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NSR database version of April 11, 2024.

Search: Author = M.Takaki

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2024IM02      Phys.Lett. B 850, 138470 (2024)

N.Imai, M.Dozono, S.Michimasa, T.Sumikama, S.Ota, S.Hayakawa, J.W.Hwang, K.Iribe, C.Iwamoto, S.Kawase, K.Kawata, N.Kitamura, S.Masuoka, K.Nakano, P.Schrock, D.Suzuki, R.Tsunoda, K.Wimmer, D.S.Ahn, O.Beliuskina, N.Chiga, N.Fukuda, E.Ideguchi, K.Kusaka, H.Miki, H.Miyatake, D.Nagae, S.Ohmika, M.Ohtake, H.J.Ong, H.Otsu, H.Sakurai, H.Shimizu, Y.Shimizu, X.Sun, H.Suzuki, M.Takaki, H.Takeda, S.Takeuchi, T.Teranishi, Y.Watanabe, Y.X.Watanabe, K.Yako, H.Yamada, H.Yamaguchi, L.Yang, R.Yanagihara, Y.Yanagisawa, K.Yoshida, S.Shimoura

Neutron capture reaction cross-section of ⁷⁹Se through the ⁷⁹Se(d, p) reaction in inverse kinematics

NUCLEAR REACTIONS ²H(⁷⁷Se, p), (⁷⁹Se, p), E=20 MeV/nucleon; measured reaction products, Eγ, Iγ. ^78,80Se; deduced γ-ray energies, γ-emission probabilities, σ, isomer ratio. Comparison with available data, TALYS and code DWUCK5 calculations. The surrogate-ratio method, the RI Beam Factory operated by the RIKEN Nishina Center and the Center for Nuclear Studies (CNS), University of Tokyo, by employing the novel "optimized energy degrading optics" (OEDO) for radioactive isotope (RI) beams.

doi: 10.1016/j.physletb.2024.138470
Citations: PlumX Metrics

2021GO09      Phys.Rev. C 103, 034327 (2021)

S.Go, E.Ideguchi, R.Yokoyama, N.Aoi, F.Azaiez, K.Furutaka, Y.Hatsukawa, A.Kimura, K.Kisamori, M.Kobayashi, F.Kitatani, M.Koizumi, H.Harada, I.Matea, S.Michimasa, H.Miya, S.Nakamura, M.Niikura, H.Nishibata, N.Shimizu, S.Shimoura, T.Shizuma, M.Sugawara, D.Suzuki, M.Takaki, Y.Toh, Y.Utsuno, D.Verney, A.Yagi

High-spin states in ³⁵S

NUCLEAR REACTIONS ²⁶Mg(¹⁸O, n2α)³⁵S, E=80 MeV; measured Eγ, Iγ, γγ-coin, (particle)γγ-coin, γγ(θ)(ADO) using GEMINI-II array with the BGO Compton suppressors at JAEA tandem accelerator facility, and ORGAM array with BGO anti-Compton suppressors at ALTO-Tandem facility. ³⁵S; deduced high-spin levels, J, π, multipolarities; calculated levels, J, π, B(M1), B(E2) using large-scale shell-model calculations with SDPF-MSD4 interaction, and compared with experimental data.

doi: 10.1103/PhysRevC.103.034327
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Data from this article have been entered in the XUNDL database. For more information, click here.

2020MI13      Phys.Rev.Lett. 125, 122501 (2020)

S.Michimasa, M.Kobayashi, Y.Kiyokawa, S.Ota, R.Yokoyama, D.Nishimura, D.S.Ahn, H.Baba, G.P.A.Berg, M.Dozono, N.Fukuda, T.Furuno, E.Ideguchi, N.Inabe, T.Kawabata, S.Kawase, K.Kisamori, K.Kobayashi, T.Kubo, Y.Kubota, C.S.Lee, M.Matsushita, H.Miya, A.Mizukami, H.Nagakura, H.Oikawa, H.Sakai, Y.Shimizu, A.Stolz, H.Suzuki, M.Takaki, H.Takeda, S.Takeuchi, H.Tokieda, T.Uesaka, K.Yako, Y.Yamaguchi, Y.Yanagisawa, K.Yoshida, S.Shimoura

Mapping of a New Deformation Region around ⁶²Ti

ATOMIC MASSES ^61,62,63,64V, ^{58,59,60,61,62}Ti, ^{55,56,57,58,59,60}Sc; measured time of flight, charge, magnetic rigidity; deduced mass excesses. Comparison with AME2016 and available data.

RADIOACTIVITY ^59,61Ti, ^56,58Sc(IT) [from ⁹Be(⁷⁰Zn, X), E=345 MeV/nucleon]; measured decay products, Eγ, Iγ; deduced γ-ray energies and intensities, T_1/2. Comparison with available data.

doi: 10.1103/PhysRevLett.125.122501
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Data from this article have been entered in the XUNDL database. For more information, click here.

2020TA11      Phys.Rev.Lett. 124, 212502 (2020)

T.L.Tang, T.Uesaka, S.Kawase, D.Beaumel, M.Dozono, T.Fujii, N.Fukuda, T.Fukunaga, A.Galindo-Uribarri, S.H.Hwang, N.Inabe, D.Kameda, T.Kawahara, W.Kim, K.Kisamori, M.Kobayashi, T.Kubo, Y.Kubota, K.Kusaka, C.S.Lee, Y.Maeda, H.Matsubara, S.Michimasa, H.Miya, T.Noro, A.Obertelli, K.Ogata, S.Ota, E.Padilla-Rodal, S.Sakaguchi, H.Sakai, M.Sasano, S.Shimoura, S.S.Stepanyan, H.Suzuki, M.Takaki, H.Takeda, H.Tokieda, T.Wakasa, T.Wakui, K.Yako, Y.Yanagisawa, J.Yasuda, R.Yokoyama, K.Yoshida, K.Yoshida, J.Zenihiro

How Different is the Core of ²⁵F from ²⁴O_g.s.?

NUCLEAR REACTIONS C, ¹H(²³F, 2p), (²⁵F, 2p), E=277 MeV/nucleon; measured reaction products. ^{20,21,22,23,24}O; deduced integrated σ, J, π, level energies, spectroscopic factors.

doi: 10.1103/PhysRevLett.124.212502
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2671. Data from this article have been entered in the XUNDL database. For more information, click here.

2018CH27      Prog.Theor.Exp.Phys. 2018, 053D01 (2018)

S.Chebotaryov, S.Sakaguchi, T.Uesaka, T.Akieda, Y.Ando, M.Assie, D.Beaumel, N.Chiga, M.Dozono, A.Galindo-Uribarri, B.Heffron, A.Hirayama, T.Isobe, K.Kaki, S.Kawase, W.Kim, T.Kobayashi, H.Kon, Y.Kondo, Y.Kubota, S.Leblond, H.Lee, T.Lokotko, Y.Maeda, Y.Matsuda, K.Miki, E.Milman, T.Motobayashi, T.Mukai, S.Nakai, T.Nakamura, A.Ni, T.Noro, S.Ota, H.Otsu, T.Ozaki, V.Panin, S.Park, A.Saito, H.Sakai, M.Sasano, H.Sato, K.Sekiguchi, Y.Shimizu, I.Stefan, L.Stuhl, M.Takaki, K.Taniue, K.Tateishi, S.Terashima, Y.Togano, T.Tomai, Y.Wada, T.Wakasa, T.Wakui, A.Watanabe, H.Yamada, Zh.Yang, M.Yasuda, J.Yasuda, K.Yoneda, J.Zenihiro

Proton elastic scattering at 200 A MeV and high momentum transfers of 1.7-2.7 fm^-1 as a probe of the nuclear matter density of 6He

NUCLEAR REACTIONS ¹H(⁶He, ⁶He), E=200 MeV/nucleon; measured reaction products; deduced σ(θ). Comparison with available data, relativistic impulse approximation model predictions.

doi: 10.1093/ptep/pty048
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2018MI08      Phys.Rev.Lett. 121, 022506 (2018)

S.Michimasa, M.Kobayashi, Y.Kiyokawa, S.Ota, D.S.Ahn, H.Baba, G.P.A.Berg, M.Dozono, N.Fukuda, T.Furuno, E.Ideguchi, N.Inabe, T.Kawabata, S.Kawase, K.Kisamori, K.Kobayashi, T.Kubo, Y.Kubota, C.S.Lee, M.Matsushita, H.Miya, A.Mizukami, H.Nagakura, D.Nishimura, H.Oikawa, H.Sakai, Y.Shimizu, A.Stolz, H.Suzuki, M.Takaki, H.Takeda, S.Takeuchi, H.Tokieda, T.Uesaka, K.Yako, Y.Yamaguchi, Y.Yanagisawa, R.Yokoyama, K.Yoshida, S.Shimoura

Magic Nature of Neutrons in Ca54 : First Mass Measurements of ^55-57Ca

ATOMIC MASSES ^55,56,57Ca, ⁴⁸Ar, ^44,46Cl, ^40,42P, ⁴⁰Si; measured charge, TOF, magnetic rigidity, and flight path length between the timing detectors; deduced m/q spectrum of reference masses, mass excesses. Comparison with AME2016 evaluation.

doi: 10.1103/PhysRevLett.121.022506
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2018NO05      Phys.Rev.Lett. 120, 172501 (2018)

S.Noji, H.Sakai, N.Aoi, H.Baba, G.P.A.Berg, P.Doornenbal, M.Dozono, N.Fukuda, N.Inabe, D.Kameda, T.Kawabata, S.Kawase, Y.Kikuchi, K.Kisamori, T.Kubo, Y.Maeda, H.Matsubara, S.Michimasa, K.Miki, H.Miya, H.Miyasako, S.Sakaguchi, Y.Sasamoto, S.Shimoura, M.Takaki, H.Takeda, S.Takeuchi, H.Tokieda, T.Ohnishi, S.Ota, T.Uesaka, H.Wang, K.Yako, Y.Yanagisawa, N.Yokota, K.Yoshida, R.G.T.Zegers

Excitation of the Isovector Spin Monopole Resonance via the Exothermic ⁹⁰Zr(¹²N, ¹²C) Reaction at 175 MeV/υ

NUCLEAR REACTIONS ⁹⁰Zr(¹²N, ¹²C), E=175 MeV/nucleon; measured reaction products, Eγ, Iγ. ⁹⁰Zr; deduced σ(θ, E), Gamow-Teller and isobaric analog transitions, isovector spin giant monopole resonance (IVSMR).

doi: 10.1103/PhysRevLett.120.172501
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2585.

2018YA18      Phys.Rev.Lett. 121, 132501 (2018)

J.Yasuda, M.Sasano, R.G.T.Zegers, H.Baba, D.Bazin, W.Chao, M.Dozono, N.Fukuda, N.Inabe, T.Isobe, G.Jhang, D.Kameda, M.Kaneko, K.Kisamori, M.Kobayashi, N.Kobayashi, T.Kobayashi, S.Koyama, Y.Kondo, A.J.Krasznahorkay, T.Kubo, Y.Kubota, M.Kurata-Nishimura, C.S.Lee, J.W.Lee, Y.Matsuda, E.Milman, S.Michimasa, T.Motobayashi, D.Muecher, T.Murakami, T.Nakamura, N.Nakatsuka, S.Ota, H.Otsu, V.Panin, W.Powell, S.Reichert, S.Sakaguchi, H.Sakai, M.Sako, H.Sato, Y.Shimizu, M.Shikata, S.Shimoura, L.Stuhl, T.Sumikama, H.Suzuki, S.Tangwancharoen, M.Takaki, H.Takeda, T.Tako, Y.Togano, H.Tokieda, J.Tsubota, T.Uesaka, T.Wakasa, K.Yako, K.Yoneda, J.Zenihiro

Extraction of the Landau-Migdal Parameter from the Gamow-Teller Giant Resonance in ¹³²Sn

NUCLEAR REACTIONS ¹H(¹³²Sn, n), E=216 MeV/nucleon; measured reaction products, En, In; deduced σ(θ, E), B(GT), parameters. Comparison with available data.

doi: 10.1103/PhysRevLett.121.132501
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2625.

2016EN04      Phys.Rev. C 93, 064312 (2016)

J.P.Entwisle, B.P.Kay, A.Tamii, S.Adachi, N.Aoi, J.A.Clark, S.J.Freeman, H.Fujita, Y.Fujita, T.Furuno, T.Hashimoto, C.R.Hoffman, E.Ideguchi, T.Ito, C.Iwamoto, T.Kawabata, B.Liu, M.Miura, H.J.Ong, J.P.Schiffer, D.K.Sharp, G.Susoy, T.Suzuki, S.V.Szwec, M.Takaki, M.Tsumura, T.Yamamoto

Change of nuclear configurations in the neutrinoless double-β decay of ¹³⁰Te → ¹³⁰Xe and ¹³⁶Xe → ¹³⁶Ba

NUCLEAR REACTIONS ^128,130Te, ^{130,132,134,136}Xe, ^136,138Ba(d, ³He), E=101 MeV; measured Ed, Id, σ(θ) using Grand Raiden (GR) spectrometer at RCNP-Osaka cyclotron facility. ^127,129Sb, ^{129,131,133,135}I, ^135,137Cs; deduced levels, L-transfers, spectroscopic factors. DWBA and optical model analysis. ^128,130Te, ^{130,132,134,136}Xe, ^136,138Ba; deduced ground state proton occupancies. Comparison with shell-model and interacting boson-model calculations.

RADIOACTIVITY ¹³⁰Te, ¹³⁶Xe(2β^-); deduced change in the configuration of valence protons between the initial and final states in the 0νββ decay mode from measurements of the cross sections in (d, ³He) reaction, nuclear matrix elements.

doi: 10.1103/PhysRevC.93.064312
Citations: PlumX Metrics
Data from this article have been entered in the XUNDL database. For more information, click here.

2016KI01      Phys.Rev.Lett. 116, 052501 (2016)

K.Kisamori, S.Shimoura, H.Miya, S.Michimasa, S.Ota, M.Assie, H.Baba, T.Baba, D.Beaumel, M.Dozono, T.Fujii, N.Fukuda, S.Go, F.Hammache, E.Ideguchi, N.Inabe, M.Itoh, D.Kameda, S.Kawase, T.Kawabata, M.Kobayashi, Y.Kondo, T.Kubo, Y.Kubota, M.Kurata-Nishimura, C.S.Lee, Y.Maeda, H.Matsubara, K.Miki, T.Nishi, S.Noji, S.Sakaguchi, H.Sakai, Y.Sasamoto, M.Sasano, H.Sato, Y.Shimizu, A.Stolz, H.Suzuki, M.Takaki, H.Takeda, S.Takeuchi, A.Tamii, L.Tang, H.Tokieda, M.Tsumura, T.Uesaka, K.Yako, Y.Yanagisawa, R.Yokoyama, K.Yoshida

Candidate Resonant Tetraneutron State Populated by the ⁴He(⁸He, ⁸Be) Reaction

NUCLEAR REACTIONS ⁴He(⁸He, ⁸Be), E=186 MeV/nucleon; measured missing-mass spectrum; deduced the tetraneutron system energy of the state with uncertainties, Q-value.

doi: 10.1103/PhysRevLett.116.052501
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2500. Data from this article have been entered in the XUNDL database. For more information, click here.

2012UE04      Prog.Theor.Phys.(Kyoto), Suppl. 196, 150 (2012)

T.Uesaka, H.Matsubara, K.Miki, S.Noji, H.Sakai, Y.Sasamoto, S.Shimoura, M.Takaki, K.Yako, for the SHARAQ Collaboration

New Experimental Studies of Nuclear Spin-Isospin Responses

NUCLEAR REACTIONS ¹²C(¹⁸O, ¹⁸Ne)¹²Be, E=80 MeV/nucleon; ²⁰⁸Pb(t, ³He)²⁰⁸Tl, E=300 MeV/nucleon; ⁷Li, ⁹⁰Zr(¹⁰C, ¹⁰B), E=200 MeV/nucleon; ⁹⁰Zr(¹²N, ¹²C), E=200 MeV/nucleon; measured reaction products, Eγ, Iγ; deduced σ(θ, E), level structure, J, π, spin-isospin responses.

doi: 10.1143/PTPS.196.150
Citations: PlumX Metrics

2011WA17      Phys.Rev. C 84, 014614 (2011)

T.Wakasa, M.Okamoto, M.Takaki, M.Dozono, K.Hatanaka, M.Ichimura, T.Noro, H.Okamura, Y.Sakemi

Complete set of polarization transfer observables for the ¹⁶O( p, n)¹⁶F reaction at 296 MeV and 0 degrees

NUCLEAR REACTIONS ¹⁶O(polarized p, n)¹⁶F, E=296 MeV; measured E(n), I(n), polarized neutrons, TOF, cross section spectrum, analyzing powers, polarized σ. Comparison with DWIA calculations. ¹⁶F; deduced levels, J, π, Gamow-Teller and spin-dipole states.

doi: 10.1103/PhysRevC.84.014614
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2352. Data from this article have been entered in the XUNDL database. For more information, click here.