Excited States in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="normal">P</mml:mi></mml:mrow><mml:mrow><mml:mn>29</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>from the Scattering of Protons by<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msup><mml:mrow><mml:mi mathvariant="normal">Si</mml:mi></mml:mrow><mml:mrow><mml:mn>28</mml:mn></mml:mrow></mml:msup></mml:mrow></mml:math>

Belote, T.A.; Kashy, E.; Risser, J.R.

doi:10.1103/physrev.122.920

Cited by 43 publications

(6 citation statements)

References 10 publications

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“…A compilation of these resonances is given in Table 29.22 of [15] which we have used with the following changes. The 6,577 and 7,272 KeV levels were not observed in elastic scattering [26]. A level at 6,577 KeV does also exist.…”

Section: Assignment Of Mirror Levels In 29si and 29pmentioning

confidence: 74%

“…Hence they appear, in general, as resonances in the elastic and/or inelastic proton scattering off 28Si. The widths of these levels could not be measured [23,26] they are, however, smaller than, say, 3 KeV. The excitation energy of the 200 KeV wide level, which is the Ep=3.98 MeV resonance, is 6,590 KeV rather than 6,577 KeV.…”

Section: Assignment Of Mirror Levels In 29si and 29pmentioning

confidence: 99%

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Spectroscopy of highly excited states in29Si

et al. 1982

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Particle y-ray coincidences have been measured in the 28Si (d, py) reaction at 6.5 and 7 MeV bombarding energy, in the 26Mg (c~, ny) reaction at 12, 14 and 15 MeV, and in the 27A1 (z, py) reaction at 9 MeV. The ;~-decay has been observed for all bound states of 29Si and for 56 unbound states up to 12,960 KeV excitation energy. Particle ?;-ray angular correlations were measured in the 2ssi (d, pT) reaction at 6.5 MeV and in the 26Mg (cg nT) reaction at 12 MeV. Spin (-parity) assignments or restrictions were obtained for nearly all bound states and some high-spin states above the binding energy. The assignment of mirror levels in 29Si and 29p has been extended to 8.2 MeV excitation energy. The excitation energies of 41 positive-parity states are reproduced by shell model calculations. The possible existence of a K~=5/2 + band with prolate deformation is discussed.

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Section: Assignment Of Mirror Levels In 29si and 29pmentioning

confidence: 74%

Section: Assignment Of Mirror Levels In 29si and 29pmentioning

confidence: 99%

Spectroscopy of highly excited states in29Si

et al. 1982

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“…However, direct inner shell ionization in projectile-like fragment ions can be accompanied by different nuclear reactions e.g. inelastic scattering [18,19], transfer reactions [20,21], stripping reactions [22], fusion reactions [23,24] etc. also.…”

Section: Theoretical Work Results and Discussionmentioning

confidence: 99%

Theoretical studies on shaking processes in nuclear transfer reactions

Sharma

Nandi

2015

Nuclear Physics A

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“…(1) of Belote, Kashy, and Risser. 11 The hard-sphere phases were put into the program as quadratic expressions, <f>i=Ai+BiE+CiE z J with E in MeV. The values of the coefficients used in the final elastic fits are given in Table I. Resonance shapes from isolated states formed with /^4 are shown in Fig.…”

Section: Elastic Scatteringmentioning

confidence: 99%

Level Assignments inO17fromC13(α

1965

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C 13 («,a)C 13 cross sections at center-of-mass angles 54.7°, 107.9°, 142.6°, and 169.6° and C 13 (a,#)0 16 cross sections at 0° have been measured at a-particle energies from 2 to 3.5 MeV. From dispersion-theory analysis, a consistent set of J* and partial-width values has been obtained for eleven states of the compound nucleus O 17 with excitation energies between 8 and 9 MeV. I. INTRODUCTIONT HE C 13 (a,w)0 16 reaction has been extensively investigated 1-5 at a-particle bombarding energies below 5 MeV. Resonances from sharp energy states of the compound nucleus O 17 are observed. We have measured 6 the C 13 (a,a)C 13 differential elastic-scattering cross sections for a-particle bombarding energies from 2.0 to 3.5 MeV at center-of-mass angles 54.7, 107.9,142.6, and 169.6°. C ls (a,n)O u differential reaction cross sections at 0° were measured simultaneously. Elastic-scattering and reaction data were analyzed to determine the J T and the a-particle and neutron partial widths of the states of O 17 corresponding to the observed resonances.The range 2 to 3.5 MeV of a-particle bombarding energies corresponds to the range 7.9 to 9 MeV of excitation energies in the compound nucleus O 17 . Values of / and of neutron and a-particle partial widths for many of the states at these excitation energies were known from C 13 (a,w)0 16 differential cross sections 2-5 and from total cross sections of O 16 for neutrons. 2 -5 » 7 From interference terms in C 13 (a,w)0 16 angular distributions, 4 -5 relative parities of a number of states were known. To determine parities and to make complete determinations of J and partial-width values, C 13 -(a,a)C 13 and O u (n y n)O u elastic-scattering experiments are necessary. The parameters of two states at the low end of the energy interval have recently been determined from analysis of 0 16 (^,w)0 16 angular distributions. 8

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Excited States inP29from the Scattering of Protons bySi28

Cited by 43 publications

References 10 publications

Spectroscopy of highly excited states in29Si

Spectroscopy of highly excited states in29Si

Theoretical studies on shaking processes in nuclear transfer reactions

Level Assignments inO17fromC13(α

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