NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = L.H.Heilbronn Found 14 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
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
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
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
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
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
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
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
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