NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = C.L.Jiang Found 128 matches. Showing 1 to 100. [Next]2023JI10 Phys.Rev. C 108, L051604 (2023) C.L.Jiang, W.F.Henning, B.P.Kay, N.Watwood Structures in the heavy-ion fusion excitation function at and above the Coulomb barrier
doi: 10.1103/PhysRevC.108.L051604
2023JI11 Phys.Rev. C 108, L051605 (2023) C.L.Jiang, W.F.Henning, C.R.Hoffman, B.P.Kay, N.Watwood Unexpected character of the heavy-ion fusion excitation function and the compound channel effect
doi: 10.1103/PhysRevC.108.L051605
2022JA08 Phys.Rev. C 105, L042802 (2022) H.Jayatissa, M.L.Avila, K.E.Rehm, R.Talwar, P.Mohr, K.Auranen, J.Chen, D.A.Gorelov, C.R.Hoffman, C.L.Jiang, B.P.Kay, S.A.Kuvin, D.Santiago-Gonzalez First direct measurement of the 13N(α, p)16O reaction relevant for core-collapse supernovae nucleosynthesis NUCLEAR REACTIONS 4He(13N, p), E=34.6 MeV; measured energies and yields of reaction products; deduced σ(Ε) in the range E(cm)=3.26–6.02 MeV, astrophysical S-factor. 4He(13N, p), T=0.8-10.0 GK; deduced astrophysical reaction rates. Comparison to other experimental data, TALYS calculations and data from REACLIB. MUlti-Sampling Ionization Chamber (MUSIC) detector filled with He-Kr gas mixture at ATLAS (ANL).
doi: 10.1103/PhysRevC.105.L042802
2022JI07 Eur.Phys.J. A 58, 72 (2022) A modified-Wong formula for heavy-ion fusion reactions
doi: 10.1140/epja/s10050-022-00703-z
2022JI10 Phys.Rev. C 105, 064601 (2022) Heavy-ion fusion cross section formula and barrier height distribution NUCLEAR REACTIONS 96Zr(40Ca, X), 194Pt(40Ca, X), 154Sm(16O, X), 144Sm(16O, X), 192Os(40Ca, X), 209Bi(11B, X), E not given; analyzed experimental data on σ and excitation functions for several fusioning systems 16O+208Pb, 32S+89Y, 40Ca+40Ca, 40Ca+96Zr, 8Ni+60Ni, 48Ca+48Ca, 40Ca+90Zr, 11Be+209Bi, 40Ca+132Sn, 58Ni+58Ni, 12C+30Si, 24Mg+30Si, 40Ar+112Sn, 40Ar+154Sm, 64Ni+124Sn; deduced excitation function, barrier height distributions, σ(E). The reciprocal of a fusion representation method based on a double integration of a parametrized barrier distribution. Applied three-Gaussian (3G) and a four-Gaussian (4G) description of barrier distribution. Claimed the existence of narrow barrier peak at energies higher than the Coulomb barrier for most fusion systems. Comparison to experimental data.
doi: 10.1103/PhysRevC.105.064601
2022MO25 J.Phys.(London) G49, 095101 (2022) G.Montagnoli, A.M.Stefanini, C.L.Jiang, K.Hagino, F.Niola, D.Brugnara, P.Colovic, G.Colucci, L.Corradi, R.Depalo, E.Fioretto, A.Goasduff, G.Pasqualato, F.Scarlassara, S.Szilner, I.Zanon Fusion of 12C + 24Mg at extreme sub-barrier energies NUCLEAR REACTIONS 12C(24Mg, X), E=25.5-48 MeV; measured reaction products, TOF; deduced evaporation residue σ(θ), fusion σ. Comparison with calculations. The XTU Tandem Van de Graaff accelerator at Laboratori Nazionali di Legnaro (LNL) of INFN.
doi: 10.1088/1361-6471/ac7edd
2021JI09 Eur.Phys.J. A 57, 235 (2021), Erratum Eur.Phys.J. A 59, 84 (2023) C.L.Jiang, B.B.Back, K.E.Rehm, K.Hagino, G.Montagnoli, A.M.Stefanini Heavy-ion fusion reactions at extreme sub-barrier energies NUCLEAR REACTIONS 64Ni(64Ni, X), E=82-102 MeV; 90Zr(90Zr, X), E=340-400 MeV; 89Y(58Ni, X), E=200-260 MeV; 24Mg, 30Si(12C, X), E=8-20 MeV; 10B(10B, X), 16O(16O, X), E<20 MeV; analyzed available data; deduced fusion barriers, the fusion hindrance effect with analytical forms of the barrier-height distributions or a modified version of the classic Wong formula.
doi: 10.1140/epja/s10050-021-00536-2
2020HA03 Phys.Rev. C 101, 015804 (2020) M.R.Hall, D.W.Bardayan, T.Baugher, A.Lepailleur, S.D.Pain, A.Ratkiewicz, S.Ahn, J.M.Allen, J.T.Anderson, A.D.Ayangeakaa, J.C.Blackmon, S.Burcher, M.P.Carpenter, S.M.Cha, K.Y.Chae, K.A.Chipps, J.A.Cizewski, M.Febbraro, O.Hall, J.Hu, C.L.Jiang, K.L.Jones, E.J.Lee, P.D.O'Malley, S.Ota, B.C.Rasco, D.Santiago-Gonzalez, D.Seweryniak, H.Sims, K.Smith, W.P.Tan, P.Thompson, C.Thornsberry, R.L.Varner, D.Walter, G.L.Wilson, S.Zhu γ-ray spectroscopy of astrophysically important states in 39Ca NUCLEAR REACTIONS 40Ca(3He, αγ)39Ca, E=30 MeV; Measured Eγ, Iγ, Eα, Iα, αγ-coin, reaction products using the GODDESS array (Gammasphere for γ detection and ORRUBA for particle detection) at the ATLAS-ANL facility. 39Ca; deduced levels, J, π, γ-branching ratios. 38K(p, γ)39Ca, T=0.1-0.4 GK; deduced resonance parameters, astrophysical reaction rates. Discussed impact on abundances of isotopes created at the endpoint of nova nucleosynthesis.
doi: 10.1103/PhysRevC.101.015804
2020HA31 Phys.Rev. C 102, 045802 (2020) M.R.Hall, D.W.Bardayan, T.Baugher, A.Lepailleur, S.D.Pain, A.Ratkiewicz, S.Ahn, J.M.Allen, J.T.Anderson, A.D.Ayangeakaa, J.C.Blackmon, S.Burcher, M.P.Carpenter, S.M.Cha, K.Y.Chae, K.A.Chipps, J.A.Cizewski, M.Febbraro, O.Hall, J.Hu, C.L.Jiang, K.L.Jones, E.J.Lee, P.D.O'Malley, S.Ota, B.C.Rasco, D.Santiago-Gonzalez, D.Seweryniak, H.Sims, K.Smith, W.P.Tan, P.Thompson, C.Thornsberry, R.L.Varner, D.Walter, G.L.Wilson, S.Zhu 19Ne level structure for explosive nucleosynthesis NUCLEAR REACTIONS 19F(3He, t)19Ne, E=30 MeV; measured reaction products, E(t), I(t), Eγ, Iγ, (triton)γ-, and (triton)γγ-coin using ORRUBA array with Micron QQQ5 telescopes for tritons and Gammasphere array for γ rays at ATLAS-ANL facility. 19Ne; deduced levels, J, π, γ-branching ratios. Comparison with earlier experimental results and with evaluated data. 18F(p, α)15O, E(cm)<0.9 MeV; calculated astrophysical S factors, and reaction rates at temperature of 0.06 to 0.4 GK.
doi: 10.1103/PhysRevC.102.045802
2020MO18 Phys.Rev. C 101, 044608 (2020) G.Montagnoli, A.M.Stefanini, C.L.Jiang, G.Colucci, S.Bottoni, D.Brugnara, P.Colovic, L.Corradi, E.Fioretto, F.Galtarossa, A.Goasduff, O.S.Khwairakpam, M.Heine, G.Jaworski, M.Mazzocco, T.Mijatovic, M.Siciliano, F.Scarlassara, S.Szilner, T.Van Patten, I.Zanon Fusion of 12C + 24Mg far below the barrier: Evidence for the hindrance effect NUCLEAR REACTIONS 12C(24Mg, X), E=26-52 MeV; measured evaporation residues (ERs), fusion σ(E) using E-ΔE and time-of-flight telescope for detection of ERs at LNL-Legnaro; deduced S factor, influence of inelastic channels on fusion, hindrance effect with energy threshold. Comparison with coupled channels calculations using the CCFULL code and Woods Saxon (WS) internuclear potential, and with systematics of energy threshold of hindrance for other medium-light systems: 12C+12C, 12C+16O, 16O+16O, 12C+30Si, 24Mg+30Si, 28Si+30Si, 16O+76Ge, and 27Al+45Sc. Discussed astrophysical significance of reactions in the carbon and oxygen burning stages of heavy stars.
doi: 10.1103/PhysRevC.101.044608
2019HA08 Phys.Rev.Lett. 122, 052701 (2019) M.R.Hall, D.W.Bardayan, T.Baugher, A.Lepailleur, S.D.Pain, A.Ratkiewicz, S.Ahn, J.M.Allen, J.T.Anderson, A.D.Ayangeakaa, J.C.Blackmon, S.Burcher, M.P.Carpenter, S.M.Cha, K.Y.Chae, K.A.Chipps, J.A.Cizewski, M.Febbraro, O.Hall, J.Hu, C.L.Jiang, K.L.Jones, E.J.Lee, P.D.O'Malley, S.Ota, B.C.Rasco, D.Santiago-Gonzalez, D.Seweryniak, H.Sims, K.Smith, W.P.Tan, P.Thompson, C.Thornsberry, R.L.Varner, D.Walter, G.L.Wilson, S.Zhu Key 19Ne States Identified Affecting γ-Ray Emission from 18F in Novae NUCLEAR REACTIONS 19F(3He, t)19Ne, E=30 MeV; measured reaction products, Eγ, Iγ; deduced γ-ray energies, J, π, S-factor, reaction rates, resonance energies. Comparison with available data.
doi: 10.1103/PhysRevLett.122.052701
2019HA14 Phys.Rev. C 99, 035805 (2019) M.R.Hall, D.W.Bardayan, T.Baugher, A.Lepailleur, S.D.Pain, A.Ratkiewicz, S.Ahn, J.M.Allen, J.T.Anderson, A.D.Ayangeakaa, J.C.Blackmon, S.Burcher, M.P.Carpenter, S.M.Cha, K.Y.Chae, K.A.Chipps, J.A.Cizewski, M.Febbraro, O.Hall, J.Hu, C.L.Jiang, K.L.Jones, E.J.Lee, P.D.O'Malley, S.Ota, B.C.Rasco, D.Santiago-Gonzalez, D.Seweryniak, H.Sims, K.Smith, W.P.Tan, P.Thompson, C.Thornsberry, R.L.Varner, D.Walter, G.L.Wilson, S.Zhu New γ-ray transitions observed in 19Ne with implications for the 15O(α, γ)19Ne reaction rate NUCLEAR REACTIONS 19F(3He, t), E=30 MeV; measured triton spectra, Eγ, Iγ, tγ- and γγ-coin using Gammasphere array for γ detection with the silicon detector array ORRUBA Dual Detectors for Experimental Structure Studies (GODDESS) at ATLAS-ANL facility. 19Ne; deduced levels, J, π, and γ-branching ratios for the decay of 4.14- and 4.20-MeV states. 15O(α, γ)19Ne, E≈18-180 keV; calculated fractional contribution of the corrected branching ratios for the 4.14 MeV, 7/2- and 4.20 MeV, 9/2- states in 19Ne to astrophysical reaction rate, which is of significance in breakout from the hot CNO cycle in type I x-ray bursts. Comparison with previous experimental values.
doi: 10.1103/PhysRevC.99.035805
2019PA57 Nucl.Instrum.Methods Phys.Res. B438, 172 (2019) R.C.Pardo, T.Palchan-Hazan, R.Scott, M.Paul, O.Nusair, W.Bauder, R.Vondrasek, D.Seweryniak, S.Baker, R.Talwar, P.Collon, F.G.Kondev, G.Youinou, M.Salvatores, G.Palmiotti, J.Berg, J.Giglio, M.T.Giglio, G.Imel, C.Nair, C.L.Jiang Laser Ablation Positive-Ion AMS of Neutron Activated Actinides NUCLEAR REACTIONS 236U, 242Pu(n, X), E not given; measured reaction products; deduced neutron transmutation rates by accelerator mass spectrometry.
doi: 10.1016/j.nimb.2018.05.004
2018AS03 Nucl.Instrum.Methods Phys.Res. A899, 6 (2018) B.W.Asher, S.Almaraz-Calderon, O.Nusair, K.E.Rehm, M.L.Avila, A.A.Chen, C.A.Dickerson, C.L.Jiang, B.P.Kay, R.C.Pardo, D.Santiago-Gonzalez, R.Talwar Development of an Isomeric beam of 26Al for nuclear reaction studies NUCLEAR REACTIONS 1H(26Mg, 26Al), E=158.5 MeV; measured reaction products, Eγ, Iγ. 26mAl; deduced σ. Comparison with available data.
doi: 10.1016/j.nima.2018.05.015
2018JI01 Phys.Rev. C 97, 012801 (2018) C.L.Jiang, D.Santiago-Gonzalez, S.Almaraz-Calderon, K.E.Rehm, B.B.Back, K.Auranen, M.L.Avila, A.D.Ayangeakaa, S.Bottoni, M.P.Carpenter, C.Dickerson, B.DiGiovine, J.P.Greene, C.R.Hoffman, R.V.F.Janssens, B.P.Kay, S.A.Kuvin, T.Lauritsen, R.C.Pardo, J.Sethi, D.Seweryniak, R.Talwar, C.Ugalde, S.Zhu, D.Bourgin, S.Courtin, F.Haas, M.Heine, G.Fruet, D.Montanari, D.G.Jenkins, L.Morris, A.Lefebvre-Schuhl, M.Alcorta, X.Fang, X.D.Tang, B.Bucher, C.M.Deibel, S.T.Marley Reaction rate for carbon burning in massive stars NUCLEAR REACTIONS 12C(12C, p)23Na, (12C, α)20Ne, E=5.5-10 MeV; measured Eγ, Iγ, (particle)γ-coin, σ(E) using Gammasphere array and an array of three annular double-sided silicon strip detectors at the ATLAS-ANL facility; deduced S factors and astrophysical reaction rates. Comparison with previous measurements, and with data from other reactions. Relevance to carbon burning is a critical phase for nucleosynthesis in massive stars.
doi: 10.1103/PhysRevC.97.012801
2018JI11 Eur.Phys.J. A 54, 218 (2018) C.L.Jiang, K.E.Rehm, B.B.Back, A.M.Stefanini, G.Montagnoli Reproducing heavy-ion fusion cross sections at extreme sub-barrier energies with a simple formula NUCLEAR REACTIONS 18O(16O, x), E=6-20 MeV; 30Si(12C, x), E=9-30 MeV;30Si(24Mg, x), E=16-32 MeV; 64Ni(28Si, x), E=44-70 MeV;64Ni(28Si, x), E=44-70 MeV;64Ni(64Ni, x), E=80-110 MeV; 124Sn(64Ni, x), E not given; 144,154Sm(16O, x), E=50-80 MeV; 197Au(11B, x), E=38-64 MeV; 208Pb(16O, x), E=64-110 MeV; calculated fusion σ(E), astrophysical S-factor vs E using simple Siwek-Wilczynski formula based on single-Gaussian distribution of fusion barrier heights; deduced parameters Rg, Vg and Wg as functions of the Coulomb barrier. Results compared to the data. Enclosed table brings results of more reaction than those named here.
doi: 10.1140/epja/i2018-12655-6
2018MO05 Phys.Rev. C 97, 024610 (2018) G.Montagnoli, A.M.Stefanini, C.L.Jiang, K.Hagino, F.Galtarossa, G.Colucci, S.Bottoni, C.Broggini, A.Caciolli, P.Colovic, L.Corradi, S.Courtin, R.Depalo, E.Fioretto, G.Fruet, A.Gal, A.Goasduff, M.Heine, S.P.Hu, M.Kaur, T.Mijatovic, M.Mazzocco, D.Montanari, F.Scarlassara, E.Strano, S.Szilner, G.X.Zhang Fusion hindrance for the positive Q-value system 12C+30Si NUCLEAR REACTIONS 12C(30Si, X), E=34-80 MeV; measured reaction products, fusion σ(E) at the XTU Tandem accelerator of INFN-LN, Legnaro. Comparison with coupled-channel calculations using Woods Saxon (WS) and Yukawa-plus-exponential (YPE) potentials.
doi: 10.1103/PhysRevC.97.024610
2018SA13 Phys.Rev.Lett. 120, 122503 (2018) D.Santiago-Gonzalez, K.Auranen, M.L.Avila, A.D.Ayangeakaa, B.B.Back, S.Bottoni, M.P.Carpenter, J.Chen, C.M.Deibel, A.A.Hood, C.R.Hoffman, R.V.F.Janssens, C.L.Jiang, B.P.Kay, S.A.Kuvin, A.Lauer, J.P.Schiffer, J.Sethi, R.Talwar, I.Wiedenhover, J.Winkelbauer, S.Zhu Probing the Single-Particle Character of Rotational States in 19F Using a Short-Lived Isomeric Beam NUCLEAR REACTIONS 2H(18F, p), E=14 MeV/nucleon; measured reaction products, Ep, Ip. 19F; deduced energy levels, J, π, relative spectroscopic factors, rotational band. Comparison with shell-model calculations.
doi: 10.1103/PhysRevLett.120.122503
2018TA12 Phys.Rev. C 97, 055801 (2018) R.Talwar, M.J.Bojazi, P.Mohr, K.Auranen, M.L.Avila, A.D.Ayangeakaa, J.Harker, C.R.Hoffman, C.L.Jiang, S.A.Kuvin, B.S.Meyer, K.E.Rehm, D.Santiago-Gonzalez, J.Sethi, C.Ugalde, J.R.Winkelbauer Experimental study of 38Ar + α reaction cross sections relevant to the 41Ca abundance in the solar system NUCLEAR REACTIONS 4He(38Ar, p), (38Ar, n), (38Ar, α'), E=133 MeV; measured energies and yields of reaction products, energy- and angle integrated σ(E) using multisampling ionization chamber (MUSIC) detector at the ATLAS-ANL facility. Comparison with previous experimental values, and with statistical model calculations using TALYS code. 41K(p, α)38Ar, 41Ca(n, α)38Ar, T=0.1-10.0 GK; deduced astrophysical reaction rates, and compared with statistical model calculations, and with REACLIB fits. Discussed relevance to 41Ca abundance in the solar system.
doi: 10.1103/PhysRevC.97.055801
2017AL29 Phys.Rev.Lett. 119, 072701 (2017) S.Almaraz-Calderon, K.E.Rehm, N.Gerken, M.L.Avila, B.P.Kay, R.Talwar, A.D.Ayangeakaa, S.Bottoni, A.A.Chen, C.M.Deibel, C.Dickerson, K.Hanselman, C.R.Hoffman, C.L.Jiang, S.A.Kuvin, O.Nusair, R.C.Pardo, D.Santiago-Gonzalez, J.Sethi, C.Ugalde Study of the 26Alm(d, p)27Al Reaction and the Influence of the 26Al 0+ Isomer on the Destruction of 26Al in the Galaxy NUCLEAR REACTIONS C, 2H(26Al, p), E=120 MeV; measured reaction products, Eγ, Iγ. 26Al; deduced σ(θ), reaction rates. Comparison with available data, DWBA calculations.
doi: 10.1103/PhysRevLett.119.072701
2017AV03 Nucl.Instrum.Methods Phys.Res. A859, 63 (2017) M.L.Avila, K.E.Rehm, S.Almaraz-Calderon, A.D.Ayangeakaa, C.Dickerson, C.R.Hoffman, C.L.Jiang, B.P.Kay, J.Lai, O.Nusair, R.C.Pardo, D.Santiago-Gonzalez, R.Talwar, C.Ugalde Study of (α, p) and (α, n) reactions with a Multi-Sampling Ionization Chamber NUCLEAR REACTIONS 4He(17O, n), (17O, α'), E=34.8 MeV; 4He(23Na, α), (23Na, p), E=51.5, 57.4 MeV; measured reaction products, Eα, Iα, Ep, Ip; deduced σ. Comparison with available data.
doi: 10.1016/j.nima.2017.03.060
2016AV06 Phys.Rev. C 94, 065804 (2016) M.L.Avila, K.E.Rehm, S.Almaraz-Calderon, A.D.Ayangeakaa, C.Dickerson, C.R.Hoffman, C.L.Jiang, B.P.Kay, J.Lai, O.Nusair, R.C.Pardo, D.Santiago-Gonzalez, R.Talwar, C.Ugalde Experimental study of the astrophysically important 23Na(α, p)26Mg and 23Na(α, n)26Al reactions NUCLEAR REACTIONS 4He(23Na, p), (23Na, n), E=51.5, 57.4 MeV; measured particle spectra, and cross section using multisampling ionization chamber (MUSIC) detector at ATLAS-ANL facility. Comparison with previous measurements, NACRE compilation, and with statistical-model calculations. Technique to measure simultaneously excitation functions of angle- and excitation energy-integrated cross sections of (α, p) and (α, n) reactions. Relevance to 26Al production in massive stars.
doi: 10.1103/PhysRevC.94.065804
2016MU05 Phys.Rev. C 93, 065502 (2016) H.P.Mumm, M.G.Huber, W.Bauder, N.Abrams, C.M.Deibel, C.R.Huffer, P.R.Huffman, K.W.Schelhammer, R.Janssens, C.L.Jiang, R.H.Scott, R.C.Pardo, K.E.Rehm, R.Vondrasek, C.M.Swank, C.M.O'Shaughnessy, M.Paul, L.Yang High-sensitivity measurement of 3He - 4He isotopic ratios for ultracold neutron experiments ATOMIC MASSES 3,4He; measured absolute isotopic ratio of 3He to 4He with a high sensitivity at ATLAS-ANL facility. Relevance to neutron half-life measurements using ultra-cold neutrons.
doi: 10.1103/PhysRevC.93.065502
2016MU06 Phys.Rev. C 93, 065803 (2016) M.Munch, M.Alcorta, H.O.U.Fynbo, M.Albers, S.Almaraz-Calderon, M.L.Avila, A.D.Ayangeakaa, B.B.Back, P.F.Bertone, P.F.F.Carnelli, M.P.Carpenter, C.J.Chiara, J.A.Clark, B.DiGiovine, J.P.Greene, J.L.Harker, C.R.Hoffman, N.J.Hubbard, C.L.Jiang, O.S.Kirsebom, T.Lauritsen, K.L.Laursen, S.T.Marley, C.Nair, O.Nusair, D.Santiago-Gonzalez, J.Sethi, D.Seweryniak, R.Talwar, C.Ugalde, S.Zhu Independent measurement of the Hoyle state β feeding from 12B using Gammasphere RADIOACTIVITY 12B(β-)[from 2H(11B, p), E=40 MeV from ATLAS-ANL facility]; measured Eγ, Iγ, γγ-coin, γγ(θ) for the Hoyle state using Gammasphere array. 12C; deduced first excited 2+ and 0+ levels, β branching ratio to the Hoyle state in 12C, logft, indication of higher clustering for the Hoyle state as compared to previous results. Comparison with theoretical calculations using antisymmetrized molecular dynamics (AMD), and with previous experimental results.
doi: 10.1103/PhysRevC.93.065803
2016RE17 Phys.Rev. C 94, 044612 (2016) K.E.Rehm, H.Esbensen, C.L.Jiang, B.B.Back, A.M.Stefanini, G.Montagnoli Moments of fusion-barrier distributions NUCLEAR REACTIONS 40,48Ca, 58,64Ni, 90,96Zr(40Ca, X), 40,48Ca, 90,96Zr(48Ca, X), 48Ca, 58,64Ni, 90,96Zr, 110Pd(32S, X), 48Ca, 64Ni, 90,96Zr, 110Pd(36S, X), 58,64Ni, 132Sn(58Ni, X), 144,148,154Sm, 186W(16O, X), 154Sm(28Si, X), 232Th(15C, X), 209Bi(6He, X), E=85-200 MeV; analyzed fusion radius parameter, moments M1, M2 and M3 of fusion barrier distributions using a new method.
doi: 10.1103/PhysRevC.94.044612
2015JI05 Phys.Rev. C 91, 044602 (2015) C.L.Jiang, A.M.Stefanini, H.Esbensen, K.E.Rehm, S.Almaraz-Calderon, M.L.Avila, B.B.Back, D.Bourgin, L.Corradi, S.Courtin, E.Fioretto, F.Galtarossa, A.Goasduff, F.Haas, M.M.Mazzocco, D.Montanari, G.Montagnoli, T.Mijatovic, R.Sagaidak, D.Santiago-Gonzalez, F.Scarlassara, E.E.Strano, S.Szilner Fusion reactions of 58, 64Ni+124Sn NUCLEAR REACTIONS 124Sn(58Ni, X), (64Ni, X), E(cm)=140-165 MeV; measured evaporation residue spectra, fusion σ(E), σ(θ). Coupled-channels calculations to study reaction mechanism. Discussed role of transfer reactions in heavy system, and S-factor maximum. Comparison with previous experimental results.
doi: 10.1103/PhysRevC.91.044602
2015MO08 Phys.Lett. B 746, 300 (2015) G.Montagnoli, A.M.Stefanini, H.Esbensen, L.Corradi, S.Courtin, E.Fioretto, J.Grebosz, F.Haas, H.M.Jia, C.L.Jiang, M.Mazzocco, C.Michelagnoli, T.Mijatovic, D.Montanari, C.Parascandolo, F.Scarlassara, E.Strano, S.Szilner, D.Torresi Oscillations above the barrier in the fusion of 28Si + 28Si NUCLEAR REACTIONS 28Si(28Si, X), E=62-78 MeV; measured fusion evaporation residues; deduced fusion σ. Comparison with coupled-channel model using the shallow M3Y + repulsion potential.
doi: 10.1016/j.physletb.2015.05.021
2014AL06 Phys.Rev.Lett. 112, 152701 (2014) S.Almaraz-Calderon, P.F.Bertone, M.Alcorta, M.Albers, C.M.Deibel, C.R.Hoffman, C.L.Jiang, S.T.Marley, K.E.Rehm, C.Ugalde Direct Measurement of the 23Na(α, p)26Mg Reaction Cross Section at Energies Relevant for the Production of Galactic 26Al NUCLEAR REACTIONS 4He(23Na, p)26Mg, E=23, 26, 28, 30 MeV; measured reaction products, Ep, Ip; deduced σ, reaction rates. Comparison with available data.
doi: 10.1103/PhysRevLett.112.152701
2014CA08 Phys.Rev.Lett. 112, 192701 (2014) P.F.F.Carnelli, S.Almaraz-Calderon, K.E.Rehm, M.Albers, M.Alcorta, P.F.Bertone, B.Digiovine, H.Esbensen, J.O.Fernandez Niello, D.Henderson, C.L.Jiang, J.Lai, S.T.Marley, O.Nusair, T.Palchan-Hazan, R.C.Pardo, M.Paul, C.Ugalde Measurements of Fusion Reactions of Low-Intensity Radioactive Carbon Beams on 12C and their Implications for the Understanding of X-Ray Bursts NUCLEAR REACTIONS 12C(10C, X), (12C, X), (13C, X), (14C, X), (15C, X), E=40-50 MeV; measured fusion reaction products; deduced S-factors, σ. Time-dependent HF calculations.
doi: 10.1103/PhysRevLett.112.192701
2014JI02 Phys.Rev. C 89, 051603 (2014) C.L.Jiang, K.E.Rehm, B.B.Back, H.Esbensen, R.V.F.Janssens, A.M.Stefanini, G.Montagnoli Influence of heavy-ion transfer on fusion reactions NUCLEAR REACTIONS 40,48Ca(40Ca, X), 48Ca(48Ca, X), E=45-65 MeV; 58,64Ni(28Si, X), 64Ni(30Si, X), E=42-66 MeV; 40,48Ca(32S, X), 48Ca(36S, X), E=36-56 MeV; 58,64Ni(58Ni, X), 64Ni(64Ni, X), E=85-114 MeV; 124,132Sn(40Ca, X), 132Sn(48Ca, X), E=104-138 MeV; 124,132Sn(58Ni, X), 132Sn(64Ni, X), E=145-200 MeV; analyzed fusion σ(E) using Wong formula; calculated average excitation energies of residual nuclei following neutron pickup reactions; deduced correlation between fusion enhancement and strength of total neutron-transfer cross sections.
doi: 10.1103/PhysRevC.89.051603
2014JI04 Phys.Rev.Lett. 113, 022701 (2014) C.L.Jiang, A.M.Stefanini, H.Esbensen, K.E.Rehm, S.Almaraz-Calderon, B.B.Back, L.Corradi, E.Fioretto, G.Montagnoli, F.Scarlassara, D.Montanari, S.Courtin, D.Bourgin, F.Haas, A.Goasduff, S.Szilner, T.Mijatovic Fusion Hindrance for a Positive-Q-Value System 24Mg + 30Si NUCLEAR REACTIONS 30Si(24Mg, X), E<30 MeV; measured fusion reaction products; deduced σ, S-factors.
doi: 10.1103/PhysRevLett.113.022701
2014MO33 Phys.Rev. C 90, 044608 (2014) G.Montagnoli, A.M.Stefanini, H.Esbensen, C.L.Jiang, L.Corradi, S.Courtin, E.Fioretto, J.Grebosz, F.Haas, H.M.Jia, M.Mazzocco, C.Michelagnoli, T.Mijatovic, D.Montanari, C.Parascandolo, F.Scarlassara, E.Strano, S.Szilner, D.Torresi Fusion of 28Si + 28, 30 Different trends at sub-barrier energies NUCLEAR REACTIONS 28,30Si(28Si, X), E=46-86 MeV; measured particle spectra, fusion σ(E), fragment energy and angular distributions using an electrostatic beam separator at INFN-LNL's XTU Tandem accelerator facility; deduced logarithmic derivatives, S-factors, double-phonon excitations, influence of transfer channels and nuclear deformation. Comparison with coupled channel calculations using various potentials.
doi: 10.1103/PhysRevC.90.044608
2013JI01 Phys.Rev.Lett. 110, 072701 (2013) C.L.Jiang, B.B.Back, H.Esbensen, R.V.F.Janssens, K.E.Rehm, R.J.Charity Origin and Consequences of 12C+12C Fusion Resonances at Deep Sub-barrier Energies NUCLEAR REACTIONS 12C(12C, X)24Mg, 12C(13C, X)25Mg, 13C(13C, X)26Mg, 12C(16O, X)28Si, 16O(16O, X)32S, E(cm)<10 MeV; analyzed available fusion σ, S-factors; deduced resonance behavior of fusion reactions at low energies.
doi: 10.1103/PhysRevLett.110.072701
2013MO01 Phys.Rev. C 87, 014611 (2013) G.Montagnoli, A.M.Stefanini, H.Esbensen, C.L.Jiang, L.Corradi, S.Courtin, E.Fioretto, A.Goasduff, J.Grebosz, F.Haas, M.Mazzocco, C.Michelagnoli, T.Mijatovic, D.Montanari, C.Parascandolo, K.E.Rehm, F.Scarlassara, S.Szilner, X.D.Tang, C.A.Ur Effects of transfer channels on near- and sub-barrier fusion of 32S + 48Ca NUCLEAR REACTIONS 48Ca(32S, X), E=60.0-89.4 MeV; measured reaction products, σ(θ, E), fusion σ(E) at Legnaro facility; deduced logarithmic slope. 48Ca(32S, X), (36S, X), E(cm)=35-60 MeV; analyzed fusion σ(E) data, energy-weighted fusion cross sections, astrophysical S factor. Coupled channel analysis with M3Y+repulsion, double-folding potential.
doi: 10.1103/PhysRevC.87.014611
2013ST14 Eur.Phys.J. A 49, 63 (2013) A.M.Stefanini, G.Montagnoli, F.Scarlassara, C.L.Jiang, H.Esbensen, E.Fioretto, L.Corradi, B.B.Back, C.M.Deibel, B.Di Giovine, J.P.Greene, H.D.Henderson, S.T.Marley, M.Notani, N.Patel, K.E.Rehm, D.Sewerinyak, X.D.Tang, C.Ugalde, S.Zhu Fusion of 60Ni + 100Mo near and below the Coulomb barrier - Multi-phonon and transfer couplings down to the hindrance region NUCLEAR REACTIONS 100Mo(60Ni, X), (64Ni, X), E=196-262 MeV; measured particle tracks; deduced fusion σ, logarithmic excitation function slope; calculated fusion σ using CCFULL CC code.
doi: 10.1140/epja/i2013-13063-2
2012KI16 Science 335, 1614 (2012) N.Kinoshita, M.Paul, Y.Kashiv, P.Collon, C.M.Deibel, B.DiGiovine, J.P.Greene, D.J.Henderson, C.L.Jiang, S.T.Marley, T.Nakanishi, R.C.Pardo, K.E.Rehm, D.Robertson, R.Scott, C.Schmitt, X.D.Tang, R.Vondrasek, A.Yokoyama A Shorter 146Sm Half-Life Measured and Implications for 146Sm-142Nd Chronology in the Solar System RADIOACTIVITY 146Sm(α); measured decay products, Eα, Iα; deduced T1/2 and its uncertainty and 146Sm/144Sm ratio. 146Sm - 142Nd clock, comparison with available data.
doi: 10.1126/science.1215510
2012MO05 Phys.Rev. C 85, 024607 (2012) G.Montagnoli, A.M.Stefanini, C.L.Jiang, H.Esbensen, L.Corradi, S.Courtin, E.Fioretto, A.Goasduff, F.Haas, A.F.Kifle, C.Michelagnoli, D.Montanari, T.Mijatovic, K.E.Rehm, R.Silvestri, PushpendraP.Singh, F.Scarlassara, S.Szilner, X.D.Tang, C.A.Ur Fusion of 40Ca+40Ca and other Ca+Ca systems near and below the barrier NUCLEAR REACTIONS 40Ca(40Ca, X), E=98-130 MeV; measured evaporation residue spectra, σ(E); deduced barrier distribution, astrophysical S factor. 48Ca(48Ca, X), E(cm)=45-70 MeV; analyzed fusion σ(E), barrier distributions. Comparison with previous experimental data and with coupled-channel calculations based on Woods-Saxon (WS), M3Y+repulsion potentials.
doi: 10.1103/PhysRevC.85.024607
2012NO01 Phys.Rev. C 85, 014607 (2012) M.Notani, H.Esbensen, X.Fang, B.Bucher, P.Davies, C.L.Jiang, L.Lamm, C.J.Lin, C.Ma, E.Martin, K.E.Rehm, W.P.Tan, S.Thomas, X.D.Tang, E.Brown Correlation between the 12C+12C, 12C+13C, and 13C+13C fusion cross sections NUCLEAR REACTIONS 12C(13C, p)24Na, 13C(13C, np)24Na, E(cm)=2.6-4.8 MeV; measured Eγ, Iγ, βγ-coin from 24Na decay; deduced thick target yield by activation method, GEANT4 simulation, fusion cross section, S factors. 12C(12C, X), (13C, X), 13C(13C, X), E(cm)=2.5-6.5 MeV; analyzed fusion cross sections, fusion barrier parameters, spectroscopic factors by fitting with Wong formula. Comparison of experimental data with two coupled-channels calculations using ingoing wave boundary condition (IWBC).
doi: 10.1103/PhysRevC.85.014607
2012TA13 J.Phys.:Conf.Ser. 337, 012016 (2012) X.D.Tang, X.Fang, B.Bucher, H.Esbensen, C.L.Jiang, K.E.Rehm, C.J.Lin Upper Limit on the molecular resonance strengths in the 12C+ 12C fusion reaction NUCLEAR REACTIONS 12,13C(12C, X), (13C, X), E(cm)=2-6.5 MeV; analyzed published data on fusion reaction S-factor; deduced average S-factor, resonances, upper limit for molecular resonance strengths, empirical relationship using CRC-AW and EWS (equivalent square well).
doi: 10.1088/1742-6596/337/1/012016
2012TA24 J.Phys.:Conf.Ser. 381, 012120 (2012) X.D.Tang, H.Esbensen, X.Fang, B.Bucher, C.L.Jiang, K.E.Rehm, C.J.Lin, E.Brown Does the 12C+12C fusion reaction trigger superburst? NUCLEAR REACTIONS 12C(12C, X), (13C, X), E(cm)≈2.0-6.5 MeV;13C(13C, X), E(cm)≈2.9-6.5 MeV; calculated fusion reaction rate, modified S-factor using CC with IWBC (incoming wave boundary condition) and different interactions. Discussed role of possible resonance near E(cm)≈1.5 MeV.
doi: 10.1088/1742-6596/381/1/012120
2011AL09 Phys.Rev.Lett. 106, 172701 (2011) M.Alcorta, K.E.Rehm, B.B.Back, S.Bedoor, P.F.Bertone, C.M.Deibel, B.DiGiovine, H.Esbensen, J.P.Greene, C.R.Hoffmann, C.L.Jiang, J.C.Lighthall, S.T.Marley, R.C.Pardo, M.Paul, A.M.Rogers, C.Ugalde, A.H.Wuosmaa Fusion Reactions with the One-Neutron Halo Nucleus 15C NUCLEAR REACTIONS 232Th(13C, X), (14C, X), (15C, X), E(cm)=50-70 MeV; measured fusion fission fragments; deduced yields, σ, 15C+232Th cross section enhancement. Comparison with experimental data, couple-channel calculations.
doi: 10.1103/PhysRevLett.106.172701
2011DE28 Phys.Rev. C 84, 045802 (2011) C.M.Deibel, K.E.Rehm, J.M.Figueira, J.P.Greene, C.L.Jiang, B.P.Kay, H.Y.Lee, J.C.Lighthall, S.T.Marley, R.C.Pardo, N.Patel, M.Paul, C.Ugalde, A.Woodard, A.H.Wuosmaa, G.Zinkann First measurement of the 33Cl(p, α)30S reaction NUCLEAR REACTIONS 1H(33Cl, α)30S, [33Cl secondary beam from 2H(32S, 33Cl), E=320 MeV primary reaction], E=208.1, 229.1, 250.6 MeV; measured Eα, Iα, particle spectra, (30S)α-coin; deduced cross sections. Enge split-pole magnetic spectrograph. Comparison of measured σ with NON-SMOKER code calculations.
doi: 10.1103/PhysRevC.84.045802
2011ES08 Phys.Rev. C 84, 064613 (2011) Effects of mutual excitations in the fusion of carbon isotopes NUCLEAR REACTIONS 13C(13C, X), E(cm)=0-18 MeV; 13C(12C, X), E(cm)=2-7 MeV; 12C(12C, X), E(cm)=1-9 MeV; calculated fusion cross section, S factors. Coupled-channels calculations based on the M3Y+repulsion, double-folding potential. Comparison with experimental data.
doi: 10.1103/PhysRevC.84.064613
2011JI14 J.Phys.:Conf.Ser. 312, 042011 (2011) C.L.Jiang, B.B.Back, H.Esbensen, R.V.F.Janssens, K.E.Rehm, X.D.Tang Do we understand heavy-ion fusion reactions of importance in stellar evolution? NUCLEAR REACTIONS 10B(10B, X), E≈0.9-3.5 MeV;16O(16O, X), E≈5.5-11.5 MeV;30Si(28Si, X), E≈23-30 MeV;48Ca(36S, X), E≈36-48 MeV;48Ca(40Ca, X), E≈46-56 MeV;48Ca(48Ca, X), E≈46-56 MeV;45Sc(27Al, X), E≈31=39 MeV;64Ni(28Si, X), E≈43-52 MeV;64Ni(64Ni, X), E≈84-100 MeV;92Zr(90Zr, X), E≈165-177 MeV; re-analyzed S-factors in fusion reactions; calculated S-factors, fusion hinderance effect.
doi: 10.1088/1742-6596/312/4/042011
2011MA51 Phys.Rev. C 84, 044332 (2011) P.Marley, D.G.Jenkins, P.J.Davies, A.P.Robinson, R.Wadsworth, C.J.Lister, M.P.Carpenter, R.V.F.Janssens, C.L.Jiang, T.L.Khoo, T.Lauritsen, D.Seweryniak, S.Zhu, S.Courtin, F.Haas, D.Lebhertz, M.Bouhelal, J.C.Lighthall, A.H.Wuosmaa, D.O'Donnell High-resolution spectroscopy of decay pathways in the 12C(12C, γ) reaction NUCLEAR REACTIONS 12C(12C, γ)24Mg, E=16 MeV; measured Eγ, Iγ, (particle)γ-, γγ-coin using Gammasphere array and Fragment mass analyzer coupled to PGAC system. 24Mg; deduced levels, J, π, bands, configuration, resonances. Particle-hole structure interpreted by PSDPF shell-model calculations.
doi: 10.1103/PhysRevC.84.044332
2010ES07 Phys.Rev. C 82, 054621 (2010) H.Esbensen, C.L.Jiang, A.M.Stefanini Hindrance in the fusion of 48Ca+48Ca NUCLEAR REACTIONS 48Ca(48Ca, X), E(cm)=45-60 MeV; analyzed fusion σ, rms radii, and S factors using coupled-channel (CC) method with Woods-Saxon and M3Y+repulsion potentials.
doi: 10.1103/PhysRevC.82.054621
2010JI03 Phys.Rev. C 81, 024611 (2010) C.L.Jiang, K.E.Rehm, H.Esbensen, B.B.Back, R.V.F.Janssens, P.Collon, C.M.Deibel, B.DiGiovine, J.M.Figueira, J.P.Greene, D.J.Henderson, H.Y.Lee, M.Notani, S.T.Marley, R.C.Pardo, N.Patel, D.Seweryniak, X.D.Tang, C.Ugalde, S.Zhu Fusion hindrance for 27Al+45Sc and other systems with a positive Q value NUCLEAR REACTIONS 45Sc(27Al, X), E=51-82 MeV; measured fragment spectra, σ, astrophysical S-factor. Comparison with coupled-channels calculations. 14N(14N, X), E=4-11 MeV; 30Si(28Si, X), E=25-31 MeV; 45Sc(27Al, X), E=32-39 MeV; 64Ni(28Si, X), E=44-51 MeV; 40Ca(40Ca, X), E=49-57 MeV; 48Ca(48Ca, X), E=46-56 MeV; 48Ca(36S, X), E=37-48 MeV; comparison of measured cross sections and astrophysical S-factors with coupled-channel calculations.
doi: 10.1103/PhysRevC.81.024611
2010JI13 Nucl.Phys. A834, 615c (2010) Survey of heavy-ion fusion hindrance and its implication on astrophysics NUCLEAR REACTIONS 64Ni(64Ni, X), E=86-100 MeV; analyzed σ, S-factor; compiled, analyzed S-factor systematics.
doi: 10.1016/j.nuclphysa.2010.01.106
2010JI14 Phys.Rev. C 82, 041601 (2010) C.L.Jiang, A.M.Stefanini, H.Esbensen, K.E.Rehm, L.Corradi, E.Fioretto, P.Mason, G.Montagnoli, F.Scarlassara, R.Silvestri, P.P.Singh, S.Szilner, X.D.Tang, C.A.Ur Fusion hindrance for Ca+Ca systems: Influence of neutron excess NUCLEAR REACTIONS 48Ca(40Ca, X), E=89.2, 107.7 MeV; measured particle spectra, σ(E, θ); deduced S factors. Comparisons of experimental σ(E) for 40Ca+40Ca, 40Ca+48Ca, 48Ca+48Ca, 40Ca+90Zr, 40Ca+96Zr and 48Ca+96Zr systems with coupled-channel calculations.
doi: 10.1103/PhysRevC.82.041601
2010LE02 Phys.Rev. C 81, 015802 (2010) H.Y.Lee, J.P.Greene, C.L.Jiang, R.C.Pardo, K.E.Rehm, J.P.Schiffer, A.H.Wuosmaa, N.J.Goodman, J.C.Lighthall, S.T.Marley, K.Otsuki, N.Patel, M.Beard, M.Notani, X.D.Tang Experimental study of the 11, 12B(n, γ) reactions and their influence on r-process nucleosynthesis of light elements NUCLEAR REACTIONS 2H(11B, p), E=81 MeV; 2H(12B, p), E=75 MeV; measured proton and 11,12,13B particle spectra, σ(θ). 12,13B; deduced levels, J, π, l-transfers. Comparison with DWBA calculations. 11B, 12B(n, γ); deduced reaction rates of astrophysical relevance, and abundances of 11B and 12B in r process.
doi: 10.1103/PhysRevC.81.015802
2010NO04 Nucl.Phys. A834, 192c (2010) M.Notani, P.Davies, B.Bucher, X.Fang, L.Lamm, C.Ma, E.Martin, W.Tan, X.D.Tang, S.Thomas, C.L.Jiang Study of the hindrance effect in sub-barrier fusion reactions NUCLEAR REACTIONS 12C(13C, p), E(cm)=2.6-5.0 MeV; measured Eβ, Iβ, Eγ, Iγ, βγ-coin, thick target yield; deduced σ, astrophysical S-factor. Comparison with data and calculations.
doi: 10.1016/j.nuclphysa.2009.12.037
2010TA05 Phys.Rev. C 81, 045809 (2010) X.D.Tang, K.E.Rehm, I.Ahmad, C.R.Brune, A.Champagne, J.P.Greene, A.Hecht, D.J.Henderson, R.V.F.Janssens, C.L.Jiang, L.Jisonna, D.Kahl, E.F.Moore, M.Notani, R.C.Pardo, N.Patel, M.Paul, G.Savard, J.P.Schiffer, R.E.Segel, S.Sinha, A.H.Wuosmaa Determination of the E1 component of the low-energy 12C(α, γ)16O cross section RADIOACTIVITY 16N(β-α); measured Eα, Iα, α12C-coin, half-life; deduced E1 component of the S factor for 12C(α, γ)16O reaction using a set of twin ionization chambers. R-matrix analysis. Comparison with previous studies. NUCLEAR REACTIONS 2H(15N, p)15N/16N/16O/20Ne, E=82 MeV; measured fragment yields.
doi: 10.1103/PhysRevC.81.045809
2009ES01 Phys.Rev. C 79, 064619 (2009) Indications of a shallow potential in 48Ca+96Zr fusion reactions NUCLEAR REACTIONS 96Zr(48Ca, X), E=86-115 MeV; 90,94,96Zr(40Ca, X), 90Zr(48Ca, X), E=78-96 MeV; analyzed fusion σ, barrier distributions and astrophysical S factors using coupled-channels calculations. Comparison with experimental data.
doi: 10.1103/PhysRevC.79.064619
2009JI04 Phys.Rev. C 79, 044601 (2009) C.L.Jiang, K.E.Rehm, B.B.Back, R.V.F.Janssens Survey of heavy-ion fusion hindrance for lighter systems NUCLEAR REACTIONS 18O(16O, X), E(cm)=6-12 MeV; 14N(14N, X), E(cm)=4-11 MeV; analyzed σ and logarithmic derivative L(E). 10B(10B, X), E not given; 12C, 14N(11B, X), E not given; 12,13C, 14N, 16O, 20Ne(12C, X), E not given; 16O(13C, X), E not given; 14N, 16O(14N, X), E not given; 16,18O, 76Ge(16O, X), E not given; 30Si(28Si, X); analyzed σ and heavy-ion reaction parameters. 16O(16O, X), E not given; analyzed astrophysical S-factors.
doi: 10.1103/PhysRevC.79.044601
2009JI08 Phys.Rev. C 80, 044613 (2009) C.L.Jiang, K.E.Rehm, D.Ackermann, I.Ahmad, J.P.Greene, B.Harss, D.Henderson, W.F.Henning, R.V.F.Janssens, J.Nolen, R.C.Pardo, P.Reiter, J.P.Schiffer, D.Seweryniak, A.Sonzogni, J.Uusitalo, I.Wiedenhover, A.H.Wuosmaa, F.Brumwell, G.McMichael, M.Paul, R.E.Segel Experimental study of the 56Ni(3He, d)57Cu reaction in inverse kinematics NUCLEAR REACTIONS 3He(56Ni, d), E=250 MeV; measured Ed, Id, σ, σ(θ). 57Cu; deduced levels, J, π, spectroscopic factors. DWBA analysis. Discussed implications for 56Ni(p, γ)57Cu reaction of astrophysical interest.
doi: 10.1103/PhysRevC.80.044613
2009QI04 Phys.Rev. C 79, 064319 (2009) J.Qian, A.Heinz, T.L.Khoo, R.V.F.Janssens, D.Peterson, D.Seweryniak, I.Ahmad, M.Asai, B.B.Back, M.P.Carpenter, A.B.Garnsworthy, J.P.Greene, A.A.Hecht, C.L.Jiang, F.G.Kondev, T.Lauritsen, C.J.Lister, A.Robinson, G.Savard, R.Scott, R.Vondrasek, X.Wang, R.Winkler, S.Zhu Spectroscopy of 257Rf NUCLEAR REACTIONS 208Pb(50Ti, n), E=233 MeV; measured Eα, Iα, ce, fission events correlated with evaporation residues, Eγ, Iγ, (ce)α-, (ce)γ-coin, isomer half-lives, (evaporation residues)-ce-α-α correlations. 257Rf; deduced levels, J, π, configurations. 257Rf; calculated excitation energies of 1-qp states and rotational bands built on 1-qp and 3-qp bandheads. A=245-257, odd-A Pu, Cm, Cf, Fm, No, Rf; Nilsson orbital systematics. RADIOACTIVITY 257Rf(α)(EC)(SF), 257mRf(α)(EC), 257Lr(α), 256Rf(SF), 253No(α)(EC); measured Eα, Iα, Eγ, fission events, (ce)α-coin, half-lives, and fission branching ratios. 253No; deduced levels, J, π, α hindrance factors, and configurations.
doi: 10.1103/PhysRevC.79.064319
2008JI04 Phys.Rev. C 78, 017601 (2008) C.L.Jiang, B.B.Back, H.Esbensen, J.P.Greene, R.V.F.Janssens, D.J.Henderson, H.Y.Lee, C.J.Lister, M.Notani, R.C.Pardo, N.Patel, K.E.Rehm, D.Seweryniak, B.Shumard, X.Wang, S.Zhu, S.Misicu, P.Collon, X.D.Tang Fusion hindrance for a positive Q-value system NUCLEAR REACTIONS 30Si(28Si, X), E=48.5-71 MeV; measured excitation functions, fusion σ. 12C(12C, X); systematics of Q-values. Comparisons with model calculations.
doi: 10.1103/PhysRevC.78.017601
2008KI05 J.Phys.(London) G35, 014033 (2008) N.Kinoshita, T.Hashimoto, T.Nakanishi, A.Yokoyama, H.Amakawa, T.Mitsugashira, T.Ohtsuki, N.Takahashi, I.Ahmad, J.P.Greene, D.J.Henderson, C.L.Jiang, M.Notani, R.C.Pardo, N.Patel, K.E.Rehm, R.Scott, R.Vondrasek, L.Jisonna, P.Collon, D.Robertson, C.Schmitt, X.D.Tang, Y.Kashiv, H.Nassar, M.Paul Ultra-sensitive detection of p-process nuclide 146Sm produced by (γ, n), (p, 2nε) and (n, 2n) reactions
doi: 10.1088/0954-3899/35/1/014033
2008SC03 Phys.Rev.Lett. 100, 112501 (2008) J.P.Schiffer, S.J.Freeman, J.A.Clark, C.Deibel, C.R.Fitzpatrick, S.Gros, A.Heinz, D.Hirata, C.L.Jiang, B.P.Kay, A.Parikh, P.D.Parker, K.E.Rehm, A.C.C.Villari, V.Werner, C.Wrede Nuclear Structure Relevant to Neutrinoless Double β Decay: 76Ge and 76Se NUCLEAR REACTIONS 74,76Ge, 76,78Se(d, p), E=15 MeV; 76Ge, 76Se(p, d), E=23 MeV; 74,76Ge, 76,78Se(3He, α), E=26 MeV; 74,76Ge, 76,78Se(α, 3He), E=40 MeV; measured reaction products energy spectra, cross sections. Deduced summed spectroscopic strengths, neutron vacancies.
doi: 10.1103/PhysRevLett.100.112501
2008WU05 Phys.Rev. C 78, 041302 (2008) A.H.Wuosmaa, J.P.Schiffer, K.E.Rehm, J.P.Greene, D.J.Henderson, R.V.F.Janssens, C.L.Jiang, L.Jisonna, J.C.Lighthall, S.T.Marley, E.F.Moore, R.C.Pardo, N.Patel, M.Paul, D.Peterson, S.C.Pieper, G.Savard, R.E.Segel, R.H.Siemssen, X.D.Tang, R.B.Wiringa Structure of 7He by proton removal from 8Li with the (d, 3He) reaction NUCLEAR REACTIONS 2H(8Li, 3He), E=76 MeV; 2H(7Li, t), (7Li, 3He), E=81 MeV; measured charged particle spectra, (particle)(particle)-coin, angular distributions, σ, σ(θ), spectroscopic factors. 7He; deduced levels, J, π. Comparisons with data from 2H(6He, p) experiment. Comparisons with nuclear structure models and variational quantum Monte Carlo calculations.
doi: 10.1103/PhysRevC.78.041302
2007FR10 Phys.Rev. C 75, 051301 (2007) S.J.Freeman, J.P.Schiffer, A.C.C.Villari, J.A.Clark, C.Deibel, S.Gros, A.Heinz, D.Hirata, C.L.Jiang, B.P.Kay, A.Parikh, P.D.Parker, J.Qian, K.E.Rehm, X.D.Tang, V.Werner, C.Wrede Pair correlations in nuclei involved in neutrinoless double Β decay: 76Ge and 76Se NUCLEAR REACTIONS 74,76Ge, 76,78Se(p, t), E=23 MeV; measured yields, cross sections and angular distributions. Compared results to DWBA calculations.
doi: 10.1103/PhysRevC.75.051301
2007GA43 Phys.Rev. C 76, 035802 (2007) L.R.Gasques, E.F.Brown, A.Chieffi, C.L.Jiang, M.Limongi, C.Rolfs, M.Wiescher, D.G.Yakovlev Implications of low-energy fusion hindrance on stellar burning and nucleosynthesis NUCLEAR REACTIONS 12C, 16O(16O, X), E < 12 MeV; 16O(16O, X), E < 15 MeV; analyzed fusion cross sections. Deduced S-factors at astrophysical energies.
doi: 10.1103/PhysRevC.76.035802
2007HA49 J.Nucl.Radiochem.Sci. 8, 109 (2007) T.Hashimoto, T.Nakanishi, A.Yokoyama, H.Amakawa, T.Mitsugashira, T.Ohtsuki, N.Takahashi, I.Ahmad, J.P.Greene, D.J.Henderson, C.L.Jiang, M.Notani, R.C.Pardo, N.Patel, K.E.Rehm, R.Scott, R.Vondrasek, L.Jisonna, P.Collon, D.Robertson, C.Schmitt, X.D.Tang, Y.Kashiv, M.Paul Technological Development for Half-life Measurement of 146Sm Nuclide NUCLEAR REACTIONS 147Sm(γ, n), E < 50 MeV; 147Sm(n, 2n), E=6-10 MeV; 147Sm(p, 2n), E=21 MeV; measured Eα, Iα.
2007JI01 Phys.Rev. C 75, 015803 (2007) C.L.Jiang, K.E.Rehm, B.B.Back, R.V.F.Janssens Expectations for 12C and 16O induced fusion cross sections at energies of astrophysical interest NUCLEAR REACTIONS 12C, 16O(12C, X), 16O(16O, X), E=5-12 MeV; analyzed fusion σ, astrophysical S-factors; calculated astrophysical reaction rates.
doi: 10.1103/PhysRevC.75.015803
2007JI10 Phys.Rev. C 75, 057604 (2007) C.L.Jiang, B.B.Back, R.V.F.Janssens, K.E.Rehm Radius of curvature of the S factor maximum in sub-barrier fusion hindrance NUCLEAR REACTIONS 13C(12C, X), E=3-7 MeV; calculated the radius of curvature of the S-factor maximum to investigate the onset of sub-barrier fusion hindrance.
doi: 10.1103/PhysRevC.75.057604
2007NA27 Phys.Rev. C 76, 054604 (2007) R.S.Naik, W.Loveland, P.H.Sprunger, A.M.Vinodkumar, D.Peterson, C.L.Jiang, S.Zhu, X.Tang, E.F.Moore, P.Chowdhury Measurement of the fusion probability PCN for the reaction of 50Ti with 208Pb NUCLEAR REACTIONS 208Pb(50Ti, X), E(cm)=183.7, 186.2, 190.2, 194.2, 202.3 MeV; measured fission fragments, cross sections, angular distributions; deduced fusion probabilities and survival probabilities for compound nuclei Z=102-113.
doi: 10.1103/PhysRevC.76.054604
2007TA34 Phys.Rev.Lett. 99, 052502 (2007) X.D.Tang, K.E.Rehm, I.Ahmad, C.R.Brune, A.Champagne, J.P.Greene, A.A.Hecht, D.Henderson, R.V.F.Janssens, C.L.Jiang, L.Jisonna, D.Kahl, E.F.Moore, M.Notani, R.C.Pardo, N.Patel, M.Paul, G.Savard, J.P.Schiffer, R.E.Segel, S.Sinha, B.Shumard, A.H.Wuosmaa New Determination of the Astrophysical S Factor SE1 of the 12C(α, γ)16O Reaction RADIOACTIVITY 16N(β-), (β-α); measured Eα, Iα, 12Cα-coin. 12C(α, γ); deduced astrophysical S-factor.
doi: 10.1103/PhysRevLett.99.052502
2007WU05 Eur.Phys.J. Special Topics 150, 79 (2007) A.H.Wuosmaa, K.E.Rehm, J.P.Greene, D.J.Henderson, R.V.F.Janssens, C.L.Jiang, L.Jisonna, J.C.Lighthall, S.T.Marley, E.F.Moore, R.C.Pardo, N.Patel, M.Paul, D.Peterson, S.C.Pieper, G.Savard, J.P.Schiffer, R.E.Segal, R.H.Siemssen, S.Sinha, X.Tang, R.B.Wiringa Nucleon transfer reactions with exotic beams at ATLAS
doi: 10.1140/epjst/e2007-00271-y
2006JI01 Phys.Rev. C 73, 014613 (2006) C.L.Jiang, B.B.Back, H.Esbensen, R.V.F.Janssens, K.E.Rehm Systematics of heavy-ion fusion hindrance at extreme sub-barrier energies NUCLEAR REACTIONS 64Ni(58Ni, X), (64Ni, X), E ≈ 85-105 MeV; 10B(10B, X), 12C(11B, X), (13C, X), 16O(12C, X), (16O, X), E ≈ 2-17 MeV; 64Ni(28Si, X), 48Ca(48Ca, X), E ≈ 45-60 MeV; 89Y(60Ni, X), 92Zr(90Zr, X), E ≈ 120-180 MeV; analyzed fusion σ, sub-barrier hindrance.
doi: 10.1103/PhysRevC.73.014613
2006JI06 Phys.Lett. B 640, 18 (2006) C.L.Jiang, B.B.Back, H.Esbensen, R.V.F.Janssens, S.Misicu, K.E.Rehm, P.Collon, C.N.Davids, J.Greene, D.J.Henderson, L.Jisonna, S.Kurtz, C.J.Lister, M.Notani, M.Paul, R.Pardo, D.Peterson, D.Seweryniak, B.Shumard, X.D.Tang, I.Tanihata, X.Wang, S.Zhu First evidence of fusion hindrance for a small Q-value system NUCLEAR REACTIONS 64Ni(28Si, X), E=63-95 MeV; measured fusion-evaporation σ, fusion excitation function; deduced hindrance at sub-barrier energies. Coupled-channels analysis.
doi: 10.1016/j.physletb.2006.07.007
2006NA02 Phys.Rev.Lett. 96, 041102 (2006) H.Nassar, M.Paul, I.Ahmad, Y.Ben-Dov, J.Caggiano, S.Ghelberg, S.Goriely, J.P.Greene, M.Hass, A.Heger, A.Heinz, D.J.Henderson, R.V.F.Janssens, C.L.Jiang, Y.Kashiv, B.S.Nara Singh, A.Ofan, R.C.Pardo, T.Pennington, K.E.Rehm, G.Savard, R.Scott, R.Vondrasek 40Ca(α, γ)44Ti Reaction in the Energy Regime of Supernova Nucleosynthesis NUCLEAR REACTIONS 4He(40Ca, γ), E(cm) ≈ 0.6-1.2 MeV/nucleon; measured yield. 40Ca(α, γ), E=low; deduced astrophysical reaction rate. Accelerator mass spectrometry.
doi: 10.1103/PhysRevLett.96.041102
2006PE17 Phys.Rev. C 74, 014316 (2006) D.Peterson, B.B.Back, R.V.F.Janssens, T.L.Khoo, C.J.Lister, D.Seweryniak, I.Ahmad, M.P.Carpenter, C.N.Davids, A.A.Hecht, C.L.Jiang, T.Lauritsen, X.Wang, S.Zhu, F.G.Kondev, A.Heinz, J.Qian, R.Winkler, P.Chowdhury, S.K.Tandel, U.S.Tandel Decay modes of 250No RADIOACTIVITY 250No(SF) [from 204Pb(48Ca, 2n)]; measured T1/2 for ground and isomeric state decay; deduced upper limit for α-decay branching ratio. 219,220Th(α) [from 176Yb(48Ca, xn)]; measured T1/2.
doi: 10.1103/PhysRevC.74.014316
2005JI02 Phys.Rev. C 71, 044613 (2005) C.L.Jiang, K.E.Rehm, H.Esbensen, R.V.F.Janssens, B.B.Back, C.N.Davids, J.P.Greene, D.J.Henderson, C.J.Lister, R.C.Pardo, T.Pennington, D.Peterson, D.Seweryniak, B.Shumard, S.Sinha, X.D.Tang, I.Tanihata, S.Zhu, P.Collon, S.Kurtz, M.Paul Hindrance of heavy-ion fusion at extreme sub-barrier energies in open-shell colliding systems NUCLEAR REACTIONS 100Mo(64Ni, X), E=196-262 MeV; measured fusion-evaporation σ, fusion excitation function; deduced hindrance at sub-barrier energies. 58,60,64Ni, 74Ge, 90,91,94Zr, 92,100Mo, 124Sn(58Ni, X), 89Y(60Ni, X), 64Ni, 74Ge, 92,96Zr, 92,100Mo, 124Sn(64Ni, X), E(cm) ≈ 120 MeV; analyzed fusion σ, sub-barrier hindrance.
doi: 10.1103/PhysRevC.71.044613
2005NA08 Phys.Rev.Lett. 94, 092504 (2005) H.Nassar, M.Paul, I.Ahmad, D.Berkovits, M.Bettan, P.Collon, S.Dababneh, S.Ghelberg, J.P.Greene, A.Heger, M.Heil, D.J.Henderson, C.L.Jiang, F.Kappeler, H.Koivisto, S.O'Brien, R.C.Pardo, N.Patronis, T.Pennington, R.Plag, K.E.Rehm, R.Reifarth, R.Scott, S.Sinha, X.Tang, R.Vondrasek Stellar (n, γ) Cross Section of 62Ni NUCLEAR REACTIONS 62Ni(n, γ), E=spectrum; measured total σ. Fast-neutron activation, accelerator mass spectrometry. Astrophysical implications discussed.
doi: 10.1103/PhysRevLett.94.092504
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
2005WU03 Phys.Rev.Lett. 94, 082502 (2005) A.H.Wuosmaa, K.E.Rehm, J.P.Greene, D.J.Henderson, R.V.F.Janssens, C.L.Jiang, L.Jisonna, E.F.Moore, R.C.Pardo, M.Paul, D.Peterson, S.C.Pieper, G.Savard, J.P.Schiffer, R.E.Segel, S.Sinha, X.Tang, R.B.Wiringa Neutron Spectroscopic Factors in 9Li from 2H(8Li, p)9Li NUCLEAR REACTIONS 2H(8Li, p), E ≈ 76 MeV; measured Ep, excitation energy spectra, σ(θ). 9Li deduced levels, J, π, spectroscopic factors. Comparison with model predictions.
doi: 10.1103/PhysRevLett.94.082502
2005WU08 Phys.Rev. C 72, 061301 (2005) A.H.Wuosmaa, K.E.Rehm, J.P.Greene, D.J.Henderson, R.V.F.Janssens, C.L.Jiang, L.Jisonna, E.F.Moore, R.C.Pardo, M.Paul, D.Peterson, Steven C.Pieper, G.Savard, J.P.Schiffer, R.E.Segel, S.Sinha, X.Tang, R.B.Wiringa Search for excited states in 7He with the (d, p) reaction NUCLEAR REACTIONS 2H(6He, p), E=69 MeV; 2H(7Li, p), E=81 MeV; measured particle spectra, σ(θ). 7He deduced ground-state J, π, excited state energy, width.
doi: 10.1103/PhysRevC.72.061301
2004JI01 Phys.Rev. C 69, 014604 (2004) C.L.Jiang, H.Esbensen, B.B.Back, R.V.F.Janssens, K.E.Rehm Analysis of heavy-ion fusion reactions at extreme sub-barrier energies NUCLEAR REACTIONS 89Y(60Ni, X), E=115-140 MeV; analyzed fusion σ, barrier distribution. 58Ni(58Ni, X), 89Y(60Ni, X), 89Y, 90,92Zr(90Zr, X), 144Sm, 208Pb(16O, X), 208Pb(19F, X), (50Ti, X), 64Ni(64Ni, X), E ≈ 100-300 MeV; analyzed fusion S-factors. Coupled-channels approach.
doi: 10.1103/PhysRevC.69.014604
2004JI05 Phys.Rev.Lett. 93, 012701 (2004) C.L.Jiang, K.E.Rehm, R.V.F.Janssens, H.Esbensen, I.Ahmad, B.B.Back, P.Collon, C.N.Davids, J.P.Greene, D.J.Henderson, G.Mukherjee, R.C.Pardo, M.Paul, T.O.Pennington, D.Seweryniak, S.Sinha, Z.Zhou Influence of Nuclear Structure on Sub-Barrier Hindrance in Ni + Ni Fusion NUCLEAR REACTIONS 64Ni(64Ni, X), E=171-220 MeV; measured fusion excitation function; deduced structure effects in sub-barrier hindrance. Comparison with similar reactions.
doi: 10.1103/PhysRevLett.93.012701
2004JI07 Prog.Theor.Phys.(Kyoto), Suppl. 154, 61 (2004) C.L.Jiang, H.Esbensen, K.E.Rehm, B.B.Back, R.V.F.Janssens, C.N.Davids, J.P.Greene, D.J.Henderson, G.Mukherjee, R.C.Pardo, T.O.Pennington, D.Seweryniak, S.Sinha, Z.Zhou, M.Paul, P.Collon, J.A.Caggiano, A.M.Heinz, I.Nishinaka Systematics of Heavy-Ion Fusion Reactions at Extreme Sub-Barrier Energies NUCLEAR REACTIONS 64Ni(64Ni, X), E=172-212 MeV; measured fusion excitation function; deduced barrier distribution. Fragment mass analyzer, S-factor analysis, fusion reaction systematics discussed.
doi: 10.1143/PTPS.154.61
2004JI09 Nucl.Phys. A746, 403c (2004) C.L.Jiang, B.B.Back, J.Nolen, K.E.Rehm, G.Savard The influence of secondary reactions in the wedge of a magnetic separator at RIA
doi: 10.1016/j.nuclphysa.2004.09.142
2004NA39 Nucl.Phys. A746, 613c (2004) H.Nassar, S.Ghelberg, M.Paul, S.Dababneh, M.Heil, F.Kappeler, R.Plag, I.Ahmad, J.P.Greene, D.J.Henderson, C.L.Jiang, R.C.Pardo, T.Pennington, K.E.Rehm, R.Scott, S.Sinha, X.Tang, R.Vondrasek, H.Koivisto, D.Berkovits, M.Bettan, R.Reifarth, P.Collon, S.O'Brien, N.Patronis Production and isobaric separation of 63Ni ions for determination of the 62Ni(n, γ)63Ni reaction cross section at stellar temperatures NUCLEAR REACTIONS 62Ni(n, γ), E=fast; measured yields.
doi: 10.1016/j.nuclphysa.2004.09.140
2004RE31 Nucl.Phys. A746, 354c (2004) K.E.Rehm, C.L.Jiang, J.P.Greene, D.Henderson, R.V.F.Janssens, E.F.Moore, G.Mukherjee, R.C.Pardo, T.Pennington, J.P.Schiffer, S.Sinha, X.D.Tang, R.H.Siemssen, L.Jisonna, R.E.Segel, A.H.Wuosmaa First studies of the 8B(α, p)11C reaction NUCLEAR REACTIONS 1H(11C, α), E=98-110 MeV; measured σ(θ). 8B(α, p), E*=8.7-9.8 MeV; deduced excitation function, astrophysical reaction rate.
doi: 10.1016/j.nuclphysa.2004.09.052
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
2004SC16 Phys.Rev.Lett. 92, 162501 (2004); Erratum Phys.Rev.Lett. 110, 169901 (2013) J.P.Schiffer, S.J.Freeman, J.A.Caggiano, C.Deibel, A.Heinz, C.-L.Jiang, R.Lewis, A.Parikh, P.D.Parker, K.E.Rehm, S.Sinha, J.S.Thomas Is the Nuclear Spin-Orbit Interaction Changing with Neutron Excess? NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(α, t), E=40 MeV; measured σ(E, θ). 113,115,117,119,121,123,125Sb levels deduced spectroscopic factors, decrease in nuclear spin-orbit interaction. Nuclides near N=82 also discussed.
doi: 10.1103/PhysRevLett.92.162501
2004WA23 Phys.Rev.Lett. 93, 142501 (2004) L.-B.Wang, P.Mueller, K.Bailey, G.W.F.Drake, J.P.Greene, D.Henderson, R.J.Holt, R.V.F.Janssens, C.L.Jiang, Z.-T.Lu, T.P.O'Connor, R.C.Pardo, K.E.Rehm, J.P.Schiffer, X.D.Tang Laser Spectroscopic Determination of the 6He Nuclear Charge Radius NUCLEAR MOMENTS 4,6He; measured isotope shift. 6He deduced charge radius. Laser spectroscopy.
doi: 10.1103/PhysRevLett.93.142501
2004WI13 Nucl.Phys. A746, 311c (2004) W.T.Winter, K.E.Rehm, C.L.Jiang, I.Ahmad, S.J.Freedman, J.Greene, A.Heinz, D.Henderson, R.V.F.Janssens, E.F.Moore, G.Mukherjee, R.C.Pardo, M.Paul, T.Pennington, G.Savard, J.P.Schiffer, D.Seweryniak, G.Zinkann Determination of the 8B neutrino spectrum RADIOACTIVITY 8B(EC); measured β-delayed Eα; deduced neutrino spectrum. 20Na(EC); measured β-delayed Eα.
doi: 10.1016/j.nuclphysa.2004.09.029
2003MU09 Nucl.Instrum.Methods Phys.Res. B204, 536 (2003) P.Muller, L.-B.Wang, K.Bailey, G.W.F.Drake, X.Du, J.Greene, A.M.Heinz, R.J.Holt, D.Henderson, R.V.Janssens, C.-L.Jiang, C.Law, Z.-T.Lu, I.D.Moore, T.P.O'Connor, R.C.Pardo, M.Paul, T.Pennington, K.E.Rehm, J.P.Schiffer Towards measuring the charge radius of 6He and 8He RADIOACTIVITY 6He(β-) [from 12C(7Li, 6He)]; measured Eβ, T1/2. Magneto-optical trap for charge radius measurement.
doi: 10.1016/S0168-583X(02)02128-6
2003PA34 Nucl.Phys. A718, 239c (2003) M.Paul, C.Feldstein, I.Ahmad, D.Berkovits, C.Bordeanu, J.Caggiano, S.Ghelberg, J.Goerres, J.Greene, M.Hass, A.Heinz, D.Henderson, S.K.Hui, R.V.F.Janssens, C.L.Jiang, S.Jiang, Y.Nirel, R.C.Pardo, T.Pennington, K.E.Rehm, G.Savard, G.Verri, R.Vondrasek, I.Wiedenhover, M.Wiescher Counting 44Ti Nuclei from the 40Ca(α, γ)44Ti Reaction NUCLEAR REACTIONS 4He(40Ca, X)44Ti, E=70.9 MeV; measured yield. 44Ti deduced resonance strength. Chemical separation, accelerator mass spectrometry.
doi: 10.1016/S0375-9474(03)00720-6
2003RE16 Phys.Rev. C 67, 065809 (2003) K.E.Rehm, A.H.Wuosmaa, C.L.Jiang, J.Caggiano, J.P.Greene, A.Heinz, D.Henderson, R.V.F.Janssens, E.F.Moore, G.Mukherjee, R.C.Pardo, T.Pennington, J.P.Schiffer, R.H.Siemssen, M.Paul, L.Jisonna, R.E.Segel Branching ratio Γα/Γγ of the 4.033 MeV 3/2+ state in 19Ne NUCLEAR REACTIONS 3He(20Ne, α), E ≈ 98 MeV; measured particle spectra, yields, (particle)(recoil)-coin; deduced excitation energy spectra. 19Ne levels deduced α-decay branching widths. 15O(α, γ), E=low; deduced astrophysical reaction rates.
doi: 10.1103/PhysRevC.67.065809
2003RE25 Nucl.Phys. A718, 151c (2003) K.E.Rehm, A.H.Wuosmaa, C.L.Jiang, J.Greene, A.Heinz, D.Henderson, R.V.F.Janssens, L.Jisonna, E.F.Moore, G.Mukherjee, R.C.Pardo, M.Paul, T.Pennington, J.P.Schiffer, R.E.Segel, R.H.Siemssen The Branching Ratio Γα/Γγ of the 4.033 MeV State in 19Ne NUCLEAR REACTIONS 3He(20Ne, α), E=105 MeV; measured particle spectra, (particle)(recoil)-coin. 19Ne levels deduced α-branching ratios, radiative widths. 15O(α, γ), E=low; deduced astrophysical reaction rates.
doi: 10.1016/S0375-9474(03)00706-1
2003RE26 Nucl.Phys. A718, 443c (2003) K.E.Rehm, W.Winter, C.L.Jiang, I.Ahmad, S.J.Freedman, J.Greene, A.Heinz, D.Henderson, R.V.F.Janssens, E.F.Moore, G.Mukherjee, R.C.Pardo, M.Paul, T.Pennington, G.Savard, J.P.Schiffer, D.Seweryniak, G.Zinkann Study of the 8B Neutrino Spectrum With a New Technique RADIOACTIVITY 8B, 20Na(α) [from 3He(6Li, n), (19F, 2n)]; measured Eα.
doi: 10.1016/S0375-9474(03)00841-8
2003WI11 Nucl.Phys. A721, 553c (2003) W.Winter, K.E.Rehm, C.L.Jiang, I.Ahmad, S.J.Freedman, J.Greene, A.Heinz, D.Henderson, R.V.F.Janssens, E.F.Moore, G.Mukherjee, R.C.Pardo, M.Paul, T.Pennington, G.Savard, J.P.Schiffer, D.Seweryniak, G.Zinkann Measurement of the 8B Neutrino Spectrum RADIOACTIVITY 8B, 20Na(β+), (EC) [from 3He(6Li, n) and 3He(19F, 2n)]; measured β-delayed Eα. Mass-separated sources.
doi: 10.1016/S0375-9474(03)01122-9
2003WI16 Phys.Rev.Lett. 91, 252501 (2003) W.T.Winter, S.J.Freedman, K.E.Rehm, I.Ahmad, J.P.Greene, A.Heinz, D.Henderson, R.V.F.Janssens, C.L.Jiang, E.F.Moore, G.Mukherjee, R.C.Pardo, T.Pennington, G.Savard, J.P.Schiffer, D.Seweryniak, G.Zinkann, M.Paul Determination of the 8B Neutrino Spectrum RADIOACTIVITY 8B, 20Na(β+α) [from 3He(6Li, n) and 3He(19F, 2n)]; measured β-delayed Eα, Iα, βα-coin; deduced neutrino spectrum. Comparison with previous results.
doi: 10.1103/PhysRevLett.91.252501
2002HA15 Phys.Rev. C65, 035803 (2002) B.Harss, C.L.Jiang, K.E.Rehm, J.P.Schiffer, J.Caggiano, P.Collon, J.P.Greene, D.Henderson, A.Heinz, R.V.F.Janssens, J.Nolen, R.C.Pardo, T.Pennington, R.H.Siemssen, A.A.Sonzogni, J.Uusitalo, I.Wiedenhover, M.Paul, T.F.Wang, F.Borasi, R.E.Segel, J.C.Blackmon, M.Smith, A.Chen, P.Parker Widths of Astrophysically Important Resonances in 18Ne NUCLEAR REACTIONS 1H(17F, p), (17F, α), E(cm)=3.07-3.94 MeV; measured σ, σ(E, θ). 17F(p, p'), E(cm) ≈ 3.5 MeV; deduced σ(θ). 14O(α, p), E=low; deduced astrophysical reaction rates. 18Ne deduced resonance parameters.
doi: 10.1103/PhysRevC.65.035803
2002JI04 Phys.Rev.Lett. 89, 052701 (2002); Comment Phys.Rev.Lett. 91, 229201 (2003) C.L.Jiang, H.Esbensen, K.E.Rehm, B.B.Back, R.V.F.Janssens, J.A.Caggiano, P.Collon, J.Greene, A.M.Heinz, D.J.Henderson, I.Nishinaka, T.O.Pennington, D.Seweryniak Unexpected Behavior of Heavy-Ion Fusion Cross Sections at Extreme Sub-Barrier Energies NUCLEAR REACTIONS 89Y(60Ni, X), E=122-136 MeV; measured fusion-evaporation σ; deduced discrepancy with model prediction at low energy. Comparison with previous results from other systems.
doi: 10.1103/PhysRevLett.89.052701
2002JI08 Nucl.Instrum.Methods Phys.Res. A492, 57 (2002) C.L.Jiang, B.B.Back, I.Gomes, A.M.Heinz, J.Nolen, K.E.Rehm, G.Savard, J.P.Schiffer Yield calculations for a facility for short-lived nuclear beams NUCLEAR REACTIONS 7Li(86Kr, X)78Ni, E ≈ 0.1-1 GeV/nucleon; 9Be(40Ar, X)19C, E ≈ 0.1-1 GeV/nucleon; calculated yields vs target thickness. Yields for many other reactions discussed.
doi: 10.1016/S0168-9002(02)01352-9
2002RE29 Phys.Rev.Lett. 89, 132501 (2002) K.E.Rehm, C.L.Jiang, I.Ahmad, J.Caggiano, P.Collon, J.P.Greene, D.Henderson, A.Heinz, R.V.F.Janssens, R.C.Pardo, T.Pennington, J.P.Schiffer, R.H.Siemssen, A.H.Wuosmaa, M.Paul, P.Mohr Large Angle Elastic Alpha Scattering on a N = Z Nucleus above A = 40 NUCLEAR REACTIONS 4He(44Ti, 44Ti), (44Ti, 44Ti'), (40Ca, 40Ca), E(cm)=21.8 MeV; measured σ(θ); deduced angle-integrated σ, optical model parameters.
doi: 10.1103/PhysRevLett.89.132501
2000SO01 Phys.Rev.Lett. 84, 1651 (2000) A.A.Sonzogni, K.E.Rehm, I.Ahmad, F.Borasi, D.L.Bowers, F.Brumwell, J.Caggiano, C.N.Davids, J.P.Greene, B.Harss, A.Heinz, D.Henderson, R.V.F.Janssens, C.L.Jiang, G.McMichael, J.Nolen, R.C.Pardo, M.Paul, J.P.Schiffer, R.E.Segel, D.Seweryniak, R.H.Siemssen, J.W.Truran, J.Uusitalo, I.Wiedenhover, B.Zabransky The 44Ti(α, p) Reaction and Its Implication on the 44Ti Yield in Supernovae NUCLEAR REACTIONS 44Ti(α, p), E(cm)=5.7-9 MeV; measured σ, astrophysical reaction rate. Comparison with statistical model calculations. Effects on the production of 44Ti in core-collapsed supernovae discussed.
doi: 10.1103/PhysRevLett.84.1651
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