Search results for "lcsh:Physics"

showing 10 items of 778 documents

NON-LINEAR MECHANICAL, ELECTRICAL AND THERMAL PHENOMENA IN PIEZOELECTRIC CRYSTALS

2003

Mechanical, electrical and thermal phenomena occurring in piezoelectric crystals were examined by non-linear approximation. For this purpose, use was made of the thermodynamic function of state, which describes an anisotropic body. Considered was the Gibbs function. The calculations included strain tensor εij = f(σkl , En, T), induction vector Dm = f(σkl , En, T) and entropy S = f(σkl , En, T) as function of stress σkl , field strength En and temperature difference T. The equations obtained apply to anisotropic piezoelectric bodies provided that the “forces” σkl , En, T acting on the crystal are known. Механічні, електричні та термічні явища у п’єзоелектричних кристалах вивчаються у неліній…

PhysicsPhysics and Astronomy (miscellaneous)Condensed matter physicsInfinitesimal strain theorypiezoelectric crystalsField strengthCondensed Matter PhysicsPiezoelectricitylcsh:QC1-999Gibbs free energyCrystalthermodynamicssymbols.namesakeNonlinear systemtensorsThermalsymbolsAnisotropylcsh:Physicsanisotropic bodiesCondensed Matter Physics
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Spectral distribution and Coulomb correction for nuclear bremsstrahlung induced by heavy targets

2021

Abstract Bremsstrahlung spectra below 250 MeV have been measured colliding 500 MeV–electrons with Cu, Ag, and Au targets. The experimental intensity ratios relative to Cu are well described by an accurate analytical high-energy theory, which accounts both for Coulomb distortion and screening. This represents the first experimental verification of the discovery by Bethe-Maximon that leading-order quantum mechanical calculations, equivalent to quasiclassical approximations, become exact at high energies and small angles. It also shows that radiative QED effects play a minor role in the covered part of the spectral distribution within the accuracy (1.6%) of the present measurements.

PhysicsQuantum electrodynamicsNuclear and High Energy PhysicsSpectral power distributionMECÂNICA QUÂNTICAHigher-order theory010308 nuclear & particles physicsBremsstrahlungBremsstrahlungIntensity ratio01 natural sciencesSpectral linelcsh:QC1-999Nuclear physicsDistortion0103 physical sciencesCoulombRadiative transfer010306 general physicsQuantumlcsh:PhysicsCoulomb correctionPhoton spectra
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Prediction of hidden charm strange molecular baryon states with heavy quark spin symmetry

2019

We have studied the meson-baryon $S-$wave interaction, using coupled channels, in the isoscalar hidden-charm strange sector and $J^P = 1/2^-,3/2^-$ and $5/2^-$. We impose constraints of heavy quark spin symmetry in the interaction and obtain the non vanishing matrix elements from an extension of the local hidden gauge approach to the charm sector. The ultraviolet divergences are renormalized using the same meson-baryon-loops regulator previously employed in the non-strange hidden charm sector, where a good reproduction of the properties of the newly discovered pentaquark states is obtained. We obtain five states of $1/2^-$, four of $3/2^-$ and one of $5/2^-$, which could be compared in the …

PhysicsQuarkNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsIsoscalarFOS: Physical sciencesStrangeness01 natural sciencesPentaquarklcsh:QC1-999BaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Hadron spectroscopyIsospin0103 physical sciencesCharm (quantum number)010306 general physicslcsh:Physics
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Three-body final state interaction in η→ 3π updated

2017

In view of the recent high-statistic KLOE data for the η→π+π−π0 decay, a new determination of the quark mass double ratio has been done. Our approach relies on a dispersive model that takes into account rescattering effects between three pions via subenergy unitarity. The latter is essential to reproduce the Dalitz plot distribution. A simultaneous description of the KLOE and WASA-at-COSY data is achieved in terms of just two real parameters. From a global fit, we determine Q=21.6±1.1. The predicted slope parameter for the neutral channel α=−0.025±0.004 is in reasonable agreement with the PDG average value.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsUnitarity010308 nuclear & particles physicsDalitz plotValue (computer science)State (functional analysis)01 natural scienceslcsh:QC1-999Nuclear physicsPionDistribution (mathematics)0103 physical sciences010306 general physicsDispersion (water waves)lcsh:PhysicsPhysics Letters B
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The baryonic spectrum of QCD 2 in the chiral limit

1991

Abstract A description of the baryonic spectrum of quantum chromodynamics in one-space-one-time dimensions for massless quarks is presented. The theory has been studied in the equivalent non-abelian bosonic representation, and four-point functions of the colored meson fields under the simplifying assumption of two colors have been calculated. The crucial role of the chiral sector in providing baryon number has been unveiled. Excited baryon states appear as pseudomesonic excitations on top of the massless baryons associated with the chiral fields.

PhysicsQuarkQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyAstrophysics::Cosmology and Extragalactic Astrophysicslcsh:QC1-999Massless particleBaryonExcited stateBaryon numberNuclear Experimentlcsh:PhysicsBosonPhysics Letters B
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Taming the higher power corrections in semileptonic B decays

2016

We study the effect of dimension 7 and 8 operators on inclusive semileptonic B decays and the extraction of |Vcb|. Using moments of semileptonic B decay spectra and information based on the Lowest-Lying State saturation Approximation (LLSA) we perform a global fit of the nonperturbative parameters of the heavy quark expansion including for the first time the O(1/mb^{4,5}) contributions. Higher power corrections appear to have a very small effect on the extraction of |Vcb|, independently of the weight we attribute to the LLSA.

PhysicsQuarkSemileptonic decayNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesState (functional analysis)01 natural sciencesSpectral linelcsh:QC1-999High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Dimension (vector space)Quantum electrodynamics0103 physical sciencesSaturation (graph theory)High Energy Physics::Experiment010306 general physicslcsh:Physics
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How to solve Fokker-Planck equation treating mixed eigenvalue spectrum?

2013

An analogy of the Fokker-Planck equation (FPE) with the Schr\"odinger equation allows us to use quantum mechanics technique to find the analytical solution of the FPE in a number of cases. However, previous studies have been limited to the Schr\"odinger potential with a discrete eigenvalue spectrum. Here, we will show how this approach can be also applied to a mixed eigenvalue spectrum with bounded and free states. We solve the FPE with boundaries located at x=\pm L/2 and take the limit L\rightarrow\infty, considering the examples with constant Schr\"{o}dinger potential and with P\"{o}schl-Teller potential. An oversimplified approach was proposed earlier by M.T. Araujo and E. Drigo Filho. A…

PhysicsStatistical Mechanics (cond-mat.stat-mech)Physics and Astronomy (miscellaneous)Spectrum (functional analysis)FOS: Physical sciencesFokker-Planck equationSchrödinger equationMathematical Physics (math-ph)Mathematics::Spectral TheoryCondensed Matter Physicslcsh:QC1-999Pöschl-Teller potentialFokker–Planck equationEigenvalues and eigenvectorsCondensed Matter - Statistical MechanicsMathematical Physicslcsh:PhysicsMathematical physics
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Composite Operator Method analysis of the underdoped cuprates puzzle

2014

The microscopical analysis of the unconventional and puzzling physics of the underdoped cuprates, as carried out lately by means of the Composite Operator Method (COM) applied to the 2D Hubbard model, is reviewed and systematized. The 2D Hubbard model has been adopted as it has been considered the minimal model capable to describe the most peculiar features of cuprates held responsible for their anomalous behavior. COM is designed to endorse, since its foundations, the systematic emergence in any SCS of new elementary excitations described by composite operators obeying non-canonical algebras. In this case (underdoped cuprates - 2D Hubbard model), the residual interactions - beyond a 2-pole…

PhysicsSuperconductivityCondensed Matter::Quantum GasesStrongly Correlated Electrons (cond-mat.str-el)Hubbard modelCondensed matter physicsCondensed Matter - SuperconductivityFOS: Physical sciencesFermi surfaceCondensed Matter Physicslcsh:QC1-999Superconductivity (cond-mat.supr-con)Minimal modelsymbols.namesakeCondensed Matter - Strongly Correlated ElectronsPauli exclusion principleCondensed Matter::SuperconductivitysymbolsAntiferromagnetismCuprateCondensed Matter::Strongly Correlated ElectronsPseudogaplcsh:Physics
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η and η′ transition form factors from Padé approximants

2014

We employ a systematic and model-independent method to extract, from space- and time-like data, the η and η′ transition form factors (TFFs) obtaining the most precise determination for their low-energy parameters and discuss the Γη→γγ impact on them. Using TFF data alone, we also extract the η − η′ mixing parameters, which are compatible to those obtained from more sophisticated and input-demanding procedures.

PhysicsTheoretical physicsPhysicsQC1-999Padé approximantSpace (mathematics)lcsh:Physicslcsh:QC1-999Mixing (physics)EPJ Web of Conferences
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Sound attenuation and anharmonic damping in solids with correlated disorder

2010

We study via self-consistent Born approximation a model for sound waves in a disordered environment, in which the local fluctuations of the shear modulus G are spatially correlated with a certain correlation length The theory predicts an enhancement of the density of states over Debye's omega(2) law (boson peak) whose intensity increases for increasing correlation length, and whose frequency position is shifted downwards as lg. Moreover, the predicted disorder-induced sound attenuation coefficient r(k) obeys a universal scaling law F(k) = f (ke) for a given variance of G. Finally, the inclusion of the lowest-order contribution to the anharmonic sound damping into the theory allows us to rec…

Physicssound attenuation; anharmonic interactions; vibrational properties of disordered solids; boson peakPhysics and Astronomy (miscellaneous)Condensed matter physicsvibrational properties of disordered solidsAnharmonicity02 engineering and technology021001 nanoscience & nanotechnologyCondensed Matter Physics01 natural sciencessound attenuationlcsh:QC1-999boson peakAmorphous solidPosition (vector)0103 physical sciencesBoson peak010306 general physics0210 nano-technologylcsh:PhysicsAcoustic attenuationanharmonic interactionsCondensed Matter Physics
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