. This coherent and oscillatory evolution constitutes a dissipative version of a quantum time-crystal. We discuss the possibility of engineering such complex dynamics with fermionic ultracold atoms in optical lattices.

Fluctuations of work in realistic equilibrium states of quantum systems with conserved quantities

SciPost Physics Proceedings SciPost (2019) 1-11

J Mur Petit, A Relaño, RA Molina, D Jaksch

The out-of-equilibrium dynamics of quantum systems is one of the most fascinating problems in physics, with outstanding open questions on issues such as relaxation to equilibrium. An area of particular interest concerns few-body systems, where quantum and thermal fluctuations are expected to be especially relevant. In this contribution, we present numerical results demonstrating the impact of conserved quantities (or ‘charges’) in the outcomes of out-of-equilibrium measurements starting from realistic equilibrium states on a few-body system implementing the Dicke model.

Exact large deviation statistics and trajectory phase transition of a deterministic boundary driven cellular automaton.

Physical review. E 100 (2019) 020103-

B Buča, JP Garrahan, T Prosen, M Vanicat

We study the statistical properties of the long-time dynamics of the rule 54 reversible cellular automaton (CA), driven stochastically at its boundaries. This CA can be considered as a discrete-time and deterministic version of the Fredrickson-Andersen kinetically constrained model (KCM). By means of a matrix product ansatz, we compute the exact large deviation cumulant generating functions for a wide range of time-extensive observables of the dynamics, together with their associated rate functions and conditioned long-time distributions over configurations. We show that for all instances of boundary driving the CA dynamics occurs at the point of phase coexistence between competing active and inactive dynamical phases, similar to what happens in more standard KCMs. We also find the exact finite size scaling behavior of these trajectory transitions, and provide the explicit "Doob-transformed" dynamics that optimally realizes rare dynamical events.

Dissipation induced nonstationarity in a quantum gas

Physical Review Letters American Physical Society 123 (2019) 260401

B Buča, D Jaksch

Nonstationary longtime dynamics was recently observed in a driven two-component Bose-Einstein condensate coupled to an optical cavity [N. Dogra, M. Landini, K. Kroeger, L. Hruby, T. Donner, and T. Esslinger, arXiv:1901.05974] and analyzed in mean-field theory. We solve the underlying model in the thermodynamic limit and show that this system is always dynamically unstable—even when mean-field theory predicts stability. Instabilities always occur in higher-order correlation functions leading to squeezing and entanglement induced by cavity dissipation. The dynamics may be understood as the formation of a dissipative time crystal. We use perturbation theory for finite system sizes to confirm the nonstationary behavior.

Symmetries and conservation laws in quantum trajectories: Dissipative freezing

Physical Review A American Physical Society 100 (2019) 042113

C Sánchez Muñoz, B Buča, J Tindall, A González-Tudela, D Jaksch, D Porras

In driven-dissipative systems, the presence of a strong symmetry guarantees the existence of several steady states belonging to different symmetry sectors. Here we show that, when a system with a strong symmetry is initialized in a quantum superposition involving several of these sectors, each individual stochastic trajectory will randomly select a single one of them and remain there for the rest of the evolution. Since a strong symmetry implies a conservation law for the corresponding symmetry operator on the ensemble level, this selection of a single sector from an initial superposition entails a breakdown of this conservation law at the level of individual realizations. Given that such a superposition is impossible in a classical, stochastic trajectory, this is a a purely quantum effect with no classical analogue. Our results show that a system with a closed Liouvillian gap may exhibit, when monitored over a single run of an experiment, a behaviour completely opposite to the usual notion of dynamical phase coexistence and intermittency, which are typically considered hallmarks of a dissipative phase transition. We discuss our results with a simple, realistic model of squeezed superradiance.

Manipulating quantum materials with quantum light (vol 99, 085116, 2019)

PHYSICAL REVIEW B 99 (2019) ARTN 099907

M Kiffner, JR Coulthard, F Schlawin, A Ardavan, D Jaksch

Diverging exchange force and form of the exact density matrix functional

Physical Review Letters American Physical Society 122 (2019) 013001

C Schilling, R Schilling

For translationally invariant one-band lattice models, we exploit the ab initio knowledge of the natural orbitals to simplify reduced density matrix functional theory (RDMFT). Striking underlying features are discovered: First, within each symmetry sector, the interaction functional F depends only on the natural occupation numbers n. The respective sets P^1_N and E^1_N of pure and ensemble N-representable one-matrices coincide. Second, and most importantly, the exact functional is strongly shaped by the geometry of the polytope E^1_N = P^1_N, described by linear constraints D^{(j)}(n)⩾0. For smaller systems, it follows as F[n]=\sum_{i,i'} V_{i,i'} \sqrt{D^{(i)}(n)D^{(i')}(n)}. This generalizes to systems of arbitrary size by replacing each D^{(i)} by a linear combination of {D^{(j)}(n)} and adding a non-analytical term involving the interaction V. Third, the gradient dF/dn is shown to diverge on the boundary ∂E^1_N, suggesting that the fermionic exchange symmetry manifests itself within RDMFT in the form of an ``exchange force''. All findings hold for systems with non-fixed particle number as well and V can be any p-particle interaction. As an illustration, we derive the exact functional for the Hubbard square.

Manipulating quantum materials with quantum light

Physical Review B American Physical Society 99 (2019) 085116-

M Kiffner, J Coulthard, F Schlawin, A Ardavan, D Jaksch

We show that the macroscopic magnetic and electronic properties of strongly correlated electron systems can be manipulated by coupling them to a cavity mode. As a paradigmatic example we consider the Fermi-Hubbard model and find that the electron-cavity coupling enhances the magnetic interaction between the electron spins in the ground-state manifold. At half filling this effect can be observed by a change in the magnetic susceptibility. At less than half filling, the cavity introduces a next-nearest-neighbor hopping and mediates a long-range electron-electron interaction between distant sites. We study the ground-state properties with tensor network methods and find that the cavity coupling can induce a phase characterized by a momentum-space pairing effect for electrons.

Collimated UV light generation by two-photon excitation to a Rydberg state in Rb vapor

OPTICS LETTERS 44 (2019) 2931-2934

M Lam, SB Pal, T Vogt, C Gross, M Kiffner, W Li

Quantum synchronisation enabled by dynamical symmetries and dissipation

New Journal of Physics IOP Publishing (2019)

J Tindall, CS Munoz, B Buca, D Jaksch

In nature, instances of synchronisation abound across a diverse range of environments. In the quantum regime, however, synchronisation is typically observed by identifying an appropriate parameter regime in a specific system. In this work we show that this need not be the case, identifying symmetry-based conditions which, when satisfied, guarantee completely synchronous, entangled limit cycles between the individual constituents of a generic open quantum system - no restrictions are placed on its microscopic details. We describe these systems as posssessing a strong dynamical symmetry and we prove that, to first order, they are completely robust to symmetry-breaking perturbations. Using these ideas we identify two central examples where synchronisation arises via this qualitatively new mechanism: a chain of quadratically dephased spin-1s and the many-body charge-dephased Hubbard model. In both cases, due to their dynamical symmetries, perfect phase-locking occurs throughout the system, regardless of the specific microscopic parameters or initial states. Furthermore, when these systems are perturbed, their non-linear responses elicit long-lived signatures of both phase and frequency-locking.

Communication: Relating the pure and ensemble density matrix functional

Journal of Chemical Physics AIP Publishing 149 (2018) 231102

C Schilling

A crucial theorem in Reduced Density Matrix Functional Theory (RDMFT) suggests that the universal pure and ensemble functionals coincide on their common domain of pure N-representable one-matrices. We refute this by a comprehensive analysis of the geometric picture underlying Levy’s constrained search. Moreover, we then show that the ensemble functional follows instead as the lower convex envelop of the pure functional. It is particularly remarkable that the pure functional determines the ensemble functional even outside its own domain of pure N-representable one-matrices. From a general perspective, this demonstrates that relaxing pure RDMFT to ensemble RDMFT does not necessarily circumvent the complexity of the one-body pure N-representability conditions (generalized Pauli constraints). Instead, the complexity may simply be transferred from the underlying space of pure N-representable one-matrices to the structure of the universal one-matrix functional