Search results for "normalization"

showing 10 items of 632 documents

Antiferromagnetic Heisenberg chains with bond alternation and quenched disorder

2004

We consider S=1/2 antiferromagnetic Heisenberg chains with alternating bonds and quenched disorder, which represents a theoretical model of the compound CuCl_{2x}Br_{2(1-x)}(\gamma-{pic})_2. Using a numerical implementation of the strong disorder renormalization group method we study the low-energy properties of the system as a function of the concentration, x, and the type of correlations in the disorder. For perfect correlation of disorder the system is in the random dimer (Griffiths) phase having a concentration dependent dynamical exponent. For weak or vanishing disorder correlations the system is in the random singlet phase, in which the dynamical exponent is formally infinity. We disc…

PhysicsCondensed matter physicsDimerGeneral Physics and AstronomyFOS: Physical sciencesFunction (mathematics)Disordered Systems and Neural Networks (cond-mat.dis-nn)Type (model theory)Renormalization groupCondensed Matter - Disordered Systems and Neural NetworksCondensed Matter::Disordered Systems and Neural Networkschemistry.chemical_compoundchemistryPhase (matter)ExponentAntiferromagnetismCondensed Matter::Strongly Correlated ElectronsSinglet state
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Effects of surface nonlinear interactions on the local critical behavior

1987

Effects of surface nonlinear interactions on the local critical behaviors are studied for an-component field in the semi-infinite space near the SB (surface-bulk) point by using renormalization group methods. The model Hamiltonian consists of a free (Gaussian) bulk part and a surface term containing aφ4 interaction. The interplay between the free bulk term and the nonlinear surface term gives rise to interesting behaviors of the local surface properties. Whereas the local susceptibility and correlation exponents retain their mean-field values, the surface crossover exponent ϕ is non-mean-field below three dimensions. To second order in e(e=3−d) we find:η‖ and\(\phi = \frac{1}{2} - \frac{{n …

PhysicsCondensed matter physicsLogarithmGaussianMonte Carlo methodGroup methodRenormalization groupCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsNonlinear systemsymbols.namesakesymbolsExponentGeneral Materials ScienceHamiltonian (quantum mechanics)Zeitschrift f�r Physik B Condensed Matter
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Image charge dynamics in time-dependent quantum transport

2012

In this work we investigate the effects of the electron-electron interaction between a molecular junction and the metallic leads in time-dependent quantum transport. We employ the recently developed embedded Kadanoff-Baym method [Phys. Rev. B 80, 115107 (2009)] and show that the molecule-lead interaction changes substantially the transient and steady-state transport properties. We first show that the mean-field Hartree-Fock (HF) approximation does not capture the polarization effects responsible for the renormalization of the molecular levels neither in nor out of equilibrium. Furthermore, due to the time-local nature of the HF self-energy there exists a region in parameter space for which …

PhysicsCondensed matter physicsMolecular junctionCondensed Matter - Mesoscale and Nanoscale Physicsta114FOS: Physical sciencesBiasingParameter spaceCondensed Matter PhysicsPolarization (waves)Method of image chargesElectronic Optical and Magnetic MaterialsSettore FIS/03 - Fisica della MateriaRenormalizationQuantum transportMesoscale and Nanoscale Physics (cond-mat.mes-hall)Moleculequantum transport
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Nonmonotonical crossover of the effective susceptibility exponent

1997

We have numerically determined the behavior of the magnetic susceptibility upon approach of the critical point in two-dimensional spin systems with an interaction range that was varied over nearly two orders of magnitude. The full crossover from classical to Ising-like critical behavior, spanning several decades in the reduced temperature, could be observed. Our results convincingly show that the effective susceptibility exponent gamma_eff changes nonmonotonically from its classical to its Ising value when approaching the critical point in the ordered phase. In the disordered phase the behavior is monotonic. Furthermore the hypothesis that the crossover function is universal is supported.

PhysicsCondensed matter physicsStatistical Mechanics (cond-mat.stat-mech)Critical phenomenaCrossoverGeneral Physics and AstronomyFOS: Physical sciencesRenormalization groupCondensed Matter - Soft Condensed MatterUniversality (dynamical systems)RenormalizationCritical point (thermodynamics)Soft Condensed Matter (cond-mat.soft)Ising modelStatistical physicsCritical exponentCondensed Matter - Statistical Mechanics
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Proton-induced deuteron breakup reaction2H(p, pp)n

1994

The “screening and renormalization” approach allows for a mathematically correct incorporation, in three-body scattering theory, of the long-ranged Coulomb interaction between charged particles. It is based on first calculating the transition amplitudes using screened Coulomb potentials. Then, after renormalization the zero-screening limit, leading to the amplitudes pertaining to unscreened Coulomb potentials, is performed numerically. Within this formalism the proton-induced breakup of deuterons is investigated, with the Coulomb repulsion between the two protons taken into account. Kinematically complete differential cross sections in various kinematic configurations are calculated and com…

PhysicsCoulomb's constantProtonNuclear TheoryCoulomb barrierBreakupAtomic and Molecular Physics and OpticsCharged particleRenormalizationQuantum electrodynamicsCoulombScattering theoryAtomic physicsNuclear ExperimentFew-Body Systems
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Complex-mass scheme and perturbative unitarity

2012

We derive cutting rules for loop integrals containing propagators with complex masses. Using a field-theoretical model of a heavy vector boson interacting with a light fermion, we demonstrate that the complex-mass scheme respects unitarity order by order in a perturbative expansion provided that the renormalized coupling constant remains real.

PhysicsCoupling constantCondensed Matter::Quantum GasesHigh Energy Physics - TheoryNuclear and High Energy PhysicsUnitarityOrder (ring theory)PropagatorFOS: Physical sciencesAstronomy and AstrophysicsFermionAtomic and Molecular Physics and OpticsVector bosonRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Scheme (mathematics)Mathematical physics
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Running couplings from adiabatic regularization

2019

We extend the adiabatic regularization method by introducing an arbitrary mass scale $\mu$ in the construction of the subtraction terms. This allows us to obtain, in a very robust way, the running of the coupling constants by demanding $\mu$-invariance of the effective semiclassical (Maxwell-Einstein) equations. In particular, we get the running of the electric charge of perturbative quantum electrodynamics. Furthermore, the method brings about a renormalization of the cosmological constant and the Newtonian gravitational constant. The running obtained for these dimensionful coupling constants has new relevant (non-logarithmic) contributions, not predicted by dimensional regularization.

PhysicsCoupling constantHigh Energy Physics - TheoryNuclear and High Energy PhysicsSemiclassical physicsFOS: Physical sciencesCosmological constantGeneral Relativity and Quantum Cosmology (gr-qc)lcsh:QC1-999General Relativity and Quantum CosmologyRenormalizationGravitational constantDimensional regularizationHigh Energy Physics - Theory (hep-th)Regularization (physics)Adiabatic processlcsh:PhysicsMathematical physics
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Interaction Of The Vector-Meson Octet With The Baryon Octet In Effective Field Theory

2015

We analyze the constraint structure of the interaction of vector mesons with baryons using the classical Dirac constraint analysis. We show that the standard interaction in terms of two independent SU(3) structures is consistent at the classical level. We then require the self-consistency condition of the interacting system in terms of perturbative renormalizability to obtain relations for the renormalized coupling constants at the one-loop level. As a result we find a universal interaction with one coupling constant which is the same as in the massive Yang-Mills Lagrangian of the vector-meson sector.

PhysicsCoupling constantNuclear and High Energy PhysicsParticle physicsMesonOctetNuclear TheoryHigh Energy Physics::LatticeDirac (software)High Energy Physics::PhenomenologyFOS: Physical sciencesVector meson dominanceNuclear Theory (nucl-th)BaryonRenormalizationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Vector meson
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Some aspects of the nonperturbative renormalization of the phi^4 model

2007

A nonperturbative renormalization of the phi^4 model is considered. First we integrate out only a single pair of conjugated modes with wave vectors +/- q. Then we are looking for the RG equation which would describe the transformation of the Hamiltonian under the integration over a shell Lambda - d Lambda < k < Lambda, where d Lambda -> 0. We show that the known Wegner--Houghton equation is consistent with the assumption of a simple superposition of the integration results for +/- q. The renormalized action can be expanded in powers of the phi^4 coupling constant u in the high temperature phase at u -> 0. We compare the expansion coefficients with those exactly calculated by the…

PhysicsCoupling constantStatistical Mechanics (cond-mat.stat-mech)Single pairFOS: Physical sciencesStatistical and Nonlinear PhysicsCondensed Matter PhysicsRenormalizationsymbols.namesakeSuperposition principlesymbolsPerturbation theory (quantum mechanics)Non-perturbativeHamiltonian (quantum mechanics)Condensed Matter - Statistical MechanicsMathematical physics
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Critical Attractor and Universality in a Renormalization Scheme for Three Frequency Hamiltonian Systems

1998

We study an approximate renormalization-group transformation to analyze the breakup of invariant tori for three degrees of freedom Hamiltonian systems. The scheme is implemented for the spiral mean torus. We find numerically that the critical surface is the stable manifold of a critical nonperiodic attractor. We compute scaling exponents associated with this fixed set, and find that they can be expected to be universal.

PhysicsCritical phenomenaGeneral Physics and AstronomyFOS: Physical sciencesTorusNonlinear Sciences - Chaotic DynamicsStable manifoldUniversality (dynamical systems)Hamiltonian systemRenormalizationAttractorChaotic Dynamics (nlin.CD)Critical exponentMathematics::Symplectic GeometryMathematical physics
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