NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = C.C.Chang Found 88 matches. 2022HE09 Phys.Rev. C 105, 065203 (2022) J.He, D.A.Brantley, C.C.Chang, I.Chernyshev, E.Berkowitz, D.Howarth, C.Korber, A.S.Meyer, H.Monge-Camacho, E.Rinaldi, C.Bouchard, M.A.Clark, A.S.Gambhir, C.J.Monahan, A.Nicholson, P.Vranas, A.Walker-Loud Detailed analysis of excited-state systematics in a lattice QCD calculation of gA
doi: 10.1103/PhysRevC.105.065203
2021HO02 Phys.Rev. C 103, 014003 (2021) B.Horz, D.Howarth, E.Rinaldi, A.Hanlon, C.C.Chang, C.Korber, E.Berkowitz, J.Bulava, M.A.Clark, W.T.Lee, C.Morningstar, A.Nicholson, P.Vranas, A.Walker-Loud Two-nucleon S-wave interactions at the SU(3) flavor-symmetric point with mud ≈ mphyss: A first lattice QCD calculation with the stochastic Laplacian Heaviside method
doi: 10.1103/PhysRevC.103.014003
2021SU25 Nat.Phys. 17, 687 (2021), Erratum Nat.Phys. 18, 473 (2022) V.Sulkosky, C.Peng, J.Chen, A.Deur, S.Abrahamyan, K.A.Aniol, D.S.Armstrong, T.Averett, S.L.Bailey, A.Beck, P.Bertin, F.Butaru, W.Boeglin, A.Camsonne, G.D.Cates, C.-C.Chang, S.Choi, E.Chudakov, L.Coman, J.C.Cornejo, B.Craver, F.Cusanno, R.De Leo, C.W.de Jager, J.D.Denton, S.Dhamija, R.Feuerbach, J.M.Finn, S.Frullani, K.Fuoti, H.Gao, F.Garibaldi, O.Gayou, R.Gilman, A.Glamazdin, C.Glashausser, J.Gomez, J.-O.Hansen, D.Hayes, F.W.Hersman, D.W.Higinbotham, T.Holmstrom, T.B.Humensky, C.E.Hyde, H.Ibrahim, M.Iodice, X.Jiang, L.J.Kaufman, A.Kelleher, K.E.Keister, W.Kim, A.Kolarkar, N.Kolb, W.Korsch, K.Kramer, G.Kumbartzki, L.Lagamba, V.Laine, G.Laveissiere, J.J.Lerose, D.Lhuillier, R.Lindgren, N.Liyanage, H.-J.Lu, B.Ma, D.J.Margaziotis, P.Markowitz, K.R.McCormick, M.Meziane, Z.-E.Meziani, R.Michaels, B.Moffit, P.Monaghan, S.Nanda, J.Niedziela, M.Niskin, R.Pandolfi, K.D.Paschke, M.Potokar, A.Puckett, V.A.Punjabi, Y.Qiang, R.D.Ransome, B.Reitz, R.Roche, A.Saha, A.Shabetai, S.Sirca, J.T.Singh, K.Slifer, R.Snyder, P.Solvignon, R.Stringer, R.Subedi, W.A.Tobias, N.Ton, P.E.Ulmer, G.M.Urciuoli, A.Vacheret, E.Voutier, K.Wang, L.Wan, B.Wojtsekhowski, S.Woo, H.Yao, J.Yuan, X.Zhan, X.Zheng, L.Zhu Measurement of the generalized spin polarizabilities of the neutron in the low-Q2 region NUCLEAR REACTIONS 3He(polarized e-, e-), E=1.1-4.4 GeV; measured reaction products, Eβ, Iβ. 1NN; deduced transverse-transverse and longitudinal-transverse interference σ, generalized neutron spin polarizabilities. Comparison with chiral effective field theory calculations.
doi: 10.1038/s41567-021-01245-9
2018NI13 Phys.Rev.Lett. 121, 172501 (2018) A.Nicholson, E.Berkowitz, H.Monge-Camacho, D.Brantley, N.Garron, C.C.Chang, E.Rinaldi, M.A.Clark, B.Joo, T.Kurth, B.C.Tiburzi, P.Vranas, A.Walker-Loud Heavy Physics Contributions to Neutrinoless Double Beta Decay from QCD
doi: 10.1103/PhysRevLett.121.172501
2010CU02 Nucl.Phys. A835, 129c (2010) F.Cusanno, A.Acha, P.Bydzovsky, C.C.Chang, E.Cisbani, C.W.De Jager, R.De Leo, S.Frullani, F.Garibaldi, D.W.Higinbotham, M.Iodice, J.J.LeRose, P.Markowitz, S.Marrone, M.Sotona, G.M.Urciuoli, and the JLab Hall A Collaboration Update of High Resolution (e, e'K+) Hypernuclear Spectroscopy at Jefferson Lab's Hall A NUCLEAR REACTIONS 9Be, 12C, 16O(e, eK+), E not given; calculated hypernuclei σ(θ, E) using DWIA with Saclay-Lyon interaction. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.01.185
2010GA29 Int.J.Mod.Phys. E19, 2487 (2010) F.Garibaldi, E.Cisbani, F.Cusanno, S.Frullani, M.Iodice, G.M.Urciuoli, R.De Leo, L.Lagamba, S.Marrone, J.J.LeRose, C.W.de Jager, R.J.Feuerbach, D.W.Higinbotham, B.Reitz, A.Acha, P.Markowitz, P.Bydzovsky, M.Sotona, C.C.Chang, J.Millener High-resolution hypernuclear spectroscopy electron scattering at JLab, HALL A NUCLEAR REACTIONS 9B, 12C, 16O(E, EK+)9Li/12B/16N, E=4 GeV; measured reaction products; deduced σ(θ, E), hypernuclear levels and relative strengths. Comparison with theoretical calculations.
doi: 10.1142/S0218301310016995
2008LE08 Nucl.Phys. A804, 116 (2008) J.J.LeRose, C.W.de Jager, R.J.Feuerbach, D.W.Higinbotham, B.Reitz, A.Acha, P.Markowitz, P.Bydzovsky, M.Sotona, C.C.Chang, E.Cisbani, F.Cusanno, S.Frullani, F.Garibaldi, R.De Leo, L.Lagamba, S.Marrone, M.Iodice, G.M.Urciuoli, for the Hall A Collaboration Hypernuclear spectroscopy via (e, e' K+) in JLab's Hall A NUCLEAR REACTIONS 9Be, 12C, 16O(e, e'K+), E=3.66 GeV; measured hypernuclei production excitation spectra, σ(E), missing mass spectra. 12B, 16N deduced hypernuclei levels, J, π.
doi: 10.1016/j.nuclphysa.2008.01.011
2003JI01 Phys.Rev. C 67, 028201 (2003) X.Jiang, R.Gilman, R.Ransome, P.Markowitz, T.-H.Chang, C.-C.Chang, G.A.Peterson, D.W.Higinbotham, M.K.Jones, N.Liyanage, J.Mitchell Search for neutral baryon resonances below pion threshold NUCLEAR REACTIONS 1H(e, e'π+X), E=1.722 GeV; measured missing mass spectra, neutral baryon resonance yield ratio.
doi: 10.1103/PhysRevC.67.028201
2003MO08 Phys.Rev. C 67, 055205 (2003) R.M.Mohring, D.Abbott, A.Ahmidouch, Ts.A.Amatuni, P.Ambrozewicz, T.Angelescu, C.S.Armstrong, J.Arrington, K.Assamagan, S.Avery, K.Bailey, K.Beard, S.Beedoe, E.J.Beise, H.Breuer, R.Carlini, J.Cha, C.C.Chang, N.Chant, E.Cisbani, G.Collins, W.Cummings, S.Danagoulian, R.De Leo, F.Duncan, J.Dunne, D.Dutta, T.Eden, R.Ent, L.Eyraud, L.Ewell, M.Finn, T.Fortune, V.Frolov, S.Frullani, C.Furget, F.Garibaldi, D.Gaskell, D.F.Geesaman, P.Gueye, K.K.Gustafsson, J.-O.Hansen, M.Harvey, W.Hinton, E.Hungerford, M.Iodice, C.Jackson, C.Keppel, W.Kim, K.Kino, D.Koltenuk, S.Kox, L.Kramer, T.Leone, A.Lung, D.Mack, R.Madey, M.Maeda, S.Majewski, P.Markowitz, T.Mart, C.J.Martoff, D.Meekins, A.Mihul, J.Mitchell, H.Mkrtchyan, S.Mtingwa, I.Niculescu, R.Perrino, D.Potterveld, J.W.Price, B.A.Raue, J.-S.Real, J.Reinhold, P.Roos, T.Saito, G.Savage, R.Sawafta, R.Segel, S.Stepanyan, P.Stoler, V.Tadevosian, L.Tang, L.Teodorescu, T.Terasawa, H.Tsubota, G.M.Urciuoli, J.Volmer, W.Vulcan, T.P.Welch, R.Williams S.Wood, C.Yan, B.Zeidman Separation of the longitudinal and transverse cross sections in the 1H(e, e'K+)Λ and 1H(e, e'K+)Σ0 reactions NUCLEAR REACTIONS 1H(e, e'K+X), E=2.4-4 GeV; measured Λ and Σ0 hyperon production transverse and longitudinal σ, missing mass spectra. Comparison with previous results.
doi: 10.1103/PhysRevC.67.055205
2001UR03 Nucl.Phys. A691, 43c (2001) G.M.Urciuoli, P.Brindza, P.Bydzovsky, C.C.Chang, E.Cisbani, F.Cusanno, R.De Leo, S.Frullani, F.Garibaldi, M.Iodice, L.Lagamba, S.Lassiter, J.J.Le Rose, P.Markowitz, M.Sotona Electroproduction of Hypernuclei: An experimental challenge
doi: 10.1016/S0375-9474(01)01005-3
1999MO02 Phys.Rev. C59, 221 (1999) J.H.Morrison, H.Baghaei, W.Bertozzi, S.Gilad, J.Glickman, C.E.Hyde-Wright, N.Kalantar-Nayestanaki, R.W.Lourie, S.Penn, P.E.Ulmer, L.B.Weinstein, B.H.Cottman, L.Ghedira, E.J.Winhold, J.R.Calarco, J.Wise, P.Boberg, C.C.Chang, D.Zhang, K.Aniol, M.B.Epstein, D.J.Margaziotis, J.M.Finn, C.Perdrisat, V.Punjabi Quasielastic 12C(e, e'p) Reaction at High Momentum Transfer NUCLEAR REACTIONS 12C(e, e'p), E=696, 796 MeV; measured σ(θ(p), θ(e), E) vs missing energy; deduced relative importance of single- and multi-nucleon knockout, dependence on energy transfer.
doi: 10.1103/PhysRevC.59.221
1998NI08 Phys.Rev.Lett. 81, 1805 (1998) G.Niculescu, R.M.Mohring, P.Gueye, D.Abbott, A.Ahmidouch, Ts.A.Amatuni, P.Ambrozewicz, T.Angelescu, C.S.Armstrong, K.Assamagan, S.Avery, K.Bailey, O.K.Baker, K.Beard, S.Beedoe, E.Beise, H.Breuer, R.Carlini, J.Cha, C.C.Chang, N.Chant, E.Cisbani, G.Collins, W.Cummings, S.Danagoulian, R.De Leo, F.Duncan, J.Dunne, D.Dutta, T.Eden, R.Ent, L.Eyraud, L.Ewell, M.Finn, T.Fortune, V.Frolov, S.Frullani, C.Furget, F.Garibaldi, D.Gaskell, D.F.Geesaman, K.K.Gustafsson, J.-O.Hansen, M.Harvey, W.Hinton, E.Hungerford, M.Iodice, C.Jackson, C.Keppel, W.Kim, K.Kino, D.Koltenuk, S.Kox, L.Kramer, T.Leone, G.Lolos, A.Lung, D.Mack, R.Madey, M.Maeda, S.Majewski, P.Markowitz, C.J.Martoff, D.Meekins, A.Mihul, J.Mitchell, H.Mkrtchyan, S.Mtingwa, I.Niculescu, R.Perrino, D.Potterveld, J.W.Price, B.A.Raue, J.-S.Real, J.Reinhold, P.Roos, T.Saito, G.Savage, R.Sawafta, R.Segel, S.Stepanyan, P.Stoler, V.Tadevosian, L.Tang, L.Teodorescu, T.Terasawa, H.Tsubota, G.M.Urciuoli, J.Volmer, W.Vulcan, P.Welch, R.Williams, S.Wood, C.Yan, B.Zeidman Longitudinal and Transverse Cross Sections in the 1H(e, e'K+)Λ Reaction NUCLEAR REACTIONS 1H(e, e'K+), E=2.445-4.045 GeV; measured eK-coin, missing mass spectra, Λ production longitudinal, transverse σ(Q2).
doi: 10.1103/PhysRevLett.81.1805
1998ST17 Phys.Rev. D58, 032003 (1998) L.M.Stuart, P.E.Bosted, L.Andivahis, A.Lung, J.Alster, R.G.Arnold, C.C.Chang, F.S.Dietrich, W.R.Dodge, R.Gearhart, J.Gomez, K.A.Griffioen, R.S.Hicks, C.E.Hyde-Wright, C.Keppel, S.E.Kuhn, J.Lichtenstadt, R.A.Miskimen, G.A.Peterson, G.G.Petratos, S.E.Rock, S.H.Rokni, W.K.Sakumoto, M.Spengos, K.Swartz, Z.Szalata, L.H.Tao Measurements of the Δ(1232) Transition Form Factor and the Ratio σn/σp from Inelastic Electron-Proton and Electron-Deuteron Scattering NUCLEAR REACTIONS 1,2H(e, e'), E=9.8 GeV; measured σ(E', θ); deduced transition form factors, Δ production σ(n)/σ(p).
doi: 10.1103/PhysRevD.58.032003
1994AN34 Phys.Rev. D50, 5491 (1994) L.Andivahis, P.E.Bosted, A.Lung, L.M.Stuart, J.Alster, R.G.Arnold, C.C.Chang, F.S.Dietrich, W.Dodge, R.Gearhart, J.Gomez, K.A.Griffioen, R.S.Hicks, C.E.Hyde-Wright, C.Keppel, S.E.Kuhn, J.Lichtenstadt, R.A.Miskimen, G.A.Peterson, G.G.Petratos, S.E.Rock, S.Rokni, W.K.Sakumoto, M.Spengos, K.Swartz, Z.Szalata, L.H.Tao Measurements of the Electric and Magnetic Form Factors of the Proton from Q2 = 1.75 to 8.83 (GeV/c)2 NUCLEAR REACTIONS 1H(e, e), E ≈ 9.8 GeV; measured σ(θ). 1H deduced electric, magnetic form factors. Model comparison.
doi: 10.1103/PhysRevD.50.5491
1994BO54 Phys.Rev. D49, 3091 (1994) P.E.Bosted, R.G.Arnold, C.C.Chang, J.Gomez, A.T.Katramatou, C.J.Martoff, G.G.Petratos, A.A.Rahbar, S.E.Rock, A.F.Sill, Z.M.Szalata, D.J.Sherden, J.M.Lambert, R.M.Lombard-Nelsen Threshold Inelastic Electron Scattering from the Proton at High Momentum Transfers NUCLEAR REACTIONS 1H(e, e), E ≈ threshold; measured σ, missing mass squared region; deduced structure function scaling.
doi: 10.1103/PhysRevD.49.3091
1994ED01 Phys.Rev. C50, R1749 (1994) T.Eden, R.Madey, W.-M.Zhang, B.D.Anderson, H.Arenhovel, A.R.Baldwin, D.Barkhuff, K.B.Beard, W.Bertozzi, J.M.Cameron, C.C.Chang, G.W.Dodson, K.Dow, M.Farkhondeh, J.M.Finn, B.S.Flanders, C.Hyde-Wright, W.-D.Jiang, D.Keane, J.J.Kelly, W.Korsch, S.Kowalski, R.Lourie, D.M.Manley, P.Markowitz, J.Mougey, B.Ni, T.Payerle, P.J.Pella, T.Reichelt, P.M.Rutt, M.Spraker, D.Tieger, W.Turchinetz, P.E.Ulmer, S.Van Verst, J.W.Watson, L.B.Weinstein, R.R.Whitney Electric Form Factor of the Neutron from the 2H(e(pol), e'n(pol))1H Reaction at Q2 = 0.255 (GeV/c)2 NUCLEAR REACTIONS 2H(polarized e, e'n), E=868 MeV; measured neutron polarization. 1n deduced electric form factor.
doi: 10.1103/PhysRevC.50.R1749
1994GO44 Phys.Rev. D49, 4348 (1994) J.Gomez, R.G.Arnold, P.E.Bosted, C.C.Chang, A.T.Katramatou, G.G.Petratos, A.A.Rahbar, S.E.Rock, A.F.Sill, Z.M.Szalata, A.Bodek, N.Giokaris, D.J.Sherden, B.A.Mecking, R.M.Lombard-Nelsen Measurement of the A Dependence of Deep-Inelastic Electron Scattering NUCLEAR REACTIONS 2H, 4He, C, 27Al, Ca, Fe, Ag, 197Au(e, e'X), E=8-24.5 GeV; measured σ, deep inelastic scattering; deduced mass dependence.
doi: 10.1103/PhysRevD.49.4348
1993EP01 Phys.Rev.Lett. 70, 2868 (1993) M.B.Epstein, K.A.Aniol, D.J.Margaziotis, B.Jiang, H.Baghaei, W.Bertozzi, W.Boeglin, L.Weinstein, S.Penn, J.Morrison, R.W.Lourie, J.M.Finn, C.F.Perdrisat, V.Punjabi, P.E.Ulmer, C.C.Chang, P.Boberg, J.Calarco, J.M.Laget Measurement of the R(LT), R(L), and R(T) Response Functions for the 4He(e, e'p)3H Reaction at Large Missing Momentum NUCLEAR REACTIONS 4He(e, e'p), E not given; measured σ(θ(e), θp, Ep); deduced longitudinal, transverse response functions. Model comparisons.
doi: 10.1103/PhysRevLett.70.2868
1993MA21 Phys.Rev. C48, R5 (1993) P.Markowitz, J.M.Finn, B.D.Anderson, H.Arenhovel, A.R.Baldwin, D.Barkhuff, K.B.Beard, W.Bertozzi, J.M.Cameron, C.C.Chang, G.W.Dodson, K.Dow, T.Eden, M.Farkhondeh, B.Flanders, C.Hyde-Wright, W.-D.Jiang, D.Keane, J.J.Kelly, W.Korsch, S.Kowalski, R.Lourie, R.Madey, D.M.Manley, J.Mougey, B.Ni, T.Payerle, P.Pella, T.Reichelt, P.M.Rutt, M.Spraker, D.Tieger, W.Turchinetz, P.E.Ulmer, S.Van Verst, J.W.Watson, L.B.Weinstein, R.R.Whitney, W.M.Zhang Measurement of the Magnetic Form Factor of the Neutron NUCLEAR REACTIONS 2H(e, e'n), E not given; measured en-coin. 1n deduced magnetic form factor. Associated particle technique.
doi: 10.1103/PhysRevC.48.R5
1993SA03 Phys.Rev. C47, 459 (1993) A.J.Sarty, K.G.R.Doss, G.Feldman, E.L.Hallin, R.E.Pywell, G.A.Retzlaff, D.M.Skopik, H.R.Weller, W.R.Dodge, J.W.Lightbody, Jr., J.S.O'Connell, C.C.Chang Measurement of the Reaction 3He(γ, pp)n and Its Relation to Three-Body Forces NUCLEAR REACTIONS 3He(γ, 2p), E=90-250 MeV bremsstrahlung; measured σ(θn, θp) vs neutron momentum; deduced two-pion-exchange, three-body absorption mechanisms role.
doi: 10.1103/PhysRevC.47.459
1993SI29 Phys.Rev. D48, 29 (1993) A.F.Sill, R.G.Arnold, P.E.Bosted, C.C.Chang, J.Gomez, A.T.Katramatou, C.J.Martoff, G.G.Petratos, A.A.Rahbar, S.E.Rock, Z.M.Szalata, D.J.Sherden, J.M.Lambert, R.M.Lombard-Nelsen Measurements of Elastic Electron-Proton Scattering at Large Momentum Transfer NUCLEAR REACTIONS 1H(e, e), E at GeV/c; measured σ(θ). 1H deduced magnetic, Dirac form factors.
doi: 10.1103/PhysRevD.48.29
1993WE01 Phys.Rev. C47, 225 (1993) L.B.Weinstein, J.Morrison, A.Perry, H.Baghaei, W.Bertozzi, W.U.Boeglin, J.M.Finn, J.Glickman, C.E.Hyde-Wright, N.Kalantar-Nayestanaki, R.W.Lourie, J.A.Nelson, S.Penn, W.W.Sapp, C.P.Sargent, P.E.Ulmer, B.H.Cottman, L.Ghedira, E.J.Winhold, J.R.Calarco, J.Wise, P.Boberg, C.C.Chang, N.S.Chant, P.G.Roos, D.Chang, K.Aniol, M.B.Epstein, D.J.Margaziotis, C.Perdrisat, V.Punjabi, R.Whitney N(*) Electroproduction and Propagation in Nuclei NUCLEAR REACTIONS 12C(γ, π-X), E=virtual bremsstrahlung; measured σ vs missing energy with p-emission; deduced N(*)-nucleus interaction features.
doi: 10.1103/PhysRevC.47.225
1992BO34 Phys.Rev. C46, 2505 (1992) P.E.Bosted, A.Lung, L.Andivahis, L.M.Stuart, J.Alster, R.G.Arnold, C.C.Chang, F.S.Dietrich, W.Dodge, R.Gearhart, J.Gomez, K.A.Griffioen, R.S.Hicks, C.E.Hyde-Wright, C.Keppel, S.E.Kuhn, J.Lichtenstadt, R.A.Miskimen, G.A.Peterson, G.G.Petratos, S.E.Rock, S.Rokni, W.K.Sakumoto, M.Spengos, K.Swartz, Z.Szalata, L.H.Tao Measurements of (ν)W2 and R = σ(L)/σ(T) from Inelastic Electron-Aluminum Scattering Near x = 1 NUCLEAR REACTIONS 27Al(e, e'X), E=1.5-5.5 GeV; measured inclusive σ per nucleon, ratio to 2H; deduced σ(L)/σ(T) vs Q2.
doi: 10.1103/PhysRevC.46.2505
1991BO21 Nucl.Phys. A527, 339c (1991) P.E.Bosted, L.Clogher, A.Lung, L.Stuart, J.Alster, R.G.Arnold, C.C.Chang, F.Dietrich, W.R.Dodge, R.Gearhart, J.Gomez, K.Griffioen, R.Hicks, C.Hyde-Wright, C.Keppel, S.Kuhn, J.Lichtenstadt, R.Miskimen, G.G.Petratos, G.A.Peterson, S.E.Rock, S.H.Rokni, W.K.Sakumoto, K.Swartz, Z.N.Szalata, L.H.Tao New Measurements of the Electric and Magnetic Elastic Form Factors of the Proton and Neutron at High Momentum Transfers NUCLEAR REACTIONS 1H(e, e'), E=1.4-10 GeV; measured electron spectra. 1H deduced magnetic form factor.
doi: 10.1016/0375-9474(91)90123-N
1991WE10 Nucl.Phys. A527, 348c (1991) L.B.Weinstein, H.Baghaei, W.Bertozzi, J.M.Finn, J.Glickman, C.E.Hyde-Wright, N.Kalantar-Nayestanaki, R.W.Lourie, J.A.Nelson, W.W.Sapp, C.P.Sargent, P.E.Ulmer, B.H.Cottman, L.Ghedira, E.J.Winhold, J.R.Calarco, J.Wise, P.Boberg, C.C.Chang, D.Zhang, D.Zhang, K.Aniol, M.B.Epstein, D.J.Margaziotis, C.Perdrisat, V.Punjabi Non-Single-Particle Interactions at Quasi-Elastic Kinematics NUCLEAR REACTIONS 12C(e, e'p), E=460 MeV; measured σ(θp, θ(e')) vs missing energy; deduced deeply bound deuteron knockout. Compiled, reviewed other data.
doi: 10.1016/0375-9474(91)90124-O
1990WE06 Phys.Rev.Lett. 64, 1646 (1990) L.B.Weinstein, H.Baghaei, W.Bertozzi, J.M.Finn, J.Glickman, C.E.Hyde-Wright, N.Kalantar-Nayestanaki, R.W.Lourie, J.A.Nelson, W.W.Sapp, C.P.Sargent, P.E.Ulmer, B.H.Cottman, L.Ghedira, E.J.Winhold, J.R.Calarco, J.Wise, P.Boberg, C.C.Chang, D.Zhang, K.Aniol, M.B.Epstein, D.J.Margaziotis, C.Perdrisat, V.Punjabi Quasielastic Reaction Mechanism Studied Using the Reaction 12C(e, e'p) NUCLEAR REACTIONS 12C(e, e'p), E not given; measured missing energy spectra; deduced subshell spectroscopic factors.
doi: 10.1103/PhysRevLett.64.1646
1989NA10 Phys.Rev. C40, 1130 (1989) A.Nadasen, P.G.Roos, N.S.Chant, C.C.Chang, G.Ciangaru, H.F.Breuer, J.Wesick, E.Norbeck (p, pα) Cluster-Knockout Reaction on 9Be at 200 MeV NUCLEAR REACTIONS 9Be(p, pα), E=200 MeV; measured σ(E1, E2, θ1, θ2). 9Be deduced α-cluster knockout spectroscopic factors. DWIA analysis.
doi: 10.1103/PhysRevC.40.1130
1987LA11 Phys.Rev. C35, 1214 (1987) F.L.Lang, C.W.Werntz, C.J.Crannell, J.I.Trombka, C.C.Chang Cross Sections for Production of the 15.10-MeV and Other Astrophysically Significant Gamma-Ray Lines through Excitation and Spallation of 12C and 16O with Protons NUCLEAR REACTIONS, ICPND 12C, 16O(p, γ), E=40, 65, 85 MeV; measured Eγ, Iγ, γ production σ(E). Other data input.
doi: 10.1103/PhysRevC.35.1214
1987WI09 Phys.Rev. C35, 1734 (1987) J.S.Winfield, N.Anantaraman, S.M.Austin, Ziping Chen, A.Galonsky, J.van der Plicht, H.-L.Wu, C.C.Chang, G.Ciangaru Mechanism of the (6Li, 6He) Reaction at Intermediate Energies and Its Suitability as a Spin Probe NUCLEAR REACTIONS 7Li, 12,14C, 26Mg, 90Zr(6Li, 6He), E=14, 25, 35 MeV/nucleon; measured σ(E(6He)), σ(θ); deduced reaction mechanism. 7Be, 12,14C, 27Al, 90Zr deduced Gamow-Teller transition strengths, level excitation mechanism. Magnetic spectrometer. DWBA analyses.
doi: 10.1103/PhysRevC.35.1734
1986AN29 Phys.Rev.Lett. 57, 2375 (1986) N.Anantaraman, J.S.Winfield, S.M.Austin, A.Galonsky, J.van der Plicht, C.C.Chang, G.Ciangaru, S.Gales (6Li, 6He) Reaction as a Probe of Spin-Transfer Strength NUCLEAR REACTIONS 7Li, 12,14C, 26Mg, 90Zr(6Li, 6He), E=210 MeV; measured σ(E(6He)), σ(θ). 7Be, 12,14N, 26Al, 90Nb levels deduced σ, Gamow-Teller transition strength correlation. Spectrograph, focal plane detector. DWBA calculations.
doi: 10.1103/PhysRevLett.57.2375
1985RO12 Nucl.Phys. A439, 721 (1985) G.Roche, J.Carroll, C.C.Chang, T.Hallman, P.N.Kirk, R.Koontz, G.Krebs, L.Madansky, T.Mulera, H.G.Pugh, L.S.Schroeder, J.Vicente Particle-Gamma Coincidence Measurements in 12C + 12C and 12C + Pb Collisions at 2.1 GeV/Nucleon Incident Energy NUCLEAR REACTIONS Pb, 12C(12C, pγ), (12C, dγ), E=2.1 GeV/nucleon; measured σ(Eγ), σ(Ep), σ(Ed), invariant mass σ.
doi: 10.1016/0375-9474(85)90335-5
1985WE12 Phys.Rev. C32, 1474 (1985) J.S.Wesick, P.G.Roos, N.S.Chant, C.C.Chang, A.Nadasen, L.Rees, N.R.Yoder, A.A.Cowley, S.J.Mills, W.W.Jacobs 2H, 3,4He(p(pol), p') and 3,4He(p(pol), d') Continuum Yields for 100 and 150 MeV Protons NUCLEAR REACTIONS 2H, 3,4He(polarized p, p'), 3,4He(polarized p, d), E=100, 150 MeV; measured inclusive σ(θ), analyzing power vs θ; deduced reaction mechanism. DWIA analysis.
doi: 10.1103/PhysRevC.32.1474
1984AR02 Phys.Rev.Lett. 52, 727 (1984) R.G.Arnold, P.E.Bosted, C.C.Chang, J.Gomez, A.T.Katramatou, G.G.Petratos, A.A.Rahbar, S.E.Rock, A.F.Sill, Z.M.Szalata, A.Bodek, N.Giokaris, D.J.Sherden, B.A.Mecking, R.M.Lombard Measurements of the A Dependence of Deep-Inelastic Electron Scattering from Nuclei NUCLEAR REACTIONS 2H, He, 9Be, C, 27Al, Ca, Fe, Ag, 197Au(e, e'), E=8-24.5 GeV; measured deep inelastic σ per nucleon; deduced mass dependence.
doi: 10.1103/PhysRevLett.52.727
1984CI03 Phys.Rev. C29, 1289 (1984) G.Ciangaru, C.C.Chang, H.D.Holmgren, A.Nadasen, P.G.Roos Three-Body Approach to the Multiple Scattering Direct Reactions: Pragmatic application to the 58Ni(p, 2p)57Co continuum NUCLEAR REACTIONS 58Ni(p, 2p), E=198 MeV; calculated σ(θ1, θ2, E1), σ(θ1, θ2, E1, E2). Multi-step direct process, three-body approach.
doi: 10.1103/PhysRevC.29.1289
1984CI04 Phys.Rev. C29, 2017 (1984) G.Ciangaru, C.C.Chang, J.R.Wu, R.W.Koontz, H.D.Holmgren Nuclear States of 28Si and 28Al from (α, t) and (α, h) Reactions at 80 MeV NUCLEAR REACTIONS 27Al(α, t), (α, 3He), E=80 MeV; measured σ(θ), σ(Et), σ(E(3He)); deduced optical model parameters. 28Si, 28Al levels deduced L, spectroscopic factors. Finite-range DWBA, shell model wave functions.
doi: 10.1103/PhysRevC.29.2017
1984TA11 Nucl.Phys. A422, 12 (1984) S.L.Tabor, G.Neuschaefer, J.A.Carr, F.Petrovich, C.C.Chang, A.Guterman, M.T.Collins, D.L.Friesel, C.Glover, S.Y.Van Der Werf, S.Raman The (3He, t) Reaction at 197 MeV on 12C, 24Mg, 28Si and 40Ca NUCLEAR REACTIONS 12C, 24Mg, Si, 40Ca(3He, t), E=197 MeV; measured σ(Et), θ=15°. 12N, 24Al, 28P, 40Sc deduced levels, isovector GDR analog. Enriched target. 40Ca(3He, 3He), E=197 MeV; measured σ(θ); deduced optical-model parameters. Enriched target. 40Ca(3He, 3He'), E=197 MeV; measured σ(θ). 40Ca levels deduced deformation parameters, isoscalar GQR. Enriched target. Macroscopic and microscopic DWA. 40Ca(3He, t), E=197 MeV; measured σ(θ). 40Sc deduced levels, GDR, isovector GQR analog. Enriched target. Macroscopic and microscopic DWA.
doi: 10.1016/0375-9474(84)90429-9
1983CA14 Phys.Rev. C28, 483 (1983); Erratum Phys.Rev. C29, 672 (1983) J.R.Calarco, S.S.Hanna, C.C.Chang, E.M.Diener, E.Kuhlmann, G.A.Fisher Absolute Cross Section for the Reaction 3H(p, γ0)4He and a Review of 4He(γ, p0)3H Measurements NUCLEAR REACTIONS 3H(p, γ0), E=8.34, 13.6 MeV; measured σ(θ=90°).
doi: 10.1103/PhysRevC.28.483
1983CI02 Phys.Rev. C27, 1360 (1983) G.Ciangaru, C.C.Chang, H.D.Holmgren, A.Nadasen, P.G.Roos, A.A.Cowley, S.Mills, P.P.Singh, M.K.Saber, J.R.Hall Continuum Spectrum in the Quasifree (p, 2p) Scattering NUCLEAR REACTIONS 58Ni(p, 2p), E=198 MeV; measured σ(θ1, E2, θ2, E2); deduced reaction mechanism. DWIA calculations, quasifree particle rescattering effect.
doi: 10.1103/PhysRevC.27.1360
1983GU04 Phys.Rev. C27, 1521 (1983) A.Guterman, G.Ciangaru, C.C.Chang, J.D.Silk, D.L.Hendrie, T.J.M.Symons, J.Mahoney Giant Resonance Excitation in the 27Al(6Li, 6He)27Si Reaction at 93 MeV NUCLEAR REACTIONS 27Al(6Li, 6He), E=93 MeV; measured σ(θ), σ(E(6He)). 27Si deduced levels, giant resonance multipolarity.
doi: 10.1103/PhysRevC.27.1521
1983KA13 Phys.Rev. C28, 105 (1983) A.M.Kalenda, B.D.Anderson, A.R.Baldwin, R.Madey, J.W.Watson, C.C.Chang, H.D.Holmgren, R.W.Koontz, J.R.Wu, H.Machner Energy and Angular Distributions of Neutrons from 90 MeV Proton and 140 MeV Alpha-Particle Bombardment of Nuclei NUCLEAR REACTIONS 27Al, 58Ni, 90Zr, 209Bi(p, n), E=90 MeV; 27Al, 58Ni, 90Zr, 209Bi(α, n), E=140 MeV; measured σ(θ, En); deduced reaction mechanisms. Plane wave impulse approximation, quasifree scattering, preequilibrium exciton, intranuclear cascade, geometry dependent hybrid models, (p, p') data comparison.
doi: 10.1103/PhysRevC.28.105
1982TA05 Phys.Rev. C25, 1253 (1982) S.L.Tabor, C.C.Chang, M.T.Collins, G.J.Wagner, J.R.Wu, D.W.Halderson, F.Petrovich Survey of the (3He, t) Reaction: Excitation of the isobaric analog of the giant dipole resonance NUCLEAR REACTIONS 12C, 16O, 27Al, 28Si, 40Ca, 46Ti, 90Zr(3He, t), (3He, 3He'), E=130, 170 MeV; measured σ(Et), σ(E(3He)), σ(θ). 16O, 27Al, 28Si, 40Ca, 46Ti, 90Zr deduced T=0, GQR. 12N, 16F, 27Si, 28P, 40Sc, 46V, 90Nb deduced IAS of T=1, GDR.
doi: 10.1103/PhysRevC.25.1253
1981AN01 Phys.Rev.Lett. 46, 226 (1981) B.D.Anderson, A.R.Baldwin, A.M.Kalenda, R.Madey, J.W.Watson, C.C.Chang, H.D.Holmgren, R.W.Koontz, J.R.Wu Proton and Neutron Inclusive Spectra and the Importance of the Single Nucleon-Nucleon Scattering Process NUCLEAR REACTIONS 27Al, 58Ni, 90Zr, 209Bi(p, pX), (p, nX), E=90 MeV; measured σ(En, θ), σ(Ep, θ); deduced nucleon-nucleon scattering mechanism dominance. PWIA, quasifree scattering calculation.
doi: 10.1103/PhysRevLett.46.226
1981CO16 Phys.Rev. C24, 387 (1981) M.T.Collins, C.C.Chang, S.L.Tabor Decay Modes of the Isoscalar Giant Quadrupole Resonance in the Zn Isotopes NUCLEAR REACTIONS 64,66,68Zn(α, αp), (α, αn), (α, 2α), E=160 MeV; measured σ(θ1, E1, θ2, E2). 64,66,68Zn deduced GQR decay branching ratios. Statistical model.
doi: 10.1103/PhysRevC.24.387
1980CO17 Phys.Rev. C22, 2633 (1980) A.A.Cowley, C.C.Chang, H.D.Holmgren Forward-Angle Proton Spectra in the Continuum from the 58Ni(p, xp) Reaction at 100 MeV NUCLEAR REACTIONS 58Ni(p, xp), E=100 MeV; measured σ(θ, Ep); deduced quasi-free nucleon-nucleon scattering effects.
doi: 10.1103/PhysRevC.22.2633
1980CO19 Phys.Rev.Lett. 45, 1930 (1980) A.A.Cowley, C.C.Chang, H.D.Holmgren, J.D.Silk, D.L.Hendrie, R.W.Koontz, P.G.Roos, C.Samanta, J.R.Wu Energy Dissipation Process for 100-MeV Protons and the Nucleon-Nucleon Interactions in Nuclei NUCLEAR REACTIONS 58Ni(p, 2p), E=100 MeV; measured pp-coin, σ(Ep1, Ep2, θ1, θ2); deduced reaction mechanism, energy dissipation process. DWIA analysis, quasifree scattering.
doi: 10.1103/PhysRevLett.45.1930
1979CO07 Phys.Rev.Lett. 42, 1440 (1979) M.T.Collins, C.C.Chang, S.L.Tabor, G.J.Wagner, J.R.Wu Decay Modes of the Isoscalar Giant Quadrupole Resonance in 58Ni NUCLEAR REACTIONS 58Ni(α, α'), (α, α'p), (α, α'n), (α, 2α), E=140 MeV; measured σ(Eα'), α'p-coin, α'n-coin, α'α-coin. 58Ni deduced branching ratios for α, p decay of GQR. Continuum, statistical model analysis.
doi: 10.1103/PhysRevLett.42.1440
1979GL01 Phys.Rev. C19, 1577 (1979) M.D.Glascock, W.F.Hornyak, C.C.Chang, R.J.Quickle Reaction 27Al + α at E = 140 Mev: I NUCLEAR REACTIONS 27Al(α, p), (α, d), (α, t), (α, 3He), (α, α'), (α, γ), E=140 MeV; measured Eγ, σγ, Doppler broadening, σ(Ep, θp), σ(Ed, θd), σ(Et, θt), σ(E(3He), θ(3He)), σ(Eα, θα); deduced reaction mechanism. Ge(Li) detector.
doi: 10.1103/PhysRevC.19.1577
1979HO31 Phys.Rev. C19, 1595 (1979) W.F.Hornyak, M.D.Glascock, C.C.Chang, J.R.Wu Reaction 27Al + α at Eα = 140 MeV: II NUCLEAR REACTIONS 27Al(α, X), E=140 MeV; measured fragment σ(θ, E); deduced fragment velocities, reaction mechanism, model characteristics. Monte Carlo, exciton model calculations.
doi: 10.1103/PhysRevC.19.1595
1979KO32 Phys.Rev.Lett. 43, 1862 (1979) R.W.Koontz, C.C.Chang, H.D.Holmgren, J.R.Wu Projectile Fragmentation Processes in 35-MeV/amu (α, xy) Reactions NUCLEAR REACTIONS 90Zr(α, pt), (α, 2d), (α, pX), E=35 MeV/nucleon; measured fragment-fragment (θ), (fragment)(fragment)-coin; deduced reaction mechanism.
doi: 10.1103/PhysRevLett.43.1862
1979VE02 Phys.Rev. C19, 1705 (1979) E.Ventura, J.R.Calarco, C.C.Chang, E.M.Diener, D.G.Mavis, S.S.Hanna, G.A.Fisher Structure in the Giant Resonance Region of 16O Observed with the Reaction 13C(3He, γ)16O NUCLEAR REACTIONS 13C(3He, γ), E=3.0-8.5 MeV; measured σ(E(3He), Eγ, θ). 16O deduced resonances, structure in giant resonance region. Enriched 13C target.
doi: 10.1103/PhysRevC.19.1705
1979WA11 Phys.Rev. C20, 1079 (1979) N.S.Wall, J.R.Wu, C.C.Chang, H.D.Holmgren Medium Energy Nuclear Reactions: 'Quasi-Two-Body Scaling' and 'Hot Spots' NUCLEAR REACTIONS 27Al, 58Ni, 90Zr, 209Bi(p, p), (p, d), (p, t), (p, α), E=90 MeV; 27Al, 58Ni, 90Zr, 209Bi(α, p), (α, d), (α, t), (α, α), E=140 MeV; calculated energy spectra; deduced characteristic parameter. Quasi two-body scaling, hot spot interpretation.
doi: 10.1103/PhysRevC.20.1079
1979WU02 Phys.Rev. C19, 370 (1979) J.R.Wu, C.C.Chang, H.D.Holmgren Charged-Particle Spectra: 80 MeV Deuterons on 27Al and 58Ni and 70 MeV Deuterons on 90Zr, 208Pb, and 232Th NUCLEAR REACTIONS 27Al, 58Ni, 90Zr, 208Pb, 232Th(d, pX), (d, dX), (d, tX), (d, 3HeX), (d, αX), E=70, 80 MeV; measured σ(θp, Ep), σ(θd, Ed), σ(θt, Et), σ(θ(3He), E(3He)), σ(θα, Eα); deduced σ(E). Comparison with preequilibrium exciton, compound nuclear evaporation, deuteron breakup model.
doi: 10.1103/PhysRevC.19.370
1979WU03 Phys.Rev. C19, 659 (1979) J.R.Wu, C.C.Chang, H.D.Holmgren Charged Particle Spectra: 140 MeV α Particle Bombardment of 27Al, 58Ni, 90Zr, 209Bi, and 232Th NUCLEAR REACTIONS 27Al, 58Ni, 90Zr, 209Bi, 232Th(α, pX), (α, dX), (α, 3HeX), (α, αX), E=140 MeV; measured σ(Ep, θp), σ(Ed, θd), σ(Et, θt), σ(E(3He), θ(3He)), σ(Eα, θα); comparison with preequilibrium exciton, evaporation, projectile breakup models.
doi: 10.1103/PhysRevC.19.659
1979WU04 Phys.Rev. C19, 698 (1979) J.R.Wu, C.C.Chang, H.D.Holmgren Charged-Particle Spectra: 90 MeV Protons on 27Al, 58Ni, 90Zr, and 209Bi NUCLEAR REACTIONS 27Al, 90Zr, 209Bi(p, pX), (p, dX), (p, tX), (p, 3HeX), (p, αX), E=90 MeV; 58Ni(p, pX), (p, dX), (p, tX), (p, 3HeX), (p, αX), E=90, 100 MeV; measured σ(Ep, θp), σ(Ed, θd), σ(Et, θt), σ(E(3He), θ(3He)), σ(Eα, θα). Comparison with pre-equilibrium exciton, evaporation models.
doi: 10.1103/PhysRevC.19.698
1979WU09 Phys.Rev. C20, 1284 (1979) J.R.Wu, C.C.Chang, H.D.Holmgren, R.W.Koontz Alpha-Particle Breakup at Incident Energies of 20 and 40 MeV/Nucleon NUCLEAR REACTIONS 27Al, 58Ni, 90Zr, 209Bi(α, p), (α, d), (α, t), (α, 3He), E=80, 160 MeV; measured differential energy spectra; deduced α breakup yield, reaction mechanism. Plane wave model.
doi: 10.1103/PhysRevC.20.1284
1978LE01 Phys.Rev. C17, 410 (1978) B.T.Leemann, H.G.Pugh, N.S.Chant, C.C.Chang d + d Four-Body Breakup Reaction at 80 MeV NUCLEAR REACTIONS 2H(d, 2n2p), E=80 MeV; measured σ(Ep1, θ1, Ep2, θ2). Coplanar geometry, PWBA analysis.
doi: 10.1103/PhysRevC.17.410
1978WU02 Phys.Rev.Lett. 40, 1013 (1978) J.R.Wu, C.C.Chang, H.D.Holmgren Breakup of α Particles in the Fields of Nuclei NUCLEAR REACTIONS 209Bi, 58Ni, 90Zr, 120Sn, 232Th(α, p), (α, d), (α, t), (α, 3He), E=140 MeV; analyzed α-particle breakup.
doi: 10.1103/PhysRevLett.40.1013
1978WU03 Phys.Rev. C17, 1540 (1978) Complex-Particle Emission in the Pre-Equilibrium Exciton Model NUCLEAR REACTIONS 12C, 16O, 27Al, 54Fe, 89Y, 120Sn, 197Au, 209Bi(p, X), E=62 MeV; 54Fe(p, X), E=29, 39 MeV; 58Ni(p, X), E=90 MeV; calculated σ. Pre-equilibrium exciton model.
doi: 10.1103/PhysRevC.17.1540
1977FR11 Phys.Rev. C16, 603 (1977) N.Frascaria, J.P.Didelez, N.S.Chant, C.C.Chang High Spin States in 206,204,202Tl Observed in (d, α) Reactions at 80 MeV NUCLEAR REACTIONS 204,206,208Pb(d, α), E=80 MeV; measured σ(θ). 202,204,206Tl levels deduced L, J, π. Microscopic DWBA analysis, shell model calculations.
doi: 10.1103/PhysRevC.16.603
1977WA05 Nucl.Phys. A281, 418 (1977) C.N.Waddell, E.M.Diener, R.G.Allas, L.A.Beach, R.O.Bondelid, E.L.Petersen, A.G.Pieper, R.B.Theus, C.C.Chang, N.S.Chant Study of the (p, pn) Reaction in Light Nuclei NUCLEAR REACTIONS 2H, 6,7Li, 9Be(p, pn), E=45, 47 MeV; measured excitation energy, energy sharing spectra. 6Be deduced energy levels (15.5, 24 MeV), parentage. PWIA, DWIA calculations.
doi: 10.1016/0375-9474(77)90506-1
1977WU02 Phys.Rev. C16, 1812 (1977) Pre-Equilibrium Particle Decay in the Photonuclear Reactions NUCLEAR REACTIONS 27Al, 63Cu, 115In, 118Sn, 181Ta, 207Pb, 209Bi, 235U(γ, X), E=55, 85 MeV; 12C(γ, X), E=110 MeV; 127I(γ, xn), E=50, 100, 150 MeV; calculated σ.
doi: 10.1103/PhysRevC.16.1812
1976BH02 Phys.Rev. C13, 2105 (1976) R.K.Bhowmik, C.C.Chang, J.-P.Didelez, H.D.Holmgren (p, 2p) Reaction on 7Li and 12C at 100 MeV NUCLEAR REACTIONS 7Li, 12C(p, 2p), E=100 MeV; measured σ(Ep), pp(θ); deduced distorted recoil momentum distributions. Separation energy resolution 0.8 MeV; DWIA analysis.
doi: 10.1103/PhysRevC.13.2105
1976CH04 Nucl.Phys. A258, 91 (1976) C.C.Chang, E.M.Diener, E.Ventura Study of the 14C(τ, γ)17O Radiative Capture Reaction from 3.2 to 7.5 MeV NUCLEAR REACTIONS 14C(3He, γ), E=3.2-7.5 MeV; measured σ(E, Eγ, θ). 17O deduced resonances, L, J, π, λ. Enriched 14C target.
doi: 10.1016/0375-9474(76)90530-3
1976DI05 Phys.Rev. C13, 1388 (1976) J.-P.Didelez, C.C.Chang, N.S.Chant, H.D.Holmgren, R.I.Steinberg, J.R.Wu Analysis of the 12C(d, 3He)11B(g.s.) Reaction at 80 MeV NUCLEAR REACTIONS 12C(d, 3He), E=80 MeV; calculated σ(θ). 11B deduced S. DWBA.
doi: 10.1103/PhysRevC.13.1388
1976WU01 Phys.Lett. 60B, 423 (1976) Pre-Equilibrium Decay in the Exciton Model NUCLEAR REACTIONS 54Fe(p, p'X), E=39, 62 MeV; calculated pre-equilibrium decay.
doi: 10.1016/0370-2693(76)90697-3
1975CH01 Phys.Rev.Lett. 34, 221 (1975) C.C.Chang, F.E.Bertrand, D.C.Kocher Isolation of the Giant Quadrupole Resonance in 58Ni via Deuteron Inelastic Scattering NUCLEAR REACTIONS 58Ni(d, d'), E=46, 70 MeV; measured σ(Ed', θ). 58Ni resonance deduced E2 nature.
doi: 10.1103/PhysRevLett.34.221
1974BH03 Nucl.Phys. A226, 365 (1974) R.K.Bhowmik, C.C.Chang, P.G.Roos, H.D.Holmgren The 6Li(p, 2p)5He Reaction at 100 MeV NUCLEAR REACTIONS 6Li(p, 2p), E=100 MeV; measured σ(E1, E2, θ(1), θ(2)). Enriched target.
doi: 10.1016/0375-9474(74)90489-8
1974CH13 Phys.Rev. C9, 1300 (1974) C.C.Chang, W.R.Dodge, J.J.Murphy, II 3He(γ, d)1H Cross Section from 10 to 21 MeV NUCLEAR REACTIONS 3He(e, d), Eγ=10-21 MeV; measured σ(Eγ, 90°).
doi: 10.1103/PhysRevC.9.1300
1974CH15 Phys.Rev. C9, 1671 (1974) 3H(3He, n)5Li Reaction from 14 to 26 MeV NUCLEAR REACTIONS 3H(3He, n), E=14-26 MeV; measured σ(E, θ). 6Li deduced resonance. Adsorbed 3H target.
doi: 10.1103/PhysRevC.9.1671
1974CH48 Phys.Rev.Lett. 33, 1493 (1974) C.C.Chang, N.S.Wall, Z.Fraenkel Gamma Rays Observed from 100-MeV Protons Interacting with 56Fe and 58Ni NUCLEAR REACTIONS 56Fe, 58Ni(p, X), E=100 MeV; measured σ(Eγ).
doi: 10.1103/PhysRevLett.33.1493
1974VE01 Nucl.Phys. A219, 157 (1974) E.Ventura, J.Calarco, C.C.Chang, E.M.Diener, E.Kuhlmann, W.E.Meyerhof Resonant Structure Observed in the 3He(3He, γ)6Be Capture Reaction NUCLEAR REACTIONS 3He(3He, γ), E=12-27 MeV; measured σ(E, θ). 6Be deduced resonances, J, π, L. Results compared with theoretical predictions. Enriched 3He gas target.
doi: 10.1016/0375-9474(74)90089-X
1973CH35 Nucl.Phys. A212, 189 (1973) C.C.Chang, H.F.Glavish, R.Avida, R.N.Boyd Elastic Scattering of Vector Polarized Deuterons by 4He NUCLEAR REACTIONS 4He(polarized d, d), E=11.5-17 MeV; measured vector analyzing power iT11(E, θ).
doi: 10.1016/0375-9474(73)90044-4
1973DI17 Nucl.Instrum.Methods 109, 585 (1973) Reduction of Neutron-Induced Background in NaI γ-Ray Spectra NUCLEAR REACTIONS 2H(p, γ); analyzed Eγ spectra.
doi: 10.1016/0029-554X(73)90579-X
1973GL01 Phys.Rev.Lett. 30, 391 (1973) H.F.Glavish, R.Avida, S.S.Hanna, E.Diener, R.N.Boyd, C.C.Chang Measurement of Multipole Mixing in Nuclear Radiation by a New Method NUCLEAR REACTIONS 24Mg(polarized p, p'γ), E=8-10 MeV; measured Iγ(θ). 24Mg deduced γ-mixing. vector polarized beam.
doi: 10.1103/PhysRevLett.30.391
1972CH22 Phys.Rev.Lett. 29, 307 (1972) C.C.Chang, E.M.Diener, E.Ventura Evidence for an Anomaly in the Excitation Function of the Reaction 2H(p, γ)3He NUCLEAR REACTIONS 2H(p, γ), E=10-17.5 MeV; measured σ(E;Eγ). 3He deduced resonance, level-width.
doi: 10.1103/PhysRevLett.29.307
1972GL01 Phys.Rev.Lett. 28, 766 (1972) H.F.Glavish, S.S.Hanna, R.Avida, R.N.Boyd, C.C.Chang, E.Diener Giant Dipole Resonances in 12C Observed with the Polarized Proton Capture Reaction NUCLEAR REACTIONS 11B(polarized p, γ), E=6-14 MeV; measured analyzing power(E;θ). 12C deduced giant E1 resonance configurations.
doi: 10.1103/PhysRevLett.28.766
1972HA52 Phys.Lett. 40B, 631 (1972) S.S.Hanna, H.F.Glavish, E.M.Diener, J.R.Calarco, C.C.Chang, R.Avida, R.N.Boyd The Giant Dipole Resonance in 16O Observed with the Polarized Proton Capture Reaction NUCLEAR REACTIONS 15N(polarized p, γ), E=7.4-15 MeV; measured σ(E), analyzing power(E;θ). 16O deduced giant E1 resonance structure.
doi: 10.1016/0370-2693(72)90614-4
1971VE10 Nucl.Phys. A173, 1 (1971) E.Ventura, C.C.Chang, W.E.Meyerhof The 3H(3He, γ)6Li Capture Reaction and the Structure of 6Li NUCLEAR REACTIONS 3H(3He, γ), E=9-26 MeV; measured σ(E, θ). 6Li deduced resonances. Results compared with theoretical predictions. Adsorbed 3H target.
doi: 10.1016/0375-9474(71)90744-5
1971WA21 Nucl.Phys. A173, 634 (1971) B.A.Watson, C.C.Chang, M.Hasinoff T = 3/2 States in 11C NUCLEAR REACTIONS 11B(3He, t), (3He, 3He'), E=29.8; 9Be(3He, n), E=8 MeV; 10B(p, p), E=3.5-5 MeV; measured reaction products .11C; deduced σ(ef), σ(E(3He'), σ(En)), σ(E;Ep', θ), T=3/2 levels, level-width.
doi: 10.1016/0375-9474(71)90976-6
1971WA31 Particles Nucl. 2, 376 (1971) B.A.Watson, C.C.Chang, S.L.Tabor Reactions Induced by the Bombardment of 40Ca with 70 MeV 16O Ions NUCLEAR REACTIONS 40Ca(16O, X), E=70 MeV; measured σ, charged particle spectra.
1971WE05 Lett.Nuovo Cim. 1, 25 (1971) L.C.Welch, C.C.Chang, H.H.Forster, C.C.Kim, D.W.Devins An Experimental Study of the 14N(p, pd)12C (g.s.) And 14N(p, pd)12C (4.4 Mev) Quasi-Elastic Reactions at 46 MeV NUCLEAR REACTIONS 14N(p, pd), E=46 MeV; measured σ(Ep, Ed, θ(p), θ(d)).
doi: 10.1007/BF02785042
1970CH13 Nucl.Instrum.Methods 79, 129 (1970) Determination of Excitation Energy of Levels and Incident Beam Energy Using a Minimum Chi-Squared Technique NUCLEAR REACTIONS 14N(p, t), (p, 3He), (p, α), E=46 MeV; measured σ(Et, θ), σ(E(3He), θ), σ(Eα, θ). 11,12C, 12N duduced levels.
doi: 10.1016/0029-554X(70)90017-0
1970WE07 Lett.Nuovo Cimento 3, 344 (1970) L.C.Welch, C.C.Chang, C.C.Kim, H.H.Forster An Attempt to Observe (p, 2p) Events from the 1h9/2 State of 209Bi NUCLEAR REACTIONS 12C, 209Bi(p, 2p), E=44 MeV; measured σ(Ep1, Ep2).
doi: 10.1007/BF02755709
1970WE09 Nucl.Phys. A158, 644 (1970) L.C.Welch, C.C.Chang, H.H.Forster, C.C.Kim, D.W.Devins, P.A.Deutchman A Study of the 14N(p, 2p)13C Reaction at 46 MeV NUCLEAR REACTIONS 14N(p, 2p), E=46 MeV; measured σ(Ep, θ).
doi: 10.1016/0375-9474(70)90212-5
1969CH22 Nucl.Phys. A136, 337 (1969) C.C.Chang, E.Bar-Avraham, H.H.Forster, C.C.Kim, P.Tomas, J.W.Verba Proton-Proton Final State Interaction in the p + 3He Reaction NUCLEAR REACTIONS 3He(p, d)2p, 3He(p, pd)p, E = 30, 46 MeV; measured σ(E;Ed, θ(d)), σ(Ep, θ(p), θ(d)) σ(Ed, θ(p), θ(d)); deduced proton pairs (internal energy E(2p) approx 0.4 MeV). Enriched target.
doi: 10.1016/0375-9474(69)90058-X
1968CH29 Phys.Letters 28B, 175 (1968) C.C.Chang, E.Bar-Avraham, H.H.Forster, C.C.Kim, J.R.Richardson, P.Tomas, J.W.Verba Proton-Proton Final State Interaction in the 3He(p, pd)p reaction NUCLEAR REACTIONS 3He(p, pd), E=46.5 MeV; measured σ(Ep, Ed, θ(p), θ(d)).
doi: 10.1016/0370-2693(68)90009-9
1968HS03 Chinese J.Phys. 6, 1(1968) Y.-C.Hsu, C.-Y.Huang, C.-C.Chang Energy and Angular Distribution of Alpha Particles in the 14N(n, α)11B Reaction at 14.1 MeV NUCLEAR REACTIONS 14N(n, α), E = 14.1 MeV; measured σ(Eα, θ). Deduced reaction mechanism.
1967HS04 Nucl.Phys. A104, 677(1967) Y.-C.Hsu, C.-Y.Huang, C.-C.Chang Angular Distributions of Alpha Particles from the Reaction 16O(n, α)13Cat E = 14.1 MeV NUCLEAR REACTIONS 16O(n, α), En=14.1 MeV; measured σ(Eα, θ). Natural target.
doi: 10.1016/0375-9474(67)90481-2
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