NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = J.F.Liang Found 103 matches. Showing 1 to 100. [Next]2023KI10 Eur.Phys.J. A 59, 112 (2023) S.H.Kim, K.Y.Chae, D.W.Bardayan, J.C.Blackmon, K.A.Chipps, R.Hatarik, K.L.Jones, M.J.Kim, R.L.Kozub, J.F.Liang, C.Matei, B.H.Moazen, C.D.Nesaraja, P.D.O'Malley, S.D.Pain, M.S.Smith Proton branching ratios in 22Mg or X-ray bursts NUCLEAR REACTIONS 24Mg(p, t), E=41 MeV; measured reaction products; deduced triton energy spectra. The Holifield Radioactive Ion Beam Facility (HRIBF) at Oak Ridge National Laboratory (ORNL). RADIOACTIVITY 22Mg(p) [from 24Mg(p, t), E=41 MeV]; analyzed decay products, p-t coin.; deduced coincident proton energy versus triton energy spectra, 21Na excitation energy spectrum, isotropic and anisotropic proton decay, resonance parameters, reaction rates for 21Na(p, γ) reaction.
doi: 10.1140/epja/s10050-023-01029-0
2022JO01 Phys.Rev. C 105, 024602 (2022) K.L.Jones, A.Bey, S.Burcher, J.M.Allmond, A.Galindo-Uribarri, D.C.Radford, S.Ahn, A.Ayres, D.W.Bardayan, J.A.Cizewski, R.F.Garcia Ruiz, M.E.Howard, R.L.Kozub, J.F.Liang, B.Manning, M.Matos, C.D.Nesaraja, P.D.O'Malley, E.Padilla-Rodal, S.D.Pain, S.T.Pittman, A.Ratkiewicz, K.T.Schmitt, M.S.Smith, D.W.Stracener, R.L.Varner Neutron transfer reactions on the ground state and isomeric state of a 130Sn beam NUCLEAR REACTIONS 9Be, 13C(130Sn, 131Sn), E=520 MeV [secondary 130Sn and 130mSn beams from U(p, F)]; measured reaction products, Eγ, Iγ, Eα, αα-coin, αγ-coin, ααγ-coin. 131Sn; deduced levels, J, π, improved energy values for 1p-2h states. Discussed the probability of one-neutron transfer from the 7- isomeric state in 130Sn. CLARION array of 11 Compton-suppressed HPGe clover detectors combined with BareBall CsI(Tl) array at HRIBF.
doi: 10.1103/PhysRevC.105.024602
2020GR01 Phys.Rev.Lett. 124, 032502 (2020) T.J.Gray, J.M.Allmond, A.E.Stuchbery, C.-H.Yu, C.Baktash, A.Gargano, A.Galindo-Uribarri, D.C.Radford, J.C.Batchelder, J.R.Beene, C.R.Bingham, L.Coraggio, A.Covello, M.Danchev, C.J.Gross, P.A.Hausladen, N.Itaco, W.Krolas, J.F.Liang, E.Padilla-Rodal, J.Pavan, D.W.Stracener, R.L.Varner Early Signal of Emerging Nuclear Collectivity in Neutron-Rich 129Sb NUCLEAR REACTIONS 50Ti(129Sb, 129Sb'), E=400 MeV; measured reaction products, Eγ, Iγ. 129Sb; deduced γ-ray energies, J, π, B(E2). Comparison with shell model calculations.
doi: 10.1103/PhysRevLett.124.032502
2019MA26 Phys.Rev. C 99, 041302 (2019); Erratum Phys.Rev. C 99, 069901 (2019) B.Manning, G.Arbanas, J.A.Cizewski, R.L.Kozub, S.Ahn, J.M.Allmond, D.W.Bardayan, K.Y.Chae, K.A.Chipps, M.E.Howard, K.L.Jones, J.F.Liang, M.Matos, C.D.Nesaraja, F.M.Nunes, P.D.O'Malley, S.D.Pain, W.A.Peters, S.T.Pittman, A.Ratkiewicz, K.T.Schmitt, D.Shapira, M.S.Smith, L.Titus Informing direct neutron capture on tin isotopes near the N=82 shell closure NUCLEAR REACTIONS 2H(124Sn, p), (126Sn, p), (128Sn, p), E=630 MeV; measured Ep, Ip, (recoils)p-coin, Q-value spectra, differential σ(θ) using Super Oak Ridge Rutgers University Barrel Array (SuperORRUBA) for light charged particle detection and ionization chamber for detection of beam intensity and recoils at Oak Ridge National Laboratory. 125,127,129Sn; deduced levels, Jπ, L-transfers, spectroscopic factors. 2H(130Sn, p), (132Sn, p); reanalyzed previous experimental data. Angular distribution data compared with Finite Range Adiabatic Wave Approximation. 124,126,128,130,132Sn(n, γ), E=30 keV; calculated direct-semidirect σ(n, γ) from spectroscopic information, and compared with various theoretical predictions. Relevance to r-process abundance calculations.
doi: 10.1103/PhysRevC.99.041302
2017CH22 Phys.Rev. C 95, 045808 (2017) K.A.Chipps, S.D.Pain, R.L.Kozub, D.W.Bardayan, J.A.Cizewski, K.Y.Chae, J.F.Liang, C.Matei, B.H.Moazen, C.D.Nesaraja, P.D.O'Malley, W.A.Peters, S.T.Pittman, K.T.Schmitt, M.S.Smith First spin-parity constraint of the 306 keV resonance in 35Cl for nova nucleosynthesis NUCLEAR REACTIONS 37Cl(p, t), E=30 MeV; measured E(t), I(t), σ(θ) using silicon detector array SIDAR, natural Cl and enriched 37Cl targets HRIBF-ORNL. DWBA analysis of σ(θ) data. 35Cl; deduced level, resonance within the Gamow window, l-transfer and Jπ for 6677-keV level (306-keV proton resonance). Relevance to reaction rate for 34S(p, γ)35Cl in astrophysical applications.
doi: 10.1103/PhysRevC.95.045808
2016LI42 Phys.Rev. C 94, 024616 (2016) J.F.Liang, J.M.Allmond, C.J.Gross, P.E.Mueller, D.Shapira, R.L.Varner, M.Dasgupta, D.J.Hinde, C.Simenel, E.Williams, K.Vo-Phuoc, M.L.Brown, I.P.Carter, M.Evers, D.H.Luong, T.Ebadi, A.Wakhle Examining the role of transfer coupling in sub-barrier fusion of 46, 50Ti + 124Sn NUCLEAR REACTIONS 46,50Ti(124Sn, X), E(cm)=120-154 MeV; 124Sn(46Ti, X), (50Ti, X), E(cm)=116-140 MeV; measured evaporation residues (ERs), fusion σ(E) for the 124Sn beam at HRIBF-ORNL facility, and 46,50Ti beams at ANU 14UD tandem accelerator facility. Comparison of experimental reduced σ(E) values and reduced barrier distributions for 40,48Ca+96Zr, 40,48Ca+124Sn, 40,48Ca+132Sn, 46,50Ti+124Sn, 58,64Ni+124Sn 58,64Ni+132Sn and 64Ni+118Sn reactions. Comparison with coupled-channel calculations using CCFULL code.
doi: 10.1103/PhysRevC.94.024616
2015AL24 Phys.Rev. C 92, 041303 (2015) J.M.Allmond, A.E.Stuchbery, A.Galindo-Uribarri, E.Padilla-Rodal, D.C.Radford, J.C.Batchelder, C.R.Bingham, M.E.Howard, J.F.Liang, B.Manning, S.D.Pain, N.J.Stone, R.L.Varner, C.-H.Yu Investigation into the semimagic nature of the tin isotopes through electromagnetic moments NUCLEAR REACTIONS C, Ti(112Sn, 112Sn'), (114Sn, 114Sn'), (116Sn, 116Sn'), (118Sn, 118Sn'), (120Sn, 120Sn'), (122Sn, 122Sn'), (124Sn, 124Sn'), E=2.9 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin, (particle)γ(θ), absolute cross sections using CLARION Ge array, BareBall CsI array, and a Bragg curve detector at HRIBF-ORNL. 112,114,116,118,120,122,124Sn; deduced E2 matrix elements, B(E2), quadrupole moments, g-factors for the first 2+ states. Coulomb excitation and GOSIA analysis. Comparison with shell model calculations, and several previous experimental measurements. Systematic differences found between results from the present experiment and a recent experiment using DSAM technique.
doi: 10.1103/PhysRevC.92.041303
2015JO03 Acta Phys.Pol. B46, 537 (2015) K.L.Jones, S.Ahn, J.M.Allmond, A.Ayres, D.W.Bardayan, T.Baugher, D.Bazin, J.S.Berryman, A.Bey, C.Bingham, L.Cartegni, G.Cerizza, K.Y.Chae, J.A.Cizewski, A.Gade, A.Galindo-Uribarri, R.F.Garcia Ruiz, R.Grzywacz, M.E.Howard, R.L.Kozub, J.F.Liang, B.Manning, M.MatoS, S.McDaniel, D.Miller, C.D.Nesaraja, P.D.O'Malley, S.Padgett, E.Padilla-Rodal, S.D.Pain, S.T.Pittman, D.C.Radford, A.Ratkiewicz, K.T.Schmitt, A.Shore, M.S.Smith, D.W.Stracener, S.R.Stroberg, J.Tostevin, R.L.Varner, D.Weisshaar, K.Wimmer, R.Winkler Recent Direct Reaction Experimental Studies with Radioactive Tin Beams
doi: 10.5506/APhysPolB.46.537
2015PA23 Phys.Rev.Lett. 114, 212501 (2015) S.D.Pain, D.W.Bardayan, J.C.Blackmon, S.M.Brown, K.Y.Chae, K.A.Chipps, J.A.Cizewski, K.L.Jones, R.L.Kozub, J.F.Liang, C.Matei, M.Matos, B.H.Moazen, C.D.Nesaraja, J.Okolowicz, P.D.O'Malley, W.A.Peters, S.T.Pittman, M.Ploszajczak, K.T.Schmitt, J.F.Shriner, Jr., D.Shapira, M.S.Smith, D.W.Stracener, G.L.Wilson Constraint of the Astrophysical 26gAl(p, γ)27Si Destruction Rate at Stellar Temperatures NUCLEAR REACTIONS 2H(26Al, p), E=117 MeV; measured reaction products, Ep, Ip; deduced σ(θ), spectroscopic factors, astrophysical reaction rates.
doi: 10.1103/PhysRevLett.114.212501
2014AL07 Phys.Rev.Lett. 112, 172701 (2014) J.M.Allmond, E.S.Stuchbery, J.R.Beene, A.Galindo-Uribarri, J.F.Liang, E.Padilla-Rodal, D.C.Radford, R.L.Varner, A.Ayres, J.C.Batchelder, A.Bey, C.R.Bingham, M.E.Howard, K.L.Jones, B.Manning, P.E.Mueller, C.D.Nesaraja, S.D.Pain, W.A.Peters, A.Ratkiewicz, K.T.Schmitt, D.Shapira, M.S.Smith, N.J.Stone, D.W.Stracener, C.-H.Yu Double-Magic Nature of 132Sn and 208Pb through Lifetime and Cross-Section Measurements NUCLEAR REACTIONS 9Be(132Sn, 8Be), (208Pb, 8Be), E=3 MeV/nucleon; measured reaction products, Eγ, Iγ, γ-γ-coin.; deduced energy levels, J, π, σ, level T1/2, B(M1), spectroscopic factors. Comparison with available data, DWBA calculations.
doi: 10.1103/PhysRevLett.112.172701
2014AL14 Phys.Rev. C 90, 014322 (2014) J.M.Allmond, A.E.Stuchbery, B.A.Brown, J.R.Beene, A.Galindo-Uribarri, C.J.Gross, J.F.Liang, E.Padilla-Rodal, D.C.Radford, R.L.Varner, A.Ayres, J.C.Batchelder, A.Bey, C.R.Bingham, M.E.Howard, K.L.Jones, B.Manning, P.E.Mueller, C.D.Nesaraja, S.D.Pain, W.A.Peters, A.Ratkiewicz, K.T.Schmitt, D.Shapira, M.S.Smith, N.J.Stone, D.W.Stracener, C.-H.Yu 2π1ν states populated in 135Te from 9Be-induced reactions with a 132Sn beam NUCLEAR REACTIONS 9Be(132Sn, nα), (132Sn, 2nα), (132Sn, 3nα), E=3 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin using HyBall and CLARION arrays at HRIBF-ORNL facility. 134,135,136Te; deduced levels, J, π. 135Te; deduced σ, spectroscopic factors, DWBA calculations, configurations. Comparison with shell model calculations for 134,135,136Te. NUCLEAR STRUCTURE 134,135,136Te; calculated levels, J, π, wavefunctions, spectroscopic factors using shell model. Comparison with experimental data.
doi: 10.1103/PhysRevC.90.014322
2014AL20 Phys.Rev. C 90, 034309 (2014) J.M.Allmond, B.A.Brown, A.E.Stuchbery, A.Galindo-Uribarri, E.Padilla-Rodal, D.C.Radford, J.C.Batchelder, M.E.Howard, J.F.Liang, B.Manning, R.L.Varner, C.-H.Yu High-precision B(E2) measurements of semi-magic 58, 60, 62, 64Ni by Coulomb excitation NUCLEAR REACTIONS C(58Ni, 58Ni'), (60Ni, 60Ni'), (62Ni, 62Ni'), (64Ni, 64Ni'), E=1.8 MeV/nucleon; measured Eγ, Iγ, γγ-, (scattered Ni particle)γ-coin, (carbon recoils)γ(θ) using CLARION array for γ rays and CsI crystals for particles at HRIBF-ORNL facility. Coulomb excitation. 58,60,62,64Ni; deduced E2 matrix elements for first 2+ to 0+ transitions, B(E2). Comparison with large-basis shell-model calculations, and with other experimental results. Systematics of B(E2) values for first 2+ states in N=28 even-A isotones.
doi: 10.1103/PhysRevC.90.034309
2014ST06 Nucl.Instrum.Methods Phys.Res. A743, 5 (2014) T.K.Steinbach, M.J.Rudolph, Z.Q.Gosser, K.Brown, B.Floyd, S.Hudan, R.T.deSouza, J.F.Liang, D.Shapira, M.Famiano Measuring the fusion cross-section of light nuclei with low-intensity beams NUCLEAR REACTIONS 12C(20O, X)32Si, E(cm)=7.05-11.96 MeV; measured reaction products; deduced fusion σ. Comparison with available data.
doi: 10.1016/j.nima.2013.12.045
2013KO17 Phys.Rev. C 87, 064612 (2013) Z.Kohley, J.F.Liang, D.Shapira, C.J.Gross, R.L.Varner, J.M.Allmond, J.J.Kolata, P.E.Mueller, A.Roberts Sub-barrier fusion enhancement with radioactive 134Te NUCLEAR REACTIONS 40Ca(134Te, X), [134Te secondary beam from U(p, X) primary reaction], E=535-619 MeV; measured evaporation residue spectra using CSSER system at HRIBF facility, σ(E), time-of-flight, ΔE1-ΔE2 contour plots. Comparison with statistical model using PACE2 computer code. Comparison of σ(E) with those in 40Ca+132Te, 48Ca+132Te, 40Ca+124Te, 48Ca+124Te, 64Ni+130Te, 58Ni+130Te reactions. Positive Q-value neutron transfer (PQNT) channels. Coupled-channel analyses.
doi: 10.1103/PhysRevC.87.064612
2013LI14 Acta Phys.Pol. B44, 427 (2013) Recent Results of Fusion Induced by Neutron-rich Radioactive Beams Studied at HRIBF NUCLEAR REACTIONS 40Ca, 58Ni(132Sn, X), 124Sn(46Ti, X), 64Ni(124Sn, X), (126Sn, X), (127Sn, X), (128Sn, X), E not given; measured fusion reaction products; deduced σ. Comparison with available data.
doi: 10.5506/APhysPolB.44.427
2013SC25 Phys.Rev. C 88, 064612 (2013) K.T.Schmitt, K.L.Jones, S.Ahn, D.W.Bardayan, A.Bey, J.C.Blackmon, S.M.Brown, K.Y.Chae, K.A.Chipps, J.A.Cizewski, K.I.Hahn, J.J.Kolata, R.L.Kozub, J.F.Liang, C.Matei, M.Matos, D.Matyas, B.Moazen, C.D.Nesaraja, F.M.Nunes, P.D.O'Malley, S.D.Pain, W.A.Peters, S.T.Pittman, A.Roberts, D.Shapira, J.F.Shriner, M.S.Smith, I.Spassova, D.W.Stracener, N.J.Upadhyay, A.N.Villano, G.L.Wilson Reactions of a 10Be beam on proton and deuteron targets NUCLEAR REACTIONS 2H(10Be, p), (10Be, d), 1H(10Be, p), E=60, 75, 90, 107 MeV; measured Ep, Ip, E(d), I(d), elastic and inelastic σ(θ, E) using SIDAR, ORRUBA, and SuperORRUBA arrays of particle detectors at HRIBF-ORNL facility. 11Be; deduced levels, and spectroscopic factors for halo nucleus. Finite-range adiabatic wave approximation (FR-ADWA) analysis.
doi: 10.1103/PhysRevC.88.064612
2013ST24 Phys.Rev. C 88, 051304 (2013) A.E.Stuchbery, J.M.Allmond, A.Galindo-Uribarri, E.Padilla-Rodal, D.C.Radford, N.J.Stone, J.C.Batchelder, J.R.Beene, N.Benczer-Koller, C.R.Bingham, M.E.Howard, G.J.Kumbartzki, J.F.Liang, B.Manning, D.W.Stracener, C.-H.Yu Electromagnetic properties of the 2+1 state in 134Te: Influence of core excitation on single-particle orbits beyond 132Sn NUCLEAR REACTIONS C(130Te, 130Te'), (134Te, 134Te'), E=390 MeV, also 343 MeV for 130Te; measured scattered particle spectra, Eγ, Iγ, (particle)γ-coin, (particle)γ(θ) using HyBall array for particles and Clarion array of Clover Ge detectors for γ rays at HRIBF-ORNL facility. Combined analysis of B(E2) from Coulomb excitation and g factor from recoil-in vacuum (RIV) method. 130,134Te; deduced level, B(E2) and g factors of first 2+ states. Comparison with previous experimental results, and with theoretical calculations. Systematics of g factors and B(E2) values for 130,132,134,136Te, and for first 2+, 4+ and 6+ states in 134Te. NUCLEAR MOMENTS 134Te; measured g factor of first 2+ state by recoil-in vacuum (RIV) method in Coulomb excitation at HRIBF-ORNL facility. Combined analysis of Coulomb excitation and recoil-in vacuum (RIV) method. Systematics of g factors of first 2+ states in 130,132,134,136Te. Comparison with theoretical calculations.
doi: 10.1103/PhysRevC.88.051304
2012AL13 Phys.Rev. C 86, 031307 (2012) J.M.Allmond, D.C.Radford, J.Pavan, K.Lagergren, C.Baktash, J.R.Beene, C.R.Bingham, L.Chaturvedi, M.Danchev, D.Fong, A.Galindo-Uribarri, P.A.Hausladen, J.K.Hwang, W.Krolas, J.F.Liang, E.Padilla-Rodal, W.Reviol, D.G.Sarantites, D.Seweryniak, D.Shapira, A.E.Stuchbery, J.P.Urrego-Blanco, R.L.Varner, X.Wang, C.-H.Yu, S.Zhu One-neutron transfer study of 135Te and 137Xe by particle-γ coincidence spectroscopy: The ν1i13/2 state at N=83 NUCLEAR REACTIONS 13C(134Te, 12C), (134Te, 13C'), (134Te, 14C), E=565 MeV; 9Be(134Te, 8Be), E=565 MeV; 13C(136Xe, 12C), E=560 MeV; 9Be(136Xe, 8Be), E=560 MeV; measured Eγ, Iγ, particle spectra, (particle)γ-, (particle)γγ-coin, (12C)γ(θ) using HyBall and Clarion arrays as HRIBF facility in ORNL for 134Te beam, and Gammasphere + Microball arrays at ATLAS facility in ANL for 136Xe beam. 134,135Te, 137Xe; deduced levels, J, π, σ, multipolarity. Comparison of measured σ with DWBA predictions, i13/2 states. Z=50-70, N=82, 83; systematics of energies of first 3-, 7/2- and 13/2+ states for even Z nuclei.
doi: 10.1103/PhysRevC.86.031307
2012AN03 Phys.Rev. C 85, 044609 (2012) J.U.Andersen, J.Chevallier, J.S.Forster, S.A.Karamian, C.R.Vane, J.R.Beene, C.J.Gross, H.F.Krause, J.F.Liang, D.Shapira, A.Uguzzoni Time delays in heavy-ion-induced fission of medium-Z nuclei, measured by crystal blocking NUCLEAR REACTIONS Mo(32S, X), E=170, 180 MeV; Mo(48Ti, X), E=225, 240 MeV; Mo(58Ni, X), E=300 MeV; W, Mo(74Ge, X), E=400, 450 MeV; measured spectra of elastically scattered ions and fission fragments, energy loss, blocking lifetimes, blocking dips from elastic scattering at HRIBF facility, fission energy distribution, fission blocking dips, time delays in fission by crystal blocking of fission fragments. Comparison with continuum-model and statistical model calculations.
doi: 10.1103/PhysRevC.85.044609
2012KO18 Phys.Rev. C 85, 054603 (2012) J.J.Kolata, A.Roberts, A.M.Howard, D.Shapira, J.F.Liang, C.J.Gross, R.L.Varner, Z.Kohley, A.N.Villano, H.Amro, W.Loveland, E.Chavez Fusion of 124, 132Sn with 40, 48Ca NUCLEAR REACTIONS 40,48Ca(124Sn, X), (132Sn, X), E(cm)=105-165 MeV; measured evaporation residue spectra, fusion σ(E); deduced reduced fusion σ(E), fusion barriers. Inverse kinematics. Wong model and PACE2 fits. Comparison with time-dependent Hartree-Fock (TDHF) and coupled-channels Born approximation (CCBA) calculations.
doi: 10.1103/PhysRevC.85.054603
2012KO36 Phys.Rev.Lett. 109, 172501 (2012) R.L.Kozub, G.Arbanas, A.S.Adekola, D.W.Bardayan, J.C.Blackmon, K.Y.Chae, K.A.Chipps, J.A.Cizewski, L.Erikson, R.Hatarik, W.R.Hix, K.L.Jones, W.Krolas, J.F.Liang, Z.Ma, C.Matei, B.H.Moazen, C.D.Nesaraja, S.D.Pain, D.Shapira, J.F.Shriner, Jr., M.S.Smith, T.P.Swan Neutron Single Particle Structure in 131Sn and Direct Neutron Capture Cross Sections NUCLEAR REACTIONS 2H(130Sn, p), E=630 MeV; 130Sn(n, γ), E<5 MeV;measured reaction products, Ep, Ip; deduced σ(θ), energy levels, J, π, properties of single-particle states, direct-semidirect σ. Comparison with available data.
doi: 10.1103/PhysRevLett.109.172501
2012LI16 Phys.Rev. C 85, 031601 (2012) J.F.Liang, C.J.Gross, Z.Kohley, D.Shapira, R.L.Varner, J.M.Allmond, A.L.Caraley, K.Lagergren, P.E.Mueller Fusion probability for neutron-rich radioactive-Sn-induced reactions NUCLEAR REACTIONS 64Ni(124Sn, X), (126Sn, X), (127Sn, X), (128Sn, X), E=560 MeV; 58Ni(132Sn, X), E=670 MeV; measured time of flight, energy loss, evaporation residue cross sections as function of the compound nucleus excitation energy; deduced fusion probability. Comparison with Statistical model calculations.
doi: 10.1103/PhysRevC.85.031601
2012RU02 Phys.Rev. C 85, 024605 (2012) M.J.Rudolph, Z.Q.Gosser, K.Brown, S.Hudan, R.T.de Souza, A.Chbihi, B.Jacquot, M.Famiano, J.F.Liang, D.Shapira, D.Mercier Near- and sub-barrier fusion of 20O incident ions with 12C target nuclei NUCLEAR REACTIONS 12C(20O, X), [20O secondary beam from C(22Ne, X), E=79 MeV/nucleon primary beam], E=19.8, 25.0, 41.0 MeV; measured particle spectra, time of flight, energy-TOF spectra, (particle)(particle)-coin, total fusion cross sections; deduced evaporation residue and light charged particle cross sections. 20O, 20F; measured energy spectrum. 12C(16O, X), E(cm)=8-17 MeV; measured particle spectra, total fusion cross sections. Comparison with statistical (EVAPOR) model predictions.
doi: 10.1103/PhysRevC.85.024605
2012SC08 Phys.Rev.Lett. 108, 192701 (2012) K.T.Schmitt, K.L.Jones, A.Bey, S.H.Ahn, D.W.Bardayan, J.C.Blackmon, S.M.Brown, K.Y.Chae, K.A.Chipps, J.A.Cizewski, K.I.Hahn, J.J.Kolata, R.L.Kozub, J.F.Liang, C.Matei, M.Matos, D.Matyas, B.Moazen, C.Nesaraja, F.M.Nunes, P.D.O'Malley, S.D.Pain, W.A.Peters, S.T.Pittman, A.Roberts, D.Shapira, J.F.Shriner, Jr., M.S.Smith, I.Spassova, D.W.Stracener, A.N.Villano, G.L.Wilson Halo Nucleus 11Be: A Spectroscopic Study via Neutron Transfer NUCLEAR REACTIONS 2H(10Be, p)11Be, E=60, 75, 90, 107 MeV; measured reaction products, light ejectiles, Ep, Ip; deduced σ(θ), spectroscopic factors for the first excited and halo neutron states. Comparison with available data.
doi: 10.1103/PhysRevLett.108.192701
2012YA04 Phys.Rev. C 85, 044620 (2012) R.Yanez, W.Loveland, J.Beckerman, M.Leonard, C.J.Gross, D.Shapira, J.F.Liang, Z.Kohley, R.L.Varner Search for inverse fission of uranium NUCLEAR REACTIONS 100Mo(124Sn, X)222U, E=595, 650 MeV; 100Mo (132Sn, X)230U, E=560 MeV; measured Eα, Iα, (ER)α-coin, cross section upper limits; calculated σ(E). 96Zr(124Sn, X), E=200-280 MeV; comparison between measured and predicted σ(E). Statistical model calculations. No evidence for inverse fission.
doi: 10.1103/PhysRevC.85.044620
2011CH56 Phys.Rev. C 84, 059801 (2011) K.A.Chipps, D.W.Bardayan, K.Y.Chae, J.A.Cizewski, R.L.Kozub, J.F.Liang, C.Matei, P.D.O'Malley, S.D.Pain, W.A.Peters, S.T.Pittman, M.S.Smith Comment on "Properties of 26Mg and 26Si in the sd shell model and the determination of the 25Al(p, γ)26Si reaction rate" NUCLEAR REACTIONS 25Al(p, γ)26Si; analyzed and discussed reaction rates for revised level and resonance energy.
doi: 10.1103/PhysRevC.84.059801
2011JO08 Phys.Rev. C 84, 034601 (2011) K.L.Jones, F.M.Nunes, A.S.Adekola, D.W.Bardayan, J.C.Blackmon, K.Y.Chae, K.A.Chipps, J.A.Cizewski, L.Erikson, C.Harlin, R.Hatarik, R.Kapler, R.L.Kozub, J.F.Liang, R.Livesay, Z.Ma, B.Moazen, C.D.Nesaraja, S.D.Pain, N.P.Patterson, D.Shapira, J.F.Shriner Jr, M.S.Smith, T.P.Swan, J.S.Thomas Direct reaction measurements with a 132Sn radioactive ion beam NUCLEAR REACTIONS 2H(132Sn, p), (132Sn, d), E=630 MeV; measured Ep, Ip, Ed, Id, elastic σ, σ(θ), DWBA analysis. 133Sn; deduced levels, J, π, l values, spectroscopic factors, configurations, asymptotic normalization coefficients. 132Sn; deduced ground-state configuration and structure. Level systematics of N=83 nuclei 133Sn, 135Te, 137Xe, 139Ba, 141Ce, 143Nd and 145Sm.
doi: 10.1103/PhysRevC.84.034601
2011KO44 Phys.Rev.Lett. 107, 202701 (2011) Z.Kohley, J.F.Liang, D.Shapira, R.L.Varner, C.J.Gross, J.M.Allmond, A.L.Caraley, E.A.Coello, F.Favela, K.Lagergren, P.E.Mueller Near-Barrier Fusion of Sn + Ni and Te + Ni Systems: Examining the Correlation between Nucleon Transfer and Fusion Enhancement NUCLEAR REACTIONS 58Ni(132Sn, X), E=515 MeV; 58,64Ni(130Te, X), E=670 MeV; measured reaction products; deduced evaporation residue, fission and fusion σ. Comparison with couple channel calculations.
doi: 10.1103/PhysRevLett.107.202701
2010CH44 Phys.Rev. C 82, 045803 (2010) K.A.Chipps, D.W.Bardayan, K.Y.Chae, J.A.Cizewski, R.L.Kozub, J.F.Liang, C.Matei, B.H.Moazen, C.D.Nesaraja, P.D.O'Malley, S.D.Pain, W.A.Peters, S.T.Pittman, K.T.Schmitt, M.S.Smith The 28Si(p, t)26Si*(p) reaction and implications for the astrophysical 25Al(p, γ)26Si reaction rate NUCLEAR REACTIONS 28Si(p, t), E=40 MeV; measured Et, It, Ep, Ip, tp-coin, σ(θ). 26Si; deduced levels, J, π, resonances, l-transfers, and proton decay branching ratios. DWBA analysis. Astrophysical relevance to the reaction rates for 25Al(p, γ).
doi: 10.1103/PhysRevC.82.045803
2010CH46 Phys.Rev. C 82, 047302 (2010) K.Y.Chae, D.W.Bardayan, J.C.Blackmon, K.A.Chipps, R.Hatarik, K.L.Jones, R.L.Kozub, J.F.Liang, C.Matei, B.H.Moazen, C.D.Nesaraja, P.D.O'Malley, S.D.Pain, S.T.Pittman, M.S.Smith Spin assignments to excited states in 22Na through a 24Mg(p, 3He)22Na reaction measurement NUCLEAR REACTIONS 24Mg(p, 3He), E=41, 41.5 MeV; measured E(3He), I(3He), σ(θ), differential σ 22Na; deduced levels, J, π, l-transfers. Distorted-wave Born approximation (DWBA) analysis of s(θ) data.
doi: 10.1103/PhysRevC.82.047302
2010JO03 Nature(London) 465, 454 (2010) K.L.Jones, A.S.Adekola, D.W.Bardayan, J.C.Blackmon, K.Y.Chae, K.A.Chipps, J.A.Cizewski, L.Erikson, C.Harlin, R.Hatarik, R.Kapler, R.L.Kozub, J.F.Liang, R.Livesay, Z.Ma, B.H.Moazen, C.D.Nesaraja, F.M.Nunes, S.D.Pain, N.P.Patterson, D.Shapira, J.F.Shriner Jr, M.S.Smith, T.P.Swan, J.S.Thomas The magic nature of 132Sn explored through the single-particle states of 133Sn NUCLEAR REACTIONS 2H(132Sn, p)133Sn, E=630 MeV; measured Ep, Ip;132Sn; deduced proton σ(θ), Q-value spectrum, properties of single-particle states in 133Sn, magic nature of 132Sn, spectroscopic factors and configurations . DWBA and FRESCO calculations, U(p, F) fission secondary beams.
doi: 10.1038/nature09048
2010LI25 Nucl.Phys. A834, 123c (2010) Highlights of heavy ion fusion induced by neutron-rich radioactive nuclei near the Coulomb barrier
doi: 10.1016/j.nuclphysa.2009.12.020
2010YA21 Phys.Rev. C 82, 054615 (2010) R.Yanez, W.Loveland, A.M.Vinodkumar, P.H.Sprunger, L.Prisbrey, D.Peterson, S.Zhu, J.J.Kolata, A.Villano, J.F.Liang Isospin dependence of capture cross sections: The 36S+208Pb reaction NUCLEAR REACTIONS 208Pb(36S, X), E(cm)=147.5, 151.7, 156.0, 160.6, 169.2, 186.3, 210.2 MeV; measured fission fragments, angular distributions, capture fission cross sections. Comparison of results to empirical prescriptions, QMD model and couple-channel calculations.
doi: 10.1103/PhysRevC.82.054615
2009CH28 Phys.Rev. C 79, 055804 (2009) K.Y.Chae, D.W.Bardayan, J.C.Blackmon, K.A.Chipps, R.Hatarik, K.L.Jones, R.L.Kozub, J.F.Liang, C.Matei, B.H.Moazen, C.D.Nesaraja, P.D.O'Malley, S.D.Pain, S.T.Pittman, M.S.Smith Constraint on the astrophysical 18Ne(α, p)21Na reaction rate through a 24Mg(p, t)22Mg measurement NUCLEAR REACTIONS 24Mg(p, t), E=41, 41.5 MeV; measured triton spectra, σ(θ). 22Mg; deduced levels, J, π. DWBA analysis of σ(θ) data. 18Ne(α, p)21Na; deduced reaction rates versus temperature.
doi: 10.1103/PhysRevC.79.055804
2009LI45 Phys.Lett. B 681, 22 (2009) J.F.Liang, J.R.Beene, A.L.Caraley, H.Esbensen, A.Galindo-Uribarri, C.J.Gross, P.E.Mueller, K.T.Schmitt, D.Shapira, D.W.Stracener, R.L.Varner Dynamic polarization in the Coulomb breakup of loosely bound 17F NUCLEAR REACTIONS 58Ni, 208Pb(17F, p), E=10 MeV/nucleon; measured Ep, Ip, (fragment)p-coin, σ(θ) using silicon strip detectors. Comparison with first-order perturbation and dynamical calculations and effect of dynamic polarization discussed.
doi: 10.1016/j.physletb.2009.09.055
2008LI48 Phys.Rev. C 78, 047601 (2008) J.F.Liang, D.Shapira, C.J.Gross, R.L.Varner, J.R.Beene, P.E.Mueller, D.W.Stracener Fusion of radioactive 132Sn with 64Ni at sub-barrier energies NUCLEAR REACTIONS 64Ni(132Sn, x), E=465 MeV; measured particle spectra, evaporation residues, σ. Comparison with coupled-channel and time-dependent Hartree-Fock calculations. Reanalyzed data at E=453 MeV.
doi: 10.1103/PhysRevC.78.047601
2008VI08 Phys.Rev. C 78, 054608 (2008) A.M.Vinodkumar, W.Loveland, J.J.Neeway, L.Prisbrey, P.H.Sprunger, D.Peterson, J.F.Liang, D.Shapira, C.J.Gross, R.L.Varner, J.J.Kolata, A.Roberts, A.L.Caraley 132Sn+96Zr reaction: A study of fusion enhancement/hindrance NUCLEAR REACTIONS 96Zr(124Sn, X), E(cm)=600 MeV; 96Zr(132Sn, X), E(cm)=192.8-249.1 MeV; calculated σ. Comparison with coupled channels calculations.
doi: 10.1103/PhysRevC.78.054608
2007BA69 Phys.Rev. C 76, 045803 (2007) D.W.Bardayan, J.C.Blackmon, R.P.Fitzgerald, W.R.Hix, K.L.Jones, R.L.Kozub, J.F.Liang, R.J.Livesay, Z.Ma, L.F.Roberts, M.S.Smith, J.S.Thomas, D.W.Visser 30S studied with the 32S(p, t)30S reaction and the 29P(p, γ)30S reaction rate NUCLEAR REACTIONS 32S(p, t), E=37 MeV; measured triton energies, angular distributions. 30S deduced levels, J, π. 29P(p, γ)30S; deduced reaction rates of astrophysical significance.
doi: 10.1103/PhysRevC.76.045803
2007JO09 Acta Phys.Pol. B38, 1205 (2007) K.L.Jones, A.S.Adekola, D.W.Bardayan, J.C.Blackmon, K.Y.Chae, K.Chipps, J.A.Cizewski, D.J.Dean, L.Erikson, R.P.Fitzgerald, A.L.Gaddis, U.Greife, C.Harlin, R.Hatarik, J.A.Howard, M.S.Johnson, R.L.Kozub, J.F.Liang, R.J.Livesay, Z.Ma, B.H.Moazen, P.D.O'Malley, C.D.Nesaraja, S.D.Pain, N.P.Patterson, S.V.Paulauskas, D.Shapira, J.F.Shriner Jr, D.J.Sissom, M.S.Smith, T.P.Swan, J.S.Thomas Single Neutron Transfer Experiments Close to the r-Process Path NUCLEAR REACTIONS 2H(82Ge, p), E=4 MeV/nucleon; 2H(84Se, p), E=4.5 MeV/nucleon; 2H(132Sn, p), E=4.77 MeV/nucleon; measured Ep and angular distributions. 83Ge, 85Se, 133Sn deduced levels, J, π and spectroscopic factors. Compared results to model calculations.
2007LI27 Phys.Rev. C 75, 054607 (2007) J.F.Liang, D.Shapira, J.R.Beene, C.J.Gross, R.L.Varner, A.Galindo-Uribarri, J.Gomez del Campo, P.A.Hausladen, P.E.Mueller, D.W.Stracener, H.Amro, J.J.Kolata, J.D.Bierman, A.L.Caraley, K.L.Jones, Y.Larochelle, W.Loveland, D.Peterson Fusion of radioactive 132Sn with 64Ni NUCLEAR REACTIONS 64Ni(132Sn, X), E=453-620 MeV; measured cross sections and angular distributions. Compared results to statistical model calculations.
doi: 10.1103/PhysRevC.75.054607
2007LI42 Nucl.Phys. A787, 219c (2007) Measurements of fusion induced by radioactive Sn and Te beams NUCLEAR REACTIONS 64Ni(132Sn, X), E(cm)=145-200 MeV; measured fusion σ. 64Ni(124Sn, X), (132Sn, X), (134Sn, X), E(cm)=145-200 MeV; measured evaporation residue σ. 64Ni(112Sn, X), (114Sn, X), (116Sn, X), (118Sn, X), (120Sn, X), (122Sn, X), (124Sn, X), (132Sn, X), E(cm)=140-205 MeV; analyzed evaporation residue σ. Comparison with coupled channel model. Radioactive secondary beams, online mass separator.
doi: 10.1016/j.nuclphysa.2006.12.035
2007LI82 Eur.Phys.J. Special Topics 150, 35 (2007) J.F.Liang, D.Shapira, C.J.Gross, R.L.Varner, H.Amro, J.R.Beene, J.D.Bierman, A.L.Caraley, A.Galindo-Uribarri, J.Gomez del Campo, P.A.Hausladen, K.L.Jones, J.J.Kolata, Y.Larochelle, W.Loveland, P.E.Mueller, D.Peterson, D.C.Radford, D.W.Stracener Measurements of fusion reactions induced by radioactive 132Sn on 64Ni NUCLEAR REACTIONS 132Sn(64Ni, X), E(cm) < 220 MeV; measured evaporation residue and fission cross sections. Compared results to model calculations.
doi: 10.1140/epjst/e2007-00259-7
2007TH15 Phys.Rev. C 76, 044302 (2007) J.S.Thomas, G.Arbanas, D.W.Bardayan, J.C.Blackmon, J.A.Cizewski, D.J.Dean, R.P.Fitzgerald, U.Greife, C.J.Gross, M.S.Johnson, K.L.Jones, R.L.Kozub, J.F.Liang, R.J.Livesay, Z.Ma, B.H.Moazen, C.D.Nesaraja, D.Shapira, M.S.Smith, D.W.Visser Single-neutron excitations in neutron-rich 83Ge and 85Se NUCLEAR REACTIONS 2H(82Ge, p), (84Se, p), E=330, 380 MeV; measured Ep, Ip, recoil-proton-coin, angular distributions; deduced asymptotic normalization coefficients, spectroscopic factors. 83Ge, 85Se; deduced levels, J, π, angular momentum using DWBA analysis. 82Ge, 84Se(n, γ), E=0-1 MeV; calculated cross sections.
doi: 10.1103/PhysRevC.76.044302
2006BA65 Phys.Rev. C 74, 045804 (2006) D.W.Bardayan, J.A.Howard, J.C.Blackmon, C.R.Brune, K.Y.Chae, W.R.Hix, M.S.Johnson, K.L.Jones, R.L.Kozub, J.F.Liang, E.J.Lingerfelt, R.J.Livesay, S.D.Pain, J.P.Scott, M.S.Smith, J.S.Thomas, D.W.Visser Astrophysically important 26Si states studied with the 28Si(p, t)26Si reaction. II. Spin of the 5.914-MeV 26Si level and galactic 26Al production NUCLEAR REACTIONS 28Si(p, t), (p, d), E=40 MeV; measured particle spectra, angular distributions. 26Si level deduced J, π. 25Al(p, γ), E=low; deduced astrophysical reaction rate.
doi: 10.1103/PhysRevC.74.045804
2006HA62 Int.J. Mass Spectrom. 251, 119 (2006) P.A.Hausladen, J.R.Beene, A.Galindo-Uribarri, Y.Larochelle, J.F.Liang, P.E.Mueller, D.Shapira, D.W.Stracener, J.Thomas, R.L.Varner, H.Wollnik Opportunistic mass measurements at the Holifield Radioactive Ion Beam Facility ATOMIC MASSES 77,78,79Cu, 83,84,85,86Ge; measured mass excesses. Isotopes produced from 238U(p, F) reaction at beam energy 42 MeV using ISOL method. Proposed technique for measuring mass differences developed at the Holifield Radioactive Ion Beam Facility (HRIBF).
doi: 10.1016/j.ijms.2006.01.020
2006LO13 Phys.Rev. C 74, 044607 (2006) W.Loveland, D.Peterson, A.M.Vinodkumar, P.H.Sprunger, D.Shapira, J.F.Liang, G.A.Souliotis, D.J.Morrissey, P.Lofy Fusion enhancement in the 38S + 208Pb reaction NUCLEAR REACTIONS 208Pb(38S, X), E(cm)=160-265 MeV; measured capture-fission excitation function; deduced interaction barrier features.
doi: 10.1103/PhysRevC.74.044607
2006VI10 Phys.Rev.C 74, 064612 (2006) A.M.Vinodkumar, W.Loveland, P.H.Sprunger, D.Peterson, J.F.Liang, D.Shapira, R.L.Varner, C.J.Gross, J.J.Kolata Capture cross sections for the near symmetric 124Sn+96Zr reaction NUCLEAR REACTIONS 96Zr(124Sn, X), E(cm)=195-265 MeV; measured capture-fission σ. Comparison with model predictions.
doi: 10.1103/PhysRevC.74.064612
2005BA82 Nucl.Phys. A758, 737c (2005) D.W.Bardayan, J.C.Blackmon, J.Gomez del Campo, R.L.Kozub, J.F.Liang, Z.Ma, L.Sahin, D.Shapira, M.S.Smith New 19Ne Level Observed with a Thick Target 18F(p, p)18F Measurement NUCLEAR REACTIONS 1H(18F, p), E(cm) ≈ 0.3-1.3 MeV; measured proton spectra, σ(θ), excitation functions. 19Ne deduced resonance parameters, excited state energy, J, π. 18F(p, α), (p, γ), E=low; calculated astrophysical reaction rates.
doi: 10.1016/j.nuclphysa.2005.05.133
2005BB05 Eur.Phys.J. A 25, Supplement 1, 643 (2005) D.W.Bardayan, J.C.Blackmon, J.Gomez del Campo, R.L.Kozub, J.F.Liang, Z.Ma, D.Shapira, L.Sahin, M.S.Smith New 19Ne resonance observed using an exotic 18F beam NUCLEAR REACTIONS 1H(18F, p), E(cm) ≈ 0.3-1.3 MeV; measured Ep, σ(θ); deduced excitation functions. 19Ne deduced resonance energies, J, π, analog states. 18F(p, α), (p, γ), E=low; calculated astrophysical reaction rates.
doi: 10.1140/epjad/i2005-06-007-3
2005BL23 Phys.Rev. C 72, 034606 (2005) J.C.Blackmon, F.Carstoiu, L.Trache, D.W.Bardayan, C.R.Brune, C.A.Gagliardi, U.Greife, C.J.Gross, C.C.Jewett, R.L.Kozub, T.A.Lewis, J.F.Liang, B.H.Moazen, A.M.Mukhamedzhanov, C.D.Nesaraja, F.M.Nunes, P.D.Parker, L.Sahin, J.P.Scott, D.Shapira, M.S.Smith, J.S.Thomas, R.E.Tribble Elastic scattering of the proton drip-line nucleus 17F NUCLEAR REACTIONS 12C, 14N(17F, 17F), E=10 MeV/nucleon; measured σ(θ); deduced parameters, reaction mechanism features. Double-folding procedure.
doi: 10.1103/PhysRevC.72.034606
2005CI07 Nucl.Instrum.Methods Phys.Res. B241, 200 (2005) J.A.Cizewski, K.L.Jones, S.D.Pain, J.S.Thomas, C.Baktash, D.W.Bardayan, J.C.Blackmon, C.Gross, J.F.Liang, D.Shapira, M.S.Smith, R.L.Kozub, B.H.Moazen, C.D.Nesaraja, H.K.Carter, M.S.Johnson, R.P.Fitzgerald, D.W.Visser, U.Greife, R.J.Livesay, W.Catford, Z.Ma Neutron transfer reactions with neutron-rich radioactive ion beams NUCLEAR REACTIONS 2H(82Ge, p), (84Se, p), E=4 MeV/nucleon; measured Ep, σ(θ). 83Ge, 85Se deduced ground and excited states energies, J, π.
doi: 10.1016/j.nimb.2005.07.025
2005LI55 Eur.Phys.J. A 25, Supplement 1, 239 (2005) J.F.Liang, D.Shapira, C.J.Gross, R.L.Varner, H.Amro, J.R.Beene, J.D.Bierman, A.L.Caraley, A.Galindo-Uribarri, J.Gomez del Campo, P.A.Hausladen, K.L.Jones, J.J.Kolata, Y.Larochelle, W.Loveland, P.E.Mueller, D.Peterson, D.C.Radford, D.W.Stracener Sub-barrier fusion induced by neutron-rich radioactive 132Sn NUCLEAR REACTIONS 64Ni(132Sn, X), E=560 MeV; measured fission fragments and evaporation residues spectra, yields.
doi: 10.1140/epjad/i2005-06-117-x
2005LI64 Int.J.Mod.Phys. E14, 1121 (2005) Fusion induced by radioactive ion beams NUCLEAR REACTIONS 209Bi, 238U(6He, X), E(cm) ≈ 18-32 MeV; 63,65Cu(6He, X), (8He, X), 188,190,192Os(6He, X), E ≈ 20-30 MeV; 209Bi(9Be, X), (10Be, X), (11Be, X), E(cm) ≈ 34-50 MeV; 208Pb(17F, X), E(cm) ≈ 80-160 MeV; 197Au(27Al, X), (29Al, X), (31Al, X), E not given; 181Ta(38S, X), E=161-254 MeV; 64Ni(132Sn, X), E(cm) ≈ 140-200 MeV; 124Sn(64Ni, X), E(cm) ≈ 150-200 MeV; compiled, analyzed fusion, fission, evaporation residue, reaction, and breakup σ.
doi: 10.1142/S021830130500382X
2005RA09 Nucl.Phys. A752, 264c (2005) D.C.Radford, C.Baktash, C.J.Barton, J.Batchelder, J.R.Beene, C.R.Bingham, M.A.Caprio, M.Danchev, B.Fuentes, A.Galindo-Uribarri, J.Gomez del Campo, C.J.Gross, M.L.Halbert, D.J.Hartley, P.Hausladen, J.K.Hwang, W.Krolas, Y.Larochelle, J.F.Liang, P.E.Mueller, E.Padilla, J.Pavan, A.Piechaczek, D.Shapira, D.W.Stracener, R.L.Varner, A.Woehr, C.-H.Yu, N.V.Zamfir Coulomb excitation and transfer reactions with rare neutron-rich isotopes NUCLEAR REACTIONS C(126Sn, 126Sn'), (128Sn, 128Sn'), (130Sn, 130Sn'), (132Sn, 132Sn'), (134Sn, 134Sn'), (132Te, 132Te'), (134Te, 134Te'), (136Te, 136Te'), E not given; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 126,128,130,132,134Sn, 132,134,136Te deduced transitions B(E2). 9Be(134Te, 8Be), 13C(134Te, 12C), E not given; measured Eγ, Iγ, γγ-, (particle)γ-coin. 135Te deduced level. Clarion, Hyball arrays.
doi: 10.1016/j.nuclphysa.2005.02.040
2005RA32 Eur.Phys.J. A 25, Supplement 1, 383 (2005) D.C.Radford, C.Baktash, C.J.Barton, J.Batchelder, J.R.Beene, C.R.Bingham, M.A.Caprio, M.Danchev, B.Fuentes, A.Galindo-Uribarri, J.Gomez del Campo, C.J.Gross, M.L.Halbert, D.J.Hartley, P.Hausladen, J.K.Hwang, W.Krolas, Y.Larochelle, J.F.Liang, P.E.Mueller, E.Padilla, J.Pavan, A.Piechaczek, D.Shapira, D.W.Stracener, R.L.Varner, A.Woehr, C.-H.Yu, N.V.Zamfir Coulomb excitation and transfer reactions with neutron-rich radioactive beams NUCLEAR REACTIONS C(126Sn, 126Sn'), (128Sn, 128Sn'), (130Sn, 130Sn'), (132Te, 132Te'), (134Te, 134Te'), (136Te, 136Te'), E not given; measured Eγ, Iγ, γγ-, (particle)γ-coin following projectile Coulomb excitation. 132,134,136Te, 126,128,130Sn deduced excitation B(E2). 9Be(134Te, 8Be), 13C(134Te, 12C), E=4.3 MeV/nucleon; measured Eγ, Iγ, γγ-coin, (particle)γ-coin; deduced single-neutron transfer σ(E). 135Te deduced levels J, π.
doi: 10.1140/epjad/i2005-06-205-y
2005RO42 Eur.Phys.J. A 25, Supplement 1, 289 (2005) M.Romoli, M.Mazzocco, E.Vardaci, M.Di Pietro, A.De Francesco, R.Bonetti, A.De Rosa, T.Glodariu, A.Guglielmetti, G.Inglima, M.La Commara, B.Martin, V.Masone, P.Parascandolo, D.Pierroutsakou, M.Sandoli, P.Scopel, C.Signorini, F.Soramel, L.Stroe, J.Greene, A.Heinz, D.Henderson, C.L.Jiang, E.F.Moore, R.C.Pardo, K.E.Rehm, A.Wuosmaa, J.F.Liang The EXODET apparatus: Features and first experimental results NUCLEAR REACTIONS 208Pb(17F, 17F), (17F, 16OX), E=90.4 Mev; measured σ(θ).
doi: 10.1140/epjad/i2005-06-187-8
2005SH44 Nucl.Instrum.Methods Phys.Res. A551, 330 (2005) D.Shapira, J.F.Liang, C.J.Gross, R.L.Varner, H.Amro, C.Harlin, J.J.Kolata, S.Novotny A high-efficiency compact setup to study evaporation residues formed in reactions induced by low-intensity radioactive ion beams NUCLEAR REACTIONS 64Ni(134Sn, X), E(cm) ≈ 150-163 MeV; measured evaporation residue σ.
doi: 10.1016/j.nima.2005.05.079
2005SH54 Eur.Phys.J. A 25, Supplement 1, 241 (2005) D.Shapira, J.F.Liang, C.J.Gross, R.L.Varner, J.R.Beene, A.Galindo-Uribarri, J.Gomez Del Campo, P.E.Mueller, D.W.Stracener, P.A.Hausladen, C.Harlin, J.J.Kolata, H.Amro, W.Loveland, K.L.Jones, J.D.Bierman, A.L.Caraley Measurement of evaporation residue cross sections from reactions with radioactive neutron-rich beams NUCLEAR REACTIONS 64Ni(132Sn, X), (124Sn, X), (134Te, X), E not given; measured evaporation residue σ.
doi: 10.1140/epjad/i2005-06-190-1
2005TH03 Phys.Rev. C 71, 021302 (2005) J.S.Thomas, D.W.Bardayan, J.C.Blackmon, J.A.Cizewski, U.Greife, C.J.Gross, M.S.Johnson, K.L.Jones, R.L.Kozub, J.F.Liang, R.J.Livesay, Z.Ma, B.H.Moazen, C.D.Nesaraja, D.Shapira, M.S.Smith First study of the level structure of the r-process nucleus 83Ge NUCLEAR REACTIONS 2H(82Ge, p), E=330 MeV; measured proton spectra, σ(θ), Q value. 83Ge deduced levels, J, π, spectroscopic factors, mass excess.
doi: 10.1103/PhysRevC.71.021302
2005TH09 Nucl.Phys. A758, 663c (2005) J.S.Thomas, D.W.Bardayan, J.C.Blackmon, J.A.Cizewski, R.P.Fitzgerald, U.Greife, C.J.Gross, M.S.Johnson, K.L.Jones, R.L.Kozub, J.F.Liang, R.J.Livesay, Z.Ma, B.H.Moazen, C.D.Nesaraja, D.Shapira, M.S.Smith, D.W.Visser Neutron Single-Particle States in r-Process Nuclei Near Closed Shells NUCLEAR REACTIONS 2H(84Se, p), (124Sn, p), E=4.5 MeV/nucleon; measured recoil proton spectra, σ(E, θ). 85Se, 125Sn deduced levels, J, π.
doi: 10.1016/j.nuclphysa.2005.05.119
2005TH12 Eur.Phys.J. A 25, Supplement 1, 371 (2005) J.S.Thomas, D.W.Bardayan, J.C.Blackmon, J.A.Cizewski, R.P.Fitzgerald, U.Greife, C.J.Gross, M.S.Johnson, K.L.Jones, R.L.Kozub, J.F.Liang, R.J.Livesay, Z.Ma, B.H.Moazen, C.D.Nesaraja, D.Shapira, M.S.Smith, D.W.Visser Single-neutron excitations in neutron-rich N = 51 nuclei NUCLEAR REACTIONS 2H(82Ge, p), E=4 MeV/nucleon; 2H(84Se, p), E=4.5 MeV/nucleon; measured Ep, recoil particle spectrum, proton angular distribution. 83Ge, 85Se deduced levels J, π, spectroscopic factors. DWBA analysis.
doi: 10.1140/epjad/i2005-06-127-8
2005VA31 Eur.Phys.J. A 25, Supplement 1, 391 (2005) R.L.Varner, J.R.Beene, C.Baktash, A.Galindo-Uribarri, C.J.Gross, J.Gomez del Campo, M.L.Halbert, P.A.Hausladen, Y.Larochelle, J.F.Liang, J.Mas, P.E.Mueller, E.Padilla-Rodal, D.C.Radford, D.Shapira, D.W.Stracener, J.-P.Urrego-Blanco, C.-H.Yu Coulomb excitation measurements of transition strengths in the isotopes 132, 134Sn NUCLEAR REACTIONS 48Ti(132Sn, 132Sn'), E=470-495 MeV; 90Zr(134Sn, 134Sn'), E=400 MeV; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 132,134Sn deduced transitions B(E2).
doi: 10.1140/epjad/i2005-06-128-7
2005YU07 Eur.Phys.J. A 25, Supplement 1, 395 (2005) C.-H.Yu, C.Baktash, J.C.Batchelder, J.R.Beene, C.Bingham, M.Danchev, A.Galindo-Uribarri, C.J.Gross, P.A.Hausladen, W.Krolas, J.F.Liang, E.Padilla, J.Pavan, D.C.Radford Coulomb excitation of odd-A neutron-rich radioactive beams NUCLEAR REACTIONS 50Ti(129Sb, 129Sb'), (129Te, 129Te'), E=400 MeV; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 129Te, 129Sb deduced transitions B(E2). Clarion, Hyball arrays.
doi: 10.1140/epjad/i2005-06-144-7
2004BA63 Phys.Rev. C 70, 015804 (2004) D.W.Bardayan, J.C.Blackmon, J.Gomez del Campo, R.L.Kozub, J.F.Liang, Z.Ma, L.Sahin, D.Shapira, M.S.Smith Search for astrophysically important 19Ne levels with a thick-target 18F(p, p)18F measurement NUCLEAR REACTIONS 1H(18F, p), E(cm) ≈ 0.3-1.3 MeV; measured Ep; deduced excitation function. 19Ne deduced levels, J, π, widths. Astrophysical implications discussed.
doi: 10.1103/PhysRevC.70.015804
2004BB08 Nucl.Phys. A746, 557c (2004) D.W.Bardayan, J.C.Blackmon, J.Gomez del Campo, R.L.Kozub, J.F.Liang, Z.Ma, D.Shapira, M.S.Smith Studies of the 18F(p, α)15O reaction rate with a 18F beam at the HRIBF NUCLEAR REACTIONS 1H(18F, p), E=0-24 MeV; measured Ep, σ(θ), excitation function. 19Ne deduced resonance width upper limit.
doi: 10.1016/j.nuclphysa.2004.09.089
2004BB10 Nucl.Phys. A746, 593c (2004) D.W.Bardayan, J.C.Blackmon, J.Gomez del Campo, R.L.Kozub, J.F.Liang, Z.Ma, D.Shapira, M.S.Smith Studies of the 18F(p, α) 15O reaction rate with a 18F beam at the HRIBF NUCLEAR REACTIONS 1H(18F, p), E=0-24 MeV; measured Ep, σ(θ), excitation function. 19Ne deduced resonance width upper limit.
doi: 10.1016/j.nuclphysa.2004.09.095
2004BE56 Nucl.Phys. A746, 471c (2004) J.R.Beene, R.L.Varner, C.Baktash, A.Galindo-Uribarri, C.J.Gross, J.Gomez del Campo, M.L.Halbert, P.A.Hausladen, Y.Larochelle, J.F.Liang, J.Mas, P.E.Mueller, E.Padilla-Rodal, D.C.Radford, D.Shapira, D.W.Stracener, J.-P.Urrego-Blanco, C.-H.Yu Coulomb excitation studies of 132, 134Sn NUCLEAR REACTIONS 48Ti(132Sn, 132Sn'), E=470, 495 MeV; 90Zr(134Sn, 134Sn'), E=400 MeV; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 132,134Sn levels deduced excitation B(E2).
doi: 10.1016/j.nuclphysa.2004.09.143
2004LI55 Prog.Theor.Phys.(Kyoto), Suppl. 154, 106 (2004) J.F.Liang, D.Shapira, C.J.Gross, J.R.Beene, J.D.Bierman, A.Galindo-Uribarri, J.Gomez del Campo, P.A.Hausladen, Y.Larochelle, W.Loveland, P.E.Mueller, D.Peterson, D.C.Radford, D.W.Stracener, R.L.Varner Sub-Barrier Fusion Enhancement in Neutron-Rich Radioactive 132Sn on 64Ni NUCLEAR REACTIONS 64Ni(132Sn, X), E(cm)=140-200 MeV; measured evaporation residue excitation function; deduced sub-barrier fusion enhancement.
doi: 10.1143/PTPS.154.106
2004LI71 Nucl.Phys. A746, 103c (2004) J.F.Liang, D.Shapira, C.J.Gross, J.R.Beene, J.D.Bierman, A.Galindo-Uribarri, J.Gomez del Campo, P.A.Hausladen, Y.Larochelle, W.Loveland, P.E.Mueller, D.Peterson, D.C.Radford, D.W.Stracener, R.L.Varner Enhanced evaporation residue cross sections in neutron-rich radioactive 132Sn on 64Ni NUCLEAR REACTIONS 64Ni(132Sn, X), (124Sn, X), E(cm) ≈ 150-200 MeV; measured evaporation residue σ; deduced sub-barrier fusion enhancement for heavier beam. Comparison with previous results, model predictions.
doi: 10.1016/j.nuclphysa.2004.09.057
2004RA27 Nucl.Phys. A746, 83c (2004) D.C.Radford, C.Baktash, J.R.Beene, B.Fuentes, A.Galindo-Uribarri, J.Gomez del Campo, C.J.Gross, M.L.Halbert, Y.Larochelle, T.A.Lewis, J.F.Liang, J.Mas, P.E.Mueller, E.Padilla, D.Shapira, D.W.Stracener, R.L.Varner, C.-H.Yu, C.J.Barton, M.A.Caprio, D.J.Hartley, N.V.Zamfir Nuclear structure studies with heavy neutron-rich RIBS at the HRIBF NUCLEAR REACTIONS C(126Sn, 126Sn'), (128Sn, 128Sn'), (130Sn, 130Sn'), (132Sn, 132Sn'), (134Sn, 134Sn'), (132Te, 132Te'), (134Te, 134Te'), (136Te, 136Te'), E < 3 MeV/nucleon; measured Eγ, Iγ, (recoil)γ-coin following projectile Coulomb excitation. 126,128,130,132,134Sn, 132,134,136Te deduced excitation B(E2). 9Be(134Te, 8Be), 13C(134Te, 12C), E ≈ 4 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin.
doi: 10.1016/j.nuclphysa.2004.09.056
2004RO23 Phys.Rev. C 69, 064614 (2004) M.Romoli, E.Vardaci, M.Di Pietro, A.De Francesco, A.De Rosa, G.Inglima, M.La Commara, B.Martin, D.Pierroutsakou, M.Sandoli, M.Mazzocco, T.Glodariu, P.Scopel, C.Signorini, R.Bonetti, A.Guglielmetti, F.Soramel, L.Stroe, J.Greene, A.Heinz, D.Henderson, C.L.Jiang, E.F.Moore, R.C.Pardo, K.E.Rehm, A.Wuosmaa, J.F.Liang Measurements of 17F scattering by 208Pb with a new type of large solid angle detector array NUCLEAR REACTIONS 208Pb(17F, 17F), E=90.4 MeV; measured σ(θ); 208Pb(19F, 19F), E=91 MeV; 208Pb(16O, 16O), (17O, 17O), E=78 MeV; analyzed σ(θ); deduced optical model parameters. 208Pb(17F, p16O), E=90.4 MeV; measured breakup σ. Exodet detector array.
doi: 10.1103/PhysRevC.69.064614
2004RO43 Nucl.Phys. A746, 522c (2004) M.Romoli, M.Mazzocco, E.Vardaci, M.Di Pietro, R.Bonetti, A.De Francesco, A.De Rosa, T.Glodariu, A.Guglielmetti, G.Inglima, M.La Commara, B.Martin, D.Pierroutsakou, M.Sandoli, P.Scopel, C.Signorini, F.Soramel, L.Stroe, J.Greene, A.Heinz, D.Henderson, C.L.Jiang, J.F.Liang, E.F.Moore, R.C.Pardo, K.E.Rehm, A.Wuosmaa Elastic scattering of 17F on 208Pb and 17F breakup cross section at Coulomb barrier energies NUCLEAR REACTIONS 208Pb(17F, 17F), E=90.4 MeV; measured σ(θ); deduced optical model parameters. 208Pb(17F, p16O), E=90.4 MeV; measured breakup σ.
doi: 10.1016/j.nuclphysa.2004.09.085
2004TH12 Nucl.Phys. A746, 178c (2004) J.S.Thomas, D.W.Bardayan, J.C.Blackmon, J.A.Cizewski, U.Greife, C.J.Gross, M.S.Johnson, K.L.Jones, R.L.Kozub, J.F.Liang, R.J.Livesay, Z.Ma, B.H.Moazen, C.D.Nesaraja, D.Shapira, M.S.Smith Studies of the neutron single-particle structure of exotic nuclei at the HRIBF NUCLEAR REACTIONS 2H(82Ge, p), E=4 MeV/nucleon; measured Ep, σ(θ). 83Ge deduced levels.
doi: 10.1016/j.nuclphysa.2004.09.032
2003HE03 Phys.Lett. B 555, 43 (2003) P.Heckman, D.Bazin, J.R.Beene, Y.Blumenfeld, M.J.Chromik, M.L.Halbert, J.F.Liang, E.Mohrmann, T.Nakamura, A.Navin, B.M.Sherrill, K.A.Snover, M.Thoennessen, E.Tryggestad, R.L.Varner Low-temperature measurement of the giant dipole resonance width NUCLEAR REACTIONS 120Sn(17O, 17O'), E=80 MeV/nucleon; measured particle spectra, Eγ, Iγ, (particle)γ-coin. 120Sn deduced width of GDR built on excited states, influence of thermal shape fluctuations. Comparison with model predictions.
doi: 10.1016/S0370-2693(03)00017-0
2003LI14 Phys.Rev. C 67, 044603 (2003) J.F.Liang, J.R.Beene, A.Galindo-Uribarri, J.Gomez del Campo, C.J.Gross, P.A.Hausladen, P.E.Mueller, D.Shapira, D.W.Stracener, R.L.Varner, J.D.Bierman, H.Esbensen, Y.Larochelle Breakup of 17F on 208Pb near the Coulomb barrier NUCLEAR REACTIONS 208Pb(17F, 16OX), E=98, 120 MeV; measured oxygen particles σ(θ); deduced reaction mechanism features. 208Pb(17F, 17F), E=98, 120 MeV; measured σ(θ). 208Pb(17F, X), E(cm) ≈ 70-120 MeV; calculated fusion σ.
doi: 10.1103/PhysRevC.67.044603
2003LI41 Phys.Rev.Lett. 91, 152701 (2003); Erratum Phys.Rev.Lett. 96, 029903 (2006) J.F.Liang, D.Shapira, C.J.Gross, J.R.Beene, J.D.Bierman, A.Galindo-Uribarri, J.Gomez del Campo, P.A.Hausladen, Y.Larochelle, W.Loveland, P.E.Mueller, D.Peterson, D.C.Radford, D.W.Stracener, R.L.Varner Enhanced Fusion-Evaporation Cross Sections in Neutron-Rich 132Sn on 64Ni NUCLEAR REACTIONS 64Ni(132Sn, X), E=453-560 MeV; measured fusion-evaporation excitation function; deduced sub-barrier enhancement, role of multinucleon transfer. Coupled channels calculation.
doi: 10.1103/PhysRevLett.91.152701
2003TR05 Phys.Rev. C 67, 064309 (2003) E.Tryggestad, T.Baumann, P.Heckman, M.Thoennessen, T.Aumann, D.Bazin, Y.Blumenfeld, J.R.Beene, T.A.Lewis, D.C.Radford, D.Shapira, R.L.Varner, M.Chartier, M.L.Halbert, J.F.Liang Low-lying E1 strength in 20O NUCLEAR REACTIONS 208Pb(18O, 18O'), (20O, 20O'), E=100 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 18,20O deduced levels, J, π, B(E1). Comparison with model predictions.
doi: 10.1103/PhysRevC.67.064309
2002LI34 Phys.Rev. C65, 051603 (2002) J.F.Liang, J.R.Beene, H.Esbensen, A.Galindo-Uribarri, J.Gomez del Campo, C.J.Gross, M.L.Halbert, P.E.Mueller, D.Shapira, D.W.Stracener, I.J.Thompson, R.L.Varner Elastic Scattering and Breakup of 17F at 10 MeV/nucleon NUCLEAR REACTIONS 208Pb(17F, 17F), (17F, 16O), E=170 MeV; measured σ(θ); deduced reaction mechanism features. Comparison with optical model predictions.
doi: 10.1103/PhysRevC.65.051603
2002LI66 Acta Phys.Hung.N.S. 16, 213 (2002) Study of Nuclear Reactions with Radioactive 17F at HRIBF NUCLEAR REACTIONS 1H(17F, p), E=33, 44 MeV; measured recoil proton spectra, excitation function. 18Ne level deduced two-proton emission features. 208Pb(17F, p16O), E=120, 170 MeV; measured σ(θ).
doi: 10.1556/APH.16.2002.1-4.24
2002TR11 Phys.Lett. 541B, 52 (2002) E.Tryggestad, T.Aumann, T.Baumann, D.Bazin, J.R.Beene, Y.Blumenfeld, B.A.Brown, M.Chartier, M.L.Halbert, P.Heckman, J.F.Liang, D.C.Radford, D.Shapira, M.Thoennessen, R.L.Varner Low-Lying Dipole Strength in 20O NUCLEAR REACTIONS 208Pb(18O, 18O'), (20O, 20O'), E=100 MeV/nucleon; measured Eγ, Iγ, (particle)γ-coin following projectile Coulomb excitation. 18,20O deduced levels, J, π, excitation B(E1), B(E2). Comparison with shell model predictions.
doi: 10.1016/S0370-2693(02)02224-4
2001GA18 Nucl.Phys. A682, 363c (2001) A.Galindo-Uribarri, J.Gomez del Campo, J.R.Beene, C.J.Gross, M.L.Halbert, J.F.Liang, S.D.Paul, D.Shapira, D.W.Stracener, R.L.Varner, E.Chavez, M.E.Ortiz Study of Resonant Reactions with Radioactive Ion Beams and Observation of Simultaneous 2p Emission NUCLEAR REACTIONS 1H(17F, pX), E=44 MeV; measured proton spectra, pp-coin, angular correlations, excitation functions. 18Ne deduced two-proton emitting state.
doi: 10.1016/S0375-9474(00)00661-8
2001GO01 Phys.Rev.Lett. 86, 43 (2001) J.Gomez del Campo, A.Galindo-Uribarri, J.R.Beene, C.J.Gross, J.F.Liang, M.L.Halbert, D.W.Stracener, D.Shapira, R.L.Varner, E.Chavez-Lomeli, M.E.Oritz Decay of a Resonance in 18Ne by the Simultaneous Emission of Two Protons NUCLEAR REACTIONS 1H(17F, p), (17F, 2p), E=33, 44 MeV; measured proton spectra, pp-coin, angular correlations, excitation functions. 18Ne level deduced simultaneous two proton decay, resonance partial and total widths. Various decay mechanisms discussed.
doi: 10.1103/PhysRevLett.86.43
2001HE17 Nucl.Phys. A687, 225c (2001) P.Heckman, D.Bazin, J.R.Beene, Y.Blumenfeld, M.J.Chromik, M.L.Halbert, J.F.Liang, E.Mohrmann, T.Nakamura, A.Navin, B.M.Sherrill, K.A.Snover, M.Thoennessen, E.Tryggestad, R.L.Varner Temperature Dependence of the GDR Width in 120Sn NUCLEAR REACTIONS 120Sn(17O, 17O'), E=80 MeV/nucleon; measured Eγ, (recoil)γ-coin, excitation energy spectra, preliminary GDR parameters. Comparison with α-induced reaction data.
doi: 10.1016/S0375-9474(01)00625-X
2001TR10 Nucl.Phys. A687, 231c (2001) E.Tryggestad, T.Aumann, D.Bazin, J.R.Beene, Y.Blumenfeld, M.Chartier, M.L.Halbert, P.Heckman, J.F.Liang, D.C.Radford, D.Shapira, B.M.Sherrill, M.Thoennessen, R.L.Varner Dipole Strength Function in 20O NUCLEAR REACTIONS 208Pb(20O, 20O'), E=100 MeV/nucleon; measured Eγ, (recoil)γ-coin following projectile Coulomb excitation. 20O deduced transitions.
doi: 10.1016/S0375-9474(01)00626-1
2001VA18 Nucl.Phys. A687, 140c (2001) R.L.Varner, J.R.Beene, M.Chartier, J.F.Liang, D.Shapira, D.Bazin, B.Blank, B.Sherrill, M.Thoennessen, P.A.DeYoung, G.F.Peaslee Excitation of the Isovector Giant Quadrupole Resonance in 208Pb by Coulomb Inelastic Scattering NUCLEAR REACTIONS 90Zr, 208Pb(17O, 17O'), (36Ar, 36Ar'), E=150 MeV/nucleon; measured inelastic scattering σ, inelastic excitation yield, isovector giant quadrupole resonance, GDR features.
doi: 10.1016/S0375-9474(01)00613-3
2000GA50 Nucl.Instrum.Methods Phys.Res. B172, 647 (2000) A.Galindo-Uribarri, J.Gomez del Campo, J.R.Beene, C.J.Gross, J.F.Liang, S.D.Paul, D.Shapira, D.W.Stracener, R.L.Varner, E.Chavez, A.Huerta, M.E.Oritz, E.Padilla, S.Pascual Study of Resonant Reactions with Radioactive Ion Beams NUCLEAR REACTIONS 1H(17O, p), E=14, 20, 33 MeV; 1H(17F, p), E=33 MeV; measured recoil proton spectra, σ(E, θ); deduced resonance features. Thick targets.
doi: 10.1016/S0168-583X(00)00220-2
2000GR21 Nucl.Instrum.Methods Phys.Res. A450, 12 (2000) C.J.Gross, T.N.Ginter, D.Shapira, W.T.Milner, J.W.McConnell, A.N.James, J.W.Johnson, J.Mas, P.F.Mantica, R.L.Auble, J.J.Das, J.L.Blankenship, J.H.Hamilton, R.L.Robinson, Y.A.Akovali, C.Baktash, J.C.Batchelder, C.R.Bingham, M.J.Brinkman, H.K.Carter, R.A.Cunningham, T.Davinson, J.D.Fox, A.Galindo-Uribarri, R.Grzywacz, J.F.Liang, B.D.MacDonald, J.MacKenzie, S.D.Paul, A.Piechaczek, D.C.Radford, A.V.Ramayya, W.Reviol, D.Rudolph, K.Rykaczewski, K.S.Toth, W.Weintraub, C.Williams, P.J.Woods, C.-H.Yu, E.F.Zganjar Performance of the Recoil Mass Spectrometer and Its Detector Systems at the Holifield Radioactive Ion Beam Facility
doi: 10.1016/S0168-9002(00)00159-5
2000LI38 Phys.Lett. 491B, 23 (2000) J.F.Liang, J.R.Beene, H.Esbensen, A.Galindo-Uribarri, J.Gomez del Campo, C.J.Gross, M.L.Halbert, P.E.Mueller, D.Shapira, D.W.Stracener, R.L.Varner Breakup of Weakly Bound 17F Well Above the Coulomb Barrier NUCLEAR REACTIONS 208Pb(17F, p16O), E=170 MeV; measured σ, fragments angular correlations, proton spectra; deduced breakup mechanism. Comparison with model predictions.
doi: 10.1016/S0370-2693(00)01016-9
1999KA14 Phys.Rev. C59, 2580 (1999) S.Kailas, D.M.Nadkarni, A.Chatterjee, A.Saxena, S.S.Kapoor, R.Vandenbosch, J.P.Lestone, J.F.Liang, D.J.Prindle, A.A.Sonzogni, J.D.Bierman Fission Fragment Folding Angle Distributions for the Systems 11B + 237Np, 12C + 236U, and 16O + 232Th in the Energy Range 1.1 < E/VB < 2.1 NUCLEAR REACTIONS 232Th(16O, F), E=100-144.8 MeV; 236U(12C, F), E=80-130 MeV; 237Np(11B, F), E=60-118 MeV; measured fission σ, folding angle distributions; deduced momentum transfer components, fission anisotropies. Saddle-point statistical model.
doi: 10.1103/PhysRevC.59.2580
1999LI32 Nucl.Instrum.Methods Phys.Res. A435, 393 (1999) J.F.Liang, D.Shapira, J.R.Beene, J.D.Bierman, A.Galindo-Uribarri, J.Gomez del Campo, C.J.Gross, M.L.Halbert, T.J.Harding, A.I.D.Macnab, S.P.McNeal, R.L.Varner, K.Zhao Detection of Fusion Residues Produced by Inverse Kinematic Reactions using a Gas-Filled Split-Pole Spectrograph NUCLEAR REACTIONS 197Au(70Ge, 70Ge), E=250 MeV; measured charge state distribution. 50Ti(75As, X), E=242, 265 MeV; measured evaporation residues energy, σ(θ). Gas-filled spectrograph, position sensitive detector.
doi: 10.1016/S0168-9002(99)00660-9
1998SO01 Phys.Rev. C57, 722 (1998) A.A.Sonzogni, J.D.Bierman, M.P.Kelly, J.P.Lestone, J.F.Liang, R.Vandenbosch Transfer and Surface Vibration Couplings in the Fusion of 40Ca + 46,48,50Ti at Near-Barrier Energies NUCLEAR REACTIONS 46,48,50Ti(40Ca, X), E=97-150 MeV; measured fusion, quasielastic σ(E, θ); deduced fusion, quasielastic σ(E), barrier distributions, surface vibration coupling parameters. Coupled-channel calculations.
doi: 10.1103/PhysRevC.57.722
1997GO22 J.Phys.(London) G23, 1315 (1997) P.R.S.Gomes, A.M.M.Maciel, R.M.Anjos, S.B.Moraes, R.Liguori Neto, R.Cabezas, C.Muri, G.M.Santos, J.F.Liang Transfer Reactions as a Doorway to Fusion NUCLEAR REACTIONS, ICPND 144Sm(16O, X), E=66 MeV; analyzed one-alpha, two-proton transfer σ(θ); 100Mo(32S, X), E=116 MeV; analyzed one-, two-nucleon transfer σ(θ); 100Mo(32S, X), E(cm)=72-92 MeV; analyzed fusion σ; deduced transfer channels fusion role.
doi: 10.1088/0954-3899/23/10/020
1997KE12 Phys.Rev. C56, 3201 (1997) M.P.Kelly, J.F.Liang, A.A.Sonzogni, K.A.Snover, J.P.S.van Schagen, J.P.Lestone Preequilibrium Particle Emission and the Giant-Dipole Resonance in Sn Nuclei NUCLEAR REACTIONS 100Mo(18O, X), E=200 MeV; measured Eγ, Iγ, (particle)γ-coin, p-, α-spectra; deduced pre-equilibrium emission features. 115In, 118Sn deduced GDR pre-equilibrium emission effects.
doi: 10.1103/PhysRevC.56.3201
1997LI07 Phys.Rev.Lett. 78, 3074 (1997) J.F.Liang, J.D.Bierman, M.P.Kelly, A.A.Sonzogni, R.Vandenbosch, J.P.S.van Schagen Entrance Channel Dependent Light Charged Particle Emission from the 156Er Compound Nucleus NUCLEAR REACTIONS 144Sm(12C, X), E=142 MeV; 96Zr(60Ni, X), E=333 MeV; measured light charged particle energy spectra, (particle)(evaporation residue)-coin. 156Er deduced decay entrance channel dependent features.
doi: 10.1103/PhysRevLett.78.3074
1997LI17 Phys.Rev. C56, 908 (1997) J.F.Liang, J.D.Bierman, M.P.Kelly, A.A.Sonzogni, R.Vandenbosch, J.P.S.van Schagen Dissipative Effects in the Formation of the 156Er Compound Nucleus NUCLEAR REACTIONS 144Sm(12C, X), E=142 MeV; 121Sb(35Cl, X), E=218 MeV; 96Zr(60Ni, X), E=333 MeV; measured E(p), I(p), E(alpha), I(alpha), (light charged particle)(residual nucleus)-coin, compound nucleus formation time scale. 156Er deduced entrance channel dependent features. Statistical model, preequilibrium decay.
doi: 10.1103/PhysRevC.56.908
1997MA60 J.Phys.(London) G23, 1215 (1997) J.C.Mahon, L.L.Lee, Jr., J.F.Liang, C.R.Morton, N.T.P.Bateman, K.Yildiz, B.M.Young Fusion and Transfer in 37Cl + 98,100Mo, 93Nb at Near Barrier Energies NUCLEAR REACTIONS, ICPND 100Mo(37Cl, X), E=118.1, 121.8, 125.1; measured σ(θ) for one-, two-proton stripping; deduced transfer form factors. 93Nb, 92,98,100Mo(37Cl, X), E(cm)=82-95 MeV; 93Nb, 92,98,100Mo(32S, X), E(cm)=78-90 MeV; measured fusion σ; deduced sub-barrier enhancement.
doi: 10.1088/0954-3899/23/10/008
1996BI10 Phys.Rev.Lett. 76, 1587 (1996) J.D.Bierman, P.Chan, J.F.Liang, M.P.Kelly, A.A.Sonzogni, R.Vandenbosch Experimental Fusion Barrier Distributions Reflecting Projectile Octupole State Coupling to Prolate and Oblate Target Nuclei NUCLEAR REACTIONS, ICPND 194Pt(40Ca, X), E(cm) ≈ 160-200 MeV; 192Os(40Ca, X), E(cm) ≈ 150-190 MeV; measured fusion σ(E); deduced targets, projectile deformations role.
doi: 10.1103/PhysRevLett.76.1587
1996BI20 Phys.Rev. C54, 3068 (1996) J.D.Bierman, P.Chan, J.F.Liang, M.P.Kelly, A.A.Sonzogni, R.Vandenbosch Fusion Barrier Distributions for Heavy Ion Systems Involving Prolate and Oblate Target Nuclei NUCLEAR REACTIONS, ICPND 192Os, 194Pt(40Ca, X), E(cm)=160-200 MeV; measured fusion σ(E). 197Au(40Ca, F), E=311, 233 MeV; measured fission fragment σ(θ); deduced fusion barriers.
doi: 10.1103/PhysRevC.54.3068
1996VA12 Phys.Rev. C54, R977 (1996) R.Vandenbosch, J.D.Bierman, J.P.Lestone, J.F.Liang, D.J.Prindle, A.A.Sonzogni, S.Kailas, D.M.Nadkarni, S.S.Kapoor Disappearance of Entrance Channel Dependence of Fission Fragment Anisotropies at Well-Above-Barrier Energies NUCLEAR REACTIONS 237Np(11B, F), E=60-118 MeV; 236U(12C, F), E=80-130 MeV; 232Th(16O, F), E=100-145 MeV; measured fission fragment σ(θ), anisotropies; deduced entrance channel independence.
doi: 10.1103/PhysRevC.54.R977
1994LI25 Phys.Rev. C50, 1550 (1994) J.F.Liang, L.L.Lee, Jr., J.C.Mahon, R.J.Vojtech Transfer Reactions in 32S + 92,98,100Mo and 93Nb at Near Barrier Energies NUCLEAR REACTIONS 92,98,100Mo, 93Nb(32S, X), E=109-125 MeV; measured quasielastic transfer σ(θ); deduced transfer, fusion, reaction σ, transfer probability. Semi-classical model, DWBA analysis.
doi: 10.1103/PhysRevC.50.1550
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