NSR Query Results


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NSR database version of May 21, 2024.

Search: Author = T.Kato

Found 19 matches.

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2019BU30      Sci. Rep. 9, 6157 (2019)

D.J.Buglewicz, A.B.Banks, H.Hirakawa, A.Fujimori, T.A.Kato

Monoenergetic 290 MeV/n carbon-ion beam biological lethal dose distribution surrounding the Bragg peak

doi: 10.1038/s41598-019-42600-4
Citations: PlumX Metrics


2012KA31      Prog.Theor.Phys.(Kyoto), Suppl. 196, 16 (2012)

T.Kato, T.Oyamada, H.Kono, S.Koseki

Time-Dependent Multiconfiguration Theory and Its Application to Ultrafast Electronic Dynamics of Molecules in an Intense Laser Field

doi: 10.1143/PTPS.196.16
Citations: PlumX Metrics


2008DI02      Chinese Physics B 17, 592 (2008)

X.-B.Ding, C.-Z.Dong, F.Koike, T.Kato, S.Fritzsche

Excitation and decay dynamics of 1s2s inner-shell double-vacancy states of neon atoms

doi: 10.1088/1674-1056/17/2/039
Citations: PlumX Metrics


2008MU03      At.Data Nucl.Data Tables 94, 161 (2008)

I.Murakami, J.Yan, H.Sato, M.Kimura, R.K.Janev, T.Kato

Excitation, ionization, and electron capture cross sections for collisions of Li3+ with ground state and excited hydrogen atoms

doi: 10.1016/j.adt.2007.10.002
Citations: PlumX Metrics


2004FA06      Phys.Rev. C 69, 034613 (2004)

D.Q.Fang, T.Yamaguchi, T.Zheng, A.Ozawa, M.Chiba, R.Kanungo, T.Kato, K.Morimoto, T.Ohnishi, T.Suda, Y.Yamaguchi, A.Yoshida, K.Yoshida, I.Tanihata

One-neutron halo structure 15C

NUCLEAR REACTIONS C(14C, X), E=83 MeV/nucleon; C(15C, X), E=51, 83 MeV/nucleon; measured reaction σ. C(15C, 14CX), (15C, 13CX), (14C, 13CX), E=83 MeV/nucleon; measured fragment longitudinal momentum distributions. 15C deduced matter density distribution, halo structure.

doi: 10.1103/PhysRevC.69.034613
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1889.


2004YA16      Nucl.Phys. A734, E73 (2004)

T.Yamaguchi, T.Zheng, A.Ozawa, M.Chiba, R.Kanungo, T.Kato, K.Morimoto, T.Ohnishi, T.Suda, Y.Yamaguchi, A.Yoshida, K.Yoshida, I.Tanihata

Neutron configuration of 16C studied via one- and two-neutron removal momentum distributions

NUCLEAR REACTIONS C(16C, 15CX), (16C, 14CX), E=83 MeV/nucleon; measured fragments longitudinal momentum distributions. C(16C, X), E=83 MeV/nucleon; measured reaction σ; deduced halo effects.

doi: 10.1016/j.nuclphysa.2004.03.023
Citations: PlumX Metrics


2003KH11      Nucl.Phys. A722, 484c (2003)

L.H.Khiem, T.Kato, K.Morimoto, M.Notani, A.Ozawa, R.Kanungo, I.Tanihata, A.Yoshida

Production of neutron-rich isotopes by fragmentation of 80 MeV/nucleon 59Co beam

NUCLEAR REACTIONS Be(59Co, X), E=80 MeV/nucleon; measured fragment isotopic production σ. Comparison with model predictions.

doi: 10.1016/S0375-9474(03)01413-1
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2143.


2003KH15      Nucl.Phys. A722, C484 (2003)

L.-H.Khiem, T.Kato, K.Morimoto, M.Notani, A.Ozawa, R.Kanungo, I.Tanihata, A.Yoshida

Production of neutron-rich isotopes by fragmentation of 80 MeV/nucleon 59Co beam

NUCLEAR REACTIONS 9Be(59Co, x), E=4.7 GeV; measured products, 54Ti, 53Ti, 52Ti, 51Ti, 50Ti, 52Sc, 51Sc, 50Sc, 49Sc, 48Sc, 47Sc, 50Ca, 49Ca, 48Ca, 47Ca, 46Ca, 45Ca, 49K, 48K, 47K, 46K, 45K, 44K, 43K, 42K, 46Ar, 45Ar, 44Ar, 43Ar, 42Ar, 41Ar, 40Ar, 43Cl, 42Cl, 41Cl, 40Cl, 39Cl, 38Cl, 37Cl, 40S, 39S, 38S, 37S, 36S, 35S, 34S, 38P, 37P, 36P, 35P, 34P, 33P, 32P, 37Si, 36Si, 35Si, 34Si, 33Si, 32Si, 31Si, 35Al, 34Al, 33Al, 32Al, 31Al, 30Al, 29Al, 32Mg, 31Mg, 30Mg, 29Mg, 28Mg, 27Mg, 26Mg, 31Na, 30Na, 29Na, 28Na, 27Na, 26Na, 25Na, 24Na; deduced σ, σ(E). Data were imported from EXFOR entry E2143.

doi: 10.1016/S0375-9474(03)01413-1
Citations: PlumX Metrics


2003YA08      Nucl.Phys. A724, 3 (2003)

T.Yamaguchi, T.Zheng, A.Ozawa, M.Chiba, R.Kanungo, T.Kato, K.Morimoto, T.Ohnishi, T.Suda, Y.Yamaguchi, A.Yoshida, K.Yoshida, I.Tanihata

Momentum distributions of 14C and 15C fragments from 16C breakup

NUCLEAR REACTIONS C(16C, 15CX), (16C, 14CX), E=83 MeV/nucleon; measured carbon fragments longitudinal momentum distributions, neutron removal σ. 16C deduced spectroscopic factor. Few-body Glauber model analysis.

doi: 10.1016/S0375-9474(03)01451-9
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1827.


2002KA18      Nucl.Instrum.Methods Phys.Res. A480, 571 (2002)

T.Kato, T.Kurosawa, T.Nakamura

Systematic Analysis of Neutron Yields from Thick Targets Bombarded by Heavy Ions and Protons with Moving Source Model

NUCLEAR REACTIONS C, Al, Cu, Pb(α, nX), (C, nX), (Ne, nX), (Ar, nX), (Fe, nX), (Xe, nX), E=100-400 MeV/nucleon; analyzed thick-target neutron yields; deduced parameters. Moving source model.

doi: 10.1016/S0168-9002(01)00949-4
Citations: PlumX Metrics


2002OZ03      Nucl.Phys. A709, 60 (2002); Erratum Nucl.Phys. A727, 465 (2003)

A.Ozawa, T.Baumann, L.Chulkov, D.Cortina, U.Datta, J.Fernandez, H.Geissel, F.Hammache, K.Itahashi, M.Ivanov, R.Janik, T.Kato, K.Kimura, T.Kobayashi, K.Markenroth, M.Meister, G.Munzenberg, T.Ohtsubo, S.Ohya, T.Okuda, A.A.Ogloblin, V.Pribora, M.Sekiguchi, B.Sitar, P.Strmen, S.Sugimoto, K.Summerer, T.Suzuki, I.Tanihata, Y.Yamaguchi

Measurements of the Interaction Cross Sections for Ar and Cl Isotopes

NUCLEAR REACTIONS C(31Ar, X), (32Ar, X), (33Ar, X), (34Ar, X), (35Ar, X), (36Ar, X), (37Ar, X), (38Ar, X), (39Ar, X), (40Ar, X), (31Cl, X), (32Cl, X), (33Cl, X), (34Cl, X), (35Cl, X), (36Cl, X), (37Cl, X), E ≈ 950 MeV/nucleon; measured interaction and inelastic σ.31,32,33,34,35,36,37,38,39,40Ar, 31,32,33,34,35,36,37Cl deduced effective radii. 32,33,34,35,36,37,38,39,40Ar deduced proton skin features.

doi: 10.1016/S0375-9474(02)01071-0
Citations: PlumX Metrics


2002ZH33      Nucl.Phys. A709, 103 (2002)

T.Zheng, T.Yamaguchi, A.Ozawa, M.Chiba, R.Kanungo, T.Kato, K.Katori, K.Morimoto, T.Ohnishi, T.Suda, I.Tanihata, Y.Yamaguchi, A.Yoshida, K.Yoshida, H.Toki, N.Nakajima

Study of Halo Structure of 16C from Reaction Cross Section Measurement

NUCLEAR REACTIONS C(12C, X), (16C, X), E=83 MeV/nucleon; measured reaction σ; deduced effective range parameter. 16C deduced neutron density distribution, halo features. Finite-range Glauber model.

doi: 10.1016/S0375-9474(02)01043-6
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1791.


2000UN01      J.Nucl.Sci.Technol.(Tokyo) 37, 627 (2000)

H.Unesaki, T.Iwasaki, T.Kitada, A.Kohashi, D.Fujiwara, M.Kuroda, T.Kato, Y.Ikeuchi, S.Shiroya

Measurement of 237Np Fission Rate Ratio Relative to 235U Fission Rate in Cores with Various Thermal Neutron Spectrum at the Kyoto University Critical Assembly

NUCLEAR REACTIONS 237Np(n, F), E=reactor; measured neutron spectra, fission rates.

doi: 10.3327/jnst.37.627
Citations: PlumX Metrics


1997MA73      Chem.Phys.Lett. 273, 291 (1997)

M.Matsushita, T.Kato

Nuclear Quadrupole Resonance of 139La Around Pr3+ Doped in LaF3. Raman Heterodyne Detection using Optical Transition of Pr3+ Ions

NUCLEAR MOMENTS 139La; measured NQR; deduced Pr-La interaction in Pr-doped LaF3, impurity local environment features.

doi: 10.1016/S0009-2614(97)00565-4
Citations: PlumX Metrics


1997SA64      Nucl.Instrum.Methods Phys.Res. A384, 435 (1997)

M.Satoh, T.Doke, T.Kato, J.Kikuchi, M.Kobayashi, K.Masuda, H.Okada

Attenuation Length of Drifting Electrons in Allene-Doped Liquid Argon

doi: 10.1016/S0168-9002(96)00870-4
Citations: PlumX Metrics


1992KA11      Nucl.Instrum.Methods Phys.Res. A311, 548 (1992)

T.Kato, T.Nakamura

Estimation of Neutron Yields from Thick Targets by High Energy 4He Ions for the Design of Shielding for a Heavy Ion Medical Accelerator

NUCLEAR REACTIONS 63,65Cu, 9Be(α, xn), E=high; measured neutron yields, σ(θ). Thick targets. Intranuclear cascade model.

doi: 10.1016/0168-9002(92)90653-L
Citations: PlumX Metrics


1992MO20      Z.Phys. A343, 373 (1992)

T.Morikawa, H.Inoue, Y.Iwata, T.Matsuoka, Y.Yoshizawa, T.Kato, S.Mitarai, J.Mukai, D.Jerrestam

Coulomb Excitation of 154Sm

NUCLEAR REACTIONS 154Sm(58Ni, 58Ni'), E=220 MeV; measured γγ-, (particle)γ-, (particle)γγ-coin, Iγ(θ) following Coulomb excitation. 154Sm deduced levels, J, π, band structure, new band excitation probability.

doi: 10.1007/BF01291541
Citations: PlumX Metrics


1978MA46      Nucl.Instrum.Methods 157, 567 (1978)

K.Masumoto, T.Kato, N.Suzuki

Activation Yield Curves of Photonuclear Reactions for Multielement Photon Activation Analysis

NUCLEAR REACTIONS 12C, 23Na, 48Ca, 52Cr, 55Mn, 89Y, 90Zr, 93Nb, 100Mo, 198,204Hg, 204Pb, 203Tl(γ, n), 25Mg, 48,49Ti, 56Fe, 96,97Mo, 199Hg(γ, p), 50Cr, 54,56Fe, 90Zr, 94Mo(γ, np), 12C, 27Al, 51V, 56Fe, 93Nb, 94Mo(γ, αn), 51V(γ, α), 50Cr, 54Fe, 92Mo, 204Pb, 203Tl(γ, 2n), 204Pb, 203Tl(γ, 3n), E=30-70 MeV bremsstrahlung; measured activation σ(E).

doi: 10.1016/0029-554X(78)90019-8
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2630.


1974KA01      J.Inorg.Nucl.Chem. 36, 1 (1974)

T.Kato, H.-T.Tsai

The Yield Distribution of Radioactive Nuclides Produced by Photospallation Reactions in 133Cs and 139La with 250 MeV Bremsstrahlung

NUCLEAR REACTIONS 133Cs, 139La(γ, xnyp), E=250 MeV; measured yields.

doi: 10.1016/0022-1902(74)80648-2
Citations: PlumX Metrics


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Note: The following list of authors and aliases matches the search parameter T.Kato: , T.A.KATO