NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = T.Tanaka Found 43 matches. 2023AD06 Eur.Phys.J. C 83, 1004 (2023), Erratum Eur.Phys.J. C 83, 1069 (2023) P.Adrich, P.Blumer, G.Caratsch, M.Chung, P.Clade, P.Comini, P.Crivelli, O.Dalkarov, P.Debu, A.Douillet, D.Drapier, P.Froelich, N.Garroum, S.Guellati-Khelifa, J.Guyomard, P.-A.Hervieux, L.Hilico, P.Indelicato, S.Jonsell, J.-P.Karr, B.Kim, S.Kim, E.-S.Kim, Y.J.Ko, T.Kosinski, N.Kuroda, B.M.Latacz, B.Lee, H.Lee, J.Lee, E.Lim, L.Liszkay, D.Lunney, G.Manfredi, B.Mansoulie, M.Matusiak, V.Nesvizhevsky, F.Nez, S.Niang, B.Ohayon, K.Park, N.Paul, P.Perez, C.Regenfus, S.Reynaud, C.Roumegou, J.-Y.Rousse, Y.Sacquin, G.Sadowski, J.Sarkisyan, M.Sato, F.Schmidt-Kaler, M.Staszczak, K.Szymczyk, T.A.Tanaka, B.Tuchming, B.Vallage, A.Voronin, D.P.van der Werf, A.Welker, D.Won, S.Wronka, Y.Yamazaki, K.-H.Yoo, P.Yzombard Production of antihydrogen atoms by 6 keV antiprotons through a positronium cloud
doi: 10.1140/epjc/s10052-023-12137-y
2023SW01 Phys.Lett. B 837, 137655 (2023) B.M.A.Swinton-Bland, J.Buete, D.J.Hinde, M.Dasgupta, T.Tanaka, A.C.Berriman, D.Y.Jeung, K.Banerjee, L.T.Bezzina, I.P.Carter, K.J.Cook, C.Sengupta, C.Simenel, E.C.Simpson, M.A.Stoyer Multi-modal mass-asymmetric fission of 178Pt from simultaneous mass-kinetic energy fitting NUCLEAR REACTIONS 144Sm(34S, F), E=146 MeV; measured fission fragments. 178Pt; deduced mass-angle distribution (MAD), the total kinetic energy (TKE) of the fission fragments, three fission modes: one mass-symmetric and two mass-asymmetric. The 14UD tandem accelerator at the Australian National University Heavy Ion Accelerator Facility.
doi: 10.1016/j.physletb.2022.137655
2023TA12 Phys.Rev. C 107, 054601 (2023) T.Tanaka, D.J.Hinde, M.Dasgupta, E.Williams, K.Vo-Phuoc, C.Simenel, E.C.Simpson, D.Y.Jeung, I.P.Carter, K.J.Cook, N.R.Lobanov, D.H.Luong, C.Palshetkar, D.C.Rafferty, K.Ramachandran Competition between fusion and quasifission in the angular momentum dependent dynamics of heavy element synthesis reactions NUCLEAR REACTIONS 196Pt(54Cr, X), E(cm)=209.5, 215.7, 219.0, 223.8 MeV;198Pt(52Cr, X), E(cm)=213.4, 218.1, 222.9, 226.7 MeV; measured reaction products; deduced capture σ(E), fission and scattering σ(θ), dependence of capture σ on the angular momentum, fragments angular momentum distribution, correlated distributions of mass and angle (MADs) of the fragments, fragments total kinetic energies, ratio of symmetric component to total fission component (quasifission and fusion-fission). ANU CUBE detector system consisting of two large-area position-sensitive MWPCs at 14UD tandem electrostatic accelerator of the Australian National University Heavy Ion Accelerator Facility.
doi: 10.1103/PhysRevC.107.054601
2022BE17 Phys.Rev. C 105, 064614 (2022) A.C.Berriman, D.J.Hinde, D.Y.Jeung, M.Dasgupta, H.Haba, T.Tanaka, K.Banerjee, T.Banerjee, L.T.Bezzina, J.Buete, K.J.Cook, S.Parker-Steele, C.Sengupta, C.Simenel, E.C.Simpson, M.A.Stoyer, B.M.A.Swinton-Bland, E.Williams Energy dependence of p + 232Th fission mass distributions: Mass-asymmetric standard I and standard II modes, and multichance fission NUCLEAR REACTIONS 232Th(p, F), E=6.2-28MeV; measured reaction products, fission fragments; deduced fission fragment yields mass distribution. Studied the influence of the multichance fission on the shape of the mass distribution. Comparison to other experimental data and GEF calculations. CUBE spectrometer consisting of large MWPCs at 14UD tandem electrostatic accelerator of the Australian National University Heavy Ion Accelerator Facility. RADIOACTIVITY 248Cm(SF); measured fission fragments; deduced fission fragment yields mass distribution.
doi: 10.1103/PhysRevC.105.064614
2021CO11 Phys.Rev. C 104, 024620 (2021) K.J.Cook, A.Chevis, T.K.Eriksen, E.C.Simpson, T.Kibedi, L.T.Bezzina, A.C.Berriman, J.Buete, I.P.Carter, M.Dasgupta, D.J.Hinde, D.Y.Jeung, P.McGlynn, S.Parker-Steele, B.M.A.Swinton-Bland, T.Tanaka, W.Wojtaczka High-precision proton angular distribution measurements of 12C (p, p') for the decay branching ratio of the Hoyle state NUCLEAR REACTIONS 12C(p, p'), E=10.20-10.70 MeV from 14UD electrostatic accelerator at HIAF-ANU facility; measured E(p), I(p), p(θ), differential σ(θ, E) for the first 2+ and second 0+ (Hoyle) state using the Breakup Array for Light Nuclei (BALiN) array of wedge shaped segmented double-sided silicon detectors (DSSDs), configured as two ΔE-E telescopes; deduced total σ(E) for the population of the first 2+ and second 0+ (Hoyle) state in 12C, thick target yields. Discussed radiative width of the Hoyle state, and possible application of measured cross sections for investigating cluster structures in 13N. Relevance to rate of carbon production in stars via radiative decay of the Hoyle state.
doi: 10.1103/PhysRevC.104.024620
2021NI08 Phys.Rev. C 104, 044617 (2021) T.Niwase, M.Wada, P.Schury, P.Brionnet, S.D.Chen, T.Hashimoto, H.Haba, Y.Hirayama, D.S.Hou, S.Iimura, H.Ishiyama, S.Ishizawa, Y.Ito, D.Kaji, S.Kimura, J.Liu, H.Miyatake, J.Y.Moon, K.Morimoto, K.Morita, D.Nagae, M.Rosenbusch, A.Takamine, T.Tanaka, Y.X.Watanabe, H.Wollnik, W.Xian, S.X.Yan α-decay-correlated mass measurement of 206, 207g, mRa using an α-TOF detector equipped multireflection time-of-flight mass spectrograph system ATOMIC MASSES 206,207,207mRa; measured time-of-flight spectra by α-decay-correlated mass spectroscopy using multireflection time-of-flight mass spectrograph (MRTOF-MS) system, with an α-TOF detector at SHE-Mass-II facility of RIBF-RIKEN; deduced mass excesses, and compared with evaluated data in AME2020. 207mRa; deduced excitation energy of the isomer, J, π. 206,207,207mRa isotopes produced in 159Tb(51V, X), E=306 MeV, followed by separation of evaporation residues using recoil ion separator GARIS-II at RIKEN. RADIOACTIVITY 206,207mRa(α)[from 159Tb(51V, X), E=306 MeV at RIBF-RIKEN]; measured Eα, Iα, T1/2 of decays of 206Ra and 207mRa, excitation energy of the isomer; deduced α-reduced width, configuration. Systematics of spins, parities, Eα, T1/2, α-branching ratios, reduced α widths for 203,203m,205,205m,207,207mRa. 198,199Po, 202,203At, 202,203Rn, 206,207Fr, 207Ra; observed α spectra from decays.
doi: 10.1103/PhysRevC.104.044617
2021TA31 Phys.Rev.Lett. 127, 222501 (2021) T.Tanaka, D.J.Hinde, M.Dasgupta, E.Williams, K.Vo-Phuoc, C.Simenel, E.C.Simpson, D.Y.Jeung, I.P.Carter, K.J.Cook, N.R.Lobanov, D.H.Luong, C.Palshetkar, D.C.Rafferty, K.Ramachandran Mass Equilibration and Fluctuations in the Angular Momentum Dependent Dynamics of Heavy Element Synthesis Reactions NUCLEAR REACTIONS 198Pt(52Cr, X)250No, E=219 MeV; 196Pt(54Cr, X)250No, E=222.9 MeV; measured reaction products; deduced correlated distributions of mass and angle is called a mass-angle distribution (MAD), scattering σ. TDHF calculations. The Heavy Ion Accelerator Facility of the Australian National University.
doi: 10.1103/PhysRevLett.127.222501
2020BA41 Phys.Rev. C 102, 024603 (2020) T.Banerjee, D.J.Hinde, D.Y.Jeung, K.Banerjee, M.Dasgupta, A.C.Berriman, L.T.Bezzina, H.M.Albers, Ch.E.Dullmann, J.Khuyagbaatar, B.Kindler, B.Lommel, E.C.Simpson, C.Sengupta, B.M.A.Swinton-Bland, T.Tanaka, A.Yakushev, K.Eberhardt, C.Mokry, J.Runke, P.Thorle-Pospiech, N.Trautmann Systematic evidence for quasifission in 9Be-, 12C-, and 16O-induced reactions forming 258, 260No NUCLEAR REACTIONS 238U(9Be, F)247Cm*, E=45-60 MeV; 244U(9Be, F)253Cf*, E=45-60 MeV; 248Cm(9Be, F)257Fm*, E=45-60 MeV; 249Cf(9Be, F)258No*, E=45-60 MeV; 248Cm(12C, F)260No*, E=60.80-89.18 MeV; 244Pu(16O, F)260No*, E=84.90-116.27 MeV; measured fission fragments, fission fragment mass and angular distributions using the CUBE spectrometer consisting of three multiwire proportional counters (MWPCs) at the Heavy Ion Accelerator Facility (HIAF) of the Australian National University; deduced reconstructed fission source velocity distributions, full momentum transfer (FMT) fission differential σ(θ, E), total and FMT fission σ(E), FMT mass-angle distributions (MADs), FMT fission angular anisotropies; analyzed mass-ratio (MR) spectra. 254,256,258,260,262No; deduced spontaneous fission mass-ratio distributions. Comparison with predictions from the transition state model (TSM) calculations for fusion fission reactions.
doi: 10.1103/PhysRevC.102.024603
2020ER03 Phys.Rev. C 102, 024320 (2020) T.K.Eriksen, T.Kibedi, M.W.Reed, A.E.Stuchbery, K.J.Cook, A.Akber, B.Alshahrani, A.A.Avaa, K.Banerjee, A.C.Berriman, L.T.Bezzina, L.Bignell, J.Buete, I.P.Carter, B.J.Coombes, J.T.H.Dowie, M.Dasgupta, L.J.Evitts, A.B.Garnsworthy, M.S.M.Gerathy, T.J.Gray, D.J.Hinde, T.H.Hoang, S.S.Hota, E.Ideguchi, P.Jones, G.J.Lane, B.P.McCormick, A.J.Mitchell, N.Palalani, T.Palazzo, M.Ripper, E.C.Simpson, J.Smallcombe, B.M.A.Swinton-Bland, T.Tanaka, T.G.Tornyi, M.O.de Vries Improved precision on the experimental E0 decay branching ratio of the Hoyle state NUCLEAR REACTIONS 12C(p, p'), E=10.5 MeV; measured electron-positron pairs for E0 transition from the first excited 0+ Hoyle state, and for E2 transition from the first 2+ state, Eγ, (ce)(ce)- and (ce)γ-coin, γ(θ), E(p), I(p) using the superconducting solenoid Super-e pair spectrometer and Si(Li) detector array for electrons and positrons, HPGe detector for γ radiation, and ANU BALiN double sided silicon strip detector array for scattered protons at the 14 UD pelletron tandem accelerator of Australian National University; deduced E0 branching ratio ΓE0π/Γ, reduction in radiative width. Comparison with previous experimental measurements; calculated 3α reaction rate within the temperature range of helium burning red giant stars using the NACRE library value. Possible impact on astrophysical calculations.
doi: 10.1103/PhysRevC.102.024320
2020HA27 Phys.Rev. C 102, 024625 (2020) H.Haba, F.Fan, D.Kaji, Y.Kasamatsu, H.Kikunaga, Y.Komori, N.Kondo, H.Kudo, K.Morimoto, K.Morita, M.Murakami, K.Nishio, J.P.Omtvedt, K.Ooe, Z.Qin, D.Sato, N.Sato, T.K.Sato, Y.Shigekawa, A.Shinohara, M.Takeyama, T.Tanaka, A.Toyoshima, K.Tsukada, Y.Wakabayashi, Y.Wang, S.Wulff, S.Yamaki, S.Yano, Y.Yasuda, T.Yokokita Production of 266Bh in the 248Cm(23Na, 5n)266Bh reaction and its decay properties RADIOACTIVITY 266,267Bh(α)[from 248Cm(23Na, 5n), (23Na, 4n), E=125.9, 130.6, 135.3 MeV]; 262Db(α), (SF)[from 266Bh α decay]; 263Db(EC), (α), (SF)[from 267Bh α decay]; 263Rf(SF)[from 263Db EC decay]; 258Lr(α), (EC)[from 262Db α decay]; 259Lr(α), (SF)[from 263Db α decay]; 258No(SF)[from 258Lr(EC); measured Eα, αα-, ααα- and α(SF)-correlations for 32 observed events using rotating wheel apparatus MANON and gas-jet transport system coupled to gas-filled recoil ion separator GARIS at RIKEN; deduced decay times, half-lives, decay branching ratios, production cross sections for 266Bh and 267Bh. Comparison with previous experimental results for half-lives and branching ratios for decay modes. NUCLEAR REACTIONS 248Cm(23Na, 5n), (23Na, 4n), E=125.9, 130.6, 135.3 MeV; measured reaction products, σ(E) at RIKEN. Comparison with HIVAP calculations, and with previous experimental results.
doi: 10.1103/PhysRevC.102.024625
2020SW02 Phys.Rev. C 102, 054611 (2020) B.M.A.Swinton-Bland, M.A.Stoyer, A.C.Berriman, D.J.Hinde, C.Simenel, J.Buete, T.Tanaka, K.Banerjee, L.T.Bezzina, I.P.Carter, K.J.Cook, M.Dasgupta, D.Y.Jeung, C.Sengupta, E.C.Simpson, K.Vo-Phuoc Mass-asymmetric fission of 205, 207, 209Bi at energies close to the fission barrier using proton bombardment of 204, 206, 208Pb NUCLEAR REACTIONS 204Pb(p, X)205Bi*, E=18.99, 20.99, 22.98, 24.99, 28.00 MeV; 206Pb(p, X)207Bi*, E=20.99, 22.98, 24.98, 28.00 MeV; 208Pb(p, X)209Bi*, E=24.98, 28.00 MeV; measured fission fragments using the CUBE fission spectrometer, with two large area position sensitive multiwire proportional counters (MWPCs), angular distributions at the 14UD tandem accelerator at Australian National University; deduced fission yields, fission mass ratios, fission mass distributions, mass-angle distribution (MAD) as a function of mass ratio, light and heavy fragment peak values. Comparison to previous experimental data, and theoretical calculations using GEF2019/1.3.
doi: 10.1103/PhysRevC.102.054611
2020TA02 Phys.Rev.Lett. 124, 052502 (2020) T.Tanaka, K.Morita, K.Morimoto, D.Kaji, H.Haba, R.A.Boll, N.T.Brewer, S.Van Cleve, D.J.Dean, S.Ishizawa, Y.Ito, Y.Komori, K.Nishio, T.Niwase, B.C.Rasco, J.B.Roberto, K.P.Rykaczewski, H.Sakai, D.W.Stracener, K.Hagino Study of Quasielastic Barrier Distributions as a Step towards the Synthesis of Superheavy Elements with Hot Fusion Reactions NUCLEAR REACTIONS 248Cm(22Ne, X), (26Mg, X), 238U(48Ca, X), E(cm)=165.1, 203.7 MeV; measured reaction products; deduced σ. Comparison with available data.
doi: 10.1103/PhysRevLett.124.052502
2020TA07 Prog.Theor.Exp.Phys. 2020, 041D02 (2020) T.Tanaka, K.Hagiwara, E.Gazzola, A.Ali, I.Ou, T.Sudo, P.K.Das, M.S.Reen, R.Dhir, Y.Koshio, M.Sakuda, A.Kimura, S.Nakamura, N.Iwamoto, H.Harada, G.Collazuol, S.Lorenz, M.Wurm, W.Focillon, M.Gonin, T.Yano Gamma-ray spectra from thermal neutron capture on gadolinium-155 and natural gadolinium NUCLEAR REACTIONS 155Gd, Gd(n, γ), E thermal; measured reaction products, Eγ, Iγ; deduced capture γ-ray energies, transition probabilities, nuclear level densities, photon strength function parameters. Comparison with available data, theoretical calculations.
doi: 10.1093/ptep/ptaa015
2019HA10 Prog.Theor.Exp.Phys. 2019, 023D01 (2019) K.Hagiwara, T.Yano, T.Tanaka, M.S.Reen, P.K.Das, S.Lorenz, Iw.Ou, T.Sudo, Y.Yamada, T.Mori, T.Kayano, R.Dhir, Y.Koshio, M.Sakuda, A.Kimura, S.Nakamura, N.Iwamoto, H.Harada, M.Wurm, W.Focillon, M.Gonin, A.Ali, G.Collazuol Gamma-ray spectrum from thermal neutron capture on gadolinium-157 NUCLEAR REACTIONS 157Gd(n, γ), E thermal; measured reaction products, Eγ, Iγ; deduced γ-ray energies and intensities. Comparison with available data.
doi: 10.1093/ptep/ptz002
2019TS02 Phys.Lett. B 790, 583 (2019) I.Tsekhanovich, A.N.Andreyev, K.Nishio, D.Denis-Petit, K.Hirose, H.Makii, Z.Matheson, K.Morimoto, K.Morita, W.Nazarewicz, R.Orlandi, J.Sadhukhan, T.Tanaka, M.Vermeulen, M.Warda Observation of the competing fission modes in 178Pt NUCLEAR REACTIONS 142Nd(36Ar, X)178Pt, E=155, 170, 180 MeV; measured reaction products; deduced fission fragment yields, first observation of a multimodal fission in the sub-lead region.
doi: 10.1016/j.physletb.2019.02.006
2018IT04 Phys.Rev.Lett. 120, 152501 (2018) Y.Ito, P.Schury, M.Wada, F.Arai, H.Haba, Y.Hirayama, S.Ishizawa, D.Kaji, S.Kimura, H.Koura, M.MacCormick, H.Miyatake, J.Y.Moon, K.Morimoto, K.Morita, M.Mukai, I.Murray, T.Niwase, K.Okada, A.Ozawa, M.Rosenbusch, A.Takamine, T.Tanaka, Y.X.Watanabe, H.Wollnik, S.Yamaki First Direct Mass Measurements of Nuclides around Z=100 with a Multireflection Time-of-Flight Mass Spectrograph NUCLEAR REACTIONS 232Th(19F, 5n)246Es, E=99.6, 103 MeV;238U(18O, 5n)251Fm, E=93.9 MeV; 203Tl(48Ca, 2n)249Md, E=215 MeV; 205Tl(48Ca, 3n)250Md, E=223 MeV; 205Tl(48Ca, 2n)251Md, E=215 MeV; 238U(19F, 5n)252md, E=98.6 MeV; 208Pb(48Ca, 2n)254No, E=219 MeV; measured reaction products, TOF; deduced mass excesses. Comparison with available data. ATOMIC MASSES 253,254Lr, 257,258Db, 261,262Bh, 266Mt; analyzed available data; deduced mass excesses.
doi: 10.1103/PhysRevLett.120.152501
2018KI21 Int.J. Mass Spectrom. 430, 134 (2018) S.Kimura, Y.Ito, D.Kaji, P.Schury, M.Wada, H.Haba, T.Hashimoto, Y.Hirayama, M.MacCormick, H.Miyatake, J.Y.Moon, K.Morimoto, M.Mukai, I.Murray, A.Ozawa, M.Rosenbusch, H.Schatz, A.Takamine, T.Tanaka, Y.X.Watanabe, H.Wollnik Atomic masses of intermediate-mass neutron-deficient nuclei with relative uncertainty down to 35-ppb via multireflection time-of-flight mass spectrograph ATOMIC MASSES 63Cu, 64,65,66Zn, 65Ga, 65,66,67Ge, 67As, 78,81Br, 80Rb, 79Sr; measured frequencies, TOF; deduced masses, new mass excess values. Comparison with AME16 evaluations. NUCLEAR REACTIONS S(36Ar, X)63Cu/64Zn/65Zn/66Zn/65Ga/65Ge/66Ge/67Ge/67As/78Br/81Br/80Rb/79Sr, E=3.30 MeV/nucleon; measured reaction products; deduced σ. Comparison with theoretical calculations of fusion-evaporation reactions.
doi: 10.1016/j.ijms.2018.05.001
2018RO14 Phys.Rev. C 97, 064306 (2018) M.Rosenbusch, Y.Ito, P.Schury, M.Wada, D.Kaji, K.Morimoto, H.Haba, S.Kimura, H.Koura, M.MacCormick, H.Miyatake, J.Y.Moon, K.Morita, I.Murray, T.Niwase, A.Ozawa, M.Reponen, A.Takamine, T.Tanaka, H.Wollnik New mass anchor points for neutron-deficient heavy nuclei from direct mass measurements of radium and actinium isotopes ATOMIC MASSES 210,211,212,214Ra, 210,211,212,213,214Ac; measured time of flight, and mass excess using multireflection time-of-flight mass spectrograph (MRTOF-MS) at superheavy element (SHE) mass facility of RIKEN-KEK, and using gas-filled recoil ion separator GARIS-II at RIKEN. Comparison with values from AME-2016. Ra and Ac isotopes produced in 169Tm(48Ca, X), E=5, 6 MeV/nucleon reaction at RIKEN. Z=82-92, N=121-129; systematics of S(2n) values.
doi: 10.1103/PhysRevC.97.064306
2017KA66 J.Phys.Soc.Jpn. 86, 034201 (2017) D.Kaji, K.Morita, K.Morimoto, H.Haba, M.Asai, K.Fujita, Z.Gan, H.Geissel, H.Hasebe, S.Hofmann, M.H.Huang, Y.Komori, L.Ma, J.Maurer, M.Murakami, M.Takeyama, F.Tokanai, T.Tanaka, Y.Wakabayashi, T.Yamaguchi, S.Yamaki, A.Yoshida Study of the Reaction 48Ca + 248Cm → 296Lv* at RIKEN-GARIS RADIOACTIVITY 292Lv, 288Fl, 284Cn, 293Lv, 289Fl, 285Cn, 294Lv, 290Fl(α) [from 248Cm(48Ca, X)296Lv, E=261.6, 258.0 MeV]; measured decay products, Eα, Iα; deduced decay branches and ratios. NUCLEAR REACTIONS 248Cm(48Ca, X)296Lv, E=261.6, 258.0 MeV; measured reaction products; deduced σ. Comparison with available data.
doi: 10.7566/jpsj.86.034201
2017SC02 Phys.Rev. C 95, 011305 (2017) P.Schury, M.Wada, Y.Ito, D.Kaji, F.Arai, M.MacCormick, I.Murray, H.Haba, S.Jeong, S.Kimura, H.Koura, H.Miyatake, K.Morimoto, K.Morita, A.Ozawa, M.Rosenbusch, M.Reponen, P.-A.Soderstrom, A.Takamine, T.Tanaka, H.Wollnik First online multireflection time-of-flight mass measurements of isobar chains produced by fusion-evaporation reactions: Toward identification of superheavy elements via mass spectroscopy ATOMIC MASSES 204,205,206Fr, 204,205,206Rn, 204,205,206At, 204,205Po, 205Bi; measured time-of-flight spectra, precise atomic masses with reference to that of 205Fr using GARIS-II recoil ion separator GARIS-II and multireflection time-of-flight mass spectrographs (MRTOF-MS) at RILAC-RIKEN facility. Isotopes produced in 165Ho, 169Tm(40Ar, X), E=4.825, 5.16 MeV/nucleon. Comparison with AME-2012 values, and previous experimental values.
doi: 10.1103/PhysRevC.95.011305
2017SM01 Phys.Lett. B 769, 1 (2017) C.Smorra, A.Mooser, M.Besirli, M.Bohman, M.J.Borchert, J.Harrington, T.Higuchi, H.Nagahama, G.L.Schneider, S.Sellner, T.Tanaka, K.Blaum, Y.Matsuda, C.Ospelkaus, W.Quint, J.Walz, Y.Yamazaki, S.Ulmer Observation of individual spin quantum transitions of a single antiproton NUCLEAR MOMENTS 1H; measured antiproton single spin-transitions.
doi: 10.1016/j.physletb.2017.03.024
2017SM05 Nature(London) 550, 371 (2017) C.Smorra, S.Sellner, M.J.Borchert, J.A.Harrington, T.Higuchi, H.Nagahama, T.Tanaka, A.Mooser, G.Schneider, M.Bohman, K.Blaum, Y.Matsuda, C.Ospelkaus, W.Quint, J.Walz, Y.Yamazaki, S.Ulmer A parts-per-billion measurement of the antiproton magnetic moment NUCLEAR MOMENTS 1H; measured frequencies; deduced g factor, nuclear magnetic moment of the antiproton.
doi: 10.1038/nature24048
2015IC01 Prog.Theor.Exp.Phys. 2015, 021D01 (2015) Y.Ichikawa, T.Nagae, H.Fujioka, H.Bhang, S.Bufalino, H.Ekawa, P.Evtoukhovitch, A.Feliciello, S.Hasegawa, S.Hayakawa, R.Honda, K.Hosomi, K.Imai, S.Ishimoto, C.W.Joo, S.Kanatsuki, R.Kiuchi, T.Koike, H.Kumawat, Y.Matsumoto, K.Miwa, M.Moritsu, M.Naruki, M.Niiyama, Y.Nozawa, R.Ota, A.Sakaguchi, H.Sako, V.Samoilov, S.Sato, K.Shirotori, H.Sugimura, S.Suzuki, To.Takahashi, T.N.Takahashi, H.Tamura, T.Tanaka, K.Tanida, A.O.Tokiyasu, Z.Tsamalaidze, B.Roy, M.Ukai, T.O.Yamamoto, S.Yang Observation of the "K- pp"-like structure in the d(π+, K+) reaction at 1.69 GeV/c NUCLEAR REACTIONS 2H(π+, K+), E=1.69 GeV; measured reaction products; deduced "K- pp"-like structure, hyperon resonance, doorway states.
doi: 10.1093/ptep/ptv002
2013MO25 Nucl.Phys. A914, 91c (2013) M.Moritsu, S.Adachi, M.Agnello, S.Ajimura, K.Aoki, H.C.Bhang, B.Bassalleck, E.Botta, S.Bufalino, N.Chiga, H.Ekawa, P.Evtoukhovitch, A.Feliciello, H.Fujioka, S.Hayakawa, F.Hiruma, R.Honda, K.Hosomi, Y.Ichikawa, M.Ieiri, Y.Igarashie, K.Imai, N.Ishibashi, S.Ishimoto, K.Itahashi, R.Iwasaki, C.W.Joo, S.Kanatsuki, M.J.Kim, S.J.Kim, R.Kiuchi, T.Koike, Y.Komatsu, V.V.Kulikov, S.Marcello, S.Masumoto, Y.Matsumoto, K.Matsuoka, K.Miwa, T.Nagae, M.Naruki, M.Niiyama, H.Noumi, Y.Nozawa, R.Ota, K.Ozawa, N.Saito, A.Sakaguchi, H.Sako, V.Samoilov, M.Sato, S.Sato, Y.Sato, S.Sawada, M.Sekimoto, K.Shirotori, H.Sugimura, S.Suzuki, H.Takahashi, T.Takahashi, T.N.Takahashi, H.Tamura, T.Tanaka, K.Tanida, A.O.Tokiyasu, N.Tomida, Z.Tsamalaidze, M.Ukai, K.Yagi, T.O.Yamamoto, S.B.Yang, Y.Yonemoto, C.J.Yoon, K.Yoshida Search for the Θ+ pentaquark at J-PARC
doi: 10.1016/j.nuclphysa.2013.01.010
2001TA03 Phys.Rev. C63, 034309 (2001) T.Tanaka, R.G.Nazmitdinov, K.Iwasawa Nonaxial Octupole Deformations in Light N = Z Nuclei at High Spins NUCLEAR STRUCTURE 32S, 56Ni; calculated rotational bands deformation, moments of inertia, related features; deduced role of non-axial octupole deformatCranked Hartree-Fock approach, Gogny interaction.
doi: 10.1103/PhysRevC.63.034309
2001TA19 Nucl.Phys. A690, 355 (2001) T.Tamae, T.Hino, H.Kawahara, M.Nomura, M.Sugawara, A.Tanaka, T.Tanaka, H.Tsubota, T.Yokokawa, T.K.Yoshida The (γ, p) Reaction in 197Au NUCLEAR REACTIONS 197Au(e, e'p), E=17-33 MeV; measured Ep, σ(θ). 197Au(γ, p), E ≈ 18-30 MeV; deduced σ(E, θ), reaction mechanism features. Shell model calculations.
doi: 10.1016/S0375-9474(01)00365-7
2000IW07 Prog.Theor.Phys.(Kyoto) 104, 777 (2000) M.Iwasaki, T.-A.Tanaka, S.Ishikawa Thermodynamic Properties of Color Superconducting Quark Matter
doi: 10.1143/PTP.104.777
2000IW08 Prog.Theor.Phys.(Kyoto) 104, 1041 (2000) M.Iwasaki, S.Ishikawa, T.-A.Tanaka Anti-Parallel Spin Pairing in Color Superconductivity
doi: 10.1143/PTP.104.1041
1999SH05 Phys.Rev. C59, 239 (1999); Erratum Phys.Rev. C61, 029901 (2000) Clusters in the Photodisintegration of 9Be NUCLEAR REACTIONS 9Be(γ, p), (γ, d), (γ, t), (γ, 3He), E=21-39 MeV; measured σ(E, θ). Cluster model analysis.
doi: 10.1103/PhysRevC.59.239
1998TA22 Phys.Rev. C58, 2765 (1998) Backbending Phenomenon in 48Cr NUCLEAR STRUCTURE 48Cr; calculated rotational bands energies, single-particle Routhians; deduced new backbending mechanism. Self-consistent cranked HFB calculations.
doi: 10.1103/PhysRevC.58.2765
1998UC01 Eur.Phys.J. A 2, 13 (1998) K.Uchiyama, K.Furuno, T.Shizuma, M.Sugita, M.Kato, Y.Tokita, M.Murasaki, N.Hashimoto, H.Takahashi, T.Komatsubara, K.Matsuura, T.Tanaka, Y.Sasaki Measurement of the Lifetime of the First 2+ State in 124Ba NUCLEAR REACTIONS 109Ag(19F, 4n), E=75 MeV; measured Eγ, Iγ, γγ-coin. 124Ba level deduced T1/2, B(E2). Systematics in Ba isotopes discussed. Recoil distance technique.
doi: 10.1007/s100500050084
1997OH07 Physica B237-238, 307 (1997) T.Ohno, T.Kanashiro, Y.Yamada, T.Yamanishi, T.Tanaka, Y.Kishimoto, K.Nakamura, Y.Michihiro 59Co Spin-Lattice Relaxation in Superconductor CoSi2 NUCLEAR MOMENTS 59Co; measured NMR; deduced spin-lattice relaxation rate in CoSi2, superconducting properties.
doi: 10.1016/S0921-4526(97)00186-5
1997TA11 Phys.Rev. C56, 180 (1997) T.Tanaka, F.Sakata, T.Marumori, K.Iwasawa Band Termination of Collective Rotation: Dynamical mechanism of occurrence NUCLEAR STRUCTURE 16O, 24Mg; calculated collective states rotational energy, density distributions vs spin, binding energies; deduced band termination related features. Time-dependent HF, self-consistent collective coordinate method.
doi: 10.1103/PhysRevC.56.180
1995MA87 Prog.Theor.Phys.(Kyoto) 93, 335 (1995) T.Marumori, F.Sakata, T.Une, T.Tanaka, A.Onoda A Possible Microscopic Description of Nuclear Collective Rotation in Band-Crossing Region - Occurrence Mechanism of s-Band -
doi: 10.1143/PTP.93.335
1995TA23 Z.Phys. A353, 79 (1995) Relativistic Wave Equation for a Boson-Fermion System
doi: 10.1007/BF01297730
1993TA08 Nucl.Phys. A559, 317 (1993) T.Tanaka, M.Hirooka, M.Sugawara, T.Tamae, H.Tsubota The (γ, p) and (γ, α) Cross Sections for 63,65Cu in the Giant Dipole Resonance Region NUCLEAR REACTIONS 63,65Cu(e, p), (e, α), E=14-60 MeV; measured σ(θ=90°); deduced σ(γ, p), σ(γ, α) at θ=90°. 63,65Cu deduced isospin splitting, photoreaction mechanism in the GDR region. Enriched targets.
doi: 10.1016/0375-9474(93)90156-R
1986SU04 Nucl.Phys. A452, 41 (1986) R.A.Sutton, M.N.Thompson, M.Hirooka, T.Tanaka, K.Shoda The Photoproton Reaction of 25Mg NUCLEAR REACTIONS 25Mg(e, p), E=15-28 MeV; measured proton spectra; deduced partial photoproton, absorption, σ(γ, np). 25Mg deduced configuration, isospin splitting of the GDR. Virtual photon.
doi: 10.1016/0375-9474(86)90507-5
1984HI11 Nucl.Phys. A431, 269 (1984) M.Hirooka, T.Tanaka, T.Hino, A.Tanaka, T.Tamae, M.Sugawara, H.Miyase 24Mg(e, α) Reaction in the Giant Resonance Region NUCLEAR REACTIONS 24Mg(e, α), E=14-24 MeV; measured σ(E(e), E(α), θ); deduced σ(γ, α) for E1, E2. Enriched target. Statistical model calculation.
doi: 10.1016/0375-9474(84)90175-1
1984TA10 Phys.Rev. C30, 350 (1984) T.Tanaka, R.M.Steffen, E.B.Shera, W.Reuter, M.V.Hoehn, J.D.Zumbro Measurement and Analysis of Muonic X Rays of 176,177,178,179,180Hf ATOMIC PHYSICS, Mesic-Atoms 176,177,178,179,180Hf; measured muonic X-rays. NUCLEAR MOMENTS 176,177,178,179,180Hf; measured muonic E X-ray, I X-ray; deduced monopole, quadrupole charge distributions, isotope shifts, rms radii. 176,177,178,179,180Hf level deduced isomer shift, quadrupole moment, B(E2). Axially symmetric rotor model comparison.
doi: 10.1103/PhysRevC.30.350
1983RY07 Nucl.Phys. A411, 105 (1983) P.J.Ryan, M.N.Thompson, K.Shoda, T.Tanaka The Photodisintegration of 24Mg NUCLEAR REACTIONS 24Mg(γ, p), (γ, n), E=28 MeV bremsstrahlung; measured proton yield vs Ep, Eγ, Iγ, σ(θp); deduced σ(γ, p)/σ(γ, n). 23Na, 23Mg levels deduced energy integrated population σ. 24Mg(γ, α), E=12-26 MeV bremsstrahlung; measured σ(θ). 24Mg deduced GDR decay characteristics, isospin purity, configuration. Magnetic spectrometer, enriched target.
doi: 10.1016/0375-9474(83)90510-9
1982HE13 At.Data Nucl.Data Tables 27, 1 (1982) B.L.Henke, P.Lee, T.J.Tanaka, R.L.Shimabukuro, B.K.Fujikawa Low-energy x-ray interaction coefficients: Photoabsorption, scattering, and reflection: E =100-2000 eV Z =1-94 COMPILATION Z=1-94; compiled theoretical σ, atomic scattering factors, parameters; deduced photoabsorption cross sections from 30 to 10 000 eV.
doi: 10.1016/0092-640x(82)90002-x
1981FU12 J.Phys.Soc.Jpn. 50, 3198 (1981) T.Fujisawa, N.Kishida, T.Kubo, T.Wada, Y.Toba, T.Hasegawa, M.Sekiguchi, N.Ueda, M.Yasue, F.Soga, H.Kamitsubo, M.Nakamura, K.Hatanaka, Y.Wakuta, T.Tanaka, A.Nagao Analyzing Power-Polarization Inequality in the Inelastic Scattering of Protons on 12C for Incident Energies from 22.0 to 29.0 MeV NUCLEAR REACTIONS 12C(polarized p, p'), E=22-29 MeV; measured P(θ), analyzing power vs θ. Proton-gamma coincidence technique.
doi: 10.1143/JPSJ.50.3198
1981RY03 Nucl.Phys. A371, 318 (1981) P.J.P.Ryan, M.N.Thompson, K.Shoda, T.Tanaka The Photoproton Decay of 27Al NUCLEAR REACTIONS 27Al(e, p), E=14.8-27.6 MeV; measured σ(Ep), σ(θ). 26Mg levels deduced population probability, photoproduction mechanism. Magnetic spectrometer, isotopically pure target.
doi: 10.1016/0375-9474(81)90070-1
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