Probing isoscalar giant resonances with multipolarity <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>L</mml:mi><mml:mo>≤</mml:mo><mml:mn>3</mml:mn></mml:mrow></mml:math> in even-<mml:math xmlns:mml="http://www.w3.org/1998/

Background-free inelastic-scattering spectra were measured for even-$A$ neodymium (Nd) isotopes using a halo-free 386-MeV $\ensuremath{\alpha}$ beam at forward angles, including ${0}^{\ensuremath{\circ}}$, to examine the influence of deformation on isoscalar giant resonances. The strength distributions of isoscalar giant resonances (with multipolarity $L\ensuremath{\le}3$) in $^{142}\mathrm{Nd}$ and $^{146\ensuremath{-}150}\mathrm{Nd}$ isotopes are determined using multipole decomposition analysis. This analysis is based on angular distributions calculated within the framework of the distorted-wave Born approximation with transition densities generated with a Woods-Saxon type potential. The isoscalar giant monopole resonance exhibits a distinct splitting into low-energy and high-energy components while going from the spherical nucleus $^{142}\mathrm{Nd}$ to the well-deformed nucleus $^{150}\mathrm{Nd}$ due to coupling with the $K=0$ component of the isoscalar giant quadrupole resonance (ISGQR). The isoscalar giant dipole resonance displays a bimodal structure, with an evidence of coupling between the dipole ($E1$) and high-energy octupole ($E3$) resonance due to deformation effects. The ISGQR splits into distinct $K$ components ($K=0$, 1, and 2) due to deformation. A signature of an overtone mode in ISGQR at an energy around 26 MeV has been obtained.

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Journal
Physical review. C
Published
2025-10-21
DOI
https://doi.org/10.1103/1p1h-5jh2
Citations
1
Primary Topic
Nuclear physics research studies
Type
article
Field-Weighted Citation Impact
1.87
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article

Probing isoscalar giant resonances with multipolarity <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>L</mml:mi><mml:mo>≤</mml:mo><mml:mn>3</mml:mn></mml:mrow></mml:math> in even-<mml:math xmlns:mml="http://www.w3.org/1998/

H. Akimune, S. Pal, S. Ota, Sierra Lisa Weyhmiller et al.
1 citations
Physical review. C
Nuclear physics research studies
1.87
article

Probing isoscalar giant resonances with multipolarity <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mrow><mml:mi>L</mml:mi><mml:mo>≤</mml:mo><mml:mn>3</mml:mn></mml:mrow></mml:math> in even-<mml:math xmlns:mml="http://www.w3.org/1998/

H. Akimune, S. Pal, S. Ota, Sierra Lisa Weyhmiller, Y.K. Gupta, J. C. Zamora, Z. Yang, T. Furuno, S. Bagchi, M.N. Harakeh, Mitsuru Itoh, Kazuya Kitamura, Soma Kawashima, T. Kawabata, Kevin Howard, L. M. Donaldson, Kyoko Nosaka, K. Inaba, U. Garg, Y. Fujikawa, Ramkrishna Pramanik, K. Khokhar, Takanobu Doi, N. Kalantar‐Nayestanaki, Y. Matsuda, Y. Hijikata, Mamoru Fujiwara, Debarati Das, Soshi Okamoto, S. Roy, S. Ishida, A. Nakagawa, S. Nakamura, Nobuyoshi Kobayashi, M. Abdullah, D. Kar
article en
1 citations

Abstract

Background-free inelastic-scattering spectra were measured for even-$A$ neodymium (Nd) isotopes using a halo-free 386-MeV $\ensuremath{\alpha}$ beam at forward angles, including ${0}^{\ensuremath{\circ}}$, to examine the influence of deformation on isoscalar giant resonances. The strength distributions of isoscalar giant resonances (with multipolarity $L\ensuremath{\le}3$) in $^{142}\mathrm{Nd}$ and $^{146\ensuremath{-}150}\mathrm{Nd}$ isotopes are determined using multipole decomposition analysis. This analysis is based on angular distributions calculated within the framework of the distorted-wave Born approximation with transition densities generated with a Woods-Saxon type potential. The isoscalar giant monopole resonance exhibits a distinct splitting into low-energy and high-energy components while going from the spherical nucleus $^{142}\mathrm{Nd}$ to the well-deformed nucleus $^{150}\mathrm{Nd}$ due to coupling with the $K=0$ component of the isoscalar giant quadrupole resonance (ISGQR). The isoscalar giant dipole resonance displays a bimodal structure, with an evidence of coupling between the dipole ($E1$) and high-energy octupole ($E3$) resonance due to deformation effects. The ISGQR splits into distinct $K$ components ($K=0$, 1, and 2) due to deformation. A signature of an overtone mode in ISGQR at an energy around 26 MeV has been obtained.

Physical review. CVol. 112(4)
University of Notre Dame (US), University of Fukui (JP), Bhabha Atomic Research Centre (IN), Konan University (JP), University of Groningen (NL), Indian Institute of Technology Dhanbad (IN), Homi Bhabha National Institute (IN), Tohoku University (JP), Kyoto University (JP), iThemba Laboratory (ZA), Michigan State University (US), The University of Osaka (JP)
Openalex Percentile: Top 11%
Nuclear physics research studies
1.87
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