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NSR database version of April 11, 2024.

Search: Author = M.Cooper

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2022NE12      Phys.Rev. C 106, 044320 (2022)

S.Neupane, J.Heideman, R.Grzywacz, M.Cooper, J.Hooker, K.L.Jones, T.T.King, N.Kitamura, M.Madurga, K.Siegl, C.R.Thornsberry, P.Wagenknecht, Z.Y.Xu, L.H.Heilbronn, M.M.Rajabali, A.Chester, A.Richard, Y.Alberty-Jones, J.Derkin, T.N.Massey, D.Soltesz, N.T.Brewer, B.C.Rasco, K.P.Rykaczewski, M.Wolinska-Cichocka, J.Clark, D.Santiago-Gonzalez, G.Savard

Demonstration of the neutron tracking capability of NEXT array in time-of-flight measurements to improve energy resolution

RADIOACTIVITY 17N, 104Nb(β-n); measured neutron time-of-flight (ToF), En, In. Data on the commissioning of the Neutron dEtector with Xn Tracking (NEXT) array consisting of 8x4 optically separated segments. Measurement of 17N decay at National Superconducting Cyclotron Laboratory (NSCL), 106Nb decay Argonne National Laboratory (ANL, CARIBU Facility).

NUCLEAR REACTIONS 27Al(d, n), E=7.44 MeV; measured neutron time-of-flight (ToF), En, In. Data on the commissioning of the Neutron dEtector with Xn Tracking (NEXT) array consisting of 8x4 optically separated segments. Deuteron beam from Ohio University Edwards Accelerator Laboratory (EAL).

doi: 10.1103/PhysRevC.106.044320
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2022RA11      Phys.Rev. C 105, 064301 (2022)

B.C.Rasco, K.P.Rykaczewski, A.Fijalkowska, M.Karny, M.Wolinska-Cichocka, R.K.Grzywacz, D.W.Stracener, E.F.Zganjar, J.C.Batchelder, J.C.Blackmon, N.T.Brewer, M.P.Cooper, K.C.Goetz, J.W.Johnson, T.King, A.Laminack, J.T.Matta, K.Miernik, M.Madurga, D.Miller, M.M.Rajabali, T.Ruland, P.Shuai, M.Stepaniuk, J.Winger

Deciphering 98Nb β decay with the Modular Total Absorption Spectrometer at ORNL

RADIOACTIVITY 98Nb(β-)[from decay chains of 98Rb and 98Sr produced in 238U(p, F) at HRIBF-ORNL facility]; measured Eγ, Iγ, total absorption γ-ray spectrum using NaI(Tl)-based Modular Total Absorption Spectrometer (MTAS); deduced average γ energy per β decay, and average ν-bar; discussed impact of measured β-feeding pattern on reactor decay heat calculations and predicted detection rates of reactor ν-bar. 98Zr; measured T1/2 with 98Zr and 98Nb in equilibrium, and compared with value in the ENSDF database. 98Mo; deduced levels, β feedings to the g.s. and excited states, logft, conversion electron per β decay from the E0 transition from the first excited 0+ state in 98Mo. Comparison with β feedings and average γ energy in the ENSDF and ENDF/B-VIII.0 databases, and with previous experimental results. Relevance to the study of β- decays of abundantly produced fission products in nuclear reactors.

doi: 10.1103/PhysRevC.105.064301
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2022SH20      Phys.Rev. C 105, 054312 (2022)

P.Shuai, B.C.Rasco, K.P.Rykaczewski, A.Fijalkowska, M.Karny, M.Wolinska-Cichocka, R.K.Grzywacz, C.J.Gross, D.W.Stracener, E.F.Zganjar, J.C.Batchelder, J.C.Blackmon, N.T.Brewer, S.Go, M.Cooper, K.C.Goetz, J.W.Johnson, C.U.Jost, T.T.King, J.T.Matta, J.H.Hamilton, A.Laminack, K.Miernik, M.Madurga, D.Miller, C.D.Nesaraja, S.Padgett, S.V.Paulauskas, M.M.Rajabali, T.Ruland, M.Stepaniuk, E.H.Wang, J.A.Winger

Determination of β-decay feeding patterns of 88Rb and 88Kr using the Modular Total Absorption Spectrometer at ORNL HRIBF

RADIOACTIVITY 88Rb(β-), 88Kr(β-)[from 238U(p, F), E=40 MeV]; measured Eγ, Iγ, Eβ, Iβ; deduced β-intensities, ground state feedings in β-decay. 88Rb; deduced T1/2. Pandemonium effect free measurements. Comparison to other experimental data. Modular Total Absorption Spectrometer (MTAS) NaI(Tl) detector array at Holifield Radioactive Ion Beam Facility (HRIBF) at the Oak Ridge National Laboratory.

doi: 10.1103/PhysRevC.105.054312
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2021ME09      Nucl.Sci.Eng. 195, 563 (2021)

V.K.Mehta, M.W.D.Cooper, R.B.Wilkerson, D.Kotlyar, D.V.Rao, S.C.Vogel

Evaluation of Yttrium Hydride (σ-YH2-x) Thermal Neutron Scattering Laws and Thermophysical Properties

NUCLEAR REACTIONS H, Y(n, n), E thermal; calculated phonon density of states for yttrium and hydrogen under harmonic approximation in yttrium hydride using Ab initio density functional theory (DFT); deduced thermal scattering laws (TSLs) for yttrium hydride using NJOY2016 code. Comparison with ENDF/B-VIII.0 evaluations.

doi: 10.1080/00295639.2020.1851632
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2008BH08      Phys.Rev. C 77, 065503 (2008)

M.Bhattacharya, D.Melconian, A.Komives, S.Triambak, A.Garcia, E.G.Adelberger, B.A.Brown, M.W.Cooper, T.Glasmacher, V.Guimaraes, P.F.Mantica, A.M.Oros-Peusquens, J.I.Prisciandaro, M.Steiner, H.E.Swanson, S.L.Tabor, M.Wiedeking

ft value of the 0+ → 0+ β+ decay of 32Ar: A measurement of isospin symmetry breaking in a superallowed decay

RADIOACTIVITY 32Ar(β+) [from 9Be(36Ar, X), E=100 MeV/nucleon]; measured Eγ, Iγ, Ep, Ip, pγ-coin. 32Ar; deduced superallowed decay branching ratio, ft value, isospin symmetry breaking correction. 32Cl; deduced levels, J, π. 31S; deduced levels, π. Comparison with theoretical data.

ATOMIC MASSES 32Cl; measured masses. Q-value method.

doi: 10.1103/PhysRevC.77.065503
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2008KA32      Phys.Rev. C 78, 037303 (2008)

R.A.Kaye, C.S.Myers, J.Doring, S.L.Tabor, S.M.Gerbick, T.D.Baldwin, D.B.Campbell, C.Chandler, M.W.Cooper, M.A.Hallstrom, C.R.Hoffman, J.Pavan, L.A.Riley, M.Wiedeking

Linear polarization measurements and negative-parity states in 80Sr

NUCLEAR REACTIONS 54Fe(28Si, 2p), E=90 MeV; 58Ni(28Si, 2pα), E=110 MeV; measured Eγ, Iγ, γγ-coin, polarization, multipolarities, mixing ratios, angular correlation, polarization. 80Sr; deduced levels, J, π, bands.

doi: 10.1103/PhysRevC.78.037303
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2007KA13      Phys.Rev. C 75, 034311 (2007)

R.A.Kaye, Y.K.Ryu, S.R.Arora, S.L.Tabor, J.Doring, Y.Sun, T.D.Baldwin, D.B.Campbell, C.Chandler, M.W.Cooper, S.M.Gerbick, O.Grubor-Urosevic, C.R.Hoffman, J.Pavan, L.A.Riley, M.Wiedeking

Transition strengths and degree of deformation in 79Sr

NUCLEAR REACTIONS 54Fe(28Si, n2p), E=90 MeV; measured Eγ, Iγ, γγ-coin, DSA. 79Sr deduced high-spin levels, J, π, configurations, T1/2, B(E2), B(M1), transition quadrupole moments, β2. Comparison with cranked mean-field and projected shell-model predictions.

doi: 10.1103/PhysRevC.75.034311
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2006LE17      Phys.Rev. C 73, 044321 (2006)

S.Lee, S.L.Tabor, T.Baldwin, D.B.Campbell, I.Calderin, C.Chandler, M.W.Cooper, C.R.Hoffman, K.W.Kemper, J.Pavan, A.Pipidis, M.A.Riley, M.Wiedeking

Structure of 26Na from the 14C(14C, d) reaction

NUCLEAR REACTIONS 14C(14C, d), E=22 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin. 26Na deduced levels, J, π, configurations. Shell model analysis.

doi: 10.1103/PhysRevC.73.044321
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2004CL02      Phys.Rev.Lett. 92, 172502 (2004)

R.R.C.Clement, D.Bazin, W.Benenson, B.A.Brown, A.L.Cole, M.W.Cooper, P.A.DeYoung, A.Estrade, M.A.Famiano, N.H.Frank, A.Gade, T.Glasmacher, P.T.Hosmer, W.G.Lynch, F.Montes, W.F.Mueller, G.F.Peaslee, P.Santi, H.Schatz, B.M.Sherrill, M.-J.van Goethem, M.S.Wallace

New Approach for Measuring Properties of rp-Process Nuclei

NUCLEAR REACTIONS H, C(34Ar, 33ArX), E=84 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following neutron removal. 33Ar deduced levels, J, π, spectroscopic factors. 32Cl(p, γ), E=low; calculated astrophysical reaction rates.

doi: 10.1103/PhysRevLett.92.172502
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2004FR33      Nucl.Phys. A746, 551c (2004)

N.Frank, T.Baumann, D.Bazin, R.R.C.Clement, M.W.Cooper, P.Heckman, W.A.Peters, A.Stolz, M.Thoennessen, M.S.Wallace

Half-life limit of 19Mg

NUCLEAR REACTIONS Be(36Ar, X), E=150 MeV/nucleon; measured fragments isotopic yields; deduced no evidence for 19Mg. 19Mg deduced T1/2 upper limit.

doi: 10.1016/j.nuclphysa.2004.09.088
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2004KA32      Phys.Rev. C 69, 064314 (2004)

R.A.Kaye, O.Grubor-Urosevic, S.L.Tabor, J.Doring, Y.Sun, R.Palit, J.A.Sheikh, T.Baldwin, D.B.Campbell, C.Chandler, M.W.Cooper, S.M.Gerbick, C.R.Hoffman, J.Pavan, L.A.Riley, M.Wiedeking

Collective excitations and shape changes in 80Y

NUCLEAR REACTIONS 54Fe(28Si, np), E=90 MeV; measured Eγ, Iγ, γγ-coin, DSA. 80Y deduced high-spin levels, J, π, T1/2, transition quadrupole moments, B(M1), B(E2). Cranked mean-field calculations.

doi: 10.1103/PhysRevC.69.064314
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2003DO01      Phys.Rev. C 67, 014315 (2003)

J.Doring, R.A.Kaye, A.Aprahamian, M.W.Cooper, J.Daly, C.N.Davids, R.C.de Haan, J.Gorres, S.R.Lesher, J.J.Ressler, D.Seweryniak, E.J.Stech, A.Susalla, S.L.Tabor, J.Uusitalo, W.B.Walters, M.Wiescher

Rotational and vibrational excitations in 84Zr studied through in-beam and 84Nb β-decay spectroscopy

NUCLEAR REACTIONS 59Co(28Si, 2np), E=99 MeV; 58Ni(32S, 2pα), E=135 MeV; measured Eγ, Iγ, γγ-coin, angular distributions. 84Zr deduced levels, J, π, rotational and vibrational excitations, deformation. Comparison with level systematics in neighboring nuclides.

RADIOACTIVITY 84Nb(EC) [from 58Ni(28Si, np)]; measured Eγ, Iγ, γγ-, βγ-coin, T1/2; deduced log ft. 84Zr deduced levels, J, π. Mass-separated source.

doi: 10.1103/PhysRevC.67.014315
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2003FR31      Phys.Rev. C 68, 054309 (2003)

N.Frank, T.Baumann, D.Bazin, R.R.C.Clement, M.W.Cooper, P.Heckman, W.A.Peters, A.Stolz, M.Thoennessen, M.S.Wallace

Half-life limit of 19Mg

NUCLEAR REACTIONS Be(36Ar, X), E=150 MeV/nucleon; measured fragment isotopic yields; deduced no evidence for 19Mg. 19Mg deduced T1/2 upper limit.

doi: 10.1103/PhysRevC.68.054309
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2003HO16      Phys.Rev. C 68, 034304 (2003)

C.R.Hoffman, S.L.Tabor, M.W.Cooper, T.Baldwin, D.B.Campbell, C.Chandler, K.W.Kemper, J.Pavan, A.Pipidis, M.A.Riley, M.Wiedeking, B.A.Brown

Structure of T=2 24Ne from 14C on 14C

NUCLEAR REACTIONS 14C(14C, α), E=22 MeV; measured Eγ, Iγ, Eα, γγ-, αγ-coin. 24Ne deduced levels, J, π, configurations. Comparison with shell model predictions, level systematics in neighboring isotopes.

doi: 10.1103/PhysRevC.68.034304
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2002CO11      Phys.Rev. C65, 051302 (2002)

M.W.Cooper, S.L.Tabor, T.Baldwin, D.B.Campbell, C.Chandler, C.R.Hoffman, K.W.Kemper, J.Pavan, A.Pipidis, M.A.Riley, M.Wiedeking

T = 5/2 27Na from 14C + 14C, and the N = 16 Shell Gap

NUCLEAR REACTIONS 14C(14C, p), E=22 MeV; measured Eγ, Iγ, Ep, γγ-, (charged particle)γ-coin. 27Na deduced levels, J, π, configurations. Shell model analysis.

doi: 10.1103/PhysRevC.65.051302
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2002CU04      Phys.Rev. C66, 024315 (2002)

N.Curtis, D.D.Caussyn, C.Chandler, M.W.Cooper, N.R.Fletcher, R.W.Laird, J.Pavan

Evidence for a molecular rotational band in the 14C + α decay of 18O and the α decay of 22Ne

NUCLEAR REACTIONS 14C(18O, α14C), (18O, α18O), E=102 MeV; measured particle spectra, angular correlations. 18O deduced levels, J, π, molecular rotational band. 22Ne deduced α-decay features.

doi: 10.1103/PhysRevC.66.024315
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2002KE04      Phys.Rev. C65, 044613 (2002)

N.Keeley, E.E.Bartosz, P.D.Cathers, M.W.Cooper, K.W.Kemper, F.Marechal, E.G.Myers, B.G.Schmidt, K.Rusek

7Li + 12C: Complete sets of analyzing powers for inelastic scattering and single-nucleon stripping

NUCLEAR REACTIONS 12C(polarized 7Li, 7Li'), (polarized 7Li, 6Li), (polarized 7Li, 6He), E=34 MeV; measured σ(E, θ), analyzing powers. Coupled channels analysis.

doi: 10.1103/PhysRevC.65.044613
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2002TA10      Yad.Fiz. 65, 745 (2002); Phys.Atomic Nuclei 65, 713 (2002)

S.L.Tabor, M.W.Cooper, D.B.Campbell, C.Chandler, K.W.Kemper, A.Pipidis, M.A.Riley, M.Wiedeking, I.Ragnarsson

Structure of Neutron-Rich s-d Shell Nuclei

NUCLEAR REACTIONS 14C(14C, 2n), (14C, p), (14C, α), E=22 MeV; measured Eγ, Iγ, γγ-, (charged particle)γ-coin. 26Mg, 27Na, 24Ne deduced levels, J, π. Comparison with shell model results.

doi: 10.1134/1.1471279
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2001BA57      Phys.Rev. C64, 014606 (2001)

E.E.Bartosz, N.Keeley, P.D.Cathers, M.W.Cooper, K.W.Kemper, F.Marechal, K.Rusek

Reorientation and Breakup Effects in Polarized 7Li + 12C Elastic Scattering

NUCLEAR REACTIONS 12C(polarized 7Li, 7Li), E=34 MeV; measured σ(θ), analyzing powers; deduced reorientation effects. optical model and coupled-discretized-continuum-channels calculations.

doi: 10.1103/PhysRevC.64.014606
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2001CA25      Phys.Rev. C63, 064601 (2001)

P.D.Cathers, E.E.Bartosz, M.W.Cooper, N.Curtis, N.Keeley, K.W.Kemper, F.Marechal, E.G.Myers, B.G.Schmidt, K.Rusek, V.Hnizdo

First Complete Set of Spin 3/2 Nuclear Scattering Analyzing Powers

NUCLEAR REACTIONS 4He(polarized 7Li, 7Li), E(cm)=11.5, 16.5 MeV; measured σ(θ), analyzing powers. Optical model analysis.

doi: 10.1103/PhysRevC.63.064601
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2001CO05      Nucl.Phys. A682, 131c (2001)

M.W.Cooper, D.B.Campbell, C.Chandler, K.W.Kemper, A.Pipidis, I.Ragnarsson, M.A.Riley, M.Wiedeking, S.L.Tabor

New γ Transitions in 27Na from 14C on 14C

NUCLEAR REACTIONS 14C(14C, p), E=22 MeV; measured Eγ, Iγ, γγ-, (particle)γ-coin. 27Na deduced levels, J, π. Comparison with shell model.

doi: 10.1016/S0375-9474(00)00631-X
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2001PR05      Nucl.Phys. A682, 200c (2001)

J.I.Prisciandaro, P.F.Mantica, D.W.Anthony, M.W.Cooper, A.Garcia, D.E.Groh, A.Komives, W.Kumarasiri, P.A.Lofy, A.M.Oros-Peusquens, S.L.Tabor, M.Wiedeking

Low-Energy Structure of Neutron-Rich Cr Isotopes

RADIOACTIVITY 58V(β-) [from 70Zn fragmentation]; measured Eγ, Iγ, βγ-coin, T1/2. 58Cr deduced level, possible J, π. Comparison with neighboring isotopes.

doi: 10.1016/S0375-9474(00)00640-0
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2001PR13      Phys.Lett. 510B, 17 (2001)

J.I.Prisciandaro, P.F.Mantica, B.A.Brown, D.W.Anthony, M.W.Cooper, A.Garcia, D.E.Groh, A.Komives, W.Kumarasiri, P.A.Lofy, A.M.Oros-Peusquens, S.L.Tabor, M.Wiedeking

New Evidence for a Subshell Gap at N = 32

RADIOACTIVITY 58V(β-) [from 9Be(70Zn, X)]; measured Eγ, Iγ, βγ-coin, T1/2. 58Cr deduced level, J, π, configuration, subshell closure. Mass separator. Level systematics in neighboring nuclides discussed.

doi: 10.1016/S0370-2693(01)00565-2
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1999AL01      Phys.Rev.Lett. 82, 41 (1999)

T.Alexopoulos, L.Antoniazzi, M.Arenton, H.C.Ballagh, H.Bingham, A.Blankman, M.Block, A.Boden, G.Bonomi, Z.L.Cao, T.Y.Chen, K.Clark, D.Cline, S.Conetti, M.Cooper, G.Corti, B.Cox, P.Creti, E.C.Dukes, C.Durandet, V.Elia, A.R.Erwin, L.Fortney, V.Golovatyuk, E.Gorini, F.Grancagnolo, K.Hagan-Ingram, M.Haire, P.Hanlet, M.He, G.Introzzi, M.Jenkins, D.Judd, W.Kononenko, W.Kowald, K.Lau, A.Ledovskoy, G.Liguori, J.Lys, P.O.Mazur, A.P.McManus, S.Misawa, G.H.Mo, C.T.Murphy, K.Nelson, M.Panareo, V.Pogosyan, S.Ramachandran, J.Rhoades, W.Selove, R.P.Smith, L.Spiegel, J.G.Sun, S.Tokar, P.Torre, J.Trischuk, L.Turnbull, D.E.Wagoner, C.R.Wang, C.Wei, W.Yang, N.Yao, N.J.Zhang, B.T.Zou

Measurement of the b(b-bar) Cross Section in 800 GeV/c Proton-Silicon Interactions

NUCLEAR REACTIONS Si(p, X), E at 800 GeV/c; measured b(b-bar) production σ.

doi: 10.1103/PhysRevLett.82.41
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1999CO10      Phys.Rev. C59, 2268 (1999)

M.W.Cooper, D.J.Hartley, R.A.Kaye, K.W.Kemper, M.A.Riley, C.Smith, G.Z.Solomon, D.A.Soltysik, S.L.Tabor

Parity Measurements in Odd-Odd 86Nb

NUCLEAR REACTIONS 58Ni(32S, n3p), E=130 MeV; measured Eγ, Iγ(θ), γ-ray linear polarization. 86Nb deduced levels J, π. Clover detector.

doi: 10.1103/PhysRevC.59.2268
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1993AN23      Nucl.Instrum.Methods Phys.Res. A337, 133 (1993)

A.Andrejczuk, E.Zukowski, L.Dobrzynski, M.J.Cooper

A Spectrometer for Compton Scattering Studies of Heavy Elements and the Problem of Bremsstrahlung Background

ATOMIC PHYSICS 27Al, Cu, Ag(γ, γ), E=412, 662 keV; measured Compton profiles; deduced bremsstrahlung background effects role. High energy Compton spectrometer.

doi: 10.1016/0168-9002(93)91146-E
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1987BA14      Phys.Rev. C35, 1425 (1987)

H.W.Baer, M.J.Leitch, R.L.Burman, M.D.Cooper, A.Z.Cui, B.J.Dropesky, G.C.Giesler, F.Irom, C.L.Morris, J.N.Knudson, J.R.Comfort, D.H.Wright, R.Gilman

Double-Analog Transition 48Ca(π+, π-)48Ti at 35 and 50 MeV

NUCLEAR REACTIONS 48Ca(π+, π-), E=35 MeV; measured σ(θ), σ(E(π)); deduced model parameters. Second-order optical potential calculations.

doi: 10.1103/PhysRevC.35.1425
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1986DE19      Int.J.Appl.Radiat.Isotop. 37, 397 (1986)

O.T.Dejesus, J.A.Martin, N.J.Yasillo, S.J.Gatley, M.D.Cooper

[18F] Fluoride from a Small Cyclotron for the Routine Synthesis of [18F] 2-Fluoro-2-Deoxy-D-Glucose

NUCLEAR REACTIONS, ICPND 18O(p, n)18F, E=15 MeV; measured residual production σ. Activation technique.


1986ER09      Phys.Rev. C34, 1822 (1986)

A.Erell, J.Alster, J.Lichtenstadt, M.A.Moinester, J.D.Bowman, M.D.Cooper, F.Irom, H.S.Matis, E.Piasetzky, U.Sennhauser

Measurements on Isovector Giant Resonances in Pion Charge Exchange

NUCLEAR REACTIONS 40Ca, 60Ni, 90Zr, 120Sn, 140Ce, 208Pb(π+, π0), (π-, π0), E=165 MeV; measured σ(θ(π), E(π)). 40Ca, 60Ni, 90Zr, 120Sn, 140Ce, 208Pb deduced isovector giant resonances, excitation σ, Γ. DWIA calculations.

doi: 10.1103/PhysRevC.34.1822
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1986FI11      Phys.Rev. C34, 619 (1986)

D.H.Fitzgerald, H.W.Baer, J.D.Bowman, M.D.Cooper, F.Irom, N.S.P.King, M.J.Leitch, E.Piasetzky, W.J.Briscoe, M.E.Sadler, K.J.Smith, J.N.Knudson

Forward-Angle Cross Sections for Pion-Nucleon Charge Exchange between 100 and 150 MeV/c

NUCLEAR REACTIONS 1H(π-, π0), E at 100-150 MeV/c; measured σ(θ) vs momentum; deduced σ(θ=0°), s-, p-wave interference minimum parameters, isospin-odd, s-wave scattering length. Partial wave analyses.

doi: 10.1103/PhysRevC.34.619
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1986LE01      Phys.Rev. C33, 278 (1986)

M.J.Leitch, H.W.Baer, J.D.Bowman, M.D.Cooper, E.Piasetzky, U.Sennhauser, H.J.Ziock, F.Irom, P.B.Siegel, M.A.Moinester

Pion Single Charge Exchange Angular Distributions at T(π) = 48 MeV

NUCLEAR REACTIONS 39K, 48Ca(π+, π0), E=48 MeV; measured σ(θ); deduced angle integrated σ. 48Sc deduced IAS excitation. 39Ca deduced IAS excitation, large quadrupole strength.

doi: 10.1103/PhysRevC.33.278
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1986PI10      Nucl.Instrum.Methods Phys.Res. A251, 536 (1986)

T.Pitkanen, D.Laundy, R.S.Holt, M.J.Cooper

The Multiple Scattering Profile in Gamma Ray Compton Studies

NUCLEAR REACTIONS Ni(γ, γ'), E=662 keV; measured multiply scattered Eγ, Iγ. Monte Carlo calculations.

doi: 10.1016/0168-9002(86)90649-2
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1986SI11      Phys.Rev. C34, 267 (1986)

E.R.Siciliano, M.D.Cooper, M.B.Johnson, M.J.Leitch

Effects of Nuclear Correlations on Low-Energy Pion Charge-Exchange Scattering

NUCLEAR REACTIONS 14C, 48Ca(π+, π+), E=50 MeV; calculated radial distortion functions. 14C, 48Ca(π+, π0), 1H(π-, π0), E=50 MeV; calculated σ(θ). Isospin invariant optical potential.

doi: 10.1103/PhysRevC.34.267
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1986UL01      Phys.Rev. C33, 2092 (1986)

J.L.Ullmann, P.W.F.Alons, J.J.Kraushaar, J.H.Mitchell, R.J.Peterson, R.A.Ristinen, J.N.Knudson, J.R.Comfort, H.W.Baer, J.D.Bowman, M.D.Cooper, D.H.Fitzgerald, F.Irom, M.J.Leitch, E.Piasetzky

Pion Single Charge Exchange on 14C from 35 to 295 MeV

NUCLEAR REACTIONS 14C(π+, π0), E=35-295 MeV; measured σ(θ), σ(E(π)); deduced parameters. 14N deduced IAS excitation σ. Comparison with models.

doi: 10.1103/PhysRevC.33.2092
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1985IR01      Phys.Rev. C31, 1464 (1985)

F.Irom, H.W.Baer, J.D.Bowman, M.D.Cooper, E.Piasetzky, U.Sennhauser, H.J.Ziock, M.J.Leitch, A.Erell, M.A.Moinester, J.R.Comfort

Pion Single Charge Exchange on 7Li at Low Energies

NUCLEAR REACTIONS 7Li(π+, π0), E=33.5, 41.1, 48.7, 58.8 MeV; measured σ(θ), σ(E(π0)). Optical model analysis.

doi: 10.1103/PhysRevC.31.1464
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1985IR02      Phys.Rev.Lett. 55, 1862 (1985)

F.Irom, M.J.Leitch, H.W.Baer, J.D.Bowman, M.D.Cooper, B.J.Dropesky, E.Piasetzky, J.N.Knudson

Energy and Mass Dependence of Low-Energy Pion Single Charge Exchange to the Isobaric Analog State

NUCLEAR REACTIONS 7Li, 14C, 15N, 39K, 120Sn(π+, π0), E ≈ 30-80 MeV; measured σ(θ), σ(E(π0)); deduced medium effects suppression evidence, parameter mass dependence. 7Be, 14N, 15O, 39Ca, 120Sb deduced IAS excitation. Pion energy quadratic function fit.

doi: 10.1103/PhysRevLett.55.1862
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1984AS05      Phys.Rev. C30, 946 (1984)

D.Ashery, D.F.Geesaman, R.J.Holt, H.E.Jackson, J.R.Specht, K.E.Stephenson, R.E.Segel, P.Zupranski, H.W.Baer, J.D.Bowman, M.D.Cooper, M.Leitch, A.Erell, J.Comuzzi, R.P.Redwine, D.R.Tieger

Inclusive Pion Single-Charge-Exchange Reactions

NUCLEAR REACTIONS 12,14C, 16,18O, Ni, 120Sn, Pb(π+, π0), (π-, π0), E=160 MeV; measured σ(E(π0), θ(π0)); deduced multiple scattering, neutron screening, Pauli blocking effects.

doi: 10.1103/PhysRevC.30.946
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1984BO27      J.Phys.(Paris), Colloq.C4, 351 (1984); See 1984Bo51

J.D.Bowman, H.W.Baer, M.D.Cooper, N.S.P.King, H.S.Matis, E.Piasetzky, U.Sennhauser, J.Alster, A.Erell, J.Lichtenstadt, M.A.Moinester, F.Irom, Q.Ingram

A Dependence of the Excitation Energy, Width, and Cross Section of the Isovector Monopole Resonance


1984BO51      J.Phys.(Paris), Colloq.C-4, 351 (1984)

J.D.Bowman, H.W.Baer, M.D.Cooper, N.S.P.King, H.S.Matis, E.Piasetzky, U.Sennhauser, J.Alster, A.Erell, J.Lichtenstadt, M.A.Moinester, F.Irom, Q.Ingram

A Dependence of the Excitation Energy, Width, and Cross Section of the Isovector Monopole Resonance

NUCLEAR REACTIONS 40Ca, 60Ni, 90Zr, 120Sn, 140Ce, 208Pb(π-, π0), E=165 MeV; measured σ(E(π0), θ(π0)), σ(θ(π0)). 40Ca, 60Ni, 90Zr(π+, π0), E not given; measured not abstracted. 40Ca, 60Ni, 90Zr deduced GDR, isovector monopole resonance. RPA, DWIA analyses.


1984CO04      Phys.Rev.Lett. 52, 1100 (1984)

M.D.Cooper, H.W.Baer, R.Bolton, J.D.Bowman, F.Cverna, N.S.P.King, M.Leitch, J.Alster, A.Doron, A.Erell, M.A.Moinester, E.Blackmore, E.R.Siciliano

Angular Distribution for 15N(π+, π0)15O(g.s.) at T(π) = 48 MeV

NUCLEAR REACTIONS 15N(π+, π0), E=48 MeV; measured σ(θ), σ(E(π0)); deduced optical potential second-order term role. 15O deduced IAS excitation.

doi: 10.1103/PhysRevLett.52.1100
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1984ER03      Phys.Rev.Lett. 52, 2134 (1984)

A.Erell, J.Alster, J.Lichtenstadt, M.A.Moinester, J.D.Bowman, M.D.Cooper, F.Irom, H.S.Matis, E.Piasetzky, U.Sennhauser, Q.Ingram

Properties of the Isovector Monopole and Other Giant Resonances in Pion Charge Exchange

NUCLEAR REACTIONS 40Ca, 60Ni, 90Zr, 120Sn, 140Ce, 208Pb(π+, π0), (π-, π0), E=165 MeV; measured σ(θ, E(π)). 40K, 40Sc, 60Co, 60Cu, 90Nb, 90Y, 120In, 120Sb, 140La, 140Pr, 208Bi, 208Tl deduced GDR, fragmentation, isovector monopole resonance. DWIA analysis, RPA wave functions.

doi: 10.1103/PhysRevLett.52.2134
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1983AS01      Phys.Rev.Lett. 50, 482 (1983)

D.Ashery, D.F.Geesaman, R.J.Holt, H.E.Jackson, J.R.Specht, K.E.Stephenson, R.E.Segel, P.Zupranski, H.W.Baer, J.D.Bowman, M.D.Cooper, M.Leitch, A.Erell, R.Chefetz, J.Comuzzi, R.P.Redwine, D.R.Tieger

Isospin Effects in Pion Single-Charge-Exchange Reactions

NUCLEAR REACTIONS 12,14C, 16,18O(π+, π0), (π-, π0), E=160 MeV; measured σ(θ), σ(E(π)); deduced σ(ratio), isobar-nucleus interaction isospin dependence.

doi: 10.1103/PhysRevLett.50.482
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1983BA13      Nucl.Phys. A396, 437c (1983)

H.W.Baer, R.Bolton, J.D.Bowman, M.D.Cooper, F.Cverna, N.S.P.King, M.Leitch, H.S.Matis, J.Alster, A.Doron, A.Erell, M.A.Moinester, E.Blackmore, E.R.Siciliano

Study of Isovector Resonances with Pion Charge Exchange

NUCLEAR REACTIONS 12C, 40Ca, 90Zr, 120Sn(π+, π0), (π-, π0), E=164 MeV; measured σ(θ), σ(θ, E(π0)). 90Y, 90Nb, 120Sb, 120In deduced isovector monopole, dipole resonances.

doi: 10.1016/0375-9474(83)90037-4
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1983BO07      Phys.Rev.Lett. 50, 1195 (1983)

J.D.Bowman, H.W.Baer, R.Bolton, M.D.Cooper, F.H.Cverna, N.S.P.King, M.Leitch, H.S.Matis, A.Erell, J.Alster, A.Doron, M.A.Moinester, E.Blackmore, E.R.Siciliano

Observation of the Nuclear Isovector Monopole Resonance

NUCLEAR REACTIONS 90Zr, 120Sn(π-, π0), (π+, π0), E=165 MeV; measured σ(θ, E(π)). 90Zr deduced GDR, isovector monopole resonance, Γ. 120Sn deduced IAS, GDR, isovector monopole resonance, Γ.

doi: 10.1103/PhysRevLett.50.1195
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1983IR04      Phys.Rev. C28, 2565 (1983)

F.Irom, J.R.Comfort, R.Jeppesen, J.J.Kraushaar, R.A.Ristinen, W.Tew, J.L.Ullmann, H.W.Baer, J.D.Bowman, M.D.Cooper, E.Piasetzky, U.Sennhauser, A.Erell, M.A.Moinester, E.R.Siciliano

Pion Single Charge Exchange on 14C

NUCLEAR REACTIONS 14C(π+, π0), E=100, 165, 230, 295 MeV; measured σ(E(π)), σ(θ=0°) vs E. 14N deduced IAS excitation energy dependence. Impulse approximation calculations.

doi: 10.1103/PhysRevC.28.2565
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1983JE01      Phys.Rev. C27, 697 (1983)

R.H.Jeppesen, M.J.Jakobson, M.D.Cooper, D.C.Hagerman, M.B.Johnson, R.P.Redwine, G.R.Burleson, K.F.Johnson, R.E.Marrs, H.O.Meyer, I.Halpern, L.D.Knutson

Pion-Nucleus Forward Scattering Amplitudes from Total Cross Section Measurements

NUCLEAR REACTIONS 27Al, 40Ca, 63,65Cu, Sn, 165Ho, Pb(π+, π+), (π+, X), (π-, π-), (π-, X), E=114-215 MeV; measured total σ, attenuation σ; deduced Coulomb distorted forward scattering amplitude real, imaginary parts. Strong absorption model.

doi: 10.1103/PhysRevC.27.697
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1983SE16      Phys.Rev.Lett. 51, 1324 (1983)

U.Sennhauser, E.Piasetzky, H.W.Baer, J.D.Bowman, M.D.Cooper, H.S.Matis, H.J.Ziock, J.Alster, A.Erell, M.A.Moinester, F.Irom

Isobaric Analog States in Pion Single-Charge-Exchange Reactions on and above the (3, 3) Resonance Energy

NUCLEAR REACTIONS 7Li, 14C, 18O, 60Ni, 90Zr, 120Sn, 140Ce, 208Pb(π+, π0), E=165, 230, 295 MeV; measured σ(θ=0°) vs E, σ(θ, E(π0)); deduced mass dependence, (3, 3) resonance role. 7Be, 14N, 18F, 60Cu, 90Nb, 120Sb, 140Pr, 208Bi deduced IAS excitation characteristics, neutron, proton density dependence.

doi: 10.1103/PhysRevLett.51.1324
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1982BA50      Phys.Rev.Lett. 49, 1376 (1982)

H.W.Baer, R.Bolton, J.D.Bowman, M.D.Cooper, F.Cverna, N.S.P.King, M.Leitch, H.S.Matis, J.Alster, A.Doron, A.Erell, M.A.Moinester, E.Blackmore, E.R.Siciliano

Observation of Analogs of the Giant-Dipole Resonance in Pion Single Charge Exchange on 40Ca

NUCLEAR REACTIONS 40Ca(π+, π0), (π-, π0), E=164 MeV; measured σ(θ, E(π0)); deduced σ(π+)/σ(π-). 40Sc deduced IAS. DWIA, Goldhaber-Teller transition density.

doi: 10.1103/PhysRevLett.49.1376
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1982CO01      Phys.Rev. C25, 438 (1982)

M.D.Cooper, H.W.Baer, J.D.Bowman, F.H.Cverna, R.H.Heffner, C.M.Hoffman, N.S.P.King, J.Piffaretti, J.Alster, A.Doron, S.Gilad, M.A.Moinester, P.R.Bevington, E.Winkelmann

3He(π-, π0) Reaction at T(π) = 200 MeV

NUCLEAR REACTIONS 3He(π-, π0), E=200 MeV; measured σ(θ), σ(θ, E(π0)); deduced σ(total) for IAR excitation, effective nucleon number, Pauli blocking. Glauber model.

doi: 10.1103/PhysRevC.25.438
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1982DO02      Phys.Rev.Lett. 48, 989 (1982)

A.Doron, J.Alster, A.Erell, S.Gilad, M.A.Moinester, R.A.Anderson, H.W.Baer, J.D.Bowman, M.D.Cooper, F.H.Cverna, C.M.Hoffman, N.S.P.King, M.J.Leitch, J.P.Piffaretti, P.R.Bevington, E.Winkelmann, C.D.Goodman

Energy Dependence of the Small-Angle Differential Cross Sections to Isobaric Analog States in 7Li(π+, π0)7Be and 13C(π+, π0)13N

NUCLEAR REACTIONS 7Li, 13C(π+, π0), E=70, 100, 150, 165, 180 MeV; measured σ(θ), σ(E(π0)). 13N, 7Be deduced IAS excitation dependence on pion energy.

doi: 10.1103/PhysRevLett.48.989
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1982DO10      Phys.Rev. C26, 189 (1982)

A.Doron, J.Alster, A.Erell, M.A.Moinester, R.A.Anderson, H.W.Baer, J.D.Bowman, M.D.Cooper, F.H.Cverna, C.M.Hoffman, N.S.P.King, M.J.Leitch, J.P.Piffaretti, C.D.Goodman

Angular Distributions of Single Pion Charge Exchange Reactions to Isobaric Analog States in Light Nuclei

NUCLEAR REACTIONS 13C, 15N(π+, π0), E=164 MeV; measured σ(θ). 13N, 15O deduced IAS excitation. Enriched targets. Semiphenomenological isobar doorway, second-order coupled-channels calculations.

doi: 10.1103/PhysRevC.26.189
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1980BA27      Phys.Rev.Lett. 45, 982 (1980)

H.W.Baer, J.D.Bowman, M.D.Cooper, F.H.Cverna, C.M.Hoffman, M.B.Johnson, N.S.P.King, J.Piffaretti, E.R.Siciliano, J.Alster, A.Doron, S.Gilad, M.Moinester, P.R.Bevington, E.Winkelmann

Observation of Isobaric Analog States in Pion Single-Charge-Exchange Reactions

NUCLEAR REACTIONS 7Li, 13C, 27Al, 58Ni, 90Zr, 120Sn, 208Pb(π+, π0), E=98 MeV; measured σ(θ). 7Be, 13N, 27Si, 58Cu, 90Nb, 120Sb, 208Bi deduced IAS. Optical model.

doi: 10.1103/PhysRevLett.45.982
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1979CO13      Phys.Rev. C20, 696 (1979)

M.D.Cooper, R.H.Jeppesen, M.B.Johnson

Coulomb Effects in the Klein-Gordon Equation for Pions

NUCLEAR REACTIONS 208Pb(π+, π+), E=100 MeV; calculated σ(θ). Klein-Gordon equation, Coulomb scattering, spinless particles, point source.

doi: 10.1103/PhysRevC.20.696
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1978BU09      Phys.Rev. C17, 1774 (1978)

R.L.Burman, M.P.Baker, M.D.Cooper, R.H.Heffner, D.M.Lee, R.P.Redwine, J.E.Spencer, T.Marks, D.J.Malbrough, B.M.Preedom, R.J.Holt, B.Zeidman

Pion Double-Charge Exchange on 16O and 18O

NUCLEAR REACTIONS 18O(π+, π-), E=95-139 MeV; measured σ(E). 16O(π+, π-), E=145 MeV; measured σ. 16Ne deduced mass excess.

doi: 10.1103/PhysRevC.17.1774
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1977CO27      Nucl.Phys. A292, 350 (1977)

M.D.Cooper, M.B.Johnson, G.B.West

Coulomb-Nuclear Interference with Pions

NUCLEAR REACTIONS 16O(π+, π+), (π-, π-), E=150-220 MeV; 40Ca(π-, π-), E=20-200 MeV; calculated Coulomb-nuclear interference.

doi: 10.1016/0375-9474(77)90624-8
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1977FI11      Phys.Rev. C16, 2367 (1977)

T.R.Fisher, J.A.Becker, B.A.Watson, H.Marshak, G.R.Burleson, M.D.Cooper, D.C.Hagerman, I.Halpern, M.J.Jakobson, R.H.Jeppesen, K.F.Johnson, L.D.Knutson, R.E.Marrs, H.O.Meyer, R.P.Redwine

Pion Cross Section Measurements on Aligned 165Ho in the (3, 3) Resonance Region

NUCLEAR REACTIONS 165Ho(π+, π+), (π-, π-), E=115, 165, 240 MeV; measured tagged pion removal σ, σ ratios for aligned, unaligned targets.

doi: 10.1103/PhysRevC.16.2367
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1977HO13      Phys.Lett. 69B, 55 (1977)

R.J.Holt, B.Zeidman, D.J.Malbrough, T.Marks, B.M.Preedom, M.P.Baker, R.L.Burman, M.D.Cooper, R.H.Heffner, D.M.Lee, R.P.Redwine, J.E.Spencer

Pion Non-Analog Double Charge Exchange: 16O(π+, π-)16Ne

NUCLEAR REACTIONS 16O(π+, π-), E=145 MeV; measured σ; deduced Q. 16Ne deduced mass excess.

doi: 10.1016/0370-2693(77)90131-9
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1977JA03      Phys.Rev.Lett. 38, 1201 (1977)

M.J.Jakobson, G.R.Burleson, J.R.Calarco, M.D.Cooper, D.C.Hagerman, I.Halpern, R.H.Jeppesen, K.F.Johnson, L.D.Knutson, R.E.Marrs, H.O.Meyer, R.P.Redwine

Neutron Radii of Calcium Isotopes from Pion Total Cross Section Measurements

NUCLEAR REACTIONS 40,44,48Ca(π+, X), (π-, X), E=90-240 MeV; measured total σ(E) differences.

doi: 10.1103/PhysRevLett.38.1201
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1977MA02      Phys.Rev.Lett. 38, 149 (1977)

T.Marks, M.P.Baker, R.L.Burman, M.D.Cooper, R.H.Heffner, R.J.Holt, D.M.Lee, D.J.Malbrough, B.M.Preedom, R.P.Redwine, J.E.Spencer, B.Zeidman

Observation of the Pion Double-Charge-Exchange Reaction 18O(π+, π-)18Ne

NUCLEAR REACTIONS 18O(π+, π-), E=139 MeV; measured σ.

doi: 10.1103/PhysRevLett.38.149
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1976CO10      Phys.Rev. C13, 1334 (1976)

M.D.Cooper, R.A.Eisenstein

Low-Energy-Pion Elastic Scattering from Light Nuclei

NUCLEAR REACTIONS 12C(π+, π+), E=30, 50 MeV; 4He(π+, π+), (π-, π-), E=50-75 MeV; analyzed σ(θ).

doi: 10.1103/PhysRevC.13.1334
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1976CO13      Nucl.Phys. A260, 352 (1976)

M.D.Cooper, M.B.Johnson

Integrated Pion-Nucleus Cross Sections

NUCLEAR REACTIONS 12C, 16O, 40Ca, 90Zr(π, X), E=172 MeV; calculated σ. 208Pb(π+, X), E=50 MeV; calculated σ.

doi: 10.1016/0375-9474(76)90050-6
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1976MA01      Nucl.Phys. A256, 1 (1976)

R.E.Marrs, E.G.Adelberger, K.A.Snover, M.D.Cooper

Upper Limits for Isospin-Forbidden γ-Decays of T=2 States in 20Ne

NUCLEAR REACTIONS 19F(p, γ), E ≈ 4.09, 5.88 MeV; measured σ(E, Eγ). 20Ne deduced isospin-forbidden transition strengths, T=2 levels.

doi: 10.1016/0375-9474(76)90090-7
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1975AD01      Phys.Rev.Lett. 34, 402 (1975)

E.G.Adelberger, H.E.Swanson, M.D.Cooper, J.W.Tape, T.A.Trainor

Parity Mixing in 19F

NUCLEAR REACTIONS 22Ne(polarized p, αγ), E=4.93 MeV; measured Eγ, CP. 19F level deduced parity nonconserving asymmetry.

doi: 10.1103/PhysRevLett.34.402
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1975MA21      Phys.Rev.Lett. 35, 202 (1975)

R.E.Marrs, E.G.Adelberger, K.A.Snover, M.D.Cooper

Mirror γ Decays in 13C and 13N

NUCLEAR REACTIONS 12C(p, γ), E=14.2-14.3 MeV; measured resonance γ-yield. 11B(3He, pγ), (3He, nγ); measured pγ-, nγ-coin. 13N level deduced γ-mixing, B(λ).

doi: 10.1103/PhysRevLett.35.202
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1974CO04      Nucl.Phys. A218, 249 (1974)

M.D.Cooper, W.F.Hornyak, P.G.Roos

Deuteron Stripping to the Single Particle States of 17O

NUCLEAR REACTIONS 16O(d, p), (d, d), E=25.4, 36.0, 63.2 MeV; measured σ(E;Ep, θ), σ(E;Ed, θ). 17O deduced levels. Enriched target.

doi: 10.1016/0375-9474(74)90003-7
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1974CO10      Nucl.Phys. A221, 528 (1974)

M.D.Cooper, W.Galati, W.F.Hornyak

Extraction of Spectroscopic Factors Using R-Matrix Theory

NUCLEAR REACTIONS 16O(n, n), E=0.5-1.3 MeV; measured nothing, analyzed σ(E) data. 17O level deduced S.

doi: 10.1016/0375-9474(74)90479-5
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1970CO06      Nucl.Phys. A142, 445 (1970)

M.D.Cooper, A.S.Figuera, G.Pfeufer, G.Randers-Pehrson

Behavior of the Cross Section for the 9Be(p, p)9Be Reaction Near the 2.06 MeV (p, n) Threshold

NUCLEAR REACTIONS 9Be(p, p), E=1.99-2.10 MeV; measured σ(E).

doi: 10.1016/0375-9474(70)90540-3
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Note: The following list of authors and aliases matches the search parameter M.Cooper: , M.C.COOPER, M.D.COOPER, M.J.COOPER, M.P.COOPER, M.W.COOPER