NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = R.Moreh Found 96 matches. 2023BE24 Eur.Phys.J. D 77, 191 (2023) The range of 208Tl from 212Bi decay in collodion thin films RADIOACTIVITY 212Bi(α); measured decay products; deduced the effective range of 208Tl in extremely thin films of Collodion (C6H8N2O9).
doi: 10.1140/epjd/s10053-023-00765-8
2023KA01 Nucl.Technology 209, 115 (2023) S.Kahane, Y.Birenbaum, R.Moreh Reactor-Driven Neutron Sources from the207Pb(γ, n) and 205Tl(γ, n) Reactions NUCLEAR REACTIONS 207Pb, 205Tl(γ, n), E thermal; measured reaction products, Eγ, Iγ; deduced σ. Comparison with available data. Reactor measurement, relevant to the SARAF accelerator.
doi: 10.1080/00295450.2022.2102847
2023KA34 Int.J.Mod.Phys. E32, 2350064 (2023) Photonuclear reaction in 67Zn NUCLEAR REACTIONS 67Zn(γ, n), E=191 KeV; measured reaction products; deduced photoexcitation σ for the 7244 keV resonance. Gamma rays were produced with 55Mn(n, γ) reaction, 577g of metallic Mn mounted on a tangential beam tube, near but outside the core of the Israel Research Reactor 2 (IRR-2).
doi: 10.1142/S0218301323500647
2016BE01 Nucl.Instrum.Methods Phys.Res. A810, 140 (2016) Y.Ben-Galim, U.Wengrowicz, R.Moreh, I.Orion, A.Raveh Using the Doppler broadened γ line of the 10B(n, αγ)7Li reaction for thermal neutron detection NUCLEAR REACTIONS 10B(n, αγ), E thermal; measured reaction products, Eγ, Iγ; deduced new method. Comparison with Monte-Carlo calculations.
doi: 10.1016/j.nima.2015.11.143
2003MO03 Phys.Rev. C 67, 014602 (2003) Doppler broadening of the n-p capture γ line NUCLEAR REACTIONS 1H(n, γ), E=low; analyzed γ-ray Doppler broadening, contribution from zero-point motion of hydrogen atom.
doi: 10.1103/PhysRevC.67.014602
2002KA58 Phys.Rev. C66, 044316 (2002) Elastic and Raman scattering of 9.0 and 11.4 MeV photons from Au, Dy, and In NUCLEAR REACTIONS Au, Dy, In(γ, γ), (γ, γ'), E=9.0-11.4 MeV; measured Eγ, σ, σ(θ). 197Au deduced deformation, GDR parameters. 160,161,162,163,164Dy deduced B(E2), quadrupole moments, GDR features. 113,115In deduced GDR features.
doi: 10.1103/PhysRevC.66.044316
1995BI08 Phys.Rev. C51, 3496 (1995) Y.Birenbaum, Z.Berant, S.Kahane, A.Wolf, R.Moreh Absolute Cross Sections for (γ, n) Transitions in Lead, Bismuth, and Terbium NUCLEAR REACTIONS Pb, 209Bi, Th(γ, n), E=6-11.4 MeV; measured absolute σ(E). Thermal neutron capture photons, 3Hen-spectrometer. Direct-semi-direct, compound nucleus models.
doi: 10.1103/PhysRevC.51.3496
1994KA27 Phys.Rev. C50, 2000 (1994) Elastic Scattering Cross Sections of 11.4 MeV Photons from 206,207,208Pb, 209Bi, and 181Ta NUCLEAR REACTIONS 206,204,208Pb, 209Bi, 181Ta(γ, γ), E=11.4 MeV; measured σ(θ) vs E. 209Bi deduced GDR parameters.
doi: 10.1103/PhysRevC.50.2000
1994MO18 Phys.Rev. C50, 2222 (1994) R.Moreh, O.Beck, U.Kneissl, J.Margraf, H.Maser, H.H.Pitz, R.-D.Herzberg, N.Pietralla, A.Zilges Width of the 3841-keV Level in 17O NUCLEAR REACTIONS 17O(γ, γ'), E=4.7 MeV bremsstrahlung; measured scattering σ. 17O level deduced Γ. Enriched target.
doi: 10.1103/PhysRevC.50.2222
1994MO25 Phys.Lett. 331B, 13 (1994) Nuclear Resonance Photon Scattering and the Uncertainty Principle NUCLEAR REACTIONS 50Cr, 62Ni, 68Zn, 208Pb(γ, γ'), E ≈ resonance; analyzed resonance γ-scattering data; deduced scattering atom zero-point mean square linear momenta. ATOMIC PHYSICS 50Cr, 62Ni, 68Zn, 208Pb(γ, γ'), E ≈ resonance; analyzed resonance γ-scattering data; deduced scattering atom zero-point mean square linear momenta.
doi: 10.1016/0370-2693(94)90936-9
1993MO23 Phys.Rev. C48, 2625 (1993) R.Moreh, O.Beck, I.Bauske, W.Geiger, R.D.Heil, U.Kneissl, J.Margraf, H.Maser, H.H.Pitz Precise Widths of the 3089 and 3684 keV Levels in 13C NUCLEAR REACTIONS 13C(γ, γ'), E=4.7 MeV bremsstrahlung; measured precise Eγ, Iγ. 13C levels deduced Γ0. Self-absorption technique, enriched target, amorphous 13C absorbers.
doi: 10.1103/PhysRevC.48.2625
1992KA50 Phys.Rev. A46, 2489 (1992) Rayleigh Scattering of Neutron Capture γ Rays from Lead NUCLEAR REACTIONS C, Pb(γ, γ), E=0.465-2.842 MeV; measured relative σ(θ). Rayleigh scattering, n-capture γ-rays. Modified relativistic form-factor calculations. ATOMIC PHYSICS C, Pb(γ, γ), E=0.465-2.842 MeV; measured relative σ(θ). Rayleigh scattering, n-capture γ-rays. Modified relativistic form-factor calculations.
doi: 10.1103/PhysRevA.46.2489
1991MO25 Nucl.Instrum.Methods Phys.Res. A309, 503 (1991) R.Moreh, R.Fedorowicz, W.V.Prestwich, T.J.Kennett, M.A.Islam A Strong Dynamic Neutron Source Based on the 209Bi(γ, n) Reaction NUCLEAR REACTIONS 209Bi(γ, n), E=7.637, 7.915 MeV; measured photoneutron spectra; deduced resonance σ, dynamic neutron source possibility. 209Bi level deduced J, π, Γ.
doi: 10.1016/0168-9002(91)90255-O
1989KA43 Phys.Rev. A40, 6950 (1989) Rayleigh Scattering of Neutron Capture γ Rays from U NUCLEAR REACTIONS U(γ, γ), E=0.4-3 MeV; measured γ-spectra, σ(θ). Modified form factor analysis. Neutron scattering γ-source.
doi: 10.1103/PhysRevA.40.6950
1989MO01 Nucl.Phys. A491, 45 (1989) Influence of Atomic Binding on the Nuclear Resonance Photon Scattering from the 7362 keV Level in 68Zn NUCLEAR REACTIONS 68Zn(γ, γ'), E ≈ resonance; measured E(γ), I(γ), σ vs temperature; deduced atomic binding role.
doi: 10.1016/0375-9474(89)90205-4
1989MO02 Phys.Rev. C39, 1247 (1989); Erratum Phys.Rev. C40, 1548 (1989) R.Moreh, T.J.Kennett, W.V.Prestwich 2H(γ, n) Absolute Cross Section at 2754 keV NUCLEAR REACTIONS 2H(γ, n), E=2.75 MeV; measured absolute photodisintegration σ. Model comparison.
doi: 10.1103/PhysRevC.39.1247
1988BI05 Phys.Rev.Lett. 61, 810 (1988); Erratum Phys.Rev.Lett. 62, 115 (1989) Y.Birenbaum, Z.Berant, A.Wolf, S.Kahane, R.Moreh Differential Cross Sections for the D(γ, n) Reaction below 10 MeV NUCLEAR REACTIONS 2H(γ, n), E=6-9 MeV; measured photodisintegration σ(θ), neutron yield. Monochromatic photon source, high resolution neutron spectrometer.
doi: 10.1103/PhysRevLett.61.810
1988MO12 Phys.Rev. C37, 2418 (1988) R.Moreh, W.C.Sellyey, D.C.Sutton, R.Vodhanel, J.Bar-Touv Strong Photon Strength in 40Ar between 8 and 11 MeV NUCLEAR REACTIONS 40Ar(γ, γ'), E=8.5, 10.3, 11.8 MeV bremsstrahlung; measured Eγ, Iγ. 40Ar deduced level energies, J, g(Γ02/Γ), Γ0/Γγ, Γ, giant dipole strength, B(E1). Resonance fluorescence technique. NUCLEAR STRUCTURE 40Ar; calculated levels, B(E2). Open shell linear response method.
doi: 10.1103/PhysRevC.37.2418
1988MO13 Phys.Rev. C37, 2428 (1988) R.Moreh, W.M.Sandefur, W.C.Sellyey, D.C.Sutton, B.H.Wildenthal Ground State M1 Strength of d5/2-1 Levels in 39K NUCLEAR REACTIONS 39K(γ, γ'), E=6.6, 8.5, 9.4 MeV bremsstrahlung; measured Eγ, Iγ. 39K levels deduced Γ, (gΓ02/Γ), B(M1).
doi: 10.1103/PhysRevC.37.2428
1987MO03 Phys.Lett. 185B, 11 (1987) Correlations between (γ, γ') and (d, τ) Excitations of Hole States in 15N and 39K NUCLEAR REACTIONS 39K, 15N(γ, γ'), E=6.6, 8.5, 9.4 MeV bremsstrahlung; 40Ca, 16O(d, 3He), E=52, 76 MeV; analyzed data. 15N, 39K deduced levels J, π, (gΓ0), B(M1), spectroscopic factors.
doi: 10.1016/0370-2693(87)91519-X
1987VO01 Phys.Rev. C35, 921 (1987) R.Vodhanel, R.Moreh, W.C.Sellyey, M.K.Brussel, B.H.Wildenthal M1 Radiation Widths in 27Al NUCLEAR REACTIONS 27Al(γ, γ'), E=7.66, 10.37 MeV; measured σ(E, θ). 27Al deduced levels, (gΓ0), B(M1). Shell model.
doi: 10.1103/PhysRevC.35.921
1987WI13 Phys.Rev. C36, 758 (1987) J.A.Winger, J.C.Hill, F.K.Wohn, R.Moreh, R.L.Gill, R.F.Casten, D.D.Warner, A.Piotrowski, H.Mach Decay of 80Zn: Implications for shell structure and r-process nucleosynthesis RADIOACTIVITY 80Zn(β-) [from 235U(n, F), E=thermal]; measured Eγ, Iγ, βγ-, γγ-coin, T1/2, Qβ; deduced log ft. 80Ga deduced levels, J, π, γ-branching. Hyperpure Ge detectors.
doi: 10.1103/PhysRevC.36.758
1986BE30 Phys.Rev. C34, 1481 (1986) Z.Berant, J.Ivri, R.Moreh, A.Wolf 1+ State in 44Ca NUCLEAR REACTIONS 44Ca(γ, γ'), E=4-7 MeV; measured Eγ, Iγ, γ(θ), polarization; deduced σ. 44Ca deduced transition γ-multipolarity, δ, Γ, Γ0, Γ/Γ0.
doi: 10.1103/PhysRevC.34.1481
1986BI12 Phys.Rev. C34, 2055 (1986) Y.Birenbaum, Z.Berant, S.Kahane, R.Moreh, A.Wolf E1-E2 Interference in 159Tb(γ, n) and 209Bi(γ, n) Reactions NUCLEAR REACTIONS 159Tb, 209Bi(γ, n), E=7-11.4 MeV; measured σ(En), σ(θ); deduced angular distribution coefficients vs energies. 159Tb, 209Bi deduced strong E1, E2 interference effects. 3He spectrometer. Compound nucleus process, direct-semidirect model.
doi: 10.1103/PhysRevC.34.2055
1986GI07 Phys.Rev.Lett. 56, 1874 (1986) R.L.Gill, R.F.Casten, D.D.Warner, A.Piotrowski, H.Mach, J.C.Hill, F.K.Wohn, J.A.Winger, R.Moreh Half-Life of 80Zn: The first measurement for an r-process waiting-point nucleus RADIOACTIVITY 80Zn(β-) [from 235U(n, F), E=thermal]; measured γγ-, βγ-coin, β endpoint spectra; deduced Q, T1/2. 80Ga deduced levels, γ-branching.
doi: 10.1103/PhysRevLett.56.1874
1986MA42 Phys.Rev. C34, 1117 (1986) H.Mach, R.L.Gill, D.D.Warner, A.Piotrowski, R.Moreh Half-Life Measurements for Neutron-Rich Ag and Cd Nuclei RADIOACTIVITY 123Ag, 123,123m,124,125,125m,127,128Cd(β-) [from 235U(n, F), E=thermal]; measured Eγ, Iγ, γγ(t); deduced T1/2.
doi: 10.1103/PhysRevC.34.1117
1985BE18 Phys.Rev. C31, 1553 (1985) Z.Berant, S.Kahane, R.Moreh, O.Shahal Probing the Microstructure of the Giant Dipole Resonance in 208Pb NUCLEAR REACTIONS 208Pb(γ, γ), E=8.999, 10.055, 11.388 MeV; measured Eγ, Iγ, σ(θ) vs Eγ. 208Pb deduced GDR, Γ. Monchromatic photon beam.
doi: 10.1103/PhysRevC.31.1553
1985BI06 Phys.Rev. C32, 1825 (1985) Y.Birenbaum, S.Kahane, R.Moreh Absolute Cross Section for the Photodisintegration of Deuterium NUCLEAR REACTIONS 2H(γ, X), E=5.97, 7.25, 7.6, 7.64, 8.8, 9, 11.39 MeV; measured photodisintegration σ. Absorption method.
doi: 10.1103/PhysRevC.32.1825
1985MO10 Phys.Rev. C31, 2314 (1985) R.Moreh, W.C.Sellyey, D.Sutton, R.Vodhanel Widths of the 6.92 and 7.12 MeV Levels in 16O and the Influence of the Effective Temperature NUCLEAR REACTIONS 16O(γ, γ'), E=9.3 bremsstrahlung; measured Eγ, Iγ; deduced O-atom effective temperature. 16O levels deduced Γ0. Water target.
doi: 10.1103/PhysRevC.31.2314
1984VO02 Phys.Rev. C29, 409 (1984) R.Vodhanel, M.K.Brussel, R.Moreh, W.C.Sellyey, T.E.Chapuran Strong M1 Transitions in 23Na below 10 MeV NUCLEAR REACTIONS 23Na(γ, γ'), E=7.66, 10.37 MeV bremsstrahlung; measured Eγ, Iγ; deduced σ temperature dependence. 23Na levels deduced Γ0/Γ, (gΓ0), γ-branching ratios, B(M1), J, π, T assignments. Photoexcitation.
doi: 10.1103/PhysRevC.29.409
1983KA26 Phys.Rev. C28, 1519 (1983) Interference between Rayleigh, Delbruck, and Nuclear Resonance Scattering Processes NUCLEAR REACTIONS Pb, 208Pb, 209Bi(γ, γ), E=4.2-9.3 MeV; measured σ(θ), Delbruck and Rayleigh scattering, nuclear resonance fluorescence, interference effects.
doi: 10.1103/PhysRevC.28.1519
1983MO06 J.Phys.(London) G9, 755 (1983) R.Moreh, O.Shahal, J.Tenenbaum Photoexcitation of Levels at 6605 keV in 48Ti and 7362 keV in 68Zn NUCLEAR REACTIONS 48Ti, 68Zn(γ, γ'), E=6.6, 7.36 MeV; measured Eγ, Iγ, γ(θ). 48Ti, 68Zn deduced levels, J, π, Γ.
doi: 10.1088/0305-4616/9/7/011
1983WE06 Phys.Rev. C28, 1959 (1983) H.R.Weller, R.G.Seyler, R.Moreh Direct-Semidirect Model Angular Distributions for Radiative Capture or Photonuclear Reactions Involving Nonzero Target or Residual Spins NUCLEAR REACTIONS 208Pb(γ, n), E=8-12 MeV; 207Pb(γ, n), E=7-10 MeV; calculated a2, a0 coefficient ratio vs E. Direct-semidirect model.
doi: 10.1103/PhysRevC.28.1959
1982MO05 Phys.Rev. C25, 1824 (1982) R.Moreh, W.M.Sandefur, W.C.Sellyey, D.C.Sutton, R.Vodhanel Strong E2 and M1 Transitions in 40Ca NUCLEAR REACTIONS 40Ca(γ, γ'), E=8.5, 11.3, 11.7 MeV bremsstrahlung; measured Eγ. 40Ca deduced levels, J, π, Γ, Γγ, B(E2), EWSR, B(M1). Resonance fluorescence technique.
doi: 10.1103/PhysRevC.25.1824
1981BE44 Nucl.Phys. A368, 201 (1981) Z.Berant, Y.Birenbaum, R.Moreh, O.Shahal Study of the 49Ti Energy Levels using the (γ, γ) and the (γ, n) Reactions NUCLEAR REACTIONS 49Ti(γ, γ'), (γ, n), E < 8.9 MeV; measured Eγ, Iγ(θ), En, σ(θn). 49Ti deduced levels, J, π, E1 transition strength, Γγ, Γ(n).
doi: 10.1016/0375-9474(81)90682-5
1981BI13 Nucl.Phys. A369, 483 (1981) Y.Birenbaum, Z.Berant, S.Kahane, A.Wolf, R.Moreh Angular Distributions of Photoneutrons from the 207,208Pb(γ, n0) Reactions NUCLEAR REACTIONS 208,207Pb(γ, n), E=7.0-11.4 MeV; measured σ(θ). 207,208Pb deduced E2-E1 and M1-E1 interference effects.
doi: 10.1016/0375-9474(81)90033-6
1981MO09 Phys.Rev. C23, 988 (1981); Erratum Phys.Rev. C24, 2394 (1981) R.Moreh, W.C.Sellyey, R.Vodhanel Gamma-Ray Widths in 15N NUCLEAR REACTIONS 15N(γ, γ'), E=10.3, 11.4 MeV bremsstrahlung; measured Eγ. 15N deduced levels, Γγ, M1, E2 transitions. Enriched LiNO3 target, resonance fluorescence technique. Weak-coupling model, SU(3) basis interpretations.
doi: 10.1103/PhysRevC.23.988
1980MO14 Phys.Lett. 92B, 286 (1980) R.Moreh, W.C.Sellyey, R.Vodhanel Effect of Molecular Orientation on the Nuclear Photon Scattering from 11B NUCLEAR REACTIONS 11B(γ, γ'), E=11.3 bremsstrahlung; measured Iγ(θ); deduced molecular orientation effect. Pyrolytic boron nitride target.
doi: 10.1016/0370-2693(80)90265-8
1980MO23 Phys.Rev. C22, 1820 (1980); Erratum Phys.Rev. C23, 2799 (1981) R.Moreh, W.C.Sellyey, R.Vodhanel Widths of 11B Levels below 9.0 MeV NUCLEAR REACTIONS 11B(γ, γ'), E=10.3 MeV bermsstrahlung; measured Eγ, Iγ, self-absorption. 11B deduced effective temperature. 11B levels deduced Γ, γ-multipolarity. Natural Boron, BN, B4C targets.
doi: 10.1103/PhysRevC.22.1820
1980NA02 Phys.Lett. 91B, 38 (1980) Inadequacy of the Dynamic Collective Model in Describing Inelastic Photon Scattering in 166Er NUCLEAR REACTIONS 166Er(γ, γ'), E=14.4-16.6 MeV bremsstrahlung; measured Eγ, branching ratios. Dynamic collective model.
doi: 10.1016/0370-2693(80)90657-7
1980SH05 Nucl.Phys. A339, 157 (1980) Nuclear Resonance Photon Scattering from 15N in the Form of BN and NH4Cl NUCLEAR REACTIONS 15N(γ, γ), E=6.324 MeV; measured temperature dependence of σ; deduced effective temperatures. Natural, enriched targets.
doi: 10.1016/0375-9474(80)90247-X
1979BI12 Phys.Lett. 88B, 239 (1979) Y.Birenbaum, Z.Berant, A.Wolf, R.Moreh Interference Effects between Multipole Resonances in the 206Pb(γ, n) Reaction NUCLEAR REACTIONS 206Pb(γ, n), E=8.5-11.4 MeV; measured σ(θ); deduced multipole mixing effects.
doi: 10.1016/0370-2693(79)90456-8
1979MO19 Nucl.Instrum.Methods 166, 69 (1979) Studies in Nuclear Spectroscopy Using the (γ, γ') and the (γ, n) Reactions. Part II. Nuclear Physics and Fundamental Scattering Processes COMPILATION 15N, 50Cr, 55Mn, 62Ni, 65Cu, 66Zn, 69Ga, 74Ge, 75As, 80Se, 86Sr, 90Zr, 93Nb, 100Mo, 112Cd, 118,120Sn, 126,130Te, 139La, 140Ce, 141Pr, 142,144,146Nd, 144,154Sm, 202Hg, 203,205Tl, 208Pb, 209Bi; compiled total, ground state Γγ. Elastic, inelastic scattering data, monochromatic photons.
doi: 10.1016/0029-554X(79)90514-7
1978BE07 Phys.Lett. 73B, 142 (1978) Interference between Nuclear Resonance and Nuclear Thomson Scattering Of Photons NUCLEAR REACTIONS 55Mn(γ, γ), E=5.5-11.4 MeV; measured σ(E).
doi: 10.1016/0370-2693(78)90819-5
1978BE45 Nucl.Phys. A306, 101 (1978) Z.Berant, J.Tenenbaum, A.Wolf, R.Moreh Study of the Energy Levels of 93Nb and 123Sb Using Nuclear Photoexcitation NUCLEAR REACTIONS 93Nb, 123Sb(γ, γ'); measured Eγ, Iγ(θ). 93Nb, 123Sb deduced levels, J, π, M1, Γ.
doi: 10.1016/0375-9474(78)90314-7
1978KA25 Phys.Rev. C18, 1217 (1978) Evidence for Destructive Interference between Rayleigh and Delbruck Scattering for 6.8-11.4-MeV Photons NUCLEAR REACTIONS 181Ta, Pb, 238U(γ, γ), E=6.84-11.39 MeV; measured σ(E, θ); deduced Rayleigh, Delbruck amplitude contribution.
doi: 10.1103/PhysRevC.18.1217
1978KA29 Nucl.Phys. A308, 88 (1978) Evidence for Coulomb Correction Effect in Delbruck Scattering of 9.0 and 7.9 MeV Photons on 238U NUCLEAR REACTIONS 238U(γ, γ), E ≈ 7.9, 9.0 MeV; measured σ(E, θ), θ=1.2°-140°; deduced Delbruck amplitude contribution. Coulomb corrections.
doi: 10.1016/0375-9474(78)90442-6
1978MO31 Nucl.Instrum.Methods 155, 429 (1978) R.Moreh, Y.Birenbaum, Z.Berant A New 86 keV Neutron Source from 207Pb(γ, n) Reaction NUCLEAR REACTIONS 207Pb(γ, n), E ≈ 7.28-9.29 MeV; measured σ(En), σ(θ); deduced σ.
doi: 10.1016/0029-554X(78)90525-6
1977BA03 Nucl.Phys. A275, 151 (1977) Elastic and Raman Scattering of 8.5-11.4 MeV Photons from 159Tb, 165Ho And 237Np NUCLEAR REACTIONS 159Tb, 165Ho, 237Np(γ, γ'), E=8.5-11.4 MeV; measured σ(E, Eγ', θ), θ=90-140°. 159Tb, 165Ho, 237Np deduced giant resonance structure.
doi: 10.1016/0375-9474(77)90281-0
1977BA55 Nucl.Phys. A288, 192 (1977) Elastic and Raman Scattering of 8.5-11.4 MeV Photons from 175Lu and 181Ta NUCLEAR REACTIONS 175Lu, 181Ta(γ, γ'), E=8.5-11.4 MeV; measured σ(E, Eγ', θ), θ=140°. 175Lu, 181Ta deduced giant dipole resonance parameters. Natural targets.
doi: 10.1016/0375-9474(77)90129-4
1977BE05 Nucl.Phys. A276, 221 (1977) Z.Berant, J.Tenenbaum, R.Moreh Nuclear Resonance Fluorescence in 146Nd and 154Sm NUCLEAR REACTIONS 146Nd, 154Sm(γ, γ'); measured Eγ, Iγ(θ). 146Nd, 154Sm deduced levels, J, π, M2/E1, Γ.
doi: 10.1016/0375-9474(77)90380-3
1977BE32 Phys.Lett. 69B, 281 (1977) Nuclear Thomson Scattering of 5.5-7.2 MeV Photons NUCLEAR REACTIONS 12C, 24Mg(γ, γ), E=5.5-7.2 MeV; measured σ(E).
doi: 10.1016/0370-2693(77)90545-7
1977JA13 Nucl.Phys. A291, 1 (1977) Studies of Nuclear Levels Around 7.5 MeV Using a High Resolution γ-Monochromator NUCLEAR REACTIONS Cd, Ce, Ba, 139La, 141Pr, 209Bi(γ, γ'), E=7.28, 7.63 MeV; measured yields, scattering spectra. 139La, 209Bi deduced levels, gΓ0. Natural targets.
doi: 10.1016/0375-9474(77)90194-4
1977KA05 Phys.Lett. 66B, 229 (1977) Rayleigh and Delbruck Scattering of 6.8-11.4 MeV Photons at θ = 1.5° NUCLEAR REACTIONS Pb, U(γ, γ), E=6.8-11.4 MeV; measured σ(E).
doi: 10.1016/0370-2693(77)90867-X
1977KA09 Nucl.Phys. A280, 180 (1977) Delbruck Scattering of 9 MeV Photons from Tantalum NUCLEAR REACTIONS 181Ta(γ, γ), E=9 MeV; measured σ(θ); deduced Delbruck-amplitude contribution.
doi: 10.1016/0375-9474(77)90302-5
1976MO14 Nucl.Phys. A262, 221 (1976) Effect of Molecular Binding on the Resonance Scattering of Photons from the 6.324 MeV Level in 15N NUCLEAR REACTIONS 15N(γ, γ), E=6.324 MeV; measured Γ, σ. Enriched targets.
doi: 10.1016/0375-9474(76)90616-3
1975MO27 Nucl.Phys. A252, 423 (1975) Absorption of 6.42 MeV Photons NUCLEAR REACTIONS Be, C, Al, Ti, V, Fe, Co, Ni, Cu, Zn, Ge, Zr, Mo, Ag, Cd, Sn, Ce, Ta, W, Au, Pb, Bi, U(γ, X), E=6.418 MeV; measured attenuation coefficients. 139La resonant scatterer.
doi: 10.1016/0375-9474(75)90509-6
1975MO28 Nucl.Phys. A252, 429 (1975) The 6.324 MeV Hole State in 15N NUCLEAR REACTIONS 15N(γ, γ'), E=6.324 MeV; measured pγ, Iγ(θ). 15N level deduced J, π, Γ, E2/M1 mixing ratio.
doi: 10.1016/0375-9474(75)90510-2
1974BA51 Nucl.Phys. A229, 417 (1974) Study of the Giant Dipole Resonance of 232Th and 238U Using Elastic and Raman Photon Scattering NUCLEAR REACTIONS 232Th, 238U(γ, γ'), E=7.9-11.4 MeV; measured σ(E, Eγ', θ), θ=90-140°. 232Th, 238U deduced giant resonance structure. Natural targets.
doi: 10.1016/0375-9474(74)90661-7
1974KA16 Phys.Rev. C9, 2384 (1974) Elastic Scattering of 7.9-MeV Photons from 181Ta NUCLEAR REACTIONS 181Ta(γ, γ), E=7.9 MeV; measured Delbruck scattering, σ(θ), θ=25-140°.
doi: 10.1103/PhysRevC.9.2384
1974MO09 Nucl.Phys. A224, 86 (1974) R.Moreh, A.Wolf, I.Jacob, A.Nof Study of the Energy Levels of 62Ni Using the (γ, γ') Reaction NUCLEAR REACTIONS 62Ni(γ, γ'), E=7646 keV; measured Eγ, Iγ, γ(θ). 62Ni deduced levels, J, π, level-width.
doi: 10.1016/0375-9474(74)90164-X
1974MO15 Nucl.Phys. A228, 77 (1974) Study of the Temperature Effect of Resonantly Scattered Capture γ-Rays NUCLEAR REACTIONS 208Pb(γ, γ), E=7.279 MeV; 62Ni(γ, γ), E=7.646 MeV; measured σ (T=4.2° K to 600° K); deduced Debye temperatures. Natural targets.
doi: 10.1016/0375-9474(74)90446-1
1974TE01 Nucl.Phys. A218, 95 (1974) Properties of Nuclear Levels Excited by Neutron Capture γ-Rays from Cobalt NUCLEAR REACTIONS 55Mn, 140Ce, 141Pr, 142Nd, 202Hg, 209Bi(γ, γ')E=0-6.5 MeV; measured Eγ, Iγ(θ), σ. 55Mn, 142Nd deduced levels, J, π, level-width. 140Ce, 141Pr, 202Hg, 209Bi levels deduced J, π, level-width. Natural targets.
doi: 10.1016/0375-9474(74)90022-0
1974WO05 Nucl.Phys. A227, 373 (1974) Properties of Nuclear Levels Photoexcited by Neutron-Capture γ-Rays of Ti and Cu NUCLEAR REACTIONS 65Cu, 100Mo, 118Sn, 126Te, 130Te, 186W, 209Bi(γ, γ'), E=6.4-7.9 MeV; measured Eγ, σ(Eγ', θ). 65Cu, 100Mo, 118Sn, 126,130Te, 186W, 209Bi deduced resonances, J, π, level-width, E2/M1 mixing ratios, level-width(E2).
doi: 10.1016/0375-9474(74)90805-7
1973MO05 Phys.Rev. C7, 1885 (1973) R.Moreh, O.Shahal, J.Tenenbaum, A.Wolf, A.Nof Study of the Energy Levels of 69Ga Using Nuclear Photoexcitation NUCLEAR REACTIONS 69Ga(γ, γ), (γ, γ'), E=thermal n-capture in Cu, V; measured Eγ, Iγ(θ), Iγ, P(γ). 69Ga deduced levels, J, π, γ-branching.
doi: 10.1103/PhysRevC.7.1885
1973MO30 Nucl.Phys. A217, 477 (1973) R.Moreh, A.Wolf, O.Shahal, J.Tenenbaum, A.Nof Study of the Energy Levels of 100Mo Using Nuclear Photoexcitation NUCLEAR REACTIONS 100Mo(γ, γ'); measured Eγ, Iγ(θ), pγ. 100Mo deduced levels, J, π, M2/E1, level widths.
doi: 10.1016/0375-9474(73)90406-5
1973MO31 Phys.Lett. 47B, 351 (1973) Delbruck Scattering of 7.9 MeV Photons NUCLEAR REACTIONS 232Th, 238U(γ, γ), E=7.9 MeV; measured σ(θ).
doi: 10.1016/0370-2693(73)90621-7
1972MO03 Nucl.Instrum.Methods 98, 13 (1972) Polarization Measurements of Resonantly Scattered Capture Gamma Rays NUCLEAR REACTIONS 62Ni(γ, γ), E=7.646 MeV; measured γ-polarization. 62Ni level deduced parity.
doi: 10.1016/0029-554X(72)90418-1
1972MO46 Nucl.Instrum.Methods 105, 557 (1972) Utilization of 11.4 MeV Photons from the 59Ni(n, γ)60Ni Reaction for Scattering Experiments NUCLEAR REACTIONS 59,61,63Ni(n, γ);E=reactor spectrum; measured Eγ, 60,62,64Ni deduced Eγ.
doi: 10.1016/0029-554X(72)90354-0
1972WO21 Phys.Rev. C6, 2276 (1972) A.Wolf, R.Moreh, A.Nof, O.Shahal, J.Tenenbaum Large E1 and M1 Radiative Widths in Nuclei Near Closed Shells NUCLEAR REACTIONS 139La, 140Ce, 141Pr, 142Nd, 144Nd, 205Tl, 209Bi(γ, γ'), E=spectrum; measured σ(E;Eγ', θ(γ')). 139La, 140Ce, 141Pr, 142,144Nd, 205Tl, 209Bi deduced levels, level-width, J, π.
doi: 10.1103/PhysRevC.6.2276
1971GA15 Phys.Rev. C4, 223 (1971) Y.Gazit, A.Katase, G.Ben-David, R.Moreh Energy and Angular Distribution of Alpha Particles Emitted in Thermal-Neutron Fission of 235U NUCLEAR REACTIONS, Fission 235U(n, F), E=thermal; measured Eα, Iα, E(fragment).
doi: 10.1103/PhysRevC.4.223
1971HA40 Phys.Lett. 36B, 68 (1971) Experimental Observation of the Nuclear Raman Effect NUCLEAR REACTIONS 232Th, 238U(γ, γ), (γ, γ'), E=8533, 8998, 9298 keV; measured elastic, Raman scattering σ.
doi: 10.1016/0370-2693(71)90109-2
1971MO10 Phys.Lett. 34B, 494 (1971) R.Moreh, D.Salzmann, G.Ben-David Forward Elastic Scattering of 9 MeV Gamma Rays NUCLEAR REACTIONS Pb, U(γ, γ), E=9 MeV; measured σ(θ).
doi: 10.1016/0370-2693(71)90663-0
1971MO26 Phys.Lett. 36B, 71 (1971) R.Moreh, A.Nof, O.Shahal, A.Wolf The M2 Radiative Widths of Nuclear Levels at About 7 MeV Excitation NUCLEAR REACTIONS 74Ge, 100Mo, 112Cd, 186W(γ, γ'); [Eγ from Ti, Fe(n, γ)]; measured σ(Eγ', θ). 74Ge, 100Mo, 112Cd, 186W transitions deduced M2 level-width, γ-mixing.
doi: 10.1016/0370-2693(71)90110-9
1971MO31 Phys.Rev. C4, 2265 (1971) Study of the Energy Levels of 112Cd Using Nuclear Photoexcitation NUCLEAR REACTIONS 112Cd(γ, γ), (γ, γ'), E from Fe(n, γ); measured σ(Eγ', θ(γ')). 112Cd deduced levels, J, π, γ-mixing, level-width.
doi: 10.1103/PhysRevC.4.2265
1971TE01 Phys.Rev. C3, 663 (1971) J.Tenenbaum, R.Moreh, Y.Wand, G.Ben-David Study of the Level Structure of 50Ti and 51Ti Using the 49Ti(n, γ) and 50Ti(n, γ) Reactions NUCLEAR REACTIONS 49,50Ti(n, γ), E=thermal; measured Eγ, Iγ, γγ(θ); deduced Q. 50,51Ti deduced levels, J, π, γ-branching.
doi: 10.1103/PhysRevC.3.663
1970MO16 Phys.Rev. C2, 249 (1970) Study of the Energy Levels of 203Tl Using (γ, γ') Reaction NUCLEAR REACTIONS 203Tl(γ, γ), (γ, γ'), E approx 6.4 MeV; measured σ(Eγ', θ(γ')), γ-polarization. 203Tl deduced levels, J, π, level-width, branching ratios.
doi: 10.1103/PhysRevC.2.249
1970MO26 Phys.Rev. C2, 1144 (1970) Radiative Widths, Spins, and Parities of Nuclear Levels in the 6-9-MeV Region Excited by Neutron Capture γ Rays NUCLEAR REACTIONS 50Cr, 62Ni, 74Ge, 75As, 109Ag, 112Cd, 139La, 141Pr, 205Tl, 208Pb(γ, γ'), E=6-9 MeV; measured σ(Eγ', θ(γ')). 50Cr, 62Ni, 74Ge, 75As, 109Ag, 112Cd, 139La, 141Pr, 205Tl, 208Pb deduced levels, J, π, level-width.
doi: 10.1103/PhysRevC.2.1144
1970MO30 Phys.Rev. C2, 1938 (1970) Use of the (γ, γ') Reaction for Studying the Energy Levels of 139La NUCLEAR REACTIONS 139La(γ, γ'), (γ, γ), E=3-8 MeV; measured σ(Eγ', θ). 139La deduced levels, J, π, level-width.
doi: 10.1103/PhysRevC.2.1938
1970MO32 Phys.Rev. C2, 2217 (1970) Study of the Energy Levels of 74Ge Using Nuclear Photoexcitation NUCLEAR REACTIONS 74Ge(γ, γ), (γ, γ'), E < 6 MeV; measured σ(θ), σ(Eγ', θ), γ-linear polarization. 74Ge deduced levels, J, π, level-width, γ-mixing, γ-branching.
doi: 10.1103/PhysRevC.2.2217
1969MO11 Phys.Rev. 178, 1961 (1969) Use of the (γ, γ') Reaction for Studying 141Pr Levels NUCLEAR REACTIONS 141Pr(γ, γ'), E approx 7.6 MeV [from Fe(n, γ)]; measured σ(Eγ', θ). 141Pr deduced resonances, levels, J, π, level-width.
doi: 10.1103/PhysRev.178.1961
1969MO17 Phys.Rev. 182, 1236 (1969) Study of the Energy Levels of 205Tl Using the (γ, γ') Reaction NUCLEAR REACTIONS 205Tl(γ, γ'), E=7.632, 7.646, 9.298 MeV; measured σ(Eγ', θ). 205Tl deduced levels, J, π, level-width, γ-branching. Ge(Li) detector.
doi: 10.1103/PhysRev.182.1236
1969MO27 Phys.Rev. 188, 1765 (1969) Use of the (γ, γ') Reaction for Studying the Energy Levels of 75As NUCLEAR REACTIONS 75As(γ, γ), (γ, γ'), E < 8 MeV; measured σ(Eγ', θ(γ')). 75As deduced levels, J, π, level-width, branching ratios.
doi: 10.1103/PhysRev.188.1765
1969TE01 Phys.Rev. 177, 1595 (1969) J.Tenenbaum, R.Moreh, Y.Wand, B.Arad, G.Ben-David Study of the Level Structure of 47Ti Using 46Ti(n, γ) Reaction NUCLEAR REACTIONS 46Ti(n, γ), E=thermal; measured Eγ, Iγ, γγ-coin, γγ(θ); deduced Q. 47Ti deduced levels, J, enriched target, Ge(Li) detector.
doi: 10.1103/PhysRev.177.1595
1969TE06 Phys.Rev. 187, 1403 (1969) J.Tenenbaum, R.Moreh, Y.Wand, G.Ben-David Study of the Level Structure of 48Ti Using the 47Ti(n, γ) Reaction NUCLEAR REACTIONS 47Ti(n, γ), E=thermal; measured Eγ, Iγ, γγ(θ); deduced Q. 48Ti deduced levels, J, π, γ-mixing.
doi: 10.1103/PhysRev.187.1403
1968MO03 Nucl.Phys. A107, 236 (1968) Decay of 23Ne RADIOACTIVITY 23Ne [from 22Ne(n, γ)]; measured Eγ, γγ-coin. 23Na deduced levels. Natural target, Ge(Li) detector.
doi: 10.1016/0375-9474(68)90740-9
1968MO06 Phys.Letters 26B, 579 (1968); Erratum Phys.Letters 27B, 377 (1968) M1 and E1 Resonant Scattering of Gamma Rays from Neutron Capture in Iron NUCLEAR REACTIONS 62Ni, 112Cd, 141Pr, 203Tl, 208Pb(γ, γ), E=7.2-7.7 MeV; measured γγ-coin, γ linear polarization correlation. 62Ni, 112Cd, 141Pr, 203Tl, 208Pb levels deduced J, π, γ-multipolarity.
doi: 10.1016/0370-2693(68)90418-8
1968SH06 Nucl.Phys. A110, 204 (1968) Calculated Gamma Transitions Between 18O Levels
doi: 10.1016/0375-9474(68)90692-1
1967MO09 Nucl.Phys. A97, 106(1967) Gamma Decay of the 5.25 and 5.37 MeV Levels of 18O NUCLEAR REACTIONS 17O(d, pγ)18O, E = 5.02 MeV; measured p-γ coin. Enriched target.
doi: 10.1016/0375-9474(67)90773-7
1967TE04 IA-1102 (1967) J.Tenenbaum, B.Arad, G.Ben-David, R.Moreh Neutron Capture Gamma Rays from Natural Titanium NUCLEAR REACTIONS Ti(n, γ), E not given; measured Eγ, Iγ. 47,48,49,50,51Ti deduced transitions. Ge(Li) detector.
1965MO16 Nucl.Phys. 74, 403(1965) The Level Structure of 18O and 19O by Stripping Reactions NUCLEAR REACTIONS 16,17,18O(d, p), E = 5.56 MeV; measured σ(Ep, θ), Q. 17,18,19O deduced levels. Enriched targets.
doi: 10.1016/0029-5582(65)90091-X
1965MO19 Nucl.Phys. 70, 293(1965) Study of the (t, p) Reaction on O16, O17 and O18 Using 5.55 MeV Tritons NUCLEAR REACTIONS 16,17,18O(t, p), E = 5.55 MeV; measured σ (θ, Ep). 18,19,20O deduced levels, J, π. Enriched targets.
doi: 10.1016/0029-5582(65)90525-0
1964MO24 Proc.Phys.Soc.(London) 84, 330 (1964) The Energy Level Structure of 19O NUCLEAR REACTIONS 17O(t, p), E=5.55 MeV; measured reaction products, Ep, Ip. 19O; deduced σ(θ), energy levels, J, π.
doi: 10.1088/0370-1328/84/2/117
1964MO25 Proc.Phys.Soc.(London) 84, 332 (1964); Erratum Proc.Phys.Soc.(London) 84, 835 (1964) The Spin and Parity of the 5.37 MeV Level in 18O NUCLEAR REACTIONS 17,18O(d, p), E=5.55 MeV; measured reaction products, Ep, Ip. 18O; deduced σ(θ), level energy, J, π.
doi: 10.1088/0370-1328/84/2/118
1963BI27 Nucl.Phys. 41, 58 (1963) M.Birk, G.Goldring, P.Hillman, R.Moreh Charge symmetry in the mirror reactions 6Li(d, p)7Li and 6Li(d, n)7Be NUCLEAR REACTIONS 6Li(d, n), 6Li(d, p), E=326.1 keV-3.2 MeV; measured products, 7Li, Eπ, Iπ; deduced σ(θ). Data were imported from EXFOR entry A1354.
doi: 10.1016/0029-5582(63)90478-4
1962MO08 Nuclear Phys. 36, 315 (1962) The O17(t, p)O19 Reaction in a Nuclear Reactor NUCLEAR STRUCTURE 17O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90454-6
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