PaperPanorama

HEP Lattice·hep-lat

Tue·Nov 30, 2021

21 papers14 primary·7 cross-listed·reconstructed*

  1. 01*

    Space-time symmetric qubit regularization of the asymptotically free two-dimensional O(4) model

    Junzhe Zhou🇺🇸 · Hersh Singh🇺🇸 · Tanmoy Bhattacharya🇺🇸 · Shailesh Chandrasekharan🇺🇸 · Rajan Gupta🇺🇸

    We explore if space-time symmetric lattice field theory models with a finite Hilbert space per lattice site can reproduce asymptotic freedom in the two-dimensional model. We focus on a simple class of such models with a five dimensional local Hilbert space. We demonstrate how even the simplest model reproduces asymptotic freedom within the D-theory formalism but at the cost of increasing the size of the Hilbert space through coupling several layers of a two-dimensional lattice. We then argue that qubit regularization can be viewed as an effective field theory (EFT) even if the continuum limit cannot be reached, as long as we can tune the model close enough to the continuum limit where perturbation theory, or other analytical techniques, become viable. We construct a simple lattice model on a single layer with a four dimensional local Hilbert space that acts like an excellent EFT of the original theory.

    hep-latcond-mat.str-elhep-thnucl-th+1PRD(2022)·14 citations
  2. 02*

    The lightest resonance from lattice QCD

    Nicolas Lang🇮🇪

    We recently presented elastic scattering from lattice QCD at MeV. The amplitude features a pole corresponding to a mass MeV and a width MeV. The results were compared to an earlier study at a higher pion mass and to a similar study in the charm-strange sector. In this contribution to LATTICE2021 I summarize these results and compare them with experiment, based on the values reported by the particle data group. Our result lies significantly below the experimental . I also relate our findings to recent studies in chiral perturbation theory. Based on work presented in JHEP2021(7),123 for the Hadron Spectrum Collaboration.

    hep-latPoS(2022)·0 citations
  3. 03*

    scattering in partially-quenched twisted-mass chiral perturbation theory

    Zachary T. Draper🇺🇸 · Stephen R. Sharpe🇺🇸

    We study pion-pion scattering in partially-quenched twisted-mass lattice QCD using chiral perturbation theory. The specific partially-quenched setup corresponds to that used in numerical lattice QCD calculations of the scattering length. We study the discretization errors proportional to , with the lattice spacing, and the errors that arise due to the use of Lüscher's two-particle quantization condition in a theory that is not unitary. We argue that the former can be as large as , but explain how they can be systematically subtracted using a calculation of the scattering amplitude in the same partially-quenched framework. We estimate the error from the violation of unitarity to be , and argue that this error will be difficult to reduce in practice.

    hep-latPRD(2022)·8 citations
  4. 04*

    The gradient flow at higher orders in perturbation theory

    Robert Harlander🇩🇪

    Various results for higher-order perturbative calculations in the gradient-flow formalism are reviewed, including the gradient-flow beta function and the small-flow-time expansion of the hadronic vacuum polarization and the energy-momentum tensor. In addition, the strategy of regions is outlined in order to obtain systematic expansions of gradient-flow integrals, for example at large and small flow times.

    hep-lathep-phPoS(2022)·7 citations
  5. 05*

    Non-Perturbative Bounds for Semileptonic Decays in Lattice QCD

    Matteo Di Carlo🇬🇧 · Guido Martinelli🇮🇹 · Manuel Naviglio🇮🇹 · Francesco Sanfilippo🇮🇹 · Silvano Simula🇮🇹 · Ludovico Vittorio🇮🇹

    We present a new method aiming at a non-perturbative, model-independent determination of the momentum dependence of the form factors entering semileptonic decays using unitarity and analyticity constraints. We extend the original proposal and, using suitable two-point functions computed non-perturbatively, we determine the form factors at low-momentum transfer from those computed explicitly on the lattice at large , without making any assumption about their dependence. As a training ground we apply the new method to the analysis of the lattice data of the semileptonic decays obtained both at finite values of the lattice spacing and at the physical pion point in the continuum limit. We show that, starting from a limited set of data at large , it is possible to determine quite precisely the form factors in a model independent way in the full kinematical range, obtaining a remarkable agreement with the direct calculation of the form factors. This finding opens the possibility to obtain non-perturbatively the form factors entering the semileptonic B decays in the full kinematical range.

    hep-lathep-exhep-phPoS(2022)·0 citations
  6. 06*

    Anomaly cancellation condition in lattice effective electroweak theory

    Vieri Mastropietro🇮🇹

    The anomaly cancellation is at the basis of the perturbative consistence of the Standard Model and it provides a partial explanation of charge quantization. We consider an effective Electroweak theory on a lattice, with a quartic interaction describing the weak forces and an interaction with the e.m. field. We prove the validity of the anomaly cancellation at a non perturbative level and with a finite lattice cut-off, even if the lattice breaks some important symmetries, on which perturbative arguments for the cancellation are based. The method of the proof has analogies with the one adopted for establishing universality in transport of quantum materials.

    hep-lathep-thJ.Math.Phys.(2023)·4 citations
  7. 07*

    Progress in lattice gauge theories

    Ed Bennett🇬🇧 · Jack Holligan🇬🇧 · Deog Ki Hong🇰🇷 · Ho Hsiao🇹🇼 · Jong-Wan Lee🇰🇷 · C.-J. David Lin🇹🇼 · Biagio Lucini🇬🇧 · Michele Mesiti🇬🇧 · Maurizio Piai🇬🇧 · Davide Vadacchino🇮🇪

    Lattice studies of gauge theories with symplectic gauge groups provide valuable information about gauge dynamics, and complement the results of lattice investigations focused on unitary gauge groups. These theories play a central role in phenomenological contexts such as composite Higgs and strongly interacting dark matter models. We report on recent progress of our lattice research programme, starting from the glueball mass spectrum and the topology of the pure gauge theory. We present our results on the mass spectrum of mesons in the quenched approximation, by varying the number of colours in the symplectic group. For the theory, we focus on results obtained with dynamical fermion matter content comprising both fundamental and 2-index antisymmetric representations of the gauge group, as dictated by a well known model of composite Higgs with partial top compositeness.

    hep-lathep-phhep-thPoS(2022)·21 citations
  8. 08*

    Progress in the determination of Mellin moments of the pion LCDA using the HOPE method

    William Detmold🇺🇸 · Anthony V. Grebe🇺🇸 · Issaku Kanamori🇯🇵 · C.-J. David Lin🇹🇼 · Santanu Mondal🇺🇸 · Robert J. Perry🇹🇼 · Yong Zhao🇺🇸

    The pion light-cone distribution amplitude (LCDA) is a central non-perturbative object of interest for the calculation of high-energy exclusive processes in quantum chromodynamics. In this article, we discuss the calculation of the second and fourth Mellin moment of the pion LCDA using a heavy-quark operator product expansion. The resulting value for the second Mellin moment is . This result is compatible with those from previous determinations of this quantity.

    hep-lathep-phnucl-thPoS(2022)·4 citations
  9. 09*

    Perturbative predictions for color superconductivity on the lattice

    Takeru Yokota🇯🇵 · Yuhma Asano🇯🇵 · Yuta Ito🇯🇵 · Hideo Matsufuru🇯🇵 · Yusuke Namekawa🇯🇵 · Jun Nishimura🇯🇵 · Asato Tsuchiya🇯🇵 · Shoichiro Tsutsui🇯🇵

    We develop a new method to investigate color superconductivity (CSC) on the lattice based on the Thouless criterion, which amounts to solving the linearized gap equation without imposing any ansatz on the structure of the Cooper pairs. We perform explicit calculations at the one-loop level with the staggered fermions on a lattice and the Wilson fermions on a lattice, which enables us to obtain the critical as a function of the quark chemical potential , below which the CSC phase is expected to appear. The obtained critical has sharp peaks at the values of corresponding to the discretized energy levels of quarks similarly to what was observed in previous studies on simplified effective models. From the solution to the linearized gap equation, one can read off the flavor and spatial structures of the Cooper pairs at the critical . In the case of massless staggered fermion, in particular, we find that the chiral symmetry of the staggered fermions is spontaneously broken by the condensation of the Cooper pairs.

    hep-lathep-phPoS(2022)·3 citations
  10. 10*

    The basics and applications of the tempered Lefschetz thimble method for the numerical sign problem

    Masafumi Fukuma🇯🇵 · Nobuyuki Matsumoto🇺🇸

    The numerical sign problem has long been a major obstacle to first-principles calculations in various important fields of physics. We report that the recently proposed algorithm, tempered Lefschetz thimble method (TLTM), and its worldvolume extension (WV-TLTM) can be a promising solution in its trustability and versatility.

    hep-lathep-thPoS(2022)·1 citation
  11. 11*

    Worldvolume tempered Lefschetz thimble method and its error estimation

    Masafumi Fukuma🇯🇵 · Nobuyuki Matsumoto🇺🇸 · Yusuke Namekawa🇯🇵

    The worldvolume tempered Lefschetz thimble method (WV-TLTM) is an algorithm towards solving the sign problem, where hybrid Monte Carlo updates are performed on a continuous accumulation of flowed surfaces foliated by the anti-holomorphic gradient flow (the worldvolume of integration surface). Sharing the advantage with the original tempered Lefschetz thimble method (TLTM) that the sign problem is resolved without introducing the ergodicity problem, the new algorithm is expected to significantly reduce the computational cost, because it eliminates the need to compute the Jacobian of the flow in generating a configuration. We demonstrate the effectiveness of the WV-TLTM with its successful application to the Stephanov model (a chiral random matrix model), for which the complex Langevin method is known to suffer from a serious wrong convergence problem. We also discuss the statistical analysis method for the WV-TLTM.

    hep-lathep-thPoS(2022)·1 citation
  12. 12*

    Estimates for the lightest baryon masses in supersymmetric Yang-Mills theory

    Sajid Ali🇩🇪 · Georg Bergner🇩🇪 · Camilo Lopez🇩🇪 · Istvan Montvay🇩🇪 · Gernot Münster🇩🇪 · Stefano Piemonte🇩🇪

    supersymmetric Yang-Mills theory describes gluons interacting with gluinos, which are spin- Majorana particles in the adjoint representation of the gauge group. In addition to glueballs and mesonic bound states, the theory contains color neutral bound states of three gluinos, which are analogous to baryons in QCD. We calculate their correlation functions, involving ``sunset diagrams'' and ``spectacle diagrams'', numerically for gauge group SU(2) and present an update on the estimates for the lowest masses.

    hep-lathep-phPoS(2021)·2 citations
  13. 13*

    Taylor expansions and Padé approximations for Lefschetz thimbles and beyond

    Kevin Zambello🇮🇹 · Francesco Di Renzo🇮🇹 · Simran Singh🇮🇹

    Deforming the domain of integration after complexification of the field variables is an intriguing idea to tackle the sign problem. In thimble regularization the domain of integration is deformed into an union of manifolds called Lefschetz thimbles. On each thimble the imaginary part of the action stays constant and the sign problem disappears. A long standing issue of this approach is how to determine the relative weight to assign to each thimble contribution in the (multi)-thimble decomposition. Yet this is an issue one has to face, as previous work has shown that different theories exist for which the contributions coming from thimbles other than the dominant one cannot be neglected. Historically, one of the first examples of such theories is the one-dimensional Thirring model. Here we discuss how Taylor expansions can be used to by-pass the need for multi-thimble simulations. If multiple, disjoint regions can be found in the parameters space of the theory where only one thimble gives a relevant contribution, multiple Taylor expansions can be carried out in those regions to reach other regions by single thimble simulations. Better yet, these Taylor expansions can be bridged by Padé interpolants. Not only does this improve the convergence properties of the series, but it also gives access to information about the analytical structure of the observables. The true singularities of the observables can be recovered. We show that this program can be applied to the one-dimensional Thirring model and to a (simple) version of HDQCD. But the general idea behind our strategy can be helpful beyond thimble regularization itself, i.e. it could be valuable in studying the singularities of QCD in the complex plane. Indeed this is a program that is currently being carried out by the Bielefeld-Parma collaboration.

    hep-latPoS(2022)·1 citation
  14. 14*

    Gradient flow scale-setting with Wilson-clover twisted-mass fermions

    Constantia Alexandrou🇨🇾 · Simone Bacchio🇨🇾 · Georg Bergner🇩🇪 · Petros Dimopoulos🇮🇹 · Jacob Finkenrath🇨🇾 · Roberto Frezzotti🇮🇹 · Marco Garofalo🇩🇪 · Bartosz Kostrzewa🇩🇪 · Giannis Koutsou🇨🇾 · Peter Labus🇩🇪 · Francesco Sanfilippo🇮🇹 · Silvano Simula🇮🇹 and 3 other authors

    We present a determination of the gradient flow scales , and in isosymmetric QCD, making use of the gauge ensembles produced by the Extended Twisted Mass Collaboration (ETMC) with flavours of Wilson-clover twisted-mass quarks including configurations close to the physical point for all dynamical flavours. The simulations are carried out at three values of the lattice spacing and the scale is set through the PDG value of the pion decay constant, yielding fm, fm and fm. Finally, fixing the kaon mass to its isosymmetric value, we determine the ratio of the kaon and pion leptonic decay constants to be .

    hep-latPoS(2022)·3 citations
  15. 15*

    Neural network evidence of a weakly first order phase transition for the two-dimensional 5-state Potts model

    Yuan-Heng Tseng🇹🇼 · Yun-Hsuan Tseng · Fu-Jiun Jiang🇹🇼

    A universal (supervised) neural network (NN), which is only trained once on a one-dimensional lattice of 200 sites, is employed to study the phase transition of the two-dimensional (2D) 5-state ferromagnetic Potts model on the square lattice. In particular, the NN is obtained by using merely two artificially made configurations as the training set. Due to the elegant features of the considered NN, results associated with systems consisting of over 4000000 spins can be obtained with ease, and convincing evidence showing the investigated phase transition is weakly first order is reached. The outcomes demonstrated here can hardly be achieved with the standard NNs that are commonly used in the literature.

    cond-mat.stat-mechcond-mat.dis-nnhep-latphysics.comp-phEur.Phys.J.Plus(2022)·1 citation
  16. 16*

    Perturbative quantum Monte Carlo method for nuclear physics

    Bing-Nan Lu🇨🇳 · Ning Li🇨🇳 · Serdar Elhatisari🇹🇷 · Yuan-Zhuo Ma🇨🇳 · Dean Lee🇺🇸 · Ulf-G. Meißner🇩🇪

    While first order perturbation theory is routinely used in quantum Monte Carlo (QMC) calculations, higher-order terms present significant numerical challenges. We present a new approach for computing perturbative corrections in projection QMC calculations. We demonstrate the method by computing nuclear ground state energies up to second order for a realistic chiral interaction. We calculate the binding energies of several light nuclei up to O by expanding the Hamiltonian around the Wigner SU(4) limit and find good agreement with data. In contrast to the natural ordering of the perturbative series, we find remarkably large second order energy corrections. This occurs because the perturbing interactions break the symmetries of the unperturbed Hamiltonian. Our method is free from the sign problem and can be applied to QMC calculations for many-body systems in nuclear physics, condensed matter physics, ultracold atoms, and quantum chemistry.

    nucl-thcond-mat.str-elhep-latPRL(2022)·48 citations
  17. 17*

    On the -Quark Potential in String Models

    Oleg Andreev🇷🇺

    We propose a string theory construction for the system of two heavy quarks and two light antiquarks. The potential of the system is a function of separation between the quarks. We define a critical separation distance below which the system can be thought of mainly as a compact tetraquark. The results show the universality of the string tension and factorization at small separations expected from heavy quark-diquark symmetry. Our estimate of the screening length is in the range of lattice QCD. We also make a comparison with the potential of the system. The potentials look very similar at small quark separations but at larger separations they differ. The reason for this is that the flattening of the potentials happens at two well-separated scales as follows from the two different mechanisms: string breaking by light quarks for and string junction annihilation for . Moreover, a similar construction can also be applied to the system.

    hep-phhep-lathep-thnucl-thPRD(2022)·27 citations
  18. 18*

    The Chiral Gross-Neveu model on the lattice via a Landau-forbidden phase transition

    Gertian Roose🇧🇪 · Jutho Haegeman🇧🇪 · Karel Van Acoleyen🇧🇪 · Laurens Vanderstraeten🇧🇪 · Nick Bultinck🇧🇪

    We study the phase diagram of the -dimensional Gross-Neveu model with both and interaction terms on a spatial lattice. The continuous chiral symmetry, which is present in the continuum model when , has a mixed 't~Hooft anomaly with the charge conservation symmetry, which guarantees the existence of a massless mode. However, the same 't~Hooft anomaly also implies that the continuous chiral symmetry is broken explicitly in our lattice model. Nevertheless, from numerical matrix product state simulations we find that, for certain parameters of the lattice model, the continuous chiral symmetry reemerges in the infrared fixed point theory, even at strong coupling. We argue that, to understand this phenomenon, it is crucial to go beyond mean-field theory (or, equivalently, beyond the leading order term in a expansion). Interestingly, on the lattice, the chiral Gross-Neveu model appears at a Landau-forbidden second order phase transition separating two distinct and unrelated symmetry-breaking orders. We point out the crucial role of two different 't Hooft anomalies or Lieb-Schultz-Mattis obstructions for this Landau-forbidden phase transition to occur.

    hep-thcond-mat.str-elhep-latJHEP(2022)·4 citations
  19. 19*

    Metropolis-style random sampling of quantum gates for the estimation of low-energy observables

    Judah F. Unmuth-Yockey🇺🇸

    We propose a quantum algorithm to compute low-energy expectation values of a quantum Hamiltonian by sampling a partition function associated with the average energy of that Hamiltonian. For any given quantum circuit-Hamiltonian pair, there is an associated average energy. The sampling is done through an accept/reject Metropolis-style algorithm on the quantum gates of the circuit itself. Observables calculated under the canonical ensemble from these samples of circuits are extrapolated from higher-energies to the ground state.

    quant-phhep-latPRD(2022)·4 citations
  20. 20*

    Spin Networks, Wilson Loops and 3nj Wigner Identities

    Manu Mathur🇮🇳 · Atul Rathor🇮🇳

    We exploit the spin network properties of the magnetic eigenstates of SU(2) Hamiltonian lattice gauge theory and use the Wilson loop operators to obtain a wide class of new identities amongst 3nj Wigner coefficients. We also show that the topological ground states of the SU(2) toric code Hamiltonian lead to Wigner 3nj identities with non-trivial phases. The method is very general and involves only the eigenvalue equations of any gauge invariant operator and their solutions. Therefore, it can be extended to any higher dimensional spin networks as well as larger SU(N) groups.

    math-phhep-lathep-thmath.MP0 citations
  21. 21*

    Reconstructing spectral functions via automatic differentiation

    Lingxiao Wang🇩🇪 · Shuzhe Shi🇨🇦 · Kai Zhou🇩🇪

    Reconstructing spectral functions from Euclidean Green's functions is an important inverse problem in many-body physics. However, the inversion is proved to be ill-posed in the realistic systems with noisy Green's functions. In this Letter, we propose an automatic differentiation(AD) framework as a generic tool for the spectral reconstruction from propagator observable. Exploiting the neural networks' regularization as a non-local smoothness regulator of the spectral function, we represent spectral functions by neural networks and use the propagator's reconstruction error to optimize the network parameters unsupervisedly. In the training process, except for the positive-definite form for the spectral function, there are no other explicit physical priors embedded into the neural networks. The reconstruction performance is assessed through relative entropy and mean square error for two different network representations. Compared to the maximum entropy method, the AD framework achieves better performance in the large-noise situation. It is noted that the freedom of introducing non-local regularization is an inherent advantage of the present framework and may lead to substantial improvements in solving inverse problems.

    hep-phcs.LGhep-latPRD(2022)·45 citations

* Reconstructed cohort: no mailing for this day survives in the archive. Papers are grouped by their submission times and arXiv's announcement cut-off, assuming announcement without delay; positions follow identifier order. Validated at ~91% exact-day agreement against the archived era.