Search results for "Chiral perturbation Theory"

showing 10 items of 294 documents

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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Hamiltonian lattice QCD at finite density: equation of state in the strong coupling limit

2001

The equation of state of Hamiltonian lattice QCD at finite density is examined in the strong coupling limit by constructing a solution to the equation of motion corresponding to an effective Hamiltonian describing the ground state of the many body system. This solution exactly diagonalizes the Hamiltonian to second order in field operators for all densities and is used to evaluate the vacuum energy density from which we obtain the equation of state. We find that up to and beyond the chiral symmetry restoration density the pressure of the quark Fermi sea can be negative indicating its mechanical instability. Our result is in qualitative agreement with continuum models and should be verifiabl…

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsChiral perturbation theoryNuclear TheoryHigh Energy Physics::LatticeLattice field theoryQCD vacuumAstrophysics (astro-ph)High Energy Physics - Lattice (hep-lat)FOS: Physical sciencesLattice QCDAstrophysicsNuclear Theory (nucl-th)symbols.namesakeHigh Energy Physics - PhenomenologyHamiltonian lattice gauge theoryHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - LatticeHigh Energy Physics - Theory (hep-th)Quantum electrodynamicssymbolsHamiltonian (quantum mechanics)Ground stateLattice model (physics)
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Baryon chiral perturbation theory

2009

We provide a short introduction to the one-nucleon sector of chiral perturbation theory and address the issue of power counting and renormalization. We discuss the infrared regularization and the extended on-mass-shell scheme. Both allow for the inclusion of further degrees of freedom beyond pions and nucleons and the application to higher-loop calculations. As applications we consider the chiral expansion of the nucleon mass to order ${\cal O}(q^6)$ and the inclusion of vector and axial-vector mesons in the calculation of nucleon form factors. Finally, we address the complex-mass scheme for describing unstable particles in effective field theory.

PhysicsHistoryChiral perturbation theoryNuclear TheoryMesonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)Nuclear TheoryDegrees of freedom (statistics)FOS: Physical sciencesComputer Science ApplicationsEducationNuclear Theory (nucl-th)BaryonRenormalizationHigh Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)PionRegularization (physics)Effective field theoryNuclear ExperimentNucleonJournal of Physics: Conference Series
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Observation of a unitary cusp in the thresholdγp→π0preaction

1997

A rigorous multipole analysis of the recent $\ensuremath{\gamma}p\ensuremath{\rightarrow}{\ensuremath{\pi}}^{0}p$ cross-section measurement is presented. The data were taken using the photon spectrometer TAPS at the tagged photon beam of the Mainz microtron. The $s$ and $p$ wave multipoles were extracted using minimal model assumptions. The predicted unitary cusp for the $s$-wave multipole ${E}_{0+}$ due to the two step $\ensuremath{\gamma}p\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}n\ensuremath{\rightarrow}{\ensuremath{\pi}}^{0}p$ reaction was observed. The results are consistent with one-loop chiral perturbation theory calculations for which three low-energy constants have been determi…

PhysicsMinimal modelNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryPhotonUnitarityPolarization (waves)Multipole expansionMicrotronUnitary statePhysical Review C
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A measurement of the CP-conserving component of the decay KS0→π+π−π0

2005

Abstract The NA48 Collaboration has measured the amplitude of the CP-conserving component of the decay K S 0 → π + π − π 0 relative to K L 0 → π + π − π 0 . For the characteristic parameter λ , the values Re λ = 0.038 ± 0.010 and Im λ = − 0.013 ± 0.007 have been extracted. These values agree with earlier measurements and with theoretical predictions from chiral perturbation theory.

PhysicsNuclear and High Energy PhysicsAngular momentumAmplitudeChiral perturbation theory010308 nuclear & particles physicsComponent (thermodynamics)Quantum mechanics0103 physical sciencesPiPerturbation theory010306 general physics01 natural sciencesPhysics Letters B
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Peripheral nucleon-nucleon phase shifts and chiral symmetry

1997

Within the one-loop approximation of baryon chiral perturbation theory we calculate all one-pion and two-pion exchange contributions to the nucleon-nucleon interaction. In fact we construct the elastic NN-scattering amplitude up to and including third order in small momenta. The phase shifts with orbital angular momentum $L\geq2 $ and the mixing angles with $J\geq2$ are given parameterfree and thus allow for a detailed test of chiral symmetry in the two-nucleon system. We find that for the D-waves the $2\pi$-exchange corrections are too large as compared with empirical phase shifts, signaling the increasing importance of shorter range effects in lower partial waves. For higher partial waves…

PhysicsNuclear and High Energy PhysicsAngular momentumChiral perturbation theoryNuclear TheoryNuclear TheoryPhase (waves)FOS: Physical sciencesNuclear Theory (nucl-th)BaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)AmplitudeQuantum electrodynamicsCoordinate spaceNuclear ExperimentNucleonMixing (physics)Nuclear Physics A
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First observation and measurement of the decay K±→π±e+e−γ

2008

Abstract Using the full data set of the NA48/2 experiment, the decay K ± → π ± e + e − γ is observed for the first time, selecting 120 candidates with 7.3 ± 1.7 estimated background events. With K ± → π ± π D 0 as normalisation channel, the branching ratio is determined in a model-independent way to be Br ( K ± → π ± e + e − γ , m e e γ > 260  MeV / c 2 ) = ( 1.19 ± 0.12 stat ± 0.04 syst ) × 10 −8 . This measured value and the spectrum of the e + e − γ invariant mass allow a comparison with predictions of chiral perturbation theory.

PhysicsNuclear and High Energy PhysicsAntiparticleChiral perturbation theoryMeson010308 nuclear & particles physicsBranching fractionHadronAnalytical chemistry01 natural sciencesNuclear physicsParticle decayPion0103 physical sciences010306 general physicsDimensionless quantityPhysics Letters B
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Improving the ultraviolet behavior in baryon chiral perturbation theory

2004

We introduce a new formulation of baryon chiral perturbation theory which improves the ultraviolet behavior of propagators and can be interpreted as a smooth cutoff regularization scheme. It is equivalent to the standard approach, preserves all symmetries and therefore satisfies the Ward identities. Our formulation is equally well defined in the vacuum, one- and few-nucleon sectors of the theory. The equations (Bethe-Salpeter, Lippmann-Schwinger, etc.) for the scattering amplitudes of the few-nucleon sector are free of divergences in the new approach. Unlike the usual cutoff regularization, our 'cutoffs' are parameters of the Lagrangian and do not have to be removed.

PhysicsNuclear and High Energy PhysicsBethe–Salpeter equationChiral perturbation theoryNuclear TheoryNuclear TheoryHigh Energy Physics::PhenomenologyPropagatorFOS: Physical sciencesRenormalizationBaryonScattering amplitudeNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Regularization (physics)Quantum electrodynamicsCutoffMathematical physics
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Correlators of left charges and weak operators in finite volume chiral perturbation theory

2002

We compute the two-point correlator between left-handed flavour charges, and the three-point correlator between two left-handed charges and one strangeness violating \Delta I=3/2 weak operator, at next-to-leading order in finite volume SU(3)_L x SU(3)_R chiral perturbation theory, in the so-called epsilon-regime. Matching these results with the corresponding lattice measurements would in principle allow to extract the pion decay constant F, and the effective chiral theory parameter g_27, which determines the \Delta I = 3/2 amplitude of the weak decays K to \pi\pi as well as the kaon mixing parameter B_K in the chiral limit. We repeat the calculations in the replica formulation of quenched c…

PhysicsNuclear and High Energy PhysicsChiral perturbation theoryFinite volume methodHigh Energy Physics::LatticeFlavourHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesFísicaParticle Physics - LatticeStrangenessweak decaysOperator (computer programming)AmplitudeHigh Energy Physics - Latticechiral Lagrangianslattice QCDLattice (order)kaon physicsPion decay constantMathematical physics
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Eta bound states in nuclei

2002

The energies and widths of bound states of the $\eta$ meson in different nuclei are obtained using the results for its selfenergy in a nuclear medium, which is evaluated in a selfconsistent manner using techniques of unitarized chiral perturbation theory. We find bound states in all studied nuclei (from $^{12}{C}$ on) and the half widths obtained are larger than the separation of the levels, what makes the experimental observation of peaks unlikely. We have paid a special attention to the region of nuclei where only the $1s$ state appears and the binding energies are of the order of magnitude of the half width, which would magnify the chances that some broad peak could be observed. This is …

PhysicsNuclear and High Energy PhysicsChiral perturbation theoryMesonNuclear TheoryBinding energyNuclear TheoryFísicaState (functional analysis)Bound stateProduction (computer science)Continuum (set theory)Atomic physicsNuclear ExperimentOrder of magnitude
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