Search results for "Fermion"

showing 10 items of 523 documents

On the Physical Propagators of QED

1993

The true variables in QED are the transverse photon components and Dirac's physical electron, constructed out of the fermionic field and the longitudinal components of the photon. We calculate the propagators in terms of these variables to one loop and demonstrate their gauge invariance. The physical electron propagator is shown not to suffer from infrared divergences in any gauge. In general, all physical Green's functions are gauge invariant and infrared-finite.

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsPhotonFermionic fieldHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyPropagatorFOS: Physical sciencesElectronInvariant (physics)Transverse planesymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)Quantum electrodynamicssymbolsGauge theory
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Short-distance contribution to the spectrum of Hawking radiation

2006

The Hawking effect can be rederived in terms of two-point functions and in such a way that it makes it possible to estimate, within the conventional semiclassical theory, the contribution of ultrashort distances to the Planckian spectrum. For Schwarzschild black holes of three solar masses the analysis shows that Hawking radiation is very robust up to frequencies of 96 T_H or 270 T_H for bosons and fermions, respectively. For primordial black holes (with masses around 10^{15} g) these frequencies turn out to be of order 52T_H and 142 T_H. Only at these frequencies and above do we find that the contribution of Planck distances is of order of the total spectrum itself. Below this scale, the c…

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsQuantum field theory in curved spacetime010308 nuclear & particles physicsSemiclassical physicsFOS: Physical sciencesFermion01 natural sciencesHigh Energy Physics::TheoryMicro black holeGeneral Relativity and Quantum CosmologyHigh Energy Physics - Theory (hep-th)Quantum electrodynamicsQuantum mechanics0103 physical sciencesQuantum gravityFísica nuclear010306 general physicsSchwarzschild radiusHawking radiationBoson
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Semi-Lorentz invariance, unitarity, and critical exponents of symplectic fermion models

2007

We study a model of N-component complex fermions with a kinetic term that is second order in derivatives. This symplectic fermion model has an Sp(2N) symmetry, which for any N contains an SO(3) subgroup that can be identified with rotational spin of spin-1/2 particles. Since the spin-1/2 representation is not promoted to a representation of the Lorentz group, the model is not fully Lorentz invariant, although it has a relativistic dispersion relation. The hamiltonian is pseudo-hermitian, H^\dagger = C H C, which implies it has a unitary time evolution. Renormalization-group analysis shows the model has a low-energy fixed point that is a fermionic version of the Wilson-Fisher fixed points. T…

PhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsUnitarityStrongly Correlated Electrons (cond-mat.str-el)010308 nuclear & particles physicsCritical phenomenaFOS: Physical sciencesKinetic termFermionMathematical Physics (math-ph)Lorentz covariance01 natural sciencesLorentz groupCondensed Matter - Strongly Correlated ElectronsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)0103 physical sciences010306 general physicsCritical exponentMathematical PhysicsMathematical physicsSymplectic geometry
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Numerical studies of Minimally Doubled Fermions

2013

We have performed the first numerical study of minimally doubled fermions of the Karsten-Wilczek class in the quenched approximation. This requires fixing the counterterms, which arise due to hypercubic symmetry breaking induced by the Karsten-Wilczek term. Non-perturbative renormalisation criteria are formulated after a detailed study of the parameter dependence of mesonic observables. Minimisation of the mass anisotropy of the pseudoscalar ground state fixes non-perturbative renormalisation conditions for the counterterm coefficients. These anisotropies are mapped out by probing different euclidean components of the transfer matrix through calculations of the pseudoscalar ground state mas…

PhysicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)Lattice (group)FOS: Physical sciencesObservableQuenched approximationFermionTransfer matrixPseudoscalarHigh Energy Physics - LatticeSymmetry breakingGround stateMathematical physics
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Negative S parameter from holographic technicolor.

2006

We present a new class of 5D models, Holographic Technicolor, which fulfills the basic requirements for a candidate of comprehensible 4D strong dynamics at the electroweak scale. It is the first Technicolor-like model able to provide a vanishing or even negative tree-level S parameter, avoiding any no-go theorem on its sign. The model is described in the large-N regime. S is therefore computable: possible corrections coming from boundary terms follow the 1/N suppression, and generation of fermion masses and the S parameter issue do split up. We investigate the model's 4D dual, probably walking Technicolor-like with a large anomalous dimension.

PhysicsHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyDuality (optimization)Boundary (topology)FOS: Physical sciencesTechnicolorFermionDual (category theory)Theoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Dimension (vector space)Quantum mechanicsElectroweak scaleSign (mathematics)Physical review letters
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Implications of new generations on neutrino masses

2011

We explore the possible implications that new families, that are being searched for at the LHC, would have on neutrino masses. In particular, we have explored the possibility that the smallness of the observed neutrino masses is naturally understood in a modified version of the Standard Model (SM) with complete extra generations of fermions, i.e., that have right-handed neutrinos, in which neutrino masses are generated at two loops. With one extra family it is not possible to fit the observed spectrum of masses and mixings. However, the radiative mass generated provides an important constraint in these kind of models, so the neutrino masses do not exceed their cosmological bound. Within the…

PhysicsHistoryParticle physicsLarge Hadron ColliderPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaContext (language use)FermionParameter spacePartícules (Física nuclear)Computer Science ApplicationsEducationStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Measurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillation
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Differences between photoluminescence spectra of type-I and type-II quantum dots

2008

Semiconductor quantum dots which trap simultaneously electrons and holes are called quantum dots of type-I. Contrary to these structures, empty dots of type-II attract only one type of charged carriers and repel the other. Particularities of confining potential are unaccessible by any direct measurements, thus recognition of quantum dot type by indirect method is highly desired. Our proposal is to distinguish between the two types of quantum dots via a comparison of photoluminescence spectra of these structures, which differ in both cases qualitatively.

PhysicsHistoryPhotoluminescenceCondensed matter physicsQuantum point contactElectronFermionCondensed Matter::Mesoscopic Systems and Quantum Hall EffectComputer Science ApplicationsEducationQuantum dot laserQuantum dotCharge carrierEmission spectrumJournal of Physics: Conference Series
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β -decay rates of Rh115,117 into Pd115,117 isotopes in the microscopic interacting boson-fermion model

2020

The structure of odd-$A ^{115,117}\mathrm{Rh}$ and $^{115,117}\mathrm{Pd}$ isotopes is studied by means of the neutron-proton interacting boson-fermion model (IBFM-2). ${J}^{P}={\frac{1}{2}}^{+}$ quantum number assignment for the $^{115,117}\mathrm{Pd}$ ground states is critically discussed and the predicted energy levels are compared to the existing experimental data. The resulting nuclear wave functions are used to compute the $\ensuremath{\beta}$-decay $ft$ values of the transitions from $^{115,117}\mathrm{Rh}$ to $^{115,117}\mathrm{Pd}$ in the microscopic IBFM-2 and the results compared with the data.

PhysicsIsotope010308 nuclear & particles physicsFermionQuantum number7. Clean energy01 natural sciences0103 physical sciencesAtomic physics010306 general physicsWave functionNuclear theoryEnergy (signal processing)BosonPhysical Review C
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A 5E-Based Learning Workshop on Various Aspects of the Hall Effect

2019

Learning activities in constructivist environments are characterized by active engagement, inquiry, problem solving, and collaboration with peers. The 5E learning cycle is a student-centered instructional model for constructivism, where the students perform five phases of instruction: Engagement, Exploration, Explanation, Elaboration, Evaluation. The purpose of this contribution is to present a 5E-based learning path of advanced physics aimed at strengthening Physics/Engineering student understanding about the quantum Hall effect, a phenomenon observed at low temperatures in a two-dimensional electron gas subject to a strong perpendicular magnetic field. The quantum Hall effect, a rare exam…

PhysicsLearning cycleSettore FIS/08 - Didattica E Storia Della Fisica5E learning cycleHall effectObservableFermionQuantum Hall effectPlanck constantSettore FIS/03 - Fisica Della MateriaSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)symbols.namesakeTheoretical physicsHall effectComposite fermionQuasiparticlesymbolsGraphene
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Electromagnetic properties of neutrinos in a background of electrons.

1989

Using covariant methods we calculate the neutrino electromagnetic vertex in a gas of electrons to lowest order in a loop expansion and to the lowest order in $\frac{1}{{M}_{W}^{2}}$. The new induced terms, while they are chirality preserving, yield additional contributions to the dipole moments in the nonrelativistic limit. These are identical for particles and antiparticles and so need not vanish for Majorana neutrinos. As applications of our formulas, the expression for the $\mathrm{plasmon}\ensuremath{\rightarrow}\ensuremath{\nu}\overline{\ensuremath{\nu}}$ decay rate is rederived and the dispersion relation of a massless neutrino propagating in matter in the presence of an external magn…

PhysicsMassless particleAntiparticleMAJORANAParticle physicsAntimatterQuantum mechanicsHigh Energy Physics::PhenomenologyElementary particleFermionNeutrinoLeptonPhysical review. D, Particles and fields
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