Search results for " Field theory"

showing 10 items of 1137 documents

Quantum transport and the phase space structure of the Wightman functions

2019

We study the phase space structure of exact quantum Wightman functions in spatially homogeneous, temporally varying systems. In addition to the usual mass shells, the Wightman functions display additional coherence shells around zero frequency $k_0=0$, which carry the information of the local quantum coherence of particle-antiparticle pairs. We find also other structures, which encode non-local correlations in time, and discuss their role and decoherence. We give a simple derivation of the cQPA formalism, a set of quantum transport equations, that can be used to study interacting systems including the local quantum coherence. We compute quantum currents created by a temporal change in a par…

High Energy Physics - TheoryNuclear and High Energy PhysicsAstrophysics and AstronomyLEPTOGENESISCosmology and Nongalactic Astrophysics (astro-ph.CO)Quantum decoherencegr-qcFOS: Physical sciencesSemiclassical physicsGeneral Relativity and Quantum Cosmology (gr-qc)114 Physical sciences01 natural sciencesGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityThermal Field Theory010306 general physicsQuantumELECTROWEAK BARYOGENESISParticle Physics - PhenomenologyPhysicsThermal quantum field theory010308 nuclear & particles physicsGeneral Relativity and Cosmologyhep-thhep-phFermionFERMIONSBaryogenesisHigh Energy Physics - PhenomenologyCP violationClassical mechanicsHigh Energy Physics - Theory (hep-th)Phase spaceastro-ph.COlcsh:QC770-798Quantum Dissipative SystemsParticle Physics - TheoryAstrophysics - Cosmology and Nongalactic AstrophysicsCoherence (physics)
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Efficient resummation of high post-Newtonian contributions to the binding energy

2021

A factorisation property of Feynman diagrams in the context the Effective Field Theory approach to the compact binary problem has been recently employed to efficiently determine the static sector of the potential at fifth post-Newtonian (5PN) order. We extend this procedure to the case of non-static diagrams and we use it to fix, by means of elementary algebraic manipulations, the value of more than one thousand diagrams at 5PN order, that is a substantial fraction of the diagrams needed to fully determine the dynamics at 5PN. This procedure addresses the redundancy problem that plagues the computation of the binding energy with respect to more "efficient" observables like the scattering an…

High Energy Physics - TheoryNuclear and High Energy PhysicsBlack HolesComputationFOS: Physical sciencesBinary numberContext (language use)General Relativity and Quantum Cosmology (gr-qc)01 natural sciencesGeneral Relativity and Quantum Cosmologysymbols.namesake0103 physical sciencesEffective field theoryFeynman diagramlcsh:Nuclear and particle physics. Atomic energy. RadioactivityStatistical physicsAlgebraic numberResummation010306 general physicsPhysics010308 nuclear & particles physicsEffective Field TheoriesObservableHigh Energy Physics - Theory (hep-th)symbolslcsh:QC770-798Classical Theories of GravityJournal of High Energy Physics
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Non-equilibrium dynamics of a scalar field with quantum backreaction

2021

We study the dynamical evolution of coupled one- and two-point functions of a scalar field in the 2PI framework at the Hartree approximation, including backreaction from out-of-equilibrium modes. We renormalize the 2PI equations of motion in an on-shell scheme in terms of physical parameters. We present the Hartree-resummed renormalized effective potential at finite temperature and critically discuss the role of the effective potential in a non-equilibrium system. We follow the decay and thermalization of a scalar field from an initial cold state with all energy stored in the potential, into a fully thermalized system with a finite temperature. We identify the non-perturbative processes of …

High Energy Physics - TheoryNuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)quantum dissipative systemsFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)QC770-798hiukkasfysiikkakosmologia114 Physical sciences01 natural sciencesGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)Nuclear and particle physics. Atomic energy. Radioactivity0103 physical sciencesThermal Field Theory010306 general physics010308 nuclear & particles physicsthermal field theoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)Nonperturbative Effectsnonperturbative effectskvanttikenttäteoriaQuantum Dissipative SystemsAstrophysics - Cosmology and Nongalactic AstrophysicsJournal of High Energy Physics
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Hawking radiation correlations in Bose-Einstein condensates using quantum field theory in curved space

2013

The density-density correlation function is computed for the Bogoliubov pseudoparticles created in a Bose-Einstein condensate undergoing a black hole flow. On the basis of the gravitational analogy, the method used relies only on quantum field theory in curved spacetime techniques. A comparison with the results obtained by ab initio full condensed matter calculations is given, confirming the validity of the approximation used, provided the profile of the flow varies smoothly on scales compared to the condensate healing length.

High Energy Physics - TheoryNuclear and High Energy PhysicsHAWKING RADIATION[PHYS.COND.GAS]Physics [physics]/Condensed Matter [cond-mat]/Quantum Gases [cond-mat.quant-gas]Black-hole evaporationFOS: Physical sciencesGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesCONDENSATI DI BOSE EINSTEINGeneral Relativity and Quantum Cosmologylaw.inventionGravitationGeneral Relativity and Quantum CosmologyCorrelation functionlawQuantum mechanics0103 physical sciencesQuantum field theory010306 general physicsCurved spaceCondensed Matter::Quantum GasesPhysicsQuantum field theory in curved spacetime[PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]Condensed Matter::Other010308 nuclear & particles physicsBlack holeHigh Energy Physics - Theory (hep-th)Quantum Gases (cond-mat.quant-gas)[PHYS.GRQC]Physics [physics]/General Relativity and Quantum Cosmology [gr-qc]Condensed Matter - Quantum GasesBose–Einstein condensateAnalog gravityHawking radiationPhysical Review D
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A non-perturbative study of massive gauge theories

2013

We consider a non-perturbative formulation of an SU(2) massive gauge theory on a space-time lattice, which is also a discretised gauged non-linear chiral model. The lattice model is shown to have an exactly conserved global SU(2) symmetry. If a scaling region for the lattice model exists and the lightest degrees of freedom are spin one vector particles with the same quantum numbers as the conserved current, we argue that the most general effective theory describing their low-energy dynamics must be a massive gauge theory. We present results of a exploratory numerical simulation of the model and find indications for the presence of a scaling region where both a triplet vector and a scalar re…

High Energy Physics - TheoryNuclear and High Energy PhysicsHiggs PhysicsHigh Energy Physics::Latticehep-latFOS: Physical sciences01 natural sciencesTheoretical physicsHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Lattice (order)0103 physical sciencesEffective field theoryGauge theory010306 general physicsConserved currentScalingLattice Gauge Field TheoriesPhysics010308 nuclear & particles physicshep-thHigh Energy Physics - Lattice (hep-lat)Físicahep-phQuantum numberHigh Energy Physics - PhenomenologyChiral modelHigh Energy Physics - Theory (hep-th)Gauge SymmetryNon-perturbativeSigma Models
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Derivation of spontaneously broken gauge symmetry from the consistency of effective field theory II: Scalar field self-interactions and the electroma…

2019

We extend our study of deriving the local gauge invariance with spontaneous symmetry breaking in the context of an effective field theory by considering self-interactions of the scalar field and inclusion of the electromagnetic interaction. By analyzing renormalizability and the scale separation conditions of three-, four- and five-point vertex functions of the scalar field, we fix the two couplings of the scalar field self-interactions of the leading order Lagrangian. Next we add the electromagnetic interaction and derive conditions relating the magnetic moment of the charged vector boson to its charge and the masses of the charged and neutral massive vector bosons to each other and the tw…

High Energy Physics - TheoryNuclear and High Energy PhysicsNuclear TheorySpontaneous symmetry breakingFOS: Physical sciences01 natural sciencesStandard ModelVector bosonNuclear Theory (nucl-th)Theoretical physicsHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective field theoryddc:530Gauge theory010306 general physicsGauge symmetryPhysics010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics - Lattice (hep-lat)lcsh:QC1-999High Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)Scalar fieldlcsh:Physics
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Derivation of spontaneously broken gauge symmetry from the consistency of effective field theory I: Massive vector bosons coupled to a scalar field

2018

We revisit the problem of deriving local gauge invariance with spontaneous symmetry breaking in the context of an effective field theory. Previous derivations were based on the condition of tree-order unitarity. However, the modern point of view considers the Standard Model as the leading order approximation to an effective field theory. As tree-order unitarity is in any case violated by higher-order terms in an effective field theory, it is instructive to investigate a formalism which can be also applied to analyze higher-order interactions. In the current work we consider an effective field theory of massive vector bosons interacting with a massive scalar field. We impose the conditions o…

High Energy Physics - TheoryNuclear and High Energy PhysicsNuclear TheorySpontaneous symmetry breakingFOS: Physical sciences53001 natural sciencesRenormalizationNuclear Theory (nucl-th)Theoretical physicsHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective field theoryddc:530Gauge theory010306 general physicsGauge symmetryPhysicsCoupling constantUnitarity010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)lcsh:QC1-999High Energy Physics - PhenomenologyHigh Energy Physics - Theory (hep-th)Scalar fieldlcsh:Physics
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Finite size spectrum of SU(N) principal chiral field from discrete Hirota dynamics

2016

Using recently proposed method of discrete Hirota dynamics for integrable (1+1)D quantum field theories on a finite space circle of length L, we derive and test numerically a finite system of nonlinear integral equations for the exact spectrum of energies of SU(N)xSU(N) principal chiral field model as functions of m L, where m is the mass scale. We propose a determinant solution of the underlying Y-system, or Hirota equation, in terms of determinants (Wronskians) of NxN matrices parameterized by N-1 functions of the spectral parameter, with the known analytical properties at finite L. Although the method works in principle for any state, the explicit equations are written for states in the …

High Energy Physics - TheoryNuclear and High Energy PhysicsSigma modelField (physics)FOS: Physical sciences2 dimensionsrepresentation-theory01 natural sciencesexcited-state energiesnonlinear integral-equationsQuantum mechanics0103 physical sciencesBound statelcsh:Nuclear and particle physics. Atomic energy. Radioactivityvolume dependenceQuantum field theory010306 general physicsS-matrixMathematical physicsPhysics[PHYS]Physics [physics][ PHYS ] Physics [physics]010308 nuclear & particles physicsWronskiano(n) sigma-modeln phase-transitionState (functional analysis)goldstone bosonsAdS/CFT correspondenceHigh Energy Physics - Theory (hep-th)lcsh:QC770-798tba equations
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Spin Glasses on Thin Graphs

1995

In a recent paper we found strong evidence from simulations that the Isingantiferromagnet on ``thin'' random graphs - Feynman diagrams - displayed amean-field spin glass transition. The intrinsic interest of considering such random graphs is that they give mean field results without long range interactions or the drawbacks, arising from boundary problems, of the Bethe lattice. In this paper we reprise the saddle point calculations for the Ising and Potts ferromagnet, antiferromagnet and spin glass on Feynman diagrams. We use standard results from bifurcation theory that enable us to treat an arbitrary number of replicas and any quenched bond distribution. We note the agreement between the f…

High Energy Physics - TheoryNuclear and High Energy PhysicsSpin glassCondensed Matter (cond-mat)FOS: Physical sciencesCondensed Matter01 natural sciencesCondensed Matter::Disordered Systems and Neural Networks010305 fluids & plasmassymbols.namesakeHigh Energy Physics - LatticeSaddle point0103 physical sciencesAntiferromagnetismFeynman diagram010306 general physicsRandom graphPhysicsBethe latticeCondensed matter physicsHigh Energy Physics - Lattice (hep-lat)Mean field theoryHigh Energy Physics - Theory (hep-th)symbolsIsing modelCondensed Matter::Strongly Correlated Electrons
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Hadronic light-by-light scattering contribution to the muon $g-2$ from lattice QCD: semi-analytical calculation of the QED kernel

2023

Hadronic light-by-light scattering is one of the virtual processes that causes the gyromagnetic factor $g$ of the muon to deviate from the value of two predicted by Dirac's theory. This process makes one of the largest contributions to the uncertainty of the Standard Model prediction for the muon $(g-2)$. Lattice QCD allows for a first-principles approach to computing this non-perturbative effect. In order to avoid power-law finite-size artifacts generated by virtual photons in lattice simulations, we follow a coordinate-space approach involving a weighted integral over the vertices of the QCD four-point function of the electromagnetic current carried by the quarks. Here we present in detai…

High Energy Physics - TheoryNuclear and High Energy Physicsmagnetic momentn-point function530 Physicsspace Euclidean4FOS: Physical sciences[PHYS.HLAT] Physics [physics]/High Energy Physics - Lattice [hep-lat]nonperturbativeEuclideandimension 4quarkHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)dimensionmuonquantum chromodynamicsquantum electrodynamicsphoton photoncomputerlatticeperturbation theoryphoton photon scatteringeffect nonperturbative[PHYS.HLAT]Physics [physics]/High Energy Physics - Lattice [hep-lat][PHYS.HTHE]Physics [physics]/High Energy Physics - Theory [hep-th]effectHigh Energy Physics - Lattice (hep-lat)scatteringphotonlattice field theoryspace530 Physikcurrent[PHYS.HPHE] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics - PhenomenologyelectromagneticHigh Energy Physics - Theory (hep-th)photon virtualn-point function 4finite size[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]virtual[PHYS.HTHE] Physics [physics]/High Energy Physics - Theory [hep-th]current electromagnetic
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