NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = D.J.Pullen Found 57 matches. 1998TI09 Phys.Rev. C58, 905 (1998) S.V.Tipnis, J.M.Campbell, G.P.Couchell, S.Li, H.V.Nguyen, D.J.Pullen, W.A.Schier, E.H.Seabury, T.R.England Yields of Short-Lived Fission Products Produced following 235U(nth, f) NUCLEAR REACTIONS 235U(n, F), E=thermal; measured Eγ, Iγ, βγ-coin; deduced independent, cumulative short-lived fission fragment yields. Helium jet, tape transport.
doi: 10.1103/PhysRevC.58.905
1996BE92 Nucl.Instrum.Methods Phys.Res. A369, 263 (1996) P.R.Bennett, W.A.Schier, G.P.Couchell, E.S.Jacobs, D.J.Pullen, M.F.Villani Relative Efficiency Measurements of Fission Fragment Transfer with a Helium Jet NUCLEAR REACTIONS 235,238U, 239Pu(n, F), E=reactor; measured fission fragment decay associated X-ray spectra; deduced helium jet fission fragment transfer relative efficiency.
doi: 10.1016/0168-9002(95)00551-X
1992VI05 Nucl.Sci.Eng. 111, 422 (1992) M.F.Villani, G.P.Couchell, M.H.Haghighi, D.J.Pullen, W.A.Schier, Q.Sharfuddin Six-Group Decomposition of Composite Delayed Neutron Spectra from 235U Fission NUCLEAR REACTIONS 235U(n, F), E=thermal; measured composite delayed neutron spectra following fission. Constrained least-squares method, six-group decomposition.
doi: 10.13182/NSE92-A15489
1988SH13 Nucl.Sci.Eng. 98, 341 (1988) Q.Sharfuddin, W.A.Schier, R.S.Tanczyn, D.J.Pullen, M.H.Haghighi, L.Fisteag, G.P.Couchell Search for an Energy Dependence in 235U Delayed Neutron Spectra NUCLEAR REACTIONS 235U(n, F), E=fast; measured delayed neutron yield vs E following fission.
doi: 10.13182/NSE88-A23534
1986SH05 Nucl.Sci.Eng. 92, 350 (1986) J.Q.Shao, G.P.Couchell, J.J.Egan, G.H.R.Kegel, S.Q.Li, A.Mittler, D.J.Pullen, W.A.Schier, E.D.Arthur Fast Neutron Inelastic Scattering Cross Sections of 238U for States between 680 and 1530 keV NUCLEAR REACTIONS 238U(n, n'), E=0.9-2.2 MeV; measured σ(θ), σ(En); deduced optical model parameters, σ(E). 238U level deduced B(λ). 239U deduced fission barrier parameters.
doi: 10.13182/NSE86-A17525
1986SH08 J.Phys.(London) G12, 237 (1986) E.Sheldon, L.E.Beghian, C.A.Ciarcia, G.P.Couchell, J.H.Dave, J.J.Egan, G.Goswami, G.H.R.Kegel, S.Q.Li, A.Mittler, D.J.Pullen, W.A.Schier, J.Q.Shao Fast-Neutron Inelastic Scattering Cross Sections for the Principal Even-Even Actinide Nuclei. I: 232Th(n, n') NUCLEAR REACTIONS 232Th(n, n'γ), (n, n'), E=0.2-3.4 MeV; analyzed σ(θ), σ(E); deduced reaction mechanism. 232Th deduced consistent σ for rotational, vibrational level excitation.
doi: 10.1088/0305-4616/12/3/011
1986SH28 J.Phys.(London) G12, 443 (1986) E.Sheldon, L.E.Beghian, D.W.S.Chan, A.Chang, G.P.Couchell, J.J.Egan, G.Goswami, G.H.R.Kegel, S.Q.Li, A.Mittler, D.J.Pullen, W.A.Schier, J.P.Shao, A.Wang Fast Neutron Inelastic-Scattering Cross Sections for the Principal Even-Even Actinide Nuclei. II: 238U(n, n') NUCLEAR REACTIONS 238U(n, n'), E=0.2-3.1 MeV; analyzed experimental, theoretical σ(E), σ(θ); deduced fluctuation σ factor F.
doi: 10.1088/0305-4616/12/5/009
1986TA18 Nucl.Sci.Eng. 94, 353 (1986) R.S.Tanczyn, Q.Sharfuddin, W.A.Schier, D.J.Pullen, M.H.Haghighi, L.Fisteag, G.P.Couchell Composite Delayed Neutron Energy Spectra for Thermal Fission of 235U NUCLEAR REACTIONS 235U(n, F), E=thermal; measured delayed neutron yields following fission. Plastic, liquid, 6Li glass scintillators.
doi: 10.13182/NSE86-A18346
1985CI05 Nucl.Sci.Eng. 91, 428 (1985) C.A.Ciarcia, G.P.Couchell, J.J.Egan, G.H.R.Kegel, S.Q.Li, A.Mittler, D.J.Pullen, W.A.Schier, J.Q.Shao Neutron Inelastic Scattering Cross Sections for States above 700 keV in 232Th NUCLEAR REACTIONS 232Th(n, n'), E=0.95-2.1 MeV; measured σ(θ). 232Th levels deduced possible J, π, K.
doi: 10.13182/NSE85-A18359
1985DA21 Nucl.Sci.Eng. 91, 187 (1985) J.H.Dave, J.J.Egan, G.P.Couchell, G.H.R.Kegel, A.Mittler, D.J.Pullen, W.A.Schier, E.Sheldon Cross Sections, Transition Schemes, and Branching Ratios for 232Th from the 232Th(n, n'γ) Reaction NUCLEAR REACTIONS 232Th(n, n'γ), E=0.77-2.1 MeV; measured Eγ, Iγ; deduced σ(θγ). 232Th deduced levels, γ-branching ratios, possible J, π. Statistical compound nucleus model.
doi: 10.13182/NSE85-A27441
1984SC45 Nucl.Instrum.Methods 227, 549 (1984) W.A.Schier, G.P.Couchell, D.J.Pullen, N.M.Sampas, C.A.Ciarcia, M.H.Haghighi, Q.Sharfuddin, R.S.Tanczyn New Experimental System for Measuring Composite Delayed-Neutron Spectra following Fission NUCLEAR REACTIONS 235U(n, F), E=fast, thermal; measured delayed neutron fission yields vs En. Pilot U, 6Li-glass scintillators, β-neutron tof system.
doi: 10.1016/0168-9002(84)90214-6
1980AL16 J.Phys.(London) G6, 731 (1980) M.N.I.Al-Jadir, H.T.Fortune, D.J.Pullen States at High E(x) in 31P NUCLEAR REACTIONS 29Si(3He, p), E=15.0 MeV; measured σ(Ep, θ). 31P deduced levels, L, J, π. DWBA analysis.
doi: 10.1088/0305-4616/6/6/010
1979BE19 Nucl.Sci.Eng. 69, 191 (1979) L.E.Beghian, G.H.R.Kegel, T.V.Marcella, B.K.Barnes, G.P.Couchell, J.J.Egan, A.Mittler, D.J.Pullen, W.A.Schier Neutron Scattering Cross Sections of Uranium-238 NUCLEAR REACTIONS 238U(n, n), (n, n'), E=0.9-3.1 MeV; measured σ(E, θ); deduced disagreement between observed, evaluated inelastic σ.
doi: 10.13182/NSE79-A20610
1978AL17 Nucl.Phys. A304, 85 (1978) M.N.Al-Jadir, H.T.Fortune, D.J.Pullen Study of 31P with the 29Si(3He, p)31P Reaction NUCLEAR REACTIONS 29Si(3He, p), E=15.0 MeV; measured σ(Ep, θ). 31P deduced levels L, J, π. DWBA analysis. Comparison with Nilsson model. Enriched target.
doi: 10.1016/0375-9474(78)90098-2
1978BE28 Nucl.Phys. A299, 412 (1978); Erratum Nucl.Phys. A312, 524 (1978) R.R.Betts, H.T.Fortune, D.J.Pullen A Study of 26Al by the 25Mg(3He, d) Reaction NUCLEAR REACTIONS 25Mg(3He, d), E=18.0 MeV; measured σ(Ed, θ). 26Al deduced levels I, J, π, (2j+1)S. DWBA analysis.
doi: 10.1016/0375-9474(78)90380-9
1978KA21 Nucl.Sci.Eng. 67, 34 (1978) P.T.Karatzas, G.P.Couchell, B.K.Barnes, L.E.Beghian, P.Harihar, A.Mittler, D.J.Pullen, E.Sheldon, N.B.Sullivan Neutron Inelastic Scattering Cross Sections for Natural Chromium Determined from the (n, n'γ) Reaction NUCLEAR REACTIONS Cr(n, n'γ), E=0.84-3.97 MeV; measured σ(E, Eγ), total inelastic σ(E). 52,53,54,50Cr levels deduced γ-branching.
doi: 10.13182/NSE78-A27235
1975CA07 Nucl.Phys. A242, 221 (1975) T.Caldwell, D.J.Pullen, O.Hansen Ti(τ, p) Reactions at 15 MeV (II). 50Ti(τ, p)52V NUCLEAR REACTIONS 50Ti(3He, p), E=15.11 MeV; measured σ(Ep, θ), Q. 52V deduced levels, J, π, L, t. Enriched target.
doi: 10.1016/0375-9474(75)90044-5
1974BE07 Phys.Rev. C9, 589 (1974) R.R.Betts, H.T.Fortune, D.J.Pullen Study of the 26Mg(3He, p)28Al Reaction NUCLEAR REACTIONS 26Mg(3He, p), E=18 MeV; measured σ(Ep, θ). 28Al deduced levels, J, π. Enriched target.
doi: 10.1103/PhysRevC.9.589
1974BE54 Nucl.Phys. A230, 235 (1974) R.R.Betts, S.Mordechai, D.J.Pullen, B.Rosner, W.Scholz Study of 71,73,75,77As with Ge(3He, d) Reactions NUCLEAR REACTIONS 70,72,74,76Ge(3He, d), E=17.0 MeV; measured σ(Ed, θ). 71,73,75,77As deduced levels, L(p), J, π. Enriched targets.
doi: 10.1016/0375-9474(74)90305-4
1973BE27 Phys.Rev. C8, 670 (1973) R.R.Betts, H.T.Fortune, D.J.Pullen Neutron Pickup from 27Al NUCLEAR REACTIONS 27Al(3He, α), E=18 MeV; measured σ(Eα, θ). 26Al deduced level, J, π, S, L.
doi: 10.1103/PhysRevC.8.670
1973RO14 Nucl.Phys. A206, 76 (1973) B.Rosner, S.Mordechai, D.J.Pullen Study of 74As by the 73Ge(3He, d) Reaction NUCLEAR REACTIONS 73Ge(3He, d), E(3He)=17 MeV; measured σ(θ). 74As deduced levels, L(p), spectroscopic strengths.
doi: 10.1016/0375-9474(73)90607-6
1973SL01 Nucl.Phys. A206, 433 (1973) D.C.Slater, E.R.Cosman, D.J.Pullen Particle Coupling to the Octupole State in 89Sr from 88Sr(p, p')88Sr Analog Resonances and 88Sr(d, p)89Sr NUCLEAR REACTIONS 88Sr(p, p'), Ep=7.65, 7.80, 7.92, 8.78, 9.75, 9.90 MeV, measured σ(E;θ). 89Y deduced isobaric analog resonances, Ip, J, π. 88Sr(d, p), Ed=10 MeV, measured σ(E, θ). 89Sr deduced L(n), S, J, π. Enriched target.
doi: 10.1016/0375-9474(73)90076-6
1972BE07 Nucl.Phys. A182, 69 (1972) R.R.Betts, O.Hansen, D.J.Pullen (tau, p) Reactions on Cr (III). [52Cr(tau, p)54Mn] NUCLEAR REACTIONS 52Cr(3He, p), E=15, 16.5 MeV; measured σ(Ep, θ), Q. 54Mn deduced levels, l, J, π, T. Enriched target.
doi: 10.1016/0375-9474(72)90202-3
1972BE51 Phys.Rev. C6, 957 (1972) R.R.Betts, H.T.Fortune, D.J.Pullen Study of the 24Mg(3He, p)26Al Reaction NUCLEAR REACTIONS 24Mg(3He, p), E=18 MeV; measured σ(Ep, θ). 26Al deduced levels, J, π, L.
doi: 10.1103/PhysRevC.6.957
1972BE55 Priv.Comm. (Oct.1972) R.R.Betts, D.J.Pullen, W.Scholz, B.Rosner
1972CA32 Nucl.Phys. A198, 529 (1972) T.Caldwell, O.Hansen, D.J.Pullen Ti(3He, p) Reactions at 15 MeV (I). 48Ti(3He, p)50V NUCLEAR REACTIONS 48Ti(3He, p), E=15.08 MeV; measured σ(Ep, θ). 50V deduced levels, J, π, L, T. Enriched target.
doi: 10.1016/0375-9474(72)90707-5
1972FL01 Phys.Rev. C5, 1356 (1972) D.G.Fleming, R.A.Broglia, K.Abdo, O.Nathan, D.J.Pullen, B.Rosner, O.Hansen Strongly Excited 1+ States in the Reactions 46,48Ca(3He, p)48,50Sc NUCLEAR REACTIONS 46,48Ca(3He, p), E=18 MeV; measured σ(θ). 48,50Sc deduced levels, L.
doi: 10.1103/PhysRevC.5.1356
1971BE19 Phys.Rev.Lett. 26, 1121 (1971) R.R.Betts, H.T.Fortune, J.D.Garrett, R.Middleton, D.J.Pullen, O.Hansen Characteristic Difference for 0+ → 0+ and 0+ → 1+ (3He, p) Transitions in the 2s-1d Shell NUCLEAR REACTIONS 16,18O, 20,22Ne, 24,26Mg, 28,29Si(3He, p), E=15-18 MeV; measured σ(θ). 24Na, 28Al levels deduced J, π.
doi: 10.1103/PhysRevLett.26.1121
1971BE30 Phys.Rev.Lett. 26, 1576 (1971) R.R.Betts, D.J.Pullen, W.Scholz, B.Rosner Positive-Parity States in Odd-Even As Isotopes NUCLEAR REACTIONS 70,72,74,76Ge(3He, d), E=17 MeV; measured σ(θ). 71,73,75,77As deduced levels, L(p), J, π, S.
doi: 10.1103/PhysRevLett.26.1576
1971CA32 Nucl.Phys. A175, 31 (1971) T.Caldwell, D.J.Pullen, T.J.Mulligan, O.Hansen The (tau, p) Reactions on Cr (II). 54Cr(tau, p)56Mn NUCLEAR REACTIONS 54Cr(3He, p), E=15.08 MeV; measured σ(Ep, θ), Q. 56Mn deduced levels, J, π, L, T. Enriched target.
doi: 10.1016/0375-9474(71)90618-X
1971FO15 Phys.Lett. 36B, 215 (1971) H.T.Fortune, R.R.Betts, P.Neogy, D.J.Pullen Location of the 'Missing' 0+, T = 1 State in 26Al NUCLEAR REACTIONS 24Mg(3He, p), E=19.5 MeV; measured σ(θ). 26Al deduced 0+, T=1 analog state.
doi: 10.1016/0370-2693(71)90072-4
1971GA04 Nucl.Phys. A164, 449 (1971) J.D.Garrett, R.Middleton, D.J.Pullen, S.A.Andersen, O.Nathan, O.Hansen Spectroscopy of 22Na with the 20Ne(3He, p) and 20Ne(6Li, α) Reactions NUCLEAR REACTIONS 20Ne(3He, p), 20Ne(6Li, α), E=15, 18 MeV; measured σ(Ep, θ), σ(Eα, θ), E(X-ray). 22Na deduced levels L, J, π, T. Enriched target.
doi: 10.1016/0375-9474(71)90773-1
1971HA24 Nucl.Phys. A167, 1 (1971) O.Hansen, T.J.Mulligan, D.J.Pullen (h, p) Reactions on Cr (I). 50Cr(h, p)52Mn NUCLEAR REACTIONS 50Cr(3He, p)E=16.5 MeV; measured σ(Ep, θ), Q. 52Mn deduced levels, J, π, L, T, isobaric analogs. Enriched target.
doi: 10.1016/0375-9474(71)90576-8
1970BE31 Phys.Rev. C2, 395 (1970) K.Bethge, D.J.Pullen, R.Middleton Level Structure of 17O and the 13C(6Li, d) and 13C(7Li, t) Reactions NUCLEAR REACTIONS 13C(7Li, t), E=17 MeV; 13C(6Li, d), E=18 MeV; measured σ(Et, θ), σ(Ed, θ). 17O deduced levels.
doi: 10.1103/PhysRevC.2.395
1970BI07 Phys.Rev. C2, 550 (1970) J.N.Bishop, D.J.Pullen, B.Rosner Level Structure of 50V NUCLEAR REACTIONS 49Ti(3He, d), E=15 MeV; measured σ(Ed, θ). 50V deduced levels, J, π, S.
doi: 10.1103/PhysRevC.2.550
1969BU03 Nucl.Phys. A131, 99 (1969) W.F.Buhl, D.Kovar, J.R.Comfort, O.Hansen, D.J.Pullen Energy Levels in 47Ti and 50V NUCLEAR REACTIONS 47Ti, 50V(p, p'), 50V(p, α), E=7.50, 12.0 MeV; measured σ(Ep'), σ(Eα). 47Ti, 50V deduced levels. Enriched targets.
doi: 10.1016/0375-9474(69)90812-4
1969PU02 Phys.Rev. 177, 1568 (1969) D.J.Pullen, B.Rosner, O.Hansen Proton Excitation in V51 NUCLEAR REACTIONS 48,50Ti(3He, d), E=16.4 MeV; measured σ(Ed, θ). 49,51V deduced levels, L(p), S.
doi: 10.1103/PhysRev.177.1568
1968BR07 Nucl.Phys. A110, 161 (1968) Level Structure of 46Ti NUCLEAR REACTIONS 45Sc(3He, d), E=15 MeV; measured σ(Ed, θ). 47Ti(3He, α), E=15 MeV; measured σ(Eα). 46Ti deduced levels, L, π. Enriched (47Ti) target.
doi: 10.1016/0375-9474(68)90689-1
1968MI01 Phys.Rev.Letters 20, 118 (1968) R.Middleton, B.Rosner, D.J.Pullen, L.Polsky Rotational States in Ne20 Excited by the Reaction O16(Li7, T) NUCLEAR STRUCTURE 16O, 20Ne; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.20.118
1968PU01 Phys.Rev. 166, 1142 (1968); Erratum Quoted by 1969Pu02 D.J.Pullen, B.Rosner, O.Hansen Proton Excitations in 49V NUCLEAR STRUCTURE 49V; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.166.1142
1968PU03 Phys.Rev. 170, 1034 (1968) Level Structures of Cu59 and Cu61 Studied by Means of the Ni58, 60(He3, d) Reactions NUCLEAR STRUCTURE 61Cu, 59Cu; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.170.1034
1967RO02 Phys.Rev.Letters 18, 13 (1967) 3/2- Ground State of V47 NUCLEAR STRUCTURE 47V; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.18.13
1967RO11 Phys.Letters 24B, 454 (1967) The 46,48,50Ti(3He, α) Reactions and Analogue States in T = 3/2 Isobaric Pairs NUCLEAR STRUCTURE 49Ti, 47Ti, 45Ti; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90269-9
1967RO13 Phys.Rev. 162, 1048 (1967) Ti46(He3, d)V47 Reaction NUCLEAR STRUCTURE 47V; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.162.1048
1966DO06 Nucl.Phys. 81, 390 (1966) W.E.Dorenbusch, O.Hansen, D.J.Pullen, T.A.Belote, G.Sidenius Levels of 48Ti Observed by the (d, α) Reaction on 50V NUCLEAR REACTIONS 50V(d, α)48Ti, E = 7.50 MeV; measured σ(Eα, θ), Q. 48Ti deduced levels, J. Enriched target.
doi: 10.1016/S0029-5582(66)80030-5
1966PU04 Bull.Am.Phys.Soc. 11, No.3, 365, GA5 (1966) Study of the Ni58(He3, D)Cu59 and Ni60(He3, D)Cu61 Reactions NUCLEAR STRUCTURE 59Cu, 61Cu; measured not abstracted; deduced nuclear properties.
1966RO13 Isobaric Spin in Nucl.Phys., J.D.Fox and D.Robson, Eds., Academic Press, p.595 (1966) B.Rosner, C.H.Holbrow, D.J.Pullen Analogue States in Co55, 57 and Cu59, 61 Excited by (He3, d) Reactions NUCLEAR STRUCTURE 59Cu, 57Co, 61Cu, 55Co; measured not abstracted; deduced nuclear properties.
1965PU01 Bull.Am.Phys.Soc. 10, No.1, 38, CD1 (1965) D.J.Pullen, A.Sperduto, E.Kashy Angular-Distribution Measurements from Ne20(d, p)Ne21 and Ne22(d, p)Ne23 NUCLEAR STRUCTURE 21Ne, 20Ne, 23Ne; measured not abstracted; deduced nuclear properties.
1964MI04 Nucl.Phys. 51, 50 (1964) A Study of Some (t, p) Reactions (I). Method and Results for Li7, B10 and B11 NUCLEAR REACTIONS 7Li, 10,11B(t, p), E=10, 11 MeV; measured reaction products, Ep, Ip; deduced Q-value, excited states.
doi: 10.1016/0029-5582(64)90251-2
1964MI05 Nucl.Phys. 51, 63 (1964) A Study of Some (t, p) Reactions (II). Results for C12, C14, O16 and O18 NUCLEAR REACTIONS 12,14C, 16,18O(t, p), E=11 MeV; measured reaction products, Ep, Ip; deduced σ(θ), excited states, J, π.
doi: 10.1016/0029-5582(64)90252-4
1964MI06 Nucl.Phys. 51, 77 (1964) A Study of Some (t, p) Reactions (III). Results for Mg26, Si28, Si29, Ca40 and Cd110 NUCLEAR STRUCTURE 30Si, 31Si, 42Ca, 112Cd, 28Mg; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90253-6
1964PU01 Nucl.Phys. 51, 88 (1964) D.J.Pullen, J.R.Rook, R.Middleton Triton Elastic Scattering from Light Nuclei
doi: 10.1016/0029-5582(64)90254-8
1963DA19 Proc.Intern.Symp.On Direct Interactions and Nucl.Reaction Mechanisms, Padua, Italy (1962), E.Clementel, C.Villi, Ed., Gordon and Breach, New York, p.795 (1963) W.Darcey, D.J.Pullen, N.W.Tanner Collective States in the Even Isotopes of Selenium NUCLEAR STRUCTURE 78Se, 80Se, 76Se; measured not abstracted; deduced nuclear properties.
1963MA27 Nucl.Phys. 44, 309 (1963) B.E.F.Macefield, R.Middleton, D.J.Pullen The Mechanism of the Reaction Se76(d, p)Se77 NUCLEAR STRUCTURE 77Se; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90029-4
1962PU01 Nuclear Phys. 36, 1 (1962) D.J.Pullen, A.E.Litherland, S.Hinds, R.Middleton Be11: A shell model anomaly NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90433-9
1961HI01 Phys.Rev.Letters 6, 113 (1961) S.Hinds, R.Middleton, A.E.Litherland, D.J.Pullen New Isotope of Carbon: C16 NUCLEAR STRUCTURE 9Li, 16O, 16C, 17N; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.6.113
1960HI18 Proc.Intern.Conf.Nuclear Structure, Kingston, Canada, D.A.Bromley, E.W.Vogt, Editors, University of Toronto Press, p.486 (1960) S.Hinds, A.E.Litherland, R.Middleton, D.J.Pullen Some Properties of Be11 NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
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