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NSR database version of April 25, 2024.

Search: Author = Y.Uwamino

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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
Citations: PlumX Metrics

2018NA09      Nucl.Instrum.Methods Phys.Res. B423, 27 (2018)

N.Nakao, Y.Uwamino, K.Tanaka

Measurement of the neutron angular distribution from a beryllium target bombarded with a 345-MeV/u ²³⁸U beam at the RIKEN RI beam factory

NUCLEAR REACTIONS ⁹Be(²³⁸U, X)¹NN, E=345 MeV/nucleon; measured reaction products, En, In; deduced σ(θ).

NUCLEAR REACTIONS ²⁰⁹Bi(n, xn)¹⁹⁸Bi/¹⁹⁹Bi/²⁰⁰Bi/²⁰¹Bi/²⁰²Bi/²⁰³Bi/²⁰⁴Bi/²⁰⁵Bi/²⁰⁶Bi, ²⁷Al(n, α), E<1 GeV; measured reaction products, Eγ, Iγ; deduced the production rates. Comparison with calculations using the Particle and Heavy Ion Transport code System (PHITS), a Monte Carlo simulation.

doi: 10.1016/j.nimb.2018.02.036
Citations: PlumX Metrics

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
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2340.

2008TA23      Appl.Radiat.Isot. 66, 1321 (2008)

K.Takamiya, Y.Ota, M.Akamine, S.Shibata, T.Shibata, Y.Ito, M.Imamura, Y.Uwamino, N.Nogawa, M.Baba, S.Iwasaki, S.Matsuyama

Excitation function for ⁶³Cu(n, p)⁶³Ni reaction in neutron energy range up to 15 MeV

NUCLEAR REACTIONS ⁶³Cu(n, p), E< 14.9 MeV; measured Εβ, Iβ, σ(E);radiochemical separation; liquid scintillation counting; comparison with JENDL-3.3, ENDF/B-VI and FENDL/A-2.0.

doi: 10.1016/j.apradiso.2008.03.011
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset23033.

2006IW01      Nucl.Instrum.Methods Phys.Res. A562, 789 (2006)

Y.Iwamoto, S.Taniguchi, N.Nakao, T.Itoga, T.Nakamura, Y.Nakane, H.Nakashima, D.Satoh, H.Yashima, H.Yamakawa, K.Oishi, Y.Uwamino, A.Tamii, K.Hatanaka, M.Baba

Measurement of neutron spectra produced in the forward direction from thick graphite, Al, Fe and Pb targets bombarded by 350 MeV protons

NUCLEAR REACTIONS C, Al, Fe, Pb(p, nX), E=350 MeV; measured neutron spectra.

doi: 10.1016/j.nima.2006.02.056
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1989.

2004YA25      Nucl.Instrum.Methods Phys.Res. B226, 243 (2004)

H.Yashima, Y.Uwamino, H.Iwase, H.Sugita, T.Nakamura, S.Ito, A.Fukumura

Cross sections for the production of residual nuclides by high-energy heavy ions

NUCLEAR REACTIONS C, Al, Cr, Fe, Cu(Ne, X), (C, X), (Ar, X), E=400 MeV/nucleon; Al, Cr, Fe, Cu(Si, X), E=800 MeV/nucleon; Cr, Fe(Ne, X), (C, X), (He, X), (p, X), E=100 MeV/nucleon; Cr, Fe(Ar, X), (Ne, X), (He, X), (p, X), E=230 MeV/nucleon; measured spallation product yields, production σ. Activation technique.

doi: 10.1016/j.nimb.2004.06.025
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1923.

2003YA20      Radiochim.Acta 91, 689 (2003)

H.Yashima, Y.Uwamino, H.Iwase, H.Sugita, T.Nakamura, S.Ito, A.Fukumura

Measurement and calculation of radioactivities of spallation products by high-energy heavy ions

NUCLEAR REACTIONS Cu(p, X), (α, X), (¹²C, X), (²⁰Ne, X), (⁴⁰Ar, X)⁷Be/²²Na/²⁴Na/²⁷Mg/²⁸Mg/²⁹Al/^34mCl/³⁸Cl/³⁹Cl/⁴¹Ar/⁴²K/⁴³K/⁴³Sc/⁴⁴Sc/^44mSc/⁴⁶Sc/⁴⁷Sc/⁴⁸Sc/⁴⁸Cr/⁴⁹Cr/⁵¹Cr/⁵⁴Mn/⁵⁶Mn/⁵²Fe/⁵⁹Fe/⁵⁵Co/⁵⁶Co/⁵⁷Co/⁵⁸Co/⁶⁰Co/⁶¹Co/^62mCo/⁵⁷Ni/⁶⁵Ni/⁶⁰Cu/⁶¹Cu/⁶⁴Cu/⁶²Zn/⁶³Zn/⁶⁵Zn, E=100, 230 MeV/nucleon; measured production σ. Activation technique.

doi: 10.1524/ract.91.12.689.23423
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1829.

2003YO10      Nucl.Instrum.Methods Phys.Res. A515, 733 (2003)

S.Yonai, T.Kurosawa, H.Iwase, H.Yashima, Y.Uwamino, T.Nakamura

Measurement of neutron from thick Fe target bombarded by 210 MeV protons

NUCLEAR REACTIONS Fe(p, nX), E=210 MeV; measured neutron spectra, angular distributions, thick target yields.

doi: 10.1016/j.nima.2003.07.007
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1858.

2002YA16      Phys.Rev. C66, 044607 (2002)

H.Yashima, Y.Uwamino, H.Sugita, T.Nakamura, S.Ito, A.Fukumura

Projectile dependence of radioactive spallation products induced in copper by high-energy heavy ions

NUCLEAR REACTIONS Cu(p, X), (α, X), (¹²C, X), (²⁰Ne, X), E=100, 230 MeV/nucleon; measured fragment isotopic yields in thick target, mass and charge distributions. Cu(p, X)²²Na/⁴⁶Sc/⁵¹Cr/⁵⁷Co/⁶¹Cu, E ≈ 25-230 MeV; Cu(α, X), (¹²C, X)²²Na/²⁴Na/³⁸Cl, E ≈ 25-230 MeV; Cu(²⁰Ne, X)²²Na/²⁴Na/³⁸Cl/⁴⁶Sc, E ≈ 25-230 MeV; deduced excitation functions. Comparison with previous results, model predictions.

doi: 10.1103/PhysRevC.66.044607
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1003.

2001SA49      Phys.Rev. C64, 034607 (2001)

H.Sato, T.Kurosawa, H.Iwase, T.Nakamura, Y.Uwamino, N.Nakao

Measurement of Double Differential Neutron Production Cross Sections by 135 MeV/nucleon He, C, Ne and 95 MeV/nucleon Ar Ions

NUCLEAR REACTIONS C, Al, Cu, Pb(α, nX), (C, nX), (Ne, nX), E=135 MeV/nucleon; C, Al, Cu, Pb(Ar, nX), E=95 MeV/nucleon; measured neutron spectra, σ(E, θ), total neutron production σ. Comparisons with model predictions.

doi: 10.1103/PhysRevC.64.034607
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1750.

2000KU29      Phys.Rev. C62, 044615 (2000)

T.Kurosawa, N.Nakao, T.Nakamura, H.Iwase, H.Sato, Y.Uwamino, A.Fukumura

Neutron Yields from Thick C, Al, Cu, and Pb Targets Bombarded by 400 MeV/nucleon Ar, Fe, Xe and 800 MeV/nucleon Si Ions

NUCLEAR REACTIONS C, ²⁷Al, Cu, Pb(Ar, nX), (Fe, nX), (Xe, nX), E=400 MeV/nucleon; C, Cu(Si, nX), E=800 MeV/nucleon; measured neutron spectra, angular distribution, thick target yields. Moving source model analysis, Monte Carlo collision calculations.

doi: 10.1103/PhysRevC.62.044615
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1756.

1999KI30      J.Nucl.Sci.Technol.(Tokyo) 36, 29 (1999)

E.J.Kim, T.Nakamura, Y.Uwamino, N.Nakanishi, M.Imamura, N.Nakao, S.Shibata, S.Tanaka

Measurements of Activation Cross Sections on Spallation Reactions for ⁵⁹Co and ^natCu at Incident Neutron Energies of 40 to 120 MeV

NUCLEAR REACTIONS ⁵⁹Co(n, X)⁵⁶Mn/⁵⁴Mn/⁵²Mn/⁵⁸Co/⁵⁷Co/⁵⁶Co/⁵⁵Co/⁵⁹Fe, E ≈ 45-75 MeV; Cu(n, X)⁵⁶Mn/⁵⁹Fe/⁶⁰Co/⁵⁸Co/⁵⁷Co/⁵⁶Co/⁶⁴Cu/⁶¹Cu/⁶⁰Cu, E ≈ 45-117 MeV; measured activation σ. Comparison with previous results, model predictions.

doi: 10.1080/18811248.1999.9726179
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22421.

1999KU22      Nucl.Instrum.Methods Phys.Res. A430, 400 (1999)

T.Kurosawa, T.Nakamura, N.Nakao, T.Shibata, Y.Uwamino, A.Fukumura

Spectral Measurements of Neutrons, Protons, Deuterons and Tritons Produced by 100 MeV/nucleon He Bombardment

NUCLEAR REACTIONS C, ²⁷Al, Cu, Pb(α, X), E=100 MeV/nucleon; measured neutron spectra, proton spectra, deuteron, triton spectra, angular distributions. Thick targets. Comparison with Monte Carlo calculations.

doi: 10.1016/S0168-9002(99)00227-2
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1809.

1999KU37      J.Nucl.Sci.Technol.(Tokyo) 36, 41 (1999)

T.Kurosawa, N.Nakao, T.Nakamura, Y.Uwamino, T.Shibata, A.Fukumura, K.Murakami

Measurements of Secondary Neutrons Produced from Thick Targets Bombarded by High Energy Neon Ions

NUCLEAR REACTIONS C, Al, Cu, Pb(Ne, nX), E=100, 180, 400 MeV/nucleon; measured neutron spectra, angular distributions, thick-target yields. Comparison with model predictions.

doi: 10.1080/18811248.1999.9726180
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1759.

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.

1998KI21      Nucl.Sci.Eng. 129, 209 (1998)

E.Kim, T.Nakamura, A.Konno, Y.Uwamino, N.Nakanishi, M.Imamura, N.Nakao, S.Shibata, S.Tanaka

Measurements of Neutron Spallation Cross Sections of ¹²C and ²⁰⁹Bi in the 20- to 150-MeV Energy Range

NUCLEAR REACTIONS ¹²C(n, 2n), E=20-150 MeV; ²⁰⁹Bi(n, xn)²⁰⁷Bi/²⁰⁶Bi/²⁰⁵Bi/²⁰⁴Bi/²⁰³Bi/²⁰²Bi/²⁰¹Bi/²⁰⁰Bi/¹⁹⁹Bi/¹⁹⁸Bi, E=20-150 MeV; measured σ. Activation method.

doi: 10.13182/NSE98-A1977
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22653.

1997UW01      Nucl.Instrum.Methods Phys.Res. A389, 463 (1997)

Y.Uwamino, T.S.Soewarsono, H.Sugita, Y.Uno, T.Nakamura, T.Shibata, M.Imamura, S.-I.Shibata

High-Energy p-Li Neutron Field for Activation Experiment

NUCLEAR REACTIONS ⁷Li(p, n), E=20-40 MeV; measured neutron σ(En, θ). ¹⁹⁷Au(n, 2n), E=8-38 MeV; ¹⁹⁷Au(n, 4n), E=24-38 MeV; ⁵⁹Co(n, 2nα), E=28-38 MeV; measured activation σ.

doi: 10.1016/S0168-9002(97)00345-8
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1826.

1996SH29      Radiochim.Acta 75, 1 (1996)

S.Shibata, T.Shibata, M.Imamura, T.Ohkubo, S.Satoh, Y.Uwamino, N.Morikawa, N.Nogawa

Measurements of the Production Cross Sections of Tritium from Oxygen using p-Be and p-Li Neutrons up to E(n) = 38 MeV

NUCLEAR REACTIONS ¹⁶O(n, t), E=15-40 MeV; measured tritium yields; deduced σ. ⁷Li, ⁹Be(p, n), E=20-40 MeV; measured neutron spectra.

doi: 10.1524/ract.1996.75.1.1
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22475.

1996UN01      Nucl.Sci.Eng. 122, 247 (1996)

Y.Uno, Y.Uwamino, T.S.Soewarsono, T.Nakamura

Measurement of the Neutron Activation Cross Sections of ¹²C, ³⁰Si, ⁴⁷Ti, ⁵²Cr, ⁵⁹Co, and ⁵⁸Ni between 15 and 40 MeV

NUCLEAR REACTIONS ¹²C, ⁵²Cr, ⁵⁹Co, ⁵⁸Ni(n, 2n), ³⁰Si, ^47,48Ti(n, np), ⁵⁹Co(n, 3n), (n, 4n), E=15-40 MeV; measured residuals production σ vs E. Activation technique, neutron beam from ⁷Li(p, n) reaction.

doi: 10.13182/NSE96-A24159
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22702.

1995NA28      Nucl.Instrum.Methods Phys.Res. A362, 454 (1995)

N.Nakao, T.Nakamura, M.Baba, Y.Uwamino, N.Nakanishi, H.Nakashima, S.-I.Tanaka

Measurements of Response Function of Organic Liquid Scintillator for Neutron Energy Range up to 135 MeV

doi: 10.1016/0168-9002(95)00193-X
Citations: PlumX Metrics

1995SH51      Nucl.Sci.Eng. 120, 40 (1995)

K.Shin, K.Miyahara, E.Tanabe, Y.Uwamino

Thick-Target Neutron Yield for Charged Particles

NUCLEAR REACTIONS C, ²⁷Al, Cu(¹²C, xn), E=75, 120 MeV; C, ²⁷Al, Cu(¹⁶O, xn), E=153 MeV; C, ²⁷Al, Cu(α, xn), E=40 MeV; measured σ(θn, En), thick target. Two-component moving source model.

doi: 10.13182/NSE95-A24104
Citations: PlumX Metrics

1995SH52      Nucl.Sci.Eng. 120, 136 (1995)

K.Shin, K.Miyahara, E.Tanabe, Y.Uwamino

Systematics in Differential Thick-Target Neutron Yields Parameterized by Moving Source Model

NUCLEAR REACTIONS C, ²⁷Al, Cu, Pb(¹²C, xn), E=120 MeV; C, ²⁷Al, Cu, Pb(¹⁶O, xn), E=153 MeV; C, Cu, Pb(α, xn), E=40, 65 MeV; ²⁷Al(α, xn), E=40 MeV; C, Cu, Fe, Pb(p, xn), E=52 MeV; measured thick target neutron differential yields. Moving source model analysis.

doi: 10.13182/NSE95-A24114
Citations: PlumX Metrics

1994SH43      Nucl.Instrum.Methods Phys.Res. A349, 506 (1994)

K.Shin, K.Miyahara, Y.Uwamino

Systematic Study of Neutron Production Cross Sections for Heavy Ions by Intranuclear Cascade-Evaporation Calculations

NUCLEAR REACTIONS ²⁷Al, Cu, U, ¹²C, ⁵⁶Fe, ²⁰⁷Pb(α, xn), (¹²C, xn), (²⁰Ne, xn), (⁴⁰Ar, xn), E=337 MeV/nucleon; analyzed neutron production data. Intranuclear cascade-evaporation calculations.

doi: 10.1016/0168-9002(94)91218-1
Citations: PlumX Metrics

1994UW01      J.Nucl.Sci.Technol.(Tokyo) 31, 1 (1994)

Y.Uwamino, H.Sugita, Y.Kondo, T.Nakamura

Measurement of Neutron Activation Cross Sections for Energies up to 40 MeV for Natural Samples of Mg, Si, Ca, V, Cr, Cu and Zn

NUCLEAR REACTIONS Mg(n, xnp)²⁴Na, Si(n, xnp)²⁸Al/²⁹Al, Si(n, xn2p)²⁷Mg, Ca(n, xnp)⁴²K/⁴³K, V(n, xn2p)⁴⁶Sc/⁴⁷Sc, Cr(n, xnp)⁵³V/⁵²V, Cu(n, xn2p)⁶²Co/^62mCo, Zn(n, xn2p)⁶⁵Ni, Zn(n, xnp)⁶⁴Cu/⁶⁶Cu/⁶⁸Cu/^68mCu, E ≤ 40 MeV; measured σ(E). Activation technique.

doi: 10.1080/18811248.1994.9735110
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22700.

1992KI08      J.Phys.(London) G18, 443 (1992)

T.Kishimoto, T.Shibata, M.Imamura, S.Shibata, Y.Uwamino

Search for Violation of the Pauli Principle through Spontaneous Neutron Emission from Lead

RADIOACTIVITY ²⁰⁸Pb; measured finite excess neutron counting rate, upper limit; deduced limits on spontaneous hole state appearance due to Pauli principle violation.

doi: 10.1088/0954-3899/18/2/023
Citations: PlumX Metrics

1992SH26      Nucl.Instrum.Methods Phys.Res. A316, 337 (1992)

T.Shibata, M.Imamura, S.Shibata, Y.Uwamino, T.Ohkubo, S.Satoh, K.Yamakoshi, N.Oyama, T.Ohsaka, N.Yamamoto, O.Hatozaki, N.Niimura

A Low Background Neutron Measuring System and Its Application to the Detection of Neutrons Produced by the D₂O Electrolysis

RADIOACTIVITY ²⁵²Cf(SF); measured fission neutron detection efficiency. Low background system.

NUCLEAR REACTIONS ²H(d, n), E=low; measured no neutron emission enhancement, no tritium production. Low background system, D₂O electrolysis.

doi: 10.1016/0168-9002(92)90919-U
Citations: PlumX Metrics

1992UW01      Nucl.Sci.Eng. 111, 391 (1992)

Y.Uwamino, H.Sugita, Y.Kondo, T.Nakamura

Measurement of Neutron Activation Cross Sections of Energy Up to 40 MeV Using Semimonenergetic p-Be Neutrons

NUCLEAR REACTIONS ⁵⁰Cr, ⁶³Cu, ⁶⁴Zn, ¹⁹⁷Au, ⁵⁵Mn, ²³Na(n, 2n), ²⁷Al, ⁵¹V(n, α), ⁵¹V, ⁶⁵Cu(n, p), ⁵⁵Mn(n, pα), (n, 4n), ¹⁹⁷Au(n, 4n), ⁶³Cu, ⁶⁴Zn(n, 3n), ⁶⁴Zn(n, t), ⁶⁴Zn, ⁶³Cu(n, 3n), E < 40 MeV; measured σ(E). Semi-monoenergetic p-Be neutrons, activation technique.

doi: 10.13182/NSE111-391
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22703.

1991NA04      Phys.Rev. C43, 1831 (1991)

T.Nakamura, H.Sugita, M.Imamura, Y.Uwamino, H.Nagai, K.Kobayashi

Measurement of the Long-Lived ²⁶Al Production Cross Section in the ²⁷Al(n, 2n) Reaction

NUCLEAR REACTIONS ²⁷Al(n, 2n), E ≈ 15.3-33.6 MeV; measured σ(E). Semi-monoenergetic beam, accelerator mass spectroscopy method.

doi: 10.1103/PhysRevC.43.1831
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22222.

1991SH25      Nucl.Instrum.Methods Phys.Res. A308, 609 (1991)

K.Shin, T.Ishii, Y.Uwamino, H.Sakai, S.Numata

Measurements of NE-213 Response Functions to Neutrons of Energies up to Several Tens of MeV

NUCLEAR REACTIONS C(n, np), E=10-73 MeV; measured detector response functions. NE-213 scintillator, quasi-monoenergetic, white neutron sources. Monte Carlo calculations.

doi: 10.1016/0168-9002(91)90074-Z
Citations: PlumX Metrics

1990IM04      Nucl.Instrum.Methods Phys.Res. B52, 595 (1990)

M.Imamura, H.Nagai, M.Takabatake, S.Shibata, K.Kobayashi, K.Yoshida, H.Ohashi, Y.Uwamino, T.Nakamura

Measurements of Production Cross Sections of ¹⁴C and ²⁶Al with High-Energy Neutrons up to E(n) = 38 MeV by Accelerator Mass Spectrometry

NUCLEAR REACTIONS O(n, X)¹⁴C, Si(n, X)²⁶Al, E ≤ 38 MeV; measured residue production σ. Accelerator mass spectrometry.

doi: 10.1016/0168-583X(90)90482-A
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22210.

1988UW01      Nucl.Instrum.Methods Phys.Res. A271, 546 (1988)

Y.Uwamino, T.Ohkubo, A.Torii, T.Nakamura

Semi-Monoenergetic Neutron Field for Activation Experiments up to 40 MeV

NUCLEAR REACTIONS ²⁷Al(n, α), ¹⁹⁷Au(n, 2n), (n, 4n), E=threshold-40 MeV; measured σ(E), σ(En); deduced reaction rates. Activation technique.

doi: 10.1016/0168-9002(88)90318-X
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2296.

1987NA12      Nucl.Instrum.Methods Phys.Res. A256, 505 (1987)

T.Nakamura, T.Ohkubo, Y.Uwamino

Spatial Distribution of Radionuclides Produced in Copper by Photonuclear Spallation Reactions

NUCLEAR REACTIONS Cu(γ, X)⁶⁰Cu/⁶¹Cu/⁶⁴Cu/⁵⁵Co/⁵⁶Co/⁵⁷Co/⁵²Mn/⁵⁶Mn/⁴⁴Sc/^44mSc/⁴⁷Sc/⁴⁸Sc, E=900 MeV bremsstrahlung; measured radionuclide production σ, spatial distributions, effective energy ranges. Ge detector. Monte Carlo calculations.

doi: 10.1016/0168-9002(87)90294-4
Citations: PlumX Metrics

1984NA06      Phys.Rev. C29, 1317 (1984); Erratum Phys.Rev. C30, 413 (1984)

T.Nakamura, Y.Uwamino

Neutron and Photon Production from Thick Targets Bombarded by 30-MeV p, 33-MeV d, 65-MeV ³He, and 65-MeV α Ions: Phenomenological analysis of experimental neutron energy spectra

NUCLEAR REACTIONS, ICPND ¹²C, ⁶³Cu, ²⁰⁸Pb(p, n), E=30 MeV; ¹²C, ⁶³Cu, ²⁰⁸Pb(d, n), E=33 MeV; ¹²C, ⁶³Cu, ²⁰⁸Pb(³He, n), (α, n), (α, γ), E=65 MeV; analyzed thick target σ(E, θ), neutron spectra; deduced reaction mechanism. Equilibrium, preequilibrium hybrid models.

doi: 10.1103/PhysRevC.29.1317
Citations: PlumX Metrics

1984SH04      Phys.Rev. C29, 1307 (1984)

K.Shin, K.Hibi, M.Fujii, Y.Uwamino, T.Nakamura

Neutron and Photon Production from Thick Targets Bombarded by 30-MeV p, 33-MeV d, 65-MeV ³He, and 65-MeV α Ions: Experiment and comparison with cascade Monte Carlo calculations

NUCLEAR REACTIONS, ICPND C, Fe, Pb, Cu(p, n), (p, γ), E=30 MeV; C, Fe, Pb, Cu(d, n), (d, γ), E=33 MeV; C, Fe, Pb, Cu(³He, n), (³He, γ), (α, n), (α, γ), E=65 MeV; measured thick target yields, σ(Eγ), σ(En); deduced σ(θ). Monte Carlo calculations.

doi: 10.1103/PhysRevC.29.1307
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2343.