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NSR database version of April 26, 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.^{31,32,33,34,35,36,37,38,39,40}Ar, ^{31,32,33,34,35,36,37}Cl deduced effective radii. ^{32,33,34,35,36,37,38,39,40}Ar 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

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