### 抄録

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.

元の言語 | 英語 |
---|---|

ページ数 | 1 |

ジャーナル | Physical Review C - Nuclear Physics |

巻 | 66 |

発行部数 | 2 |

DOI | |

出版物ステータス | 出版済み - 1 1 2002 |

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### All Science Journal Classification (ASJC) codes

- Nuclear and High Energy Physics

### これを引用

*Physical Review C - Nuclear Physics*,

*66*(2). https://doi.org/10.1103/PhysRevC.66.024609

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

研究成果: ジャーナルへの寄稿 › 記事

*Physical Review C - Nuclear Physics*, 巻. 66, 番号 2. https://doi.org/10.1103/PhysRevC.66.024609

}

TY - JOUR

T1 - Intermediate structures in [Formula Presented] studied with the γ-ray recoil method

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 - 2002/1/1

Y1 - 2002/1/1

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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U2 - 10.1103/PhysRevC.66.024609

DO - 10.1103/PhysRevC.66.024609

M3 - Article

AN - SCOPUS:85035261230

VL - 66

JO - Physical Review C - Nuclear Physics

JF - Physical Review C - Nuclear Physics

SN - 0556-2813

IS - 2

ER -