Publications year: 2023 2022 2021 2020 2019 2018
Villain model with long-range couplings
Giachetti G., Defenu N., Ruffo S., Trombettoni A.
The nearest-neighbor Villain, or periodic Gaussian, model is a useful tool to understand the physics of the topological defects of the two-dimensional nearest-neighbor XY model, as the two models share the same symmetries and are in the same universality class. The long-range counterpart of the two-dimensional XY has been recently shown to exhibit a non-trivial critical behavior, with a complex phase diagram including a range of values of the power-law exponent of the couplings decay, σ, in which there are a magnetized, a disordered and a critical phase [1]. Here we address the issue of whether the critical behavior of the two-dimensional XY model with long-range couplings can be described by the Villain counterpart of the model. After introducing a suitable generalization of the Villain model with long-range couplings, we derive a set of renormalization-group equations for the vortex-vortex potential, which differs from the one of the long-range XY model, signaling that the decoupling of spin-waves and topological defects is no longer justified in this regime. The main results are that for σ < 2 the two models no longer share the same universality class. Remarkably, within a large region of its the phase diagram, the Villain model is found to behave similarly to the one-dimensional Ising model with 1/r2 interactions.
Erratum: Entanglement transitions from stochastic resetting of non-Hermitian quasiparticles (Phys. Rev. B (2022) 105 (L241114) DOI: 10.1103/PhysRevB.107.L241114)
Turkeshi X., Dalmonte M., Fazio R., Schirò M.
Our paper introduced a phenomenological quasiparticle picture describing monitored many-body systems. A central point of our work is that the system's non-Hermitian Hamiltonian (nHH) quasiparticles reveal insights into the measurement-induced phases. In particular, the quasiparticle picture explains the emergence of a logarithmic phase in noninteracting monitored fermions when the nHH gap is closed and an area-law phase when the nHH gap is open [a fact numerically observed in a variety of works (see, e.g., Ref. [1])] To qualitatively support our claims, we have introduced an archetypal model: the transverse field Ising chain under quantum jumps monitoring of the transverse magnetization. Here, the correlation matrix fully captures the dynamics by the system's Gaussianity. (Figure Presented). In conclusion, the new analysis confirms the qualitative description given by the quasiparticle picture for monitored fermionic systems in a wide range of parameters, provided finite-size effects are considered. We are grateful to A. Paviglianiti and A. Silva for pointing out a problem in our original numerical implementation.
Underground Tests of Quantum Mechanics by the VIP Collaboration at Gran Sasso
Napolitano F., Addazi A., Bassi A., Bazzi M., Bragadireanu M., Cargnelli M., Clozza A., De Paolis L., Del Grande R., Derakhshani M., Donadi S., Fiorini C., Guaraldo C., Iliescu M., Laubenstein M., Manti S., Marcianò A., Marton J., Miliucci M., Milotti E., Piscicchia K., Porcelli A., Scordo A., Sgaramella F., Sirghi D.L., Sirghi F., Doce O.V., Zmeskal J., Curceanu C.
Modern physics lays its foundations on the pillars of Quantum Mechanics (QM), which has been proven successful to describe the microscopic world of atoms and particles, leading to the construction of the Standard Model. Despite the big success, the old open questions at its very heart, such as the measurement problem and the wave function collapse, are still open. Various theories consider scenarios which could encompass a departure from the predictions of the standard QM, such as extra-dimensions or deformations of the Lorentz/Poincaré symmetries. At the Italian National Gran Sasso underground Laboratory LNGS, we search for evidence of new physics proceeding from models beyond standard QM, using radiation detectors. Collapse models addressing the foundations of QM, such as the gravity-related Diósi–Penrose (DP) and Continuous Spontaneous Localization (CSL) models, predict the emission of spontaneous radiation, which allows experimental tests. Using a high-purity Germanium detector, we could exclude the natural parameterless version of the DP model and put strict bounds on the CSL one. In addition, forbidden atomic transitions could prove a possible violation of the Pauli Exclusion Principle (PEP) in open and closed systems. The VIP-2 experiment is currently in operation, aiming at detecting PEP-violating signals in Copper with electrons; the VIP-3 experiment upgrade is foreseen to become operative in the next few years. We discuss the VIP-Lead experiment on closed systems, and the strong bounds it sets on classes of non-commutative quantum gravity theories, such as the (Formula presented.) –Poincaré theory.
A Novel Approach to Parameter Determination of the Continuous Spontaneous Localization Collapse Model
Piscicchia K., Porcelli A., Bassi A., Bazzi M., Bragadireanu M., Cargnelli M., Clozza A., De Paolis L., Del Grande R., Derakhshani M., Lajos D., Donadi S., Guaraldo C., Iliescu M., Laubenstein M., Manti S., Marton J., Miliucci M., Napolitano F., Scordo A., Sgaramella F., Sirghi D.L., Sirghi F., Vazquez Doce O., Zmeskal J., Curceanu C.
Models of dynamical wave function collapse consistently describe the breakdown of the quantum superposition with the growing mass of the system by introducing non-linear and stochastic modifications to the standard Schrödinger dynamics. Among them, Continuous Spontaneous Localization (CSL) was extensively investigated both theoretically and experimentally. Measurable consequences of the collapse phenomenon depend on different combinations of the phenomenological parameters of the model—the strength (Formula presented.) and the correlation length (Formula presented.) —and have led, so far, to the exclusion of regions of the admissible ((Formula presented.)) parameters space. We developed a novel approach to disentangle the (Formula presented.) and (Formula presented.) probability density functions, which discloses a more profound statistical insight.
Multicriticality in Yang-Lee edge singularity
Lencsés M., Miscioscia A., Mussardo G., Takács G.
In this paper we study the non-unitary deformations of the two-dimensional Tricritical Ising Model obtained by coupling its two spin ℤ2 odd operators to imaginary magnetic fields. Varying the strengths of these imaginary magnetic fields and adjusting correspondingly the coupling constants of the two spin ℤ2 even fields, we establish the presence of two universality classes of infrared fixed points on the critical surface. The first class corresponds to the familiar Yang-Lee edge singularity, while the second class to its tricritical version. We argue that these two universality classes are controlled by the conformal non-unitary minimal models M(2, 5) and M(2, 7) respectively, which is supported by considerations based on PT symmetry and the corresponding extension of Zamolodchikov’s c-theorem, and also verified numerically using the truncated conformal space approach. Our results are in agreement with a previous numerical study of the lattice version of the Tricritical Ising Model [1]. We also conjecture the classes of universality corresponding to higher non-unitary multicritical points obtained by perturbing the conformal unitary models with imaginary coupling magnetic fields.
Deploying an Inter-European Quantum Network
Ribezzo D., Zahidy M., Vagniluca I., Biagi N., Francesconi S., Occhipinti T., Oxenløwe L.K., Lončarić M., Cvitić I., Stipčević M., Pušavec Ž., Kaltenbaek R., Ramšak A., Cesa F., Giorgetti G., Scazza F., Bassi A., De Natale P., Cataliotti F.S., Inguscio M., Bacco D., Zavatta A.
Around 40 years have passed since the first pioneering works introduced the possibility of using quantum physics to enhance communications safety. Nowadays, quantum key distribution (QKD) exited the physics laboratories to become a mature technology, triggering the attention of States, military forces, banks, and private corporations. This work takes on the challenge of bringing QKD closer to a consumer technology: deployed optical fibers by telecommunication companies of different States have been used to realize a quantum network, the first-ever connecting three different countries. This work also emphasizes the necessity of networks where QKD can come up besides classical communications, whose coexistence currently represents the main limitation of this technology. This network connects Trieste to Rijeka and Ljubljana via a trusted node in Postojna. A key rate of over 3 kbps in the shortest link and a 7-hour-long measurement demonstrate the system's stability and reliability. The network has been used to present the QKD at the G20 Digital Ministers' Meeting in Trieste. The experimental results, together with the interest that one of the most important events of international politics has attracted, showcase the maturity of the QKD technology bundle, placing it in the spotlight for consumer applications in the near term.
Tunable critical Casimir forces counteract Casimir–Lifshitz attraction
Schmidt F., Callegari A., Daddi-Moussa-Ider A., Munkhbat B., Verre R., Shegai T., Käll M., Löwen H., Gambassi A., Volpe G.
In developing micro- and nanodevices, stiction between their parts, that is, static friction preventing surfaces in contact from moving, is a well-known problem. It is caused by the finite-temperature analogue of the quantum electrodynamical Casimir–Lifshitz forces, which are normally attractive. Repulsive Casimir–Lifshitz forces have been realized experimentally, but their reliance on specialized materials severely limits their applicability and prevents their dynamic control. Here we demonstrate that repulsive critical Casimir forces, which emerge in a critical binary liquid mixture upon approaching the critical temperature, can be used to counteract stiction due to Casimir–Lifshitz forces and actively control microscopic and nanoscopic objects with nanometre precision. Our experiment is conducted on a microscopic gold flake suspended above a flat gold-coated substrate immersed in a critical binary liquid mixture. This may stimulate the development of micro- and nanodevices by preventing stiction as well as by providing active control and precise tunability of the forces acting between their constituent parts.
Fractional dynamics and modulational instability in long-range Heisenberg chains
Laetitia M.Y., Nguenang J.P., Paglan P.A., Dauxois T., Trombettoni A., Ruffo S.
We study the effective dynamics of ferromagnetic spin chains in presence of long-range interactions. We consider the Heisenberg Hamiltonian in one dimension for which the spins are coupled through power-law long-range exchange interactions with exponent α. We add to the Hamiltonian an anisotropy in the z-direction. In the framework of a semiclassical approach, we use the Holstein–Primakoff transformation to derive an effective long-range discrete nonlinear Schrödinger equation. We then perform the continuum limit and we obtain a fractional nonlinear Schrödinger-like equation. Finally, we study the modulational instability of plane-waves in the continuum limit and we prove that, at variance with the short-range case, plane waves are modulationally unstable for α<3. We also study the dependence of the modulation instability growth rate and critical wave-number on the parameters of the Hamiltonian and on the exponent α.
Fundamental Problems in Statistical Physics XV—Preface
Rosso A., Speck T., Gambassi A.
Quantum phase diagram of high-pressure hydrogen
Monacelli L., Casula M., Nakano K., Sorella S., Mauri F.
Hydrogen is the most abundant element in the Universe. However, understanding the properties of dense hydrogen is still an open challenge because—under megabar pressures—the quantum nature of both electrons and protons emerges, producing deviations from the common behaviour of condensed-matter systems. Experiments are challenging and can access only limited observables, and the interplay between electron correlation and nuclear quantum motion makes standard simulations unreliable. Here we present the computed phase diagram of hydrogen and deuterium at low temperatures and high pressures using state-of-the-art methods to describe both many-body electronic correlation and quantum anharmonic motion of protons. Our results show that the long-sought atomic metallic hydrogen phase—predicted to host room-temperature superconductivity—forms at 577(4) GPa. The anharmonic vibrations of nuclei pushes the stability of this phase towards pressures much larger than previous estimates or attained experimental values. Before atomization, molecular hydrogen transforms from a metallic phase (phase III) to another metallic structure that is still molecular (phase VI) at 410(20) GPa. Isotope effects increase the pressures of both transitions by 63 and 32 GPa, respectively. We predict signatures in optical spectroscopy and d.c. conductivity that can be experimentally used to distinguish between the two structural transitions.
Entanglement and negativity Hamiltonians for the massless Dirac field on the half line
Rottoli F., Murciano S., Tonni E., Calabrese P.
We study the ground-state entanglement Hamiltonian of several disjoint intervals for the massless Dirac fermion on the half-line. Its structure consists of a local part and a bi-local term that couples each point to another one in each other interval. The bi-local operator can be either diagonal or mixed in the fermionic chiralities and it is sensitive to the boundary conditions. The knowledge of such entanglement Hamiltonian is the starting point to evaluate the negativity Hamiltonian, i.e. the logarithm of the partially transposed reduced density matrix, which is an operatorial characterisation of entanglement of subsystems in mixed states. We find that the negativity Hamiltonian inherits the structure of the corresponding entanglement Hamiltonian. We finally show how the continuum expressions for both these operators can be recovered from exact numerical computations in free-fermion chains.
Interface dynamics in the two-dimensional quantum Ising model
Balducci F., Gambassi A., Lerose A., Scardicchio A., Vanoni C.
In a recent paper [Phys. Rev. Lett. 129, 120601 (2022)0031-900710.1103/PhysRevLett.129.120601], we have shown that the dynamics of interfaces, in the symmetry-broken phase of the two-dimensional ferromagnetic quantum Ising model, displays a robust form of ergodicity breaking. In this paper, we elaborate more on the issue. First, we discuss two classes of initial states on the square lattice, the dynamics of which is driven by complementary terms in the effective Hamiltonian and may be solved exactly: (a) Strips of consecutive neighboring spins aligned in the opposite direction of the surrounding spins and (b) a large class of initial states, characterized by the presence of a well-defined "smooth"interface separating two infinitely extended regions with oppositely aligned spins. The evolution of the latter states can be mapped onto that of an effective one-dimensional fermionic chain, which is integrable in the infinite-coupling limit. In this case, deep connections with noteworthy results in mathematics emerge, as well as with similar problems in classical statistical physics. We present a detailed analysis of the evolution of these interfaces both on the lattice and in a suitable continuum limit, including the interface fluctuations and the dynamics of entanglement entropy. Second, we provide analytical and numerical evidence supporting the conclusion that the observed nonergodicity - arising from Stark localization of the effective fermionic excitations - persists away from the infinite-Ising-coupling limit, and we highlight the presence of a timescale T∼ecLlnL for the decay of a region of large linear size L. The implications of our work for the classic problem of the decay of a false vacuum are also discussed.
Slow melting of a disordered quantum crystal
Balducci F., Scardicchio A., Vanoni C.
The melting of the corner of a crystal is a classical, real-world, nonequilibrium statistical mechanics problem which has shown several connections with other branches of physics and mathematics. For a perfect, classical crystal in two and three dimensions the solution is known: The crystal melts reaching a certain asymptotic shape, which keeps expanding ballistically. In this paper, we move onto the quantum realm and show that the presence of quenched disorder slows down severely the melting process. Nevertheless, we show that there is no many-body localization transition, which could impede the crystal to be completely eroded. We prove such claim both by a perturbative argument, using the forward approximation, and via numerical simulations. At the same time we show how, despite the lack of localization, the erosion dynamics is slowed from ballistic to logarithmic, therefore pushing the complete melting of the crystal to extremely long timescales.
Publications year: 2023 2022 2021 2020 2019 2018

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