Search results for "Mathematical physics"

showing 10 items of 2687 documents

Massless Spectra and Gauge Couplings at One-Loop on Non-Factorisable Toroidal Orientifolds

2018

So-called `non-factorisable' toroidal orbifolds can be rewritten in a factorised form as a product of three two-tori by imposing an additional shift symmetry. This finding of Blaszczyk et al., arXiv:1111.5852, provides a new avenue to Conformal Field Theory methods, by which the vector-like massless matter spectrum - and thereby the type of gauge group enhancement on orientifold invariant fractional D6-branes - and the one-loop corrections to the gauge couplings in Type IIA orientifold theories can be computed in addition to the well-established chiral matter spectrum derived from topological intersection numbers among three-cycles. We demonstrate this framework for the $\mathbb{Z}_4 \times…

PhysicsCouplingHigh Energy Physics - TheoryNuclear and High Energy PhysicsToroid010308 nuclear & particles physicsConformal field theoryFOS: Physical sciencesTorus01 natural sciencesMassless particleHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Gauge groupOrientifoldQuantum electrodynamics0103 physical scienceslcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityInvariant (mathematics)010306 general physicsMathematical physics
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form factor at order of chiral perturbation theory

2001

Abstract This paper describes the calculation of the electromagnetic form factor of the K 0 meson at order p 6 of chiral perturbation theory which is the next-to-leading order correction to the well-known p 4 result achieved by Gasser and Leutwyler. On the one hand, at order p 6 the chiral expansion contains 1- and 2-loop diagrams which are discussed in detail. Especially, a numerical procedure for calculating the irreducible 2-loop graphs of the sunset topology is presented. On the other hand, the chiral Lagrangian L (6) produces a direct coupling of the K 0 current with the electromagnetic field tensor. Due to this coupling one of the unknown parameters of L (6) occurs in the contribution…

PhysicsCouplingNuclear and High Energy PhysicsChiral perturbation theoryMesonCharge radiusHigh Energy Physics::LatticeForm factor (quantum field theory)Order (group theory)Direct couplingMathematical physicsElectromagnetic tensorNuclear Physics B
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Equivalence betweenXYand dimerized models

2010

The spin-$1/2$ chain with $\mathit{XY}$ anisotropic coupling in the plane and the $\mathit{XX}$ isotropic dimerized chain are shown to be equivalent in the bulk. For finite systems, we prove that the equivalence is exact in given parity sectors, after taking care of the precise boundary conditions. The proof is given constructively by finding unitary transformations that map the models onto each other. Moreover, we considerably generalized our mapping and showed that even in the case of fully site-dependent couplings the $\mathit{XY}$ chain can be mapped onto an $\mathit{XX}$ model. This result has potential application in the study of disordered systems.

PhysicsCouplingQuantum PhysicsAngular momentumStrongly Correlated Electrons (cond-mat.str-el)Statistics::ApplicationsIsotropyFinite systemFOS: Physical sciencesParity (physics)01 natural sciencesUnitary stateAtomic and Molecular Physics and Optics010305 fluids & plasmasCondensed Matter - Other Condensed MatterCondensed Matter - Strongly Correlated ElectronsQuantum mechanics0103 physical sciencesBoundary value problemQuantum Physics (quant-ph)010306 general physicsAnisotropyOther Condensed Matter (cond-mat.other)Mathematical physicsPhysical Review A
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Non-Adiabatic Aspects of Time-Dependent Hamiltonian Systems

1994

Extreme adiabatic behavior furnishes great simplification in the treatment of linear time-dependent Hamiltonian systems. But the actual time variation of the parameters is only finitely, rather than infinitely, slow. Then one is forced to consider corrections to the adiabatic limit.

PhysicsCovariant Hamiltonian field theoryLimit (mathematics)Adiabatic processHamiltonian systemMathematical 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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The Fock Bundle of a Dirac Operator and Infinite Grassmannians

1989

In the earlier chapters we have studied representations of current algebras in fermionic Fock spaces. A (fermionic) Fock space is determined by a single Dirac operator D. To set up a Fock space we need a splitting of a complex Hilbert space H to the subspaces H± corresponding to positive and negative frequencies of D. However, in an interacting quantum field theory one really should consider a bundle of Fock spaces parametrized by different Dirac operators. For example, in Yang-Mills theory any smooth vector potential defines a Dirac operator and one must consider the whole bunch of these operators and associated Fock spaces if one wants to describe the interaction of the vector potential w…

PhysicsCurrent (mathematics)High Energy Physics::LatticeDirac (software)Hilbert spaceTopologyDirac operatorFock spacesymbols.namesakeFock stateDirac spinorsymbolsQuantum field theoryMathematical physics
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Fully Covariant and Conformal Formulation of the Z4 System Compared to the BSSN Formulation in Spherical Symmetry

2014

We have generalized a covariant and conformal version of the Z4 system of the Einstein equations by adopting a reference metric approach, that we denote as fCCZ4, well suited for curvilinear as well as Cartesian coordinates. We implement this formalism in spherical polar coordinates under the assumption of spherical symmetry using a partially-implicit Runge-Kutta (PIRK) method, without using any regularization scheme, and show that our code can evolve both vacuum and non-vacuum spacetimes without encountering instabilities. We have performed several tests and compared the Hamiltonian constraint violations of the fCCZ4 system, for different choices of certain free parameters, with these of B…

PhysicsCurvilinear coordinatesSpherical coordinate systemConformal maplaw.inventionGeneral Relativity and Quantum CosmologyClassical mechanicsHamiltonian constraintlawCovariant transformationCartesian coordinate systemCircular symmetryMathematical physicsFree parameter
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A 16 channel high resolution (<11 ps RMS) Time-to-Digital Converter in a Field Programmable Gate Array

2012

A 16-channel Time-to-Digital Converter (TDC) was implemented in a general purpose Field-Programmable Gate Array (FPGA). The fine time calculations are achieved by using the dedicated carry-chain lines. The coarse counter defines the coarse time stamp. In order to overcome the negative effects of temperature and power supply dependency bin-by-bin calibration is applied. The time interval measurements are done using 2 channels. The time resolution of channels are calculated for 1 clock cycle and a minimum of 10.3 ps RMS on two channels, yielding 7.3 ps RMS (10.3 ps/√2) on a single channel is achieved.

PhysicsCycles per instructionbusiness.industryElectrical engineeringPower (physics)Time-to-digital converterOpticsGate arrayCalibrationTimestampbusinessField-programmable gate arrayInstrumentationMathematical PhysicsCommunication channelJournal of Instrumentation
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Beta decay of the new isotope101Sn

1995

The very neutron-deficient isotope 101Sn was produced in a 50Cr(58Ni, 2p5n) reaction and its decay properties were determined for the first time. By using chemically selective ion sources of an on-line mass separator, the energy spectrum and the half-life (3 ± 1 s) of beta-delayed protons of 101Sn were measured. These results are compared to theoretical predictions.

PhysicsDecay schemeIsotopeSeparator (oil production)Condensed Matter PhysicsBeta decayAtomic and Molecular Physics and OpticsBeta-decay stable isobarsIonNuclear physicsEnergy spectrumAtomic physicsNuclear ExperimentMathematical PhysicsPhysica Scripta
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Natural occupation numbers: When do they vanish?

2013

The non-vanishing of the natural orbital occupation numbers of the one-particle density matrix of many-body systems has important consequences for the existence of a density matrix-potential mapping for nonlocal potentials in reduced density matrix functional theory and for the validity of the extended Koopmans' Theorem. On the basis of Weyl's theorem we give a connection between the differentiability properties of the ground state wave function and the rate at which the natural occupations approach zero when ordered as a descending series. We show, in particular, that the presence of a Coulomb cusp in the wave function leads, in general, to a power law decay of the natural occupations, whe…

PhysicsDensity matrixCusp (singularity)Quantum Physics010304 chemical physicsSeries (mathematics)Basis (linear algebra)Strongly Correlated Electrons (cond-mat.str-el)ta114Atomic Physics (physics.atom-ph)General Physics and AstronomyFOS: Physical sciences01 natural sciencesPhysics - Atomic PhysicsCondensed Matter - Strongly Correlated Electrons0103 physical sciencesCoulombDensity functional theoryDifferentiable functionPhysical and Theoretical Chemistry010306 general physicsWave functionQuantum Physics (quant-ph)Mathematical physicsJournal of Chemical Physics
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