NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = T.Sanami Found 32 matches. 2021KI01 Nucl.Instrum.Methods Phys.Res. A989, 164965 (2021) T.Kim Tuyet, T.Sanami, H.Yamazaki, T.Itoga, A.Takeuchi, Y.Namito, S.Miyamoto, Y.Asano Energy and angular distribution of photo-neutrons for 16.6 MeV polarized photon on medium-heavy targets NUCLEAR REACTIONS Ti, Fe, Cu, Sn, 197Au, Pb(polarized γ, xn), E=16.6 MeV; measured reaction products, En, In; deduced σ(θ, E), σ(θ).
doi: 10.1016/j.nima.2020.164965
2021OY01 Nucl.Instrum.Methods Phys.Res. A990, 164977 (2021) T.Oyama, T.Sanami, H.Yashima, M.Hagiwara, N.Nakao, A.Infantino, E.Iliopoulou, R.Froeschl, S.Roesler, T.Kajimoto, E.Lee, S.Nagaguro, T.Matsumoto, A.Masuda, Y.Uwamino Measurements of secondary-particle emissions from copper target bombarded with 24-GeV/c protons NUCLEAR REACTIONS 27Al, Cu(p, X)24Na, 93Nb(p, X)92Nb, In(p, X)115In, 209Bi(p, X)206Bi/205Bi/204Bi/203Bi/206Po, E=24 GeV; measured reaction products, Eγ, Iγ; deduced σ. Comparison with the EXFOR library.
doi: 10.1016/j.nima.2020.164977
2020SU10 Nucl.Instrum.Methods Phys.Res. B470, 15 (2020) K.Sugihara, N.Shigyo, E.Lee, T.Sanami, K.Tanaka Measurement of thick target neutron yields from 7 MeV/U α incidence on 209Bi NUCLEAR REACTIONS 209Bi(α, n), E=7 MeV/nucleon; measured reaction products, En, In; deduced thick target neutron yields. Comparison with calculations.
doi: 10.1016/j.nimb.2020.02.037
2018HA35 J.Radioanal.Nucl.Chem. 318, 569 (2018) M.Hagiwara, H.Yashima, T.Sanami, S.Yonai Measurement of the excitation function of 96Zr(α, n)99Mo for an alternative production source of medical radioisotopes NUCLEAR REACTIONS 96Zr(α, n), E=11-23 MeV; measured reaction products, Eγ, Iγ; deduced σ, thick target yields. Comparison with experimental data, TENDL-2017 library.
doi: 10.1007/s10967-018-6118-4
2018OY01 Nucl.Instrum.Methods Phys.Res. B434, 29 (2018) T.Oyama, M.Hagiwara, T.Sanami, H.Yashima, N.Nakao, E.J.Lee, E.Iliopoulou, R.Froeschl, A.Infantino, S.Roesler Measurement and calculation of thermal neutrons induced by the 24 GeV/c proton bombardment of a thick copper target NUCLEAR REACTIONS Cu(p, X)1NN, E=24 GeV; measured reaction products, En, In; deduced neutron flux, yield. Comparison with theoretical calculations.
doi: 10.1016/j.nimb.2018.08.016
2016SA44 Nucl.Instrum.Methods Phys.Res. B387, 10 (2016) D.Satoh, T.Kajimoto, N.Shigyo, Y.Itashiki, Y.Imabayashi, Y.Koba, N.Matsufuji, T.Sanami, N.Nakao, Y.Uozumi Distributions of neutron yields and doses around a water phantom bombarded with 290-MeV/nucleon and 430-MeV/nucleon carbon ions NUCLEAR REACTIONS H, O(C, n), E=290, 430 MeV/nucleon; measured reaction products, En, In; deduced neutron yields and doses. Comparison with Monte-Carlo simulation code PHITS.
doi: 10.1016/j.nimb.2016.09.011
2014KA34 Nucl.Instrum.Methods Phys.Res. B337, 68 (2014) T.Kajimoto, N.Shigyo, T.Sanami, Y.Iwamoto, M.Hagiwara, H.S.Lee, A.Soha, E.Ramberg, R.Coleman, D.Jensen, A.Leveling, N.V.Mokhov, D.Boehnlein, K.Vaziri, Y.Sakamoto, K.Ishibashi, H.Nakashima Measurements and parameterization of neutron energy spectra from targets bombarded with 120 GeV protons NUCLEAR REACTIONS C, Al, Cu, W(p, n), E=120 GeV; measured reaction products, En, In; deduced yields. Comparison with PHITS and FLUKA calculations.
doi: 10.1016/j.nimb.2014.07.019
2014SA48 Nucl.Data Sheets 119, 241 (2014) Target Mass Dependency of Light Mass Fragment Energy Spectra for Intermediate Energy Proton Induced Reactions NUCLEAR REACTIONS C, Al, Ti, Cu, Ag(p, x), E=40, 140, 200, 300 MeV; measured charged reaction products at θ=30, 60, 90, 120 using BCC (Bragg curve counter); deduced σ(θ, E) for the Li emission; deduced temperature parameter, normalization parameter, renormalization of fission barrier from the fit of the Maxwellian-type spectra to the data.
doi: 10.1016/j.nds.2014.08.066
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
2011HA61 J.Korean Phys.Soc. 59, 2035s (2011) M.Hagiwara, T.Sanami, K.Masumoto, Y.Iwamoto, N.Matsuda, Y.Sakamoto, Y.Nakane, H.Nakashima, Y.Uwamino Spectrum Measurement of Neutrons and Gamma-Rays from Thick H182O Target Bombarded with 18 MeV Protons NUCLEAR REACTIONS H, 18O(p, n), E=18 MeV; measured thick target En, In(θ), Eγ, Iγ; deduced neutron, γ yields; calculated yields, σ(E, θ) using MCNPX, PHITS, TENDL.
doi: 10.3938/jkps.59.2035
2011KA42 J.Korean Phys.Soc. 59, 2063s (2011) Y.Kasugai, N.Matsuda, Y.Iwamoto, Y.Sakamoto, H.Nakashima, H.Matsumura, N.Kinoshita, H.Iwase, T.Sanami, M.Hagiwara, H.Hirayama, H.Yashima, N.Sigyo, H.Arakawa, K.Ishibashi, N.Mokhov, A.Leveling, D.Boehnlein, K.Vaziri, G.Lauten, S.Wayne, V.Cupps, B.Kershisnik, S.Benesch, T.Nakamura, K.Oishi, K.Niita Shielding Experiments under JASMIN Collaboration at Fermilab (I) Overview of the Research Activities
doi: 10.3938/jkps.59.2063
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
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
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
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
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
2009NA20 Nucl.Technology 168, 482 (2009) H.Nakashima, Y.Sakamoto, Y.Iwamoto, N.Matsuda, Y.Kasugai, Y.Nakane, F.Masukawa, N.V.Mokhov, A.F.Leveling, D.J.Boehnlein, K.Vaziri, T.Sanami, H.Matsumura, M.Hagiwara, H.Iwase, N.Kinoshita, H.Hirayama, K.Oishi, T.Nakamura, H.Arakawa, N.Shigyo, K.Ishibashi, H.Yashima, N.Nakao, K.Niita Experimental Studies of Shielding and Irradiation Effects at High-Energy Accelerator Facilities
doi: 10.13182/NT09-A9229
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
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
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
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
2001MI17 Ann.Nucl.Energy 28, 937 (2001) T.Miura, M.Baba, M.Ibaraki, T.Win, T.Sanami, Y.Hirasawa Measurements of Double-Differential Neutron Emission Cross-Sections of 238U and 232Th for 2.6, 3.6 and 11.8 MeV Neutrons NUCLEAR REACTIONS 238U, 232Th(n, nX), E=2.6, 3.6, 11.8 MeV; measured neutron emission σ(E, θ). Comparison with evaluated data.
doi: 10.1016/S0306-4549(00)00102-X
2000MI04 Ann.Nucl.Energy 27, 625 (2000) T.Miura, M.Baba, M.Ibaraki, T.Sanami, T.Win, Y.Hirasawa, N.Hirakawa Measurement of Neutron Inelastic Scattering Cross-Section for the First Level of 238U in Hundreds of keV Range NUCLEAR REACTIONS 238U(n, n'), E=350-855 keV; measured σ(E, θ). Comparison with data library.
doi: 10.1016/S0306-4549(99)00074-2
2000SA06 Nucl.Instrum.Methods Phys.Res. A440, 403 (2000) T.Sanami, M.Baba, K.Saito, N.Hirakawa (n, α) Cross-Section Measurement using a Gaseous Sample and a Gridded Ionization Chamber NUCLEAR REACTIONS 12C(n, α), E=14.1 MeV; measured σ. Gaseous sample, gridded ionization chamber.
doi: 10.1016/S0168-9002(99)00945-6
1999IW02 J.Nucl.Sci.Technol.(Tokyo) 36, 127 (1999) T.Iwasaki, K.Saito, M.Baba, T.Sanami, Y.Nauchi, N.Hirakawa Measurement of Fast Neutron-Induced Fission Cross Section Ratio of Neptunium-237 Relative to Uranium-235 between 6 and 120 keV NUCLEAR REACTIONS 237Np(n, F), E=6-120 keV; measured fission σ.
doi: 10.1080/18811248.1999.9726190
1999KA20 J.Nucl.Sci.Technol.(Tokyo) 36, 256 (1999) T.Kawano, T.Sanami, M.Baba, H.Nakashima Analysis of 58Ni(n, α) Reaction Cross Sections with the Hauser-Feshbach Statistical Theory and the Bayesian Parameter Estimation Method NUCLEAR REACTIONS 58Ni(n, α), E=2-8 MeV; analyzed σ, σ(E), σ(θ). 58Ni(n, n'), (n, p), E=2-8 MeV; analyzed σ. 58Ni, 58Co, 55Fe deduced level density parameters. Hauser-Feshbach statistical theory, Bayesian parameter estimation method.
doi: 10.1080/18811248.1999.9726206
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. 1999WI12 J.Nucl.Sci.Technol.(Tokyo) 36, 486 (1999) T.Win, M.Baba, M.Ibaraki, T.Miura, T.Sanami, T.Iwasaki, N.Hirakawa Measurement of Prompt Fission Neutron Spectrum of Neptunium-237 for 0.62 MeV Incident Neutrons NUCLEAR REACTIONS 237Np(n, F), E=0.62 MeV; measured prompt fission neutron spectra; deduced Maxwellian distribution parameters. Comparison with evaluated data, previous measurements.
doi: 10.1080/18811248.1999.9726231
1998IB02 J.Nucl.Sci.Technol.(Tokyo) 35, 843 (1998) M.Ibaraki, M.Baba, S.Matsuyama, T.Sanami, T.Win, T.Miura, N.Hirakawa Measurements of Double-Differential Neutron Emission Cross Sections of 6Li, 7Li and 9Be for 11.5 MeV and 18.0 MeV Neutrons NUCLEAR REACTIONS 6,7Li, 9Be(n, nX), E=11.5, 18.0 MeV; measured neutron spectra, σ(En, θ), σ(θ). Comparison with evaluated data sets.
doi: 10.1080/18811248.1998.9733956
1998SA65 J.Nucl.Sci.Technol.(Tokyo) 35, 851 (1998) T.Sanami, M.Baba, T.Kawano, S.Matsuyama, T.Kiyosumi, Y.Nauchi, K.Saito, N.Hirakawa High Resolution Measurements of Double Differential (n, α) Cross Sections of 58Ni and natNi between 4.2 and 6.5 MeV Neutrons NUCLEAR REACTIONS 58Ni, Ni(n, α), E=4.2-6.5 MeV; measured σ(Eα, θ). Comparison with theory.
doi: 10.1080/18811248.1998.9733957
1997SA68 Nucl.Instrum.Methods Phys.Res. A394, 368 (1997) T.Sanami, M.Baba, I.Matsuyama, S.Matsuyama, T.Kiyosumi, Y.Nauchi, N.Hirakawa Measurement of 14N(n, p)14C Cross Section for kT = 25.3 keV Maxwellian Neutrons using Gridded Ionization Chamber NUCLEAR REACTIONS 14N(n, p), E ≈ 25 keV; measured σ. Maxwellian neutron energy distribution. Implications for astrophysical s-process discussed.
doi: 10.1016/S0168-9002(97)00698-0
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
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