NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = N.M.Hintz Found 68 matches. 2001MI33 Phys.Rev. C64, 054608 (2001) D.N.Mihailidis, N.M.Hintz, A.Sethi, E.J.Stephenson High Spin Two-Neutron-Hole States via the 208Pb(p, t)206Pb Reaction at 120 MeV NUCLEAR REACTIONS 208Pb(polarized p, t), E=120 MeV; measured σ(E, θ), Ay(E, θ). 206Pb deduced levels, J, π, spectroscopic factors. DWBA analysis, comparison with shell model predictions.
doi: 10.1103/PhysRevC.64.054608
1995MA44 Phys.Rev. C52, 291 (1995) A.M.Mack, N.M.Hintz, D.Cook, M.A.Franey, J.Amann, M.Barlett, G.W.Hoffmann, G.Pauletta, D.Ciskowski, M.Purcell Proton Scattering by 206,207,208Pb at 650 MeV: Phenomenological analysis NUCLEAR REACTIONS 206,207,208Pb(polarized p, p), (polarized p, p'), E=650 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters. 206,208Pb levels deduced B(λ), neutron-proton matrix element ratios. Phenomenological analysis.
doi: 10.1103/PhysRevC.52.291
1994ST03 Phys.Rev. C49, 2118 (1994) Extraction of Neutron Densities from Elastic Proton Scattering by 206,207,208Pb at 650 MeV NUCLEAR REACTIONS 40Ca(polarized p, p), E=650 MeV; analyzed σ(θ), analyzing power, spin rotation parameter vs θ; deduced t-matrix. 206,207,208Pb(polarized p, p), E=650 MeV; analyzed σ(θ), analyzing power data. 206,207,208Pb deduced neutron densities differences.
doi: 10.1103/PhysRevC.49.2118
1994ST07 Phys.Rev. C48, 2479 (1994) Constraints on the Nuclear Compressibility from Analysis of the Breathing Mode and Density Differences of Lead Isotopes NUCLEAR STRUCTURE 208,206,207Pb; calculated charge, neutron densities differences; deduced constraints on nuclear compressibility parameter. Skyrme-type interactions.
doi: 10.1103/PhysRevC.48.2479
1992HI01 Phys.Rev. C45, 601 (1992) N.M.Hintz, X.H.Yang, M.Gazzaly, S.J.Seestrom-Morris, C.L.Morris, D.C.Cook, A.M.Mack, J.W.McDonald, S.Mordechai, D.S.Oakley, C.F.Moore, M.Lynker, J.D.Zumbro Determination of Neutron and Proton Multipole Matrix Elements in 208Pb from π- and π+ Scattering at 180 MeV NUCLEAR REACTIONS 208Pb(π+, π+), (π+, π+'), (π-, π-'), (π-, π-), E=180 MeV; measured σ(θ). 208Pb levels deduced neutron, proton multipole matrix elements.
doi: 10.1103/PhysRevC.45.601
1992HI04 Phys.Rev. C45, 1098 (1992) N.M.Hintz, A.M.Lallena, A.Sethi Modifications of the Tensor and Spin-orbit Interactions and the Stretched States in 208Pb NUCLEAR REACTIONS 208Pb(p, p'), E=318 MeV; analyzed σ(θ). 208Pb(e, e'), E=335.4 MeV; analyzed σ(θ); deduced quenching factors, effective masses.
doi: 10.1103/PhysRevC.45.1098
1991BR27 Phys.Rev. C44, 2653 (1991) Proton-Nucleus Scattering and Density Dependent Meson Masses in the Nucleus NUCLEAR REACTIONS 208Pb(p, p), E=796 MeV; 208Pb, 58Ni, 40Ca(p, p), E=498 MeV; calculated σ(θ); deduced density dependent meson masses role. Relativistic impulse approximation.
doi: 10.1103/PhysRevC.44.2653
1991SE04 Phys.Rev. C44, 700 (1991) A.Sethi, N.M.Hintz, D.N.Mihailidis, A.M.Mack, M.Gazzaly, K.W.Jones, G.Pauletta, L.Santi, D.Goutte Inelastic Proton Scattering from Pt Isotopes and the Interacting Boson Model NUCLEAR REACTIONS 194,196Pt(polarized p, p), (polarized p, p'), E=647 MeV; measured σ(θ), analyzing power vs θ; deduced model parameters. 194,196Pt levels deduced deformation parameters, E2, E4 matrix elements, B(λ). Coupled-channels analysis, interacting boson model.
doi: 10.1103/PhysRevC.44.700
1988HI01 Phys.Rev. C37, 692 (1988) N.M.Hintz, D.Cook, M.Gazzaly, M.A.Franey, M.L.Barlett, G.W.Hoffmann, R.Fergerson, J.McGill, G.Pauletta, R.L.Boudrie, J.B.McClelland, K.W.Jones Energy Dependence of Neutron-Proton Matrix Element Ratios Derived from 25-800 MeV Energy Proton Scattering NUCLEAR REACTIONS 58Ni, 208Pb(p, p), (p, p'), E=318-800 MeV; measured σ(θ); deduced potential deformation lengths. 40Ca, 58Ni, 208Pb levels deduced neutron, proton matrix element ratio. Other data input.
doi: 10.1103/PhysRevC.37.692
1987CO06 Phys.Rev. C35, 456 (1987) D.Cook, N.M.Hintz, M.M.Gazzaly, G.Pauletta, R.W.Fergerson, G.W.Hoffmann, J.B.McClelland, K.W.Jones High Spin States in 208Pb NUCLEAR REACTIONS 208Pb(p, p), (p, p'), E=318 MeV; measured σ(θ). 208Pb levels deduced proton, electron quenching factor differences. Enriched target. DWIA analyses.
doi: 10.1103/PhysRevC.35.456
1987GI08 Phys.Rev. C36, 2436 (1987) J.N.Ginocchio, G.Wenes, R.D.Amado, D.C.Cook, N.M.Hintz, M.M.Gazzaly Medium Energy Proton Scattering from 154Gd and the Interacting Boson Model of Nuclei NUCLEAR REACTIONS 154Gd(p, p'), E=650 MeV; measured σ(θ). 154Gd levels deduced B(λ). Interacting boson model quadrupole hadronic transition operator, compared to boson electromagnetic operator.
doi: 10.1103/PhysRevC.36.2436
1984HI10 Phys.Rev. C30, 1976 (1984) N.M.Hintz, M.A.Franey, M.M.Gazzaly, D.Cook, G.S.Kyle, D.Dehnhard, S.J.Seestrom-Morris, G.W.Hoffmann, M.Barlett, G.S.Blanpied, J.A.McGill, J.B.McClelland, R.L.Boudrie, F.Irom, G.Pauletta High Spin States in 28Si and 58Ni NUCLEAR REACTIONS 28Si, 58Ni(p, p'), E=333, 498, 800 MeV; measured σ(θ), σ(Ep). 28Si, 58Ni levels deduced transition densities. DWIA, other (p, p'), (e, e') data analysis.
doi: 10.1103/PhysRevC.30.1976
1983GA09 Phys.Rev. C28, 294 (1983) M.M.Gazzaly, N.M.Hintz, M.A.Franey, J.Dubach, W.C.Haxton Neutron and Proton Transition Matrix Elements for 90Zr from a Microscopic Analysis of 0.8 GeV Proton Inelastic Scattering NUCLEAR REACTIONS 90Zr(p, p'), E=0.8 GeV; measured absolute σ(θ). 90Zr levels deduced core to total deformation parameter ratio, enhancement factors, neutron, proton matrix element ratios. DWIA, shell model transition densities.
doi: 10.1103/PhysRevC.28.294
1982BL01 Phys.Rev. C25, 422 (1982) G.S.Blanpied, N.M.Hintz, G.S.Kyle, M.A.Franey, S.J.Seestrom-Morris, R.K.Owen, J.W.Palm, D.Dehnhard, M.L.Barlett, C.J.Harvey, G.W.Hoffmann, J.A.McGill, R.P.Liljestrand, L.Ray Elastic and Inelastic Scattering of 0.8 GeV Protons from 24Mg and 26Mg NUCLEAR REACTIONS 24,26Mg(p, p), (p, p'), E=0.8 GeV; measured σ(θ). 24,26Mg deduced deformation lengths, multipole moments. Optical model, DWBA, coupled-channels analyses, rotational model.
doi: 10.1103/PhysRevC.25.422
1982GA02 Phys.Rev. C25, 408 (1982) M.M.Gazzaly, N.M.Hintz, G.S.Kyle, R.K.Owen, G.W.Hoffmann, M.Barlett, G.Blanpied Neutron-Proton Decomposition of Transition Matrix Elements from a Comparison of 800 MeV Proton Scattering with Electromagnetic Methods NUCLEAR REACTIONS 90Zr, 120Sn, 144Sm, 208Pb(p, p'), E=800 MeV; measured σ(θ). 90Zr, 120Sn, 144Sm, 208Pb, 40Ca, 58Ni deduced deformation lengths, neutron, proton matrix element ratios. Optical model, DWBA analyses.
doi: 10.1103/PhysRevC.25.408
1982SE12 Phys.Rev. C26, 2131 (1982) S.J.Seestrom-Morris, J.M.Moss, J.B.McClelland, W.D.Cornelius, T.A.Carey, N.M.Hintz, M.Gazzaly, M.A.Franey, S.Nanda, B.Aas Spin-Flip Probability in 12C(p(pol), p'(pol))12C at 397 MeV NUCLEAR REACTIONS 12C(polarized p, p'), E=397 MeV; measured spin-flip probability. DWBA, effective interaction, Cohen-Kurath wave functions.
doi: 10.1103/PhysRevC.26.2131
1981HO20 Phys.Rev. C24, 541 (1981) G.W.Hoffmann, L.Ray, M.Barlett, W.R.Coker, J.McGill, G.S.Adams, G.J.Igo, F.Irom, A.T.M.Wang, C.A.Whitten, Jr., R.L.Boudrie, J.F.Amann, C.Glashausser, N.M.Hintz, G.S.Kyle, G.S.Blanpied A(y)(θ) for p(pol) + 208Pb Elastic Scattering at 0.8 GeV and a Test of Multiple Scattering Theory NUCLEAR REACTIONS 208Pb(polarized p, p), E=0.8 GeV; measured analyzing power vs θ. Microscopic optical model, second-order Kerman-McManus-Thaler multiple scattering approach, electromagnetic spin-orbit term.
doi: 10.1103/PhysRevC.24.541
1980BA30 Phys.Rev. C22, 1168 (1980) M.L.Bartlett, J.A.McGill, L.Ray, M.M.Bartlett, G.W.Hoffmann, N.M.Hintz, G.S.Kyle, M.A.Franey, G.Blanpied Proton Scattering from 154Sm and 176Yb at 0.8 GeV NUCLEAR REACTIONS 154Sm, 176Yb(p, p), (p, p'), E=0.8 GeV; measured σ(θ); deduced optical model parameters. 154Sm, 176Yb levels deduced deformation lengths. DWBA, coupled channel analysis, rotational model. Enriched targets.
doi: 10.1103/PhysRevC.22.1168
1980HO09 Phys.Rev. C21, 1488 (1980) G.W.Hoffman, L.Ray, M.Barlett, J.McGill, G.S.Adams, G.J.Igo, F.Irom, A.T.M.Wang, C.A.Whitten, Jr., R.L.Boudrie, J.F.Amann, C.Glashausser, N.M.Hintz, G.S.Kyle, G.S.Blanpied 0.8 GeV p + 208Pb Elastic Scattering and the Quantity Δr(np) NUCLEAR REACTIONS 208Pb(p, p), E=0.8 GeV; measured σ(θ); deduced neutron, proton rms radius difference. Microscopic optical model analysis.
doi: 10.1103/PhysRevC.21.1488
1980KY01 Phys.Lett. 91B, 353 (1980) G.S.Kyle, N.M.Hintz, M.S.Oothoudt, M.Kaletka, P.M.Lang, H.Nann, K.K.Seth, D.K.McDaniels, P.M.Varghese, T.Kozlowski, D.G.Madland, C.L.Morris, J.C.Pratt, J.E.Spencer, N.Tanaka, H.A.Thiessen, G.S.Blanpied, G.W.Hoffmann, R.P.Liljestrand, J.C.Fong, G.Igo, R.J.Ridge, C.A.Whitten, Jr. Elastic and Inelastic Scattering of 800 MeV Protons by 58Ni NUCLEAR REACTIONS 58Ni(p, p), (p, p'), E=800 MeV; measured σ(θ). 58Ni levels deduced deformation lengths. DWBA analysis.
doi: 10.1016/0370-2693(80)90994-6
1979BL04 Phys.Rev. C20, 1490 (1979) G.Blanpied, N.M.Hintz, G.S.Kyle, J.W.Palm, R.Liljestrand, M.Barlett, C.Harvey, G.W.Hoffmann, L.Ray, D.G.Madland Proton Scattering from 24Mg at 0.8 GeV NUCLEAR REACTIONS 24Mg(p, p'), E=0.8 GeV; measured σ(θ). 24Mg levels deduced deformation length. Optical model, DWBA, coupled-channels, symmetric, asymmetric rotator model analyses.
doi: 10.1103/PhysRevC.20.1490
1979IG01 Phys.Lett. 81B, 151 (1979) G.Igo, G.S.Adams, T.S.Bauer, G.Pauletta, C.A.Whitten, Jr., A.Wriekat, G.W.Hoffmann, G.S.Blanpied, W.R.Coker, C.Harvey, R.P.Liljestrand, L.Ray, J.E.Spencer, H.A.Thiessen, C.Glashausser, N.M.Hintz, M.A.Oothoudt, H.Nann, K.K.Seth, B.E.Wood, D.K.McDaniels, M.Gazzaly Elastic Differential Cross Sections and Analyzing Powers for Polarized p + 40,42,44,48Ca at 0.8 GeV NUCLEAR REACTIONS 40,42,44,48Ca(polarized p, p), E=0.8 GeV; measured σ(θ), A(θ); deduced rms radii of neutrons. Kerman-McManus-Thaler optical potential analysis.
doi: 10.1016/0370-2693(79)90510-0
1979RA15 Phys.Lett. 83B, 275 (1979) L.Ray, T.Kozlowski, D.G.Madland, C.L.Morris, J.C.Pratt, J.E.Spencer, N.Tanaka, H.A.Thiessen, G.S.Kyle, N.M.Hintz, M.A.Oothoudt, P.M.Lang, H.Nann, K.K.Seth, D.K.McDaniels, P.M.Varghese, G.S.Blanpied, G.W.Hoffmann, R.P.Liljestrand, J.C.Fong, G.Igo, R.J.Ridge, R.M.Rolfe, C.A.Whitten, Jr. Coupled-Channels Effects in 0.8 GeV Proton Inelastic Scattering from 58Ni NUCLEAR REACTIONS 58Ni(p, p'), E=0.8 GeV; calculated σ(θ). Coupled channel, DWBA calculations with multistep, multiphonon mixing.
doi: 10.1016/0370-2693(79)91106-7
1978BL02 Phys.Rev. C18, 1436 (1978) G.S.Blanpied, W.R.Coker, R.P.Liljestrand, G.W.Hoffmann, L.Ray, D.Madland, C.L.Morris, J.C.Pratt, J.E.Spencer, H.A.Thiessen, T.Kozlowski, N.M.Hintz, G.S.Kyle, M.A.Oothoudt, T.S.Bauer, G.Igo, R.J.Ridge, C.A.Whitten, Jr., P.M.Lang, H.Nann, K.K.Seth Proton Elastic and Inelastic Scattering at 0.8 GeV from 12,13C and 208Pb NUCLEAR REACTIONS 12,13C, 208Pb(p, p'), E=0.8 GeV; measured σ(θ). 12,13C, 208Pb deduced deformation length. Optical potential, DWBA analysis. Enriched targets.
doi: 10.1103/PhysRevC.18.1436
1978HO05 Phys.Rev.Lett. 40, 1256 (1978) G.W.Hoffman, G.S.Blanpied, W.R.Coker, R.P.Liljestrand, N.M.Hintz, M.A.Oothoudt, T.S.Bauer, G.Igo, G.Pauletta, J.Soukup, C.A.Whitten, Jr., D.Madland, J.C.Pratt, L.Ray, J.E.Spencer, H.A.Thiessen, H.Nann, K.K.Seth, C.Glashausser, D.K.McDaniels, J.Tinsley, P.Varghese Analyzing Power in Proton-Nucleus Elastic Scattering at 0.8 GeV NUCLEAR REACTIONS 12C, 58Ni, 90Zr, 208Pb(polarized p, p), E=0.8 GeV; measured A(θ), σ(θ).
doi: 10.1103/PhysRevLett.40.1256
1978HO12 Phys.Lett. 76B, 383 (1978) G.W.Hoffmann, G.S.Blanpied, W.R.Coker, R.P.Liljestrand, L.Ray, J.E.Spencer, H.A.Thiessen, N.M.Hintz, M.A.Oothoudt, T.S.Bauer, G.Igo, G.Pauletta, J.Soukup, C.A.Whitten, Jr., H.Nann, K.K.Seth, C.Glashausser, D.K.McDaniels, J.Tinsley, P.Varghese Analysis of Elastic Scattering of 0.8 GeV Polarized Protons from 116Sn and 124Sn NUCLEAR REACTIONS 116,124Sn(polarized p, p), E=800 MeV; analyzed A(θ), σ(θ). Spin-dependent Kerman-McManus-Thaler formalism.
doi: 10.1016/0370-2693(78)90888-2
1978HO18 Phys.Lett. 79B, 376 (1978) G.W.Hoffmann, G.S.Blanpied, W.R.Coker, C.Harvey, R.P.Liljestrand, G.S.Adams, T.S.Bauer, G.Igo, G.Pauletta, C.A.Whitten, Jr., A.Wriekat, L.Ray, J.E.Spencer, H.A.Thiessen, H.Nann, K.K.Seth, N.M.Hintz, G.Kyle, M.A.Oothoudt, B.E.Wood, D.K.McDaniels, C.Glashausser, M.Gazzaly Elastic Differential Cross Sections and Analyzing Powers for p + 54Fe, 58,64Ni at 800 MeV NUCLEAR REACTIONS 54Fe, 58,64Ni(polarized p, p), E=800 MeV; measured σ(θ); deduced neutron density distribution. Approximately model-independent analysis.
doi: 10.1016/0370-2693(78)90386-6
1977BL09 Phys.Rev.Lett. 39, 1447 (1977); Erratum Phys.Rev.Lett. 40, 420 (1978) G.S.Blanpied, W.R.Coker, R.P.Liljestrand, L.Ray, G.W.Hoffman, D.Madland, C.L.Morris, J.C.Pratt, J.E.Spencer, H.A.Thiessen, N.M.Hintz, G.S.Kyle, M.A.Oothoudt, T.S.Bauer, J.C.Fong, G.Igo, R.J.Ridge, C.A.Whitten, Jr., Y.Kozlowski, D.K.McDaniels, P.Varghese, P.M.Lang, H.Nann, K.K.Seth, C.Glashausser Elastic Scattering of 0.8-GeV Protons from 12C, 58Ni, and 208Pb NUCLEAR REACTIONS 12C, 58Ni, 208Pb(p, p), E=0.8 GeV; measured σ(θ).
doi: 10.1103/PhysRevLett.39.1447
1976SH15 Phys.Rev. C13, 2288 (1976) Osmium Isotopes with the (p, t) Reactions NUCLEAR REACTIONS 186,187,189,190,192Os(p, t), E=19 MeV; measured σ(Et, θ). 184,185,187,188,190Os deduced levels, K, L, J, π. Pairing plus DWBA.
doi: 10.1103/PhysRevC.13.2288
1975KU14 Nucl.Phys. A247, 152 (1975) A Study of the Nucleus 107Ag in the Core-Excitation Model with the (p, t) and (τ, d) Reactions NUCLEAR REACTIONS 107,109Ag, 104,105,106,108,110Pd(p, t), E=19.000 MeV; measured σ(Et, θ). 107Ag(p, t), E=19.000 MeV; deduced Q. 106Pd, 107Ag(3He, d), E=18.000 MeV; measured σ(Ed, θ). 107Ag deduced levels, J, π, L, S. Enriched, natural targets.
doi: 10.1016/0375-9474(75)90283-3
1975TA12 Phys.Rev. C12, 108 (1975) H.Taketani, H.L.Sharma, N.M.Hintz Shape Transitional Aspects of Odd-A Eu Isotopes Studied by the (p, t) Reaction NUCLEAR REACTIONS 151,153Eu(p, t), E=18.5, 19.0 MeV; measured σ(Et, θ); deduced Q. 149,151Eu deduced levels, J, π, L.
doi: 10.1103/PhysRevC.12.108
1975WE14 Nucl.Instrum.Methods 124, 317 (1975) D.J.Weber, N.M.Hintz, D.Dehnhard Equilibrium Charge-State Distributions for 16O Ions at 20-65 MeV NUCLEAR REACTIONS Au(16O, 16O), E=20-65 MeV; measured charge-state distribution.
doi: 10.1016/0029-554X(75)90578-9
1973KR20 Nucl.Phys. A216, 549 (1973) T.P.Krick, N.M.Hintz, D.Dehnhard The Distribution of Electric Multipole Strength in 19F from Inelastic Scattering of 25 MeV α-Particles NUCLEAR REACTIONS 19F(α, α'), (α, α), E=25.0 MeV; measured σ(θ). Deduced optical potential. 19F levels deduced J, π, β(L) deformation parameters by DWBA, coupled channels analyses. Natural target.
doi: 10.1016/0375-9474(73)90169-3
1973OO01 Nucl.Phys. A213, 221 (1973) The (p, t) Reactions on Nuclei in the Rare Earth Region NUCLEAR REACTIONS 168,170,171,172,173,174,176Yb, 178,180Hf, Gd, Dy, Er, Hf, Ta, W, Os, Au(p, t), 176Yb(p, p'), E=19 MeV; measured σ(Et, θ), Q. 166,168,169,170,171,172,174Yb, 176,178Hf deduced levels, J, π. 112,113,114,116Cd, 154,155,156,157,158,160Gd, 160,161,162,163,164Dy, 164,166,167,168,170Er, 176,177,179Hf, 181Ta, 182,183,184,186W, 188,189,190,192Os(p, t), E=19 MeV; measured Q. Enriched, natural targets.
doi: 10.1016/0375-9474(73)90148-6
1973SH09 Phys.Rev. C7, 2567 (1973) H.L.Sharma, R.Seltz, N.M.Hintz Search for an Excited Rotational Band in 98Mo with the (p, t) Reaction NUCLEAR REACTIONS 100Mo(p, t), E=19 MeV; measured σ(Et, θ). 98Mo deduced levels, L, J, π.
doi: 10.1103/PhysRevC.7.2567
1973SH18 Phys.Rev.Lett. 31, 1517 (1973) New K = 0 Bands and Two-Phonon Gamma Vibrations in 188Os and 190Os NUCLEAR REACTIONS 190,192Os(p, t), E=19.0 MeV; measured σ(Et, θ). 188,190Os deduced levels, J, π, B(E2).
doi: 10.1103/PhysRevLett.31.1517
1973SO12 Nucl.Phys. A217, 438 (1973) A.Sourkes, H.Ohnuma, N.M.Hintz A Study of 50V Using the Direct Reactions 49Ti(3He, d) and 51V(d, t) NUCLEAR REACTIONS 49Ti(3He, d), 51V(d, t), E(3He)=22 MeV, Ed=19.5 MeV; measured σ(Ed, θ), σ(Et, θ). 50V deduced levels, L, S. Enriched target.
doi: 10.1016/0375-9474(73)90404-1
1973TA28 Proc.Int.Conf.Nuclear Physics, Munich, J.de Boer, H.J.Mang, Eds., North-Holland Publ.Co., Amsterdam, Vol.1, p.229 (1973) H.Taketani, H.L.Sharma, N.M.Hintz Shape Transition Observed in the Odd-A Eu Isotopes by (p, t) and (3He, d) Reactions
1972DE47 Nucl.Phys. A195, 385 (1972) The (p, t) Reaction on Even Isotopes of Sm NUCLEAR REACTIONS 148,150,152,154Sm(p, t), E=19.00 MeV; measured σ(Et, θ), Q. 146,148,150,152Sm deduced levels, J, π. Enriched targets.
doi: 10.1016/0375-9474(72)91067-6
1972KU31 COO-1265-126, p.77 (1972) A Study of the Nucleus 107Ag in the Core-Excitation Model via the (p, t) and (3He, d) Reactions NUCLEAR REACTIONS 109Ag(p, t), 106Pd(3He, d), E not given; measured σ(θ). 107Ag(p, t), E not given; measured Q. 107Ag deduced levels, J, π, S.
1970DE06 Phys.Rev. C1, 460 (1970) Octupole and Quadrupole Transition Rates in F19 from Scattering of 15-MeV Deuterons NUCLEAR REACTIONS 19F(d, d), (d, d'), E=15 MeV; measured σ(Ed', θ). 19F levels deduced B(EL), β(L).
doi: 10.1103/PhysRevC.1.460
1970DE16 Phys.Rev.Lett. 25, 44 (1970) Excited Rotational Band in 'Spherical' 150Sm NUCLEAR REACTIONS 152Sm(p, t), E=10, 19 MeV; measured σ(Et, θ). 150Sm deduced levels, J, π, L, level spacings.
doi: 10.1103/PhysRevLett.25.44
1970OO01 Phys.Lett. 32B, 270 (1970); Priv.Comm. (1973) M.Oothoudt, N.M.Hintz, P.Vedelsby A Pairing Phase Transition in the Yb Isotopes NUCLEAR REACTIONS 170,172,174,176Yb(p, t), E=19 MeV; measured σ(Et, θ). 168,170,172,174Yb deduced L=0 transition strengths.
doi: 10.1016/0370-2693(70)90525-3
1969WA04 Priv.Comm. (1969) R.A.Wallen, H.Ohnuma, N.M.Hintz NUCLEAR STRUCTURE 48Sc; measured not abstracted; deduced nuclear properties.
1967JO03 Phys.Rev. 153, 1169 (1967) Nuclear Level-Density Fluctuations and Tests of the Compound Statistical Model NUCLEAR STRUCTURE 60Ni, 64Zn, 62Ni, 66Zn, 65Cu, 63Cu, 61Cu; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.153.1169
1967RE02 Phys.Rev. 153, 1283 (1967) G.M.Reynolds, J.R.Maxwell, N.M.Hintz Study of the (p, t) Reaction on the Pb Isotopes NUCLEAR STRUCTURE 204Pb, 206Pb, 205Pb, 202Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.153.1283
1966MA30 Phys.Rev. 151, 1000 (1966) J.R.Maxwell, G.M.Reynolds, N.M.Hintz (p, t) Reaction on the Isotopes of Sm and Nd, N=88 and 90 NUCLEAR STRUCTURE 150Sm, 146Nd, 148Sm, 148Nd; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.151.1000
1966MA35 Phys.Letters 22, 454 (1966) J.R.Maxwell, G.M.Reynolds, N.M.Hintz Three L = 0 Transitions in the 57Fe(p, t)55Fe Reaction NUCLEAR STRUCTURE 55Fe; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(66)91224-8
1965BA20 Phys.Rev. 139, B830 (1965) G.Bassani, N.M.Hintz, C.D.Kavaloski, J.R.Maxwell, G.M.Reynolds (p, t) Ground-State L = 0 Transitions in the Even Isotopes of Sn and Cd at 40 MeV, N = 62 to 74 NUCLEAR STRUCTURE 116Sn, 118Sn, 114Sn, 114Cd, 112Sn, 122Sn, 120Sn, 108Cd, 112Cd, 110Sn, 110Cd; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.139.B830
1965JO16 Univ.Minnesota Linear Accelerator Lab. Annual Progr.Rept., p. 54 (1965) Inelastic Proton Scattering at 10 MeV and the Statistical Model NUCLEAR STRUCTURE 60Ni, 58Ni, 64Zn, 63Cu, 66Zn, 65Cu; measured not abstracted; deduced nuclear properties.
1965MA47 Univ.Minn.Linear Accelerator Lab.Annual Progr.Rept., p.88 (1965) J.R.Maxwell, G.M.Reynolds, N.M.Hintz The (p, t) Reaction on the Isotopes of Sm and Nd, N=88 and 90 NUCLEAR STRUCTURE 150Sm, 148Nd, 148Sm, 146Nd; measured not abstracted; deduced nuclear properties.
1964AD05 Nucl.Phys. 59, 601 (1964) Angular correlations in the reaction C12(p, p'γ)C12* at 40 MeV NUCLEAR REACTIONS 12C(p, p'), E=39.3 MeV; measured reaction products, Eγ, Iγ; deduced inelastic proton-gamma angular correlation. Comparison with DWBA calculations.
doi: 10.1016/0029-5582(64)90037-9
1964BA34 Phys. Rev. 136, B1006 (1964) G.Bassani, N.M.Hintz, C.D.Kavaloski Nuclear Structure Information from the (p, t) Reaction, A = 46 to A = 70 NUCLEAR STRUCTURE 51Cr, 53Cr, 53Mn, 56Fe, 52Fe, 54Fe, 46Ti, 50Cr, 48Ti, 49V, 44Ti, 66Zn, 62Zn, 63Cu, 64Zn, 61Cu, 62Ni, 56Ni, 57Co, 60Ni, 58Ni, 68Zn; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.136.B1006
1964SH07 Bull.Am.Phys.Soc. 9, No.4, 391, BA16 (1964) (p, d) Reactions in 1 P3/2 Shell Nuclei NUCLEAR STRUCTURE 6Li, 9Be, 12C, 11B, 7Li, 10B; measured not abstracted; deduced nuclear properties.
1964ST15 Phys.Rev. 135, B330 (1964) Inelastic Proton Scattering at 40 MeV NUCLEAR STRUCTURE 27Al, 208Pb, 207Pb, 206Pb, 12C, 7Li, 63Cu, 54Fe, 56Fe, 58Ni, 60Ni, 40Ca; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.135.B330
1963KA26 Phys.Rev. 132, 813 (1963) C.D.Kavaloski, G.Bassani, N.M.Hintz (p, d) Nuclear Structure Studies on Nuclei between A=12 and A=48 NUCLEAR STRUCTURE 12C, 16O, 23Mg, 24Mg, 47Ti, 39Ca, 31S, 33S; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.132.813
1963RE09 Nucl.Phys. 44, 338 (1963) N.W.Reay, N.M.Hintz, L.L.Lee, Jr. Radiative Capture Above the Giant Resonance in C12 NUCLEAR STRUCTURE 7Li, 11B; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90032-4
1962BA35 Bull.Am.Phys.Soc. 7, No.8, 551, U1 (1962) G.Bassani, C.D.Kavaloski, N.M.Hintz (p, t) Reactions on Medium A Nuclei at 40 MeV NUCLEAR STRUCTURE 56Fe, 55Mn, 54Fe, 48Ti, 65Cu, 63Cu, 58Ni, 60Ni; measured not abstracted; deduced nuclear properties.
1962KA19 Bull.Am.Phys.Soc. 7, No.9, 551, U2 (1962) C.D.Kavaloski, G.Bassani, N.M.Hintz (p, d) Nuclear-Structure Studies at 40 MeV in the Region 16 ≤ A ≤ 40 NUCLEAR STRUCTURE 24Mg, 23Mg, 33S, 31S, 39Ca; measured not abstracted; deduced nuclear properties.
1961HI02 Bull.Am.Phys.Soc. 6, No.3, 260, KA12 (1961) N.M.Hintz, L.L.Lee, Jr., T.Stovall Inelastic Scattering of Protons at 40 MeV. I NUCLEAR STRUCTURE 12C, 24Mg; measured not abstracted; deduced nuclear properties.
1961LE04 Bull.Am.Phys.Soc. 6, No. 3, 260, KA13 (1961) L.L.Lee, Jr., N.M.Hintz, C.D.Kavaloski, T.Stovall Inelastic Scattering of Protons at 40 MeV. II NUCLEAR STRUCTURE 60Ni, 58Ni, 56Fe; measured not abstracted; deduced nuclear properties.
1960ME14 Proc.Intern.Conf.Nuclear Structure, Kingston, Canada, D.A.Bromley, E.W.Vogt, Editors, Univ.Of Toronto Press, p.231 (1960) Charged Particle and Total Reaction Cross Sections for Protons at 9.85 MeV
1960ME15 Phys.Rev.Lett. 5, 207 (1960) Charged particle and total reaction cross sections for protons at 9.8 5 MeV NUCLEAR REACTIONS C(p, x), 27Al(p, x), Ti(p, x), V(p, x), Fe(p, x), 59Co(p, x), Ni(p, x), 63Cu(p, x), 65Cu(p, x), 66Zn(p, x), Ag(p, x), Sn(p, x), E=9.8 MeV; measured products; deduced σ, σ(E), σ(θ, E). Data were imported from EXFOR entry C1042.
doi: 10.1103/PhysRevLett.5.207
1957HI56 Phys.Rev. 106, 1201 (1957) Proton-Nucleus Elastic Scattering at 9.8 MeV
doi: 10.1103/PhysRev.106.1201
1956EI15 Phys.Rev. 103, 645 (1956) Test of the Statistical Assumption in Nuclear Reactions NUCLEAR REACTIONS 40Ar(p, p'), E=8.5, 9.0, 9.8 MeV; measured σ(E, θ).
doi: 10.1103/PhysRev.103.645
1954BL89 Phys.Rev. 96, 1023 (1954) J.M.Blair, N.M.Hintz, D.M.Van Patter Radiative Capture of Deuterons by He3
doi: 10.1103/PhysRev.96.1023
1954HI38 Phys.Rev. 93, 924 (K5) (1954) N.M.Hintz, J.M.Blair, D.M.Van Patter Gamma-Radiation from an Excited State of Li5 NUCLEAR REACTIONS 3He(d, γ), 7Li(p, γ), E=0.46 MeV; measured reaction products; deduced σ assuming thick-target yield for resonant state.
1952HI66 Phys.Rev. 88, 19 (1952) Excitation Functions to 100 MeV NUCLEAR REACTIONS 11B(p, n), 12C(p, x), 27Al(p, x), 34S(p, n), E=100 keV-118 MeV; measured products, 22Na, 24Na, 18F, 11C, 34Cl, Eν, Iν; deduced σ, σ(E). Data were imported from EXFOR entry B0076.
doi: 10.1103/PhysRev.88.19
Back to query form |