Search results for "Ground state"

showing 10 items of 928 documents

Determination of the B(E3, 0+ → 3−)-excitation strength in octupole-correlated nuclei near A ≈224 by the means of Coulomb excitation at REX-ISOLDE

2013

The IS475 collaboration conducted Coulomb-excitation experiments with postaccelerated radioactive 220Rn and 224Ra beams at the REX-ISOLDE facility. The beam particles (Ebeam ≈ 2.83 MeV/u) were Coulomb excited using 60Ni, 114Cd, and 120Sn scattering targets. De-excitation γ-rays were detected employing the Miniball array and scattered particles were detected in a silicon detector. Exploiting the Coulomb-excitation code GOSIA for each nucleus several matrix elements could be obtained from the measured γ-ray yields. The extracted 3−||Ê3||0+ matrix element allows for the conclusion that, while 220Rn represents an octupole vibrational system, 224Ra has already substantial octupole correlations i…

PhysicsHistoryScatteringCoulomb excitationPhysics and Astronomy(all)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Charged particleParticle detectorComputer Science ApplicationsEducationNuclear physics25.70.De; 27.90.+b; 23.20.Js/dk/atira/pure/subjectarea/asjc/3100Excited stateCoulombPhysics::Accelerator PhysicsAtomic physicsGround stateExcitationComputingMilieux_MISCELLANEOUS
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Spectroscopy of exotic states of 13C

2014

The differential cross-sections of the elastic and inelastic 13C + α scattering were measured at E (α) = 65 MeV. The radii of the states: 8.86 (1/2¯), 3.09 (1/2+ ) and 9.90 (3/2¯) MeV were determined by the Modified diffraction model (MDM). The radii of the first two levels are enhanced relatively that of the ground state of 13C, confirming the suggestion that the 8.86 MeV state could be an analogue of the Hoyle state in 12C and the 3.09 MeV state has a neutron halo. No enhancement of the radius of the 9.90 MeV state was observed. peerReviewed

PhysicsHoyle stateta114ScatteringPhysicsQC1-999Nuclear TheoryState (functional analysis)RadiusDiffraction modelNeutronHaloAtomic physicsGround stateSpectroscopyNuclear Experiment
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Polarons in thet-J model

1991

A convenient form of the Peierls-Hubbard Hamiltonian is obtained for the case when the Hubbard repulsion is the largest energy parameter. It allows to consider in the spin-wave approximation the properties of the one-hole low-lying excitations of a 2d lattice. For the parameters approximately corresponding to La2CuO4 it is shown that the hole polarons in the CuO2 planes of lightly doped samples are of large size with a solitonlike-shaped highly asymmetric wave function oriented along the diagonals of the planes or of small size depending on the value of the electron-phonon coupling. In both cases the cooperative effect of the electron-phonon and electron-magnon interactions leads to a large…

PhysicsHubbard modelCondensed matter physicsPhononCondensed Matter PhysicsElectronic Optical and Magnetic MaterialsBrillouin zonesymbols.namesakeEffective mass (solid-state physics)Condensed Matter::Superconductivityt-J modelsymbolsCondensed Matter::Strongly Correlated ElectronsGeneral Materials ScienceGround stateWave functionHamiltonian (quantum mechanics)Zeitschrift f�r Physik B Condensed Matter
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Determination of the ground-state hyperfine structure in neutral229Th

2012

The ground-state hyperfine structure of neutral 229Th has been measured for the first time using high-resolution resonance ionization spectroscopy. The measurements were performed as a preparatory work aimed at the identification of the predicted low-lying 7.6 eV isomer in 229Th through an investigation of its hyperfine structure. The hyperfine coupling constants have been extracted for the atomic ground state as well as for three excited states at 26 096, 26 113 and 38 278 cm−1. Due to rather small splittings not all hyperfine components were completely resolved and therefore an extensive χ2-error analysis was performed to achieve reliable results. The ground-state transition to the excite…

PhysicsHyperfine couplingExcited stateResonance ionizationPhysics::Atomic PhysicsAtomic physicsCondensed Matter PhysicsSpectroscopyGround stateHyperfine structureAtomic and Molecular Physics and OpticsJournal of Physics B: Atomic, Molecular and Optical Physics
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New ground state constants of 12CH335Cl and 12CH337Cl from global polyad analysis

2005

Abstract A global analysis of the infrared spectrum of chloromethane involving the ground state and the 13 vibrational states lying up to 2600 cm −1 was recently achieved using high resolution Fourier transform spectra of pure isotopomers. More than 20 000 transitions (cold and hot bands) for each isotopomer 12 CH 3 35 Cl and 12 CH 3 37 Cl have been assigned and fitted with a standard deviation of about 3 × 10 −4  cm −1 close to the experimental precison. As part of this global effort, improved ground state constants up to sextic centrifugal distortion terms have been determined for each isotopomer taking advantage of the numerous allowed and perturtation-allowed transitions simultaneously …

PhysicsInfraredChloromethaneRotational–vibrational spectroscopyPolyadAtomic and Molecular Physics and OpticsStandard deviationIsotopomerschemistry.chemical_compoundNuclear magnetic resonancechemistryDistortionPhysical and Theoretical ChemistryAtomic physicsGround stateSpectroscopyJournal of Molecular Spectroscopy
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The electron affinity of phosphorus

2007

We have measured the energies of all three fine structure components in the 3PJ ground state of the negative ion of phosphorus using laser photodetachment threshold spectroscopy. The experiment yielded an electron affinity of 746.68(6) meV. The ΔJ = 2–0, 2–1 and 1–0 fine structure splittings were determined to be 32.73(7) meV, 22.48(7) meV and 10.25(3) meV, respectively. In the experiment, a mass selected beam of P− ions was merged with the output from a pulsed infrared optical parametric oscillator. The residual atoms produced in the photodetachment process were detected and used as a monitor of the photon-energy dependence of the relative cross section. The Wigner law was fitted to each o…

PhysicsInfraredCondensed Matter PhysicsLaserAtomic and Molecular Physics and Opticslaw.inventionIonlawElectron affinityOptical parametric oscillatorAtomic physicsGround stateSpectroscopyBeam (structure)Journal of Physics B: Atomic, Molecular and Optical Physics
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Analysis of the Infrared Fourier Transform Spectrum of the Spectra of Silane in the Range 2930-3300 cm(-1).

1999

The infrared spectrum of (28)SiH(4) between 2930 and 3300 cm(-1) was recorded using the Laboratoire de Physique Moleculaire et Applications (LPMA.) Fourier transform spectrometer. The instrumental response function width chosen makes it possible to obtain a Doppler-limited spectrum. The observed spectrum belongs to the tetrad built with one quantum of stretching mode (nu(1) or nu(3)) and one quantum of bending mode (nu(2) or nu(4)). The excited states are formed from eight vibrational sublevels: nu(1) + nu(2)(E), nu(1) + nu(4)(F(2)), nu(2) + nu(3)(F(1) + F(2)), and nu(3) + nu(4)(A(1) + E + F(1) + F(2)). The intricacy of the upper states was resolved using the variations of the line strength…

PhysicsInfraredExtrapolationAtomic and Molecular Physics and OpticsSpectral linesymbols.namesakeNuclear magnetic resonanceFourier transformExcited statesymbolsPhysical and Theoretical ChemistryAtomic physicsGround stateTetradHamiltonian (quantum mechanics)SpectroscopyJournal of molecular spectroscopy
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High-Resolution Spectroscopy and Preliminary Analysis of the ν1/ν8 Dyad of SF535Cl

2001

Abstract The Fourier transform infrared spectrum of monoisotopic SF 5 35 Cl has been recorded in the 650- to 960-cm −1 region at a temperature of 203 K, a pressure of 0.2 mbar, and an instrumental bandwidth of 0.002 cm −1 . The ν 1 /ν 8 dyad near 900 cm −1 has been analyzed with an effective Hamiltonian developed up to the fourth order and the help of a recently developed set of programs called C 4 v TDS ( C 4 v Top Data System, http://www.u-bourgogne.fr/LPUB/C4VTDS.html ); 1346 transitions for ν 1 , 351 transitions for ν 8 , and 406 ground state combination differences have been assigned and fitted. A global fit has been obtained with an rms of 0.00082 cm −1 for the ν 1 ( a 1 ) band, of 0.…

PhysicsInfraredHigh resolutionAtomic and Molecular Physics and OpticsPreliminary analysissymbols.namesakeFourier transformNuclear magnetic resonancesymbolsMonoisotopic massPhysical and Theoretical ChemistryAtomic physicsHamiltonian (quantum mechanics)Ground stateSpectroscopySpectroscopyJournal of Molecular Spectroscopy
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Study of the Fundamental Bands of 70GeD4 by High-Resolution Raman and Infrared Spectroscopy: First Experimental Determination of the Equilibrium Bond…

2002

Abstract The four fundamental bands of 70 GeD 4 have been analyzed using the STDS software developed in Dijon (http://www.u-bourgogne.fr/LPUB/sTDS.html). Both infrared and Raman spectra were used to observe all fundamental bands. Infrared spectra of monoisotopic 70 GeD 4 were recorded in the regions 600 and 1500 cm −1 using the Bruker 120HR interferometer at Wuppertal. The resolution (1/maximum optical path difference) was between 2.3 and 3.3×10 −3 cm −1 for the ν 3 and ν 4 infrared-active fundamental bands as well as for the interacting ν 2 band. A high-resolution stimulated Raman spectrum of the ν 1 band has been recorded in Madrid. The instrumental resolution of the Raman spectrum was 3.…

PhysicsInfraredResolution (electron density)Infrared spectroscopyAtomic and Molecular Physics and OpticsBond lengthchemistry.chemical_compoundsymbols.namesakeNuclear magnetic resonancechemistryGermanesymbolsPhysical and Theoretical ChemistryAtomic physicsGround stateRaman spectroscopySpectroscopyOptical path lengthJournal of Molecular Spectroscopy
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Analysis of the infrared Fourier transform spectrum of the Dyad of 116SnH4

1990

Abstract The FTIR spectrum of monoisotopic 116SnH4 has been recorded with the Bruker 120 HR interferometer at Giessen, West Germany, in the ν 2 ν 4 range extending from 600 to 850 cm−1. The resolution (FWHM) was 2.1 × 10−3 cm−1. The Dyad ν 2 ν 4 (0100, 0001) was analyzed using a sixth-order Hamiltonian. The analysis of infrared transitions enabled us to determine 10 ground state parameters, 9 ν2 parameters, 17 ν4 parameters, and 18 interaction parameters. Of 3800 calculated transitions assigned to observed lines, 1183 unblended lines have been selected for the data refinement. For J ≤ 19, the value of the standard deviation is of the order of magnitude of the estimated experimental accuracy…

PhysicsInfraredRotational transitionAtomic and Molecular Physics and Opticssymbols.namesakeFull width at half maximumFourier transformNuclear magnetic resonancesymbolsMonoisotopic massPhysical and Theoretical ChemistryAtomic physicsFourier transform infrared spectroscopyGround stateHamiltonian (quantum mechanics)SpectroscopyJournal of Molecular Spectroscopy
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