Search results for "Ground State"

showing 10 items of 928 documents

Halo-like structure in 7He nucleus

2020

Abstract A study of the neutron structure of the ground state of 7He has been performed by means of registration and analysis of the decay channels of the residual nuclei following absorption of stopped pions. In particular, the reaction 9Be ( π − , d )X have been investigated where X denotes any system with five neutrons and two protons – the constituencies of a 7He nucleus. It was shown that the structure of 7He is determined by correlations of two neutrons in the states 6He (0+), 6He (2+) and one neutron in the shell p3/2. The 4He+3n structure is not manifested in the ground state of 7He. The obtained results are consistent with the known data on considerable mixture of configurations “6…

PhysicsDiffractionHistoryRadiusComputer Science ApplicationsEducationPionmedicine.anatomical_structureTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYExcited statemedicineNeutronHaloAtomic physicsGround stateNucleusJournal of Physics: Conference Series
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PNO-CI and CEPA studies of electron correlation effects

1974

Ab initio calculations of the potential curves of low laying electronic states of OH are performed on the basis of a variational configuration interaction wavefunction (PNO-CI) and the coupled electron pair approximation (CEPA). The latter approach yields a ground state potential curve which deviates from the RKR curve by less than 200 cm−1 in the region from 0.7 to 1.6 A. Calculated ground state constants are as follows (experimental values in parentheses): r e = 0.972 (0.971) A, B e = 18.85 (18.87) cm−1, α e = 0.727 (0.714) cm−1, ω e = 3742 (3739) cm−1, ω e χ e = 85.3 (86.4) cm−1, μ0 = 1.686 (1.66) D, D e = 4.35 (4.63) eV,IP = 12.78 (13.36?) eV, El.Aff. = 1.51 (1.83) eV, v 00(2Π↔2Σ+) = 32…

PhysicsDipoleElectron pairElectronic correlationAb initio quantum chemistry methodsIonizationElectron affinityChiropracticsPhysical and Theoretical ChemistryConfiguration interactionAtomic physicsGround stateTheoretica Chimica Acta
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Solvation of triplet Rydberg states of molecular hydrogen in superfluid helium

2004

We report ab initio interaction potentials, transition dipole moments, and radiative lifetimes for the four lowest triplet states of ${\mathrm{H}}_{2}:$ $b$ ${}^{3}{\ensuremath{\Sigma}}_{u}^{+},$ $c$ ${}^{3}{\ensuremath{\Pi}}_{u},$ $a$ ${}^{3}{\ensuremath{\Sigma}}_{g}^{+},$ and $e$ ${}^{3}{\ensuremath{\Sigma}}_{u}^{+},$ and their response to the perturbation due to approaching ground state He atom. Hybrid density functional\char21{}quantum Monte Carlo calculations employing the ab initio interaction potentials are then used for calculating the liquid structure around the molecular excimers in bulk superfluid ${}^{4}\mathrm{He}.$ Calculations demonstrate a wide variety of possible solvation …

PhysicsDipolesymbols.namesakeHelium-4Absorption spectroscopyQuantum Monte CarloMetastabilityAb initioRydberg formulasymbolsAtomic physicsGround stateAtomic and Molecular Physics and OpticsPhysical Review A
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Shell-model study of the highly forbidden beta decay 48 Ca → 48 Sc

1999

Ordinary β− decay of the 0+ ground state of 48Ca is studied. Partial half-lives for the highly-forbidden transitions to the three lowest-lying states (6+,5+,4+) of 48Sc are calculated by using both the harmonic oscillator and the Woods-Saxon mean-field wave functions. We find the decay to be dominated, as expected, by the unique fourth-forbidden transition to the excited 5+ state of 48Sc. The theoretical beta-decay half-life of 48Ca is found to be 1.1−0.6+0.8·1021 years which is approximately 25 times longer than the measured double-beta-decay half-life of T1/22ν = (4.3−1.1+2.4[stat] ± 1.4[syst])·1019 years.

PhysicsDouble beta decayExcited stateSHELL modelGeneral Physics and AstronomyState (functional analysis)Atomic physicsGround stateWave functionBeta decayHarmonic oscillatorEurophysics Letters (EPL)
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Calculation of atomic spectra and transition amplitudes for superheavy element Db (Z=105)

2018

Atomic spectra and other properties of superheavy element dubnium (Db, $Z=105$) are calculated using recently developed method combining configuration interaction with perturbation theory [the CIPT method, V. A. Dzuba, J. C. Berengut, C. Harabati, and V. V. Flambaum, Phys. Rev. A 95, 012503 (2017)]. These include energy levels for low-lying states of Db and Db II, electric dipole transition amplitudes between the ground state and low-lying states of opposite parity, isotope shift for these transitions, and the ionization potential of Db. Similar calculations for Ta, which is a lighter analog of Db, are performed to control the accuracy of the calculations.

PhysicsDubniumAtomic Physics (physics.atom-ph)FOS: Physical scienceschemistry.chemical_elementConfiguration interaction7. Clean energy01 natural sciences010305 fluids & plasmasPhysics - Atomic PhysicsAmplitudechemistry0103 physical sciencesPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)Atomic physicsElectric dipole transitionIonization energyPerturbation theory010306 general physicsGround stateSpectroscopyNuclear Experiment
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Production and detection of atomic hexadecapole at Earth’s magnetic field

2007

We report a novel method that allows selective creation and detection of a macroscopic long lived hexadecapole polarization in the F = 2 ground state of 87Rb atoms at Earth's magnetic field (510 mG).

PhysicsEarth's magnetic fieldchemistryNonlinear opticschemistry.chemical_elementAtomic physicsGround statePolarization (waves)Magnetic fieldRubidiumFrontiers in Optics 2007/Laser Science XXIII/Organic Materials and Devices for Displays and Energy Conversion
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Mo̸ller polarimetry with polarized atomic hydrogen at MESA

2013

A new generation of parity violation (PV) electron scattering experiments are planned to be carried out at the Institut fur Kernphysik in Mainz. These experiments will be performed at low energies of 100-200 MeV using the new accelerator MESA (Mainz Energy recovering Superconducting Accelerator). One of the main challenges of such experiments is to achieve an accuracy in beam polarization measurements that must be below 0.5%. This very high accuracy can be reached using polarized atomic hydrogen gas, stored in an ultra-cold magnetic trap, as the target for electron beam polarimetry based on Mo/ller scattering. Electron spin-polarized atomic hydrogen can be stored at high densities of 1016 c…

PhysicsElastic scatteringHydrogenchemistryScatteringMagnetic trapchemistry.chemical_elementPhysics::Atomic PhysicsElectronAtomic physicsGround stateElectron scatteringMagnetic fieldAIP Conference Proceedings
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Spin-density waves in superdeformed quantum dots

1998

Abstract Electronic shell structure and spin effects in deformed quantum dots are investigated using spin-density functional theory. We recently suggested (Koskinen et al., Phys. Rev. Lett. 79 (1997) 1389) that for circular dots, depending on the density of the two-dimensional electron gas and the electron number, a spin-density wave-like state can occur as a possible ground state. Here these studies are extended to deformed and superdeformed dots, which approach the limit of a finite quantum wire.

PhysicsElectron densityCondensed matter physicsQuantum wireQuantum point contactCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter PhysicsAtomic and Molecular Physics and OpticsElectronic Optical and Magnetic MaterialsQuantum dotPrincipal quantum numberGround stateFermi gasSpin-½Physica E: Low-dimensional Systems and Nanostructures
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Quantum dot state initialization by control of tunneling rates

2019

We study the loading of electrons into a quantum dot with dynamically controlled tunnel barriers. We introduce a method to measure tunneling rates for individual discrete states and to identify their relaxation paths. Exponential selectivity of the tunnel coupling enables loading into specific quantum dot states by tuning independently energy and rates. While for the single-electron case orbital relaxation leads to fast transition into the ground state, for electron pairs triplet-to-singlet relaxation is suppressed by long spin-flip times. This enables the fast gate-controlled initialization of either a singlet or a triplet electron pair state in a quantum dot with broad potential applicati…

PhysicsElectron pairCondensed Matter - Mesoscale and Nanoscale PhysicsFOS: Physical sciences02 engineering and technologyElectronCondensed Matter::Mesoscopic Systems and Quantum Hall Effect021001 nanoscience & nanotechnology01 natural sciencesMolecular physicsQuantum technologyQuantum dotMesoscale and Nanoscale Physics (cond-mat.mes-hall)0103 physical sciencesRelaxation (physics)Singlet state010306 general physics0210 nano-technologyGround stateQuantum tunnellingPhysical Review B
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Alpha-particle transfer from 6Li to 28Si leading to high excitation of 32S

2006

The excitation of 32S to energies from 24 to 37 MeV followed by its decay to 28Si has been brought about by the two-step alpha transfer reaction 28Si(6Li,d)32S*→α+28Si. A sudden perishing of the decay to the 28Si ground state occurs at 31 MeV of excitation. At about the same energy an increase in the decay to the first excited 2+ state is observed. The yields of 28Si in its ground state or excited to the 21+ and 41+ state prohibit strong fluctuations. This supports the assumption of the existence of states at high excitation in 32S. The results are based on d–α coincidences, which were found to exhibit a strong forward–backward correlation.

PhysicsExcited stateAlpha particleAtomic physicsCondensed Matter PhysicsGround stateMathematical PhysicsAtomic and Molecular Physics and OpticsExcitationPhysica Scripta
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