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NSR database version of May 24, 2024.

Search: Author = M.Takada

Found 18 matches.

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2021KA03      Nucl.Instrum.Methods Phys.Res. B487, 38 (2021)

T.Kajimoto, K.Tanaka, S.Endo, S.Kamada, H.Tanaka, M.Takada, T.Hamano

Double differential cross sections of neutron production by 135 and 180 MeV protons on A-150 tissue-equivalent plastic

NUCLEAR REACTIONS C, O(p, n), E=135, 180 MeV; measured reaction products, Eγ, Iγ, En, In; deduced neutron production σ(θ, E) using PHITS, FLUKA, and Geant4 codes.

doi: 10.1016/j.nimb.2020.11.014
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2695.

2014SH20      Nucl.Data Sheets 119, 303 (2014)

N.Shigyo, U.Uozumi, H.Uehara, T.Nishizawa, T.Mizuno, M.Takamiya, T.Hashiguchi, D.Satoh, T.Sanami, Y.Koba, M.Takada, N.Matsufuji

Measurement of 100- and 290-MeV/A Carbon Incident Neutron Production Cross Sections for Carbon, Nitrogen and Oxygen

NUCLEAR REACTIONS C, N, O(12C, n), E=100, 290 MeV/nucleon; measured En, In(θ) using NE213; deduced σ(θ, E); calculated σ(θ, E) using PHITS. Only carbon results shown.

doi: 10.1016/j.nds.2014.08.083
Citations: PlumX Metrics

2011KO02      J.Nucl.Sci.Technol.(Tokyo) 48, 227 (2011)

K.Kosako, K.Oishi, T.Nakamura, M.Takada, K.Sato, T.Kamiyama, Y.Kiyanagi

Angular Distribution of Photoneutrons from Copper and Tungsten Targets Bombarded by 18, 28, and 38 MeV Electrons

NUCLEAR REACTIONS Cu, W(γ, n), E=18, 28, 38 MeV; measured reaction activation products, Eγ, Iγ; deduced photoneutron σ(E), σ(θ). Comparison with experimental data, MCNP5 and JENDL-3.3 library.

doi: 10.3327/jnst.48.227
Citations: PlumX Metrics

2011MO29      J.Korean Phys.Soc. 59, 1789s (2011)

D.Moriguchi, Y.Nakamura, T.Kajimoto, Y.Koba, M.Ueyama, M.Yoshioka, N.Shigyo, Y.Uozumi, D.Satoh, T.Sanami, M.Takada, N.Matsufuji

Measurement of Neutron-Production Cross Sections for 290 MeV/u Carbon Ion Incidence

NUCLEAR REACTIONS 12C(12C, n), E=290 MeV/nucleon; measured En, In(θ) using NE213; deduced σ(En, θ); calculated σ(En, θ) using PHITS, SCINFUL-QMD.

doi: 10.3938/jkps.59.1789
Citations: PlumX Metrics

2011SA22      Nucl.Instrum.Methods Phys.Res. A644, 59 (2011)

D.Satoh, D.Moriguchi, T.Kajimoto, H.Uehara, N.Shigyo, M.Ueyama, M.Yoshioka, Y.Uozumi, T.Sanami, Y.Koba, M.Takada, N.Matsufuji

Measurement of neutron-production double-differential cross-sections on carbon bombarded with 290-MeV/nucleon carbon and oxygen ions

NUCLEAR REACTIONS C(C, xn), (O, xn), E=290 MeV/nucleon; measured reaction products, neutron TOF; deduced σ(θ, E). Comparison with Monte-Carlo simulation and experimental data.

doi: 10.1016/j.nima.2011.04.054
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2341.

2011SA62      J.Korean Phys.Soc. 59, 1741s (2011)

D.Satoh, D.Moriguchi, T.Kajimoto, Y.Koba, Y.Nakamura, N.Shigyo, M.Ueyama, Y.Uozumi, M.Yoshioka, N.Matsufuji, M.Takada, T.Sanami

Neutron-Production Double-Differential Cross Sections from Heavy-Ion Interactions

COMPILATION Al, Cu(α, nx), E=230 MeV/nucleon;C, Cu, Pb(C, nx), E=290, 400 MeV/nucleon;C, Cu(N, nx), E=400 MeV/nucleon;C, Cu, Pb(Ne, nx), E=400, 600 MeV/nucleon;C, Cu, Pb(Ar, nx), E=400, 560 MeV/nucleon;C, Cu, Pb(Kr, nx), (Xe, nx), E=400 MeV/nucleon; re-analyzed σ(E, θ) using new set on neutron-detection efficiency of NE-213 calculated with SCINFUL-QMD; calculated σ(E, θ) using PHITS, FLUKA, MCNPX, GEANT4.

doi: 10.3938/jkps.59.1741
Citations: PlumX Metrics

2011SA64      J.Korean Phys.Soc. 59, 1805s (2011)

T.Sanami, M.Hagiwara, H.Iwase, M.Takada, D.Satoh, Y.Iwamoto, S.Kunieda, H.Yashima, A.Tamii, M.Baba

Fragment DDX Measurement of Proton Induced Reactions on Light-Medium Nuclei for Energy Range from Reaction Threshold to a Few Hundred MeV

NUCLEAR REACTIONS C(p, Li), E=40, 50, 70, 80 MeV;N, O(p, Li), (p, Be), (p, B), (p, C), E=70 MeV; measured charged ejectiles using BCC (Bragg curve counter); deduced σ(E, θ); Calculated σ(E, θ) using PHITS code with three different INC models (also at higher incident energies than are the measured data).

doi: 10.3938/jkps.59.1805
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2339.

2011YO14      J.Korean Phys.Soc. 59, 1971s (2011)

M.Yoshioka, M.Ueyama, Y.Koba, Y.Nakamura, T.Kajimoto, D.Moriguchi, Y.Uozumi, N.Shigyo, D.Sato, T.Sanami, M.Takada

Study of Pulse Shape Discrimination of Sub-MeV Neutrons From Gamma-Rays with Liquid Scintillator

doi: 10.3938/jkps.59.1971
Citations: PlumX Metrics

2010TA14      J.Nucl.Sci.Technol.(Tokyo) 47, 932 (2010)

M.Takada, K.Yajima, H.Yasuda, T.Sato, T.Nakamura

Measurement of Atmospheric Neutron and Photon Energy Spectra at Aviation Altitudes using a Phoswich-Type Neutron Detector

doi: 10.1080/18811248.2010.9720972
Citations: PlumX Metrics

2008HA19      Nucl.Instrum.Methods Phys.Res. A592, 73 (2008)

M.Hagiwara, T.Sanami, T.Oishi, M.Baba, M.Takada

Extension of energy acceptance of Bragg curve counter at the high-energy end

NUCLEAR REACTIONS C(p, X)6Li/7Li/7Be, E=70 MeV; measured E, double differential σ; Bragg curve counter; Energy loss.

doi: 10.1016/j.nima.2008.03.108
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2110.

2008SA46      Nucl.Instrum.Methods Phys.Res. A 589, 193 (2008)

T.Sanami, M.Hagiwara, T.Oishi, M.Baba, M.Takada

A Bragg curve counter with an active cathode to improve the energy threshold in fragment measurements

NUCLEAR REACTIONS C(p, x), E=70 MeV; measured products, -1B, -1C; deduced σ(θ, E). Data were imported from EXFOR entry E2106.

doi: 10.1016/j.nima.2008.02.015
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2106.

2007SA56      Nucl.Instrum.Methods Phys.Res. A583, 507 (2007)

D.Satoh, T.Kurosawa, T.Sato, A.Endo, M.Takada, H.Iwase, T.Nakamura, K.Niita

Reevaluation of secondary neutron spectra from thick targets upon heavy-ion bombardment

NUCLEAR REACTIONS C, Al, Cu, Pb(C, X), E=400 MeV/nucleon; C, Cu(Si, X), E=800 MeV/nucleon; C, Al, Cu, Pb(Fe, X), E=400 MeV/nucleon; C, Al, Cu, Pb(Xe, X), E=400 MeV/nucleon; analyzed experimental data of secondary neutron spectra, comparisons with calculations using Monte-Carlo heavy-ion transport code PHITS.

doi: 10.1016/j.nima.2007-09-023
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2079.

2005MB11      Radiochim.Acta 93, 497 (2005)

H.Matsumura, T.Sanami, K.Masumoto, N.Nakao, A.Toyoda, M.Kawai, T.Aze, H.Nagai, M.Takada, H.Matsuzaki

Target dependence of beryllium fragment production in neutron- and alpha-induced nuclear reactions at intermediate energies

NUCLEAR REACTIONS C, 27Al, Cu, Ag, 197Au(α, X)7Be, E=400 MeV; Cu, Ag, 197Au(α, X)10Be, E=400 MeV; C, 27Al, Cu, Ag, 197Au(n, X)7Be, E < 500 MeV; Cu, Ag, 197Au(n, X)10Be, E < 500 MeV; measured yields. Comparison with photonuclear data.

doi: 10.1524/ract.2005.93.9-10.497
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22911.

2005TA17      Nucl.Instrum.Methods Phys.Res. A545, 765 (2005)

M.Takada, E.Mihara, T.Nakamura, T.Honma, K.Kono, K.Fujitaka

Neutron irradiation field produced by 25 MeV deuterons bombarding on thick beryllium target for radiobiological study

NUCLEAR REACTIONS 9Be(d, nX), E=25 MeV; measured En, Eγ, thick-target yield. Irradiation field for biological studies.

doi: 10.1016/j.nima.2005.02.028
Citations: PlumX Metrics

2001TA17      Nucl.Instrum.Methods Phys.Res. A465, 512 (2001)

M.Takada, S.Taniguchi, T.Nakamura, K.Fujitaka

Neutron Spectrometry in a Mixed Field of Neutrons and Protons with a Phoswich Neutron Detector Part II: Application of the phoswich neutron detector to neutron spectrum measurements

NUCLEAR REACTIONS 9Be(p, nX), (p, pX), E=70 MeV; measured En, Ep. C(12C, X), E=100 MeV/nucleon; measured fragment spectra.

doi: 10.1016/S0168-9002(01)00614-3
Citations: PlumX Metrics

1999NA02      Nucl.Instrum.Methods Phys.Res. A420, 218 (1999)

N.Nako, Y.Uwamino, T.Nakamura, T.Shibata, N.Nakanishi, M.Takada, E.Kim, T.Kurosawa

Development of a Quasi-Monoenergetic Neutron Field using the 7Li(p, n)7Be Reaction in the 70-210 MeV Energy Range at RIKEN

NUCLEAR REACTIONS 7Li(p, n), E=70-210 MeV; measured neutron spectra. Quasi-monoenergetic neutron field. Liquid scintillator, TOF.

doi: 10.1016/S0168-9002(98)01146-2
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2298.

1996BB13      Nucl.Instrum.Methods Phys.Res. A376, 115 (1996)

M.Baba, M.Takada, T.Iwasaki, S.Matsuyama, T.Nakamura, H.Ohguchi, T.Nakao, T.Sanami, N.Hirakawa

Development of Monoenergetic Neutron Calibration Fields between 8 keV and 15 MeV

NUCLEAR REACTIONS 45Sc, 7Li, 2,3H(p, n), E ≤ 4.5 MeV; measured energy spectra. Tof technique, monoenergetic neutron calibration fields development.

doi: 10.1016/0168-9002(96)00190-8
Citations: PlumX Metrics

1996TA23      Nucl.Instrum.Methods Phys.Res. A372, 253 (1996)

M.Takada, T.Nakamura, M.Baba, T.Iwasaki, T.Kiyosumi

Characterization of 22 and 33 MeV Quasi-Monoenergetic Neutron Fields for Detector Calibration at CYRIC

NUCLEAR REACTIONS 7Li(p, n), E=25, 35 MeV; measured neutron spectra, absolute fluence; deduced quasi-monoenergetic neutron fields, E=22, 33 MeV. Proton recoil telescope, Li target activation method, tof with liquid scintillator.

doi: 10.1016/0168-9002(95)01247-8
Citations: PlumX Metrics

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