NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = A.Galonsky Found 134 matches. Showing 1 to 100. [Next]2013IZ01 Phys.Rev. C 88, 065808 (2013) R.Izsak, A.Horvath, A.Kiss, Z.Seres, A.Galonsky, C.A.Bertulani, Zs.Fulop, T.Baumann, D.Bazin, K.Ieki, C.Bordeanu, N.Carlin, M.Csanad, F.Deak, P.DeYoung, N.Frank, T.Fukuchi, A.Gade, D.Galaviz, C.R.Hoffman, W.A.Peters, H.Schelin, M.Thoennessen, G.I.Veres Determining the 7Li(n, γ) cross section via Coulomb dissociation of 8Li NUCLEAR REACTIONS C, Pb(8Li, n), [8Li secondary beam from 9Be(18O, X), E=120 MeV/nucleon primary reaction], E=69.5 MeV/nucleon; 8Li(γ, n)7Li, [γ from 8Li beam impinging on C and Pb targets], E(8Li)=69.5 MeV/nucleon; measured TOF, position and angle of 8Li particles, neutron spectra from Coulomb dissociation of 8Li, E(n), I(n) using MONA neutron detector array at NSCL-MSU cyclotron facility; reconstructed neutron 7Li energy spectra and momentum vectors; deduced σ(E) for 7Li(n, γ)8Li reaction. Surrogate method. Comparison of σ with previous experimental results, and with low-energy effective field theory calculations.
doi: 10.1103/PhysRevC.88.065808
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
2006HO14 Eur.Phys.J. A 27, Supplement 1, 217 (2006) A.Horvath, K.Ieki, A.Kiss, A.Galonsky, M.Thoennessen, T.Baumann, D.Bazin, C.A.Bertulani, C.Bordeanu, N.Carlin, M.Csanad, F.Deak, P.DeYoung, N.Frank, T.Fukuchi, Zs.Fulop, A.Gade, D.Galaviz, C.Hoffman, R.Izsak, W.A.Peters, H.Schelin, A.Schiller, R.Sugo, Z.Seres, G.I.Veres Can the neutron-capture cross sections be measured with Coulomb dissociation? NUCLEAR REACTIONS C, Pb(8Li, n7Li), E=41 MeV/nucleon; measured particle spectra, angular distributions; deduced nuclear and Coulomb contributions.
doi: 10.1140/epja/i2006-08-033-6
2006WA18 Phys.Rev. C 74, 014605 (2006) R.E.Warner, F.Carstoiu, J.A.Brown, F.D.Becchetti, D.A.Roberts, B.Davids, A.Galonsky, R.M.Ronningen, M.Steiner, M.Horoi, J.J.Kolata, A.Nadasen, C.Samanta, J.Schwarzenberg, K.Subotic Reaction and proton-removal cross sections of 6Li, 7Be, 10B, 9, 10, 11C, 12N, 13, 15O, and 17Ne on Si at 15 to 53 MeV/nucleon NUCLEAR REACTIONS Si(6Li, X), (7Be, X), (10B, X), (9C, X), (10C, X), (11C, X), (12N, X), (13O, X), (15O, X), (17Ne, X), E=15-53 MeV/nucleon; measured reaction and proton-removal σ. 6Li, 7Be, 10B, 9,10,11C, 12N, 13,15O, 17Ne deduced radii. Comparison with Glauber model predictions.
doi: 10.1103/PhysRevC.74.014605
2004AM07 Nucl.Sci.Eng. 147, 73 (2004) T.M.Amos, R.R.Doering, A.Galonsky, R.Jolly, M.K.Zigrang Production of Neutrons with Protons of 22, 30, and 40 MeV in Stopping Targets of Carbon, Aluminum, Copper, Silver, Tantalum, and Lead NUCLEAR REACTIONS C, Al, Cu, Ag, Ta, Pb(p, nX), E < 40 MeV; measured neutron spectra, angular distributions; deduced yields.
doi: 10.13182/NSE04-A2420
2004WA06 Phys.Rev. C 69, 024612 (2004) R.E.Warner, F.D.Becchetti, J.A.Brown, A.Galonsky, J.H.Kelley, A.Nadasen, R.M.Ronningen, J.A.Tostevin, J.S.Winfield, P.Zecher Proton removal from 8B, 9C, and 12C on Si at 20-70 MeV/nucleon NUCLEAR REACTIONS Si(8B, 7BeX), (9C, 8BX), (9C, 7BeX), (12C, 11BX), E=20-70 MeV/nucleon; measured one- and two-proton removal σ; deduced quenching factors. Shell model calculations, eikonal reaction theory.
doi: 10.1103/PhysRevC.69.024612
2003HO22 Nucl.Phys. A719, 9c (2003) A.Horvath, A.Galonsky, N.Carlin, F.Deak, T.Gomi, V.Guimaraes, Y.Higurashi, K.Hiroshi, K.Ieki, Y.Iwata, A.Kiss, J.Kolata, T.Rauscher, H.Schelin, J.von Schwarzenberg, Z.Seres, S.Takeuchi, S.Typel, R.Warner, J.Weiner Measurements of astrophysical neutron capture cross sections via the inverse reaction NUCLEAR REACTIONS C, Al, Cu, Sn, Pb(15C, nX), E=35 MeV/nucleon; C, Al, Cu, Sn, Pb(9Li, nX), E=40 MeV/nucleon; measured neutron spectra, (fragment)(neutron)-coin, dissociation yields. 8Li, 14C(n, γ), E=low; deduced astrophysical reaction rates.
doi: 10.1016/S0375-9474(03)00951-5
2003KO07 Phys.Rev. C 67, 015806 (2003) H.Kobayashi, K.Ieki, A.Horvath, A.Galonsky, N.Carlin, F.Deak, T.Gomi, V.Guimaraes, Y.Higurashi, Y.Iwata, A.Kiss, J.J.Kolata, T.Rauscher, H.Schelin, Z.Seres, R.Warner Astrophysical reaction rate for the 8Li(n, γ)9Li reaction NUCLEAR REACTIONS Pb(9Li, n8Li), E=39.7 MeV/nucleon; measured neutron and lithium spectra. 8Li(n, γ), E not given; deduced σ, astrophysical reaction rate upper limits. Comparison with previous results.
doi: 10.1103/PhysRevC.67.015806
2002WA04 Phys.Rev. C65, 034306 (2002) J.Wang, A.Galonsky, J.J.Kruse, E.Tryggestad, R.H.White-Stevens, P.D.Zecher, Y.Iwata, K.Ieki, A.Horvath, F.Deak, A.Kiss, Z.Seres, J.J.Kolata, J.von Schwarzenberg, R.E.Warner, H.Schelin Dissociation of 6He NUCLEAR REACTIONS C, Al, Cu, Sn, Pb, U(6He, 2nα), (6He, αX), E=23.9 MeV/nucleon; measured Eα, En, nα-coin, parallel momentum distributions, angular correlations, two-neutron removal σ; deduced Coulomb contribution, other reaction mechanism features. 6He deduced halo neutron correlations. Comparisons with model predictions.
doi: 10.1103/PhysRevC.65.034306
2001AU02 Phys.Rev. C63, 034322 (2001) S.M.Austin, E.Adamides, A.Galonsky, T.Nees, W.A.Sterrenburg, D.E.Bainum, J.Rapaport, E.Sugarbaker, C.C.Foster, C.D.Goodman, D.J.Horen, C.A.Goulding, M.B.Greenfield Splitting of the Dipole and Spin-Dipole Resonances NUCLEAR REACTIONS 90,92,94Zr(p, n), E=79.2, 119.4 MeV; measured σ(E, θ); deduced splitting between GDR and spin-dipole resonance. NUCLEAR STRUCTURE 90,92,94Zr, 112,116,124Sn, 208Pb; calculated resonance energies, dipole-spin-dipole splitting.
doi: 10.1103/PhysRevC.63.034322
2001CH31 Phys.Lett. 505B, 21 (2001) L.Chen, B.Blank, B.A.Brown, M.Chartier, A.Galonsky, P.G.Hansen, M.Thoennessen Evidence for an l = 0 Ground State in 9He NUCLEAR REACTIONS 9Be(11Be, X)9He/10Li, 28 MeV/nucleon; measured (fragment)(neutron)-coin, relative velocities. 9He, 10Li deduced ground-state L.
doi: 10.1016/S0370-2693(01)00313-6
2001CH46 Phys.Lett. 510B, 24 (2001) M.Chartier, J.R.Beene, B.Blank, L.Chen, A.Galonsky, N.Gan, K.Govaert, P.G.Hansen, J.Kruse, V.Maddalena, M.Thoennessen, R.L.Varner Identification of the 10Li Ground State NUCLEAR REACTIONS 9Be(11Be, X)8Li/9Li/10Be, E=46 MeV/nucleon; measured Eγ, Iγ, (fragment)γ-coin. 10Li deduced ground-state configuration.
doi: 10.1016/S0370-2693(01)00602-5
2001WA40 Phys.Rev. C64, 044611 (2001) R.E.Warner, M.H.McKinnon, J.S.Needleman, N.C.Shaner, F.D.Becchetti, D.A.Roberts, A.Galonsky, R.M.Ronningen, M.Steiner, J.A.Brown, J.J.Kolata, A.Nadasen, K.Subotic Total Reaction and Neutron-Removal Cross Sections of (30-60)A MeV Be Isotopes on Si and Pb NUCLEAR REACTIONS Si(7Be, X), (9Be, X), (10Be, X), (11Be, X), (12Be, X), (14Be, X), Pb(10Be, X), (11Be, X), (12Be, X), E=30-60 MeV/nucleon; measured reaction σ, neutron-removal σ. 7,9,10,11,12,14Be deduced radii. Glauber model calculations.
doi: 10.1103/PhysRevC.64.044611
2000IW05 Phys.Rev. C62, 064311 (2000) Y.Iwata, K.Ieki, A.Galonsky, J.J.Kruse, J.Wang, R.H.White-Stevens, E.Tryggestad, P.D.Zecher, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, J.von Schwarzenberg, R.E.Warner, H.Schelin Dissociation of 8He NUCLEAR REACTIONS Al(8He, n6He), Sn, Pb(8He, 2n6He), E=24 MeV/nucleon; measured invariant mass spectra, relative momentum distributions; deduced sequential decay contribution, dipole strength function, sum rules. 8He deduced excited state J, π, Γ. Secondary beam from 16O fragmentation.
doi: 10.1103/PhysRevC.62.064311
2000WA23 Phys.Rev. C62, 024608 (2000) R.E.Warner, M.H.McKinnon, N.C.Shaner, F.D.Becchetti, A.Nadasen, D.A.Roberts, J.A.Brown, A.Galonsky, J.J.Kolata, R.M.Ronningen, M.Steiner, K.Subotic Total Reaction and Neutron-Removal Cross Sections of (30-60)A MeV He and Li Isotopes on Pb NUCLEAR REACTIONS Pb(α, X), (6He, X), (8He, X), (6Li, X), (7Li, X), (8Li, X), (9Li, X), (11Li, X), E=30-60 MeV/nucleon; measured total σ. Pb(11Li, 9Li), (6He, α), (8He, α), (8He, 6He), E=30-60 MeV/nucleon; measured neutron-removal σ; deduced role of electromagnetic dissociation. Microscopic model calculations. Secondary beams from 18O fragmentation.
doi: 10.1103/PhysRevC.62.024608
1999HE45 Nucl.Sci.Eng. 132, 1 (1999) L.Heilbronn, R.S.Cary, M.Cronqvist, F.Deak, K.Frankel, A.Galonsky, K.Holabird, A.Horvath, A.Kiss, J.Kruse, R.M.Ronningen, H.Schelin, Z.Seres, C.E.Stronach, J.Wang, P.Zecher, C.Zeitlin Neutron yields from 155 MeV/Nucleon Carbon and Helium Stopping in Aluminum NUCLEAR REACTIONS 27Al(α, X), (12C, X), E=155 MeV/nucleon; measured reaction products, En, In; deduced yields, number of neutrons per interaction.
doi: 10.13182/nse98-41
1999TH01 Phys.Rev. C59, 111 (1999) M.Thoennessen, S.Yokoyama, A.Azhari, T.Baumann, J.A.Brown, A.Galonsky, P.G.Hansen, J.H.Kelley, R.A.Kryger, E.Ramakrishnan, P.Thirolf Population of 10Li by Fragmentation NUCLEAR REACTIONS 9Be(18O, X)10Li, E=80 MeV/nucleon; measured n-9Li relative velocity spectra. 10Li deduced low-lying s-wave strength.
doi: 10.1103/PhysRevC.59.111
1998GA33 Phys.Rev. C58, 2161 (1998) S.J.Gaff, A.Galonsky, C.K.Gelbke, T.Glasmacher, M.Huang, J.J.Kruse, G.J.Kunde, R.Lemmon, W.G.Lynch, M.B.Tsang, J.Wang, P.D.Zecher, F.Deak, A.Horvath, A.Kiss, Z.Seres, K.Ieki, Y.Iwata Time Scales from Two-Neutron Intensity Interferometry for the Reaction 40Ar + 165Ho at E/A = 25 MeV NUCLEAR REACTIONS 165Ho(40Ar, X), E=25 MeV/nucleon; measured neutron spectra, coincidence neutron yields; deduced correlation function, source radius, lifetime. Two-neutron intensity interferometry.
doi: 10.1103/PhysRevC.58.2161
1998WA16 Nucl.Phys. A635, 292 (1998) R.E.Warner, H.Thirumurthy, J.Woodroffe, F.D.Becchetti, J.A.Brown, B.S.Davids, A.Galonsky, J.J.Kolata, J.J.Kruse, M.Y.Lee, A.Nadasen, T.W.O'Donnell, D.A.Roberts, R.M.Ronningen, C.Samanta, P.Schwandt, J.von Schwarzenberg, M.Steiner, K.Subotic, J.Wang, J.A.Zimmerman Reaction Cross Sections in Si of Light Proton-Halo Candidates 12N and 17Ne NUCLEAR REACTIONS Si(12N, X), (15O, X), (17Ne, X), E=29-53 MeV/nucleon; measured total reaction σ, charge-removal σ; deduced dependence on proton separation energy. Radioactive beams, Glauber model, proton-halo nuclei.
doi: 10.1016/S0375-9474(98)00163-8
1998ZE01 Phys.Rev. C57, 959 (1998) P.D.Zecher, A.Galonsky, S.J.Gaff, J.J.Kruse, G.Kunde, E.Tryggestad, J.Wang, R.E.Warner, D.J.Morrissey, K.Ieki, Y.Iwata, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, J.von Schwarzenberg, H.Schelin Measurement of the 8Li(n, γ)9Li Cross Section at Astrophysical Energies by Reverse Kinematics NUCLEAR REACTIONS U, Pb(9Li, n8Li), E=30 MeV/nucleon; measured σ. 8Li(n, γ), E=0.25, 0.75 MeV; deduced σ upper limit. Astrophysical implications discussed. Radioactive beam.
doi: 10.1103/PhysRevC.57.959
1997DE58 Acta Phys.Hung.N.S. 5, 13 (1997) F.Deak, A.Horvath, A.Kiss, Z.Seres, A.Galonsky, H.Hama, L.Heilbronn, D.W.Sackett, H.R.Schelin Production Rates of Excited Fragment Isotopes from the 36Ar + Ag Reaction at 35 MeV/nucleon NUCLEAR REACTIONS Ag(36Ar, X), E=35 MeV/nucleon; measured Z=3-5 excited fragments σ(θ) vs kinetic energy; deduced total production of neutron unbound states. Thermal model.
1996GA08 Nucl.Phys. A599, 353c (1996) A.Galonsky, J.J.Kruse, W.G.Lynch, D.J.Morrissey, N.Orr, J.Ottarson, D.Sackett, B.M.Sherrill, J.Wang, J.Winger, P.Zecher, K.Ieki, Y.Iwata, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, R.E.Warner, H.Schelin, D.L.Humphrey Soft Dipole Resonance in Exotic Nuclei ( Question ) NUCLEAR REACTIONS Pb(11Li, X), E=30 MeV/nucleon; measured projectile three-body breakup energy spectrum, three-particle momenta; deduced no soft dipole resonance. 11Li deduced no dineutron. Virtual photon induced photodisintegration of 11Li.
doi: 10.1016/0375-9474(96)00078-4
1996IE01 Phys.Rev. C54, 1589 (1996) K.Ieki, A.Galonsky, D.Sackett, J.J.Kruse, W.G.Lynch, D.J.Morrissey, N.A.Orr, B.M.Sherrill, J.A.Winger, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, R.E.Warner, D.L.Humphrey Is There a Bound Dineutron in 11Li ( Question ) NUCLEAR REACTIONS 208Pb(11Li, 2n9Li), E=28 MeV/nucleon; measured 9Li(2n)-coin; deduced angular correlation between two neutrons in the rest frame of 11Li. 11Li level deduced no bound dineutron evidence.
doi: 10.1103/PhysRevC.54.1589
1996WA27 Phys.Rev. C54, 1700 (1996) R.E.Warner, R.A.Patty, P.M.Voyles, A.Nadasen, F.D.Becchetti, J.A.Brown, H.Esbensen, A.Galonsky, J.J.Kolata, J.Kruse, M.Y.Lee, R.M.Ronningen, P.Schwandt, J.von Schwarzenberg, B.M.Sherrill, K.Subotic, J.Wang, P.Zecher Total Reaction and 2n-Removal Cross Sections of 20-60A MeV 4,6,8He, 6-9,11Li, and 10Be on Si NUCLEAR REACTIONS, ICPND Si(6Li, X), (7Li, X), (8Li, X), (9Li, X), (11Li, X), (10Be, X), (α, X), (6He, X), (8He, X), E=20-60 MeV/nucleon; measured reaction σ, 2n-removal σ for some projectiles. 4,6,8He, 6,7,8,9,11Li, 10Be deduced matter distributions. Microscopic, strong absorption optical models.
doi: 10.1103/PhysRevC.54.1700
1995DE24 Phys.Rev. C52, 219 (1995) F.Deak, A.Horvath, A.Kiss, Z.Seres, A.Galonsky, C.K.Gelbke, H.Hama, L.Heilbronn, D.Krofcheck, W.G.Lynch, D.W.Sackett, H.R.Schelin, M.B.Tsang, J.Kasagi, T.Murakami Internal Excitation of Intermediate Mass Fragments from Collisions of 36Ar + Ag Nuclei at 35 MeV/nucleon NUCLEAR REACTIONS Ag(36Ar, X), E=35 MeV/nucleon; measured intermediate mass fragments (Li-Mg) population ratios.
doi: 10.1103/PhysRevC.52.219
1995WA01 Phys.Rev. C51, 178 (1995) R.E.Warner, F.D.Becchetti, J.W.Janecke, D.A.Roberts, D.Butts, C.L.Carpenter, J.M.Fetter, A.Muthukrishnan, J.J.Kolata, K.Lamkin, M.Belbot, M.Zahar, A.Galonsky, K.Ieki, P.Zecher Elastic Scattering of 10 MeV 6He from 12C, (nat)Ni, and 197Au NUCLEAR REACTIONS 12C, Ni, 197Au(6He, 6He), E=10 MeV; measured σ(θ). Optical model analysis.
doi: 10.1103/PhysRevC.51.178
1995WA19 Phys.Rev. C52, R1166 (1995) R.E.Warner, J.H.Kelley, P.Zecher, F.D.Becchetti, J.A.Brown, C.L.Carpenter, A.Galonsky, J.Kruse, A.Muthukrishnan, A.Nadasen, R.M.Ronningen, P.Schwandt, B.M.Sherrill, J.Wang, J.S.Winfield Evidence for a Proton Halo in 8B: Enhanced total reaction cross sections at 20 to 60 MeV/nucleon NUCLEAR REACTIONS, ICPND Si(8B, X), (12C, X), (14N, X), E=20-60 MeV/nucleon; measured total reaction σ. 8B deduced proton halo. Si is both target and detector.
doi: 10.1103/PhysRevC.52.R1166
1994HO02 Phys.Rev. C49, 1012 (1994) A.Horvath, F.Deak, A.Kiss, Z.Seres, A.Galonsky, C.K.Gelbke, H.Hama, L.Heilbronn, D.Krofcheck, W.G.Lynch, D.W.Sackett, H.R.Schelin, M.B.Tsang, J.Kasagi, T.Murakami Fragment Isotope Spectra from the 36Ar + Ag Reaction at 35 MeV/nucleon NUCLEAR REACTIONS Ag(36Ar, X), E=35 MeV/nucleon; measured inclusive fragment σ(E, θ); deduced total fragment production σ charge, mass dependence.
doi: 10.1103/PhysRevC.49.1012
1993IE01 Phys.Rev.Lett. 70, 730 (1993) K.Ieki, D.Sackett, A.Galonsky, C.A.Bertulani, J.J.Kruse, W.G.Lynch, D.J.Morrissey, N.A.Orr, H.Schulz, B.M.Sherrill, A.Sustich, J.A.Winger, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, R.E.Warner, D.L.Humphrey Coulomb Dissociation of 11Li NUCLEAR REACTIONS Pb(11Li, X), E=28 MeV/nucleon; measured nn-correlation following projectile dissociation; deduced dissociation mechanism.
doi: 10.1103/PhysRevLett.70.730
1993KR09 Phys.Rev. C47, R2439 (1993) R.A.Kryger, A.Azhari, A.Galonsky, J.H.Kelley, R.Pfaff, E.Ramakrishnan, D.Sackett, B.M.Sherrill, M.Thoennessen, J.A.Winger, S.Yokoyama Neutron Decay of 10Li Produced by Fragmentation NUCLEAR REACTIONS C(18O, X), E=80 MeV/nucleon; measured n(9Li)-coin. 10Li deduced level, neutron decay features.
doi: 10.1103/PhysRevC.47.R2439
1993SA21 Phys.Rev. C48, 118 (1993) D.Sackett, K.Ieki, A.Galonsky, C.A.Bertulani, H.Esbensen, J.J.Kruse, W.G.Lynch, D.J.Morrissey, N.A.Orr, B.M.Sherrill, H.Schulz, A.Sustich, J.A.Winger, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.J.Kolata, R.E.Warner, D.L.Humphrey Electromagnetic Excitation of 11Li NUCLEAR REACTIONS Pb(11Li, X), E=28 MeV/nucleon; measured 9Li(n)-, γ(9Li)-coin following 11Li Coulomb dissociation; deduced dissociation σ, photonuclear σ(E1), breakup mechanism.
doi: 10.1103/PhysRevC.48.118
1993SC04 Nucl.Sci.Eng. 113, 184 (1993) H.R.Schelin, A.Galonsky, C.K.Gelbke, H.Hama, L.Heilbronn, D.Krofcheck, W.G.Lynch, D.Sackett, M.B.Tsang, X.Yang, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.Kasagi, T.Murakami Neutron Production in Heavy-Ion Reactions at 35 and 50 MeV/Nucleon NUCLEAR REACTIONS Ag(14N, xn), E=50 MeV/nucleon; measured neutron spectra. Moving source model analysis.
doi: 10.13182/NSE93-A24007
1992WA13 Nucl.Instrum.Methods Phys.Res. A314, 113 (1992) R.E.Warner, R.J.Orr, W.F.Waite, C.P.Browne, S.E.Darden, A.Rollefson, J.J.Kolata, L.Van Wormer, A.Galonsky, D.Sackett, F.D.Becchetti Measurement of the 6Li + (nat)Si Reaction Cross Section at 18 to 28 MeV with a Magnetic Spectrograph and Position-Sensitive Si Detector NUCLEAR REACTIONS, ICPND Si(6Li, X), E=18-28 MeV; measured average reaction σ. Two-dimensional position-sensitive Si detector in magnetic spectrograph focal plane.
doi: 10.1016/0168-9002(92)90503-V
1992YO04 Phys.Rev. C46, 961 (1992) K.Yoshida, J.Kasagi, H.Hama, M.Sakurai, M.Kodama, K.Furutaka, K.Ieki, W.Galster, T.Kubo, M.Ishihara, A.Galonsky Neutron Emission for the Fusion of 40Ar + Ni, 92Mo, 122Sn Reactions at E/A = 26 MeV NUCLEAR REACTIONS Ni, 92Mo, 122Sn(40Ar, nX), E=26 MeV/nucleon; measured neutron energy spectra, σ(θ); deduced hot nuclei nuclear level density parameter.
doi: 10.1103/PhysRevC.46.961
1991DE07 Phys.Rev. C43, 2432 (1991) F.Deak, A.Kiss, Z.Seres, A.Galonsky, L.Heilbronn Isotope Yield Ratios of Fragments from Heavy-Ion Reactions NUCLEAR REACTIONS, ICPND C, Ni, Ag, 165Ho(14N, X), E=35 MeV/nucleon; analyzed isotope yield ratios for X=Li, Be, B, C isotopes. Statistical multi-fragmentation model.
doi: 10.1103/PhysRevC.43.2432
1991HE07 Phys.Rev. C43, 2318 (1991) L.Heilbronn, A.Galonsky, C.K.Gelbke, W.G.Lynch, T.Murakami, D.Sackett, H.Schelin, M.B.Tsang, F.Deak, A.Kiss, Z.Seres, J.Kasagi, B.A.Remington Production of Neutron-Unbound States in Intermediate-Mass Fragments from 14N + Ag Reactions at E/A = 35 MeV NUCLEAR REACTIONS Ag(14N, nX), E=35 MeV/nucleon; measured γ(fragment)-coin, X=Li, Be, B, C isotopes; deduced source temperatures, amount of sequential feeding.
doi: 10.1103/PhysRevC.43.2318
1991SA10 Phys.Rev. C44, 384 (1991) D.Sackett, A.Galonsky, C.K.Gelbke, H.Hama, L.Heilbronn, D.Krofcheck, W.Lynch, H.R.Schelin, M.B.Tsang, X.Yang, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.Kasagi, T.Murakami Neutron Inclusive Measurements of 36Ar + Ag Reactions at 35 MeV/Nucleon NUCLEAR REACTIONS Ag(36Ar, nX), E=35 MeV/nucleon; measured inclusive σ(θ, E); deduced neutron multiplicities, nuclear temperatures. Moving source fits.
doi: 10.1103/PhysRevC.44.384
1990DE25 Phys.Rev. C42, 1029 (1990) F.Deak, A.Kiss, Z.Seres, A.Galonsky, L.Heilbronn, H.R.Schelin Light Fragments from 14N + Ag Collisions at 35 MeV/Nucleon NUCLEAR REACTIONS Ag(14N, X), E=35 MeV/nucleon; measured σ(fragment θ, En, θn); deduced model parameters. Moving source model.
doi: 10.1103/PhysRevC.42.1029
1990GA07 Phys.Rev. C41, 1845 (1990) U.Garg, K.B.Beard, D.Ye, A.Galonsky, T.Murakami, J.S.Winfield, Y.-W.Lui, D.H.Youngblood Experimental Test of a Newly Proposed Empirical Relationship between the Centroid and Width of the Giant Quadrupole Resonance and the Neutron Binding Energy of the Nucleus NUCLEAR REACTIONS 58,64Ni(14N, 14N'), E=700 MeV; measured σ(E(14N)). 58,64Ni deduced GDR parameters.
doi: 10.1103/PhysRevC.41.1845
1990WA12 Nucl.Phys. A516, 416 (1990) R.E.Warner, K.M.Berland, W.F.Rulla, D.A.Francis, J.J.Kolata, Z.Ayer, S.E.Darden, X.J.Kong, G.Liu, A.Morsad, S.McGimpsey, A.A.Rollefson, A.Galonsky, A.Nadasen, J.S.Winfield, F.D.Becchetti Total Nuclear Reaction Probabilities and Average Cross Sections for 16 to 23 MeV 6Li in Silicon NUCLEAR REACTIONS, ICPND Si(6Li, X), E=15.6, 20.3, 23 MeV; measured reaction probabilities, energy averaged total reaction σ.
doi: 10.1016/0375-9474(90)90316-E
1990WA17 Phys.Rev. C42, 2143 (1990) R.E.Warner, E.Cheung, C.F.Perdrisat, V.Punjabi, C.A.Davis, R.Helmer, A.Galonsky, L.Heilbronn, D.Krofcheck, S.E.Darden, J.J.Kolata, F.D.Becchetti, P.Schwandt Spectral Function of p-n Pairs in 6Li, from the 6Li(p, pα)pn Reaction at 200 MeV NUCLEAR REACTIONS 6Li(polarized p, pα), E=200 MeV; measured σ(θp, θα, Ep, Eα) vs (pn)-internal momentum. 6Li deduced dα-cluster probability.
doi: 10.1103/PhysRevC.42.2143
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
1989DE05 Phys.Rev. C39, 733 (1989) F.Deak, A.Kiss, Z.Seres, A.Galonsky, C.K.Gelbke, L.Heilbronn, W.Lynch, T.Murakami, H.Schelin, M.B.Tsang, B.A.Remington, J.Kasagi Dependence of 12B Excitation Energy on Its Kinetic Energy in the 14N + Ag Reaction at E/A = 35 MeV NUCLEAR REACTIONS Ag(14N, 12BX), E=490 MeV; measured σ(θ) vs ejectile energy, n(11B)-coin following ejectile breakup.
doi: 10.1103/PhysRevC.39.733
1989HE24 Phys.Rev. C40, 2576 (1989); Erratum Phys.Rev. C43, 2898 (1991) L.Heilbronn, A.Galonsky, X.Yang, F.Deak, A.Kiss, Z.Seres Determination of Energies and Widths of Neutron-Unbound States from Heavy-Ion Collisions NUCLEAR REACTIONS Ag(14N, 8Be), (14N, 9Li), E=35 MeV/nucleon; measured n(fragment)-coin, relative energy spectra following ejectile breakup. 9Li, 8Be level deduced E, Γ.
doi: 10.1103/PhysRevC.40.2576
1989KA15 Phys.Rev. C40, R1 (1989) E.Kashy, W.Bauer, Y.Chen, A.Galonsky, J.Gaudiello, M.Maier, D.J.Morrissey, R.A.Pelak, M.B.Tsang, J.Yurkon Search for Neutron Emission from Deuterium-Loaded Palladium NUCLEAR REACTIONS 2H(d, n), E=low; measured possible neutron emission upper limit. Heavy water electrolysis, palladium cathode.
doi: 10.1103/PhysRevC.40.R1
1989KI13 Nucl.Phys. A499, 131 (1989) A.Kiss, F.Deak, Z.Seres, G.Caskey, A.Galonsky, B.Remington, L.Heilbronn Fragment Production in 14N + C, Ni, Ho Reactions at 35 MeV/Nucleon NUCLEAR REACTIONS C, Ni, 165Ho(14N, X), E=35 MeV/nucleon; measured σ(fragment θ, E) for X=Li, Be, B, C, N. Spectra decomposition into quasielastic, deep inelastic components.
doi: 10.1016/0375-9474(89)90274-1
1989SC08 Phys.Rev. C39, 1827 (1989) H.R.Schelin, A.Galonsky, C.K.Gelbke, L.Heilbronn, W.G.Lynch, T.Murakami, M.B.Tsang, X.Yang, G.Zhang, B.A.Remington, F.Deak, A.Kiss, Z.Seres, J.Kasagi Neutron Inclusive Measurements in 14N + Ag Reactions at 35 MeV/Nucleon NUCLEAR REACTIONS Ag(14N, nX), E=35 MeV/nucleon; measured σ(θn, En); deduced angle integrated σ.
doi: 10.1103/PhysRevC.39.1827
1989SE03 Nucl.Phys. A492, 315 (1989) Z.Seres, F.Deak, A.Kiss, G.Caskey, A.Galonsky, L.Heilbronn, B.Remington Analysis of Projectile Fragmentation in Intermediate-Energy Heavy-Ion Collisions NUCLEAR REACTIONS 165Ho(14N, X), E=35 MeV/nucleon; analyzed fragment momentum spectra for X=7,9,10Be, 10,11,12B, 11,12,13C; deduced model parameters.
doi: 10.1016/0375-9474(89)90089-4
1988BL09 Phys.Rev. C37, 2469 (1988) C.Bloch, W.Benenson, A.I.Galonsky, E.Kashy, J.Heltsley, L.Heilbronn, M.Lowe, R.J.Radtke, B.Remington, J.Kassagi, D.J.Morrissey Neutrons in Coincidence with Intermediate Mass Fragments at Large Angles from 14N + Ag Reactions at E/A = 20 and 35 MeV NUCLEAR REACTIONS Ag(14N, X), E=20, 35 MeV/nucleon; measured neutron spectra shapes, multiplicities σ(fragment θ, E) for X=6,7Li, 7,9Be, 10,11B; deduced model parameters. Moving source.
doi: 10.1103/PhysRevC.37.2469
1988CA06 Phys.Rev. C37, 969 (1988) G.Caskey, L.Heilbronn, B.Remington, A.Galonsky, F.Deak, A.Kiss, Z.Seres Fragment Spectra from Reactions Induced by 35 MeV/Nucleon 14N on 165Ho NUCLEAR REACTIONS 165Ho(14N, X), E=35 MeV/nucleon; measured σ(fragment θ, E) for X=7,9,10Be, 6,7,8,9Li, 11,12,13B, 10,11,12,13,14,15C. Coalescence model analyses.
doi: 10.1103/PhysRevC.37.969
1988DE44 Acta Phys.Acad.Sci.Hung. 64, 219 (1988) F.Deak, A.Kiss, Z.Seres, G.Caskey, A.Galonsky, B.Remington Energetic Gamma Rays in Coincidence with Light Fragments from Collisions of 35 MeV/u 14N Ions NUCLEAR REACTIONS C, Ni, 165Ho(14N, X), E=35 MeV/nucleon; measured fragment(γ)-coin, γ(θ); deduced reaction mechanism.
1988GL02 Phys.Rev.Lett. 60, 1201 (1988) Comment on ' Giant M1 Resonance in 90Zr ' NUCLEAR REACTIONS 90Zr(p, p'), E=319 MeV; 90Zr(γ, γ'), E not given; analyzed data. 90Zr deduced giant resonance excitation probability probe dependence.
doi: 10.1103/PhysRevLett.60.1201
1988KI06 Phys.Rev. C38, 170 (1988) A.Kiss, F.Deak, Z.Seres, G.Caskey, A.Galonsky, L.Heilbronn, B.Remington Target Mass Dependence of Neutron Emission in Collisions with 35 MeV/Nucleon 14N Ions NUCLEAR REACTIONS 165Ho, Ni, C(14N, nX), E=35 MeV/nucleon; measured (projectile-like fragment)n-coin, neutron spectra, multiplicities.
doi: 10.1103/PhysRevC.38.170
1988RE13 Phys.Rev. C38, 1746 (1988) B.A.Remington, M.Blann, A.Galonsky, L.Heilbronn, F.Deak, A.Kiss, Z.Seres Boltzmann Master Equation Analysis of Preequilibrium Neutron Emission from Heavy-Ion Collisions at 35 MeV/Nucleon NUCLEAR REACTIONS 165Ho(14N, xn), E=35 MeV/nucleon; analyzed data; deduced reaction mechanism. Boltzmann master equation model.
doi: 10.1103/PhysRevC.38.1746
1988WA09 Phys.Rev. C37, 1884 (1988) R.E.Warner, C.P.Browne, S.E.Darden, J.J.Kolata, A.Rollefson, P.A.Kimoto, A.Galonsky Total Nuclear Reaction Probabilities for 2 to 6 MeV/Nucleon d and 3He in Si NUCLEAR REACTIONS Si(d, X), E=4-13 MeV; Si(3He, X), E=5-18 MeV; measured energy integrated, energy averaged total reaction σ. Optical model comparison.
doi: 10.1103/PhysRevC.37.1884
1987BL13 Phys.Rev. C36, 203 (1987) C.Bloch, W.Benenson, A.I.Galonsky, E.Kashy, J.Heltsley, L.Heilbronn, M.Lowe, B.Remington, D.J.Morrissey, J.Kasagi Neutron Decay of Excited Nuclear States in Heavy Ion Collisions NUCLEAR REACTIONS Ag(14N, nX), E=35 MeV/nucleon; measured (fragment)n-coin, yields for X=7,8Li. 7,8Li levels deduced neutron decay characteristics, nuclear temperature.
doi: 10.1103/PhysRevC.36.203
1987DE07 Nucl.Phys. A464, 133 (1987) F.Deak, A.Kiss, Z.Seres, G.Caskey, A.Galonsky, C.K.Gelbke, B.Remington, M.B.Tsang, J.J.Kolata Neutron Emission from 14N + 165Ho Collisions at 35 MeV/u NUCLEAR REACTIONS 165Ho(14N, nX), E=35 MeV/nucleon; measured (projectile-like fragment)n-coin, neutron spectra, multiplicities.
doi: 10.1016/0375-9474(87)90427-1
1987DE37 Nucl.Instrum.Methods Phys.Res. A258, 67 (1987) F.Deak, A.Kiss, Z.Seres, G.Caskey, A.Galonsky, B.Remington Method for the Study of Neutron Emission from Light Fragments in Intermediate Energy Heavy-Ion Collisions NUCLEAR REACTIONS 165Ho(14N, X), E=35 MeV/nucleon; analyzed neutron energy spectra, (fragment)(n)-coin, Li, Be, B, C isotope relative velocity spectra; deduced light fragments neutron emission mechanism.
doi: 10.1016/0168-9002(87)90080-5
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
1987GA17 Phys.Lett. 197B, 511 (1987) A.Galonsky, G.Caskey, L.Heilbronn, B.Remington, H.Schelin, F.Deak, A.Kiss, Z.Seres, J.Kasagi Temperatures Determined from Neutron Emission in Nucleus-Nucleus Collisions NUCLEAR REACTIONS 165Ho(14N, xn), E=35 MeV/nucleon; measured σ(θn, En); deduced temperatures.
doi: 10.1016/0370-2693(87)91045-8
1987KI05 Phys.Lett. 184B, 149 (1987) A.Kiss, F.Deak, Z.Seres, G.Caskey, A.Galonsky, L.Heilbronn, B.A.Remington, J.Kasagi Excitation of Discrete Particle-Unbound States in Heavy-Ion Collisions NUCLEAR REACTIONS 165Ho(14N, nX), E=490 MeV; measured (fragment)n-coin, (fragment)neutron relative velocity spectra for X=7Li, 10Be, 11B, 12C. 8Li, 11Be, 12B, 13C level deduced Γ. ΔE-E telescopes, liquid scintillators.
doi: 10.1016/0370-2693(87)90559-4
1987MA19 Phys.Rev. C35, 2011 (1987); Erratum Phys.Rev. C36, 1647 (1987) R.Madey, B.S.Flanders, B.D.Anderson, A.R.Baldwin, C.Lebo, J.W.Watson, S.M.Austin, A.Galonsky, B.H.Wildenthal, C.C.Foster Gamow-Teller Strength in the 26Mg(p, n)26Al Reaction at 135 MeV and Its Fractionation into T=0, 1, and 2 Isospin Channels NUCLEAR REACTIONS, MECPD 26Mg(p, n), E=134.4 MeV; measured σ(En); deduced σ(θ). 26Al deduced levels, J, π, T, Gamow-Teller transition strength distribution. Tof. DWIA.
doi: 10.1103/PhysRevC.35.2011
1987SE10 Fizika(Zagreb) 19, Supplement 1, 59 (1987) Z.Seres, G.Caskey, F.Deak, A.Galonsky, A.Kiss, B.Remington Excitations of Projectile-like Fragments in Intermediate Energy Heavy-Ion Collisions NUCLEAR REACTIONS 12C, Ni, 165Ho(14N, X), E=35 MeV/nucleon; measured (fragment)n-coin; deduced projectile-like excitation, decay mechanisms.
1987WA25 Nucl.Phys. A472, 522 (1987) R.E.Warner, F.G.Johnson, C.P.Browne, A.Rollefson, A.Galonsky, A.Nadasen The 9Be(3He, 2α)α Reaction from 12 to 24 MeV and Coherent Sequential Decay NUCLEAR REACTIONS, MECPD 9Be(3He, 2α), E=12-24 MeV; measured σ(E1, θ1, θ2). 8Be deduced level α-decay mechanism. 9Be deduced cluster characteristics.
doi: 10.1016/0375-9474(87)90043-1
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
1987WI09 Phys.Rev. C35, 1734 (1987) J.S.Winfield, N.Anantaraman, S.M.Austin, Ziping Chen, A.Galonsky, J.van der Plicht, H.-L.Wu, C.C.Chang, G.Ciangaru Mechanism of the (6Li, 6He) Reaction at Intermediate Energies and Its Suitability as a Spin Probe NUCLEAR REACTIONS 7Li, 12,14C, 26Mg, 90Zr(6Li, 6He), E=14, 25, 35 MeV/nucleon; measured σ(E(6He)), σ(θ); deduced reaction mechanism. 7Be, 12,14C, 27Al, 90Zr deduced Gamow-Teller transition strengths, level excitation mechanism. Magnetic spectrometer. DWBA analyses.
doi: 10.1103/PhysRevC.35.1734
1986AN29 Phys.Rev.Lett. 57, 2375 (1986) N.Anantaraman, J.S.Winfield, S.M.Austin, A.Galonsky, J.van der Plicht, C.C.Chang, G.Ciangaru, S.Gales (6Li, 6He) Reaction as a Probe of Spin-Transfer Strength NUCLEAR REACTIONS 7Li, 12,14C, 26Mg, 90Zr(6Li, 6He), E=210 MeV; measured σ(E(6He)), σ(θ). 7Be, 12,14N, 26Al, 90Nb levels deduced σ, Gamow-Teller transition strength correlation. Spectrograph, focal plane detector. DWBA calculations.
doi: 10.1103/PhysRevLett.57.2375
1986CA16 Phys.Rev. C34, 506 (1986) G.Caskey, A.Galonsky, B.Remington, F.Deak, A.Kiss, Z.Seres Evaporation Recoil Effects: Asymmetries in neutron, projectile-fragment coincidences for 35 MeV/nucleon 14N + 165Ho reactions NUCLEAR REACTIONS 165Ho(14N, nX), E=35 MeV/nucleon; calculated neutron multiplicity vs θn, En, σ(θn, En), n(projectile like fragment)-coin asymmetry; deduced evaporation recoil effects.
doi: 10.1103/PhysRevC.34.506
1986RE13 Phys.Rev. C34, 1685 (1986) B.A.Remington, G.Caskey, A.Galonsky, C.K.Gelbke, L.Heilbronn, J.Heltsley, M.B.Tsang, F.Deak, A.Kiss, Z.Seres, J.Kasagi, J.J.Kolata Neutron-Fragment Coincidence Measurements in 14N + Ho and 14N + Ni Reactions at 35 MeV/Nucleon NUCLEAR REACTIONS Ni, 165Ho(14N, nX), E=35 MeV/nucleon; measured inclusive neutron, fragment spectra, σ(θn, En, fragment θ). Liquid scintillator, ΔE-E identification.
doi: 10.1103/PhysRevC.34.1685
1986WA11 Nucl.Phys. A453, 605 (1986) R.E.Warner, B.A.Vaughan, D.L.Friesel, P.Schwandt, J.-Q.Yang, G.Caskey, A.Galonsky, B.Remington, A.Nadasen The Noncoplanar 7Li(p, pd)5He and 7Li(p, pt)4He Reactions at E(p)=200 MeV, and Evidence for Deuteron Clustering in 7Li NUCLEAR REACTIONS 7Li(p, pd), (p, pt), E=200 MeV; measured σ(Ed, θp, θd, φ), σ(Ep, θp, θt, φ); deduced optical model parameters, d+5He momentum distribution width. 7Li deduced deuteron spectroscopic factors. Enriched target, Ge detectors. DWIA calculations.
doi: 10.1016/0375-9474(86)90254-X
1985CA18 Phys.Rev. C31, 1597 (1985) G.Caskey, A.Galonsky, B.Remington, M.B.Tsang, C.K.Gelbke, A.Kiss, F.Deak, Z.Seres, J.J.Kolata, J.Hinnefeld, J.Kasagi Asymmetric Neutron Emission in 14N + 165Ho Reactions at 35 MeV/nucleon NUCLEAR REACTIONS 165Ho(14N, nX), E=490 MeV; measured σ(En), σ(fragment E), neutron multiplicity spectra, σ(θn, En, fragment E, θ), σ(fragment θ, E); deduced neutron emission asymmetry, moving source parameters.
doi: 10.1103/PhysRevC.31.1597
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
1985KA03 Phys.Rev. C31, 858 (1985); Erratum Phys.Rev. C32, 1107 (1985) J.Kasagi, B.Remington, A.Galonsky, F.Haas, J.J.Kolata, L.Satkowiak, M.Xapsos, R.Racca, F.W.Prosser Neutron Spectra and Level Density Parameters from the 16O + 12C Fusion Reaction NUCLEAR REACTIONS, ICPND 12C(16O, np), (16O, n2p), E=53.7, 56 MeV; 12C(16O, nα), E=43.2, 46, 48.3, 53.7, 56 MeV; measured residual yields vs En, σ(θn); deduced effective radius parameter energy dependence. 27,28Si, 26,27Al, 25Na, 23,24Mg deduced level density, pairing energy parameters.
doi: 10.1103/PhysRevC.31.858
1985WA25 Nucl.Phys. A443, 64 (1985) R.E.Warner, J.-Q.Yang, D.L.Friesel, P.Schwandt, G.Caskey, A.Galonsky, B.Remington, A.Nadasen, N.S.Chant, F.Khazaie, C.Wang Comparison of the Noncoplanar 6Li(p, pd)4He Reactions at 120 and 200 MeV NUCLEAR REACTIONS 6Li(p, pd), E=200.2 MeV; measured σ(E(d), θ(p), θ(d), φ); deduced potentials. 6Li level deduced spectroscopic factor. Enriched target, Ge detectors.
doi: 10.1016/0375-9474(85)90321-5
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
1984TA02 Phys.Rev. C29, 764 (1984) T.N.Taddeucci, R.R.Doering, A.Galonsky, S.M.Austin (p, n) Reactions on 14C and 14N and the Effective Nucleon-Nucleon Interaction NUCLEAR REACTIONS 14N(p, n), E=35.2 MeV; 14C(p, n), E=25.7, 35, 45 MeV; measured σ(θ); deduced optical potential isovector component energy dependence. 14N levels deduced spectroscopic coefficients, Gamow-Teller transition strengths. DWBA, Lane model analyses.
doi: 10.1103/PhysRevC.29.764
1984WA09 Nucl.Phys. A422, 205 (1984) R.E.Warner, R.S.Wakeland, J.-Q.Yang, D.L.Friesel, P.Schwandt, G.Caskey, A.Galonsky, B.Remington, A.Nadasen The Noncoplanar 6Li(p, pd)4He Reaction at 120 MeV, and the 6Li Cluster Momentum Wave Function NUCLEAR REACTIONS 6Li(p, pd), E=119.6 MeV; measured σ(Ed, θd, Ep, φ); deduced reaction mechanism. 6Li deduced α-d cluster spectroscopic factor, momentum distribution. Enriched target. DWIA calculations.
doi: 10.1016/0375-9474(84)90514-1
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
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
1983WA09 Nucl.Phys. A401, 521 (1983) R.E.Warner, K.Blum, D.Friesel, P.Schwandt, P.P.Singh, A.Galonsky Multibody Final States of the 6Li + 6Li Reaction at 97 MeV NUCLEAR REACTIONS 6Li(6Li, 2α), 6Li(6Li, 2d), E=97.5 MeV; measured σ(θ1, θ2, E1, E2) for two-, three-α breakup; deduced reaction mechanisms. Single, double spectator pole models.
doi: 10.1016/0375-9474(83)90363-9
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
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
1981HO03 Phys.Lett. 99B, 383 (1981) D.J.Horen, C.D.Goodman, D.E.Bainum, C.C.Foster, C.Gaarde, C.A.Goulding, M.B.Greenfield, J.Rapaport, T.N.Taddeucci, E.Sugarbaker, T.Masterson, S.M.Austin, A.Galonsky, W.Sterrenburg Energy Systematics of the Giant Gamow-Teller Resonance and a Charge-Exchange Dipole Spin-Flip Resonance NUCLEAR REACTIONS 90,92,94Zr, 112,116,124Sn, 169Tm, 208Pb(p, n), E=120, 160, 200 MeV; measured σ(En, θ). 90,92,94Nb, 112,116,124Sb, 169Yb, 208Bi deduced giant Gamow-Teller, charge exchange dipole spin-flip resonance energy systematics. Tof.
doi: 10.1016/0370-2693(81)90553-0
1981KA30 Phys.Lett. 104B, 434 (1981) J.Kasagi, S.Saini, T.C.Awes, A.Galonsky, C.K.Gelbke, G.Poggi, D.K.Scott, K.L.Wolf, R.L.Legrain Comparison of Non-Compound Neutron and Proton Emission in 16O Induced Reactions on 238U at 310 MeV NUCLEAR REACTIONS, Fission 238U(16O, nF), (16O, pF), E=310 MeV; measured σ(E, θ) vs neutron, proton number, n(fragment)-, p(fragment)-coin. Coalescence model.
doi: 10.1016/0370-2693(81)90509-8
1980BE23 Phys.Rev.Lett. 45, 11 (1980) U.E.P.Berg, S.M.Austin, R.DeVito, A.I.Galonsky, W.A.Sterrenburg Comparison of 24,25,26Mg(p, n)24,25,26Al Cross Sections with Giant M1 Strength NUCLEAR REACTIONS 24,25,26Mg(p, n), E=35 MeV; measured σ(θ). 24,25,26Al deduced large spin-isospin-flip transitions, analog states.
doi: 10.1103/PhysRevLett.45.11
1980CE01 Phys.Rev. C21, 2471 (1980) R.A.Cecil, B.D.Anderson, A.R.Baldwin, R.Madey, A.Galonsky, P.Miller, L.Young, F.M.Waterman Neutron Angular and Energy Distributions from 710-MeV Alphas Stopping In Water, Carbon, Steel, and Lead, and 640-MeV Alphas Stopping in Lead NUCLEAR REACTIONS 2H, O, C, Fe(α, xn), E=710 MeV; Pb(α, xn), E=640, 710 MeV; measured σ(θn, En), stopped α; deduced total integrated neutron yield. Intranuclear cascade model.
doi: 10.1103/PhysRevC.21.2471
1980HU11 Phys.Rev. C22, 1522 (1980) R.Huffman, A.Galonsky, R.Markham, C.Williamson Elastic Scattering of 6Li at 73.7 MeV NUCLEAR REACTIONS 58Ni, 90Zr, 124Sn, 208Pb(6Li, 6Li), E=73.7 MeV; measured σ(θ); deduced optical-model parameters.
doi: 10.1103/PhysRevC.22.1522
1980IW02 Phys.Rev. C22, 456 (1980) Y.Iwasaki, A.Galonsky, D.J.Weber 48Ca(d, n)49Sc Reaction at Ed=20 MeV; Proton Single-Particle States in 49Sc NUCLEAR REACTIONS 48Ca(d, n), E=20 MeV; measured σ(θ). 49Sc levels deduced C2S. DWBA analysis.
doi: 10.1103/PhysRevC.22.456
1980ST26 Phys.Rev.Lett. 45, 1839 (1980) W.A.Sterrenburg, S.M.Austin, R.P.DeVito, A.Galonsky Q-Value Systematics for Isovector Giant Resonances Excited by (p, n) Reactions on Zr, Nb, Mo, Sn, and Pb Isotopes NUCLEAR REACTIONS 112,116,120,122,124Sn, 90,91,93,94,92Zr, 93Nb, 94,96,97,98Mo, 208Pb(p, n), E=45 MeV; measured σ(En); deduced Q-value systematics. 90Nb, 116,120,124Sb, 208Bi deduced IAS, isospin splitting of GDR.
doi: 10.1103/PhysRevLett.45.1839
1980WI05 Phys.Rev. C21, 1344 (1980) C.Williamson, A.Galonsky, R.Huffman, R.Markham Inelastic Scattering of 6Li from 58Ni at 71 MeV NUCLEAR REACTIONS 58Ni(6Li, 6Li'), E=71.2 MeV; measured σ(θ). 58Ni levels deduced deformation lengths.
doi: 10.1103/PhysRevC.21.1344
1979DJ01 Nucl.Phys. A325, 93 (1979) A.Djaloeis, J.-P.Didelez, A.Galonsky, W.Oelert Giant-Resonance Excitation by 130 MeV 3He NUCLEAR REACTIONS 24Mg, 90Zr, 120Sn, 208Pb(3He, 3He'), E=130 MeV; measured σ(θ); deduced giant resonance multipolarity, energy-weighted sum rule strength. Enriched target. DWBA analysis.
doi: 10.1016/0375-9474(79)90154-4
1979DO14 Phys.Rev. C20, 1627 (1979) R.R.Doering, T.N.Taddeucci, A.Galonsky, D.M.Patterson 14C(p, n)14N and the Isovector Tensor Component of the Effective Two-Nucleon Interaction NUCLEAR REACTIONS 14C(p, n), E=35 MeV; measured σ(θ); deduced tensor force. DWBA analysis.
doi: 10.1103/PhysRevC.20.1627
1979JO09 Phys.Rev. C20, 2052 (1979) C.H.Johnson, A.Galonsky, R.L.Kernell (p, n) Reaction for 89 < A < 130 and an Anomalous Optical Model Potential for Sub-Coulomb Protons NUCLEAR REACTIONS 105,106,108,110Pd, 107,109Ag, 111,112,113,114,116Cd, 125,126,128,130Te, 89Y, 93Nb, 103Rh(p, n), E=2.5-5.8 MeV; measured σ; deduced optical model parameters. Enriched targets. Pd, Ag, Cd, In, Te(p, n), E=2.5-5.8 MeV; measured σ; deduced optical model parameters. Natural targets.
doi: 10.1103/PhysRevC.20.2052
1978DJ01 Nucl.Phys. A306, 221 (1978) A.Djaloeis, J.-P.Didelez, A.Galonsky, W.Oelert Elastic Scattering of 130 MeV 3He NUCLEAR REACTIONS 24Mg, 90Zr, 120Sn, 208Pb(3He, 3He), E=130 MeV; measured σ(θ). Enriched targets; optical model analysis.
doi: 10.1016/0375-9474(78)90324-X
1978GA04 Phys.Lett. 74B, 176 (1978) A.Galonsky, J.P.Didelez, A.Djaloeis, W.Oelert Observations of the T = 4 and T = 5 Components of the Giant Gamow-Teller Resonance in the (3He, t) Reaction at 130 MeV NUCLEAR REACTIONS 90Zr(3He, t), E=130 MeV; measured σ(Et, θ). 90Nb deduced giant Gamow-Teller resonances.
doi: 10.1016/0370-2693(78)90546-4
1978SC25 Phys.Lett. 79B, 30 (1978) S.D.Schery, S.M.Austin, A.Galonsky, L.E.Young, U.E.P.Berg Cross Sections for the Quasielastic 112,116,124Sn(p, n) and 58Ni(p, n) Reactions: A Test of the Forward Scattering Amplitude Approximation NUCLEAR REACTIONS 112,116,124Sn(p, n), E=35.3 MeV; measured relative σ(θ) for quasielastic scattering. Isotopically mixed targets. 58Ni(p, n), E=32 MeV; measured σ(θ). DWBA analysis with complex isospin potential in FSA approximation; deduced importance of finite-range correction.
doi: 10.1016/0370-2693(78)90428-8
1977BH02 Z.Phys. A280, 267 (1977) R.Bhowmik, R.R.Doering, A.Galonsky, P.S.Miller Proton Decay of the Isobaric Analogs of the Ground States of 207Pb and 208Pb NUCLEAR REACTIONS 207,208Pb(p, np), E=25 MeV; measured np-coin. 207,208Pb deduced proton decay of IAS, resolved width anomalies.
doi: 10.1007/BF01434352
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