Search results for "Good quantum number"

showing 7 items of 7 documents

Nonadiabatic transitions between lambda-doubling states in the capture of a diatomic molecule by an ion

2008

The low-energy capture of a dipolar diatomic molecule in an adiabatically isolated electronic state with a good quantum number Hund’s coupling case a by an ion occurs adiabatically with respect to rotational transitions of the diatom. However, the capture dynamics may be nonadiabatic with respect to transitions between the pair of the -doubling states belonging to the same value of the intrinsic angular momentum j. In this work, nonadiabatic transition probabilities are calculated which define the -doubling j-specific capture rate coefficients. It is shown that the transition from linear to quadratic Stark effect in the ion-dipole interaction, which damps the T �1/2 divergence of the captur…

IonsAngular momentumTime FactorsRotationChemistryStatic ElectricityGeneral Physics and AstronomyElectronsElectronDiatomic moleculeIonGood quantum numbersymbols.namesakeDipoleStark effectsymbolsQuantum TheoryThermodynamicsPhysical and Theoretical ChemistryAtomic physicsAdiabatic processAlgorithmsThe Journal of Chemical Physics
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Nuclear weak response from the combined study of beta-decay and charge-exchange reaction

2009

Studying the weak nuclear response, especially the Gamow-Teller (GT) transitions, of stable as well as unstable pf-shell nuclei, is one of the key issues in nuclear and astro-nuclear physics. We study the decay half-lives and the GT transitions starting from Tz = ±1 and ±2 mirror nuclei, respectively, by means of β decays and complementary hadronic (3 He , t) charge-exchange reactions. Under the assumption that isospin is a good quantum number, symmetry is expected for mirror nuclei and the GT transitions starting from the mirror nuclei. The half-lives and branching ratios and the measured strength distributions of GT transitions are compared and also combined for the understanding of the …

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsHadronNuclear TheoryNuclear structureGeneral Physics and Astronomy[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Key issues01 natural sciencesGood quantum numberNuclear physicsIsospin0103 physical sciencesMirror nucleiAtomic physics010306 general physicsNuclear ExperimentCharge exchange
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Isomeric states in Rf256

2021

The question of the number and origin of isomeric states in $^{256}\mathrm{Rf}$ arose from two independent experiments but remained unanswered for a decade. To shed light on this puzzle, we studied isomeric decay in $^{256}\mathrm{Rf}$ by measuring conversion electrons with fast fully digital electronics. $^{256}\mathrm{Rf}$ was produced in the fusion-evaporation reactions of $^{50}\mathrm{Ti}+^{207}\mathrm{Pb}$ and $^{50}\mathrm{Ti}+^{208}\mathrm{Pb}$ at the gas-filled recoil separator TransActinide Separator and Chemistry Apparatus. Among a total of 120 decays of $^{256}\mathrm{Rf}$, we detected 22 and 12 decays proceeding through one and two isomeric states. Half-lives of the low- and hi…

PhysicsGood quantum numbereducation.field_of_studyPopulationTransactinide elementProduction (computer science)ElectronAtomic physicseducationRecoil separatorPhysical Review C
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Identifying spin and parity of charmonia in flight with lattice QCD

2019

The spectrum of charmonium resonances contains a number of unanticipated states along with several conventional quark-model excitations. The hadrons of different quantum numbers $J^P$ appear in a fairly narrow energy band, where $J^P$ refers to the spin-parity of a hadron at rest. This poses a challenge for Lattice QCD studies of (coupled-channel) meson-meson scattering aimed at the determination of scattering amplitudes and resonance pole positions. A wealth of information for this purpose can be obtained from the lattice spectra in frames with nonzero total momentum. These are particularly dense since hadrons with different $J^P$ contribute to any given lattice irreducible representation.…

PhysicsQuantum chromodynamicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::LatticeHigh Energy Physics - Lattice (hep-lat)ddc:530High Energy Physics::PhenomenologyQuark modelLattice field theoryFOS: Physical sciencesLattice QCD530 PhysikQuantum number01 natural sciencesGood quantum numberHigh Energy Physics - PhenomenologyHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Irreducible representationHadron spectroscopy0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsPhysical Review D
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The T[sub z] = −1→ T[sub z] =0 beta decays and comparison with Charge Exchange reactions

2011

Gamow‐Teller (GT) transitions can be studied in both β decay and charge exchange (CE) reactions. If isospin is a good quantum number, then the Tz = −1→0 and Tz = +1→0 GT mirror transitions, are identical. Therefore, a comparison of the results from studies of β decay and CE should shed light on this assumption. Accordingly we have studied the β decay of the Tz = −1 fp‐shell nuclei, 54Ni, 50Fe, 46Cr, and 42Ti, produced in fragmentation and we have compared our results with the spectra from (3He, t) measurements on the mirror Tz = +1 target nuclei studied in high resolution at RCNP, Osaka. The β decay experiments were performed as part of the STOPPED beam RISING campaign at GSI.

PhysicsGood quantum numberNuclear physicsDecay schemeFragmentation (mass spectrometry)Helium-3IsospinAtomic physicsBeta decaySpectral lineParticle detectorAIP Conference Proceedings
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Non-isospectral Hamiltonians, intertwining operators and hidden hermiticity

2011

We have recently proposed a strategy to produce, starting from a given hamiltonian $h_1$ and a certain operator $x$ for which $[h_1,xx^\dagger]=0$ and $x^\dagger x$ is invertible, a second hamiltonian $h_2$ with the same eigenvalues as $h_1$ and whose eigenvectors are related to those of $h_1$ by $x^\dagger$. Here we extend this procedure to build up a second hamiltonian, whose eigenvalues are different from those of $h_1$, and whose eigenvectors are still related as before. This new procedure is also extended to crypto-hermitian hamiltonians.

PhysicsQuantum PhysicsGeneral Physics and AstronomyFOS: Physical sciencesMathematical Physics (math-ph)Eigenvalues and eigenvectors of the second derivativeMathematics::Geometric Topologylaw.inventionGood quantum numbersymbols.namesakeintertwining relationsOperator (computer programming)IsospectralInvertible matrixlawQuantum electrodynamicssymbolsHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Settore MAT/07 - Fisica MatematicaEigenvalues and eigenvectorsEigenvalue perturbationMathematical PhysicsMathematical physics
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Tz = ±1 → 0 ISOSPIN SYMMETRY GAMOW-TELLER TRANSITIONS IN pf-SHELL NUCLEI

2010

Studying the Gamow-Teller (GT) transitions of stable as well as unstable pf-shell nuclei is one of the key issues in nuclear and astro-nuclear physics. Under the assumption that isospin T is a good quantum number, symmetry is expected for mirror nuclei and the GT transitions starting from the mirror nuclei. We study the GT transitions starting from Tz = ±1 mirror nuclei, respectively, by means of hadronic (3 He , t) charge-exchange reactions and complementary β decays.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryHadronShell (structure)General Physics and AstronomyAstronomy and AstrophysicsKey issuesSymmetry (physics)Nuclear physicsGood quantum numberIsospinMirror nucleiNuclear ExperimentModern Physics Letters A
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