NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = S.Miyamoto Found 30 matches. 2024SH01 Phys.Rev. C 109, 014302 (2024) T.Shizuma, M.Omer, T.Hayakawa, F.Minato, S.Matsuba, S.Miyamoto, N.Shimizu, Y.Utsuno Parity assignment for low-lying dipole states in 58Ni
doi: 10.1103/PhysRevC.109.014302
2024UT01 Phys.Rev. C 109, 014617 (2024) H.Utsunomiya, S.Goriely, M.Kimura, N.Shimizu, Y.Utsuno, G.M.Tveten, T.Renstrom, T.Ari-izumi, S.Miyamoto Photoneutron emission cross sections for 13C
doi: 10.1103/PhysRevC.109.014617
2023LA08 Phys.Rev. C 108, 025804 (2023) A.C.Larsen, G.M.Tveten, T.Renstrom, H.Utsunomiya, E.Algin, T.Ari-izumi, K.O.Ay, F.L.Bello Garrote, L.Crespo Campo, F.Furmyr, S.Goriely, A.Gorgen, M.Guttormsen, V.W.Ingeberg, B.V.Kheswa, I.K.B.Kullmann, T.Laplace, E.Lima, M.Markova, J.E.Midtbo, S.Miyamoto, A.H.Mjos, V.Modamio, M.Ozgur, F.Pogliano, S.Riemer-Sorensen, E.Sahin, S.Shen, S.Siem, A.Spyrou, M.Wiedeking New experimental constraint on the 185W(n, γ)186W cross section NUCLEAR REACTIONS 182,183,184W(γ, n), E=6.5-13 MeV; measured In, En; deduced σ(E), γ-ray strength function (GSF). 186W(α, α'γ), E=30 MeV; measured Eα, Iα, Eγ, Iγ, αγ-coin; deduced nuclear level density (NLD), γ-ray strength function (GSF). 185W(n, γ), T=0.5-1.1 GK; calculated Maxwellian averaged σ(E) (MACS), reaction rate (stellar reactivity), compared with experimental results, and recommended σ in compilations by Bao et al. Comparison to other experimental data, TALYS calculations and KADONIS-1.0 data. Photoneutron reactions were measured with quasi-monochromatic photon beam at NewSubaru synchrotron radiation facility using 4π detector consisting of 20 3He proportional counters. Experiment on inelastic α-scattering was performed at the Oslo Cyclotron Laboratory (OCL) using CACTUS NaI(Tl) scintillator γ-ray detector array, the Silicon Ring (SiRi) detector array and beam from MC-35 Scanditronix cyclotron.
doi: 10.1103/PhysRevC.108.025804
2023MU12 Phys.Rev. C 107, 064317 (2023) M.Murata, T.Kawabata, S.Adachi, H.Akimune, S.Amano, Y.Fujikawa, T.Furuno, K.Inaba, Y.Ishii, S.Miyamoto, M.Tsumura, H.Utsunomiya Photodisintegration cross section of 4He in the giant dipole resonance energy region NUCLEAR REACTIONS 4He(γ, n), (γ, p), E=23-30 MeV; measured charged particles (p, t, 3He), charged particles trajectories; deduced σ(E), giant dipole resonance parameters. Comparison to other experimental results. Quasi-monoenergetic photon beam produced via the laser Compton scattering technique. TPC-based gaseous active target (MAIKo) at BL01 beamline of the NewSUBARU synchrotron radiation facility.
doi: 10.1103/PhysRevC.107.064317
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
2021SH08 Phys.Rev. C 103, 024309 (2021) T.Shizuma, F.Minato, M.Omer, T.Hayakawa, H.Ohgaki, S.Miyamoto Low-lying electric and magnetic dipole strengths in 207Pb NUCLEAR REACTIONS 207Pb(polarized γ, γ'), E(maximum)=5.8, 6.3, 6.8 MeV quasimonochromatic photon beam generated by laser Compton scattering (LCS) with relativistic electrons circulating in the NewSUBARU storage ring; measured Eγ, Iγ at azimuthal angles of 0° and 90° relative to the polarization plane, azimuthal intensity ratios using two HPGe detectors at the LASTI of the University of Hyogo. 207Pb; deduced levels, J, π, branching ratios Γ0/Γ, integrated scattering cross sections, gΓ02/Γ, B(E1)(up), B(M1)(up), E1 and M1 photoabsorption cross sections, coherent excitations of spin-flip 1p-1h states in the 206Pb core. Nuclear resonance fluorescence (NRF) study. Comparison with particle-vibration coupling (PVC), with the quasiparticle random-phase approximation (QRPA) calculations using SkM*, SGII, and SkP interactions, and with previous experimental results.
doi: 10.1103/PhysRevC.103.024309
2019KR16 Acta Phys.Pol. B50, 487 (2019) M.Krzysiek, H.Utsunomiya, I.Gheorghe, D.M.Filipescu, T.Renstrom, G.M.Tveten, S.Belyshev, K.Stopani, H.Wang, G.Fan, Y.-W.Lui, D.Symochko, S.Goriely, A.-C.Larsen, S.Siem, V.Varlamov, B.Ishkhanov, T.Ari-izumi, S.Miyamoto Photoneutron Cross-section Measurements for 165Ho by the Direct Neutron-Multiplicity Sorting at NewSUBARU NUCLEAR REACTIONS 165Ho(γ, γ'), E=11.5-43.2 MeV; measured In, neutron multiplicity; deduced photoneutron σ(E). Flat-efficeincy neutron detector for direct neutron-multiplicity sorting method.
doi: 10.5506/aphyspolb.50.487
2019UT01 Phys.Rev. C 99, 024609 (2019) H.Utsunomiya, T.Renstrom, G.M.Tveten, S.Goriely, T.Ari-izumi, D.Filipescu, J.Kaur, Y.-W.Lui, W.Luo, S.Miyamoto, A.C.Larsen, S.Hilaire, S.Peru, A.J.Koning γ-ray strength function for thallium isotopes relevant to the 205Pb - 205Tl chronometry NUCLEAR REACTIONS 203,205Tl(γ, n), E=7.9-13.0 MeV; measured E(n), I(n), σ(E) using 4π 3He proportional counter array for neutron detection at NewSUBARU synchrotronic radiation facility; deduced GDR parameters and γ-ray strength function (γSF), the latter on the basis of the Hartree-Fock-Bogolyubov plus quasiparticle random-phase approximation using the Gogny D1M interaction for E1 and M1 components with the zero-limit correction (QRPA+D1M+0lim). 203,205Tl(n, γ), Eγ=0.001-4 MeV; calculated σ(E) with the D1M+QRPA+0lim, and compared with available experimental results. 204Tl(n, γ), T=0-1 GK; calculated Maxwellian averaged σ(E) (MACS) with the D1M+QRPA+0lim strength function, and compared with experimental results, and recommended σ in compilations by Bao et al.
doi: 10.1103/PhysRevC.99.024609
2019UT02 Phys.Rev. C 100, 034605 (2019) H.Utsunomiya, T.Renstrom, G.M.Tveten, S.Goriely, T.Ari-izumi, V.W.Ingeberg, B.V.Kheswa, Y.-W.Lui, S.Miyamoto, S.Hilaire, S.Peru, A.J.Koning γ-ray strength function for barium isotopes NUCLEAR REACTIONS 137Ba(γ, n)136Ba, E=7-13 MeV; 138Ba(γ, n)137Ba, E=8.75-13 MeV from laser Compton scattering at the NewSUBARU synchrotron radiation facility at the University of Hyogo; measured En, In; deduced σ(E), E1 and M1 γ-strength functions; σ(E) compared to TALYS calculations. The photoneutron data used to constrain the γ strength function on the basis of the Hartree-Fock-Bogolyubov plus quasiparticle random phase approximation using the Gogny D1M interaction. Comparison with previous experimental data. 131,133Ba(n, γ), kT=30 keV; estimated Maxwellian-averaged cross sections.
doi: 10.1103/PhysRevC.100.034605
2018UT03 Phys.Rev. C 98, 054619 (2018) H.Utsunomiya, T.Renstrom, G.M.Tveten, S.Goriely, S.Katayama, T.Ari-izumi, D.Takenaka, D.Symochko, B.V.Kheswa, V.W.Ingeberg, T.Glodariu, Y.-W.Lui, S.Miyamoto, A.C.Larsen, J.E.Midtbo, A.Gorgen, S.Siem, L.Crespo Campo, M.Guttormsen, S.Hilaire, S.Peru, A.J.Koning Photoneutron cross sections for Ni isotopes: Toward understanding (n, γ) cross sections relevant to weak s-process nucleosynthesis NUCLEAR REACTIONS 58,60,61,64Ni(γ, n), E=8.00-22.02 MeV; measured E(n), I(n), σ(E) using 3He proportional counters for neutrons and LaBr3(Ce) detector for γ-flux at NewSUBARU synchrotron radiation facility; deduced γ-ray strength functions (γSF); compared σ(E) with previous experimental data, and with TALYS predictions. 58,60,63,64(n, γ), E=0.01-10 MeV; calculated radiative σ(E) and Maxwellian averaged σ (MACS) in terms of the experimentally constrained γ-ray strength functions from the Hartree-Fock-Bogolyubov plus quasiparticle-random-phase approximation (HFB+QRPA) based on the Gogny D1M interaction for E1 and M1 components, supplemented with the M1 upbend. Relevance to the s-process nucleosynthesis, and radioactive nuclei at the s-process branching points.
doi: 10.1103/PhysRevC.98.054619
2017FU06 Physics of Part.and Nuclei 48, 124 (2017) M.Fujiwara, K.Nakai, N.Takahashi, T.Hayakawa, T.Shizuma, S.Miyamoto, G.T.Fan, A.Takemoto, M.Yamaguchi, M.Nishimura Production of medical 99mTc isotope via photonuclear reaction
doi: 10.1134/S1063779617010075
2017GH09 Phys.Rev. C 96, 044604 (2017); Erratum Phys.Rev. C 99, 059901 (2019) I.Gheorghe, H.Utsunomiya, S.Katayama, D.Filipescu, S.Belyshev, K.Stopani, V.Orlin, V.Varlamov, T.Shima, S.Amano, S.Miyamoto, Y.-W.Lui, T.Kawano, S.Goriely Photoneutron cross-section measurements in the 209Bi (γ, xn) reaction with a new method of direct neutron-multiplicity sorting NUCLEAR REACTIONS 209Bi(γ, n), (γ, np), (γ, 2n), (γ, 2np), (γ, 3n), (γ, 3np), (γ, 4n), (γ, 4np), E=threshold-40 MeV; measured E(n), I(n), photoneutron σ(E) using quasimonochromatic laser Compton-scattering (LCS) γ-ray beams at the NewSUBARU synchrotron radiation facility at the University of Hyogo, and novel technique of direct neutron-multiplicity sorting method. Comparison with previous experimental data from Livermore and Saclay, and with bremsstrahlung data, and with theoretical calculations using the TALYS reaction code. Comparison with Hartree-Fock Bogoliubov plus quasiparticle random phase approximation (HFB+QRPA) with Gogny D1M interaction for both E1 and M1 components of the GDR. Discussed threshold behavior of photoneutron emission in terms of average neutron kinetic energy.
doi: 10.1103/PhysRevC.96.044604
2017SH41 Phys.Rev. C 96, 044316 (2017) T.Shizuma, T.Hayakawa, I.Daito, H.Ohgaki, S.Miyamoto, F.Minato Low-lying dipole strength in 52Cr NUCLEAR REACTIONS 52Cr(polarized γ, γ'), E(max)=8.8, 9.4, 10.1, 11.0, 12.1 MeV quasimonochromatic, linearly polarized photon beam from NewSUBARU synchrotron radiation facility at the University of Hyogo; measured Eγ, Iγ, γγ(θ), polarization asymmetry, multipolarities. 52Cr; deduced levels, J, π, Γ02/Γ, B(E1), B(M1), cumulative M1 and E1 strengths, configurations. Comparison with previous experimental results, and with RPA and SRPA calculations using SGII and SGII+Te1 interactions.
doi: 10.1103/PhysRevC.96.044316
2017YA12 Phys.Rev. C 95, 044307 (2017) T.Yamagata, S.Nakayama, H.Akimune, S.Miyamoto Effect of the nuclear medium on α-cluster excitation in 6Li NUCLEAR REACTIONS 6Li(γ, n), (γ, 2n), (γ, 3n), E=4.9 to 53.6 MeV; measured E(n), I(n) using an array of 41 3He-gas proportional counters, σ(E) using NewSUBARU electron storage-ring facility at Hyougo, Japan. 6Li; deduced energy, width and other parameters of the Giant dipole resonance (GDR) consisting of two resonances, the low- and high-energy dipole resonances (LEDR and HEDR), TRK sum rule, α-cluster excitation. Comparison with previous experimental results, and with GDR parameters in 4He.
doi: 10.1103/PhysRevC.95.044307
2016HA11 Phys.Rev. C 93, 044313 (2016) T.Hayakawa, T.Shizuma, S.Miyamoto, S.Amano, A.Takemoto, M.Yamaguchi, K.Horikawa, H.Akimune, S.Chiba, K.Ogata, M.Fujiwara Spatial anisotropy of neutrons emitted from the 56Fe(γ, n)55Fe reaction with a linearly polarized γ-ray beam NUCLEAR REACTIONS 56Fe(polarized γ, n), (polarized γ, γ'), E<16.7 MeV laser Compton scattered beam at NewSUBARU electron storage ring; measured neutron spectra by TOF method, angular distribution of neutrons, neutron azimuthal anisotropy. 55Fe; deduced levels, J, π.
doi: 10.1103/PhysRevC.93.044313
2015NY01 Phys.Rev. C 91, 015808 (2015) H.-T.Nyhus, T.Renstrom, H.Utsunomiya, S.Goriely, D.M.Filipescu, I.Gheorghe, O.Tesileanu, T.Glodariu, T.Shima, K.Takahisa, S.Miyamoto, Y.-W.Lui, S.Hilaire, S.Peru, M.Martini, L.Siess, A.J.Koning Photoneutron cross sections for neodymium isotopes: Toward a unified understanding of (γ, n) and (n, γ) reactions in the rare earth region NUCLEAR REACTIONS 143,144,145,146,148Nd(γ, n), E=7.55-13.00 MeV laser Compton scattered (LCS) rays; measured neutron spectra, σ(E) at GACKO (Gamma Collaboration Hutch of Konan University) using SUBARU synchrotron radiation facility; deduced σ(E) for 147Nd(n, γ) by combining present (γ, n) data with existing (n, γ) data for 142,143,144,145,146,148Nd(n, γ), and using γ-SF method. Comparison of σ(E) for 147Nd(n, γ) with JENDL-4.0, ENDF/B-VII.1, and ROSFOND-2010 evaluated libraries. Comparison with predictions of Skyrme-Fock-Bogoliubov (HFB) plus quasiparticle random phase approximation (QRPA) model, and axially symmetric-deformed Gogny HFB plus QRPA model of E1 γ-ray strength using TALYS code. Comparison with previous experimental data.
doi: 10.1103/PhysRevC.91.015808
2015UT03 Phys.Rev. C 92, 064323 (2015) H.Utsunomiya, S.Katayama, I.Gheorghe, S.Imai, H.Yamaguchi, D.Kahl, Y.Sakaguchi, T.Shima, K.Takahisa, S.Miyamoto Photodisintegration of 9Be through the 1/2+ state and cluster dipole resonance NUCLEAR REACTIONS 9Be(γ, n), E=1.67-2.11, 5.58-16.11 MeV, [γ beam from Compton backscattering of CO2 laser photons with relativistic electrons]; measured Eγ, E(n), I(n), σ(Eγ) at the NewSUBARU synchrotron radiation facility; deduced Breit-Wigner parameters of B(E1), Γγ, and Γn for 1/2+ state, energy and strength of cluster dipole resonance (CDR). Comparison with the cluster dipole sum rule, and with previous experimental results.
doi: 10.1103/PhysRevC.92.064323
2014FI17 Phys.Rev. C 90, 064616 (2014) D.M.Filipescu, I.Gheorghe, H.Utsunomiya, S.Goriely, T.Renstrom, H.-T.Nyhus, O.Tesileanu, T.Glodariu, T.Shima, K.Takahisa, S.Miyamoto, Y.-W.Lui, S.Hilaire, S.Peru, M.Martini, A.J.Koning Photoneutron cross sections for samarium isotopes: Toward a unified understanding of (γ, n) and (n, γ) reactions in the rare earth region NUCLEAR REACTIONS 144,147,148,149,150,152,154Sm(γ, n), E=6-17 MeV; measured E(n), I(n), monochromatic and nonmonochromatic σ(E). Comparison with previous experimental results, and predictions from Skyrme HFB+QRPA using BSk7 interaction, and axially deformed Gogny HFB+QRPA models using D1M interaction. 147,148,149,150,151,152Sm(n, γ), E=0.001-1 MeV; analyzed measured σ(E) with a TALYS calculation using D1M+QRPA calculation for the E1 strength function. 153Sm(n, γ), E=0.001-1 MeV; predicted σ(E) from TALYS calculations using γ-strength function (γSF) approach. Comparison with evaluated libraries JENDL-4.0, ENDF/B-VII.1, ROSFOND-2010.
doi: 10.1103/PhysRevC.90.064616
2014HO14 Phys.Lett. B 737, 109 (2014) K.Horikawa, S.Miyamoto, T.Mochizuki, S.Amano, D.Li, K.Imasaki, Y.Izawa, K.Ogata, S.Chiba, T.Hayakawa Neutron angular distribution in (γ, n) reactions with linearly polarized γ-ray beam generated by laser Compton scattering NUCLEAR REACTIONS 197Au, 127I, Cu(polarized γ, n), E<16.7 MeV; measured reaction products, En, In, Eγ, Iγ; deduced yields, neutron angular distribution anisotropy. Comparison with available data.
doi: 10.1016/j.physletb.2014.08.024
2011EJ01 J.Phys.Soc.Jpn. 80, 094202 (2011) H.Ejiri, T.Shima, S.Miyamoto, K.Horikawa, Y.Kitagawa, Y.Asano, S.Date, Y.Ohashi Resonant Photonuclear Reactions for Isotope Transmutation NUCLEAR REACTIONS 100Mo, 197Au(γ, n), 100Mo(γ, p), E=12-16 MeV; measured reaction products, Eγ, Iγ; deduced relative yields, effective σ.
doi: 10.1143/JPSJ.80.094202
2008HA21 Phys.Rev. C 77, 068801 (2008) T.Hayakawa, T.Shizuma, S.Miyamoto, S.Amano, K.Horikawa, K.Ishihara, M.Mori, K.Kawase, M.Kando, N.Kikuzawa, S.Chiba, T.Mochizuki, T.Kajino, M.Fujiwara Half-life of the 164Ho by the (γ, n) reaction from laser Compton scattering gamma rays at the electron storage ring NewSUBARU NUCLEAR REACTIONS 165Ho(γ, n), E=3.3-16.7 MeV; measured Eγ, Iγ, half-life; calculated σ. 164Ho; deduced levels, J, π. RADIOACTIVITY 164Ho(β+), (β-); measured Eγ, Iγ. 164Dy, 164Er; deduced levels, J, π.
doi: 10.1103/PhysRevC.77.068801
2006HA51 Phys.Rev.C 74, 065802 (2006) T.Hayakawa, S.Miyamoto, Y.Hayashi, K.Kawase, K.Horikawa, S.Chiba, K.Nakanishi, H.Hashimoto, T.Ohta, M.Kando, T.Mochizuki, T.Kajino, M.Fujiwara Half-life of 184Re populated by the (γ, n) reaction from laser Compton scattering γ rays at the electron storage ring NewSUBARU RADIOACTIVITY 184,184mRe(EC), (β+) [from 185Re(γ, n)]; measured Eγ, Iγ, T1/2. 184W deduced transitions. NUCLEAR REACTIONS 185Re(γ, n), E ≈ 2-20 MeV; measured β-delayed Eγ, Iγ; deduced isomer yield ratio.
doi: 10.1103/PhysRevC.74.065802
2005LI13 J.Nucl.Sci.Technol.(Tokyo) 42, 259 (2005) D.Li, K.Imasaki, S.Miyamoto, S.Amano, T.Mochizuki Experiment on Photonuclear Reaction Induced by Laser Compton Scattering Gamma-Ray NUCLEAR REACTIONS 197Au(γ, n), E=spectrum; measured activation yield. Incident gammas from laser Compton scattering.
doi: 10.1080/18811248.2005.9726388
2002IS12 Nucl.Phys. B(Proc.Supp.) S111, 309 (2002) N.Ishihara, R.Ito, Y.Kunimi, T.Emura, Y.Kato, T.Nishi, Y.Sakamoto, N.Tamura, S.Kitamura, S.Miyamoto, Y.Nagasaka, T.Ohama, T.Inagaki, K.Omata, S.Takeda, Y.Yamada Search for neutrinoless double beta decay with DCBA
doi: 10.1016/S0920-5632(02)01731-0
1996HO22 Phys.Rev. C54, 2429 (1996) M.Hosaka, K.Ishii, M.Ohura, A.Terakawa, S.Miyamoto, Z.Guan, H.Orihara, J.Kasagi High Energy γ-Ray Production from Be, C, and Al Targets with 65 MeV 3He Bombardment NUCLEAR REACTIONS 9Be, C, 27Al(3He, 3He'), E=65 MeV; measured high energy σ(θ, Eγ). Potential bremsstrahlung calculations.
doi: 10.1103/PhysRevC.54.2429
1994IC01 Phys.Lett. 323B, 278 (1994) T.Ichihara, M.Ishihara, H.Ohnuma, T.Niizeki, Y.Tajima, T.Yamamoto, Y.Fuchi, S.Kubono, M.H.Tanaka, H.Okamura, S.Ishida, S.Miyamoto, H.Toyokawa Charge-Exchange Reaction 12C(12C, 12N)12B at E/A = 135 MeV NUCLEAR REACTIONS 12C(12C, 12N), (12C, 12C), E=135 MeV/nucleon; measured σ(θ), energy spectra; deduced model parameters. DWBA analysis.
doi: 10.1016/0370-2693(94)91220-3
1994IC02 Nucl.Phys. A569, 287c (1994) T.Ichihara, T.Niizeki, H.Okamura, H.Ohnuma, H.Sakai, Y.Fuchi, K.Hatanaka, M.Hosaka, S.Ishida, K.Kato, S.Kato, H.Kawashima, S.Kubono, S.Miyamoto, H.Orihara, N.Sakamoto, S.Takaku, Y.Tajima, M.H.Tanaka, H.Toyokawa, T.Uesaka, T.Yamamoto, T.Yamashita, M.Yosoi, M.Ishihara Spin-Isospin Resonances Observed in the (d, 2He) and (12C, 12N) Reactions at E/A = 135 MeV NUCLEAR REACTIONS 28Si(d, X), E=260 MeV; measured 2He energy spectra. 28Si, 12,13C(12C, 12N), E=135 MeV/nucleon; measured σ(θ); deduced model parameters, reaction mechanism, strong selectivity of ΔS=1, ΔT=1 transitions. 12B levels deduced transfer L. DWBA analysis.
doi: 10.1016/0375-9474(94)90119-8
1994NI17 J.Alloys and Compounds 213/214, 417 (1994) I.Nishinaka, M.Tanikawa, S.Miyamoto, K.Sueki, H.Nakahara, K.Tsukada, M.Magara, Y.Nagame, H.Ikezoe, T.Ohtsuki Fragment mass and kinetic energy distributions from fission of light actinides NUCLEAR REACTIONS 209Bi(16O, F), (18O, F), E ≈ 85 MeV; measured fission fragment kinetic energy and mass distributions.
doi: 10.1016/0925-8388(94)90948-2
1994OR07 Nucl.Phys. A577, 9c (1994) H.Orihara, G.C.Zhong, M.Hosaka, H.Ishimaru, K.Itoh, S.Miyamoto, T.Terakawa, K.Ishii, A.Narita, Y.Fujii, T.Nakagawa, K.Miura, H.Ohnuma Gamow-Teller Strengths Near the Ground States in A = 110 - 120 Nuclei Studied by (p, n) Reaction NUCLEAR REACTIONS 110,112,114,116Cd, 116,118,120Sn(p, n), E=35 MeV; measured neutron spectra, σ(θ). 112,114In, 118,120Sb deduced Gamow-Teller transition strength.
doi: 10.1016/0375-9474(94)90826-5
1985MI08 Nucl.Instrum.Methods 234, 588 (1985) S.Miyamoto, Y.Okumura, H.Tsunemi, M.Nakagawa A High Background Rejection Method in a Proportional Counter using Field-Adjusting Electrodes as Guard Cathodes RADIOACTIVITY 55Fe, 104Cd(EC); measured X-ray rise time distributions. High background rejection method, proportional counter.
doi: 10.1016/0168-9002(85)91012-5
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