NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = L.Heilbronn Found 60 matches. 2023BU09 Phys.Rev. C 108, 024609 (2023) N.Burahmah, J.R.Griswold, L.H.Heilbronn, L.A.Bernstein, A.S.Voyles, J.T.Morrell, M.Zach, R.Copping 229Pa cross section measurements via deuteron irradiation of 232Th NUCLEAR REACTIONS 232Th(d, n)233Pa, 232Th(d, 2n)232Pa, 232Th(d, 4n)230, Pa232Th(d, 5n)229Pa, 232Th(d, 6n)228Pa, E=31.0, 35.2, 41.4, 49.6 MeV; measured Eγ, Iγ; deduced σ(E). Comparison other experimental data and to the calculations made with TALYS-1.9, EMPIRE-3.2.3, CoH-3.5.4, PHITS-3.1 and ALICE-2020 codes. Irradiation took place at the Lawrence Berkeley National Laboratory 88-Inch Cyclotron. Isotope of Pa in the irradiated target was chemically separated and activity was measured with HPGe coaxial detector at Oak Ridge National Laboratory.
doi: 10.1103/PhysRevC.108.024609
2023RA13 Nucl.Instrum.Methods Phys.Res. B542, 87 (2023) H.N.Ratliff, N.A.McGirl, M.R.Beach, L.A.Castellanos, M.S.Clowdsley, L.H.Heilbronn, C.LaTessa, J.W.Norbury, A.Rusek, M.Sivertz, A.P.Srikrishna, H.-C.Wang, C.Zeitlin Double-differential primary target neutron yields from dual-thick-target proton and heavy ion accelerator experiments NUCLEAR REACTIONS 27Al, C, H(Si, X), (C, X)1NN, E=400 MeV/nucleon; measured reaction products, En, In; deduced yields, σ(θ, E). The NASA Space Radiation Laboratory.
doi: 10.1016/j.nimb.2023.06.001
2022BR05 Phys.Rev.Lett. 128, 212503 (2022) L.J.Broussard, J.L.Barrow, L.DeBeer-Schmitt, T.Dennis, M.R.Fitzsimmons, M.J.Frost, C.E.Gilbert, F.M.Gonzalez, L.Heilbronn, E.B.Iverson, A.Johnston, Y.Kamyshkov, M.Kline, P.Lewiz, C.Matteson, J.Ternullo, L.Varriano, S.Vavra Experimental Search for Neutron to Mirror Neutron Oscillations as an Explanation of the Neutron Lifetime Anomaly NUCLEAR REACTIONS B, C(n, X), E cold; measured reaction products, En, In. 1NN; deduced neutron transmission, neutron conversions, increase the apparent neutron lifetime. The Spallation Neutron Source, the National Institute of Standards and Technology Beam Lifetime experiment.
doi: 10.1103/PhysRevLett.128.212503
2022KO12 Phys. Rev. Res. 4, 021001 (2022) K.Kolos, V.Sobes, R.Vogt, C.E.Romano, M.S.Smith, L.A.Bernstein, D.A.Brown, M.T.Burkey, Y.Danon, M.A.Elsawi, B.L.Goldblum, L.H.Heilbronn, S.L.Hogle, J.Hutchinson, B.Loer, E.A.McCutchan, M.R.Mumpower, E.M.O'Brien, C.Percher, P.N.Peplowski, J.J.Ressler, N.Schunck, N.W.Thompson, A.S.Voyles, W.Wieselquist, M.Zerkle Current nuclear data needs for applications
doi: 10.1103/PhysRevResearch.4.021001
2022NE12 Phys.Rev. C 106, 044320 (2022) S.Neupane, J.Heideman, R.Grzywacz, M.Cooper, J.Hooker, K.L.Jones, T.T.King, N.Kitamura, M.Madurga, K.Siegl, C.R.Thornsberry, P.Wagenknecht, Z.Y.Xu, L.H.Heilbronn, M.M.Rajabali, A.Chester, A.Richard, Y.Alberty-Jones, J.Derkin, T.N.Massey, D.Soltesz, N.T.Brewer, B.C.Rasco, K.P.Rykaczewski, M.Wolinska-Cichocka, J.Clark, D.Santiago-Gonzalez, G.Savard Demonstration of the neutron tracking capability of NEXT array in time-of-flight measurements to improve energy resolution RADIOACTIVITY 17N, 104Nb(β-n); measured neutron time-of-flight (ToF), En, In. Data on the commissioning of the Neutron dEtector with Xn Tracking (NEXT) array consisting of 8x4 optically separated segments. Measurement of 17N decay at National Superconducting Cyclotron Laboratory (NSCL), 106Nb decay Argonne National Laboratory (ANL, CARIBU Facility). NUCLEAR REACTIONS 27Al(d, n), E=7.44 MeV; measured neutron time-of-flight (ToF), En, In. Data on the commissioning of the Neutron dEtector with Xn Tracking (NEXT) array consisting of 8x4 optically separated segments. Deuteron beam from Ohio University Edwards Accelerator Laboratory (EAL).
doi: 10.1103/PhysRevC.106.044320
2021BU04 Appl.Radiat.Isot. 172, 109676 (2021) N.Burahmah, J.R.Griswold, L.H.Heilbronn, S.Mirzadeh Transport model predictions of 225Ac production cross sections via energetic p, d and α irradiation of 232Th targets NUCLEAR REACTIONS 232Th(p, X)225Ac/227Ac/227Th/229Th/225Ra/223Ra/231Pa/230Pa, E<80 MeV; 232Th(d, 4n), (p, 4n), E<160 MeV; calculated σ using Monte Carlo transport codes (PHITS and MCNP6). Comparison with available data.
doi: 10.1016/j.apradiso.2021.109676
2019BR01 Appl.Radiat.Isot. 144, 54 (2019) K.Broderick, R.Lusk, J.Hinderer, J.Griswold, R.Boll, M.Garland, L.Heilbronn, S.Mirzadeh Reactor production of promethium-147 NUCLEAR REACTIONS 146Nd(n, γ), E thermal; measured reaction products, Eγ, Iγ; deduced production yields, σ, resonance integral. Comparison with available data. RADIOACTIVITY 147Nd(β-) [from 146Nd(n, γ), E thermal]; measured decay products, Eγ, Iγ; deduced T1/2.
doi: 10.1016/j.apradiso.2018.10.025
2019TS03 Nucl.Instrum.Methods Phys.Res. B449, 62 (2019) P.-E.Tsai, L.H.Heilbronn, B.-L.Lai, Y.Iwata, T.Murakami, R.-J.Sheu Thick target neutron yields from 100- and 230-MeV/nucleon helium ions bombarding water, PMMA, and iron NUCLEAR REACTIONS Fe, O(α, X)1NN, E=100, 230 MeV/nucleon; measured reaction products, En, In; deduced thick target neutron yields. Comparison with theoretical calculations.
doi: 10.1016/j.nimb.2019.04.030
2018GR09 Phys.Rev. C 98, 044607 (2018) J.R.Griswold, C.U.Jost, D.W.Stracener, S.H.Bruffey, D.Denton, M.Garland, L.Heilbronn, S.Mirzadeh Production of 229Th for medical applications: Excitation functions of low-energy protons on 232Th targets NUCLEAR REACTIONS 232Th(p, n), (p, 3n), (p, 4n), (p, 5n)228Pa/229Pa/230Pa/232Pa, E=13-39.9 MeV; measured reaction products, Eγ, Iγ, σ(E) by activation method, and effective σ(E) for 229Th production using natural Th targets at HRIBF-ORNL facility. 229Pa(α), (EC); measured T1/2, branching ratio for α and EC decay modes. Comparison with previous experimental values and theoretical predictions using PHITS and MCNP6 simulation codes.
doi: 10.1103/PhysRevC.98.044607
2018TS01 Nucl.Instrum.Methods Phys.Res. B416, 16 (2018) P.-E.Tsai, B.-L.Lai, L.H.Heilbronn, R.-J.Sheu Benchmark of neutron production cross sections with Monte Carlo codes NUCLEAR REACTIONS Li, C, 27Al, Cu, Pb(12C, X), (20Ne, X), (40Ar, X), (84Kr, X), (132Xe, X)1NN, E=135-600 MeV/nucleon; calculated σ(θ, E) using Monte Carlo simulation codes PHITS, FLUKA, and MCNP6. Comparison with experimental data.
doi: 10.1016/j.nimb.2017.11.029
2016GR18 Appl.Radiat.Isot. 118, 366 (2016) J.R.Griswold, D.G.Medvedev, J.W.Engle, R.Copping, J.M.Fitzsimmons, V.Radchenko, J.C.Cooley, M.E.Fassbender, D.L.Denton, K.E.Murphy, A.C.Owens, E.R.Birnbaum, K.D.John, F.M.Nortier, D.W.Stracener, L.H.Heilbronn, L.F.Mausner, S.Mirzadeh Large scale accelerator production of 225Ac: Effective cross sections for 78-192 MeV protons incident on 232Th targets NUCLEAR REACTIONS 232Th(p, X)225Ac/226Ac/227Ac/227Th/228Th/99Mo/140Ba/139Ce/141Ce/143Ce/144Ce, E=78-192 MeV; measured reaction products, Eγ, Iγ; deduced effective production σ, yields. Comparison with available data.
doi: 10.1016/j.apradiso.2016.09.026
2016PH02 Phys.Rep. 612, 1 (2016) D.G.Phillips II, W.M.Snow, K.Babu, S.Banerjee, D.V.Baxter, Z.Berezhiani, M.Bergevin, S.Bhattacharya, G.Brooijmans, L.Castellanos, M.-C.Chen, C.E.Coppola, R.Cowsik, J.A.Crabtree, P.Das, E.B.Dees, A.Dolgov, P.D.Ferguson, M.Frost, T.Gabriel, A.Gal, F.Gallmeier, K.Ganezer, E.Golubeva, G.Greene, B.Hartfiel, A.Hawari, L.Heilbronn, C.Johnson, Y.Kamyshkov, B.Kerbikov, M.Kitaguchi, B.Z.Kopeliovich, V.B.Kopeliovich, V.A.Kuzmin, C-Y.Liu, P.McGaughey, M.Mocko, R.Mohapatra, N.Mokhov, G.Muhrer, H.P.Mumm, L.Okun, R.W.Pattie, Jr., C.Quigg, E.Ramberg, A.Ray, A.Roy, A.Ruggles, U.Sarkar, A.Saunders, A.P.Serebrov, H.M.Shimizu, R.Shrock, A.K.Sikdar, S.Sjue, S.Striganov, L.W.Townsend, R.Tschirhart, A.Vainshtein, R.Van Kooten, Z.Wang, A.R.Young Neutron-antineutron oscillations: Theoretical status and experimental prospects COMPILATION A=1; compiled experimental and theoretical information.
doi: 10.1016/j.physrep.2015.11.001
2015TS03 Nucl.Technology 192, 222 (2015) Experiment Design of Secondary Neutron and Charged-Particle Measurement with Stopping Targets Bombarded by 100 and 230 MeV/amu 4He Ions NUCLEAR REACTIONS H, O, Fe(α, X), E=100, 230 MeV/nucleon; calculated influence of the target geometry on the σ(θ) of secondary particles. Transport model code PHITS (Particle and Heavy Ion Transport code System).
doi: 10.13182/NT14-130
2012NO04 Radiat.Meas. 47, 315 (2012) J.W.Norbury, J.Miller, A.M.Adamczyk, L.H.Heilbronn, L.W.Townsend, S.R.Blattnig, R.B.Norman, S.B.Guetersloh, C.J.Zeitlin Nuclear data for space radiation COMPILATION Z<100; compiled elemental and isotopic σ, σ(θ), σ(θ, E).
doi: 10.1016/j.radmeas.2012.03.004
2011HE14 Nucl.Sci.Eng. 169, 279 (2011) L.Heilbronn, C.J.Zeitlin, Y.Iwata, T.Murakami, T.Nakamura, S.Yonai, R.M.Ronningen, H.Iwase Neutron-Production Yields from 400 MeV/Nucleon Iron Stopping in Carbon, Aluminum, Copper, and Lead Targets NUCLEAR REACTIONS C, Al, Cu, Pb(56Fe, X), E=400 MeV/nucleon; measured reaction products, En, In; deduced thick target yields and ratios, σ(E, θ).
doi: 10.13182/NSE10-112
2011ZE01 Phys.Rev. C 83, 034909 (2011) C.Zeitlin, J.Miller, S.Guetersloh, L.Heilbronn, A.Fukumura, Y.Iwata, T.Murakami, S.Blattnig, R.Norman, S.Mashnik Fragmentation of 14N, 16O, 20Ne, and 24Mg nuclei at 290 to 1000 MeV/nucleon NUCLEAR REACTIONS H, C, Al, Cu, Sn, Pb(14N, X), (16O, X), (20Ne, X), (24Mg, X); E=290-1000 MeV/nucleon; measured particle spectra, cross sections, large and small acceptance angles. Comparison with NUCFRG2 and PHITS predictions.
doi: 10.1103/PhysRevC.83.034909
2008ZE02 Phys.Rev. C 77, 034605 (2008) C.Zeitlin, S.Guetersloh, L.Heilbronn, J.Miller, A.Fukumura, Y.Iwata, T.Murakami, L.Sihver, D.Mancusi Fragmentation cross sections of medium-energy 35Cl, 40Ar, and 48Ti beams on elemental targets NUCLEAR REACTIONS H, C, Al, Cu, Sn, Pb(35Cl, X), E=290, 400, 650 MeV/nucleon; H, C, Al, Cu, Sn, Pb(40Ar, X), E=650, 1000 MeV/nucleon; H, C, Al, Cu, Sn, Pb(48Ti, X), E=1000 MeV/nucleon; measured charge changing cross sections, fragment production cross sections.
doi: 10.1103/PhysRevC.77.034605
2007BL24 Nucl.Instrum.Methods Phys.Res. B 261, 974 (2007) D.L.Bleuel, M.A.Mcmahan, L.Ahle, B.R.Barquest, J.Cerny, L.H.Heilbronn, C.C.Jewett Characterization of a tunable quasi-monoenergetic neutron beam from deuteron breakup NUCLEAR REACTIONS Ti(d, np), Ta(d, np), E=20-29 MeV; measured products, Eπ, Iπ; deduced σ(θ, E). Data were imported from EXFOR entry C1595.
doi: 10.1016/j.nimb.2007.04.125
2007HE22 Nucl.Sci.Eng. 157, 142 (2007) L.Heilbronn, C.J.Zeitlin, Y.Iwata, T.Murakami, H.Iwase, T.Nakamura, T.Nunomiya, H.Sato, H.Yashima, R.M.Ronningen, K.Ieki Secondary Neutron-Production Cross Sections from Heavy-Ian Interactions Between 230 and 600 MeV/Nucleon NUCLEAR REACTIONS Al, Cu(α, nX), E=230 MeV/nucleon; C, Cu(N, nX), E=400 MeV/nucleon; C, Cu, Pb(Si, nX), E=600 MeV/nucleon; H, Li, C, Al(Fe, nX), E=500 MeV/nucleon; H, Li, C, Al, Cu, Pb(Kr, nX), E=400 MeV/nucleon; H, Li, C, Al, Cu, Pb(Xe, nX), E=400 MeV/nucleon; measured secondary neutron production cross sections and angular distributions.
doi: 10.13182/NSE07-A2719
2007LA29 Nucl.Phys. A791, 434 (2007) C.La Tessa, L.Sihver, C.Zeitlin, J.Miller, S.Guetersloh, L.Heilbronn, D.Mancusi, Y.Iwata, T.Murakami Test of weak and strong factorization in nucleus-nucleus collisions at several hundred MeV/nucleon NUCLEAR REACTIONS H, C, Al, Cu, Sn, Pb(40Ar, X), E=400 MeV/nucleon; C, Al, Cu, Sn, Pb(12C, X), (20Ne, X), (28Si, X), E=290, 400 MeV/nucleon; measured partial and total charge changing cross sections. Deduced factorization parameters.
doi: 10.1016/j.nuclphysa.2007.04.016
2007LA30 Nucl.Phys. A791, 451 (2007) C.La Tessa, L.Sihver, D.Mancusi, C.Zeitlin, J.Miller, S.Guetersloh, L.Heilbronn Weak and strong factorization properties in nucleus-nucleus collisions in the energy region 290-2100 MeV/nucleon
doi: 10.1016/j.nuclphysa.2007.04.025
2007MA01 Nucl.Instrum.Methods Phys.Res. B254, 30 (2007) D.Mancusi, L.Sihver, K.Gustafsson, C.La Tessa, S.B.Guetersloh, C.J.Zeitlin, J.Miller, L.H.Heilbronn, K.Niita, T.Sato, H.Nakashima, T.Murakami, Y.Iwata PHITS - benchmark of partial charge-changing cross sections for intermediate-mass systems NUCLEAR REACTIONS H, C, Al, Cu, Sn, Pb(40Ar, X), E=400 MeV/nucleon; calculated partial charge-changing σ.
doi: 10.1016/j.nimb.2006.10.070
2007ZE01 Nucl.Phys. A784, 341 (2007) C.Zeitlin, A.Fukumura, S.B.Guetersloh, L.H.Heilbronn, Y.Iwata, J.Miller, T.Murakami Fragmentation cross sections of 28Si at beam energies from 290 A to 1200 A Mev NUCLEAR REACTIONS H, C, Al, Cu, Sn, Pb(28Si, X), E=290-1200 MeV/nucleon; measured fragmentation σ. Comparison with model predictions.
doi: 10.1016/j.nuclphysa.2006.10.088
2007ZE02 Phys.Rev. C 76, 014911 (2007) C.Zeitlin, S.Guetersloh, L.Heilbronn, J.Miller, A.Fukumura, Y.Iwata, T.Murakami Fragmentation cross sections of 290 and 400 MeV/nucleon 12C beams on elemental targets NUCLEAR REACTIONS C, Al, Cu, Sn, Pb(12C, X), E=290, 400 MeV/nucleon; measured fragment production cross sections and angular distributions. Compared results to model calculations.
doi: 10.1103/PhysRevC.76.014911
2006HE07 Phys.Rev. C 73, 024603 (2006) L.Heilbronn, Y.Iwata, H.Iwase, T.Murakami, H.Sato, T.Nakamura, R.M.Ronningen, K.Ieki, I.Gudowska, N.Sobolevsky Secondary neutron-production cross sections from heavy-ion interactions in composite targets NUCLEAR REACTIONS O, Mg, Si, Ca, Fe(C, X), E=290 MeV/nucleon; O, Mg, Si, Ca, Fe(Ne, X), E=600 MeV/nucleon; measured neutron spectra, σ(E, θ). Comparison with model predictions.
doi: 10.1103/PhysRevC.73.024603
2006ZE03 Nucl.Instrum.Methods Phys.Res. B252, 308 (2006) C.Zeitlin, S.B.Guetersloh, L.H.Heilbronn, J.Miller Measurements of materials shielding properties with 1 GeV/nuc 56Fe NUCLEAR REACTIONS H, Be, C, Al, Cu, Sn, Pb(56Fe, X), E=1 GeV/nucleon; measured fragment spectra, charge distributions for elemental and composite targets; deduced target shielding properties.
doi: 10.1016/j.nimb.2006.08.011
2001IW05 Phys.Rev. C64, 054609 (2001) Y.Iwata, T.Murakami, H.Sato, H.Iwase, T.Nakamura, T.Kurosawa, L.Heilbronn, R.M.Ronningen, K.Ieki, Y.Tozawa, K.Niita Double-Differential Cross Sections for the Neutron Production from Heavy-Ion Reactions at Energies E/A = 290-600 MeV NUCLEAR REACTIONS C, Cu, Pb(C, nX), (Ne, nX), (Ar, nX), E=290-600 MeV/nucleon; measured neutron spectra, σ(En, θ), integrated σ; deduced equilibrium and pre-equilibrium components, related reaction mechanism features. Comparison with moving-source model predictions.
doi: 10.1103/PhysRevC.64.054609
2001ZE05 Phys.Rev. C64, 024902 (2001) C.Zeitlin, A.Fukumura, L.Heilbronn, Y.Iwata, J.Miller, T.Murakami Fragmentation Cross Sections of 600 MeV/Nucleon 20Ne on Elemental Targets NUCLEAR REACTIONS H, C, 27Al, Cu, Sn, Ta, Pb(20Ne, X), E=600 MeV/nucleon; charge-changing and fragment production σ, fragment charge distributions. Comparisons with model predictions.
doi: 10.1103/PhysRevC.64.024902
1999HE45 Nucl.Sci.Eng. 132, 1 (1999) L.Heilbronn, R.S.Cary, M.Cronqvist, F.Deak, K.Frankel, A.Galonsky, K.Holabird, A.Horvath, A.Kiss, J.Kruse, R.M.Ronningen, H.Schelin, Z.Seres, C.E.Stronach, J.Wang, P.Zecher, C.Zeitlin Neutron yields from 155 MeV/Nucleon Carbon and Helium Stopping in Aluminum NUCLEAR REACTIONS 27Al(α, X), (12C, X), E=155 MeV/nucleon; measured reaction products, En, In; deduced yields, number of neutrons per interaction.
doi: 10.13182/nse98-41
1999HT01 Phys.Rev. C59, 336 (1999) M.M.Htun, R.Madey, W.M.Zhang, M.Elaasar, D.Keane, B.D.Anderson, A.R.Baldwin, J.Jiang, A.Scott, Y.Shao, J.W.Watson, K.Frankel, L.Heilbronn, G.Krebs, M.A.McMahan, W.Rathbun, J.Schambach, G.D.Westfall, S.Yennello, C.Gale, J.Zhang Neutrons from Multiplicity-Selected La-La and Nb-Nb Collisions at 400A MeV and La-La Collisions at 250A MeV NUCLEAR REACTIONS La(La, nX), E=250, 400 MeV/nucleon; Nb(Nb, nX), E=250 MeV/nucleon; measured neutron emission σ(θ, φ) vs rapidity; deduced maximum azimuthal anisotropy ratio vs θ, neutron flow features. Comparison with BUU calculations.
doi: 10.1103/PhysRevC.59.336
1998HE33 Phys.Rev. C58, 3451 (1998) L.Heilbronn, R.Madey, M.Elaasar, M.Htun, K.Frankel, W.G.Gong, B.D.Anderson, A.R.Baldwin, J.Jiang, D.Keane, M.A.McMahan, W.H.Rathbun, A.Scott, Y.Shao, J.W.Watson, G.D.Westfall, S.Yennello, W.-M.Zhang Neutron Yields from 435 MeV/nucleon Nb Stopping in Nb and 272 MeV/nucleon Nb Stopping in Nb and Al NUCLEAR REACTIONS 93Nb(93Nb, nX), E=272, 435 MeV/nucleon; 27Al(93Nb, nX), E=272 MeV/nucleon; measured neutron stopping-target yields, multiplicity, σ(En, θ). Comparison to model calculations.
doi: 10.1103/PhysRevC.58.3451
1998WI09 Phys.Rev. C57, 1865 (1998) W.K.Wilson, S.Beedoe, R.Bossingham, M.Bougteb, J.Carroll, W.G.Gong, T.Hallman, L.Heilbronn, H.Z.Huang, G.Igo, P.Kirk, G.Krebs, A.Letessier-Selvon, L.Madansky, F.Manso, D.Magestro, H.S.Matis, J.Miller, C.Naudet, R.J.Porter, M.Prunet, G.Roche, L.S.Schroeder, P.Seidl, M.Toy, Z.F.Wang, R.C.Welsh, A.Yegneswaran, and the DLS Collaboration Inclusive Dielectron Cross Sections in p + p and p + d Interactions at Beam Energies from 1.04 to 4.88 GeV NUCLEAR REACTIONS 1,2H(p, e+e-), E=1.04-4.88 GeV; measured dielectron σ(E, θ); deduced integrated σ, reaction mechanism features.
doi: 10.1103/PhysRevC.57.1865
1997DE58 Acta Phys.Hung.N.S. 5, 13 (1997) F.Deak, A.Horvath, A.Kiss, Z.Seres, A.Galonsky, H.Hama, L.Heilbronn, D.W.Sackett, H.R.Schelin Production Rates of Excited Fragment Isotopes from the 36Ar + Ag Reaction at 35 MeV/nucleon NUCLEAR REACTIONS Ag(36Ar, X), E=35 MeV/nucleon; measured Z=3-5 excited fragments σ(θ) vs kinetic energy; deduced total production of neutron unbound states. Thermal model.
1997PO11 Phys.Rev.Lett. 79, 1229 (1997) R.J.Porter, S.Beedoe, R.Bossingham, M.Bougteb, W.B.Christie, J.Carroll, W.G.Gong, T.Hallman, L.Heilbronn, H.Z.Huang, G.Igo, P.Kirk, G.Krebs, A.Letessier-Selvon, L.Madansky, F.Manso, H.S.Matis, J.Miller, C.Naudet, M.Prunet, G.Roche, L.S.Schroeder, P.Seidl, Z.F.Wang, R.C.Welsh, W.K.Wilson, A.Yegneswaran, and the DLS Collaboration Dielectron Cross Section Measurements in Nucleus-Nucleus Reactions at 1.0A GeV NUCLEAR REACTIONS Ca(Ca, X), (α, X), (d, X), C(C, X), E=1 GeV/nucleon; measured dielectron production σ; deduced mass-independent scaling, dynamics related features.
doi: 10.1103/PhysRevLett.79.1229
1997ZE02 Phys.Rev. C56, 388 (1997) C.Zeitlin, L.Heilbronn, J.Miller, S.E.Rademacher, T.Borak, T.R.Carter, K.A.Frankel, W.Schimmerling, C.E.Stronach Heavy Fragment Production Cross Sections from 1.05 GeV/nucleon 56Fe in C, Al, Cu, Pb, and CH2 Targets NUCLEAR REACTIONS, ICPND H, C, 27Al, Cu, Pb(56Fe, X), E=1.05 GeV/nucleon; measured total σ vs charge exchange, fragment production σ; deduced enhanced even-Z production. Model comparisons.
doi: 10.1103/PhysRevC.56.388
1995DE24 Phys.Rev. C52, 219 (1995) F.Deak, A.Horvath, A.Kiss, Z.Seres, A.Galonsky, C.K.Gelbke, H.Hama, L.Heilbronn, D.Krofcheck, W.G.Lynch, D.W.Sackett, H.R.Schelin, M.B.Tsang, J.Kasagi, T.Murakami Internal Excitation of Intermediate Mass Fragments from Collisions of 36Ar + Ag Nuclei at 35 MeV/nucleon NUCLEAR REACTIONS Ag(36Ar, X), E=35 MeV/nucleon; measured intermediate mass fragments (Li-Mg) population ratios.
doi: 10.1103/PhysRevC.52.219
1995MA15 Nucl.Phys. A583, 617c (1995) H.S.Matis, S.Beedoe, M.Bougteb, J.Carroll, W.Christie, W.Gong, T.Hallman, L.Heilbronn, H.Huang, P.N.Kirk, G.Krebs, G.Igo, A.Letessier-Selvon, L.Madansky, F.Manso, J.Miller, C.Naudet, R.J.Porter, M.Prunet, G.Roche, L.S.Schroeder, P.Seidl, Z.F.Wang, R.Welsh, W.K.Wilson, A.Yegneswaran, and the DLS Collaboration Dilepton Production from p-p to Ca-Ca at the Bevalac NUCLEAR REACTIONS Ca(Ca, X), E=1.05 GeV/nucleon; 2,1H(p, X), E=1-4.9 GeV; measured dilepton production σ ratio, transverse momentum, rapidity, mass spectra; deduced pp-, nn-systems features.
doi: 10.1016/0375-9474(94)00735-6
1994HO02 Phys.Rev. C49, 1012 (1994) A.Horvath, F.Deak, A.Kiss, Z.Seres, A.Galonsky, C.K.Gelbke, H.Hama, L.Heilbronn, D.Krofcheck, W.G.Lynch, D.W.Sackett, H.R.Schelin, M.B.Tsang, J.Kasagi, T.Murakami Fragment Isotope Spectra from the 36Ar + Ag Reaction at 35 MeV/nucleon NUCLEAR REACTIONS Ag(36Ar, X), E=35 MeV/nucleon; measured inclusive fragment σ(E, θ); deduced total fragment production σ charge, mass dependence.
doi: 10.1103/PhysRevC.49.1012
1994HU03 Phys.Rev. C49, 314 (1994) H.Z.Huang, S.Beedoe, M.Bougteb, J.Cailiu, J.Carroll, T.Hallman, L.Heilbronn, G.Igo, P.Kirk, G.Krebs, A.Letessier-Selvon, B.Luttrell, F.Manso, L.Madansky, H.S.Matis, D.Miller, J.Miller, C.Naudet, R.J.Porter, G.Roche, L.S.Schroeder, P.A.Seidl, Z.F.Wang, R.Welsh, W.K.Wilson, A.Yegneswaran, and the DLS Collaboration Mass and Transverse Momentum Dependence of Dielectron Production in p + d and p + p Collisions at 4.9 GeV NUCLEAR REACTIONS 1,2H(p, X), E=4.9 GeV; measured dielectron σ, mass, transverse momentum dependence.
doi: 10.1103/PhysRevC.49.314
1993SC04 Nucl.Sci.Eng. 113, 184 (1993) H.R.Schelin, A.Galonsky, C.K.Gelbke, H.Hama, L.Heilbronn, D.Krofcheck, W.G.Lynch, D.Sackett, M.B.Tsang, X.Yang, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.Kasagi, T.Murakami Neutron Production in Heavy-Ion Reactions at 35 and 50 MeV/Nucleon NUCLEAR REACTIONS Ag(14N, xn), E=50 MeV/nucleon; measured neutron spectra. Moving source model analysis.
doi: 10.13182/NSE93-A24007
1993WI16 Phys.Lett. 316B, 245 (1993) W.K.Wilson, S.Beedoe, M.Bougteb, J.Cailiu, J.Carroll, W.G.Gong, T.Hallman, L.Heilbronn, H.Z.Huang, G.Igo, P.Kirk, G.Krebs, A.Letessier-Selvon, L.Madansky, F.Manso, H.S.Matis, D.Miller, J.Miller, C.Naudet, R.J.Porter, G.Roche, L.S.Schroeder, P.Seidl, M.Toy, Z.F.Wang, R.Welsh, A.Yegneswaran Relative Dielectron Yields in p + p and p + d Interactions from E(beam) = 1.0-4.9 GeV and the DLS Collaboration NUCLEAR REACTIONS 2,1H(p, X), E=1.03-4.9 GeV; measured relative dielectron yield, beam, invariant mass dependences; deduced dielectron production mechanism.
doi: 10.1016/0370-2693(93)90321-8
1992HU08 Phys.Lett. 297B, 233 (1992) H.Z.Huang, S.Beedoe, M.Bougteb, J.Cailiu, J.Carroll, T.Hallman, L.Heilbronn, G.Igo, P.Kirk, G.Krebs, A.Letessier-Selvon, B.Luttrell, F.Manso, L.Madansky, H.S.Matis, D.Miller, J.Miller, C.Naudet, R.J.Porter, G.Roche, L.S.Schroeder, P.A.Seidl, Z.F.Wang, R.Welsh, W.K.Wilson, A.Yegneswaran, and the DLS Collaboration Dielectron Yields in p + d and p + p Collisions at 4.9 GeV NUCLEAR REACTIONS 1,2H(d, X), E=4.9 GeV; measured dielectron yield; deduced dielectron origin features.
doi: 10.1016/0370-2693(92)91254-7
1991DE07 Phys.Rev. C43, 2432 (1991) F.Deak, A.Kiss, Z.Seres, A.Galonsky, L.Heilbronn Isotope Yield Ratios of Fragments from Heavy-Ion Reactions NUCLEAR REACTIONS, ICPND C, Ni, Ag, 165Ho(14N, X), E=35 MeV/nucleon; analyzed isotope yield ratios for X=Li, Be, B, C isotopes. Statistical multi-fragmentation model.
doi: 10.1103/PhysRevC.43.2432
1991HE07 Phys.Rev. C43, 2318 (1991) L.Heilbronn, A.Galonsky, C.K.Gelbke, W.G.Lynch, T.Murakami, D.Sackett, H.Schelin, M.B.Tsang, F.Deak, A.Kiss, Z.Seres, J.Kasagi, B.A.Remington Production of Neutron-Unbound States in Intermediate-Mass Fragments from 14N + Ag Reactions at E/A = 35 MeV NUCLEAR REACTIONS Ag(14N, nX), E=35 MeV/nucleon; measured γ(fragment)-coin, X=Li, Be, B, C isotopes; deduced source temperatures, amount of sequential feeding.
doi: 10.1103/PhysRevC.43.2318
1991SA10 Phys.Rev. C44, 384 (1991) D.Sackett, A.Galonsky, C.K.Gelbke, H.Hama, L.Heilbronn, D.Krofcheck, W.Lynch, H.R.Schelin, M.B.Tsang, X.Yang, F.Deak, A.Horvath, A.Kiss, Z.Seres, J.Kasagi, T.Murakami Neutron Inclusive Measurements of 36Ar + Ag Reactions at 35 MeV/Nucleon NUCLEAR REACTIONS Ag(36Ar, nX), E=35 MeV/nucleon; measured inclusive σ(θ, E); deduced neutron multiplicities, nuclear temperatures. Moving source fits.
doi: 10.1103/PhysRevC.44.384
1990DE25 Phys.Rev. C42, 1029 (1990) F.Deak, A.Kiss, Z.Seres, A.Galonsky, L.Heilbronn, H.R.Schelin Light Fragments from 14N + Ag Collisions at 35 MeV/Nucleon NUCLEAR REACTIONS Ag(14N, X), E=35 MeV/nucleon; measured σ(fragment θ, En, θn); deduced model parameters. Moving source model.
doi: 10.1103/PhysRevC.42.1029
1990WA17 Phys.Rev. C42, 2143 (1990) R.E.Warner, E.Cheung, C.F.Perdrisat, V.Punjabi, C.A.Davis, R.Helmer, A.Galonsky, L.Heilbronn, D.Krofcheck, S.E.Darden, J.J.Kolata, F.D.Becchetti, P.Schwandt Spectral Function of p-n Pairs in 6Li, from the 6Li(p, pα)pn Reaction at 200 MeV NUCLEAR REACTIONS 6Li(polarized p, pα), E=200 MeV; measured σ(θp, θα, Ep, Eα) vs (pn)-internal momentum. 6Li deduced dα-cluster probability.
doi: 10.1103/PhysRevC.42.2143
1989DE05 Phys.Rev. C39, 733 (1989) F.Deak, A.Kiss, Z.Seres, A.Galonsky, C.K.Gelbke, L.Heilbronn, W.Lynch, T.Murakami, H.Schelin, M.B.Tsang, B.A.Remington, J.Kasagi Dependence of 12B Excitation Energy on Its Kinetic Energy in the 14N + Ag Reaction at E/A = 35 MeV NUCLEAR REACTIONS Ag(14N, 12BX), E=490 MeV; measured σ(θ) vs ejectile energy, n(11B)-coin following ejectile breakup.
doi: 10.1103/PhysRevC.39.733
1989HE24 Phys.Rev. C40, 2576 (1989); Erratum Phys.Rev. C43, 2898 (1991) L.Heilbronn, A.Galonsky, X.Yang, F.Deak, A.Kiss, Z.Seres Determination of Energies and Widths of Neutron-Unbound States from Heavy-Ion Collisions NUCLEAR REACTIONS Ag(14N, 8Be), (14N, 9Li), E=35 MeV/nucleon; measured n(fragment)-coin, relative energy spectra following ejectile breakup. 9Li, 8Be level deduced E, Γ.
doi: 10.1103/PhysRevC.40.2576
1989KI13 Nucl.Phys. A499, 131 (1989) A.Kiss, F.Deak, Z.Seres, G.Caskey, A.Galonsky, B.Remington, L.Heilbronn Fragment Production in 14N + C, Ni, Ho Reactions at 35 MeV/Nucleon NUCLEAR REACTIONS C, Ni, 165Ho(14N, X), E=35 MeV/nucleon; measured σ(fragment θ, E) for X=Li, Be, B, C, N. Spectra decomposition into quasielastic, deep inelastic components.
doi: 10.1016/0375-9474(89)90274-1
1989SC08 Phys.Rev. C39, 1827 (1989) H.R.Schelin, A.Galonsky, C.K.Gelbke, L.Heilbronn, W.G.Lynch, T.Murakami, M.B.Tsang, X.Yang, G.Zhang, B.A.Remington, F.Deak, A.Kiss, Z.Seres, J.Kasagi Neutron Inclusive Measurements in 14N + Ag Reactions at 35 MeV/Nucleon NUCLEAR REACTIONS Ag(14N, nX), E=35 MeV/nucleon; measured σ(θn, En); deduced angle integrated σ.
doi: 10.1103/PhysRevC.39.1827
1989SE03 Nucl.Phys. A492, 315 (1989) Z.Seres, F.Deak, A.Kiss, G.Caskey, A.Galonsky, L.Heilbronn, B.Remington Analysis of Projectile Fragmentation in Intermediate-Energy Heavy-Ion Collisions NUCLEAR REACTIONS 165Ho(14N, X), E=35 MeV/nucleon; analyzed fragment momentum spectra for X=7,9,10Be, 10,11,12B, 11,12,13C; deduced model parameters.
doi: 10.1016/0375-9474(89)90089-4
1988BL09 Phys.Rev. C37, 2469 (1988) C.Bloch, W.Benenson, A.I.Galonsky, E.Kashy, J.Heltsley, L.Heilbronn, M.Lowe, R.J.Radtke, B.Remington, J.Kassagi, D.J.Morrissey Neutrons in Coincidence with Intermediate Mass Fragments at Large Angles from 14N + Ag Reactions at E/A = 20 and 35 MeV NUCLEAR REACTIONS Ag(14N, X), E=20, 35 MeV/nucleon; measured neutron spectra shapes, multiplicities σ(fragment θ, E) for X=6,7Li, 7,9Be, 10,11B; deduced model parameters. Moving source.
doi: 10.1103/PhysRevC.37.2469
1988CA06 Phys.Rev. C37, 969 (1988) G.Caskey, L.Heilbronn, B.Remington, A.Galonsky, F.Deak, A.Kiss, Z.Seres Fragment Spectra from Reactions Induced by 35 MeV/Nucleon 14N on 165Ho NUCLEAR REACTIONS 165Ho(14N, X), E=35 MeV/nucleon; measured σ(fragment θ, E) for X=7,9,10Be, 6,7,8,9Li, 11,12,13B, 10,11,12,13,14,15C. Coalescence model analyses.
doi: 10.1103/PhysRevC.37.969
1988KI06 Phys.Rev. C38, 170 (1988) A.Kiss, F.Deak, Z.Seres, G.Caskey, A.Galonsky, L.Heilbronn, B.Remington Target Mass Dependence of Neutron Emission in Collisions with 35 MeV/Nucleon 14N Ions NUCLEAR REACTIONS 165Ho, Ni, C(14N, nX), E=35 MeV/nucleon; measured (projectile-like fragment)n-coin, neutron spectra, multiplicities.
doi: 10.1103/PhysRevC.38.170
1988RE13 Phys.Rev. C38, 1746 (1988) B.A.Remington, M.Blann, A.Galonsky, L.Heilbronn, F.Deak, A.Kiss, Z.Seres Boltzmann Master Equation Analysis of Preequilibrium Neutron Emission from Heavy-Ion Collisions at 35 MeV/Nucleon NUCLEAR REACTIONS 165Ho(14N, xn), E=35 MeV/nucleon; analyzed data; deduced reaction mechanism. Boltzmann master equation model.
doi: 10.1103/PhysRevC.38.1746
1987BL13 Phys.Rev. C36, 203 (1987) C.Bloch, W.Benenson, A.I.Galonsky, E.Kashy, J.Heltsley, L.Heilbronn, M.Lowe, B.Remington, D.J.Morrissey, J.Kasagi Neutron Decay of Excited Nuclear States in Heavy Ion Collisions NUCLEAR REACTIONS Ag(14N, nX), E=35 MeV/nucleon; measured (fragment)n-coin, yields for X=7,8Li. 7,8Li levels deduced neutron decay characteristics, nuclear temperature.
doi: 10.1103/PhysRevC.36.203
1987GA17 Phys.Lett. 197B, 511 (1987) A.Galonsky, G.Caskey, L.Heilbronn, B.Remington, H.Schelin, F.Deak, A.Kiss, Z.Seres, J.Kasagi Temperatures Determined from Neutron Emission in Nucleus-Nucleus Collisions NUCLEAR REACTIONS 165Ho(14N, xn), E=35 MeV/nucleon; measured σ(θn, En); deduced temperatures.
doi: 10.1016/0370-2693(87)91045-8
1987KI05 Phys.Lett. 184B, 149 (1987) A.Kiss, F.Deak, Z.Seres, G.Caskey, A.Galonsky, L.Heilbronn, B.A.Remington, J.Kasagi Excitation of Discrete Particle-Unbound States in Heavy-Ion Collisions NUCLEAR REACTIONS 165Ho(14N, nX), E=490 MeV; measured (fragment)n-coin, (fragment)neutron relative velocity spectra for X=7Li, 10Be, 11B, 12C. 8Li, 11Be, 12B, 13C level deduced Γ. ΔE-E telescopes, liquid scintillators.
doi: 10.1016/0370-2693(87)90559-4
1986RE13 Phys.Rev. C34, 1685 (1986) B.A.Remington, G.Caskey, A.Galonsky, C.K.Gelbke, L.Heilbronn, J.Heltsley, M.B.Tsang, F.Deak, A.Kiss, Z.Seres, J.Kasagi, J.J.Kolata Neutron-Fragment Coincidence Measurements in 14N + Ho and 14N + Ni Reactions at 35 MeV/Nucleon NUCLEAR REACTIONS Ni, 165Ho(14N, nX), E=35 MeV/nucleon; measured inclusive neutron, fragment spectra, σ(θn, En, fragment θ). Liquid scintillator, ΔE-E identification.
doi: 10.1103/PhysRevC.34.1685
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