Search results for "Number"

showing 10 items of 3939 documents

Electronic and magnetic structure of artificial atoms

1999

The concept of shell structure has been found useful in the description of semiconductor quantum dots, which today can be made so small that they contain less than 20 electrons. We review the experimental discovery of magic numbers and spin alignment following Hund’s rules in the addition spectra of vertical quantum dots, and show that these results compare well to model calculations within spin density functional theory. We further discuss the occurrence of spin density waves in quantum dots and quantum wires. For deformable two-dimensional quantum dots (for example, jellium clusters on surfaces), we study the interplay between Hund’s rules and Jahn–Teller deformations and investigate the …

PhysicsQuantum spin Hall effectCondensed matter physicsQuantum dotPrincipal quantum numberQuantum point contactCondensed Matter::Strongly Correlated ElectronsSpin engineeringCondensed Matter::Mesoscopic Systems and Quantum Hall EffectQuantum numberMagnetic quantum numberSpin quantum numberAtomic and Molecular Physics and OpticsThe European Physical Journal D
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QUANTUM SPIN CHAINS WITH COMPOSITE SPIN

1988

The ground state of quantum spin chains with two spin-1/2 operators per site is determined from finite chain calculations and compared to predictions from the continuum limit. As particular cases, results for the spin-1 Heisenberg chain, the spin-1 model with bilinear and biquadratic exchange and the extended Hubbard model are analysed.

PhysicsQuantum spin chainsContinuum (measurement)Condensed matter physicsHubbard modelQuantum mechanicsComposite numberGeneral EngineeringBilinear interpolationCondensed Matter::Strongly Correlated ElectronsGround stateLe Journal de Physique Colloques
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Mixed internal-external state approach for quantum computation with neutral atoms on atom chips

2006

We present a realistic proposal for the storage and processing of quantum information with cold Rb atoms on atom chips. The qubit states are stored in hyperfine atomic levels with long coherence time, and two-qubit quantum phase gates are realized using the motional states of the atoms. Two-photon Raman transitions are used to transfer the qubit information from the internal to the external degree of freedom. The quantum phase gate is realized in a double-well potential created by slowly varying dc currents in the atom chip wires. Using realistic values for all experimental parameters (currents, magnetic fields, ...) we obtain high gate fidelities (above 99.9%) in short operation times (~ 1…

PhysicsQuantum technologyOpen quantum systemComputer Science::Emerging TechnologiesQubitPrincipal quantum numberQuantum simulatorPhysics::Atomic PhysicsQuantum informationAtomic physicsQuantum numberQuantum computer
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The rotational spectrum of 17O2 up to the THz region

2016

Abstract The investigation of the pure rotational spectrum of the 17O2 isotopic species of molecular oxygen has been extended with respect to previous investigations to the submillimeter-wave region, from 230 GHz up to 1.06 THz. The resulting spectroscopic parameters, which have an accuracy comparable to that of the constants obtained from an updated isotopic invariant fit involving data for three electronic states and six isotopologues [Yu et al. High resolution spectral analysis of oxygen. IV. Energy levels, partition sums, bandconstants, RKR potentials, Franck–Condon factors involving the X 3 Σ g − , a 1 Δ g , and b 1 Σ g + states. J Chem Phys 2014;141:174302/1–12], permit the prediction…

PhysicsQuantum-chemical calculationAtomic and Molecular Physics and OpticRadiation010304 chemical physicsTerahertz radiationRadiationRotational and hyperfine parameter010402 general chemistry01 natural sciencesAtomic and Molecular Physics and OpticsRotational spectrum0104 chemical sciences17O2 isotopologue0103 physical sciencesPartition (number theory)IsotopologueAtomic physicsInvariant (mathematics)Constant (mathematics)SpectroscopyHyperfine structureSpectroscopyJournal of Quantitative Spectroscopy and Radiative Transfer
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Constraining multi-Higgs flavour models

2014

To study a flavour model with a non-minimal Higgs sector one must first define the symmetries of the fields; then identify what types of vacua exist and how they may break the symmetries; and finally determine whether the remnant symmetries are compatible with the experimental data. Here we address all these issues in the context of flavour models with any number of Higgs doublets. We stress the importance of analysing the Higgs vacuum expectation values that are pseudo-invariant under the generators of all subgroups. It is shown that the only way of obtaining a physical CKM mixing matrix and, simultaneously, non-degenerate and non-zero quark masses is requiring the vacuum expectation value…

PhysicsQuarkCP ViolationParticle physicsMassesPhysics and Astronomy (miscellaneous)Group (mathematics)High Energy Physics::LatticeFlavourHigh Energy Physics::PhenomenologyFOS: Physical sciencesContext (language use)Discrete SymmetriesAnglesSymmetry (physics)Higgs sectorHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Physics and AstronomyHiggs bosonHigh Energy Physics::ExperimentBaryon numberEngineering (miscellaneous)
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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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Charm and bottom baryon decays in the Bethe-Salpeter approach: Heavy to heavy semileptonic transitions

1998

Charm and bottom baryons and mesons are studied within the framework of a relativistically covariant 3D reduction of the Bethe-Salpeter equation. We carry out an analysis of semileptonic decays of heavy hadrons within this framework using explicit oscillator-type wave functions where we calculate Isgur-Wise functions, decay rates and asymmetry parameters. Within this model we also study the effect of interactions between the light quarks inside the heavy baryon and how they affect the values of the computed heavy baryon observables. We also elaborate on the role of relativistic effects in the calculation of the heavy baryon Isgur-Wise function.

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsBethe–Salpeter equationMesonmedia_common.quotation_subjectHadronNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesAsymmetryNuclear physicsBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentCharm (quantum number)Relativistic quantum chemistryNuclear Experimentmedia_common
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Effective Lagrangian approach to neutrinoless double beta decay and neutrino masses

2012

Neutrinoless double beta ($0\nu\beta\beta$) decay can in general produce electrons of either chirality, in contrast with the minimal Standard Model (SM) extension with only the addition of the Weinberg operator, which predicts two left-handed electrons in the final state. We classify the lepton number violating (LNV) effective operators with two leptons of either chirality but no quarks, ordered according to the magnitude of their contribution to \znbb decay. We point out that, for each of the three chirality assignments, $e_Le_L, e_Le_R$ and $e_Re_R$, there is only one LNV operator of the corresponding type to lowest order, and these have dimensions 5, 7 and 9, respectively. Neutrino masse…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaType (model theory)Lepton numberPartícules (Física nuclear)Standard Model (mathematical formulation)High Energy Physics - PhenomenologyOperator (computer programming)High Energy Physics - Phenomenology (hep-ph)Double beta decayBeyond Standard ModelNeutrino PhysicsHigh Energy Physics::ExperimentNeutrinoLepton
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Spectator Effects in the Heavy Quark Effective Theory

1996

We present a complete analysis of the Heavy Quark Effective Theory Lagrangian at order $1/m^2$ in the leading logarithmic approximation, including effects induced by spectator quarks. At this order new correction terms appear in the effective Lagrangian, as four-quark operators containing both heavy and light quark fields. We compute the coefficients of these operators to one-loop order and in the leading-logarithmic approximation. Two of them break the heavy quark spin symmetry and we estimate their contribution to the hyperfine splitting of the heavy mesons in the factorization approximation. We find that they make a positive contribution to the hyperfine splitting of about 10% of the mea…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsLogarithmMesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)FactorizationHeavy quark effective theoryOrder (group theory)High Energy Physics::ExperimentCharm (quantum number)Nuclear ExperimentHyperfine structure
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Four-quark spectroscopy within the hyperspherical formalism

2006

We present a generalization of the hyperspherical harmonic formalism to study systems made of quarks and antiquarks of the same flavor. This generalization is based on the symmetrization of the $N-$body wave function with respect to the symmetric group using the Barnea and Novoselsky algorithm. The formalism is applied to study four-quark systems by means of a constituent quark model successful in the description of the two- and three-quark systems. The results are compared to those obtained by means of variational approaches. Our analysis shows that four-quark systems with exotic $0^{+-}$ and non-exotic $2^{++}$ quantum numbers may be bound independently of the mass of the quark. $2^{+-}$ …

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaConstituent quarkFew-body systemsQuantum numberHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)SymmetrizationInvariant massHigh Energy Physics::ExperimentWave function
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