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NSR database version of August 4, 2015.

Search: Author = G.M.Crawley

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2008AN15     Phys.Rev. C 78, 065803 (2008)

N.Anantaraman, S.M.Austin, B.A.Brown, G.M.Crawley, A.Galonsky, R.G.T.Zegers, B.D.Anderson, A.R.Baldwin, B.S.Flanders, R.Madey, J.W.Watson, C.C.Foster

Electron capture strength for 60, 62Ni and 58, 60, 62, 64Ni(p, n)58, 60, 62, 64Cu reactions at 134.3 MeV

NUCLEAR REACTIONS 58,60,62,64Ni(p, n), E=134.3 MeV; measured neutron spectra, angular distributions, σ; calculated B(GT), reaction rates. 58,60,62,64Cu; deduced levels. Comparison with (n, p) reactions, shell model calculations.

doi: 10.1103/PhysRevC.78.065803
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1743.


2004SH28     Phys.Lett. B 596, 54 (2004)

A.Shrivastava, Y.Blumenfeld, N.Keeley, T.Zerguerras, T.Aumann, D.Bazin, M.Chromik, G.M.Crawley, T.Glasmacher, K.W.Kemper, F.Marechal, D.J.Morrissey, T.Nakamura, A.Navin, E.C.Pollacco, D.Santonocito, B.M.Sherrill, T.Suomijarvi, M.Thoennessen, E.Tryggestad, R.L.Varner

11Be continuum studied through proton scattering

NUCLEAR REACTIONS 1H(11Be, 11Be), (11Be, 11Be'), E=63.7 MeV/nucleon; measured excitation energy spectra, σ(θ). 11Be deduced levels, J, π, configurations.

doi: 10.1016/j.physletb.2004.06.070
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1172.


2000YO09     Phys.Rev. C62, 044604 (2000)

G.H.Yoo, G.M.Crawley, J.H.Kelley, N.A.Orr, J.C.Stasko, J.S.Winfield, S.Gales, S.Fortier, H.Laurent, T.Suomijarvi, J.E.Finck

Proton Decay following the Transfer Reaction (7Li, 6He) on 40Ca and 90Zr

NUCLEAR REACTIONS 40Ca, 90Zr(7Li, 6He), E=50 MeV/nucleon; measured E(6He), proton spectra and angular distribution following residual nucleus decay, (helium)p-coin; deduced reaction mechanism features. Comparison with model predictions.

doi: 10.1103/PhysRevC.62.044604


1999AI02     Phys.Rev. C60, 034614 (1999)

N.Aissaoui, N.Added, N.Carlin, G.M.Crawley, S.Danczyk, J.Finck, M.M.de Moura, D.Hirata, D.J.Morrissey, S.J.Sanders, J.Stasko, M.Steiner, A.A.P.Suaide, E.M.Szanto, A.Szanto de Toledo, M.Thoennessen, J.A.Winger

Strong Absorption Radii from Reaction Cross Section Measurements for Neutron-Rich Nuclei

NUCLEAR REACTIONS Si(30Al, X), (31Al, X), (32Al, X), (33Al, X), (32Si, X), (33Si, X), (34Si, X), (35Si, X), (36Si, X), (34P, X), (35P, X), (36P, X), (37P, X), (38P, X), (39P, X), (36S, X), (37S, X), (38S, X), (39S, X), (40S, X), (41S, X), (39Cl, X), (40Cl, X), (41Cl, X), (42Cl, X), (43Cl, X), (44Cl, X), (41Ar, X), (42Ar, X), (43Ar, X), (44Ar, X), (45Ar, X), (46Ar, X), (44K, X), (45K, X), (46K, X), (47K, X), (48K, X), (46Ca, X), (47Ca, X), (48Ca, X), (49Ca, X), (50Ca, X), (49Sc, X), (50Sc, X), (51Sc, X), (52Sc, X), (53Ti, X), (54Ti, X), E ≈ 38-80 MeV/nucleon; measured mean energy-integrated reaction σ. 30,31,32,33Al, 32,33,34,35,36Si, 34,35,36,37,38,39P, 36,37,38,39,40,41S, 39,40,41,42,43,44Cl, 41,42,43,44,45,46Ar, 44,45,46,47,48K, 46,47,48,49,50Ca, 49,50,51,52Sc, 53,54Ti deduced strong absorption radii. Secondary beams from 55Mn fragmentation.

doi: 10.1103/PhysRevC.60.034614


1997LI15     Phys.Rev. C56, 250 (1997)

I.Licot, N.Added, N.Carlin, G.M.Crawley, S.Danczyk, J.Finck, D.Hirata, H.Laurent, D.J.Morrissey, M.M.de Moura, H.R.Schelin, J.Stasko, M.Steiner, A.A.P.Suaide, A.Szanto de Toledo, E.M.Szanto, M.Thoennessen, J.A.Winger

Reaction Cross Sections and Radii for f-p Shell Exotic Neutron-Rich Nuclei

NUCLEAR REACTIONS, ICPND Si(41Ar, X), (42Ar, X), (43Ar, X), (44Ar, X), (45Ar, X), (46Ar, X), (44K, X), (45K, X), (46K, X), (47K, X), (48K, X), (49K, X), (46Ca, X), (47Ca, X), (48Ca, X), (49Ca, X), (50Ca, X), (51Ca, X), (49Sc, X), (50Sc, X), (51Sc, X), (52Sc, X), (53Sc, X), E=52-69 MeV/nucleon; measured reaction σ. 41,42,43,44,45,46Ar, 44,45,46,47,48,49K, 46,47,48,49,50,51Ca, 49,50,51,52,53Sc deduced strong absorption radii, neutron separation energies. Comparison to Glauber model, RMF theory.

doi: 10.1103/PhysRevC.56.250


1996BE16     Nucl.Phys. A599, 265c (1996)

D.Beaumel, S.Fortier, S.Gales, J.Guillot, H.Langevin-Joliot, H.Laurent, J.M.Maison, J.Vernotte, J.Bordewijk, S.Brandenburg, A.Krasznahorkay, G.M.Crawley, C.P.Massolo, M.Renteria, A.Khendriche

Decay Properties of High-Lying Single-Particles Modes

NUCLEAR REACTIONS 64Ni, 90Zr, 120Sn, 208Pb(α, n3He), E=120 MeV; measured neutron spectra, nn(θ). 91Zr, 209Pb deduced resonances, J, π, neutron decay features.

doi: 10.1016/0375-9474(96)00068-1


1996LH02     Phys.Rev. C54, 593 (1996)

I.Lhenry, T.Suomijarvi, Y.Blumenfeld, Ph.Chomaz, N.Frascaria, J.P.Garron, J.C.Roynette, J.A.Scarpaci, D.Beaumel, S.Fortier, S.Gales, H.Laurent, A.Gillibert, G.M.Crawley, J.Finck, G.Yoo, J.Barreto

One-Nucleon Transfer Reactions to Continuum States Induced by Heavy Ion Projectiles

NUCLEAR REACTIONS 207Pb, 209Bi, 59Co(20Ne, 19Ne), (20Ne, 21Na), (20Ne, 19F), E=48 MeV/nucleon; 207Pb, 209Bi, 63Cu(36Ar, 35Ar), (36Ar, 37K), E=42 MeV/nucleon; measured σ(E, θ); deduced structure, particle-hole states, collective strength. RPA, DWBA calculations, Bonaccorso-Brink single-particle transfer model.

doi: 10.1103/PhysRevC.54.593


1996WI05     Phys.Rev. C54, 125 (1996)

J.S.Winfield, D.Beaumel, S.Gales, H.Laurent, I.Lhenry, J.M.Maison, G.M.Crawley, S.Danczyk, S.E.Hirzebruch, J.C.Stasko, T.Suomijarvi

The (7Li, 7Beγ) Reaction and Isovector Spin Strength in 40Ca

NUCLEAR REACTIONS 12C, 40Ca(7Li, 7Be), E=70 MeV/nucleon; measured (particle)γ-coin. 40Ca deduced continuum isovector spin strength. Spectrometer, CsI detectors.

doi: 10.1103/PhysRevC.54.125


1995FO19     Phys.Rev. C52, 2401 (1995)

S.Fortier, D.Beaumel, S.Gales, J.Guillot, H.Langevin-Joliot, H.Laurent, J.M.Maison, J.Bordewijk, S.Brandenburg, A.Krasznahorkay, G.M.Crawley, C.P.Massolo, M.Renteria, A.Khendriche

Damping of Unbound Single-Particle Modes

NUCLEAR REACTIONS 64Ni, 90Zr, 120Sn(α, 3He), E=120 MeV; measured 3He-spectra, neutron spectra following residual decay, n(3He)-coin. 91Zr, 121Sn, 65Ni deduced non-statistical neutron branching ratios. Statistical analysis.

doi: 10.1103/PhysRevC.52.2401


1995LH02     Nucl.Phys. A583, 115c (1995)

I.Lhenry, D.Beaumel, S.Fortier, S.Gales, H.Laurent, J.M.Maison, F.Azaiez, Y.Blumenfeld, J.Guillot, H.Langevin-Joliot, T.Suomijarvi, S.Brandenburg, G.M.Crawley, J.Finck, J.Stasko

A Search for the Isovector Monopole Resonance in 208Pb

NUCLEAR REACTIONS 208Pb(13C, 13N), E=60 MeV/nucleon; measured σ(θ), missing energy spectra. 208Tl deduced level, neutron decay features.

doi: 10.1016/0375-9474(94)00643-2


1994BE07     Phys.Rev. C49, 2444 (1994)

D.Beaumel, S.Fortier, S.Gales, J.Guillot, H.Langevin-Joliot, H.Laurent, J.M.Maison, J.Vernotte, J.A.Bordewijk, S.Brandenburg, A.Krasznahorkay, G.M.Crawley, C.P.Massolo, M.Renteria

Decay Modes of High-Lying Single-Particle States in 209Pb

NUCLEAR REACTIONS 208Pb(α, n3He), E=122 MeV; measured E(3He), (3He)n-, γ(3He)-coin, neutron angular correlations. 209Pb deduced direct decay branching ratios, Γ(spreading)/Γ, Γn/Γ for structures at high excitation. Statistical model calculations.

doi: 10.1103/PhysRevC.49.2444


1994LA10     Nucl.Phys. A569, 297c (1994)

H.Laurent, S.Gales, D.Beaumel, G.M.Crawley, J.E.Finck, S.Fortier, J.M.Maison, C.P.Massolo, D.J.Mercer, J.S.Winfield, G.H.Yoo

Spin-Isospin Multipole Excitations by Means of the (6Li, 6He) Reaction at 100 A.MeV

NUCLEAR REACTIONS 12,13C, 58Ni, 90Zr, 208Pb(6Li, 6He), E=100 MeV/nucleon; measured σ(θ, E(6He)). 13,12N, 58Cu, 90Nb, 208Bi deduced spin-isospin multipole excitation features.

doi: 10.1016/0375-9474(94)90120-1


1993WI03     Phys.Lett. 299B, 214 (1993)

J.A.Winger, D.P.Bazin, W.Benenson, G.M.Crawley, D.J.Morrissey, N.A.Orr, R.Pfaff, B.M.Sherrill, M.Steiner, M.Thoennessen, S.J.Yennello, B.M.Young

Halflife Measurements of the rp-Process Nuclei 61Ga, 63Ge, and 65As

RADIOACTIVITY 61,62Ga, 63,64Ge, 65,66As(β+)[from 58Ni(78Kr, X), E=75 MeV/nucleon]; measured TOF, Ie, Ee summed decay spectra; deduced T1/2, implications to rp-process.

doi: 10.1016/0370-2693(93)90250-L


1993WI18     Phys.Rev. C48, 3097 (1993)

J.A.Winger, D.P.Bazin, W.Benenson, G.M.Crawley, D.J.Morrissey, N.A.Orr, R.Pfaff, B.M.Sherrill, M.Thoennessen, S.J.Yennello, B.M.Young

Half-Life Measurements for 61Ga, 63Ge, and 65As and Their Importance in the rp Process

RADIOACTIVITY 61,62Ga, 63Ge, 65,66As(β+) [from 58Ni(84Kr, X), E=75 MeV/nucleon]; measured β-decay summed spectra. 66As, 62,61Ga, 63Ge deduced T1/2. 65As deduced T1/2, proton partial T1/2, Q(β), mass excess, proton separation energy. Implications to rp-process.

NUCLEAR REACTIONS 58Ni(84Kr, X), E=75 MeV/nucleon; measured β-decay summed spectra; deduced evidence for 66Se.

doi: 10.1103/PhysRevC.48.3097


1993YO01     Phys.Rev. C47, 1200 (1993)

G.H.Yoo, G.M.Crawley, N.A.Orr, J.S.Winfield, J.E.Finck, S.Gales, Ph.Chomaz, I.Lhenry, T.Suomijarvi

High-Lying Resonances Observed in Heavy-Ion Transfer Reactions

NUCLEAR REACTIONS 207,208Pb, 209Bi, 89Y, 90,91Zr(7Li, 6Li), (7Li, 6He), (12C, 13C), (12C, 13N), E=30 MeV/nucleon; measured σ(θ, E); deduced structure.

doi: 10.1103/PhysRevC.47.1200


1992KR13     Phys.Rev. C46, 1416 (1992)

D.Krofcheck, W.Bauer, G.M.Crawley, S.Howden, C.A.Ogilvie, A.Vander Molen, G.D.Westfall, W.K.Wilson, R.S.Tickle, C.Djalali, C.Gale

Disappearance of Flow as a Probe of the Nuclear Equation of State

NUCLEAR REACTIONS 93Nb(93Nb, X), E=97, 145 MeV/nucleon; 139La(139La, X), E=100-160 MeV/nucleon; measured fragment in-plane transverse momentum spectra, multiplicity distributions; deduced flow disappearance as balance between attractive, repulsive scattering.

doi: 10.1103/PhysRevC.46.1416


1991MA06     Phys.Rev. C43, 1687 (1991)

C.P.Massolo, S.Fortier, S.Gales, F.Azaiez, E.Gerlic, J.Guillot, E.Hourani, H.Langevin-Joliot, J.M.Maison, J.P.Schapira, G.M.Crawley

Onset of Neutron Single-Particle Strengths in the Tin Isotopic Chain

NUCLEAR REACTIONS 124,122,120,118,116,112Sn(α, 3He), E=183 MeV; measured σ(θ) vs excitation energy; deduced model parameters. 113,117,119,121,123,125Sn levels deduced L, C2S, neutron particle response function. Enriched targets. DWBA analysis.

doi: 10.1103/PhysRevC.43.1687


1990FO04     Phys.Rev. C41, 2689 (1990)

S.Fortier, S.Gales, S.M.Austin, W.Benenson, G.M.Crawley, C.Djalali, J.S.Winfield, G.Yoo

One-Nucleon-Transfer Reactions Induced by 20Ne at 500 and 600 MeV

NUCLEAR REACTIONS 90Zr, 208Pb(20Ne, 19Ne), (20Ne, 21Ne), (20Ne, 21Na), E=500, 600 MeV; measured σ(fragment E, θ) vs excitation. 91Zr, 209Pb deduced structure characteristics. DWBA analysis. Enriched targets.

doi: 10.1103/PhysRevC.41.2689


1989CR02     Phys.Rev. C39, 311 (1989)

G.M.Crawley, C.Djalali, N.Marty, M.Morlet, A.Willis, N.Anantaraman, B.A.Brown, A.Galonsky

Isovector and Isoscalar Spin-Flip Excitations in Even-Even s-d Shell Nuclei Excited by Inelastic Proton Scattering

NUCLEAR REACTIONS 24,26Mg, 28Si, 32S(p, p'), E=201 MeV; measured σ(θ). 24,26Mg, 28Si, 32S deduced 1+ states, B(M1). Enriched targets. DWBA analysis, shell model calculations.

doi: 10.1103/PhysRevC.39.311


1989KR11     Phys.Rev.Lett. 63, 2029 (1989)

D.Krofcheck, W.Bauer, G.M.Crawley, C.Djalali, S.Howden, C.A.Ogilvie, A.Vander Molen, G.D.Westfall, W.K.Wilson, R.S.Tickle, C.Gale

Disappearance of Flow in Heavy-Ion Collisions

NUCLEAR REACTIONS 139La(139La, X), E=50-130 MeV/nucleon; measured average in-plane transverse momentum vs c.m. rapidity; deduced flow disappearance.

doi: 10.1103/PhysRevLett.63.2029


1989WI07     Phys.Rev. C39, 1395 (1989)

J.S.Winfield, E.Adamides, S.M.Austin, G.M.Crawley, M.F.Mohar, C.A.Ogilvie, B.Sherrill, M.Torres, G.Yoo, A.Nadasen

12C-Induced Single Particle Transfer Reactions at E/A = 50 MeV

NUCLEAR REACTIONS 90Zr, 12C(12C, 13C), 208Pb, 27Al(12C, 11B), 40Ca(12C, 11C), E=600 MeV; measured σ(θ). 11C, 28Si, 41Ca, 89Y, 209Bi level deduced spectroscopic factors.

doi: 10.1103/PhysRevC.39.1395


1988WI09     Phys.Lett. 203B, 345 (1988)

J.S.Winfield, S.M.Austin, G.M.Crawley, C.Djalali, C.A.Ogilvie, R.J.Smith, Z.Chen, M.Torres

Energy Dependence of 12C + 12C Single-Neutron Transfer Cross Sections

NUCLEAR REACTIONS 12C(12C, 13C), E=25, 35, 50 MeV/nucleon; measured σ(θ); deduced σ(E), model parameters.

doi: 10.1016/0370-2693(88)90180-3


1987DJ01     Phys.Rev. C35, 1201 (1987)

C.Djalali, G.M.Crawley, B.A.Brown, V.Rotberg, G.Caskey, A.Galonsky, N.Marty, M.Morlet, A.Willis

Spin-Flip Transitions in 16O and 18O Excited by Inelastic Proton Scattering

NUCLEAR REACTIONS 16,18O(p, p'), E=201 MeV; measured σ(θ). 16,18O deduced levels, J, π, B(M1). Gas targets, DWBA analysis.

doi: 10.1103/PhysRevC.35.1201
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0042.


1987FO16     Phys.Rev. C36, 1830 (1987)

S.Fortier, S.Gales, S.M.Austin, W.Benenson, G.M.Crawley, C.Djalali, J.H.Lee, J.van der Plicht, J.S.Winfield

Search for High Excitation Energy Structures in 90Zr and 208Pb, via 20Ne Inelastic Scattering

NUCLEAR REACTIONS 90Zr, 208Pb(20Ne, 20Ne'), E=500, 600 MeV; measured σ(E(20Ne')); deduced structure, excitation mechanism.

doi: 10.1103/PhysRevC.36.1830


1987JA06     Phys.Rev. C35, 1751 (1987)

B.V.Jacak, G.D.Westfall, G.M.Crawley, D.Fox, C.K.Gelbke, L.H.Harwood, B.E.Hasselquist, W.G.Lynch, D.K.Scott, H.Stocker, M.B.Tsang, G.Buchwald, T.J.M.Symons

Fragment Production in Intermediate Energy Heavy Ion Reactions

NUCLEAR REACTIONS Ca, Au(40Ar, X), E=42, 92, 137 MeV/nucleon; Al, Au(20Ne, X), E=100, 156 MeV/nucleon; measured σ(fragment E, θ), for X=1,2,3H, 3,4,6He, 6,7,8,9Li, 7,9,10Be, 10,11,12B, C, N; deduced moving source parameters. NaI-Si, multi-Si telescopes. Coalescence, quantum statistical models.

doi: 10.1103/PhysRevC.35.1751


1987WI03     Nucl.Phys. A464, 315 (1987)

A.Willis, M.Morlet, N.Marty, C.Djalali, G.M.Crawley, A.Galonsky, V.Rotberg, B.A.Brown

Excitation of 1+ amd 2- States in the Neon Isotopes

NUCLEAR REACTIONS 20,22Ne(p, p'), E=201 MeV; measured σ(θ). 20,22Ne deduced levels, J, π. DWIA calculations.

doi: 10.1016/0375-9474(87)90340-X
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0849.


1985DJ01     Phys.Rev. C31, 758 (1985)

C.Djalali, N.Marty, M.Morlet, A.Willis, J.-C.Jourdain, N.Anantaraman, G.M.Crawley, A.Galonsky

Proton Excitation of 1+ States in 208Pb and a Lower Limit on the Strength of the Isoscalar Spin-Flip Part of the Effective Nucleon-Nucleon Interaction

NUCLEAR REACTIONS 208Pb(p, p'), E=201 MeV; measured σ(θ); deduced spin-flip interaction volume integral. 208Pb deduced isovector M1 transition strength. DWBA analysis.

doi: 10.1103/PhysRevC.31.758


1985DJ02     Phys.Lett. 164B, 269 (1985)

C.Djalali, N.Marty, M.Morlet, A.Willis, J.C.Jourdain, D.Bohle, U.Hartmann, G.Kuchler, A.Richter, G.Caskey, G.M.Crawley, A.Galonsky

On the Nature of Low-Lying Collective 1+ States in the Heavy Deformed Nuclei 154Sm, 156Gd and 164Dy and in the f7/2 Shell Nucleus 46Ti

NUCLEAR REACTIONS 46Ti, 154Sm, 156Gd, 164Dy(p, p'), E=201 MeV; measured σ(Ep'), σ(θ). 46Ti(e, e'), E=30 MeV; 156Gd(e, e'), E=25 MeV; measured σ(E(e')). 46Ti, 154Sm, 146Gd, 164Dy deduced B(M1), spin contribution upper limit to M1 excitations.

doi: 10.1016/0370-2693(85)90324-7


1985FI05     Nucl.Phys. A441, 57 (1985)

J.E.Finck, G.M.Crawley, D.Weber, P.A.Smith

The 206,204Pb(p, α)203,201Tl Reactions at 35 MeV

NUCLEAR REACTIONS 204,206Pb(p, α), E=35 MeV; measured σ(Eα), σ(θ). 201,203Tl deduced levels, J, π. Cluster model, DWBA analysis.

doi: 10.1016/0375-9474(85)90167-8
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0068.


1985FR13     Phys.Rev. C32, 975 (1985)

K.A.Frankel, J.A.Bistirlich, R.Bossingham, H.R.Bowman, K.M.Crowe, C.J.Martoff, D.L.Murphy, J.O.Rasmussen, J.P.Sullivan, E.Yoo, W.A.Zajc, J.P.Miller, O.Hashimoto, M.Koike, J.Peter, W.Benenson, G.M.Crawley, E.Kashy, J.A.Nolen, Jr., J.Quebert

Pion Production Near Mid-Rapidity in High-Energy Heavy-Ion Collisions

NUCLEAR REACTIONS C, Ca, U(40Ar, X), E=1050 MeV/nucleon; 9Be, 23Na, 19F(20Ne, X), E=655 MeV/nucleon; measured σ(θ(π+), E(π+)), σ(θ(π-), E(π-)); deduced ratio. Coulomb effect calculation comparison.

doi: 10.1103/PhysRevC.32.975


1985HA19     Phys.Rev. C32, 145 (1985)

B.E.Hasselquist, G.M.Crawley, B.V.Jacak, Z.M.Koenig, G.D.Westfall, J.E.Yurkon, R.S.Tickle, J.P.Dufour, T.J.M.Symons

Light-Particle-Complex-Fragment Coincidence Cross Sections from Intermediate Energy Nucleus-Nucleus Collisions

NUCLEAR REACTIONS 197Au, 27Al(12C, dX), (12C, tX), E=30 MeV/nucleon; measured inclusive σ(θp, Ep), σ(θd, Ed), σ(θt, Et). 197Au(40Ar, pX), (40Ar, dX), (40Ar, tX), (40Ar, 3HeX), (40Ar, αX), E=92 MeV/nucleon; measured inclusive σ(θp, Ep), σ(θd, Ed), σ(θt, Et), σ(θ(3He), E(3He)), σ(θα, Eα). Moving source model.

doi: 10.1103/PhysRevC.32.145


1985LA15     Phys.Rev. C32, 440 (1985)

B.G.Lay, S.M.Banks, B.M.Spicer, G.G.Shute, V.C.Officer, R.M.Ronningen, G.M.Crawley, N.Anantaraman, R.P.DeVito

Multipole Moments of 176Yb and 182W Nuclei from Inelastic Scattering of 134 MeV Protons

NUCLEAR REACTIONS 176Yb, 182W(polarized p, p), (polarized p, p'), E=134 MeV; measured σ(Ep'), σ(θ), asymmetry vs θ; deduced optical model parameters. 176Yb, 182W deduced β2, β4, β6, multipole moments. Phenomenological optical model, coupled-channels analysis.

doi: 10.1103/PhysRevC.32.440


1985SE16     Aust.J.Phys. 38, 27 (1985)

M.E.Sevior, G.M.Crawley, D.G.Sargood

States in 40Ca near 12 MeV Excitation from the 39K(p, γ)40Ca Reaction

NUCLEAR REACTIONS 39K(p, γ), (p, p'γ), E=3.79-3.84 MeV; measured Eγ, Iγ, σ(E, Eγ). 40Ca deduced resonances, possible J, π, resonance strength.


1985WE14     Nucl.Instrum.Methods 238, 347 (1985)

G.D.Westfall, J.E.Yurkon, J.Van Der Plicht, Z.M.Koenig, B.V.Jacak, R.Fox, G.M.Crawley, M.R.Maier, B.E.Hasselquist, R.S.Tickle, D.Horn

A Logarithmic Detection System Suitable for a 4π Array

NUCLEAR REACTIONS 197Au(14N, X), E=35 MeV/nucleon; 58Ni(35Cl, X), E=230 MeV; 12C(12C, X), E=30 MeV/nucleon; measured fragment, charge spectra.


1984AN05     Phys.Rev.Lett. 52, 1409 (1984)

N.Anantaraman, B.A.Brown, G.M.Crawley, A.Galonsky, C.Djalali, N.Marty, M.Morlet, A.Willis, J.-C.Jourdain, B.H.Wildenthal

Observation of Quenching in Isoscalar and Isovector 0+ → 1+ Transitions in 28Si(p, p')

NUCLEAR REACTIONS 28Si(p, p'), E=201 MeV; measured σ(Ep'), σ(θ). 28Si levels deduced excitation σ, B(M1), isoscalar, isovector channel quenching. DWIA calculations.

doi: 10.1103/PhysRevLett.52.1409


1984GA24     Phys.Lett. 144B, 323 (1984)

S.Gales, C.P.Massolo, F.Azaiez, S.Fortier, E.Gerlic, J.Guillot, E.Hourani, J.M.Maison, J.P.Schapira, G.M.Crawley

High-Lying Neutron Particle States Observed via the (α, 3He) Reaction at 183 MeV

NUCLEAR REACTIONS 116,118,120Sn(α, 3He), E=183 MeV; measured σ(θ, E(3He)), σ(θ). 117,119Sn deduced high lying neutron states. 121Sn deduced high lying neutron states, possible J, π, C2S. DWBA analysis.

doi: 10.1016/0370-2693(84)91270-X


1984WE03     Phys.Rev. C29, 861 (1984)

G.D.Westfall, Z.M.Koenig, B.V.Jacak, L.H.Harwood, G.M.Crawley, M.W.Curtin, C.K.Gelbke, B.Hasselquist, W.G.Lynch, A.D.Panagiotou, D.K.Scott, H.Stocker, M.B.Tsang

Light Particle Spectra from 35 MeV/Nucleon 12C-Induced Reactions on 197Au

NUCLEAR REACTIONS 197Au(12C, pX), (12C, dX), (12C, tX), (12C, 3HeX), (12C, αX), (12C, 6HeX), E=35 MeV/nucleon; measured inclusive σ(Ep, θ), σ(Ed, θ), σ(Et, θ), σ(E(3He), θ), σ(Eα, θ), σ(E(6He, θ)); deduced moving source parameters, composite particle to proton yield ratio. Quantum statistical, hydrodynamic, thermal models.

doi: 10.1103/PhysRevC.29.861


1983CR01     Phys.Lett. 127B, 322 (1983)

G.M.Crawley, N.Anantaraman, A.Galonsky, C.Djalali, N.Marty, M.Morlet, A.Willis, J.-C.Jourdain

Observation of l=0, Spin-Flip Transitions in 48Ca

NUCLEAR REACTIONS 48Ca(p, p'), E=201 MeV; measured σ(Ep') vs θ ≤ 12°; deduced optical model parameters. 48Ca deduced L=0, spin-flip transition strength. DWBA analysis.

doi: 10.1016/0370-2693(83)91009-2


1983DJ05     Nucl.Phys. A410, 399 (1983); Erratum Nucl.Phys. A417, 564 (1984)

C.Djalali, N.Marty, M.Morlet, A.Willis, J.C.Jourdain, N.Anantaraman, G.M.Crawley, A.Galonsky, J.Duffy

Excitation of ΔL = 0 Spin-Flip Transitions in the N = 28 Isotones by 201 MeV Proton Inelastic Scattering

NUCLEAR REACTIONS 50Ti, 52Cr, 54Fe(p, p'), E=201 MeV; measured σ(θ). 50Ti, 52Cr, 54Fe deduced 1+ states. DWIA calculations.

doi: 10.1016/0375-9474(83)90633-4


1983FI10     Nucl.Phys. A407, 163 (1983)

J.E.Finck, G.M.Crawley, J.A.Nolen, Jr., R.T.Kouzes

A Study of 206Pb by Inelastic Scattering of 35 MeV Protons

NUCLEAR REACTIONS 206Pb(p, p'), E=35 MeV; measured σ(Ep'), σ(θ). 206Pb deduced levels, L, deformation β(L). Collective, microscopic models, RPA, TDA wave functions.

doi: 10.1016/0375-9474(83)90313-5
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0672.


1983GA07     Nucl.Phys. A398, 19 (1983)

S.Gales, G.M.Crawley, D.Weber, B.Zwieglinski

Neutron-Hole Strength Distributions in Heavy Nuclei (II). The 144,148,152Sm(3He, α)143,147,151Sm and the 144,148,150,152,154Sm(p, d)143,147,149,151,153Sm Reactions

NUCLEAR REACTIONS 144,148,152Sm(3He, α), E=70 MeV; measured σ(Eα, θ); 144,148,150,152,154Sm(p, d), E=42 MeV; measured σ(Ed, θ). 143,147,149,151,153Sm deduced levels, L, J, π, C2S. Enriched target, magnetic spectrometer. Zero-range, finite-range DWBA calculations, inner-shells analysis. Comparison with the quasiparticle phonon, Nilsson models.

doi: 10.1016/0375-9474(83)90646-2


1983KA18     Phys.Rev. C28, 1065 (1983)

J.Kasagi, G.M.Crawley, E.Kashy, J.Duffy, S.Gales, E.Gerlic, D.Friesel

Highly Excited Hole Strength Observed in the 90Zr(p(pol), d)89Zr Reaction

NUCLEAR REACTIONS 90Zr(polarized p, d), E=90 MeV; measured σ(Ed), σ(θ), analyzing power vs θ. 89Zr deduced levels, J, π, C2S. Finite-range DWBA.

doi: 10.1103/PhysRevC.28.1065
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0388.


1983MA09     Nucl.Phys. A396, 145c (1983)

N.Marty, C.Djalali, M.Morlet, A.Willis, J.C.Jourdain, N.Anantaraman, G.M.Crawley, A.Galonsky

Proton Excitation of the M1 Resonances in the Ni Isotopes

NUCLEAR REACTIONS 58,60,62,64Ni(p, p'), E=200 MeV; measured σ(θ, Ep'). 58,60,62,64Ni deduced M1 resonances, transition strength distribution, isospin components.

doi: 10.1016/0375-9474(83)90015-5


1983RO11     Phys.Rev. C28, 123 (1983)

R.M.Ronningen, G.M.Crawley, N.Anantaraman, S.M.Banks, B.M.Spicer, G.G.Shute, V.C.Officer, J.M.R.Wastell, D.W.Devins, D.L.Friesel

Multipole Moments of 154Sm and 166Er by Inelastic Scattering of 134 MeV Protons

NUCLEAR REACTIONS 154Sm, 166Er(polarized p, p'), E=134 MeV; measured σ(Ep'), σ(θ), A(θ); deduced deformed optical model parameters. 154Sm, 166Er deduced β2, β4, β6. Enriched targets, magnetic spectrograph. Coupled-channels calculations.

doi: 10.1103/PhysRevC.28.123


1983ZW02     Phys.Rev. C28, 542 (1983)

B.Zwieglinski, G.M.Crawley, J.A.Nolen, Jr., R.M.Ronningen

Coupled Channel Effects in 26Mg(p, p') at 40 MeV

NUCLEAR REACTIONS 26Mg(p, p'), E=40 MeV; measured σ(Ep), σ(θ); deduced optical model parameters. 26Mg levels deduced interference effects, multipole matrix elements, inelastic transition rates. Coupled-channels method, shell model wave functions. Enriched target.

doi: 10.1103/PhysRevC.28.542
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1286.


1982CR01     Phys.Lett. 109B, 8 (1982)

G.M.Crawley, W.Benenson, G.Bertsch, S.Gales, D.Weber, B.Zwieglinski

Pairing Model Predictions for (p, t) Experiments on the Cadmium Isotopes

NUCLEAR REACTIONS 110,112,114,116Cd(p, t), E=42 MeV; measured σ(Et). 106Cd(p, t), E=42 MeV; measured σ(Et), Q. 110,112,114,116,106Cd deduced two-particle pickup from deep orbits. 104Cd deduced mass excess. Split-pole spectrograph, position sensitive proportional counter. Pairing model.

doi: 10.1016/0370-2693(82)90450-6


1982CR02     Phys.Rev. C26, 87 (1982)

G.M.Crawley, N.Anantaraman, A.Galonsky, C.Djalali, N.Marty, M.Morlet, A.Willis, J.-C.Jourdain, P.Kitching

M1 Strength in Zirconium Isotopes by Proton Inelastic Scattering

NUCLEAR REACTIONS 90,92,94,96Zr(p, p'), E=200 MeV; measured σ(θ). 90,92,94,96Zr deduced levels, Γ, possible giant M1 resonance. Microscopic DWIA analysis.

doi: 10.1103/PhysRevC.26.87


1982DJ04     Nucl.Phys. A388, 1 (1982)

C.Djalali, N.Marty, M.Morlet, A.Willis, J.C.Jourdain, N.Anantaraman, G.M.Crawley, A.Galonsky, P.Kitching

Systematics of the Excitation of M1 Resonances in Medium Heavy Nuclei by 200 MeV Proton Inelastic Scattering

NUCLEAR REACTIONS 51V, 58,60,62Ni, 68Zn, 90,92,94,96Zr, 92,94,96,98,100Mo, 120,124Sn, 140Ce(p, p'), E=200 MeV; measured σ(θ). 51V, 58,60,62Ni, 68Zn, 90,92,94,96Zr, 92,94,96,98,100Mo, 120,124Sn, 140Ce deduced resonances, Γ, T, M1 character.

doi: 10.1016/0375-9474(82)90505-X
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0805.


1982FR05     Phys.Rev. C25, 1102 (1982)

K.A.Frankel, J.A.Bistirlich, R.Bossingham, H.R.Bowman, K.M.Crowe, C.J.Martoff, D.Murphy, J.O.Rasmussen, J.P.Sullivan, W.A.Zajc, J.P.Miller, O.Hashimoto, M.Koike, J.Peter, W.Benenson, G.M.Crawley, E.Kashy, J.A.Nolen, Jr., J.Quebert

Pions Produced near the Center-of-Mass Velocity in Heavy-Ion Collisions

NUCLEAR REACTIONS C, Ca, U(40Ar, π+), (40Ar, π-), E=1.05 GeV/nucleon; measured σ(E, θ).

doi: 10.1103/PhysRevC.25.1102


1982GA18     Nucl.Phys. A381, 173 (1982)

S.Gales, G.M.Crawley, D.Weber, B.Zwieglinski

Neutron-Hole Strength Distributions in Heavy Nuclei (I): The reactions 124,130Te(3He, α)123,129Te and 122,124,130Te(p, d)121,123,129Te

NUCLEAR REACTIONS 124,130Te(3He, α), E=70 MeV; measured σ(Eα, θ). 122,124,130Te(p, d), E=42 MeV; measured σ(θ). 121,123,129Te deduced levels, L, J, π, C2S. Enriched targets, magnetic spectrometer. DWBA, inner-shell analysis.

doi: 10.1016/0375-9474(82)90139-7


1982PE06     Nucl.Phys. A383, 355 (1982)

F.Petrovich, R.H.Howell, C.H.Poppe, S.M.Austin, G.M.Crawley

Nucleon Scattering from Light Nuclei (I). The Targets 6Li and 7Li

NUCLEAR REACTIONS 6,7Li(p, p), (p, p'), E=24.4 MeV; measured σ(Ep'), σ(θ); 6,7Li(p, p), (p, p'), (p, n), E=24-50 MeV; analyzed data. Distorted wave approximation, microscopic folding model.

doi: 10.1016/0375-9474(82)90083-5


1982SU01     Phys.Rev. C25, 1499 (1982)

J.P.Sullivan, J.A.Bistirlich, H.R.Bowman, R.Bossingham, T.Buttke, K.M.Crowe, K.A.Frankel, C.J.Martoff, J.Miller, D.L.Murphy, J.O.Rasmussen, W.A.Zajc, O.Hashimoto, M.Koike, J.Peter, W.Benenson, G.M.Crawley, E.Kashy, J.A.Nolen, Jr.

Strong Coulomb Effects on Pions Produced in Heavy Ion Collisions

NUCLEAR REACTIONS C, Na, F, Cu, U(20Ne, π+), (20Ne, π-), E=280-480 MeV/nucleon; C, K, Cl(40Ar, π+), (40Ar, π-), E=535 MeV/nucleon; measured σ(Eπ, θπ); deduced Coulomb effects, projectile fragment charges.

doi: 10.1103/PhysRevC.25.1499


1982WE11     Phys.Lett. 116B, 118 (1982)

G.D.Westfall, B.V.Jacak, N.Anantaraman, M.W.Curtin, G.M.Crawley, C.K.Gelbke, B.Hasselquist, W.G.Lynch, D.K.Scott, B.M.Tsang, M.J.Murphy, T.J.M.Symons, R.Legrain, T.J.Majors

Energy Dependence of Nuclear Matter Disassembly in Heavy Ion Collisions

NUCLEAR REACTIONS 197Au(20Ne, pX), (20Ne, dX), (20Ne, tX), (20Ne, αX), E=100, 156 MeV/nucleon; measured σ(Ep, θp), σ(Ed, θd), σ(Et, θt), σ(Eα, θα); deduced light particle production σ, ratios, temperature, source velocity.

doi: 10.1016/0370-2693(82)90988-1


1982ZW02     Nucl.Phys. A389, 301 (1982)

B.Zwieglinski, W.Benenson, G.M.Crawley, S.Gales, D.Weber

Study of 11B at High Excitations with the 9Be(3He, p)11B and 9Be(α, d)11B Reactions

NUCLEAR REACTIONS 9Be(3He, p), E=38 MeV; 9Be(α, d), E=48 MeV; measured σ(E(p), θ), σ(E(d)). 11B deduced levels, widths, isospin purity, L, normalization factors. DWBA analysis, shell-model form factors. Natural targets.

doi: 10.1016/0375-9474(82)90521-8


1981AN08     Phys.Rev.Lett. 46, 1318 (1981)

N.Anantaraman, G.M.Crawley, A.Galonsky, C.Djalali, N.Marty, M.Morlet, A.Willis, J.-C.Jourdain

Observation of M1 Strength by the Inelastic Scattering of 200-MeV Protons

NUCLEAR REACTIONS Ca, 90,92,94Zr(p, p'), E=201 MeV; measured σ(θ, Ep'). 90,92,94Zr deduced giant M1 resonance, Γ.

doi: 10.1103/PhysRevLett.46.1318


1981CR01     Phys.Rev. C23, 589 (1981)

G.M.Crawley, W.Benenson, G.Bertsch, S.Gales, D.Weber, B.Zwieglinski

Hole States in the Tin Isotopes Observed by the (p, t) Reaction

NUCLEAR REACTIONS 112,116,118,120,122,124Sn(p, t), E=42 MeV; measured σ(Et, θ); 117,119Sn(p, d), E=42 MeV; measured σ(Ed). 110,114,116,118,120,122Sn deduced broad resonances, Γ. DWBA analysis. Enriched targets.

doi: 10.1103/PhysRevC.23.589
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1349.


1981CR02     Phys.Rev. C23, 1818 (1981)

G.M.Crawley, J.Kasagi, S.Gales, E.Gerlic, D.Friesel, A.Bacher

Spin of Deep Hole States from (p(pol), d) Reactions

NUCLEAR REACTIONS 90Zr, 120Sn(polarized p, d), E=90 MeV; measured σ(θ), analyzing power vs θ; deduced optical model parameters. 89Zr, 119Sn levels deduced J, π, C2S.

doi: 10.1103/PhysRevC.23.1818
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0385.


1981FI07     Phys.Lett. 107B, 182 (1981)

J.E.Finck, G.M.Crawley, J.A.Nolen, Jr., R.Kouzes

Systematics of Collective States in Lead Nuclei from Inelastic Proton Scattering

NUCLEAR REACTIONS 206Pb(p, p'), E=35 MeV; measured σ(θ). 206Pb deduced levels, transition strengths. Collective DWBA analysis.

doi: 10.1016/0370-2693(81)90808-X
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0672.


1981IW02     Phys.Rev. C23, 1960 (1981)

Y.Iwasaki, G.M.Crawley, J.E.Finck

Core Excitations in 63Cu by the 63Cu(p, p')63Cu and 65Cu(p, t)63Cu Reactions

NUCLEAR REACTIONS 65Cu(p, t), 63Cu(p, p'), E=40 MeV; measured σ(θ), momentum spectra. 63Cu levels deduced L, J, π, configuration. DWBA analysis, core-particle coupling interpretation.

doi: 10.1103/PhysRevC.23.1960


1981MO02     Nucl.Phys. A352, 221 (1981)

R.A.Moyer, R.W.Finlay, G.M.Crawley

Energy Dependence in Proton Inelastic Scattering

NUCLEAR REACTIONS 92Mo(p, p), (p, p'), E=24.89, 29.84, 34.9, 45.3 MeV; measured σ(θ); deduced optical-model parameters. 92Mo levels deduced deformation lengths. Magnetic spectrometer, enriched target.

doi: 10.1016/0375-9474(81)90377-8
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0622.


1981RO09     Phys.Rev.Lett. 47, 635 (1981)

R.M.Ronningen, R.C.Melin, J.A.Nolen, Jr., G.M.Crawley, C.E.Bemis, Jr.

Higher-Order Deformations of 232Th and 234,236,238U

NUCLEAR REACTIONS 232Th, 234,236,238U(p, p), (p, p'), E=35 MeV; measured σ(θ). 232Th, 234,236,238U deduced deformation parameters β2, β4, β6, multipole moments. Coupled-channels calculations, deformed spin-orbit interaction.

doi: 10.1103/PhysRevLett.47.635
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0153.


1980CR02     Phys.Rev. C22, 316 (1980)

G.M.Crawley, S.Gales, D.Weber, B.Zwieglinski, W.Benenson, D.Friesel, A.Bacher, B.M.Spicer

Deep Hole States Observed in (p, t) Reactions

NUCLEAR REACTIONS 120,122,124Sn(p, t), E=89 MeV; measured σ(Et, θ). 118,120,122Sn deduced levels, Γ. DWBA, enriched targets.

doi: 10.1103/PhysRevC.22.316


1979BE31     Phys.Rev.Lett. 43, 683 (1979)

W.Benenson, G.Bertsch, G.M.Crawley, E.Kashy, J.A.Nolen, Jr., H.Bowman, J.G.Ingersoll, J.O.Rasmussen, J.Sullivan, M.Koike, M.Sasao, J.Peter, T.E.Ward

Low-Energy Pion Production at 0° with Heavy Ions from 125 to 400 MeV/Nucleon

NUCLEAR REACTIONS Na, F, Cu, U(20Ne, π+), (20Ne, π-), E=125-400 MeV/nucleon; measured σ(0°), σ(π+)/σ(π-); discussed reaction mechanisms.

doi: 10.1103/PhysRevLett.43.683


1979IW03     Phys.Rev. C20, 861 (1979)

Y.Iwasaki, G.M.Crawley, R.G.Markham, J.E.Finck, J.H.Kim

Octupole States in 63Cu and the Weak-Coupling Picture

NUCLEAR REACTIONS 63Cu(p, p'), E=400 MeV; measured σ(Ep', θ). 63Cu deduced levels, octupole transitions. Weak coupling model.

doi: 10.1103/PhysRevC.20.861


1979KI14     Phys.Rev. C20, 2084 (1979)

C.H.King, J.E.Finck, G.M.Crawley, J.A.Nolen, Jr., R.M.Ronningen

Multipole Moments of 154Sm, 176Yb, 232Th, and 238U from Proton Inelastic Scattering

NUCLEAR REACTIONS 154Sm, 176Yb, 232Th, 238U(p, p'), E=35 MeV; measured σ(Ep', θ); deduced optical model, β2, β4 parameters. Enriched targets, emulsion plates, proportional counter. Coupled channels calculations, rotation model.

doi: 10.1103/PhysRevC.20.2084
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0001.


1979WE02     Nucl.Phys. A313, 385 (1979)

D.J.Weber, G.M.Crawley, W.Benenson, E.Kashy, H.Nann

Study of 60Zn and 61Zn

NUCLEAR REACTIONS 58Ni(12C, 10Be), 58Ni(12C, 9Be), E=77 MeV; measured σ(E(10Be), θ), σ(E(9Be), θ). 60Zn, 61Zn deduced levels. 64Zn(3He, 6He), E=70 MeV; measured σ; deduced Q. 61Zn deduced mass excess, levels. Enriched targets. Atomic mass 61Zn.

doi: 10.1016/0375-9474(79)90508-6
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC2082.


1979ZW02     Phys.Rev. C20, 2449 (1979)

B.Zwieglinski, G.M.Crawley, J.A.Nolen, Jr.

The Two-Step Pickup-Stripping Process in the 24Mg(p, p')24Mg Reaction at 40 MeV to Some Negative Parity States in 24Mg

NUCLEAR REACTIONS 24Mg(p, p'), E=40 MeV; measured σ(θ); deduced reaction mechanism. Two-step coupled-channels calculation.

doi: 10.1103/PhysRevC.20.2449


1978FR11     Z.Phys. A286, 307 (1978)

A.D.Frawley, G.M.Crawley, C.L.Hollas

Fluctuations in Inelastic Proton Scattering from 58Ni in the Energy Range 17.1 to 20.6 MeV

NUCLEAR REACTIONS 58Ni(p, p), (p, p'), E=17.1-20.6 MeV; measured σ(E, θ). 59Cu levels deduced Γ. Enriched target.


1978GA09     Phys.Rev.Lett. 41, 292 (1978)

S.Gales, G.M.Crawley, D.Weber, B.Zwieglinski

Observation of the T > = 45/2 Components of Deep Hole States in 207Pb via the (3He, α) Reaction at 70 MeV

NUCLEAR REACTIONS 208Pb(3He, α), E=70 MeV; measured σ(Eα, θ). 207Pb deduced levels, S.

doi: 10.1103/PhysRevLett.41.292


1978GA23     Phys.Rev. C18, 2475 (1978)

S.Gales, G.M.Crawley, D.Weber, B.Zwieglinski

Inner Hole States in 207Pb via the 208Pb(3He, α)207Pb Reaction at 70 MeV

NUCLEAR REACTIONS 208Pb(3He, α), E=70 MeV; measured σ(E, θ). 207Pb deduced levels, L, J, π, C2S, inner shell S. Enriched target, magnetic spectrometer.

doi: 10.1103/PhysRevC.18.2475


1978RO08     Phys.Rev. C17, 1535 (1978)

R.G.H.Robertson, T.L.Khoo, G.M.Crawley, A.B.McDonald, E.G.Adelberger, S.J.Freedman

Mass of Lowest T = 2 State of 12C

NUCLEAR REACTIONS 14C(p, t), E ≈ 45 MeV; measured σ; deduced Q. 12C deduced level, T, Γ. 12C(p, t), E=45 MeV; measured σ; deduced Q. 10C deduced level.

doi: 10.1103/PhysRevC.17.1535


1978SM06     Phys.Rev. C18, 2486 (1978)

P.A.Smith, G.M.Crawley, G.G.Markham, D.Weber

208Pb(p, α)205Tl Reaction

NUCLEAR REACTIONS 208Pb(p, α), E=35 MeV; measured σ(θ). 205Tl deduced levels, J, π. Enriched target. Cluster model DWBA analysis. Compared with weak coupling model.

doi: 10.1103/PhysRevC.18.2486
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0666.


1978ZW01     Phys.Rev. C17, 872 (1978)

B.Zwieglinski, G.M.Crawley, H.Nann, J.A.Nolen, Jr.

Inelastic Scattering of 40 MeV Protons from 24Mg. I. Natural Parity Transitions

NUCLEAR REACTIONS 24Mg(p, p'), E=40 MeV; measured σ(Ep', θ); deduced optical model parameters. 24Mg levels deduced β, L, J, π.

doi: 10.1103/PhysRevC.17.872


1978ZW02     Phys.Rev. C18, 1228 (1978)

B.Zwieglinski, G.M.Crawley, W.Chung, H.Nann, J.A.Nolen, Jr.

Inelastic Scattering of 40 MeV Protons from 24Mg. II. Microscopic Calculations for Positive Parity States

NUCLEAR REACTIONS 24Mg(p, p'), E=40 MeV; calculated σ(θ) to positive parity states; deduced collective enhancement factors. Microscopic DWBA.

doi: 10.1103/PhysRevC.18.1228


1977CR04     Phys.Rev.Lett. 39, 1451 (1977)

G.M.Crawley, W.Benenson, D.Weber, B.Zwieglinski

Observation of Hole States at High Excitation in (p, t) Reactions

NUCLEAR REACTIONS 106Cd, 104Pd, 116,118,120,122,124Sn(p, t), E=42 MeV; measured σ(Et, θ). 114,116,118,120,122Sn deduced enhancements, widths.

doi: 10.1103/PhysRevLett.39.1451
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1349.


1976BA67     Aust.J.Phys. 29, 245 (1976)

F.C.Barker, G.M.Crawley, P.S.Miller, W.F.Steele

The Ghost Anomaly in the 9Be(p, d)8Be Reaction

NUCLEAR REACTIONS 9Be(p, d), E=39.91 MeV; measured σ(θ); deduced anomaly.


1976CR03     Phys.Lett. 64B, 143 (1976)

G.M.Crawley, W.F.Steele, J.N.Bishop, P.A.Smith, S.Maripuu

A Determination of the Mass and Some Energy Levels of the Nuclide 44Ar

NUCLEAR REACTIONS 48Ca(3He, 7Be), E=70 MeV; measured σ(E(7Be), θ). 44Ar deduced levels, mass excess.

doi: 10.1016/0370-2693(76)90315-4


1976HI10     Phys.Rev.Lett. 37, 130 (1976)

G.T.Hickey, D.C.Weisser, J.Cerny, G.M.Crawley, A.F.Zeller, T.R.Ophel, D.F.Hebbard

Use of the Four-Neutron Transfer Reaction 18O(18O, 14O)22O to Determine The Mass of 22O

NUCLEAR REACTIONS 18O(18O, 14O), E=100 MeV; measured σ; deduced Q. 22O deduced mass excess.

doi: 10.1103/PhysRevLett.37.130


1976HI14     J.Phys.(London) G2, L143 (1976)

G.T.Hickey, G.M.Crawley, D.C.Weisser, N.Shikazono

Mass Measurement of 62Fe Using the 64Ni(18O, 20Ne)62Fe Reaction

NUCLEAR REACTIONS 64Ni(18O, 20Ne), E=96 MeV; measured σ(20Ne, θ); deduced Q. 62Fe deduced level, mass excess.

doi: 10.1088/0305-4616/2/9/004


1976MO07     Phys.Lett. 61B, 167 (1976)

A.Moalem, W.Benenson, G.M.Crawley, T.L.Khoo

Decay Modes of the Giant Resonance Region in 40Ca

NUCLEAR REACTIONS 40Ca(3He, 3He'), E=70 MeV; measured p3He'(θ), 3He'α(θ). 40Ca resonance deduced Γp/Γα.

doi: 10.1016/0370-2693(76)90617-1


1976ST11     Nucl.Phys. A266, 424 (1976)

W.F.Steele, P.A.Smith, J.E.Finck, G.M.Crawley

A Survey of the (3He, 7Be) Reaction at 70 MeV

NUCLEAR REACTIONS 12,13C, 16O, 24,26Mg, 40,42,44Ca, 58,60,62,64Ni, 90Zr, 120,124Sn, 144Sm, 206Pb(3He, 7Be), E=70 MeV; measured σ(θ); deduced S α. 60Fe, 120Cd deduced mass excess. 8,9Be, 12C, 20,22Ne, 36,38,40Ar, 54,56,58,60Fe, 86Sr, 116,120Cd deduced levels.

doi: 10.1016/0375-9474(76)90368-7


1975GA18     Phys.Rev. C12, 1072 (1975)

A.Galonsky, G.M.Crawley, P.S.Miller, R.R.Doering, D.M.Patterson

Discrepancies between Formation and Decay of Isobaric Analog States of Pb and Bi

NUCLEAR REACTIONS 208Pb(p, n), (p, np), E=21-35 MeV; measured σ; deduced σ discrepancy.

doi: 10.1103/PhysRevC.12.1072


1975WA03     Phys.Rev. C11, 486 (1975)

W.T.Wagner, G.M.Crawley, G.R.Hammerstein

High Resolution (p, p') on 207Pb and 209Bi

NUCLEAR REACTIONS 207Pb, 209Bi(p, p'), E=35 MeV; measured σ(Ep', θ). 207Pb, 209Bi deduced levels, L, β, J, π.

doi: 10.1103/PhysRevC.11.486


1975WA18     Phys.Rev. C12, 757 (1975)

W.T.Wagner, G.M.Crawley, G.R.Hammerstein, H.McManus

High-Resolution Study of 208Pb with 35-MeV Protons

NUCLEAR REACTIONS 208Pb(p, p), E=35 MeV; measured σ(θ). 208Pb deduced levels, L, β(L).

doi: 10.1103/PhysRevC.12.757
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0225.


1974HA02     Phys.Rev. C9, 252 (1974)

J.C.Hardy, H.Schmeing, W.Benenson, G.M.Crawley, E.Kashy, H.Nann

Fermi Beta Decay: The Masses of 22Mg, 26Si, 30S, and 34Ar

NUCLEAR REACTIONS 24Mg, 28Si, 32S, 36Ar(p, t), E=40.2 MeV; measured Q values. 22Mg, 26Si, 30S, 34Ar deduced masses, ft values, mirror asymmetries for A=26, 34.

doi: 10.1103/PhysRevC.9.252


1974LA01     Phys.Rev. C9, 646 (1974); Erratum Phys.Rev. C10, 427 (1974)

W.A.Lanford, G.M.Crawley

207Pb(p, d)206Pb Reaction and Some Matrix Elements of the Effective Interaction

NUCLEAR REACTIONS 207Pb(p, d), E=35 MeV; measured σ(Ed, θ). 206Pb deduced levels, S, sum rules.

doi: 10.1103/PhysRevC.9.646


1974MO26     Nucl.Phys. A236, 307 (1974)

A.Moalem, W.Benenson, G.M.Crawley

A Study of the Nuclear Continuum in 16O by Inelastic 3He Scattering

NUCLEAR REACTIONS 16O(3He, 3He'), E=71 MeV; measured σ(E(3He'), θ). 16O resonances deduced E2 strength.

doi: 10.1016/0375-9474(74)90256-5


1973CR02     Phys.Rev. C8, 574 (1973)

G.M.Crawley, P.S.Miller, G.J.Igo, J.Kulleck

High-Resolution Study of 48Ca(p, t)46Ca at E = 39 MeV

NUCLEAR REACTIONS 48Ca(p, t), E=39 MeV; measured σ(Et, θ). 46Ca deduced levels, J, π.

doi: 10.1103/PhysRevC.8.574


1973CR05     Phys.Rev. C8, 2477 (1973)

G.M.Crawley, E.Kashy, W.Lanford, H.G.Blosser

High-Resolution Study of the Particle-Hole Multiplets in 208Bi

NUCLEAR REACTIONS 209Bi(p, d), E=35 MeV; measured σ(Ed, θ). 208Bi deduced levels, J, π, S.

doi: 10.1103/PhysRevC.8.2477


1973MO10     Phys.Rev.Lett. 31, 482 (1973)

A.Moalem, W.Benenson, G.M.Crawley

Excitation of Giant Resonances by Inelastic 3He Scattering

NUCLEAR REACTIONS 27Al, 40Ca, 58Ni, 90Zr, 122Sn, 197Au, 208Pb, 209Bi(3He, 3He'), E=71 MeV; measured σ(E;θ).

doi: 10.1103/PhysRevLett.31.482


1973WA29     Phys.Rev. C8, 2504 (1973)

W.T.Wagner, G.R.Hammerstein, G.M.Crawley, J.R.Borysowicz, F.Petrovich

35-MeV Proton Inelastic Scattering from Low-Lying States in 207Pb

NUCLEAR REACTIONS 207Pb(p, p'), E=35 MeV; measured σ(θ).

doi: 10.1103/PhysRevC.8.2504


1972CR04     Phys.Rev. C6, 306 (1972)

G.M.Crawley, P.S.Miller

Proton Decay of the Isobaric Analogs of the Ground States of 206Pb, 207Pb, 208Pb, and 209Bi

NUCLEAR REACTIONS 206,207,208Pb(p, np), E=21.3-35 MeV; measured σ(E;Ep, θ). 206,207Bi, 208Bi, 209Po deduced isobaric analog states, level-width, Coulomb energy differences.

doi: 10.1103/PhysRevC.6.306


1972CR07     Phys.Rev. C6, 1890 (1972)

G.M.Crawley, P.S.Miller, A.Galonsky, T.Amos, R.Doering

Widths of Analog States in Bi and Po from (p, n) Spectra

NUCLEAR REACTIONS 206,207,208Pb, 209Bi(p, n), E=25 MeV; measured σ(En). 209Po-209Bi, 208Bi-208Pb, 207Bi- 207Pb, 206Bi- 206Pb deduced Coulomb energy differences, isobaric analog states, level-width.

doi: 10.1103/PhysRevC.6.1890


1970CR03     Phys.Lett. 32B, 92 (1970)

G.M.Crawley, S.M.Austin, W.Benenson, V.A.Madsen, F.A.Schmittroth, M.J.Stomp

Evidence for a Tensor Effective Two-Body Interaction in the 14N(p, p') 2.31 MeV Excitation

NUCLEAR REACTIONS 14N(p, p'), E=24.8 MeV; measured σ(Ep', θ).

doi: 10.1016/0370-2693(70)90594-0
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0476.


1970CR05     Phys.Rev. C2, 1071 (1970)

G.M.Crawley, W.Benenson, P.S.Miller, D.L.Bayer, R.St.Onge, A.Kromminga

Properties of the 209Bi Ground-State Analog in 209Po

NUCLEAR REACTIONS 209Bi(p, n), (p, d), (p, np), E=24-30 MeV; measured σ(E;θ), σ(E;Ed, θ), σ(E;En, θ). 209Po deduced level, level-width, isobaric analog. 209Po-209Bi deduced Coulomb energy difference.

doi: 10.1103/PhysRevC.2.1071


1970HI06     Phys.Rev.Lett. 25, 829 (1970)

R.A.Hinrichs, R.Sherr, G.M.Crawley, I.Proctor

Anomalous L = 1 Shapes of Angular Distribution for (3He, t) Transitions to 0+ Antianalog States in 64,66Ga and 40K

NUCLEAR REACTIONS 40Ar, 64,66Zn(3He, t), E=35 MeV; measured σ(θ). 40K, 64,66Ga deduced transitions, antianalog states.

doi: 10.1103/PhysRevLett.25.829


1970PO03     Nucl.Phys. A147, 65 (1970)

D.L.Powell, G.M.Crawley, B.V.N.Rao, B.A.Robson

Deuteron-Induced Reactions in 6Li, 9Be and 10B at Bombarding Energies of 4.5 to 6.0 MeV

NUCLEAR REACTIONS 6Li(d, d), (d, p), E=4.5-5.5 MeV; measured σ(E, θ), σ(E, Ep, θ). 9Be(d, d), (d, p), E=4.5-6.0 MeV; measured σ(E, θ), σ(E, Ep, θ). 10B(d, p), E=4.5-5.5 MeV; measured σ(E, Ep, θ). Enriched targets.

doi: 10.1016/0375-9474(70)90510-5
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1432.


1968AU05     Phys.Letters 27B, 570 (1968)

S.M.Austin, G.M.Crawley

The Spin-Isospin Dependent Interaction from Inelastic Proton Scattering on 6Li

NUCLEAR STRUCTURE 6Li; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(68)90035-X


1968AU06     Phys.Rev. 176, 1227(1968)

S.M.Austin, P.J.Locard, W.Benenson, G.M.Crawley

6Li(p, p')6Li(3.56 Mev) Reaction from E = 24.3 to 46.4 MeV and the Effective Interaction

NUCLEAR REACTIONS 6Li(p, p'γ), E=24.3-46.4 MeV; measured Eγ, σ; deduced optical model parameters. Ge(Li) detector.

doi: 10.1103/PhysRev.176.1227


1968CR03     Phys.Rev. 167, 1070 (1968)

G.M.Crawley, G.T.Garvey

Inelastic Scattering in the 2s-1d Shell. II. Odd-A Nuclei

NUCLEAR STRUCTURE 31P, 23Na, 19F, 27Al, 25Mg; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.167.1070
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0615.


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