Intermediate structures in [Formula Presented] studied with the γ-ray recoil method

H. Fujita; M. Hijiya; Y. Inotani; T. Mukae; K. Koga; M. Koga; F. Nakamura; S. Koto; T. Sugimitsu; N. Ikeda; S. Morinobu; Y. Sugiyama; Y. Tomita; H. Ikezoe; Y. Yamanouti; K. Ideno; S. Hamada; T. Ikuta

doi:10.1103/PhysRevC.66.024609

Intermediate structures in [Formula Presented] studied with the γ-ray recoil method

H. Fujita, M. Hijiya, Y. Inotani, T. Mukae, K. Koga, M. Koga, F. Nakamura, S. Koto, T. Sugimitsu, N. Ikeda, S. Morinobu, Y. Sugiyama, Y. Tomita, H. Ikezoe, Y. Yamanouti, K. Ideno, S. Hamada, T. Ikuta

Applied Nuclear Physics

Research output: Contribution to journal › Article › peer-review

Abstract

The intermediate structures in [Formula Presented] inelastic scattering were investigated at energies around [Formula Presented] in the [Formula Presented] single excitation and the [Formula Presented] mutual excitation channels and at [Formula Presented] in the [Formula Presented] single excitation channel. The angular distributions of the magnetic substate cross sections for the [Formula Presented] (4.439 MeV) state of [Formula Presented] were measured by using the γ-ray recoil method in the center-of-mass ejectile-axis frame. It is shown that the structures at [Formula Presented] and 31.8 MeV in the [Formula Presented] channel are interpreted as resonances of [Formula Presented] or [Formula Presented] which decay dominantly through the aligned configurations with [Formula Presented] On the other hand, the structure at [Formula Presented] is accounted for by assuming the overlap of two resonances having spins and parities of [Formula Presented] and [Formula Presented] In the [Formula Presented] channel, little oscillatory structures are observed in the m-substate angular distributions so that the resonance spins cannot be extracted.

Original language	English
Pages (from-to)	14
Number of pages	1
Journal	Physical Review C - Nuclear Physics
Volume	66
Issue number	2
DOIs	https://doi.org/10.1103/PhysRevC.66.024609
Publication status	Published - 2002

All Science Journal Classification (ASJC) codes

Nuclear and High Energy Physics

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10.1103/PhysRevC.66.024609

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Fujita, H., Hijiya, M., Inotani, Y., Mukae, T., Koga, K., Koga, M., Nakamura, F., Koto, S., Sugimitsu, T., Ikeda, N., Morinobu, S., Sugiyama, Y., Tomita, Y., Ikezoe, H., Yamanouti, Y., Ideno, K., Hamada, S., & Ikuta, T. (2002). Intermediate structures in [Formula Presented] studied with the γ-ray recoil method. Physical Review C - Nuclear Physics, 66(2), 14. https://doi.org/10.1103/PhysRevC.66.024609

Fujita, H, Hijiya, M, Inotani, Y, Mukae, T, Koga, K, Koga, M, Nakamura, F, Koto, S, Sugimitsu, T, Ikeda, N, Morinobu, S, Sugiyama, Y, Tomita, Y, Ikezoe, H, Yamanouti, Y, Ideno, K, Hamada, S & Ikuta, T 2002, 'Intermediate structures in [Formula Presented] studied with the γ-ray recoil method', Physical Review C - Nuclear Physics, vol. 66, no. 2, pp. 14. https://doi.org/10.1103/PhysRevC.66.024609

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title = "Intermediate structures in [Formula Presented] studied with the γ-ray recoil method",

abstract = "The intermediate structures in [Formula Presented] inelastic scattering were investigated at energies around [Formula Presented] in the [Formula Presented] single excitation and the [Formula Presented] mutual excitation channels and at [Formula Presented] in the [Formula Presented] single excitation channel. The angular distributions of the magnetic substate cross sections for the [Formula Presented] (4.439 MeV) state of [Formula Presented] were measured by using the γ-ray recoil method in the center-of-mass ejectile-axis frame. It is shown that the structures at [Formula Presented] and 31.8 MeV in the [Formula Presented] channel are interpreted as resonances of [Formula Presented] or [Formula Presented] which decay dominantly through the aligned configurations with [Formula Presented] On the other hand, the structure at [Formula Presented] is accounted for by assuming the overlap of two resonances having spins and parities of [Formula Presented] and [Formula Presented] In the [Formula Presented] channel, little oscillatory structures are observed in the m-substate angular distributions so that the resonance spins cannot be extracted.",

author = "H. Fujita and M. Hijiya and Y. Inotani and T. Mukae and K. Koga and M. Koga and F. Nakamura and S. Koto and T. Sugimitsu and N. Ikeda and S. Morinobu and Y. Sugiyama and Y. Tomita and H. Ikezoe and Y. Yamanouti and K. Ideno and S. Hamada and T. Ikuta",

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AU - Fujita, H.

AU - Hijiya, M.

AU - Inotani, Y.

AU - Mukae, T.

AU - Koga, K.

AU - Koga, M.

AU - Nakamura, F.

AU - Koto, S.

AU - Sugimitsu, T.

AU - Ikeda, N.

AU - Morinobu, S.

AU - Sugiyama, Y.

AU - Tomita, Y.

AU - Ikezoe, H.

AU - Yamanouti, Y.

AU - Ideno, K.

AU - Hamada, S.

AU - Ikuta, T.

PY - 2002

Y1 - 2002

N2 - The intermediate structures in [Formula Presented] inelastic scattering were investigated at energies around [Formula Presented] in the [Formula Presented] single excitation and the [Formula Presented] mutual excitation channels and at [Formula Presented] in the [Formula Presented] single excitation channel. The angular distributions of the magnetic substate cross sections for the [Formula Presented] (4.439 MeV) state of [Formula Presented] were measured by using the γ-ray recoil method in the center-of-mass ejectile-axis frame. It is shown that the structures at [Formula Presented] and 31.8 MeV in the [Formula Presented] channel are interpreted as resonances of [Formula Presented] or [Formula Presented] which decay dominantly through the aligned configurations with [Formula Presented] On the other hand, the structure at [Formula Presented] is accounted for by assuming the overlap of two resonances having spins and parities of [Formula Presented] and [Formula Presented] In the [Formula Presented] channel, little oscillatory structures are observed in the m-substate angular distributions so that the resonance spins cannot be extracted.

AB - The intermediate structures in [Formula Presented] inelastic scattering were investigated at energies around [Formula Presented] in the [Formula Presented] single excitation and the [Formula Presented] mutual excitation channels and at [Formula Presented] in the [Formula Presented] single excitation channel. The angular distributions of the magnetic substate cross sections for the [Formula Presented] (4.439 MeV) state of [Formula Presented] were measured by using the γ-ray recoil method in the center-of-mass ejectile-axis frame. It is shown that the structures at [Formula Presented] and 31.8 MeV in the [Formula Presented] channel are interpreted as resonances of [Formula Presented] or [Formula Presented] which decay dominantly through the aligned configurations with [Formula Presented] On the other hand, the structure at [Formula Presented] is accounted for by assuming the overlap of two resonances having spins and parities of [Formula Presented] and [Formula Presented] In the [Formula Presented] channel, little oscillatory structures are observed in the m-substate angular distributions so that the resonance spins cannot be extracted.

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Intermediate structures in [Formula Presented] studied with the γ-ray recoil method

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