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U and
ThFilipescu, D.*; Gheorghe, I.*; Goriely, S.*; Nishio, Katsuhisa; Utsunomiya, Hiroaki*; Suzaki, Fumi; Hirose, Kentaro; 10 of others*
Physical Review C, 109(4), p.044602_1 - 044602_23, 2024/04
Times Cited Count:4 Percentile:67.20(Physics, Nuclear)
CUtsunomiya, Hiroaki*; Goriely, S.*; Kimura, Masaaki*; Shimizu, Noritaka*; Utsuno, Yutaka; Tveten, G. M.*; Renstr
m, T.*; Ariizumi, Takashi*; Miyamoto, Shuji*
Physical Review C, 109(1), p.014617_1 - 014617_7, 2024/01
Times Cited Count:3 Percentile:54.52(Physics, Nuclear)no abstracts in English

Tamii, Atsushi*; Pellegri, L.*; S
derstr
m, P.-A.*; Allard, D.*; Goriely, S.*; Inakura, Tsunenori*; Khan, E.*; Kido, Eiji*; Kimura, Masaaki*; Litvinova, E.*; et al.
European Physical Journal A, 59(9), p.208_1 - 208_21, 2023/09
Times Cited Count:15 Percentile:90.47(Physics, Nuclear)no abstracts in English
Kawano, Toshihiko*; Cho, Y. S.*; Dimitriou, P.*; Filipescu, D.*; Iwamoto, Nobuyuki; Plujko, V.*; Tao, X.*; Utsunomiya, Hiroaki*; Varlamov, V.*; Xu, R.*; et al.
Nuclear Data Sheets, 163, p.109 - 162, 2020/01
Times Cited Count:149 Percentile:99.72(Physics, Nuclear)Goriely, S.*; Dimitriou, P.*; Wiedeking, M.*; Belgya, T.*; Firestone, R.*; Kopecky, J.*; Krti
ka, M.*; Plujko, V.*; Schwengner, R.*; Siem, S.*; et al.
European Physical Journal A, 55(10), p.172_1 - 172_52, 2019/10
Times Cited Count:127 Percentile:94.79(Physics, Nuclear)Dimitriou, P.*; Belgya, T.*; Cho, Y.-S.*; Filipescu, D.*; Firestone, R.*; Goriely, S.*; Iwamoto, Nobuyuki; Kawano, Toshihiko*; Kopecky, J.*; Krticka, M.*; et al.
EPJ Web of Conferences, 178, p.06005_1 - 06005_3, 2018/05
Times Cited Count:2 Percentile:70.58(Optics)no abstracts in English
PbKondo, Takeo*; Utsunomiya, Hiroaki*; Goriely, S.*; Iwamoto, Chihiro*; Akimune, Hidetoshi*; Yamagata, Tamio*; Toyokawa, Hiroyuki*; Harada, Hideo; Kitatani, Fumito; Lui, Y.-W.*; et al.
Nuclear Data Sheets, 119, p.310 - 313, 2014/05
Times Cited Count:2 Percentile:17.58(Physics, Nuclear)
,n) and (n,
)reactionsUtsunomiya, Hiroaki*; Goriely, S.*; Kondo, Takeo*; Iwamoto, Chihiro*; Akimune, Hidetoshi*; Yamagata, Tamio*; Toyokawa, Hiroyuki*; Harada, Hideo; Kitatani, Fumito; Lui, Y.-W.*; et al.
Physical Review C, 88(1), p.015805_1 - 015805_6, 2013/07
Times Cited Count:90 Percentile:96.79(Physics, Nuclear)
-ray strength function method; A Way from photoneutron emission to radiative neutron captureUtsunomiya, Hiroaki*; Akimune, Hidetoshi*; Yamagata, Tamio*; Iwamoto, Chihiro*; Goriely, S.*; Daoutidis, I.*; Toyokawa, Hiroyuki*; Harada, Hideo; Kitatani, Fumito; Iwamoto, Nobuyuki; et al.
Proceedings of 14th International Symposium on Capture
-Ray Spectroscopy and Related Topics, p.505 - 514, 2013/05
Kondo, Takeo*; Utsunomiya, Hiroaki*; Goriely, S.*; Daoutidis, I.*; Iwamoto, Chihiro*; Akimune, Hidetoshi*; Okamoto, Akiyuki*; Yamagata, Tamio*; Kamata, Masaki*; Ito, Osamu*; et al.
Physical Review C, 86(1), p.014316_1 - 014316_7, 2012/07
Times Cited Count:47 Percentile:88.41(Physics, Nuclear)Using quasi-monochromatic laser-Compton scattering
rays, total photoneutron cross sections were measured for
Pb near neutron threshold with a high-efficiency 4
neutron detector. Partial
1 and
1 photoneutron cross sections along with total cross sections were determined for
Pb at four energies near threshold by measuring anisotropies in photoneutron emission with linearly-polarized
rays. The
1 strength dominates over the
1 strength in the neutron channel where
1 photoneutron cross sections show extra strength of the pygmy dipole resonance in
Pb near the neutron threshold corresponding to 0.32-0.42% of the Thomas-Reiche-Kuhn sum rule. Several 
units of B(
1)
strength were observed in
Pb just above neutron threshold, which correspond to an
1 cross section less than 10% of the total photoneutron cross section.
Sn and the
-ray strength function methodUtsunomiya, Hiroaki*; Goriely, S.*; Kamata, Masaki*; Akimune, Hidetoshi*; Kondo, Takeo*; Ito, Osamu*; Iwamoto, Chihiro*; Yamagata, Tamio*; Toyokawa, Hiroyuki*; Lui, Y.-W.*; et al.
Physical Review C, 84(5), p.055805_1 - 055805_6, 2011/11
Times Cited Count:47 Percentile:89.61(Physics, Nuclear)Photoneutron cross sections were measured for
Sn,
Sn,
Sn,
Sn, and
Sn near neutron threshold with quasi-monochromatic laser-Compton scattering
-rays. A systematic analysis of the present photoneutron data and existing neutron-capture data is made using the
-ray strength function on the basis of the HFB+QRPA model of E1 strength supplemented with a pygmy dipole resonance, which was deduced from a previous study on
Sn and
Sn. Radiative neutron capture cross sections for two radioactive nuclei,
Sn and
Sn, are deduced through the
-ray strength function method.
SF methodUtsunomiya, Hiroaki*; Goriely, S.*; Akimune, Hidetoshi*; Yamagata, Tamio*; Kondo, Takeo*; Iwamoto, Chihiro*; Okamoto, Akiyuki*; Harada, Hideo; Kitatani, Fumito; Goko, Shinji*; et al.
AIP Conference Proceedings 1377, p.255 - 259, 2011/10
Times Cited Count:0 Percentile:0.00(Astronomy & Astrophysics)
SF method to palladiumUtsunomiya, Hiroaki*; Goriely, S.*; Arteaga, D. P.*; Daoutidis, I.*; Akimune, Hidetoshi*; Yamagata, Tamio*; Kondo, Takeo*; Iwamoto, Chihiro*; Kamata, Masaki*; Ito, Osamu*; et al.
AIP Conference Proceedings 1377, p.450 - 452, 2011/10
Times Cited Count:0 Percentile:0.00(Astronomy & Astrophysics)
SF method; Determination of radiative neutron-capture cross section for unstable nucleiUtsunomiya, Hiroaki*; Goriely, S.*; Akimune, Hidetoshi*; Harada, Hideo; Kitatani, Fumito; Goko, Shinji*; Toyokawa, Hiroyuki*; Yamada, Kawakatsu*; Lui, Y.-W.*
Journal of the Korean Physical Society, 59(2), p.1713 - 1716, 2011/08
Times Cited Count:2 Percentile:19.22(Physics, Multidisciplinary)
-ray strength function method and its application to
PdUtsunomiya, Hiroaki*; Goriely, S.*; Akimune, Hidetoshi*; Harada, Hideo; Kitatani, Fumito; Goko, Shinji*; Toyokawa, Hiroyuki*; Yamada, Kawakatsu*; Kondo, Takeo*; Ito, Osamu*; et al.
Physical Review C, 82(6), p.064610_1 - 064610_5, 2010/12
Times Cited Count:45 Percentile:88.48(Physics, Nuclear)The
-ray strength function method (
SF method) is devised to indirectly determine radiative neutron capture cross sections for radioactive nuclei. This method is applied here to the
Pd case. Photoneutron cross sections were measured for
Pd near neutron threshold with quasi-monochromatic laser-Compton-scattering
-ray beams. These photoneutron cross sections as well as the reverse radiative neutron capture cross sections for
Pd are used to provide constraints on the
Pd(n,
)
Pd cross section.
Se as a probe of neutron capture for the s-process branch-point nucleus 
Makinaga, Ayano*; Hohara, Shinya*; Utsunomiya, Hiroaki*; Goko, Shinji*; Kaihori, Takeshi*; Akimune, Hidetoshi*; Yamagata, Tamio*; Goriely, S.*; Toyokawa, Hiroyuki*; Harano, Hideki*; et al.
Proceedings of Science (Internet), 28, p.239_1 - 239_4, 2010/12
no abstracts in English
Zr near thresholdUtsunomiya, Hiroaki*; Goriely, S.*; Akimune, Hidetoshi*; Yamagata, Tamio*; Kondo, Takeo*; Iwamoto, Chihiro*; Ito, Osamu*; Kamata, Masaki*; Io, Masanori*; Kususe, Koichi*; et al.
AIP Conference Proceedings 1377, p.447 - 449, 2010/10
Times Cited Count:0 Percentile:0.00(Astronomy & Astrophysics)
Zr; A Systematic experimental study of photoneutron and radiative neutron capture cross sections for zirconium isotopesUtsunomiya, Hiroaki*; Goriely, S.*; Akimune, Hidetoshi*; Harada, Hideo; Kitatani, Fumito; Goko, Shinji; Toyokawa, Hiroyuki*; Yamada, Kawakatsu*; Kondo, Takeo*; Ito, Osamu*; et al.
Physical Review C, 81(3), p.035801_1 - 035801_5, 2010/03
Times Cited Count:39 Percentile:86.95(Physics, Nuclear)This manuscript presents photoneutron cross sections for
Zr. Combining the present data with the previously published Zr data, we investigated the
-ray strength function for zirconium isotopes systematically. We present a unified picture of the
-ray strength function that consists of the HFB + QRPA model of E1 strength accompanied by an extra M1 strength attributable to giant M1 resonance. It is shown that the
-ray strength function reproduces both (g,n) and (n,g) cross sections for Zr isotopes consistently.
Se; Implications for the s-process branching at
SeMakinaga, Ayano*; Utsunomiya, Hiroaki*; Goriely, S.*; Kaihori, Takeshi*; Goko, Shinji*; Akimune, Hidetoshi*; Yamagata, Tamio*; Toyokawa, Hiroyuki*; Matsumoto, Tetsuro*; Harano, Hideki*; et al.
Physical Review C, 79(2), p.025801_1 - 025801_8, 2009/02
Times Cited Count:26 Percentile:79.22(Physics, Nuclear)Photoneutron cross sections were measured for
Se immediately above the neutron separation energy with quasimonochromatic
-ray beams to experimentally constrain the E1
strength function for
Se. Two sets of the
strength function and the level density that equally meet the experimental constraint predict largely different neutron capture cross sections for
Se. Based on the Maxwell-averaged cross sections of the latest compilation complemented with the predicted cross sections for
Se, we calculated
N values of the main s-process component using a phenomenological model and deduced empirical abundances of the weak s-process component.
Se; Implications for the s-process thermometerMakinaga, Ayano*; Utsunomiya, Hiroaki*; Kaihori, Takeshi*; Yamagata, Tamio*; Akimune, Hidetoshi*; Goriely, S.*; Toyokawa, Hiroyuki*; Matsumoto, Tetsuro*; Harano, Hideki*; Harada, Hideo; et al.
Nuclear Physics A, 805(1-4), p.564 - 566, 2008/06
Photoneutron cross sections were measured for
Se near the neutron threshold energy with quasi-monochromatic
rays. Using the
Se(
,
) cross section as experimental constraints on the E1
strength function, we estimate the neutron capture rates for
Se. The solar abundance ratio of s-only nuclides
Kr and
Kr are analyzed in terms of the s-process branching at
Se within the local approximation. The corresponding temperature and neutron density regimes are discussed in the light of the s-process scenario in massive stars.