Energy levels of light nuclei A = 16–17

Ajzenberg‐Selove, F.

doi:10.1016/0375-9474(71)90035-2

Cited by 282 publications

(13 citation statements)

References 10 publications

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“…The detection system was energy calibrated with radioactive sources 6~ 54Mn, 22Na, 228Th, and 88y [ 17]. High energy calibration points were provided by the 6129.70_+0.28 keV line from the contaminant 19F(p,~y)160 reaction [18]. The linearity of the analyzing system was studied separately with the above sources and a 56Co source.…”

Section: Decay Schemementioning

confidence: 99%

Excited levels and isobaric analogue states in55Co investigated with the54Fe(p, ?)55Co reaction

Erlandsson

Lyttkens

1977

Z Physik A

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The yield curve for the S4Fe(p, 7)~5Co reaction in the energy region Ev= 1.5-2.9 MeV has been recorded and the decay of ten resonances has been investigated. For six of the resonances the strengths have been determined. The angular distributions of the gamma rays have been recorded for four resonances to obtain spins or spin limitations for excited levels. In addition the lifetimes of 10 bound levels were determined with the Doppler Shift Attenuation Method. The isobaric analogues of the ground state and five excited states in 55Fe are discussed.

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Section: Decay Schemementioning

confidence: 99%

Excited levels and isobaric analogue states in55Co investigated with the54Fe(p, ?)55Co reaction

Erlandsson

Lyttkens

1977

Z Physik A

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“…The average uncertainty concerning the particle production cross sections of nat N(d,d 0 [26][27][28][29][30][31][32] and two works recently [33,34]. Previous results were compiled in [35][36][37]. Because of the high Q value of the reaction, very high states are excited in the compound nucleus 16 O (E x ≥ 20 MeV).…”

Section: Particle Production Cross Sectionsmentioning

confidence: 99%

Measurement of gamma-ray production cross sections for nuclear reactions 14N(d,pγ)15N and 28Si(d,pγ)29Si

Csedreki

Uzonyi

Szikszai

et al. 2014

Nuclear Instruments and Methods in Physics Research Section B:

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In this work the differential cross sections for gamma-ray emission from the 14 implanted Si detector at 135 0 with respect to the beam direction in the deuteron energy range 0.65 -2.0 MeV. The target was a thin silicon-nitride film. Gamma-ray angular distribution measurements were performed to determine the possible anisotropy of the gamma-ray emission, and the measured cross section values were converted into total gamma-ray producing cross sections for most of the gamma-ray emissions. The average uncertainties of nitrogen and silicon gamma-ray production cross sections are 5% and 12%, respectively and 8% concerning the particle production cross section of nat N(d,d 0

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“…A rather unique method of using the time-of-flight spectra peak channels for all angles simultaneously was used to extract the excitation energies [1]. Given in Table 1 are the excitation energies as measured in the present experiment and as tabulated by Ajzenberg-Selove [4]. …”

Section: Resultsmentioning

confidence: 99%

“…Of particular interest in the present investigation was the sixth excited state of ~70 (Ex=5.22 MeV) for which no counterpart in 17F had been reported in the literature until recently [1][2][3]. With the exception of the sixth excited state of 170 the energy level parameters [4] of 170 and 17F nearly coincide through the first twelve excited states (6 MeV excitation energy). The 5.22 MeV state of 170 is weakly excited in the 160 (d, p)170 reaction [5], but is moderately excited in the ~5N(aHe, p)170 [6], 14N(a, p)170 [7], 13C(6Li, d)170 and 13C(7Li, 0170 [8] reactions.…”

Section: Introductionmentioning

confidence: 94%

Investigation of states in17F by the15N(3He,n)17F reaction

Etten

Thornton

1973

Z. Physik

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The absolute differential cross sections for several levels in the lSN(3He, n)17F reaction were measured at laboratory scattering angles from 0 to 140 degrees using neutron time-of-flight techniques. Angular distributions were obtained at effective helion bombarding energies of 3.8 and 4.8 MeV. A new state was identified at 5.18__+ 0.02 MeV excitation energy which is probably the analogue of the 5.217 MeV state in 170. Spectroscopic factors were obtained for the low-lying states using distorted wave method calculations.

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Energy levels of light nuclei A = 16–17

Cited by 282 publications

References 10 publications

Excited levels and isobaric analogue states in55Co investigated with the54Fe(p, ?)55Co reaction

Excited levels and isobaric analogue states in55Co investigated with the54Fe(p, ?)55Co reaction

Measurement of gamma-ray production cross sections for nuclear reactions 14N(d,pγ)15N and 28Si(d,pγ)29Si

Investigation of states in17F by the15N(3He,n)17F reaction

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