NSR Query Results
Output year order : Descending NSR database version of April 23, 2024. Search: Author = K.Nakai Found 58 matches. 2017FU06 Physics of Part.and Nuclei 48, 124 (2017) M.Fujiwara, K.Nakai, N.Takahashi, T.Hayakawa, T.Shizuma, S.Miyamoto, G.T.Fan, A.Takemoto, M.Yamaguchi, M.Nishimura Production of medical 99mTc isotope via photonuclear reaction
doi: 10.1134/S1063779617010075
2006IS04 Phys.Lett. B 640, 82 (2006) H.Ishiyama, T.Hashimoto, T.Ishikawa, Y.X.Watanabe, S.K.Das, H.Miyatake, Y.Mizoi, T.Fukuda, M.-H.Tanaka, Y.Fuchi, N.Yoshikawa, Y.Hirayama, S.C.Jeong, T.Nomura, I.Katayama, S.Mitsuoka, K.Nishio, M.Matsuda, P.K.Saha, S.Ichikawa, H.Ikezoe, T.Furukawa, H.Izumi, T.Shimoda, K.Nakai A new measurement of the astrophysical 8Li(α, n)11B reaction NUCLEAR REACTIONS 4He(8Li, n), E(cm)=0.7-2.6 MeV; measured σ(E), particle spectra. Comparison with other results.
doi: 10.1016/j.physletb.2006.07.036
2004HA54 Nucl.Phys. A746, 330c (2004) T.Hashimoto, T.Ishikawa, T.Kawamura, K.Nakai, H.Ishiyama, Y.X.Watanabe, H.Miyatake, M.H.Tanaka, N.Yoshikawa, S.C.Jeong, Y.Fuchi, I.Katayama, T.Nomura, S.K.Das, P.K.Saha, T.Fukuda, K.Nishio, S.Mitsuoka, H.Ikezoe, M.Matsuda, S.Ichikawa, T.Furukawa, H.Izumi, T.Shimoda, Y.Mizoi, M.Terasawa Measurement of the 8Li(α, n)11B reaction cross sections of astrophysical interest NUCLEAR REACTIONS 4He(8Li, n), E=14.6 MeV; measured excitation energy spectra. 8Li(α, n), E(cm)=0.5-3 MeV; deduced excitation function. Astrophysical implications discussed.
doi: 10.1016/j.nuclphysa.2004.09.040
2004MI34 Nucl.Phys. A738, 401 (2004) H.Miyatake, H.Ishiyama, M.-H.Tanaka, Y.X.Watanabe, N.Yoshikawa, S.C.Jeong, Y.Matsuyama, Y.Fuchi, T.Nomura, T.Hashimoto, T.Ishikawa, K.Nakai, S.K.Das, P.K.Saha, T.Fukuda, K.Nishio, S.Mitsuoka, H.Ikezoe, S.Ichikawa, M.Matsuda, Y.Mizoi, T.Furukawa, H.Izumi, T.Shimoda, M.Terasawa Exclusive measurement of the astrophysical 8Li(α, n) reaction cross section NUCLEAR REACTIONS 4He(8Li, n), E(cm)=0.9-2.8 MeV; measured σ, excitation energy spectrum. Comparison with previous results.
doi: 10.1016/j.nuclphysa.2004.04.070
2003IS12 Nucl.Phys. A718, 481c (2003) H.Ishiyama, T.Hashimoto, T.Kawamura, T.Ishikawa, H.Miyatake, M.H.Tanaka, Y.Fuchi, N.Yoshikawa, S.C.Jeong, Y.Watanabe, H.Kawakami, I.Katayama, T.Nomura, S.Mitsuoka, K.Nishio, M.Matsuda, S.Ichikawa, H.Ikezoe, T.Furukawa, H.Yano, H.Izumi, Y.Mizoi, M.Terasawa, T.Fukuda, K.Nakai, T.Shimoda Direct measurements of (α, n) and (p, n) reaction cross sections using light neutron-rich radioactive nuclear beams NUCLEAR REACTIONS 2H(7Li, 6He), (11B, 12B), (22Ne, 20F), 4He(7Li, 10Be), 9Be(7Li, 8Li), E not given; 2H(18O, 16N), E=73 MeV; calculated radioactive beam yields. Application to further cross section measurements discussed.
doi: 10.1016/S0375-9474(03)00863-7
2003IS13 Nucl.Phys. A718, 484c (2003) T.Ishikawa, H.Ishiyama, T.Hashimoto, T.Kawamura, H.Miyatake, M.H.Tanaka, Y.Fuchi, N.Yoshikawa, S.C.Jeong, Y.Watanabe, H.Kawakami, I.Katayama, T.Nomura, S.Mitsuoka, K.Nishio, M.Matsuda, S.Ichikawa, H.Ikezoe, T.Furukawa, H.Yano, H.Izumi, Y.Mizoi, M.Terasawa, T.Fukuda, K.Nakai, T.Shimoda Measurement of the 16N(α, n) reaction cross section NUCLEAR REACTIONS 4He(16N, n), E(cm) ≈ 1-4.5 MeV; measured σ.
doi: 10.1016/S0375-9474(03)00864-9
2003NA33 Nucl.Phys. A721, 673c (2003) Spin-Dependent Interactions in Hyperon-Nucleon Scattering
doi: 10.1016/S0375-9474(03)01150-3
2002KA65 Eur.Phys.J. A 15, 295 (2002) T.Kadowaki, J.Asai, W.Imoto, S.Iwata, M.Kurosawa, K.Nakai, A.Sato, K.Imai, H.Takahashi, C.J.Yoon, T.Maruta, M.Ieiri, T.Nagae, H.Noumi, T.Fukuda, P.K.Saha, B.Bassalleck Asymmetry measurement of the polarized Σ+p elastic scattering and the hyperon-nucleon spin-orbit interaction NUCLEAR REACTIONS 1H(π+, K+), E at 1.6 GeV/c; measured Σ hyperon polarization, hyperon-proton scattering asymmetry.
doi: 10.1140/epja/i2002-10054-4
2001AH08 Nucl.Instrum.Methods Phys.Res. A 457, 137 (2001) J.K.Ahn, H.Akikawa, J.Arvieux, B.Bassalleck, M.S.Chung, H.En'yo, T.Fukuda, H.Funahashi, S.V.Golovkin, A.M.Gorin, Y.Goto, M.Hanabata, T.Hayakawa, A.Ichikawa, M.Ieiri, K.Imai, M.Ishino, H.Kanda, Y.D.Kim, Y.Kondo, E.N.Kozarenko, I .E.Kreslo, J.M.Lee, A.Masaike, S.Mihara, K.Nakai, K.Nakazawa, K.Ozawa, A.Sato, H.D.Sato, K.S.Sim, T.Tabaru, F.Takeutchi, P.Tlusty, H.Torii, K.Yamamoto, S.Yokkaichi, M.Yoshida Active target-detector with scintillating fibers for hyperon-proton scattering NUCLEAR REACTIONS 1H(p, p), E=262.8 MeV; measured products, Eπ, Iπ; deduced σ(θ). Data were imported from EXFOR entry E1830.
doi: 10.1016/S0168-9002(00)00768-3
2001HA21 Nucl.Phys. A686, 591 (2001) T.Hashimoto, K.Nakai, Y.Wakasaya, I.Tanihata, Z.Fulop, H.Kumagai, A.Ozawa, K.Yoshida, R.Goswami Half-Life of 44Ti RADIOACTIVITY 44Ti(EC) [from 9Be(46Ti, X)]; measured Eγ, Iγ, T1/2. Comparison with previous results.
doi: 10.1016/S0375-9474(00)00566-2
1990TO03 Phys.Lett. 235B, 245 (1990) K.Tokushuku, H.Enyo, T.Nagae, H.Sano, S.Sasaki, M.Sekimoto, R.Chiba, K.Ichimaru, T.Mori, H.Yokota, I.Arai, J.Chiba, K.Nakai Analysis of Deuteron Spectra from Hadron-Nucleus Reactions at Several GeV/c with the Coalescence Model NUCLEAR REACTIONS 27Al, Pb(p, pX), (p, dX), E at 4 GeV/c; measured proton, deuteron spectra. Coalescence model.
doi: 10.1016/0370-2693(90)91958-E
1989YO03 Phys.Rev. C39, 2090 (1989) H.Yokota, S.Igarashi, K.Hama, T.Mori, T.Katsumi, K.Nakayama, K.Ichimaru, R.Chiba, K.Nakai, J.Chiba Direct (π+, pd) Cross Sections for Light Nuclei NUCLEAR REACTIONS 6,7Li, C(π+, pd), E=70, 130, 165 MeV; measured σ(θp, θd); deduced quasifree π+t → pd σ.
doi: 10.1103/PhysRevC.39.2090
1989YO05 Phys.Rev. C40, 270 (1989) H.Yokota, S.Igarashi, K.Hama, T.Mori, T.Katsumi, K.Ichimaru, K.Nakayama, R.Chiba, K.Nakai, J.Chiba Inclusive (π+, p) and (π+, pp) Cross Sections for Light Nuclei in the Resonance Energy Region NUCLEAR REACTIONS 6,7Li, C(π+, pX), (π+, 2p), E=70, 130, 165 MeV; measured σ(θ), σ(θp1, θp2); deduced effective numbers of quasideuteron.
doi: 10.1103/PhysRevC.40.270
1989YO07 Phys.Rev. C40, 1069 (1989) H.Yokota, S.Igarashi, K.Hama, T.Mori, T.Katsumi, K.Ichimaru, K.Nakayama, R.Chiba, K.Nakai, J.Chiba Broad Component of the (π+, pp) Angular Correlation NUCLEAR REACTIONS 6Li, 12C(π+, 2p), (π-, 2p), E=165 MeV; measured σ(θ1, θ2); deduced σ(θ) ratio, reaction mechanism.
doi: 10.1103/PhysRevC.40.1069
1987NA11 Phys.Lett. 191B, 31 (1987) T.Nagae, S.Sasaki, K.Tokushuku, H.Sano, M.Sekimoto, I.Arai, A.Manabe, H.Nunokawa, H.Sakamoto, K.Aoki, J.Chiba, K.Nakai Quasifree Production of Δ0 Isobars in Proton-Nucleus Reactions at 3.88 GeV/c NUCLEAR REACTIONS 2H, C, 27Al, Cu(p, p'), E at 3.88 GeV/c; measured proton spectra, σ(θ) vs momentum; deduced quasifree isobar production σ vs mass. Large acceptance spectrometer. Theoretical calculations.
doi: 10.1016/0370-2693(87)91316-5
1987YO01 Phys.Rev.Lett. 58, 191 (1987) H.Yokota, T.Mori, T.Katsumi, S.Igarashi, K.Hama, R.Chiba, K.Nakai, J.Chiba, H.Enyo, S.Sasaki, T.Nagae, M.Sekimoto Direct Observation of Multiple-Scattering Processes in Pion Absorption NUCLEAR REACTIONS 6Li, C(π-, 2p), E=70, 130, 165 MeV; measured σ(θ1, θ2); deduced multiple-scattering processes. Counter telescopes, plastic scintillators. Intranuclear cascade calculations.
doi: 10.1103/PhysRevLett.58.191
1986NA03 Phys.Rev. C33, 1002 (1986) K.Nakayama, H.Yokota, K.Ichimaru, Y.Takahata, F.Suekane, R.Chiba, K.Nakai, I.Arai, H.Enyo, S.Sasaki, T.Nagae, M.Sekimoto Pion Absorption on Nuclei at 65 MeV NUCLEAR REACTIONS C, 27Al, Cu, Ta(π+, p), (π-, p), (π+, d), (π-, d), (π+, 2p), (π-, 2p), (π+, np), (π-, np), E=65 MeV; measured σ(θ), pp-, nn- correlations; deduced nucleon-nucleon pair pion absorption σ ratio.
doi: 10.1103/PhysRevC.33.1002
1986YO05 Phys.Lett. 175B, 23 (1986) H.Yokota, K.Nakayama, K.Ichimaru, Y.Takahata, F.Suekane, R.Chiba, K.Nakai, I.Arai, H.Enyo, S.Sasaki, T.Nagae, M.Sekimoto Deuteron Emission from Pion Absorption at T(π) = 65 MeV NUCLEAR REACTIONS C, 27Al, Cu, Ta(π+, d), (π-, d), (π+, p), (π+, 2p), (π+, pd), E=65 MeV; measured σ(θ), σ(θ1, θ2); deduced pion absorption mechanism.
doi: 10.1016/0370-2693(86)90324-2
1986YO06 Phys.Rev.Lett. 57, 807 (1986) H.Yokota, K.Nakayama, K.Ichimaru, T.Katsumi, T.Mori, S.Igarashi, K.Hama, R.Chiba, K.Nakai, J.Chiba, H.Enyo, S.Sasaki, T.Nagae, M.Sekimoto Pion Absorption on T = 1 Nucleon Pairs at T(π) = 70 MeV NUCLEAR REACTIONS 6,7Li(π+, np), (π-, np), E=70 MeV; measured np(θ); deduced σ(θ), two-nucleon absorption component.
doi: 10.1103/PhysRevLett.57.807
1983SH49 Nucl.Phys. A408, 525 (1983) T.A.Shibata, K.Nakai, H.En'yo, S.Sasaki, M.Sekimoto, I.Arai, K.Nakayama, K.Ichimaru, H.Nakamura-Yokota, R.Chiba Particle Production in the Target-Rapidity Region from Hadron-Nucleus Reactions at Several GeV NUCLEAR REACTIONS C(p, π-), C(p, π+), C(π+, π-), C(π+, π+), 12C(p, x), 12C(π+, x), Cu(p, π-), Cu(p, π+), Cu(p, x), Cu(π+, π-), Cu(π+, π+), Cu(π+, x), Pb(p, π-), Pb(p, π+), Pb(p, x), Pb(π+, π-), Pb(π+, π+), Pb(π+, x), E=747 MeV-12 GeV; measured products, Eπ, Iπ; deduced σ(θ). Data were imported from EXFOR entry O0597.
doi: 10.1016/0375-9474(83)90244-0
1983YO04 Phys.Rev.Lett. 51, 1530 (1983) H.Yokota, K.Nakayama, K.Ichimaru, Y.Takahata, F.Suekane, R.Chiba, K.Nakai, E.Arai, H.Enyo, S.Sasaki, T.Nagae, M.Sekimoto Isospin Dependence of Pion Absorption by Light Nuclei NUCLEAR REACTIONS C, 27Al(π+, p), (π-, p), (π+, 2p), (π+, np), E=65 MeV; measured σ(θ) ratio, integrated two-nucleon yield ratios, pp(θ), pn(θ); deduced pion absorption mechanism.
doi: 10.1103/PhysRevLett.51.1530
1981SH03 Nucl.Instrum.Methods 179, 67 (1981) T.A.Shibata, T.Kobayashi, T.Numao, J.Chiba, K.Nakai, T.Yamazaki, O.Hashimoto, H.Hamagaki, M.Taino, A.Yamamoto, S.Kurokawa, H.Hirabayashi A Low-Momentum π-μ Channel at the KEK 12 GeV Proton Synchrotron NUCLEAR REACTIONS C, Al, Cu(p, π+), (p, π-), (p, α), (p, p), (p, d), (p, 3He), E=12 GeV; measured σ(θ, particle momentum). C, Al, Cu(π, X), E=20-300 MeV; measured σ(absorption), γ-multiplicities vs E. Pions from 12 GeV primary proton beam.
doi: 10.1016/0029-554X(81)91163-0
1980NA03 Phys.Rev.Lett. 44, 1446 (1980) K.Nakai, T.Kobayashi, T.Numao, T.A.Shibata, J.Chiba, K.Masutani Measurements of Cross Sections for Pion Absorption by Nuclei NUCLEAR REACTIONS Al, Ti, Cu, Sn, Au(π+, X), (π-, X), E=20-280 MeV; measured Eγ, Iγ, γγ-, πγ-, πγγ-coin, γ-multiplicity; deduced pion absorption σ(E). Optical model analysis.
doi: 10.1103/PhysRevLett.44.1446
1979CH26 Phys.Rev. C20, 1332 (1979) J.Chiba, K.Nakai, I.Tanihata, S.Nagamiya, H.Bowman, J.Ingersoll, J.O.Rasmussen Low-Energy Pion Production with 800 MeV/N 20Ne NUCLEAR REACTIONS Na, Cu, Pb(20Ne, π+), E=800 MeV/nucleon; measured σ(E(π), θπ).
doi: 10.1103/PhysRevC.20.1332
1979HA58 J.Phys.Soc.Jpn. 47, 1806 (1979) H.Hamagaki, Y.Nojiri, K.Sugimoto, K.Nakai Hyperfine Interactions of 12B Implanted in Ferromagnetic Nickel NUCLEAR MOMENTS 12B [from 11B(d, p), E=1.5 MeV]; measured hyperfine interaction vs T; deduced hfs field in Ni. NMR technique, implantation in ferromagnetic Ni.
doi: 10.1143/JPSJ.47.1806
1979NA12 Phys.Rev. C20, 2210 (1979) K.Nakai, J.Chiba, I.Tanihata, M.Sasao, H.Bowman, S.Nagamiya, J.O.Rasmussen Low-Energy Pion Production in High-Energy Nucleus-Nucleus Collisions NUCLEAR REACTIONS C, Na, F, Cu, Pb(20Ne, π+), E=400 MeV/nucleon; measured σ(Eπ, θπ).
doi: 10.1103/PhysRevC.20.2210
1978SH18 Nucl.Phys. A308, 513 (1978) T.Shibata, H.Ejiri, J.Chiba, S.Nagamiya, K.Nakai In-Beam Nuclear Gamma-Ray Studies of Relativistic Heavy Ion Reactions NUCLEAR REACTIONS Sr(12C, X), E=3-12.6 GeV; Na, S, Ca(12C, X), E=3-4.8 GeV; Na, S, Ca(α, X), E=1.6 GeV; measured σ(Eγ), Iγ.
doi: 10.1016/0375-9474(78)90563-8
1977CH23 J.Phys.Soc.Jap. 43, 1109 (1977) J.Chiba, R.S.Hayano, M.Sekimoto, H.Nakayama, K.Nakai Band Structures of the 135La, 133La and 129Cs Nuclei NUCLEAR REACTIONS 133Cs, 127I(α, 2n), E=28 MeV; 133Cs(3He, 3n), E=33 MeV; measured Eγ, σ(Eγ, θ), γγ(t). 135,133La, 129Cs deduced levels, K, J, π, T1/2. Natural targets. Ge(Li) detectors.
doi: 10.1143/JPSJ.43.1109
1977NA27 Nucl.Phys. A293, 137 (1977) H.Nakayama, J.Chiba, M.Sekimoto, K.Nakai Structure of the Transitional Nucleus 149Eu NUCLEAR REACTIONS 150Sm(p, 2nγ), E=18-26 MeV; measured Eγ, σ(Eγ), σ(Eγ, θ), γγ-coin, γγ-delayed coin. 149Eu deduced levels, J, π. Enriched target.
doi: 10.1016/0375-9474(77)90482-1
1976IK04 Hyperfine Interactions 2, 331 (1976) H.Ikezoe, G.D.Sprouse, H.Hamagaki, Y.Yamazaki, H.Nakayama, K.Nakai Nuclear g-Factor of the 6+ Isomeric State of 138Ba and Nuclear Spin Relaxation in Noble Gases NUCLEAR REACTIONS 136Xe(α, 2nγ), E=28 MeV; measured spin rotation. 138Ba level deduced g.
doi: 10.1007/BF01021162
1975MA02 Nucl.Phys. A237, 182 (1975) E.Matthias, E.Recknagel, O.Hashimoto, S.Nagamiya, K.Nakai, T.Yamazaki, Y.Yamazaki The g-Factor Measurement for the 8+ Isomeric State of 86Sr Produced in Kr Gas NUCLEAR REACTIONS Kr(α, 2n), E=22 MeV; measured αγ(θ, H, t). 86mSr deduced g. Stroboscopic method, natural Kr gas target.
doi: 10.1016/0375-9474(75)90471-6
1974HA06 Nucl.Phys. A218, 180 (1974) O.Hashimoto, A.Sumi, T.Nomura, S.Nagamiya, K.Nakai, T.Yamazaki, K.Miyano Measurement of the g-Factor of the 0.57 ms 7+ State in 202Tl NUCLEAR REACTIONS Hg(p, xn), E=28 MeV; measured γ(θ, H, t). 202Tl level deduced g.
doi: 10.1016/0375-9474(74)90029-3
1974NA08 Phys.Rev.Lett. 32, 1380 (1974) K.Nakai, D.Proetel, R.M.Diamond, F.S.Stephens Lifetimes and g Factors in Decoupled Bands NUCLEAR REACTIONS 122,124Sn(40Ar, xnγ), E=171 MeV; measured Eγ, DSA, γ(θ, H). 157,159Er levels deduced T1/2; 157Er level deduced g.
doi: 10.1103/PhysRevLett.32.1380
1974RE09 Phys.Lett. 52B, 414 (1974) E.Recknagel, Y.Yamazaki, O.Hashimoto, S.Nagamiya, K.Nakai Magnetic Moment of the 29/2+ Isomeric State in 213Fr NUCLEAR REACTIONS 204Hg(14N, 5nγ), E=94 MeV; measured γ(θ, H), Eγ. 213Fr level deduced g. Stroboscopic resonance method.
doi: 10.1016/0370-2693(74)90113-0
1974YA09 Phys.Rev.Lett. 33, 1614 (1974) Y.Yamazaki, O.Hashimoto, H.Ikezoe, S.Nagamiya, K.Nakai, T.Yamazaki Blocking Effect of the M1 Core Polarization Studied from the g Factor Of the 8+ State in 214Ra NUCLEAR REACTIONS 206Pb(12C, 4nγ), E=90 MeV; measured γ(θ, H). 214Ra level deduced g.
doi: 10.1103/PhysRevLett.33.1614
1973LE09 Nucl.Phys. A213, 1 (1973) J.R.Leigh, K.Nakai, K.H.Maier, F.Puhlhofer, F.S.Stephens, R.M.Diamond Energy-Level Systematics of Odd-Mass Lanthanum Isotopes; a New Coupling Scheme NUCLEAR REACTIONS 130,128,126,124,122Te(11B, 4nγ), E=40, 45, 50, 52.6, 56.5 MeV; 124Sn(14N, 5nγ), 120,118,116Sn(14N, 3nγ), E=50.5, 53, 58, 62, 64.8, 67, 68.5, 72, 76 MeV; 112Sn(16O, 2npγ), E=72, 76, 82, 88, 94 MeV; measured σ(Eγ, θ), γγ-coin, γγ(t). 125,127,129,131,133,135,137La deduced levels, J, π, T1/2, γ-multipolarity. Enriched targets. Ge(Li) detector.
doi: 10.1016/0375-9474(73)90178-4
1973NA08 Phys.Lett. 44B, 443 (1973) K.Nakai, P.Kleinheinz, J.R.Leigh, K.H.Maier, F.S.Stephens, R.M.Diamond, G.Lovhoiden Prolate Deformation in Neutron-Deficient Lanthanum Isotopes NUCLEAR REACTIONS 116,118,120,122Sn(14N, xnγ), E=not given; measured Eγ, Iγ(θ), γγ-coin. 130Ba(α, t), E=27 MeV; 138Ba(3He, d), E=22 MeV; measured σ(Et), σ(Ed), L. 125,127,129,131,133,135,137,139La deduced levels, J, π.
doi: 10.1016/0370-2693(73)90329-8
1973NA18 Nucl.Phys. A211, 381 (1973) S.Nagamiya, Y.Yamazaki, O.Hashimoto, T.Nomura, K.Nakai, T.Yamazaki Magnetic Moments of the [πh29/2]8+ States in Po Isotopes and of the [(πh29/2)8+ X νp-11/2]17/2- State in 209Po NUCLEAR REACTIONS 204,206Pb(3He, 3nγ), E=30 MeV; 204Pb(α, 2nγ), E=29 MeV; 208Pb(3He, 3nγ), E=28 MeV; 207Pb(α, 2nγ), E=28 MeV; 208Pb(α, 2nγ), E=25 MeV; measured γ(θ, H, t). 204,206,208,209,210Po levels deduced g, stroboscopic method.
doi: 10.1016/0375-9474(73)90727-6
1973YA06 Phys.Lett. 44B, 440 (1973) Y.Yamazaki, S.Nagamiya, T.Nomura, K.Nakai, T.Yamazaki Magnetic Moment of a Core-Excited Isomeric State in 210Po NUCLEAR REACTIONS 208Pb(α, 2nγ), E=33 MeV; measured Iγ(θ, H). 210Po level deduced g.
doi: 10.1016/0370-2693(73)90328-6
1972FI16 Phys.Scr. 5, 27 (1972) A.Filevich, K.-G.Rensfelt, J.Sztarkier, K.Nakai, I.Bergstrom The g-Factor of the 15- State in 210At NUCLEAR REACTIONS 209Bi(α, 3nγ), E not given; measured αγ(θ, H, t). 210At level deduced g. Stroboscopic method.
doi: 10.1088/0031-8949/5/1-2/005
1972MA10 Nucl.Phys. A183, 289 (1972) K.H.Maier, K.Nakai, J.R.Leigh, R.M.Diamond, F.S.Stephens Effective Single-Particle Magnetic Moments Around 208Pb NUCLEAR STRUCTURE 206,207,208Pb, 207,209,210,211Bi, 205Tl, 208,209,210Po; calculated effective single-particle μ.
doi: 10.1016/0375-9474(72)90660-4
1972MA24 Nucl.Phys. A186, 97 (1972) K.H.Maier, K.Nakai, J.R.Leigh, R.M.Diamond, F.S.Stephens Stroboscopic Measurement of the g-Factors of the 7- Isomer in 206Pb and the 21/2+ Isomer in 207Bi NUCLEAR REACTIONS 204Hg(α, 2nγ), E=26 MeV; 204Hg(7Li, 4nγ), E=41 MeV; measured αγ(θ, H, t). 206mPb, 207mBi deduced μ. Stroboscopic method.
doi: 10.1016/0375-9474(72)90127-3
1972NA08 Nucl.Phys. A189, 526 (1972) K.Nakai, B.Herskind, J.Blomqvist, A.Filevich, K.-G.Rensfelt, J.Sztarkier, I.Bergstrom, S.Nagamiya The g-Factor of the 12+ Isomeric State in 206Pb and the Effective Orbital g-Factor of the Neutron NUCLEAR REACTIONS 204Hg(α, 2nγ), E=27 MeV; measured αγ(θ, H, t). 206mPb deduced g, neutron effective orbital g.
doi: 10.1016/0375-9474(72)90311-9
1972ST18 Phys.Rev.Lett. 29, 438 (1972) F.S.Stephens, R.M.Diamond, J.R.Leigh, T.Kammuri, K.Nakai Decoupled Yrast States in Odd-Mass Nuclei
doi: 10.1103/PhysRevLett.29.438
1971DI02 Phys.Rev. C3, 344 (1971) R.M.Diamond, F.S.Stephens, K.Nakai, R.Nordhagen Lifetimes of Ground-Band States in 148, 150, 152Sm NUCLEAR REACTIONS 148,150,152Sm(40Ar, 40Ar'γ), E not given; measured σ(E(40Ar'), Eγ), recoil distance. 148,150,152Sm levels deduced T1/2, B(E2).
doi: 10.1103/PhysRevC.3.344
1971NA04 Phys.Lett. 34B, 269 (1971) Evidence for Oblate Deformation of the 9/2- Isomeric State in 199Tl NUCLEAR STRUCTURE 199Tl; analyzed γ-mixing; deduced oblate deformation.
doi: 10.1016/0370-2693(71)90600-9
1971NA06 Phys.Lett. 34B, 389 (1971) K.Nakai, F.S.Stephens, R.M.Diamond Quadrupole Moment of the First Excited State in 36Ar NUCLEAR REACTIONS 206Pb(36Ar, 36Ar'γ), E=150 MeV; measured σ(E(36Ar'), Eγ, θ(γ)). 36Ar level deduced quadrupole moment, B(E2). Coulomb excitation, reorientation effect.
doi: 10.1016/0370-2693(71)90633-2
1971NA10 Phys.Rev.Lett. 27, 155 (1971) K.Nakai, B.Skaali, N.J.S.Hansen, B.Herskind Nuclear Lifetime and g Factor of the 19/2- Isomeric State in 43Sc NUCLEAR REACTIONS 40Ca(α, pγ), E = 19 MeV; measured αγ(θ, H, t). 43mSc level deduced g, T1/2.
doi: 10.1103/PhysRevLett.27.155
1970NA05 Phys.Rev.Lett. 24, 903 (1970) K.Nakai, J.L.Quebert, F.S.Stephens, R.M.Diamond Quadrupole Moments of First Excited States in 28Si, 32S, and 40Ar NUCLEAR REACTIONS 206Pb(28Si, 28Si'γ), E=100-120 MeV; 206Pb(32S, 32S'γ), E=130-150 MeV; 130Te(40Ar, 40Ar'γ), E=110-125 MeV; measured σ(E(28Si'), Eγ, θ(γ)), σ(E(32S'), Eγ, θ(γ)), σ(E(40Ar'), Eγ, θ(γ)). 28Si, 32S, 40Ar levels deduced quadrupole moment.
doi: 10.1103/PhysRevLett.24.903
1970NA07 Nucl.Phys. A150, 114 (1970) K.Nakai, F.S.Stephens, R.M.Diamond Quadrupole Moments of the First Excited States in 20Ne and 22Ne NUCLEAR REACTIONS 120Sn, 130Te, 148Sm(20Ne, 20Ne'γ), (22Ne, 22Ne'γ), E=50-75 MeV; measured σ(E(Ne'), Eγ, θ(Ne'), θ(γ)). 20,22Ne levels deduced quadrupole moment, B(E2). Coulomb excitation, reorientation experiment.
doi: 10.1016/0375-9474(70)90461-6
1970NO01 Nucl.Phys. A142, 577 (1970) R.Nordhagen, G.Goldring, R.M.Diamond, K.Nakai, F.S.Stephens Perturbed Angular Distributions from 120,122,124Sn(40Ar, 4n)156,158,160Er Reaction Products NUCLEAR REACTIONS 120,122,124Sn(40Ar, 4nγ), E=148 MeV; 150Sm(20Ne, 20Ne'γ), E=68 MeV; measured γγ(θ, H, t). 156,158,160Er levels deduced g.
doi: 10.1016/0375-9474(70)90814-6
1970QU02 Nucl.Phys. A150, 68 (1970) J.L.Quebert, K.Nakai, R.M.Diamond, F.S.Stephens Lifetime Measurement of the First Excited State in 206Pb NUCLEAR REACTIONS 206Pb(40Ar, 40Ar'γ), E=170 MeV; measured recoil-distance, Doppler-shift. 206Pb level deduced T1/2, B(E2).
doi: 10.1016/0375-9474(70)90456-2
1968SU05 J.Phys.Soc.Japan 25, 1258(1968) K.Sugimoto, K.Nakai, K.Matuda, T.Minamisono Magnetic Moments of Short-Lived β-Radioactive Nuclei, 12B and 12N NUCLEAR MOMENTS 12B, 12N; measured μ. Nuclear magnetic resonance, recoil polarization, asymmetric β-decay.
doi: 10.1143/JPSJ.25.1258
1967SU03 Phys.Letters 25B, 130 (1967) K.Sugimoto, K.Nakai, K.Matuda, T.Minamisono Nuclear Magnetic Resonance of 20-ms 12B NUCLEAR STRUCTURE 12B; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90203-1
1967SU09 Contrib.Intern.Conf.Nucl.Struct., Tokyo, p.196 (1967); Oral Report K.Sugimoto, K.Nakai, K.Matuda, T.Minamisono Magnetic Moment of 12B NUCLEAR STRUCTURE 12N; measured not abstracted; deduced nuclear properties.
1966SU01 J.Phys.Soc. Japan 21, 213 (1966) K.Sugimoto, A.Mizobuchi, K.Nakai, K.Matuda Magnetic Moment of F17 - Nuclear Magnetic Resonance by Polarization Following O16(d, n)F17 Reaction NUCLEAR STRUCTURE 17F; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.21.213
1965SU02 Phys.Letters 18, 38 (1965) K.Sugimoto, A.Mizobuchi, K.Nakai, K.Matuda Nuclear Magnetic Resonance of Polarized 17F Formed Through the 16O(d, n)17F Reaction NUCLEAR STRUCTURE 17F, 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(65)90023-5
1964SU01 Phys.Rev. 134, B539 (1964) K.Sugimoto, A.Mizobuchi, K.Nakai Quadrupole Moment of the Second Excited State of F19 NUCLEAR STRUCTURE 19F; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.134.B539
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