NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = S.Tanaka Found 77 matches. 2023TA23 Phys.Rev. C 108, 054607 (2023) S.Tanaka, N.Nishimura, F.Minato, Y.Aritomo Postfission properties of uranium isotopes: A hybrid method with Langevin dynamics and the Hauser-Feshbach statistical model
doi: 10.1103/PhysRevC.108.054607
2022TA02 Phys.Rev. C 105, L021602 (2022) S.Tanaka, K.Hirose, K.Nishio, K.R.Kean, H.Makii, R.Orlandi, K.Tsukada, Y.Aritomo Angular momentum transfer in multinucleon transfer channels of 18O +237Np NUCLEAR REACTIONS 237Np(18O, X)236Np/237Np/238Np/239Np/237Pu/238Pu/239Pu/240Pu/239Am/240Am/241Am/242Am, E=162 MeV; measured fission fragments, angular distribution of fission fragments; deduced angular anisotropy, average angular momenta. Beam from JAEA tandem accelerator.
doi: 10.1103/PhysRevC.105.L021602
2020VE07 Phys.Rev. C 102, 054610 (2020) M.J.Vermeulen, K.Nishio, K.Hirose, K.R.Kean, H.Makii, R.Orlandi, K.Tsukada, I.Tsekhanovich, A.N.Andreyev, S.Ishizaki, M.Okubayashi, S.Tanaka, Y.Aritomo Measurement of fission-fragment mass distributions in the multinucleon transfer channels of the 18O + 237Np reaction NUCLEAR REACTIONS 237Np(18O, X)234U*/235U*/236U*/237U*/236Np*/237Np*/238Np*/239Np*/238Pu*/239Pu*/240Pu*/241Pu*/240Am*/241Am*/242Am*/243Am*/242Cm*/243Cm*/244Cm*/245Cm*/244Bk*/245Bk*/246Bk*, E=162.0 MeV from tandem accelerator facility of Japan Atomic Energy Agency (JAEA); measured fission fragments from the fission of reaction products U(A=234-237), Np(A=236-239), Pu(A=238-241), Am(A=240-243), Cm(A=242-244) and Bk(A=244-246) using ΔE-E silicon telescope to detect ejectiles, and four multiwire proportional counters, to detect fission fragments (FFs); deduced yields of fission fragments as a function of their mass and total excitation energy for each multi-nucleon transfer (MNT) channel, fission-fragment mass distributions as function of excitation energy of 7-70 MeV, most probable total excitation energy for each channel, light-fragment and heavy-fragment mass distributions. Comparison with Langevin theoretical calculations including the multichance fission (MCF) process of fission after neutron evaporation.
doi: 10.1103/PhysRevC.102.054610
2019MI06 Phys.Rev. C 99, 051601 (2019) Y.Miyamoto, Y.Aritomo, S.Tanaka, K.Hirose, K.Nishio Origin of the dramatic change of fission mode in fermium isotopes investigated using Langevin equations RADIOACTIVITY 250,252,254,256,258,260Fm(SF); calculated mass distributions, total kinetic energy (TKE) distributions, potential energy on the elongation-mass asymmetry plane, potential energy contours, and fission modes of fission fragments at low-excitation energies using Langevin equations of three-dimensional nuclear-shape parametrization. 237,238,239,240U, 239,240,241,242Np, 241,242,243Pu, 247,248,249,250Cm, 249,250,251,252Bk, 251,252,253,254Cf(SF); calculated fission-fragment mass distributions in the excitation-energy range of 10-20 MeV for four neck parameters using Langevin equations. Comparison with experimental data.
doi: 10.1103/PhysRevC.99.051601
2019TA21 Phys.Rev. C 100, 064605 (2019) S.Tanaka, Y.Aritomo, Y.Miyamoto, K.Hirose, K.Nishio Effects of multichance fission on isotope dependence of fission fragment mass distributions at high energies NUCLEAR REACTIONS 238U(18O, X)237U/238U/239U/240U/239Np/240Np/241Np/242Np/242Pu/243Pu/244Pu, E*=15, 25, 35, 45, 55 MeV; 237Np(18O, X)234U/235U/236U/236Np/237Np/238Np/238Pu/239Pu/240Pu/241Pu, E*=15, 25, 35, 45, 55 MeV; calculated fission fragment mass distributions (FFMD), fraction or probability of each fission chance using Langevin approach, and statistical model code GEF, including multichance fission (MCF). Comparison with experimental data from JAEA Tokai tandem facility. 234,235,236,237,238,239,240U, 236,237,238,239,240,241,242Np, 238,239,240,241,242,243,244Pu; calculated S(2n), fission barriers, mean number of neutron emission before fission using the GEF code.
doi: 10.1103/PhysRevC.100.064605
2017HI10 Phys.Rev.Lett. 119, 222501 (2017) K.Hirose, K.Nishio, S.Tanaka, R.Leguillon, H.Makii, I.Nishinaka, R.Orlandi, K.Tsukada, J.Smallcombe, M.J.Vermeulen, S.Chiba, Y.Aritomo, T.Ohtsuki, K.Nakano, S.Araki, Y.Watanabe, R.Tatsuzawa, N.Takaki, N.Tamura, S.Goto, I.Tsekhanovich, A.N.Andreyev Role of Multichance Fission in the Description of Fission-Fragment Mass Distributions at High Energies NUCLEAR REACTIONS 238U(18O, X)237U/238U/239U/240U/240Np/241Np/242Np/241Pu/242Pu/243Pu/244Pu, E=157.5 MeV; measured reaction products; deduced fragment yields.
doi: 10.1103/PhysRevLett.119.222501
2016MA03 Nucl.Phys. A946, 104 (2016) K.Matsushita, T.Nishio, S.Tanaka, M.Tsuneda, A.Sugiura, K.Ieki Measurement of proton-induced target fragmentation cross sections in carbon
doi: 10.1016/j.nuclphysa.2015.11.007
2014OH03 Few-Body Systems 55, 725 (2014) K.Ohnaka, K.Sagara, Y.Maeda, K.Ishibashi, S.Kimura, S.Tanaka, T.Fukunaga, J.Yasuda, T.Yabe, K.Yashima, Y.Eguchi, H.Shimoda, T.Sueta, S.Kuroita Systematic Measurement of pd Breakup Cross Section Around Space Star NUCLEAR REACTIONS 2H(p, 2p), E=7.5-13 MeV; measured reaction products, Ep, Ip; deduced σ, σ(θ, E). Comparison with available data.
doi: 10.1007/s00601-014-0890-7
2009SA54 Nucl.Instrum.Methods Phys.Res. A 610, 660 (2009) T.Sanami, M.Hagiwara, T.Oishi, M.Hosokawa, S.Kamada, Su.Tanaka, Y.Iwamoto, H.Nakashima, M.Baba .A Bragg curve counter with an internal production target for the measurement of the double-differential cross-section of fragment production induced by neutrons at energies of tens of MeV NUCLEAR REACTIONS 12C(n, x), E=65 MeV; measured products, 6,7Li, B, 7,9Be; deduced σ(θ, E). Data were imported from EXFOR entry 23111.
doi: 10.1016/j.nima.2009.09.011
2007SA30 J.Nucl.Sci.Technol.(Tokyo) 44, 657 (2007) S.Sato, Y.Verzilov, K.Ochiai, M.Wada, C.Kutsukake, S.Tanaka, Y.Abe, M.Seki, Y.Oginuma, M.Kawabe, T.Nishitani, C.Konno Neutronics Experimental Study on Tritium Production in Solid Breeder Blanket Mockup with Neutron Reflector
doi: 10.1080/18811248.2007.9711854
2007WA45 J.Phys.Soc.Jpn. 76, 114202 (2007) Y.Wakabayashi, T.Fukuchi, Y.Gono, A.Odahara, S.Tanaka, M.Inoue, T.Sasaki, M.Kibe, N.Hokoiwa, T.Shinozuka, M.Fujita, A.Yamazaki, T.Sonoda, C.S.Lee, Y.K.Kwon, J.Y.Moon, J.H.Lee High-Spin States in 93Nb NUCLEAR REACTIONS 82Se(16O, 4np), E=100 MeV; measured prompt and delayed Eγ, Iγ, γγ-coin, γ(θ), DCO ratios; 93Nb; deduced high-spin levels, J, π, isomer T1/2, configurations, γ linear polarization. Deformed independent particle model calculations.
doi: 10.1143/JPSJ.76.114202
2006AL34 IEEE trans.nucl.sci. 53, 270 (2006) J.Allison, K.Amako, J.Apostolakis, H.Araujo, P.Arce Dubois, M.Asai, G.Barrand, R.Capra, S.Chauvie, R.Chytracek, G.A.P.Cirrone, G.Cooperman, G.Cosmo, G.Cuttone, G.G.Daquino, M.Donszelmann, M.Dressel, G.Folger, F.Foppiano, J.Generowicz, V.Grichine, S.Guatelli, P.Gumplinger, A.Heikkinen, I.Hrivnacova, A.Howard, S.Incerti, V.Ivanchenko, T.Johnson, F.Jones, T.Koi, R.Kokoulin, M.Kossov, H.Kurashige, V.Lara, S.Larsson, F.Lei, O.Link, F.Longo, M.Maire, A.Mantero, B.Mascialino, I.McLaren, P.Mendez Lorenzo, K.Minamimoto, K.Murakami, P.Nieminen, L.Pandola, S.Parlati, L.Peralta, J.Perl, A.Pfeiffer, M.G.Pia, A.Ribon, P.Rodrigues, G.Russo, S.Sadilov, G.Santin, T.Sasaki, D.Smith, N.Starkov, S.Tanaka, E.Tcherniaev, B.Tome, A.Trindade, P.Truscott, L.Urban, M.Verderi, A.Walkden, J.P.Wellisch, D.C.Williams, D.Wright, H.Yoshida Geant4 Developments and Applications
doi: 10.1109/TNS.2006.869826
2006FU06 Phys.Rev. C 73, 067303 (2006) T.Fukuchi, S.Tanaka, T.Sasaki, Y.Gono, A.Odahara, T.Morikawa, M.Shibata, H.Watanabe, S.Motomura, T.Tsutsumi, O.Kashiyama, K.Saitoh, Y.Wakabayashi, T.Kishida, S.Kubono, M.Ishihara Level structure and excitation energy of a high-spin isomer in 150Ho NUCLEAR REACTIONS 141Pr(16O, 7n), E=165 MeV; measured prompt and delayed Eγ, Iγ, γγ-coin. 150Ho deduced levels, J, π, configurations, high-spin isomer T1/2.
doi: 10.1103/PhysRevC.73.067303
2005FU01 Eur.Phys.J. A 24, 249 (2005) T.Fukuchi, Y.Gono, A.Odahara, S.Tanaka, M.Inoue, Y.Wakabayashi, T.Sasaki, M.Kibe, N.Hokoiwa, T.Shinozuka, M.Fujita, A.Yamazaki, T.Sonoda, C.S.Lee, Y.K.Kwon, J.Y.Moon, J.H.Lee High-spin isomer in 93Mo NUCLEAR REACTIONS 82Se(16O, 5n), (16O, 6n), E=100 MeV; measured prompt and delayed Eγ, Iγ, γγ-coin, γ-ray linear polarization. 93Mo deduced high-spin levels, J, π, configurations, isomeric states T1/2. 92Mo deduced levels, J, π.
doi: 10.1140/epja/i2004-10145-2
2005SA46 Nucl.Phys. A758, 427c (2005) K.Sagara, T.Teranishi, H.Oba, M.Oshiro, M.Kouzuma, K.Nishida, N.Ikeda, S.Tanaka Direct measurement of 4He(12C, 16O)γ reaction cross section around Ecm = 2.4 MeV at KUTL NUCLEAR REACTIONS 4He(12C, 16O), E(cm)=2.4 MeV; measured particle spectra, σ. Long-time chopper for background reduction.
doi: 10.1016/j.nuclphysa.2005.05.079
2002LE15 J.Korean Phys.Soc. 40, 793 (2002) J.H.Lee, C.S.Lee, J.Y.Huh, J.Y.Moon, Y.K.Kwon, Y.Gono, T.Fukuchi, S.Tanaka, T.Shinozuka, M.Fujita, A.Yamazaki, T.Sonoda, Y.K.Kim, J.S.Chai Linear Polarization Measurement of Gamma Rays in 155Gd by using a Segmented Compton Polarimeter NUCLEAR REACTIONS 154Sm(α, 3n), E=35 MeV; measured Eγ, Iγ, γγ-coin, γ-ray polarization. 155Gd deduced high-spin levels, J, π. Segmented planar Ge detector.
2000IB01 Nucl.Instrum.Methods Phys.Res. A446, 536 (2000) M.Ibaraki, M.Baba, T.Miura, Y.Hirasawa, Y.Nauchi, H.Nakashima, S.-I.Meigo, O.Iwamoto, S.Tanaka Experimental Method for Neutron Elastic Scattering Cross-Section Measurement in 40-90 MeV Region at TIARA NUCLEAR REACTIONS C, Fe, Pb(n, n), E=40-90 MeV; measured elastic σ(θ).
doi: 10.1016/S0168-9002(99)01274-7
1999BA73 Nucl.Instrum.Methods Phys.Res. A428, 454 (1999) M.Baba, Y.Nauchi, T.Iwasaki, T.Kiyosumi, M.Yoshioka, S.Matsuyama, N.Hirakawa, T.Nakamura, Su.Tanaka, S.Meigo, H.Nakashima, Sh.Tanaka, N.Nakao Characterization of 40-90 MeV 7Li(p, n) Neutron Source at TIARA using a Proton Recoil Telescope and a TOF Method NUCLEAR REACTIONS 7Li(p, n), E=43-87 MeV; measured neutron spectra, production σ. Proton recoil telescope.
doi: 10.1016/S0168-9002(99)00161-8
1999KI30 J.Nucl.Sci.Technol.(Tokyo) 36, 29 (1999) E.J.Kim, T.Nakamura, Y.Uwamino, N.Nakanishi, M.Imamura, N.Nakao, S.Shibata, S.Tanaka Measurements of Activation Cross Sections on Spallation Reactions for 59Co and natCu at Incident Neutron Energies of 40 to 120 MeV NUCLEAR REACTIONS 59Co(n, X)56Mn/54Mn/52Mn/58Co/57Co/56Co/55Co/59Fe, E ≈ 45-75 MeV; Cu(n, X)56Mn/59Fe/60Co/58Co/57Co/56Co/64Cu/61Cu/60Cu, E ≈ 45-117 MeV; measured activation σ. Comparison with previous results, model predictions.
doi: 10.1080/18811248.1999.9726179
1999NA14 J.Nucl.Sci.Technol.(Tokyo) 36, 143 (1999) Y.Nauchi, M.Baba, T.Sanami, M.Ibaraki, T.Iwasaki, N.Hirakawa, S.Tanaka, S.-I.Meigo, H.Nakashima, H.Takada, T.Nakamura, Y.Watanabe Measurements of (n, xp), (n, xd) Double Differential Cross Sections of Carbon and Aluminum for 65 and 75 MeV Neutrons NUCLEAR REACTIONS C, 27Al(n, pX), (n, dX), E=65, 75 MeV; measured σ(E, θ). Comparison with model predictions. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23015. 1998IW02 J.Nucl.Sci.Technol.(Tokyo) 35, 169 (1998) T.Iwasaki, Y.Sakuya, N.Hirakawa, H.Nakashima, Y.Sakamoto, H.Takada, S.Tanaka Measurement and Analysis of Fission Rate Distributions of 237Np and 238U in a Polyethylene System with a 65 MeV Neutron Source NUCLEAR REACTIONS 237Np, 238U(n, F), E < 65 MeV; measured fission rates vs polyethylene thickness. Comparison with NMTC/JAERI calculations. Implications for accelerator-driven transmutation system.
doi: 10.1080/18811248.1998.9733841
1998KI21 Nucl.Sci.Eng. 129, 209 (1998) E.Kim, T.Nakamura, A.Konno, Y.Uwamino, N.Nakanishi, M.Imamura, N.Nakao, S.Shibata, S.Tanaka Measurements of Neutron Spallation Cross Sections of 12C and 209Bi in the 20- to 150-MeV Energy Range NUCLEAR REACTIONS 12C(n, 2n), E=20-150 MeV; 209Bi(n, xn)207Bi/206Bi/205Bi/204Bi/203Bi/202Bi/201Bi/200Bi/199Bi/198Bi, E=20-150 MeV; measured σ. Activation method.
doi: 10.13182/NSE98-A1977
1998MO03 Nucl.Phys. A629, 282c (1998) T.Morii, D.Roy, K.Sudoh, Z.-X.Sun, S.Tanaka, T.Yamanishi Color-Octet Mechanism in Low-p(T) ψ'-Productions NUCLEAR REACTIONS 1H(polarized p, X), E(cm)=50 GeV; calculated ψ' production associated two-spin asymmetry A(LL).
doi: 10.1016/S0375-9474(97)00700-8
1997IS12 Nucl.Instrum.Methods Phys.Res. A385, 215 (1997) K.Ishii, I.Nakamura, Y.Fujii, F.Kajino, J.Kanzaki, K.Kawagoe, Y.Kurihara, K.Nagai, M.Nozaki, T.Ohkubo, Y.Sugimoto, H.Takeda, S.Tanaka, K.Taruma, Y.Yamaoka, C.Yokoyama Performance Studies of a Lead-Scintillation Fiber Calorimeter Prototype for the Linear Collider Detector
doi: 10.1016/S0168-9002(96)01045-5
1996JO25 J.Phys.Soc.Jpn. 65, 2585 (1996) K.Jouda, S.Tanaka, K.Ichikawa, O.Aita X-Ray Photoemission and X-Ray Emission Spectra in Rare-Earth Trifluorides ATOMIC PHYSICS Pr, 19F, Nd(γ, X), (X, γ), E=low; measured photoemission, X-ray spectra; deduced charge transfer energy, effective hybridization mass dependences.
doi: 10.1143/JPSJ.65.2585
1996ZH18 Physica C260, 197 (1996) G.-Q.Zheng, Y.Kitaoka, K.Asayama, K.Hamada, H.Yamauchi, S.Tanaka NMR Study of Local Hole Distribution, Spin Fluctuation and Superconductivity in Tl2Ba2Ca2Cu3O10 NUCLEAR MOMENTS 63Cu, 17O, 205Tl; measured NMR; deduced spin fluctuation, local hole distribution, superconductivity related features in Tl2Ba2Ca2Cu3O10.
doi: 10.1016/0921-4534(96)00092-5
1995MO38 Prog.Theor.Phys.(Kyoto), Suppl. 120, 231 (1995) T.Morii, S.-C.Tanaka, T.Yamanishi The Spin-Dependent Gluon Distribution in a Proton NUCLEAR STRUCTURE 1H; calculated polarized gluon distribution vs x.
doi: 10.1143/PTPS.120.231
1995NA23 Phys.Rev. A51, 3036 (1995) Y.Namito, S.Ban, H.Hirayama, N.Nariyama, H.Nakashima, Y.Nakane, Y.Sakamoto, N.Sasamoto, Y.Asano, S.Tanaka Compton Scattering of 20- to 40-keV Photons NUCLEAR REACTIONS 27Al, C, Fe, Cu, 197Au, Pb(γ, γ), E=20-40 keV; measured Compton scattering spectra; deduced incoherent scattering function. High purity Ge detectors. ATOMIC PHYSICS 27Al, C, Fe, Cu, 197Au, Pb(γ, γ), E=20-40 keV; measured Compton scattering spectra; deduced incoherent scattering function. High purity Ge detectors.
doi: 10.1103/PhysRevA.51.3036
1995NA28 Nucl.Instrum.Methods Phys.Res. A362, 454 (1995) N.Nakao, T.Nakamura, M.Baba, Y.Uwamino, N.Nakanishi, H.Nakashima, S.-I.Tanaka Measurements of Response Function of Organic Liquid Scintillator for Neutron Energy Range up to 135 MeV
doi: 10.1016/0168-9002(95)00193-X
1994BA37 J.Nucl.Sci.Technol.(Tokyo) 31, 163 (1994) S.Ban, H.Hirayama, Y.Namito, S.-I.Tanaka, H.Nakashima, Y.Nakane, N.Nariyama Calibration of Silicon PIN Photodiode for Measuring Intensity of 7 ≈ 40 keV Photons
doi: 10.1080/18811248.1994.9735132
1994BB17 Proc.Intern.Conf.Nuclear Data for Science and Technology, Gatlinburg, Tennesse, 9-13 May, 1994, J.K.Dickens, Ed., American Nuclear Society, Vol.1, p .90 (1994) M.Baba, T.Kiyosumi, T.Iwasaki, M.Yoshioka, S.Matsuyama, N.Hirakawa, T .Nakamura, Su.Tanaka, R.Tanaka, Sh.Tanaka, H.Nakashima, S.Meigo Characterization and Application of 20-90 MeV 7Li(p, n) Neutron Source at Tiara NUCLEAR REACTIONS 7Li(p, x), E=43-67 MeV; measured products, Eν, Inulln; deduced σ(θ, E), σ(θ). Data were imported from EXFOR entry O0659. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0659. 1994MO02 Phys.Lett. 322B, 253 (1994) T.Morii, S.Tanaka, T.Yamanishi Effects of the Large Gluon Polarization on xg1(d)(x) and J/(PSI) Productions at Polarized ep and pp Collisions NUCLEAR REACTIONS 1H(polarized e, X), E=high; calculated spin-dependent J/(PSI) leptoproduction differential σ; deduced large gluon polarization role. NUCLEAR STRUCTURE 2H; calculated spin-dependent structure function; deduced large gluon polarization role.
doi: 10.1016/0370-2693(94)91116-9
1993BA50 Appl.Radiat.Isot. 44, 769 (1993) S.Ban, H.Hirayama, Y.Namito, S.Tanaka, H.Nakashima, Y.Nakane, M.Yoshizawa, N.Nariyama Measurement of the Photon Energy-Absorption Coefficient for Air, Nitrogen and Argon at 30 keV
doi: 10.1016/0969-8043(93)90147-3
1992IT03 J.Phys.Soc.Jpn. 61, 1287 (1992) Y.Itoh, H.Yasuoka, Y.Fujiwara, Y.Ueda, T.Machi, I.Tomeno, K.Tai, N.Koshizuka, S.Tanaka 63Cu(2) Nuclear Spin-Spin Relaxation in YBa2Cu3O(6.98), YBa2(63Cu)3O(7-δ), and YBa2Cu4O8 NUCLEAR MOMENTS 63Cu; measured nuclear quadrupole resonance; deduced 63Cu(2) spin-spin relaxation in YBa2Cu3O(6.98), YBa2(63Cu)3O(7-δ) and YBa2Cu4O8.
doi: 10.1143/JPSJ.61.1287
1992KO23 Phys.Rev. D46, 2854 (1992) K.Kobayakawa, T.Morii, S.Tanaka, T.Yamanishi Polarization of Partons in the Proton NUCLEAR STRUCTURE 1H; calculated structure function; deduced polarized gluons role.
doi: 10.1103/PhysRevD.46.2854
1987KA41 Nucl.Phys. A473, 31 (1987) S.Kakigi, K.Fukunaga, T.Ohsawa, A.Okihana, T.Sekioka, H.Nakamura-Yokota, S.Tanaka, S.Kato Multiple Scattering Effect for Quasifree Scattering in the 3He(p, pp)2H Reaction at 64.8 MeV NUCLEAR REACTIONS, MECPD 3He(p, 2p), E=64.8 MeV; measured σ(E1, θ1, θ2). PWIA analysis, double-scattering effect.
doi: 10.1016/0375-9474(87)90153-9
1986FU05 Nucl.Phys. A456, 48 (1986) K.Fukunaga, S.Kakigi, T.Ohsawa, A.Okihana, T.Sekioka, H.Nakamura-Yokota, S.Tanaka Breakup of 4He with Polarized Protons at 65 MeV NUCLEAR REACTIONS 4He(polarized p, p'), (polarized p, pt), E=65.05; measured σ(E(p), θ(p)), A(E(p), θ(p)), σ(E(p), E(t), θ(p), θ(t)), A(E(p), E(t), θ(p), θ(t)). Three-body model analysis.
doi: 10.1016/0375-9474(86)90365-9
1984TA14 Phys.Rev. C30, 911 (1984) S.Tanaka, K.J.Moody, G.T.Seaborg Transfer Reaction Cross Sections from the Interactions of 20Ne and 22Ne with 232Th NUCLEAR REACTIONS 232Th(20Ne, X)227Pa/228Pa/229Pa/230Pa/232Pa/233Pa/234Pa/231U/237U/233Np/234Np/236Np/236mNp/238Np, E=114, 129 MeV; 232Th(22Ne, X)229Pa/230Pa/232Pa/233Pa/234Pa/237U/239U/240U/234Np/236mNp/238Np/239Np, E=114 MeV; measured residuals production σ, σ(E). Activation technique.
doi: 10.1103/PhysRevC.30.911
1982FU10 Nucl.Phys. A390, 19 (1982) K.Fukunaga, T.Ohsawa, S.Kakigi, A.Okihana, S.Tanaka, T.Sekioka, H.Nakamura-Yokota Energy Spectra of Deuterons and Protons for the d + d Reaction at 60 MeV NUCLEAR REACTIONS 2H(d, d), (d, p), E=59.9 MeV; measured σ(Ed, θd), σ(Ep, θp). Four-body model analysis.
doi: 10.1016/0375-9474(82)90603-0
1981FU11 Nucl.Phys. A369, 289 (1981) K.Fukunaga, S.Kakigi, T.Ohsawa, A.Okihana, S.Tanaka, T.Sekioka, H.Nakamura-Yokota, S.Kato Deuteron Breakup with 3He at 89.4 and 118.9 MeV NUCLEAR REACTIONS 2H(3He, 3Hep), (3He, tp), (3He, 2d), E=89.4, 118.9; measured σ(E1, E2, θ1, θ2). Three-body, four-body model analysis.
doi: 10.1016/0375-9474(81)90021-X
1980KA20 J.Phys.Soc.Jpn. 48, 1797 (1980) S.Kakigi, K.Fukunaga, T.Ohsawa, S.Tanaka, A.Okihana, H.Nakamura-Yokota, T.Sekioka, N.Fujiwara Excited States of 4He Observed in the 4He(α, αd)2H Reaction at 119 MeV NUCLEAR REACTIONS 4He(α, α'), (α, αd), E=119 MeV; measured Eα, σ(Eα, θα, θd). 4He deduced levels, J, π. Kinematically complete experiment.
doi: 10.1143/JPSJ.48.1797
1980TA11 Nucl.Phys. A341, 199 (1980) S.Tanaka, N.Fujiwara, K.Fukunaga, T.Higo, T.Ohsawa, A.Okihana, T.Sekioka, T.Miyanaga, T.Yanabu Continuum Energy Spectra of 3He Scattered by 3He at 120 MeV NUCLEAR REACTIONS 3He(3He, 3He'), E=120 MeV; measured σ(E(3He), θ); deduced reaction mechanism. 3He deduced no excited states.
doi: 10.1016/0375-9474(80)90308-5
1979OK01 J.Phys.Soc.Jpn. 46, 707 (1979) A.Okihana, N.Fujiwara, H.Nakamura-Yokota, T.Yanabu, K.Fukunaga, T.Ohsawa, S.Tanaka The D(d, d)D, D(d, p)T and D(d, 3He)n Reactions at 13.2 MeV NUCLEAR REACTIONS 2H(d, d), (d, p), (d, t), (d, 3He), E=13.2 MeV; measured σ(θ); deduced σ(θ) for 2H(d, n). Optical model. DWBA analysis.
doi: 10.1143/JPSJ.46.707
1978FU03 J.Phys.Soc.Jpn. 44, 1413 (1978) K.Fukunaga, T.Ohsawa, N.Fujiwara, S.Tanaka, A.Okihana, T.Yanabu Excited States of 4He Observed in the 6Li + d Reaction NUCLEAR REACTIONS 6Li(d, α), (d, dα), E=13.6 MeV; measured σ(Eα, θ), σ(Ed, Eα, θ). 4He level deduced Γ, J, π.
doi: 10.1143/JPSJ.44.1413
1978FU08 J.Phys.Soc.Jpn. 45, 1783 (1978) K.Fukunaga, N.Fujiwara, S.Kakigi, T.Ohsawa, H.Nakamura-Yokota, S.Tanaka, A.Okihana, T.Sekioka, T.Higo, T.Miyanaga Breakup Reaction of 3He by 3He at 120 MeV NUCLEAR REACTIONS 3He(3He, 3Hep), (3He, 3Hed), E=120 MeV; measured 3He-p, 3He-d coin spectra. 3He level deduced no evidence. Quasi-free, final state interaction analysis.
doi: 10.1143/JPSJ.45.1783
1978TA04 J.Phys.Soc.Jpn. 44, 1405 (1978) The 9Be(d, t)8Be and 9Be(d, α)7Li Reaction in the Energy Range from 12.17 MeV to 14.43 MeV NUCLEAR REACTIONS 9Be(d, t), (d, α), E=12.17-14.43 MeV; measured σ(θ).
doi: 10.1143/JPSJ.44.1405
1978TA12 J.Phys.Soc.Jpn. 45, 733 (1978) S.Tanaka, K.Fukunaga, S.Kakigi, T.Ohsawa, N.Fujiwara, T.Yanabu Elastic and Inelastic Scattering of Deuterons by 9Be in the Energy Range of 12.17 MeV to 14.43 MeV NUCLEAR REACTIONS 9Be(d, d), (d, d'), E=12.17-14.43 MeV; measured σ(E, θ). 9Be deduced β2. Optical model, DWBA, coupled-channel analyses.
doi: 10.1143/JPSJ.45.733
1978TA23 Nucl.Phys. A311, 38 (1978) T.Tanabe, M.Yasue, K.Sato, F.Soga, M.Igarashi, K.Ogino, Y.Kadota, Y.Saito, S.Tanaka, F.Shimokoshi Study of the (3He, t) Reaction on 48Ca at 82 MeV NUCLEAR REACTIONS 48Ca(3He, 3He), (3He, d), (3He, α), (3He, t), E=82 MeV; measured σ(θ). Enriched target. Second-order zero-range, full-finite range. DWBA analysis.
doi: 10.1016/0375-9474(78)90500-6
1977FU09 J.Phys.Soc.Jap. 42, 725 (1977) K.Fukunaga, T.Ohsawa, S.Kakigi, S.Tanaka, N.Fujiwara Continuous Energy Spectra of Alpha-Particles from 11B(p, α)8Be Reaction NUCLEAR REACTIONS 11B(p, α), E=6.5-7.3 MeV; measured σ(E;Eα, θ).
doi: 10.1143/JPSJ.42.725
1977KI03 J.Phys.Soc.Jap. 42, 1083 (1977) T.Kitagaki, Y.Ohnuki, S.Tanaka, S.Homma, K.Abe, M.Higuchi, Y.Watase, H.Shimotono Reaction γ + p → p + π0 + π0 in the Medium Energy Region NUCLEAR REACTIONS 1H(γ, π0), E ≤ 1160 MeV; measured σ(E).
doi: 10.1143/JPSJ.42.1083
1976IN04 J.Inorg.Nucl.Chem. 38, 1425 (1976) Production of 7Be from Proton Bombardment of Light Elements NUCLEAR REACTIONS Be, B, N, O(p, 7Be), E ≤ 52 MeV; measured σ(E, E(7Be)).
doi: 10.1016/0022-1902(76)90001-4
1976KO19 J.Inorg.Nucl.Chem. 38, 2157 (1976) K.Komura, S.Tanaka, M.Uesugi, M.Sakanoue Proton Induced Reactions of 151Eu and 153Eu up to E = 52 MeV NUCLEAR REACTIONS 151,153Eu(p, X), E ≤ 52 MeV; measured σ(E) for production of 146,147,148,149,151,153Gd, 146,147,148,149Eu.
doi: 10.1016/0022-1902(76)80185-6
1976TA12 J.Phys.Soc.Jap. 41, 361 (1976) T.Tanabe, K.Koyama, M.Yasue, H.Yokomizo, K.Sato, J.Kokame, N.Koori, S.Tanaka The (3He, 3He), (3He, 3He') and (3He, α) Reactions on 12C at 82.1 MeV NUCLEAR REACTIONS 12C(3He, 3He), E=82.1 MeV; measured σ(θ); deduced optical potential parameters. 12C(3He, 3He'), (3He, α), E=82.1 MeV; measured σ(θ). 12C levels deduced β.
doi: 10.1143/JPSJ.41.361
1975TA11 J.Inorg.Nucl.Chem. 37, 2002 (1975) S.Tanaka, K.Sakamoto, K.Komura, M.Furukawa Production of 26Al from α-Particle Bombardment of Mg, Al and Si NUCLEAR REACTIONS Mg, Al, Si(α, X), E < 46 MeV; measured σ for production of 26Al.
doi: 10.1016/0022-1902(75)80937-7
1974TO10 Nucl.Phys. A232, 417 (1974) The Level Structure of 50V and the 5.255 MeV Isobaric Analog Resonance In 51V Studied by 50Ti(p, n) and (p, nγ) Reactions NUCLEAR REACTIONS 50Ti(p, n), (p, nγ), E=3.8-5.4 MeV; measured σ(Ep;En, θ), σ(Ep;Eγ, θ). 50V deduced levels, J, π, branching ratios, γ-mixing. 51V analog resonance deduced J, π. Enriched target.
doi: 10.1016/0375-9474(74)90629-0
1973KO22 Nucl.Phys. A213, 426 (1973) K.Komura, K.Sakamoto, S.Tanaka Concerning the β-Decay of 176Lu RADIOACTIVITY 176Lu; measured γγ-coin; deduced β- branch, log ft. 176Hf deduced levels.
doi: 10.1016/0375-9474(73)90162-0
1972KO50 Nucl.Phys. A198, 73 (1972) K.Komura, K.Sakamoto, S.Tanaka The Half-Life of Long-Lived 176Lu RADIOACTIVITY 176Lu; measured Iγ, γγ-coin; deduced T1/2.
doi: 10.1016/0375-9474(72)90772-5
1972TA03 Nucl.Phys. A179, 513 (1972) S.Tanaka, Y.Tomita, K.Ideno, S.Kikuchi Fast-Neutron Scattering from 139La, 141Pr, Er and 209Bi NUCLEAR REACTIONS 139La, 141Pr, Er, 209Bi(n, n), (n, n'), E=1.45-3.58 MeV; measured σ(E, En', θ). Natural targets.
doi: 10.1016/0375-9474(72)90387-9
1972TA16 J.Inorg.Nucl.Chem. 34, 2419 (1972) Nuclear Reactions of Nickel with Protons up to 56 MeV NUCLEAR REACTIONS 58Ni(p, pn), (p, p2n), (p, 2p), (p, 2pn), (p, α), (p, 2p2n), (p, αpn), 60Ni(p, n), (p, 2pn), (p, 2p2n), (p, αn), (p, α2n), 61Ni(p, n), 62Ni(p, n), 64Ni(p, n), 58Ni(p, αp2n), (p, α2pn), 60Ni(p, p3n), (p, α), (p, 2p3n), (p, α2pn), 61Ni(p, α), E=5-56 MeV; measured σ(E).
doi: 10.1016/0022-1902(72)80187-8
1971FU11 Nucl.Phys. A174, 539 (1971) M.Furukawa, K.Shizuri, K.Komura, K.Sakamoto, S.Tanaka Production of 26Al and 22Na from Proton Bombardment of Si, Al and Mg
doi: 10.1016/0375-9474(71)90401-5
1971KI05 J.Phys.Soc.Jap. 30, 595 (1971) T.Kitagaki, Y.Ohnuki, S.Tanaka, S.Homma, K.Abe Photoproduction of Two Neutral Pions from Hydrogen Near Threshold NUCLEAR REACTIONS 1H(γ, 2π0) , E < 730 MeV; measured σ(E).
doi: 10.1143/JPSJ.30.595
1970TA01 Phys.Rev. C2, 160 (1970) S.Tanaka, P.H.Stelson, W.T.Bass, J.Lin Levels in 53Mn, 58Co, 63Zn, and 70Ga from the (p, n) Reaction NUCLEAR REACTIONS 53Cr, 58Fe, 63Cu, 70Zn(p, n), E=2.74-6.35 MeV; measured σ(E;En). 53Mn, 58Co, 63Zn, 70Ga deduced levels.
doi: 10.1103/PhysRevC.2.160
1969TS02 Nucl.Phys. A125, 641(1969) K.Tsukada, S.Tanaka, Y.Tomita, M.Maruyama Elastic and Inelastic Scattering of Fast Neutrons from Iron, Nickel Andtungsten NUCLEAR REACTIONS Fe, Ni, W(n, n), (n, n'), E=0.694-4.49 MeV; measured σ(E; En', θ).
doi: 10.1016/0375-9474(69)90754-4
1968HU18 Phys.Rev. 171, 1297 (1968) Production Of 7Be, 22Na, and 24Na Fragments From Heavy Elements At 3, 10, And 30 Gev NUCLEAR REACTIONS Ag(p, x), Ta(p, x), 197Au(p, x), Pb(p, x), U(p, x), E=3-30 GeV; measured products, 7Be, 24Na, 22Na; deduced σ, σ(E). Data were imported from EXFOR entry C0341.
doi: 10.1103/PhysRev.171.1297
1964PO08 Phys.Rev. 135, B122 (1964) Formation of Sodium and Potassium Nuclides in the Bombardment of Light Elements with 29-GeV Protons NUCLEAR REACTIONS Ti, Fe, Cu(p, x), E=28.9 GeV; measured products, 22Na, 24Na, 42K, 43K; deduced σ, σ(E). Data were imported from EXFOR entry C0270.
doi: 10.1103/PhysRev.135.B122
1963HU14 Phys.Rev. 129, 434 (1963) J.Hudis, I.Dostrovsky, G.Friedlander, J.R.Grover, N.T.Porile, L.P.Remsberg, R.W.Stoenner, S.Tanaka Energy Dependence of Product Yields in Copper Spallation by Protons between 3 and 30 GeV NUCLEAR REACTIONS Cu, 65Cu(p, x), E=3-30 GeV; measured products, 63Cu, 7Be, 22Na, 24Na, 37Ar, 41Ar, 42K, 43K, 45Ti, 52Fe, 59Fe, 55Co, 56Co, 57Co, 58Co, 61Co, 60Cu, 61Cu, 62Cu, 64Cu; deduced σ, σ(E). Data were imported from EXFOR entry C0289.
doi: 10.1103/PhysRev.129.434
1963PO15 Nucl.Phys. 43, 500 (1963) N.T.Porile, S.Tanaka, H.Amano, M.Furukawa, S.Iwata, M.Yagi Nuclear reactions of Ga69 and Ga71 with 13-56 MeV protons NUCLEAR REACTIONS 69Ga(p, 2n), 69Ga(p, 2np), 69Ga(p, 3n), 69Ga(p, 3n2p), 69Ga(p, 3n3p), 69Ga(p, 3np), 69Ga(p, 3p), 69Ga(p, 4n), 69Ga(p, 4np), 69Ga(p, 5n2p), 69Ga(p, 6n2p), 69Ga(p, n), 69Ga(p, np), 71Ga(p, 2n3p), 71Ga(p, 3n), 71Ga(p, 3np), 71Ga(p, 4n), 71Ga(p, 4np), 71Ga(p, 5n), 71Ga(p, 5n2p), 71Ga(p, 5n3p), 71Ga(p, 5np), 71Ga(p, 6n), 71Ga(p, n2p), 71Ga(p, np), E=12.4-57.5 MeV; measured products, 69Ge, Eν, Iν; deduced σ, σ(E). Data were imported from EXFOR entry P0014.
doi: 10.1016/0029-5582(63)90370-5
1963PO16 Phys.Rev. 130, 1541 (1963) Nuclear Structure Effects In High-Energy (p, pn) Reactions NUCLEAR REACTIONS 65Cu, 66Zn(p, np), 70Ge(p, 2n), 70Ge(p, np), 72Ge(p, 2n), 72Ge, 76Se, 79Br, 81Br(p, np), E=2.9 GeV; measured products, 64Cu, Eπ, Iπ; deduced σ, σ(E). Data were imported from EXFOR entry C0282.
doi: 10.1103/PhysRev.130.1541
1963PO17 Phys.Rev. 132, 397 (1963) (p, pxn) Reactions of Br79 and Br81 with 2.9-GeV protons NUCLEAR REACTIONS 79,81Br(p, x), E=2.9 GeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry C0300.
doi: 10.1103/PhysRev.132.397
1961FU01 J.Phys.Soc.Japan 16, 129 (1961) NUCLEAR REACTIONS 16O(α, np), E=20-40 MeV; measured excitation function.
doi: 10.1143/JPSJ.16.129
1961TS07 J.Phys.Soc.Jpn 16, 166 (1961) K.Tsukada, S.Tanaka, M.Maruyama Inelastic Scattering of Neutrons by the Time-of-Flight Method NUCLEAR STRUCTURE 80Se, 77Se, 68Zn, 56Fe, 46Ti; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.16.166
1960FU06 J.Phys.Soc.Japan 15, 2167 (1960) M.Furukawa, Y.Ishizaki, Y.Nakano, T.Nozaki, Y.Saji, S.Tanaka Excitation Function for the Reaction B11(p, n)C11 up to Ep = 15 MeV and Energy Levels of C12 NUCLEAR STRUCTURE 17F, 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.15.2167
1960TA09 J.Phys.Soc.Japan 15, 545 (1960) S.Tanaka, M.Furukawa, T.Mikumo, S.Iwata, M.Yagi, H.Amano NUCLEAR STRUCTURE 56Mn, 54Mn, 58Co, 56Co, 57Co; measured not abstracted; deduced nuclear properties.
1960TA20 J.Phys.Soc.Japan 15, 2125 (1960) S.Tanaka, M.Furukawa, S.Iwata, M.Yagi, H.Amano, T.Mikumo Excitation Functions for Alpha-Particle Reaction on Fe56 and Fe57 NUCLEAR STRUCTURE 60Ni, 61Ni; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.15.2125
1960TA21 J.Phys.Soc.Japan 15, 2159 (1960) Reactions of Nickel with Alpha-Particles NUCLEAR STRUCTURE 64Zn, 66Zn, 65Zn, 62Zn, 68Zn; measured not abstracted; deduced nuclear properties.
doi: 10.1143/JPSJ.15.2159
1959ON26 J.Phys.Soc.Japan 14, 117 (1959) K.Ono, J.Shimada, K.Kuroda, O.Tanaka, H.Kamitsubo, A.Ito, S.Tanaka, M.Imaizumi Yields and Angular Distributions of Protons from F19(d, p)F20 and F19(d, p)F20
doi: 10.1143/JPSJ.14.117
1959TA04 J.Phys.Soc.Japan 14, 1269 (1959) Excitation Functions for (p, n) Reactions with Titanium, Vanadium, Chromium, Iron and Nickel up to Ep = 14 MeV
doi: 10.1143/JPSJ.14.1269
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