NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = H.J.Hausman Found 46 matches. 1990RA16 Nucl.Phys. A515, 338 (1990) D.P.Rath, R.N.Boyd, H.J.Hausman, M.S.Islam, G.W.Kolnicki 7Li(3He, p)9Be Reaction and Primordial Nucleosynthesis NUCLEAR REACTIONS, ICPND 7Li(3He, p), E(cm)=0.5-2 MeV; measured σ(Ep, θ); deduced astrophysical S-factor, other quantities. Natural target.
doi: 10.1016/0375-9474(90)90371-R
1990RO03 Nucl.Phys. A507, 413 (1990) A.A.Rollefson, V.Wijekumar, C.P.Browne, M.Wiescher, H.J.Hausman, W.Y.Kim, P.Schmalbrock Spectroscopic Factors for Proton Unbound Levels in 26Al and Their Influence on Stellar Reaction Rates NUCLEAR REACTIONS, ICPND 25Mg(3He, d), E=15 MeV; measured σ(Ed, θ); deduced 25Mg(p, γ) reaction rate. 26Al deduced levels, spectroscopic factors, resonance strengths. Enriched target.
doi: 10.1016/0375-9474(90)90301-2
1989KA02 Phys.Rev. C39, 340 (1989) J.D.Kalen, H.J.Hausman, A.Abduljalil, W.Kim, D.G.Marchlenski, J.P.McDermott, T.W.Rackers, S.L.Blatt, M.A.Kovash, A.D.Bacher Radiative Proton Capture to Excited States in 16O NUCLEAR REACTIONS 15N(p, γ), E=20-90 MeV; measured σ(θ), analyzing power. 16O deduced GDR parameters.
doi: 10.1103/PhysRevC.39.340
1989KO29 Phys.Rev. C40, R1093 (1989) M.A.Kovash, B.Anderson-Pugh, M.T.McEllistrem, J.K.Ternes, J.H.Trice, J.L.Weil, S.L.Blatt, H.J.Hausman, D.G.Marchlenski, A.D.Bacher Quadrupole and Octupole Radiation from 16O Near 39 MeV Excitation NUCLEAR REACTIONS 15N(polarized p, γ), E=24.4, 28.8 MeV; measured Eγ, Iγ, σ(θ), analyzing power vs θ; deduced σ(E2)/σ(E1), σ(E3)/σ(E1). 16O deduced isovector quadrupole, octupole resonance components.
doi: 10.1103/PhysRevC.40.R1093
1988HA04 Phys.Rev. C37, 503 (1988) H.J.Hausman, S.L.Blatt, T.R.Donoghue, J.Kalen, W.Kim, D.G.Marchlenski, T.W.Rackers, P.Schmalbrock, M.A.Kovash, A.D.Bacher Ground State Proton Capture Reactions from 20 to 100 MeV NUCLEAR REACTIONS, MECPD 11B, 12C, 15N, 16O, 27Al(p, α), (polarized p, γ), E=20-100 MeV; measured Eγ, Iγ, σ(θ), analyzing power vs θ. 12C, 13N, 16O, 17F, 28Si deduced GDR, parameters, EWSR.
doi: 10.1103/PhysRevC.37.503
1988RA15 Phys.Rev. C37, 1759 (1988) T.W.Rackers, S.L.Blatt, T.R.Donoghue, H.J.Hausman, J.Kalen, W.Kim, D.G.Marchlenski, M.Wiescher, M.A.Kovash, A.D.Bacher Proton Radiative Capture by 15N, 16O, 27Al, and 28Si NUCLEAR REACTIONS, MECPD 15N, 27Al, 16O, 28Si(polarized p, γ), E=20.8 MeV; measured Eγ, Iγ, analyzing power vs θ following capture; deduced reaction mechanism. Direct-semidirect model.
doi: 10.1103/PhysRevC.37.1759
1985HA05 Phys.Rev. C31, 660 (1985) H.J.Hausman, S.L.Blatt, R.N.Boyd, T.R.Donoghue, R.G.Seyler, D.G.Marchlenski, T.W.Rackers, P.Schmalbrock, L.G.Arnold, M.A.Kovash, A.D.Bacher, C.C.Foster Evidence for Multistep Processes in Proton Capture Reactions NUCLEAR REACTIONS 11B(p, γ), E=29.9 MeV; 6Li(p, γ), E=44.4 MeV; measured Eγ, Iγ following proton capture; deduced reaction mechanism. 7Be level deduced population via entrance channel multi-step excitation.
doi: 10.1103/PhysRevC.31.660
1985WI03 Nucl.Phys. A436, 561 (1985) V.Wijekumar, P.Schmalbrock, H.J.Hausman, T.R.Donoghue, M.Wiescher, H.R.Suiter, C.P.Browne, A.A.Rollefson, R.W.Tarara Proton Threshold States in 26Al NUCLEAR REACTIONS 27Al(3He, α), E=9, 12 MeV; 24Mg(3He, p), E=12, 15, 18 MeV; measured σ(Eα), σ(θ). 26Al deduced levels, J, π, L. Enriched target.
doi: 10.1016/0375-9474(85)90086-7
1984BL10 Phys.Rev. C30, 423 (1984) S.L.Blatt, H.J.Hausman, L.G.Arnold, R.G.Seyler, R.N.Boyd, T.R.Donoghue, P.Koncz, M.A.Kovash, A.D.Bacher, C.C.Foster Proton Radiative Capture into Closed-Shell and Closed-Shell-Plus-One-Proton Nuclei NUCLEAR REACTIONS 11B, 12C(p, γ), (polarized p, γ), E=24-80 MeV; measured σ(θ), analyzing power vs θ; deduced reaction mechanism.
doi: 10.1103/PhysRevC.30.423
1982WA12 Phys.Rev. C26, 107 (1982) P.H.Wallace, H.J.Hausman, J.N.McKamy, H.R.Suiter Proton Partial Decay Widths from the Intermediate Structure in 41Sc NUCLEAR REACTIONS 40Ca(p, p'), (polarized p, p'), E=5.9-6.5 MeV; measured σ(Ep', E), σ(θ), analyzing power, spin flip vs θ. 41Sc deduced resonances, J, π, Γ, Γp, Γp', configuration.
doi: 10.1103/PhysRevC.26.107
1982WE08 Phys.Rev. C25, 2921 (1982) H.R.Weller, H.Hasan, S.Manglos, G.Mitev, N.R.Roberson, S.L.Blatt, H.J.Hausman, R.G.Seyler, R.N.Boyd, T.R.Donoghue, M.A.Kovash, A.D.Bacher, C.C.Foster Proton Capture to Bound and Unbound States of 12C NUCLEAR REACTIONS 11B(p, γ), E=23-60 MeV; measured σ(E). 11B(polarized p, γ), E=28.7 MeV; measured σ(θ), A(θ). 12C deduced possible giant resonances. Direct capture calculations.
doi: 10.1103/PhysRevC.25.2921
1981BO37 Nucl.Phys. A372, 51 (1981) R.N.Boyd, E.Sugarbaker, S.L.Blatt, T.R.Donoghue, H.J.Hausman, S.E.Vigdor The 46,48Ti(p(pol), α)43,45Sc Reaction at Intermediate Energy NUCLEAR REACTIONS 46,48Ti(polarized p, α), E=79.2 MeV; measured σ(θ), A(θ). 43,45Sc deduced levels, j-transfer, π. DWBA, multi-step analysis, microscopic form factors. Enriched 46,48Ti targets.
doi: 10.1016/0375-9474(81)90086-5
1980WA11 Phys.Rev. C22, 65 (1980) P.H.Wallace, H.J.Hausman, H.R.Suiter, R.L.West Properties of the 2p-1h Intermediate Structure in 41Sc NUCLEAR REACTIONS 40Ca(p, p'), E=6.02-6.48 MeV; measured pγ(θ), σ(E, Ep'). 40Ca(polarized p, p), E=6.0-6.4 MeV; measured analyzing power vs E, θ. 41Sc deduced resonances, J, π, intermediate structure.
doi: 10.1103/PhysRevC.22.65
1979KO05 Phys.Rev.Lett. 42, 700 (1979) M.A.Kovash, S.L.Blatt, R.N.Boyd, T.R.Donoghue, H.J.Hausman, A.D.Bacher Radiative Capture of Intermediate-Energy Protons to High-Lying States In Light Nuclei NUCLEAR REACTIONS 11B(p, γ), E=40, 60, 80 MeV; 27Al(p, γ), E=35, 40, 80 MeV; 12C(p, γ), E=40 MeV; measured Eγ, Iγ. 12C, 28Si deduced evidence for second-harmonic giant resonances. 13N deduced evidence for high-lying single-particle states.
doi: 10.1103/PhysRevLett.42.700
1979TE04 Phys.Rev. C19, 2155 (1979) G.H.Terry, H.J.Hausman, N.Tsoupas Angular Correlation Measurements over the Intermediate Structure in 71As NUCLEAR REACTIONS 70Ge(p, p'γ), E=4.95-5.19 MeV; measured p'γ(θ). 71As resonances deduced J, π, Γ, Γp. Enriched target.
doi: 10.1103/PhysRevC.19.2155
1978TE03 Phys.Rev.Lett. 41, 934 (1978) G.H.Terry, H.J.Hausman, T.R.Donoghue, H.R.Suiter, P.H.Wallace Properties of the Intermediate Structure in 71As NUCLEAR REACTIONS 70Ge(p, p'γ), E=5.05 MeV; measured p'γ(θ). 70Ge(polarized p, p), E=5.05 MeV; measured σ(θ), A(θ). 71As deduced resonances, J, π.
doi: 10.1103/PhysRevLett.41.934
1977HA43 Phys.Rev. C16, 2428 (1977) H.J.Hausman, R.G.Seyler, P.H.Wallace Cusps in Proton-Induced Reactions on Intermediate-Mass Nuclei NUCLEAR REACTIONS 48Ti(p, n), E=4.7-5.4 MeV; measured σ(E, θ); deduced cusps. Statistical model calculations.
doi: 10.1103/PhysRevC.16.2428
1976TS02 Phys.Rev. C13, 510 (1976) N.Tsoupas, H.J.Hausman, N.L.Gearhart, G.H.Terry Partial Decay Widths of Resonances in 29P NUCLEAR REACTIONS 28Si(p, p'γ), E=3.0-5.2 MeV; measured σ(E, θ), pγ-coin. 29P deduced resonances, Γ, J, π.
doi: 10.1103/PhysRevC.13.510
1974GE12 Phys.Rev. C10, 1739 (1974) N.L.Gearhart, H.J.Hausman, J.F.Morgan, G.A.Norton, N.Tsoupas Spectroscopy of 29P via the 28Si(p, p'γ) Reaction NUCLEAR REACTIONS 28Si(p, p), (p, p'γ), E=3.1-5.7 MeV; measured σ(E), p'γ(θ). 29P levels deduced J, π.
doi: 10.1103/PhysRevC.10.1739
1974NO05 Phys.Rev. C9, 1594 (1974) G.A.Norton, N.L.Gearhart, H.J.Hausman, J.F.Morgan Sub-Coulomb (d, p) Stripping on the N = 82 Isotones NUCLEAR REACTIONS 139La, 140Ce, 141Pr, 142Nd, 144Sm(d, p), E=5.8 MeV; measured σ(Ep, θ). 140La, 141Ce, 142Pr, 143Nd, 145Sm levels deduced reduced normalization.
doi: 10.1103/PhysRevC.9.1594
1974NO06 Phys.Rev. C9, 1601 (1974) G.A.Norton, H.J.Hausman, J.F.Morgan Comparison of Sub-Coulomb (d, p) Stripping to Analog Resonance Results for N = 82 Isotones NUCLEAR REACTIONS 138Ba, 140Ce, 142Nd, 144Sm(d, p), (p, p); analyzed σ. 139Ba, 141Ce, 143Nd, 145Sm levels deduced reduced normalization.
doi: 10.1103/PhysRevC.9.1601
1973NO05 Phys.Rev.Lett. 31, 769 (1973) G.A.Norton, H.J.Hausman, J.J.Kent, J.F.Morgan, R.G.Seyler Comparison of Sub-Coulomb Stripping and Analog-Resonance Results Near Closed Shells NUCLEAR REACTIONS 90,92Zr, 92Mo, 138Ba, 140Ce, 142Nd, 144Sm, 208Pb(d, p); calculated σ(θ). 91,93Zr, 93Mo, 139Ba, 141Ce, 143Nd, 145Sm, 209Pb levels calculated S.
doi: 10.1103/PhysRevLett.31.769
1973SI30 Phys.Rev. C8, 1413 (1973) J.W.D.Sinclair, N.L.Gearhart, H.J.Hausman, J.F.Morgan, G.A.Norton, W.S.Steiner Spectroscopy of 67Zn via Analog Resonances in 67Ga NUCLEAR REACTIONS 66Zn(p, p), (p, p'γ), E=3.0-5.8 MeV; measured σ(E), pγ(θ). 67Ga resonances deduced J, π, L.
doi: 10.1103/PhysRevC.8.1413
1972DU11 Phys.Rev. C6, 792 (1972) J.R.Duray, H.J.Hausman, N.L.Gearhart, J.W.D.Sinclair, W.S.Steiner Spectroscopy of 25Al by Means of the Reaction 24Mg(p, p'1γ)24Mg NUCLEAR REACTIONS 24Mg(p, p'γ), (p, p), E=3.4-4.9 MeV; measured σ(E;θ), p'γγ-triple correlation. 25Al deduced levels, resonances, J, π, level-width.
doi: 10.1103/PhysRevC.6.792
1972MO43 Phys.Rev. C6, 2126 (1972) J.F.Morgan, N.L.Gearhart, H.J.Hausman, J.J.Kent, G.A.Norton, J.W.D.Sinclair 50Ti(p, p'γ) Angular-Correlation Study at Isobaric Analog Resonances NUCLEAR REACTIONS 50Ti(p, p'γ), E=3-5 MeV; measured σ(E, Ep', θ), p'γ(θ). 51V deduced levels, J, π.
doi: 10.1103/PhysRevC.6.2126
1971ST27 Phys.Rev. C4, 1684 (1971) W.S.Steiner, H.J.Hausman, J.J.Kent, J.R.Duray, N.L.Gearhart, J.W.D.Sinclair Spectroscopy of Some Low-Lying States in 69Zn NUCLEAR REACTIONS 68Zn(p, p), (p, p'γ), E=3.9-6.1 MeV; measured σ(E;θ), σ(E;Ep', θ, θ(p'γ)), p'γγ-triple correlation. 69Ga deduced isobaric analog resonances, level-width, S, L.
doi: 10.1103/PhysRevC.4.1684
1970AR10 Phys.Rev. C1, 2152 (1970) R.G.Arns, J.R.Duray, H.J.Hausman, D.B.Nichols, R.G.Seyler Possible Role of Isobaric Analog States in 56Fe(p, p') NUCLEAR REACTIONS 56Fe(p, p), (p, p'), E=2.0-6.0 MeV; measured σ(E); deduced spin-flip probability. 57Co deduced isobaric analog resonances.
doi: 10.1103/PhysRevC.1.2152
1969DU07 Nucl.Phys. A136, 153 (1969) J.R.Duray, H.J.Hausman, G.K.Marshall, J.W.Sinclair, W.S.Steiner Determination of the Spin of the 6.92 MeV Level of 25Al NUCLEAR REACTIONS 24Mg(p, p'γ), E = 4.76-5.26 MeV; measured σ(E;Ep', θ(p'γ)). 25Al deduced resonances, J. Natural target.
doi: 10.1016/0375-9474(69)90044-X
1969NI10 Phys.Rev. 183, 945 (1969) D.B.Nichols, R.G.Arns, H.J.Hausman, R.G.Seyler Reaction Mechanisms in 56Fe(p, p') from 5 to 6 MeV NUCLEAR REACTIONS 56Fe(p, p'γ), E = 4.96, 5.58, 5.88 MeV; measured σ(E;Ep', Eγ, θ), spin-flip probability; deduced direct reaction contribution. Enriched 56Fe target.
doi: 10.1103/PhysRev.183.945
1968BL17 Nucl.Instr.Methods 61, 232 (1968) S.L.Blatt, D.B.Nichols, R.G.Arns, J.D.Goss, H.J.Hausman New Thick-Target Technique for Charged-Particle Radiative Capture Studies NUCLEAR REACTIONS 12C(p, γ), E < 5 MeV; measured σ(E;Eγ). 13N deduced resonances, level-width.
doi: 10.1016/0029-554X(68)90549-1
1967HA37 Phys.Rev. 164, 1407 (1967) H.J.Hausman, R.M.Humes, R.G.Seyler Energy Dependence of (p, p'γ) Correlations in Ti48 NUCLEAR STRUCTURE 48Ti; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.164.1407
1966HA24 Phys.Rev. 148, 1136 (1966) H.J.Hausman, W.E.Davis, C.V.Phillips, R.P.Sullivan, G.R.Unrine Si28(d, pγ)Si29 Angular Correlations from 4 to 6 MeV NUCLEAR STRUCTURE 29Si; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.148.1136
1965DE32 Nucl.Phys. 64, 513 (1965) G.F.Dell, W.D.Ploughe, H.J.Hausman Total Reaction Cross Sections in the Mass Range 45 to 65 NUCLEAR REACTIONS 45Sc(p, n), 51V(p, n), 55Mn(p, n), 63Cu(p, n), 65Cu(p, n), E=3.2-6.7 MeV; measured products, 45Ti, Eν, Iν; deduced σ, σ(E). Data were imported from EXFOR entry B0064.
doi: 10.1016/0029-5582(65)90576-6
1965HU04 Phys.Rev. 139, B846 (1965) (p, p'γ) Angular Correlations in Ti48 NUCLEAR STRUCTURE 48Ti; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.139.B846
1964HU03 Bull.Am.Phys.Soc. 9, No.6, 650, Q5 (1964) R.M.Humes, T.R.Donoghue, H.J.Hausman Energy Dependence of (p, p'γ) Correlations in Ti48 NUCLEAR STRUCTURE 48Ti; measured not abstracted; deduced nuclear properties.
1963HU15 Phys.Rev. 130, 1522 (1963) R.M.Humes, G.F.Dell Jr, W.D.Ploughe, H.J.Hausman (p, n) Cross Sections at 6.75 MeV NUCLEAR REACTIONS 45Sc(p, n), 51V(p, n), 55Mn(p, n), 63Cu(p, n), 65Cu(p, n), 69Ga(p, n), 71Ga(p, n), 79Br(p, n), E=6.7 MeV; measured products, 45Ti, Eν, Iν; deduced σ, σ(E). Data were imported from EXFOR entry B0061.
doi: 10.1103/PhysRev.130.1522
1963KL01 Bull.Am.Phys.Soc. 8, No.6, 486, T4 (1963) R.W.Klingenemith, H.J.Hausman, W.D.Ploughe Elastic Scattering of He3 at 20 MeV
1962AX01 Bull.Am.Phys.Soc. 7, No.8, 532, B10 (1962) P.Axelrod, W.D.Ploughe, H.J.Hausman Angular Distribution of Elastically Scattered 19-MeV He3 Nuclei NUCLEAR STRUCTURE 12C, 197Au, 27Al; measured not abstracted; deduced nuclear properties.
1961BO04 Phys.Rev. 121, 1504 (1961) H.F.Bowsher, G.F.Dell, H.J.Hausman Si28(p, p'γ) Angular Correlations NUCLEAR STRUCTURE 28Si; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.121.1504
1960BO18 Bull.Am.Phys.Soc. 5, No.6, 406, B10 (1960) H.F.Bowsher, G.F.Dell, H.J.Hausman Si28(p, p'γ) Angular Correlations NUCLEAR STRUCTURE 28Si; measured not abstracted; deduced nuclear properties.
1960HA21 Phys.Rev. 118, 1237 (1960) H.J.Hausman, G.F.Dell, H.F.Bowsher (p, p'γ) Angular Correlations at Low Energy NUCLEAR STRUCTURE 12C, 28Si, 32S, 52Cr, 20Ne; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.118.1237
1959HA12 Bull.Am.Phys.Soc. 4, No.8, 445, C11 (1959) H.J.Hausman, G.F.Dell, H.F.Bowsher (p, p'ν) Angular Correlations at Low Energy
1959LA06 Phys.Rev. 114, 560 (1959) H.A.Lackner, G.F.Dell, H.J.Hausman Evidence for Direct Interactions at Low Energy
doi: 10.1103/PhysRev.114.560
1952AR29 Phys.Rev. 88, 1291 (1952) J.C.Arthur, A.J.Allen, R.S.Bender, H.J.Hausman, C.J.McDole Energy Levels in Light Nuclei
doi: 10.1103/PhysRev.88.1291
1952AR32 Phys.Rev. 87, 237 YA3 (1952) J.S.Arthur, A.J.Allen, R.S.Bender, H.J.Hausman, C.J.McDole, L.M.Diana, K.B.Rhodes, R.A.Barjon Energy Levels Resulting from 8-Mev Protons on Be9, C12, N14, S32 NUCLEAR REACTIONS 9Be, 12C, 14N, 32S(p, p'), (p, p), E=8 MeV; measured reaction products, Ep, Ip, Eα, Iα; deduced excited states, energy levels.
doi: 10.1103/PhysRev.87.179
1952HA74 Phys.Rev. 87, 238 YA6 (1952) H.J.Hausman, A.J.Allen, J.S.Arthur, R.S.Bender, C.J.McDole, L.M.Diana, K.B.Rhodes, R.A.Barjon Excited States of Mg24, Cr52, and Mn55 NUCLEAR REACTIONS 24Mg, 52Cr, 55Mn(p, p'), E=8 MeV; measured reaction products, Ep, Ip; deduced proton groups, excited states energies.
doi: 10.1103/PhysRev.87.179
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