NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = G.Crawley Found 114 matches. Showing 1 to 100. [Next]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
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
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
1999AN13 Nucl.Phys. A648, 3 (1999) T.Annakkage, J.Janecke, J.S.Winfield, G.P.A.Berg, J.A.Brown, G.Crawley, S.Danczyk, M.Fujiwara, D.J.Mercer, K.Pham, D.A.Roberts, J.Stasko, G.H.Yoo Isovector Giant Resonances in 6He, 12B, 90Y, 120In, and 208Tl Observed in the (7Li, 7Be) Charge-Exchange Reaction NUCLEAR REACTIONS H, C, 6Li, 12C, 90Zr, 120Sn, 208Pb(7Li, 7Be), E=350 MeV; measured particle spectra, angular distributions, Eγ, Iγ(θ). 6He, 12B, 90Y, 120In, 208Tl deduced resonance features, spinflip ratios, spinflip enhancement, effective number of participating protons. Microscopic one-step distorted-wave analysis with shell-model transition amplitudes.
doi: 10.1016/S0375-9474(99)00015-9
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
1996JA08 Nucl.Phys. A599, 191c (1996) J.Janecke, T.Annakkage, K.Pham, D.A.Roberts, J.A.Brown, G.Crawley, S.Danczik, D.J.Mercer, J.Stasko, J.S.Winfield, G.H.Yoo, G.P.A.Berg, M.Fujiwara Isovector Giant Resonances in 6He, 12B, 90Y, 120In, and 208Tl NUCLEAR REACTIONS 6Li, 12C, 90Zr, 120Sn, 208Pb(7Li, 7Be), E=350 MeV; measured σ(θ), 7Be spectra, γ(7Be)-coin. 6He, 12B, 90Y, 120In, 208Tl deduced isovector giant resonances, J, π, width.
doi: 10.1016/0375-9474(96)00061-9
1996JA11 Phys.Rev. C54, 1070 (1996) J.Janecke, T.Annakkage, G.P.A.Berg, B.A.Brown, J.A.Brown, G.Crawley, S.Danczyk, M.Fujiwara, D.J.Mercer, K.Pham, D.A.Roberts, J.Stasko, J.S.Winfield, G.H.Yoo Structure of the Neutron-Halo Nucleus 6He NUCLEAR REACTIONS 6Li(7Li, 7Be), E=350 MeV; measured σ(θ). 6He deduced resonances, J, π. Microscopic finite-range DWBA.
doi: 10.1103/PhysRevC.54.1070
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
1990ET01 Nucl.Phys. A518, 572 (1990) M.C.Etchegoyen, A.Etchegoyen, A.O.Macchiavelli, G.Crawley, C.Djalali, M.Renteria, A.Szanto de Toledo, G.Westfall 18O + 58Ni Reaction at 35 MeV/Nucleon NUCLEAR REACTIONS, ICPND 58Ni(18O, X), E=630 MeV; measured fragment σ(θ), σ(Z, A) vs fragment momentum, integrated σ, fragments momentum width; deduced distribution reduced width.
doi: 10.1016/0375-9474(90)90147-E
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
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
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
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.
doi: 10.1071/PH850027
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.
doi: 10.1016/0168-9002(85)90472-3
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
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
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
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
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
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
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
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
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
1981ST08 Phys.Rev. C23, 2447 (1981) G.L.Struble, L.G.Mann, R.G.Lanier, W.M.Buckley, J.Kern, G.Crawley, S.Gales, D.Mueller, F.Girshick Influence of Complex States and Deformation on Neutron Pairing Vibrations in the Even Sm Istopes NUCLEAR REACTIONS 144,148,150,152,154Sm(p, t), E=42 MeV; measured σ(Et, θt); deduced level systematics in Sm isotopes. 142Sm deduced levels, J. Enriched targets, Q3D, Enge split-pole spectrographs. DWBA.
doi: 10.1103/PhysRevC.23.2447
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
1980ST13 Phys.Lett. 93B, 26 (1980) G.L.Struble, L.G.Mann, R.G.Lanier, W.M.Buckley, J.Kern, G.Crawley, S.Gales, D.Mueller, F.Girshick The Behavior of High-Energy Neutron Pairing Strength in the Samarium Isotopes NUCLEAR REACTIONS 144,148,150,152,154Sm(p, t), E=42 MeV; measured σ(θ, Et). 142Sm deduced structure. 146,148Sm deduced two-neutron transfer strength localization. Shell model. Q3D spectrograph, Enge split-pole spectrometer.
doi: 10.1016/0370-2693(80)90087-8
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
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
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.
doi: 10.1007/BF01408262
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
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
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.
doi: 10.1071/PH760245
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
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) 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) 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
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