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NSR database version of April 11, 2024.

Search: Author = S.Fukuda

Found 49 matches.

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2022FU05      Few-Body Systems 63, 37 (2022)

M.Fukutome, M.Fukuda, M.Tanaka, D.Nishimura, M.Takechi, T.Ohtsubo, M.Mihara, K.Matsuta, T.Suzuki, T.Yamaguchi, T.Izumikawa, S.Sato, S.Fukuda, A.Kitagawa, H.Takahashi, Y.Kimura, S.Sugawara, K.Takatsu, G.Takayama

One-Neutron Removal Cross Sections for 16N Isomeric State

NUCLEAR REACTIONS 9Be(18O, X)16N, E=160 MeV/nucleon; 9Be(15N, X)16N, E=169 MeV/nucleon; measured reaction products; deduced one-neutron σ with different isomeric ratios. Comparison with theoretical calculations. The HIMAC synchrotron accelerator facility of the National Institute of Radiological Sciences.

doi: 10.1007/s00601-021-01721-1
Citations: PlumX Metrics


2017DU04      Acta Phys.Pol. B48, 473 (2017)

H.Du, M.Fukuda, D.Nishimura, M.Takechi, T.Suzuki, Y.Tanaka, I.Kato, M.Tanaka, K.Abe, T.Izumikawa, H.Oikawa, T.Ohtsubo, J.Ohno, Y.Kanke, H.Kikuchi, A.Kitagawa, S.Sato, U.Sayama, J.Shimaya, S.Suzuki, Y.Takeuchi, T.Takemoto, N.Tadano, R.Tamura, J.Nagumo, K.Nishizuka, S.Fukuda, K.Hori, S.Matsunaga, A.Mizukami, M.Mihara, E.Miyata, D.Murooka, S.Yamaoka, T.Yamaguchi

Nuclear Structure of 15, 16C via Reaction Cross-section Measurements

NUCLEAR REACTIONS 1H, 9Be, 12C, 27Al(15C, x), (16C, x), E=40-140 MeV/nucleon; measured outgoing particles using ΔE-E counter telescope; deduced reaction σ, mass and charge density of 14,15,16C vs radius, mass and charge radii using the data supplemented by published data at different eneegies. Compared with data on radii (both experimental and calculations) from other groups.

doi: 10.5506/APhysPolB.48.473
Citations: PlumX Metrics


2017MI04      Acta Phys.Pol. B48, 409 (2017)

E.Miyata, M.Takechi, T.Ohtsubo, M.Fukuda, D.Nishimura, K.Abe, K.Aoki, A.Ikeda, T.Izumikawa, H.Oikawa, K.Ohnishi, S.Ohmika, I.Kato, Y.Kanke, N.Kanda, R.Kanbe, H.Kikuchi, A.Kitagawa, S.Sato, H.Shimamura, J.Shimaya, S.Suzuki, T.Suzuki, R.Takagaki, H.Takahashi, Y.Takei, Y.Takeuchi, T.Takenouchi, N.Tadano, M.Tanaka, Y.Tanaka, K.Chikaato, H.Du, J.Nagumo, K.Nishizuka, T.Nishimura, S.Fukuda, M.Machida, A.Mizukami, M.Mihara, J.Muraoka, S.Yagi, S.Yamaoka, T.Yamaguchi, K.Yokoyama

Development of High Resolution TOF Detector for RI Beams Using Cherenkov Radiation

doi: 10.5506/APhysPolB.48.409
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2017TA06      Acta Phys.Pol. B48, 461 (2017)

M.Tanaka, M.Fukuda, D.Nishimura, M.Takechi, S.Suzuki, H.Du, Y.Tanaka, K.Aoki, S.Fukuda, A.Honma, T.Izumikawa, Y.Kamisho, N.Kanda, I.Kato, Y.Kanke, A.Kitagawa, J.Kohno, M.Machida, K.Matsuta, M.Mihara, E.Miyata, Y.Morita, J.Muraoka, D.Murooka, T.Nagai, M.Nagashima, K.Ohnishi, J.Ohno, T.Ohtsubo, H.Oikawa, S.Sato, H.Shimamura, T.Sugihara, T.Suzuki, N.Tadano, R.Takagaki, Y.Takei, A.Takenouchi, S.Yagi, T.Yamaguchi, S.Yamaki, S.Yamaoka

Reaction Cross Sections for 13-15B and One-neutron Halo in 14B

NUCLEAR REACTIONS 1H, 9Be, 12C, 27Al(13B, x), (14B, x), (15B, x), E=50-130 MeV/nucleon; measured reaction products; deduced reaction σ; calculated σ using Glauber-type approach; deduced nuclear matter density distribution, matter and charge radii for 13,15B and one-neutron halo 14B. Cross sections compared also with asymptotical σ at relativistic energy; nuclear radii with both calculations and data for B isotopes published in literature.

doi: 10.5506/APhysPolB.48.461
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2707.


2015FA03      Phys.Rev. C 91, 014614 (2015)

G.W.Fan, M.Fukuda, D.Nishimura, X.L.Cai, S.Fukuda, I.Hachiuma, C.Ichikawa, T.Izumikawa, M.Kanazawa, A.Kitagawa, T.Kuboki, M.Lantz, M.Mihara, M.Nagashima, K.Namihira, Y.Ohkuma, T.Ohtsubo, Z.z.Ren, S.Sato, Z.Q.Sheng, M.Sugiyama, S.Suzuki, T.Suzuki, M.Takechi, T.Yamaguchi, W.Xu

Density distribution of 8Li and 8B and capture reaction at low energy

NUCLEAR REACTIONS 9Be, 12C, 27Al(8Li, X), E=30-110 MeV, [8Li secondary beam produced in 9Be(13C, X), E=130 MeV/nucleon primary reaction]; measured reaction products, reaction σ(E) at HIMAC synchrotron and fragment-separator facility of NIRS, Japan; deduced density distributions of 8B and 8Li using modified Glauber model, halo structure of 8B. 7Li(n, γ)8Li, E=0.01 eV-1 MeV; 7Be(p, γ)8B, E=0-0.5 MeV; calculated capture σ(E) for (n, γ) and S(E) factor for (p, γ) reactions using density distributions determined in present work, comparison with experimental data.

doi: 10.1103/PhysRevC.91.014614
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2479.


2014FA18      Phys.Rev. C 90, 044321 (2014)

G.W.Fan, M.Fukuda, D.Nishimura, X.L.Cai, S.Fukuda, I.Hachiuma, C.Ichikawa, T.Izumikawa, M.Kanazawa, A.Kitagawa, T.Kuboki, M.Lantz, M.Mihara, M.Nagashima, K.Namihira, Y.Ohkuma, T.Ohtsubo, Z.Ren, S.Sato, Z.Q.Shen, M.Sugiyama, S.Suzuki, T.Suzuki, M.Takechi, T.Yamaguchi, B.J.Xu, W.Xu

Structure of 8Li from a reaction cross-section measurement

NUCLEAR REACTIONS 1H, 9Be, 12C, 27Al(8Li, 8Li'), E=30-110 MeV/nucleon, [secondary 8Li beam from 9Be(13C, X), E=130 MeV/nucleon primary reaction]; measured particle spectra by Bρ-ΔE-TOF technique, reaction σ(E) at HIMAC synchrotron and NIRS fragment-separator facility in Japan. 8Li; deduced density distribution, matter radius, tendency for 8Li as a skin nucleus. Modified Glauber model analysis of experimental data. Comparison with previous experimental results and with calculations based on harmonic oscillator (HO)+Yukawa and HO+single-particle model (SPM) functions.

doi: 10.1103/PhysRevC.90.044321
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2479. Data from this article have been entered in the XUNDL database. For more information, click here.


2010FU07      Nucl.Phys. A834, 461c (2010)

M.Fukuda, D.Nishimura, M.Takechi, M.Mihara, K.Matsuta, R.Matsumiya, T.Kuboki, K.Namihira, I.Hachiuma, T.Yamaguchi, T.Suzuki, Y.Okuma, M.Nagashima, T.Ohtsubo, Y.Shimbara, T.Izumikawa, K.Tanaka, T.Suda, S.Momota, T.Minamisono, W.Xu, G.W.Fan, S.Fukuda, S.Sato, M.Kanazawa, A.Kitagawa

Directional correlation of nuclear-collision probability for aligned beams of deformed nucleus

NUCLEAR REACTIONS C(10B, X), E not given; measured σ with aligned beam; deduced momentum distribution, relative reaction probability.

doi: 10.1016/j.nuclphysa.2010.01.064
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2010NI17      Nucl.Phys. A834, 470c (2010)

D.Nishimura, M.Fukuda, M.Takechi, M.Mihara, D.Ishikawa, J.Komurasaki, K.Matsuta, R.Matsumiya, T.Kuboki, M.Yoshitake, T.Suzuki, T.Yamaguchi, S.Nakajima, K.Saito, M.Miura, I.Hachiuma, K.Namihira, T.Ohtsubo, Y.Shimbara, R.Watanabe, Y.Ohkuma, T.Izumikawa, K.Tanaka, T.Suda, A.Ozawa, Y.Yasuda, T.Moriguchi, S.Momota, S.Fukuda, S.Sato, M.Kanazawa, A.Kitagawa

Distinction between Proton-Neutron Density Distribution of Halo Nuclei at the Nuclear Surface via Reaction Cross Sections

NUCLEAR REACTIONS 1H, C(8B, X), (11Be, X), E≈50-120 MeV/nucleon; measured total σ; calculated σ using Glauber theory assuming halo nuclei. Secondary radioactive beams. Transmission method.

doi: 10.1016/j.nuclphysa.2010.01.067
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2710.


2010YA11      Phys.Rev. C 82, 014609 (2010)

T.Yamaguchi, M.Fukuda, S.Fukuda, G.W.Fan, I.Hachiuma, M.Kanazawa, A.Kitagawa, T.Kuboki, M.Lantz, M.Mihara, M.Nagashima, K.Namihira, D.Nishimura, Y.Okuma, T.Ohtsubo, S.Sato, T.Suzuki, M.Takechi, W.Xu

Energy-dependent charge-changing cross sections and proton distribution of 28Si

NUCLEAR REACTIONS C(28Si, X), E=100-600 MeV/nucleon; measured particle spectra, σ(E); deduced energy dependence of charge-changing cross section. Comparison with Glauber-type calculation.

doi: 10.1103/PhysRevC.82.014609
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2283.


2002MI37      Z.Naturforsch. 57a, 595 (2002)

T.Minamisono, K.Matsuta, K.Minamisono, S.Kudo, M.Ogura, S.Fukuda, K.Sato, M.Mihara, M.Fukuda, S.Takeda, S.Y.Zhu

Quadrupole Moments of the 40Ca Core Plus One Nucleon Nuclei 41Sc and 41Ca

NUCLEAR MOMENTS 41Sc, 41Ca; measured NMR and NQR spectra; deduced quadrupole moments, electric field gradients in TiO2 crystals.


2001MI40      Hyperfine Interactions 136/137, 225 (2001)

T.Minamisono, K.Matsuta, K.Minamisono, S.Kudo, M.Ogura, S.Fukuda, K.Sato, M.Mihara, M.Fukuda

Precise Quadrupole Moment of the Doubly Closed Shell Plus One Proton Nucleus 41Sc

NUCLEAR MOMENTS 45Sc; measured Fourier-transformed pulse-NMR spectrum in TiO2 crystal. 41Sc; analyzed β-NQR data; deduced quadrupole moment. Comparison with model prediction.

doi: 10.1023/A:1020588417313
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1999FU08      Nucl.Phys. A656, 209 (1999)

M.Fukuda, M.Mihara, T.Fukao, S.Fukuda, M.Ishihara, S.Ito, T.Kobayashi, K.Matsuta, T.Minamisono, S.Momota, T.Nakamura, Y.Nojiri, Y.Ogawa, T.Ohtsubo, T.Onishi, A.Ozawa, T.Suzuki, M.Tanigaki, I.Tanihata, K.Yoshida

Density Distribution of 8B Studied via Reaction Cross Sections

NUCLEAR REACTIONS 9Be, 12C, 27Al(8B, X), (7Be, X), E≈ 35, 60 MeV/nucleon; 9Be, 12C, 27Al(6Li, X), E≈ 40 MeV/nucleon; measured interaction, reaction σ. 9Be, 12C, 27Al(8B, 7Be), E≈ 35, 60 MeV/nucleon; measured 1-proton removal σ. 8B deduced rms radius, halo features, density distributions. Glauber model analysis. Secondary beams from 12C fragmentation.

doi: 10.1016/S0375-9474(99)00308-5
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1903.


1999MA46      Phys.Lett. 459B, 81 (1999)

K.Matsuta, K.Sato, M.Fukuda, M.Mihara, T.Yamaguchi, M.Sasaki, T.Miyake, K.Minamisono, T.Minamisono, M.Tanigaki, T.Ohtsubo, T.Onishi, Y.Nojiri, S.Momota, S.Fukuda, K.Yoshida, A.Ozawa, T.Kobayashi, I.Tanihata, J.R.Alonso, G.F.Krebs, T.J.M.Symons, H.Kitagawa, H.Sagawa

Quadrupole Moment of the Proton Drip-Line Nuclide 13O

RADIOACTIVITY 13O(β+) [from Be(16O, X)]; measured β-NQR spectrum; deduced quadrupole moment. Comparison with shell model predictions.

doi: 10.1016/S0370-2693(99)00620-6
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1999MB13      Hyperfine Interactions 120/121, 673 (1999)

K.Matsuta, T.Onishi, M.Fukuda, T.Minamisono, H.Akai, M.Sasaki, T.Yamaguchi, T.Miyake, K.Sato, K.Minamisono, F.Ohsumi, Y.Muramoto, S.Oui, C.Ha, K.Tanaka, K.Kidera, A.Morishita, A.Kitagawa, M.Torikoshi, M.Kanazawa, T.Nishio, S.Koda, T.Ohtsubo, S.Fukuda, Y.Nojiri, S.Momota, A.Ozawa, K.Yoshida, T.Suzuki, T.Kobayashi, I.Tanihata, S.S.Hanna, J.R.Alonso, G.F.Krebs, T.J.M.Symons

Electromagnetic moments of short lived β emitters 21F, 23Mg, 27Si and 39Ca

NUCLEAR MOMENTS 21F, 23Mg, 27Si, 39Ca; measured asymmetry change as a function of the frequency; deduced magnetic moments, electrical quadrupole coupling constants. Comparison with OXBASH shell model calculations.

doi: 10.1023/A:1017036009679
Citations: PlumX Metrics


1999OG03      Phys.Lett. 451B, 11 (1999)

H.Ogawa, K.Asahi, K.Sakai, A.Yoshimi, M.Tsuda, Y.Uchiyama, T.Suzuki, K.Suzuki, N.Kurokawa, M.Adachi, H.Izumi, H.Ueno, T.Shimoda, S.Tanimoto, N.Takahashi, W.-D.Schmidt-Ott, M.Schafer, S.Fukuda, A.Yoshida, M.Notani, T.Kubo, H.Okuno, H.Sato, N.Aoi, K.Yoneda, H.Iwasaki, N.Fukuda, N.Fukunishi, M.Ishihara, H.Miyatake

Magnetic Moment and Electric Quadrupole Moment of the 18N Ground State

RADIOACTIVITY 18N(β-) [from 22Ne fragmentation]; measured β-NMR. 18Ne deduced μ, quadrupole moment.

NUCLEAR REACTIONS 12C(22Ne, X)18N, E=110 MeV/nucleon; measured fragment polarization.

doi: 10.1016/S0370-2693(99)00219-1
Citations: PlumX Metrics


1999SA75      Nucl.Phys. (Supplement) A654, 735c (1999)

K.Sato, M.Tanigaki, T.Onishi, M.Fukuda, T.Minamisono, M.Mihara, K.Matsuta, S.Takeda, M.Sasaki, T.Yamaguchi, T.Miyake, K.Minamisono, A.Morishita, F.Osumi, Y.Muramoto, S.Oui, T.Fukao, Y.Matsumoto, T.Ohtsubo, S.Fukuda, Y.Nojiri, S.Momota, K.Yoshida, A.Ozawa, T.Kobayashi, I.Tanihata, A.Kitagawa, M.Torikoshi, H.Sagawa, H.Kitagawa, G.F.Krebs, J.R.Alonso, T.J.M.Symons

Quadrupole Moments of Short-Lived β-Emitters 13, 19O and 21F

RADIOACTIVITY 13O(β+) [from 9Be(16O, X), E=135 MeV/nucleon]; 19O(β-) [from 18O(d, p), E=3.25 MeV]; 21F(β-) [from 9Be(22Ne, X), E=100 MeV/nucleon]; measured β-NQR spectrum in TiO2, MgF2. 13O, 19O, 21F deduced quadrupole moments. Comparison with neighboring nuclei and with theoretical results. Halo effects discussed.

doi: 10.1016/S0375-9474(00)88538-3
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1998MI10      Phys.Lett. 420B, 31 (1998)

T.Minamisono, T.Ohtsubo, K.Sato, S.Takeda, S.Fukuda, T.Izumikawa, M.Tanigaki, T.Miyake, T.Yamaguchi, N.Nakamura, H.Tanji, K.Matsuta, M.Fukuda, Y.Nojiri

Quadrupole Moment of the Proton Rich β-Emitting Nucleus 12N

RADIOACTIVITY 12N(β+); measured β-NMR. 12N deduced quadrupole moment. Modified β-NMR technique.

doi: 10.1016/S0370-2693(97)01553-0
Citations: PlumX Metrics


1998OG04      J.Phys.(London) G24, 1399 (1998)

H.Ogawa, K.Asahi, K.Sakai, A.Yoshimi, M.Tsuda, Y.Uchiyama, T.Suzuki, K.Suzuki, N.Kurokawa, M.Adachi, H.Izumi, H.Ueno, T.Shimoda, S.Tanimoto, N.Takahashi, W.-D.Schmidt-Ott, M.Schafer, S.Fukuda, A.Yoshida, M.Notani, T.Kubo, H.Okuno, H.Sato, N.Aoi, K.Yoneda, H.Iwasaki, N.Fukuda, N.Fukunishi, M.Ishihara

Static Moments of the 18N Ground State

RADIOACTIVITY 18N(β-) [from 22Ne primary beam fragmentation]; measured Iβ(H, t). 18N deduced ground-state Q, μ. β-NMR technique.


1998OZ01      J.Phys.(London) G24, 143 (1998)

A.Ozawa, M.Fujimaki, S.Fukuda, S.Ito, T.Kobayashi, S.Momota, T.Suzuki, I.Tanihata, K.Yoshida, G.Kraus, G.Munzenberg

Measurement of the β-Decay Branching Ratio of 17Ne into the First Excited State of 17F

RADIOACTIVITY 17Ne(β+) [from 20Ne fragmentation]; measured Eγ, Iγ; deduced β-branching ratio to 17F first excited state, log ft, asymmetry relative to mirror nucleus 17N.

doi: 10.1088/0954-3899/24/1/018
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1997KO06      Nucl.Phys. A616, 189c (1997)

A.A.Korsheninnikov, E.A.Kuzmin, E.Yu.Nikolsky, C.A.Bertulani, O.V.Bochkarev, S.Fukuda, T.Kobayashi, S.Momota, B.G.Novatsky, A.A.Ogloblin, A.Ozawa, V.Pribora, I.Tanihata, K.Yoshida

Elastic and Inelastic Scattering of Exotic Nuclei

NUCLEAR REACTIONS 1H(11Li, 11Li), E=62, 75 MeV/nucleon; 1H(9Li, 9Li), E=60 MeV/nucleon; 1H(8He, 8He), E=66, 73, 32 MeV/nucleon; 1H(6He, 6He), (11Li, 11Li), (8He, 8He), E=800 MeV/nucleon; 1H(14Be, 14Be), 1H(t, t), E ≈ 65-75 MeV/nucleon; measured σ(θ). 11Li, 8,6He deduced extended neutron distributions.

doi: 10.1016/S0375-9474(97)00088-2
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1997KO11      Phys.Rev.Lett. 78, 2317 (1997)

A.A.Korsheninnikov, E.A.Kuzmin, E.Yu.Nikolsky, O.V.Bochkarev, S.Fukuda, S.A.Goncharov, S.Ito, T.Kobayashi, S.Momota, B.G.Novatsky, A.A.Ogloblin, A.Ozawa, V.Pribora, I.Tanihata, K.Yoshida

L = 1 Excitation in the Halo Nucleus 11Li

NUCLEAR REACTIONS 11Li(p, p), (p, p'), (p, X), (p, pX), E=68 MeV/nucleon; measured σ(θ), inclusive proton spectra. 11Li deduced resonances, excited, ground state structure.

doi: 10.1103/PhysRevLett.78.2317
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1710.


1997KO12      Nucl.Phys. A617, 45 (1997)

A.A.Korsheninnikov, E.Yu.Nikolsky, C.A.Bertulani, S.Fukuda, T.Kobayashi, E.A.Kuzmin, S.Momota, B.G.Novatsky, A.A.Ogloblin, A.Ozawa, V.Pribora, I.Tanihata, K.Yoshida

Scattering of Radioactive Nuclei 6He and 3H by Protons: Effects of neutron skin and halo in 6He, 8He, and 11Li

NUCLEAR REACTIONS 1H(6He, p), (6He, pα), (6He, pnα), E=71 MeV/nucleon; 1H(t, p), E=73.5 MeV/nucleon; measured proton spectra, σ(θ); analyzed σ(θ) for beams 8,6He, other data. 6,8He, 11Li deduced neutron halo effects.

doi: 10.1016/S0375-9474(96)00492-7
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1683.


1997PE14      Phys.Lett. 405B, 224 (1997)

M.Petrascu, I.Tanihata, T.Kobayashi, A.Isbasescu, H.Petrascu, A.Korsheninnikov, E.Nikolsky, S.Fukuda, H.Kumagai, S.Momota, A.Ozawa, K.Yoshida, C.Bordeanu, I.David, I.Lazar, I.Mihai, G.Vaman, M.Giurgiu

Neutron Pre-Emission at the Fusion of 11Li Halo Nuclei with Si Targets

NUCLEAR REACTIONS Si(9Li, X), Si(11Li, X), E=11.2-15.2 MeV/nucleon; measured neutron spectra, transverse momentum distribution; deduced fusion, pre-emitted neutron related features.

doi: 10.1016/S0370-2693(97)00579-0
Citations: PlumX Metrics


1996KO02      Phys.Rev. C53, R537 (1996)

A.A.Korsheninnikov, E.Yu.Nikolsky, T.Kobayashi, A.Ozawa, S.Fukuda, E.A.Kuzmin, S.Momota, B.G.Novatsky, A.A.Ogloblin, V.Pribora, I.Tanihata, K.Yoshida

Spectroscopy of the Halo Nucleus 11Li by an Experimental Study of 11Li + p Collisions

NUCLEAR REACTIONS 1H(11Li, 11Li), (11Li, X), E=75 MeV/nucleon; measured σ(θ), proton spectra. 11Li deduced levels, halo characteristics.

doi: 10.1103/PhysRevC.53.R537
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1996MA37      Hyperfine Interactions 97/98, 501 (1996)

K.Matsuta, M.Fukuda, M.Tanigaki, T.Minamisono, Y.Nojiri, H.Akai, T.Izumikawa, M.Nakazato, M.Mihara, T.Yamaguchi, A.Harada, M.Sasaki, T.Miyake, T.Onishi, K.Minamisono, T.Fukao, K.Sato, Y.Matsumoto, T.Ohtsubo, S.Fukuda, K.Yoshida, A.Ozawa, S.Momota, T.Kobayashi, I.Tanihata, J.R.Alonso, G.F.Krebs, T.J.M.Symons

Hyperfine Interactions of 13O and 23Mg Implanted in Pt

RADIOACTIVITY 13O(β+) [from 9Be(16O, X), E=135 MeV/nucleon]; 23Mg(β+) [from 197Au(24Mg, X), E=100 MeV/nucleon]; measured β time spectra, NMR techniques, implantation in Pt; deduced hyperfine interaction, spin relaxation time, Knight shift.

doi: 10.1007/BF02150192
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1996MA38      Hyperfine Interactions 97/98, 519 (1996)

K.Matsuta, T.Minamisono, M.Tanigaki, M.Fukuda, Y.Nojiri, M.Mihara, T.Onishi, T.Yamaguchi, A.Harada, M.Sasaki, T.Miyake, K.Minamisono, T.Fukao, K.Sato, Y.Matsumoto, T.Ohtsubo, S.Fukuda, S.Momota, K.Yoshida, A.Ozawa, T.Kobayashi, I.Tanihata, J.R.Alonso, G.F.Krebs, T.J.M.Symons

Magnetic Moments of Proton Drip-Line Nuclei 13O and 9C

RADIOACTIVITY 13O(β+) [from 9Be(16O, X), E=135 MeV/nucleon]; 9C(β+) [from 12C(12C, X), E=70 MeV/nucleon]; measured β-NMR, polarized sources; deduced μ, spin expectation values.

doi: 10.1007/BF02150194
Citations: PlumX Metrics


1995MA48      Nucl.Phys. A588, 153c (1995)

K.Matsuta, M.Fukuda, M.Tanigaki, T.Minamisono, Y.Nojiri, M.Mihara, T.Onishi, T.Yamaguchi, A.Harada, M.Sasaki, T.Miyake, S.Fukuda, K.Yoshida, A.Ozawa, T.Kobayashi, I.Tanihata, J.R.Alonso, G.F.Krebs, T.J.M.Symons

Magnetic Moment of Proton Drip-Line Nucleus 9C

RADIOACTIVITY 9C(β+) [from 12C(12C, X), E=67 MeV/nucleon]; measured μ; deduced spin expectation value. β-NMR technique, polarized radioactive beam. Model comparison.

doi: 10.1016/0375-9474(95)00115-H
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1993FU06      Phys.Lett. 307B, 278 (1993)

M.Fukuda, T.Izumikawa, T.Ohtsubo, M.Tanigaki, S.Fukuda, Y.Nakayama, K.Matsuta, Y.Nojiri, T.Minamisono

Magnetic Moment of the Short-Lived β-Emitter 23Mg

RADIOACTIVITY 23Mg(β+) [from 24Mg(3He, α), E=4.8 MeV]; measured β asymmetry, NMR, polarized nuclei; deduced μ.

doi: 10.1016/0370-2693(93)90219-8
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1993FU12      Hyperfine Interactions 78, 117 (1993)

M.Fukuda, T.Izumikawa, T.Ohtsubo, M.Tanigaki, S.Fukuda, Y.Nakayama, K.Matsuta, Y.Nojiri, T.Minamisono

Magnetic Moment of 23Mg

RADIOACTIVITY 23Mg(β+) [from 24Mg(3He, α), E=4.8 MeV]; measured β-NMR spectra, asymmetry change; deduced μ. Model comparison.

doi: 10.1007/BF00568125
Citations: PlumX Metrics


1993MA67      Hyperfine Interactions 78, 123 (1993)

K.Matsuta, A.Ozawa, Y.Nojiri, T.Minamisono, M.Fukuda, S.Momota, T.Ohtsubo, S.Fukuda, K.Sugimoto, I.Tanihata, K.Yoshida, K.Omata, J.R.Alonso, G.F.Krebs, T.J.M.Symons

Beta-NMR Detection of Beta-Emitting Fragment 43Ti

RADIOACTIVITY 43Ti(β+) [from C(46Ti, X), E ≈ 116 MeV/nucleon]; measured β-NMR in Pt; deduced μ, meson exchange, configuration mixing effects role.

doi: 10.1007/BF00568126
Citations: PlumX Metrics


1993MA68      Hyperfine Interactions 78, 127 (1993)

K.Matsuta, A.Ozawa, Y.Nojiri, T.Minamisono, M.Fukuda, S.Momota, T.Ohtsubo, S.Fukuda, K.Sugimoto, I.Tanihata, K.Yoshida, K.Omata, J.R.Alonso, G.F.Krebs, T.J.M.Symons

Fragment Polarization of 43Tl in the 46Ti + C Collision

NUCLEAR REACTIONS C(46Ti, X), E=116 MeV/nucleon; measured projectile fragmentation, 43Ti fragment spin polarization; deduced reaction mechanism. Beta asymmetry technique.

doi: 10.1007/BF00568127
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1993MA72      Hyperfine Interactions 80, 1219 (1993)

K.Matsuta, A.Ozawa, Y.Nojiri, T.Minamisono, M.Fukuda, S.Momota, T.Ohtsubo, S.Fukuda, K.Sugimoto, I.Tanihata, K.Yoshida, K.Omata, J.R.Alonso, G.F.Krebs, T.J.M.Symons

Production of Unstable Nuclei Far from the Stability Line: Its scope and limitations

RADIOACTIVITY 20,21F(β-); 37,39Ca(β+); compiled, reviewed T1/2 data. 43Ti(β-); compiled, reviewed μ, T1/2 data. Production and study of unstable nuclei.

doi: 10.1007/BF00567486
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1993MI09      Nucl.Phys. A559, 239 (1993)

T.Minamisono, S.Fukuda, T.Ohtsubo, A.Kitagawa, Y.Nakayama, Y.Someda, S.Takeda, M.Fukuda, K.Matsuta, Y.Nojiri

Quadrupole Moment of the Doubly-Closed-Shell-Plus-One-Nucleon Nucleus 41Sc and Its Core Deformation

RADIOACTIVITY 41Sc(β+) [from 40Ca(d, n), E=4.1 MeV]; measured β asymmetry; deduced quadrupole moment. Recoil polarization, β-NMR technique, asymmetric β-distribution method.

doi: 10.1016/0375-9474(93)90189-5
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1993MI33      Hyperfine Interactions 78, 111 (1993)

T.Minamisono, T.Ohtsubo, S.Fukuda, Y.Nakayama, T.Araki, K.Mashitani, K.Matsuda, E.Takahashi, M.Tanigaki, M.Tanaka, H.Shiohara, Y.Someda, Y.Aoki, A.Kitagawa, M.Fukuda, K.Matsuta, Y.Nojiri

Precise Measurement of the Magnetic Moment of Doubly Closed Shell+1 Nucleon Nucleus 17F(I(π) = (5/2)+, T1/2 = 64.5s)

RADIOACTIVITY 17F(β+); measured β-NMR spectra asymmetry change in NaF; deduced μ.

doi: 10.1007/BF00568124
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1993MI34      Hyperfine Interactions 78, 159 (1993)

T.Minamisono, T.Ohtsubo, Y.Nakayama, S.Fukuda, T.Izumikawa, M.Tanigaki, M.Matsui, S.Takeda, N.Nakamura, M.Fukuda, K.Matsuta, Y.Nojiri

New Determination of Quadrupole Coupling Constants of Li Isotopes in Single Crystals LiIO3 and LiNbO3

RADIOACTIVITY 8Li(β-); measured modified β-NMR spectra in LiO3, LiNbO3; deduced quadrupole moment, quadrupole coupling constants.

doi: 10.1007/BF00568132
Citations: PlumX Metrics


1993MI35      Hyperfine Interactions 78, 165 (1993)

T.Minamisono, T.Ohtsubo, I.Minami, A.Kitagawa, S.Fukuda, Y.Nakayama, M.Fukuda, K.Matsuta, Y.Nojiri, S.Takeda, H.Sagawa, H.Kitagawa

Giant Quadrupole Moment and Proton Halo Discovered in 8B

RADIOACTIVITY 8B(β+); calculated quadrupole moment; deduced proton halo role.

doi: 10.1007/BF00568133
Citations: PlumX Metrics


1993MI36      Hyperfine Interactions 78, 169 (1993)

T.Minamisono, T.Ohtsubo, I.Minami, S.Fukuda, A.Kitagawa, Y.Nakayama, M.Fukuda, K.Matsuta, Y.Nojiri

Precise Measurement of Quadrupole Moment of 8B by Use of a Modified β-NMR

RADIOACTIVITY 8B(β+); 12B(β-); measured modified β-NMR spectra in Mg; deduced quadrupole moment.

doi: 10.1007/BF00568134
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1993MI37      Hyperfine Interactions 78, 191 (1993)

T.Minamisono, S.Fukuda, T.Ohtsubo, M.Tanigaki, A.Kitagawa, M.Fukuda, K.Matsuta, Y.Nojiri, S.Takeda

Quadrupole Moment of 41Sc by Use of New Nuclear Quadrupole Resonance Detection

RADIOACTIVITY 41Sc(β+); measured β-NMR spectra in TiO2; deduced quadrupole moment.

doi: 10.1007/BF00568138
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1993MI40      Hyperfine Interactions 80, 1315 (1993)

T.Minamisono, T.Ohtsubo, S.Fukuda, I.Minami, Y.Nakayama, M.Fukuda, K.Matsuta, Y.Nojiri

New Nuclear Quadrupole Resonance Technique in β-NMR

RADIOACTIVITY 41Sc(β+) [from 40Ca(d, n), E=4.1 MeV]; measured NQR spectra; deduced quadrupole coupling constant, quadrupole moment. Modified β-NMR technique, 45Sc data input.

doi: 10.1007/BF00567497
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1993OH05      Hyperfine Interactions 78, 185 (1993)

T.Ohtsubo, M.Tanigaki, S.Fukuda, Y.Nakayama, S.Takeda, N.Nakamura, H.Tanji, M.Fukuda, K.Matsuta, Y.Nojiri, T.Minamisono

Hyperfine Interactions of 12B in BN (Hexagonal)

RADIOACTIVITY 12B(β-) [from 11B(d, p), E=1.5 MeV]; measured modified β-NMR spectra; deduced hyperfine interactions, quadrupole moment. Quadrupole resonance technique.

doi: 10.1007/BF00568137
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1993OH11      Hyperfine Interactions 80, 1051 (1993)

T.Ohtsubo, Y.Nakayama, I.Minami, M.Tanigaki, S.Fukuda, A.Kitagawa, M.Fukuda, K.Matsuta, Y.Nojiri, H.Akai, T.Minamisono

Electric Field Gradient in Mg and Zn Detected by β-Emitters, 8Li and 12B

RADIOACTIVITY 8Li(β-); 12B(β-); measured NQR; deduced quadrupole coupling constants in hcp Mg, Zn.

doi: 10.1007/BF00567464
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1992MA63      Nucl.Instrum.Methods Phys.Res. B70, 304 (1992)

K.Matsuta, A.Ozawa, Y.Nojiri, T.Minamisono, M.Fukuda, A.Kitagawa, T.Ohtsubo, S.Momota, S.Fukuda, Y.Matsuo, H.Takechi, I.Minami, K.Sugimoto, I.Tanihata, K.Omata, S.Shimoura, J.R.Alonso, G.F.Krebs, T.J.M.Symons

A Fragment Separator at LBL for the Beta-NMR Experiment

RADIOACTIVITY 37K(β+); 39Ca(β+) [from 197Au(40Ca, X), E=118 MeV/nucleon]; 43Ti(EC) [from 9Be(46Ti, X), E=240 MeV/nucleon]; measured NMR, polarized nuclei.

doi: 10.1016/0168-583X(92)95946-O
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1992MI18      Phys.Rev.Lett. 69, 2058 (1992)

T.Minamisono, T.Ohtsubo, I.Minami, S.Fukuda, A.Kitagawa, M.Fukuda, K.Matsuta, Y.Nojiri, S.Takeda, H.Sagawa, H.Kitagawa

Proton Halo of 8B Discolosed by Its Giant Quadrupole Moment

RADIOACTIVITY 8B(β+); measured β-NMR; deduced quadrupole moment, proton halo characteristics. Modified β-NMR technique.

doi: 10.1103/PhysRevLett.69.2058
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1986AD11      J.Phys.Soc.Jpn., Suppl. 55, 1042 (1986)

M.Adachi, N.Yamada, M.Taya, T.Kohno, A.Makishima, T.Suzuki, S.Fukuda, M.Fukuda, T.Nagafuchi, H.Taketani

Measurement of the atomic polarization and nuclear magnetic moment of the 2+1 state in 22Ne with a tilted-foil method

NUCLEAR REACTIONS 19F(α, p), E=8 MeV; measured Eγ, Iγ(θ, H, t). 22Ne level deduced g factor. Tilted-foil method.


1986KO01      Phys.Rev. C33, 392 (1986)

T.Kohno, M.Adachi, S.Fukuda, M.Taya, M.Fukuda, H.Taketani, Y.Gono, M.Sugawara, Y.Ishikawa

Level Structure and Electromagnetic Properties in 212Ra

NUCLEAR REACTIONS 204Pb(12C, 4nγ), E=70-90 MeV; measured Eγ, Iγ, γ(θ), I(ce), γγ-, ce(γ)-coin, γ linear polarization. 212Ra deduced levels, J, π, ICC, T1/2, B(E2), B(E3), g, configurations. Ge(Li) detector, hyperpure Ge-Compton polarimeter, superconducting solenoid with Si(Li) detector.

doi: 10.1103/PhysRevC.33.392
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1985AD09      Nucl.Phys. A442, 361 (1985)

M.Adachi, T.Kohno, A.Makishima, S.Fukuda, M.Fukuda, M.Taya, H.Taketani

g-Factors of High-Spin Isomeric States in 216Ra

NUCLEAR REACTIONS 208Pb(12C, 4nγ), E=80 MeV; measured Iγ(θ, H, t). 216Ra deduced levels, isomer g, T1/2, J, π, configurations. Pulsed beam, enriched target, Ge(Li) detector.

doi: 10.1016/0375-9474(85)90149-6
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1976FU03      Phys.Lett. 62B, 146 (1976)

S.Fukuda, Y.Torizuka

Evidence for the Giant Monopole Resonance in 90Zr

NUCLEAR REACTIONS 90Zr(e, e'), E=183 MeV; measured electron scattering. 90Zr deduced monopole, multipole strengths, E0 resonance.

doi: 10.1016/0370-2693(76)90489-5
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1974NA21      Phys.Lett. 53B, 168 (1974)

I.C.Nascimento, J.R.Moreira, J.Goldemberg, S.Fukuda, T.Terasawa, T.Saito, K.Hosoyama, Y.Torizuka

Elastic Electron Scattering from the M7 Magnetization Density of 51V

NUCLEAR REACTIONS 51V(e, e); measured σ(θ). 51V deduced M7 magnetic moment.

doi: 10.1016/0370-2693(74)90522-X
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1972FU14      Phys.Rev.Lett. 29, 1109 (1972)

S.Fukuda, Y.Torizuka

Giant Multipole Resonances in 90Zr Observed by Inelastic Electron Scattering

NUCLEAR REACTIONS 90Zr(e, e'), E=150, 183, 250 MeV; measured σ(Ee', θ). 90Zr deduced giant multipole resonances, J, π, B(E1), B(E2).

doi: 10.1103/PhysRevLett.29.1109
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