Search results for "TRANSFORMATION"

showing 10 items of 1634 documents

Benchmark calculations of electromagnetic sum rules with a symmetry-adapted basis and hyperspherical harmonics

2020

We demonstrate the ability to calculate electromagnetic sum rules with the \textit{ab initio} symmetry-adapted no-core shell model. By implementing the Lanczos algorithm, we compute non-energy weighted, energy weighted, and inverse energy weighted sum rules for electric monopole, dipole, and quadrupole transitions in $^4$He using realistic interactions. We benchmark the results with the hyperspherical harmonics method and show agreement within $2\sigma$, where the uncertainties are estimated from the use of the many-body technique. We investigate the dependence of the results on three different interactions, including chiral potentials, and we report on the $^4$He electric dipole polarizabi…

PhysicsNuclear Theory010308 nuclear & particles physicsLorentz transformationLanczos algorithmInverseFOS: Physical sciences01 natural sciencesNuclear Theory (nucl-th)Dipolesymbols.namesakePolarizabilityHarmonicsQuantum mechanics0103 physical sciencesQuadrupolesymbols010306 general physicsEnergy (signal processing)
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Relativistic effects in quasifree deuteron electrodisintegration compared to a covariant model

1994

Deuteron disintegration by electrons is calculated in a covariant model for the quasifree region, where final-state interaction and two-body currents can be negiected, and is compared to a phenomenological approach in which one adds to the nonrelativistic one-body current relativistic contributions of lowest order and the kinematic wave-function boost. It is shown that ap/M-reduction of the relativistic theory contains the expressions of the phenomenological approach. The inclusion of relativistic contributions leads to a less frame-dependent description and the deviation from the covariant theory becomes small at low and medium energy and momentum transfers. Furthermore, the dependence of …

PhysicsNuclear TheoryHadronElementary particleElectronAtomic and Molecular Physics and OpticsRelativistic particleMomentumsymbols.namesakeQuantum electrodynamicsDirac equationsymbolsCovariant transformationRelativistic quantum chemistryFew-Body Systems
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A CRITICAL VIEW ON THE PERTURBATIVE RG METHOD

2012

The perturbative renormalization group (RG) treatment of the Ginzburg–Landau model is reconsidered based on the Feynman diagram technique. We derive RG flow equations, exactly calculating all vertices appearing in the perturbative RG transformation of the φ4 model up to the ε3 order of the ε-expansion. The Fourier-transformed two-point correlation function G(k) has been considered. Although the ε-expansion of X(k) = 1/G(k) is well defined on the critical surface, we have revealed an inconsistency with the exact rescaling of X(k), represented as an expansion in powers of k at k →0. This new result can serve as a basis to challenge the correctness of the ε-expansion-based perturbative RG met…

PhysicsNuclear and High Energy PhysicsBasis (linear algebra)Critical phenomenaAstronomy and AstrophysicsRenormalization groupAtomic and Molecular Physics and Opticssymbols.namesakeTransformation (function)Correlation functionFlow (mathematics)symbolsFeynman diagramOrder (group theory)Mathematical physicsInternational Journal of Modern Physics A
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On the chiral covariant approach to ρρ scattering

2017

We examine in detail a recent work (D.~G\"ulmez, U.-G.~Mei\ss ner and J.~A.~Oller, Eur. Phys. J. C 77:460 (2017)), where improvements to make $\rho\rho$ scattering relativistically covariant are made. The paper has the remarkable conclusion that the $J=2$ state disappears with a potential which is much more attractive than for $J=0$, where a bound state is found. We trace this abnormal conclusion to the fact that an "on-shell" factorization of the potential is done in a region where this potential is singular and develops a large discontinuous and unphysical imaginary part. A method is developed, evaluating the loops with full $\rho$ propagators, and we show that they do not develop singula…

PhysicsNuclear and High Energy PhysicsBethe–Salpeter equationNuclear TheoryMeson010308 nuclear & particles physicsPropagatorAstronomy and AstrophysicsState (functional analysis)01 natural sciencesHigh Energy Physics - PhenomenologySingularityFactorization0103 physical sciencesBound stateCovariant transformation010306 general physicsInstrumentationMathematical physicsChinese Physics C
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A Quantum Mechanical Model of the Reissner-Nordstrom Black Hole

1997

We consider a Hamiltonian quantum theory of spherically symmetric, asymptotically flat electrovacuum spacetimes. The physical phase space of such spacetimes is spanned by the mass and the charge parameters $M$ and $Q$ of the Reissner-Nordstr\"{o}m black hole, together with the corresponding canonical momenta. In this four-dimensional phase space, we perform a canonical transformation such that the resulting configuration variables describe the dynamical properties of Reissner-Nordstr\"{o}m black holes in a natural manner. The classical Hamiltonian written in terms of these variables and their conjugate momenta is replaced by the corresponding self-adjoint Hamiltonian operator, and an eigenv…

PhysicsNuclear and High Energy PhysicsCanonical quantizationVacuum stateFOS: Physical sciencesCanonical transformationGeneral Relativity and Quantum Cosmology (gr-qc)WKB approximationGeneral Relativity and Quantum CosmologyBlack holesymbols.namesakeGeneral Relativity and Quantum CosmologyQuantum mechanicsPhase spacesymbolsHamiltonian (quantum mechanics)Eigenvalues and eigenvectors
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Locality properties of Neuberger's lattice Dirac operator

1998

The gauge covariant lattice Dirac operator D which has recently been proposed by Neuberger satisfies the Ginsparg-Wilson relation and thus preserves chiral symmetry. The operator also avoids a doubling of fermion species, but its locality properties are not obvious. We now prove that D is local (with exponentially decaying tails) if the gauge field is sufficiently smooth at the scale of the cutoff. Further analytic and numerical studies moreover suggest that the locality of the operator is in fact guaranteed under far more general conditions.

PhysicsNuclear and High Energy PhysicsChiral symmetryHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)LocalityFOS: Physical sciencesFísicaParticle Physics - LatticeFermionDirac operatorsymbols.namesakeHigh Energy Physics - LatticeLattice (order)symbolsCutoffCovariant transformationGauge theoryMathematical physics
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Fully covariant and conformal formulation of the Z4 system in a reference-metric approach: Comparison with the BSSN formulation in spherical symmetry

2014

We adopt a reference-metric approach to generalize a covariant and conformal version of the Z4 system of the Einstein equations. We refer to the resulting system as ``fully covariant and conformal", or fCCZ4 for short, since it is well suited for curvilinear as well as Cartesian coordinates. We implement this fCCZ4 formalism in spherical polar coordinates under the assumption of spherical symmetry using a partially-implicit Runge-Kutta (PIRK) method and show that our code can evolve both vacuum and non-vacuum spacetimes without encountering instabilities. Our method does not require regularization of the equations to handle coordinate singularities, nor does it depend on constraint-preservi…

PhysicsNuclear and High Energy PhysicsCurvilinear coordinates010308 nuclear & particles physicsFOS: Physical sciencesSpherical coordinate systemGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesGeneral Relativity and Quantum Cosmologylaw.inventionGeneral Relativity and Quantum CosmologyNumerical relativityClassical mechanicsHamiltonian constraintlaw0103 physical sciencesGravitational singularityCartesian coordinate systemCovariant transformationCircular symmetry010306 general physicsPhysical Review D
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Multiparticle correlations in the Schwinger mechanism

2009

We discuss the Schwinger mechanism in scalar QED and derive the multiplicity distribution of particles created under an external electric field using the LSZ reduction formula. Assuming that the electric field is spatially homogeneous, we find that the particles of different momenta are produced independently, and that the multiplicity distribution in one mode follows a Bose-Einstein distribution. We confirm the consistency of our results with an intuitive derivation by means of the Bogoliubov transformation on creation and annihilation operators. Finally we revisit a known solvable example of time-dependent electric fields to present exact and explicit expressions for demonstration.

PhysicsNuclear and High Energy PhysicsDistribution (number theory)010308 nuclear & particles physicsMode (statistics)Scalar (physics)Creation and annihilation operatorsFOS: Physical sciences01 natural sciencesBogoliubov transformationHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Correlation functionQuantum electrodynamicsElectric field0103 physical sciencesGauge theory010306 general physicsMathematical physics
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Covariant approximation averaging

2015

We present a new class of statistical error reduction techniques for Monte-Carlo simulations. Using covariant symmetries, we show that correlation functions can be constructed from inexpensive approximations without introducing any systematic bias in the final result. We introduce a new class of covariant approximation averaging techniques, known as all-mode averaging (AMA), in which the approximation takes account of contributions of all eigenmodes through the inverse of the Dirac operator computed from the conjugate gradient method with a relaxed stopping condition. In this paper we compare the performance and computational cost of our new method with traditional methods using correlation…

PhysicsNuclear and High Energy PhysicsHigh Energy Physics::LatticeMonte Carlo methodLattice field theoryHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesLattice QCDDirac operatorsymbols.namesakeHigh Energy Physics - LatticeConjugate gradient methodLattice gauge theoryQuantum mechanicssymbolsCovariant transformationVector mesonMathematical physics
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Covariant phase space quantization of the Jackiw-Teitelboim model of two-dimensional gravity

1992

Abstract On the basis of the covariant phase space formulation of field theory we analyze the Jackiw-Teitelboim model of two-dimensional gravity on a cylinder. We compute explicitly the symplectic structure showing that the (reduced) phase space is the cotangent bundle of the space of conjugacy classes of the PSL(2, R ) group. This makes it possible to quantize the theory exactly. The Hilbert space is given by the character functions of the PSL (2, R ) group. As a byproduct, this implies the complete equivalence with the PSL (2, R )-topological gravity model.

PhysicsNuclear and High Energy PhysicsHilbert spaceCotangent spaceSpace (mathematics)symbols.namesakeConjugacy classPhase spaceQuantum mechanicssymbolsCotangent bundlePhase space formulationCovariant transformationMathematical physicsPhysics Letters B
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