NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = D.Trautmann Found 88 matches. 2017SI04 Phys.Rev. C 95, 012501 (2017) Reexamination of proton rms radii from low-q power expansions NUCLEAR STRUCTURE 1H; analyzed proton rms radii determined in electron scattering, and from Lamb shift measurements in muonic hydrogen; discussed and resolved discrepancy in the two types of measurements related to problems with expansions of the proton form factors in terms of q2n.
doi: 10.1103/PhysRevC.95.012501
2014SI02 Phys.Rev. C 89, 012201 (2014) Proton root-mean-square radii and electron scattering NUCLEAR REACTIONS 1H(e, e), E not given; analyzed parameterization of the nucleon form factors fitted to e-p scattering data with corresponding densities to have a physical behavior at large radii; deduced proton root-mean-square radius.
doi: 10.1103/PhysRevC.89.012201
2009WE02 Phys.Rev. C 80, 024602 (2009) F.Weissbach, K.Hencken, D.Kiselev, D.Trautmann Improved radiative corrections to (e, e'p) experiments: Explicit treatment of kinematical corrections in multiphoton bremsstrahlung
doi: 10.1103/PhysRevC.80.024602
2009WE06 Phys.Rev. C 80, 064605 (2009) F.Weissbach, K.Hencken, D.Trautmann, I.Sick Improved radiative corrections and proton charge form factor from the Rosenbluth separation technique
doi: 10.1103/PhysRevC.80.064605
2008FI03 Nucl.Instrum.Methods Phys.Res. B266, 2255 (2008) I.Fijal-Kirejczyk, M.Jaskola, A.Korman, D.Banas, J.Braziewicz, J.Choinski, U.Majewska, M.Pajek, W.Kretchmer, G.Lapicki, T.Mukoyama, D.Trautmann L-subshell ionization of heavy elements by S ions with energy of 0.4-3.8 MeV/amu ATOMIC PHYSICS 197Au, 209Bi(32S, X), E=12.8-41.6, 65-120 MeV; measured E(L X-ray), I(L X-ray), production σ. Comparison with semiclassical and coupled-subshell models.
doi: 10.1016/j.nimb.2008.03.047
2007AS06 Eur.Phys.J. A 33, 11 (2007) Focusing of high-energy particles in the electrostatic field of a homogeneously charged sphere and the effective momentum approximation
doi: 10.1140/epja/i2007-10432-4
2006DR02 Eur.Phys.J. C 45, 783 (2006) U.Dreyer, T.Baier, K.Hencken, D.Trautmann Lepton-pair production from deep inelastic scattering peripheral relativistic heavy ion collisions NUCLEAR REACTIONS Pb(p, X), (Pb, X), E=high; calculated lepton pair production σ(x) in peripheral collisions.
doi: 10.1140/epjc/s2005-02452-1
2006HE04 Phys.Rev.Lett. 96, 012303 (2006) K.Hencken, G.Baur, D.Trautmann Transverse Momentum Distribution of Vector Mesons Produced in Ultraperipheral Relativistic Heavy Ion Collisions NUCLEAR REACTIONS Pb(Pb, X), 197Au(197Au, X), E=high; calculated vector mesons transverse momentum distributions for ultraperipheral collisions.
doi: 10.1103/PhysRevLett.96.012303
2006WE08 Eur.Phys.J. A 30, 477 (2006) F.Weissbach, K.Hencken, D.Rohe, I.Sick, D.Trautmann Improved radiative corrections for (e, e'p) experiments: Beyond the peaking approximation and implications of the soft-photon approximation NUCLEAR REACTIONS H(e, e'p), E=high; calculated bremsstrahlung spectra, angular distributions. Soft-photon approximation, peaking approximation.
doi: 10.1140/epja/i2005-10319-4
2005AS07 Eur.Phys.J. A 26, 167 (2005) A.Aste, C.von Arx, D.Trautmann Coulomb distortion of relativistic electrons in the nuclear electrostatic field NUCLEAR REACTIONS 40Ca, 208Pb(e, e'X), E ≈ 100-500 MeV; calculated electron wave functions, Coulomb distortion effects. Effective momentum approximation.
doi: 10.1140/epja/i2005-10169-0
2004AS05 Eur.Phys.J. A 21, 161 (2004) A.Aste, K.Hencken, D.Trautmann Coulomb corrections for coherent electroproduction of vector mesons: Eikonal approximation NUCLEAR REACTIONS 16O, 208Pb(e, X), E not given; calculated Coulomb corrections to vector meson production σ.
doi: 10.1140/epja/i2003-10182-3
2004AS10 Nucl.Phys. A743, 259 (2004) A.Aste, K.Hencken, J.Jourdan, I.Sick, D.Trautmann Coulomb corrections for quasielastic (e, e') scattering: eikonal approximation NUCLEAR REACTIONS 208Pb(e, e'), E=310-645 MeV; calculated quasielastic scattering σ(E, θ), Coulomb distortion effects. Eikonal approximation.
doi: 10.1016/j.nuclphysa.2004.08.001
2004HE03 Nucl.Phys. A733, 200 (2004) K.Hencken, G.Baur, D.Trautmann A cluster version of the GGT sum rule NUCLEAR STRUCTURE 4,6,8He, 16,17,18,19,20,21,22O; analyzed photoabsorption σ. Cluster sum rule.
doi: 10.1016/j.nuclphysa.2004.01.001
2004HE13 Phys.Rev. C 69, 054902 (2004) K.Hencken, G.Baur, D.Trautmann Production of QED pairs at small impact parameter in relativistic heavy ion collisions NUCLEAR REACTIONS 197Au(197Au, X), Pb(Pb, X), E=high; calculated electron-positron pair production σ, energy and transverse momentum distributions.
doi: 10.1103/PhysRevC.69.054902
2003BB06 Nucl.Phys. A729, 787 (2003) G.Baur, K.Hencken, A.Aste, D.Trautmann, S.R.Klein Multi-photon exchange processes in ultraperipheral relativistic heavy-ion collisions
doi: 10.1016/j.nuclphysa.2003.09.006
2003BB08 Prog.Part.Nucl.Phys. 51, 487 (2003) G.Baur, K.Hencken, D.Trautmann Electromagnetic Dissociation as a Tool for Nuclear Structure and Astrophysics
doi: 10.1016/S0146-6410(03)00097-8
2002AS03 Eur.Phys.J. C 23, 545 (2002) A.Aste, G.Baur, K.Hencken, D.Trautmann, G.Scharf Electron-Positron Pair Production in the External Electromagnetic Field of Colliding Relativistic Heavy Ions
doi: 10.1007/s100520200891
2002BA47 Phys.Rep. 364, 359 (2002) G.Baur, K.Hencken, D.Trautmann, S.Sadovsky, Y.Kharlov Coherent γγ and γA Interactions in Very Peripheral Collisions at Relativistic Ion Colliders
doi: 10.1016/S0370-1573(01)00101-6
2002BA60 Phys.Rev. C65, 064602 (2002) P.Banerjee, G.Baur, K.Hencken, R.Shyam, D.Trautmann Postacceleration Effects in the Coulomb Dissociation of Neutron Halo Nuclei NUCLEAR REACTIONS Pb(11Be, n10Be), (19C, n18C), E=5-72 MeV/nucleon; calculated σ(E, θ), fragment relative energy distributions; deduced postacceleration effects.
doi: 10.1103/PhysRevC.65.064602
2001BA54 Prog.Part.Nucl.Phys. 46, 99 (2001) G.Baur, K.Hencken, D.Trautmann, S.Typel, H.H.Wolter Electromagnetic Dissociation as a Tool for Nuclear Structure and Astrophysics
doi: 10.1016/S0146-6410(01)00113-2
2000HE01 Phys.Rev. C61, 027901 (2000) K.Hencken, D.Trautmann, G.Baur Production of Low Mass Electron Pairs Due to the Photon-Photon Mechanism in Central Collisions NUCLEAR REACTIONS 197Au(S, X), (Pb, X), (197Au, X), E=high; calculated electron-positron pair yields from electromagnetic mechanism.
doi: 10.1103/PhysRevC.61.027901
1999BA53 Prog.Part.Nucl.Phys. 42, 357 (1999) G.Baur, K.Hencken, D.Trautmann Photon-Photon and Photon-Hadron Interactions at Relativistic Heavy Ion Colliders
doi: 10.1016/S0146-6410(99)00089-7
1999HE02 Phys.Rev. C59, 841 (1999) K.Hencken, D.Trautmann, G.Baur Calculation of Higher-Order Effects in Electron-Positron Pair Production in Relativistic Heavy Ion Collisions NUCLEAR REACTIONS Pb(Pb, X), 197Au(197Au, X), E=high; calculated single, multiple pair-production σ; deduced impact parameter dependence.
doi: 10.1103/PhysRevC.59.841
1999HE24 Phys.Rev. C60, 034901 (1999) K.Hencken, D.Trautmann, G.Baur Bremsstrahlung from Electrons and Positrons in Peripheral Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS 197Au(197Au, X), E=high; calculated electron-positron pair production associated bremsstrahlung σ(E, θ).
doi: 10.1103/PhysRevC.60.034901
1998BA75 J.Phys.(London) G24, 1657 (1998) G.Baur, K.Hencken, D.Trautmann Photon-Photon Physics in Very Peripheral Collisions of Relativistic Heavy Ions NUCLEAR REACTIONS 1H(p, X), Ca(Ca, X), 197Au(197Au, X), Pb(Pb, X), E=high; calculated electromagnetic processes in peripheral collisions, meson production σ, pair production σ, related features.
doi: 10.1088/0954-3899/24/9/003
1998ME15 Eur.Phys.J. C 2, 741 (1998) H.Meier, K.Hencken, D.Trautmann, G.Baur Bremsstrahlung Pair Production in Relativistic Heavy Ion Collision NUCLEAR REACTIONS 1H(p, X), Ca(Ca, X), 197Au(197Au, X), Pb(Pb, X), E=high; calculated electron, muon bremsstrahlung pair production σ.
doi: 10.1007/s100520050178
1998SI21 Nucl.Phys. A637, 559 (1998) On the rms Radius of the Deuteron NUCLEAR REACTIONS 2H(e, e), E not given; analyzed data. 2H deduced rms radius. Comparison with NN-scattering, isotope shifts results.
doi: 10.1016/S0375-9474(98)00334-0
1996DH02 Nucl.Instrum.Methods Phys.Res. B117, 218 (1996) B.B.Dhal, H.C.Padhi, D.Trautmann A Strange Projectile Dependence of L2-Subshell Ionization Cross Section of Au for 28Si and 32S Ion Bombardment NUCLEAR REACTIONS 197Au(28Si, X), (32S, X), E=10-15 MeV; measured L X-ray spectra; deduced ionization σ. ATOMIC PHYSICS 197Au(28Si, X), (32S, X), E=10-15 MeV; measured L X-ray spectra; deduced ionization σ.
doi: 10.1016/0168-583X(96)00278-9
1996HE09 Phys.Rev. C53, 2532 (1996) K.Hencken, D.Trautmann, G.Baur Equivalent Photon Approach to Simultaneous Excitation in Heavy Ion Collision NUCLEAR REACTIONS 197Au, C(C, X), 197Au(197Au, X), E not given; calculated simultaneous excitation σ. Equivalent photon approach.
doi: 10.1103/PhysRevC.53.2532
1996PA45 Phys.Rev. A54, 3014 (1996) H.C.Padhi, B.B.Dhal, V.Nanal, K.G.Prasad, P.N.Tandon, D.Trautmann L-Subshell Ionization Studies in Au and Bi for 19F and 28Si Large-Ion Bombardment NUCLEAR REACTIONS 197Au, 209Bi(19F, X), E=30-57 MeV; 197Au, 209Bi(28Si, X), E=36-84 MeV; measured L-subshell X-ray production, subshell ionization σ. ATOMIC PHYSICS 197Au, 209Bi(19F, X), E=30-57 MeV; 197Au, 209Bi(28Si, X), E=36-84 MeV; measured L-subshell X-ray production, subshell ionization σ.
doi: 10.1103/PhysRevA.54.3014
1996SI05 Phys.Lett. 375B, 16 (1996) On the rms-Radius of the Deuteron NUCLEAR REACTIONS 2H(e, e), E not given; analyzed global data. 2H deduced rms charge radius.
doi: 10.1016/0370-2693(96)00214-6
1995HE24 Nucl.Phys. A591, 548 (1995) K.Hencken, H.Muhry, I.Sick, D.Trautmann, G.Baur Colour Van der Waals Effects in Pb-Pb Scattering ( Question ) NUCLEAR REACTIONS 208Pb(208Pb, 208Pb), E=1130 MeV; calculated σ(θ); deduced relativistic effects, vacuum polarization, polarizability, quasimolecules formation, colour Van der Waals contribution roles.
doi: 10.1016/0375-9474(95)00212-J
1995SE17 Phys.Rev. A52, 1125 (1995) J.Semaniak, J.Braziewicz, M.Pajek, T.Czyzewski, L.Glowacka, M.Jaskola, M.Haller, R.Karschnick, W.Kretschmer, Z.Halabuka, D.Trautmann L-Subshell Ionization of Heavy Elements by Carbon and Nitrogen Ions of Energy 0.4-1.8 MeV/amu NUCLEAR REACTIONS Hf, Ta, W, Os, Ir, Pt, 209Bi, Th, 197Au(14N, X), E=0.4-1.8 MeV/nucleon; measured L X-ray spectra; deduced X-ray production, subshell ionization σ. ATOMIC PHYSICS Hf, Ta, W, Os, Ir, Pt, 209Bi, Th, 197Au(14N, X), E=0.4-1.8 MeV/nucleon; measured L X-ray spectra; deduced X-ray production, subshell ionization σ.
doi: 10.1103/PhysRevA.52.1125
1994BB14 Z.Phys. A347, 255 (1994) Applicability of First and Second Order WKB Approximation to Elastic Scattering of Two Particles Interacting by Long-Range Forces
doi: 10.1007/BF01289792
1994BR38 J.Phys.(London) B27, 1535 (1994) J.Braziewicz, J.Semaniak, T.Czyzewski, L.Glowacka, M.Jaskola, M.Haller, R.Karschnick, W.Kretschmer, D.Trautmann L-Subshell Ionization of Rare Earth Elements by Carbon Ion Bombardment NUCLEAR REACTIONS La, Ce, Pr, Nd, Sm, Eu, Dy, Er(12C, X), (13C, X), E=0.4-2.8 MeV/nucleon; measured L shell X-ray production σ. ATOMIC PHYSICS La, Ce, Pr, Nd, Sm, Eu, Dy, Er(12C, X), (13C, X), E=0.4-2.8 MeV/nucleon; measured L shell X-ray production σ.
doi: 10.1088/0953-4075/27/8/014
1994SE16 Nucl.Instrum.Methods Phys.Res. B86, 185 (1994) J.Semaniak, J.Braziewicz, T.Czyzewski, L.Glowacka, M.Haller, M.Jaskola, R.Karschnick, A.P.Kobzev, M.Pajek, W.Kretschmer, D.Trautmann L-Subshell Ionization by 14N Ions NUCLEAR REACTIONS La, 197Au(14N, X), E=1.75-22.4 MeV; measured L X-ray yields, subshell ionization σ. ATOMIC PHYSICS La, 197Au(14N, X), E=1.75-22.4 MeV; measured L X-ray yields, subshell ionization σ.
doi: 10.1016/0168-583X(94)96173-5
1991BR30 Phys.Rev. A44, 2868 (1991) H.Brauning, K.Ullmann, V.Dangendorf, H.Schmidt-Bocking, D.Trautmann, Th.Kauer Influence of Recoil Effect in Ti K-Shell Ionization Probabilities NUCLEAR REACTIONS Ti(p, X), (d, X), (α, X), E=0.5 MeV/nucleon; measured K-shell ionization probabilities. Semi-classical approximation calculations. ATOMIC PHYSICS Ti(p, X), (d, X), (α, X), E=0.5 MeV/nucleon; measured K-shell ionization probabilities. Semi-classical approximation calculations.
doi: 10.1103/PhysRevA.44.2868
1991BR31 J.Phys.(London) B24, 1669 (1991) E.Braziewicz, J.Braziewicz, T.Czyzewski, L.Glowacka, M.Jaskola, T.Kauer, A.P.Kobzev, M.Pajek, D.Trautmann L-Subshell Ionization of Rare Earth Elements by Light Ion Bombardment NUCLEAR REACTIONS 139La, Pr, Nd, Eu, Tb, 165Ho, Er(p, X), E=0.1-0.9 MeV; 139La, Pr, Nd, Eu, Tb, 165Ho, Er(d, X), E=0.2-2.1 MeV; 139La, Pr, Nd, Eu, Tb, 165Ho, Er(3He, X), E=0.3-0.9 MeV; 139La, Pr, Nd, Eu, Tb, 165Ho, Er(α, X), E=0.4-0.9 MeV; measured L-subshell ionization σ(E). Model comparison. ATOMIC PHYSICS 139La, Pr, Nd, Eu, Tb, 165Ho, Er(p, X), E=0.1-0.9 MeV; 139La, Pr, Nd, Eu, Tb, 165Ho, Er(d, X), E=0.2-2.1 MeV; 139La, Pr, Nd, Eu, Tb, 165Ho, Er(3He, X), E=0.3-0.9 MeV; 139La, Pr, Nd, Eu, Tb, 165Ho, Er(α, X), E=0.4-0.9 MeV; measured L-subshell ionization σ(E). Model comparison.
doi: 10.1088/0953-4075/24/7/020
1991TR03 Nucl.Phys. A533, 528 (1991) D.Trautmann, G.Baur, D.Vetterli, P.Egelhof, R.Henneck, M.Jaskola, H.Muhry, I.Sick Vacuum Polarization in Sub-Coulomb 12C-12C Scattering (II) NUCLEAR REACTIONS 12C(12C, 12C), E=4 MeV; calculated relative σ(θ); deduced vacuum polarization effects. High precision.
doi: 10.1016/0375-9474(91)90531-A
1991VE02 Nucl.Phys. A533, 505 (1991) D.Vetterli, W.Boeglin, P.Egelhof, R.Henneck, M.Jaskola, A.Klein, H.Muhry, I.Sick, D.Trautmann, G.Baur Effects of Vacuum Polarization on Sub-Coulomb 12C-12C Scattering (I) NUCLEAR REACTIONS 12C(12C, 12C), E=4 MeV; measured relative σ(θ); deduced vacuum polarization. High precision.
doi: 10.1016/0375-9474(91)90530-J
1990CA38 Europhys.Lett. 13, 231 (1990) M.Carlen, J.-Cl.Dousse, M.Gasser, J.Kern, Ch.Rheme, P.Rymuza, Z.Sujkowski, D.Trautmann X-Ray Kβ Satellites Induced in Molybdenum by 4He Ions NUCLEAR REACTIONS Mo(α, X), E=28 MeV; measured K X-ray spectra; deduced M-shell ionization probability. ATOMIC PHYSICS Mo(α, X), E=28 MeV; measured K X-ray spectra; deduced M-shell ionization probability.
doi: 10.1209/0295-5075/13/3/007
1990PA28 Nucl.Instrum.Methods Phys.Res. B52, 109 (1990) M.Pajek, A.P.Kobzev, D.Trautmann, Th.Kauer Systematic Measurements of K-Shell Ionization by 3He Ions of Energy 0.6-3.6 MeV NUCLEAR REACTIONS 27Al, 31P, Ar, Cr, Ti, Fe, Ni, Ge, Se, 93Nb, Pd(3He, X), E=0.6-3.6 MeV; measured X-ray spectra; deduced K-shell ionization σ. ATOMIC PHYSICS 27Al, 31P, Ar, Cr, Ti, Fe, Ni, Ge, Se, 93Nb, Pd(3He, X), E=0.6-3.6 MeV; measured X-ray spectra; deduced K-shell ionization σ.
doi: 10.1016/0168-583X(90)90577-H
1989KA44 J.Phys.Soc.Jpn. 58, 3929 (1989) T.Kambara, T.Mizogawa, Y.Awaya, Y.Kanai, R.Schuch, K.Shima, D.Trautmann Impact Parameter Dependent Probability of Au L3-Shell Ionization by 40.7 MeV Ar Ions NUCLEAR REACTIONS 197Au(40Ar, X), E=40.7 MeV; measured (X-ray)(40Ar)-coin; deduced L-shell ionization probability.
doi: 10.1143/JPSJ.58.3929
1989SO07 Nucl.Instrum.Methods Phys.Res. B42, 456 (1989) R.S.Sokhi, D.Crumpton, D.Trautmann Ionisation of L Subshells of Heavy Atoms by Deuteron Collision ATOMIC PHYSICS W, Au, Pb, Bi(d, X), E=1-3 MeV; measured L-subshell ionization σ. Model comparisons.
doi: 10.1016/0168-583X(89)90100-6
1989TR13 Nucl.Instrum.Methods Phys.Res. B42, 449 (1989) On the SCA-Description of the Energy- and Impact Parameter Dependence of K-Shell Ionization Cross Sections ATOMIC PHYSICS Ta, Ho, Tb, Sm, Nd(p, X), E ≈ 1-7 MeV; calculated K-shell ionization σ relative to experiment. P(3He, X), E ≈ 0.5-2.5 MeV; Nd(p, X), E ≈ 1-6 MeV; Ti(C, X), E ≈ 1-4.25 MeV; calculated K-shell ionization σ(E).
doi: 10.1016/0168-583X(89)90099-2
1989VE03 Phys.Rev.Lett. 62, 1453 (1989) D.Vetterli, W.Boeglin, P.Egelhof, R.Henneck, M.Jaskola, A.Klein, H.Muhry, G.R.Plattner, I.Sick, D.Trautmann, G.Baur, A.Weller Effects of Vacuum Polarization in Hadron-Hadron Scattering NUCLEAR REACTIONS 12C(12C, 12C), E=4 MeV; measured σ(θ), Mott scattering; deduced Coulomb interaction related vaccum polarization.
doi: 10.1103/PhysRevLett.62.1453
1988BA07 Helv.Phys.Acta 61, 219 (1988) G.Baur, W.Boeglin, P.Egelhof, R.Henneck, M.Jaskola, A.Klein, H.Muhry, G.R.Plattner, I.Sick, D.Trautmann, D.Vetterli Effects of the Vacuum Polarization on Coulomb 12C - 12C-Scattering NUCLEAR REACTIONS 12C(12C, 12C), E=4 MeV; measured σ(θ); deduced Coulomb scattering vacuum polarization role.
1987PF04 J.Phys.(London) B20, 3453 (1987) M.Pfuetzner, J.Szerypo, Z.Zelazny, F.M.El-Ashry, M.Goclowski, L.Glowacka, D.Trautmann, M.Jaskola The K-Shell Ionisation of 73Ta Induced by Low-Energy Protons and Deuterons NUCLEAR REACTIONS Ta(p, X), E=1.1-3.8 MeV; Ta(d, X), E=1.2-3.2 MeV; measured K shell ionization σ.
doi: 10.1088/0022-3700/20/14/017
1987SZ04 J.Phys.(London) B20, 5475 (1987) J.Szerypo, M.Pfuetzner, W.Kretschmer, R.Schmitt, W.Schuster, A.Bienkowski, L.Glowacka, D.Trautmann, M.Jaskola The K-Shell Ionisation of Atoms with Z ≥ 60 by Protons ATOMIC PHYSICS Nd, Sm, Tb, Ho, Ta(p, X), E=2.7-10 MeV; measured K-shell ionisation σ.
doi: 10.1088/0022-3700/20/20/024
1986SI12 Phys.Lett. 176B, 260 (1986) R.Singer, D.Trautmann, P.Hanggi, G.Baur Alpha Particle Tunnelling in the Field of a Magnetic Monopole RADIOACTIVITY 147Sm(α); calculated T1/2 variation due to tunnelling in magnetic monopole field.
doi: 10.1016/0370-2693(86)90160-7
1985AA01 Nucl.Phys. A439, 45 (1985) E.H.L.Aarts, R.A.R.L.Malfliet, R.J.De Meijer, S.Y.Van Der Werf, G.Baur, R.Shyam, F.Rosel, D.Trautmann Comparison between a Distorted-Wave Breakup Model Description and a Quasi-Free Breakup Model Description of 3He Projectile Breakup Data at 52 MeV NUCLEAR REACTIONS 28Si, 58Ni(3He, dX), (3He, dp), E=52 MeV; calculated inclusive σ(θd, Ed), σ(θp, θd, Ed). Quasifree breakup, DWBA.
doi: 10.1016/0375-9474(85)90208-8
1984SH12 Phys.Rev. C30, 1109 (1984); Erratum Phys.Rev. C31, 287 (1985) R.Shyam, G.Baur, F.Rosel, D.Trautmann Test of the Theory of Inelastic Break-Up for the (3He, d) Break-Up Reaction NUCLEAR REACTIONS 165Ho, 166,167Er(3He, d), E=100 MeV; calculated elastic, inelastic breakup σ(Ed, θd). Post form DWBA theory.
doi: 10.1103/PhysRevC.30.1109
1983BA37 Phys.Rev. C28, 946 (1983) G.Baur, R.Shyam, F.Rosel, D.Trautmann Calculation of Proton-Neutron Coincidence Cross Sections in 56 MeV Deuteron-Induced Breakup Reactions by Post Form Distorted-Wave Born Approximation NUCLEAR REACTIONS 12C, 51V, 118Sn(d, np), E=56 MeV; analyzed σ(θp, θn), σ(θp, θn, Ep); deduced spectator breakup mechanism. DWBA analysis.
doi: 10.1103/PhysRevC.28.946
1983SH09 Phys.Rev. C27, 2393 (1983) R.Shyam, G.Baur, A.Budzanowski, J.Bojowald, H.Dabrowski, C.Mayer-Boricke, W.Oelert, G.Riepe, M.Rogge, P.Turek, F.Rosel, D.Trautmann Explanation of 3He and Triton Rates in the Alpha Breakup Inclusive Cross Sections NUCLEAR REACTIONS 58Ni, 90Zr, 120Sn, 209Bi(α, t), (α, 3He), E=172.5 MeV; measured σ(θ, Et), σ(θ, E(3He)); deduced α-breakup mechanism. Inclusive breakup, post form DWBA.
doi: 10.1103/PhysRevC.27.2393
1983TR13 Nucl.Instrum.Methods 214, 21 (1983) Accurate Calculation of Inner-Shell Ionization ATOMIC PHYSICS Ni(p, X), E=0.6 MeV; Sn(Cl, X), E=44 MeV; calculated inner shell ionization probability. Relativistic Hartree-Fock-Slater wave functions, screened Coulomb potential.
doi: 10.1016/0167-5087(83)90535-5
1982CU02 Lett.Nuovo Cim. 34, 229 (1982) A.Cunsolo, A.Foti, G.Imme, G.Pappalardo, G.Raciti, F.Rizzo, N.Saunier, G.Baur, R.Shyam, F.Rosel, D.Trautmann Inclusive Deuteron Spectra from the 6Li + 12C Collision at 34 MeV NUCLEAR REACTIONS 12C(6Li, dX), E=34 MeV; measured σ(θ, Ed) inclusive; deduced optical model parameters. Zero-range DWBA, breakup, deuteron spectator model.
doi: 10.1007/BF02817116
1981BA48 Helv.Phys.Acta 53, 506 (1981) G.Baur, R.Shyam, F.Rosel, D.Trautmann Projectile Fragmentation and Stripping to Unbound States: An important reaction mechanism for peripheral nucleus-nucleus collisions NUCLEAR REACTIONS 181Ta, 119Sn, 93Nb, 62Ni, 27Al(d, p), E=25.5 MeV; 62Ni(3He, d), (3He, p), E=24.3 MeV; 58Ni(α, 3He), E=100 MeV; 62Ni(α, 3He), E=172.5 MeV; 58Ni, 90Zr(α, 3He), E=140 MeV; calculated projectile breakup probability vs (L). Elastic, inelastic fragmentation.
1981KL06 Nucl.Phys. A370, 205 (1981) J.Kleinfeller, J.Bisplinghoff, J.Ernst, T.Mayer-Kuckuk, G.Baur, B.Hoffmann, R.Shyam, F.Rosel, D.Trautmann Study of Inclusive Proton Spectra from Low Energy Deuteron Reactions in Terms of Spectator Break-Up and Coulomb Dissociation of the Projectile NUCLEAR REACTIONS 27Al, 62Ni, 93Nb, 119Sn, 181Ta, 232Th(d, pX), E=15 MeV; measured σ(Ep), σ(θ). Solid-state counter telescopes.
doi: 10.1016/0375-9474(81)90073-7
1980BA14 Phys.Rev. C21, 2668 (1980) G.Baur, R.Shyam, F.Rosel, D.Trautmann Importance of the Breakup Mechanism for Composite Particle Scattering NUCLEAR REACTIONS 27Al, 62Ni, 93Nb, 181Ta, 197Au(d, p), E=25.5, 80 MeV; 58,62Ni, 90Zr(α, 3He), E=100, 140, 172.5 MeV; calculated breakup, reaction σ, total σ. Optical model.
doi: 10.1103/PhysRevC.21.2668
1980SH17 Phys.Rev. C22, 1401 (1980) R.Shyam, G.Baur, F.Rosel, D.Trautmann Elastic and Inelastic Breakup of the 3He Particle NUCLEAR REACTIONS 51V, 90Zr(3He, d), E=90MeV; calculated σ(θd, Ed), elastic, inclusive breakup; 51V, 90Zr(3He, dp), E=90 MeV; calculated σ(θd, θp, Ed); deduced reaction mechanism. DWBA breakup theory.
doi: 10.1103/PhysRevC.22.1401
1980TR01 Nucl.Instrum.Methods 169, 259 (1980) On the Semiclassical Description of Coulomb Ionization of Inner Shells NUCLEAR REACTIONS Au(p, p), E=1 MeV; Ag(p, p), E=2 MeV; calculated sub-shell ionization probability. Semiclassical approximation.
doi: 10.1016/0029-554X(80)90086-5
1979BA10 Nucl.Phys. A315, 241 (1979) G.Baur, M.Pauli, F.Rosel, D.Trautmann The Break-up Mechanism for Heavy Ion Reactions in the Case of (9Be, 8Be) NUCLEAR REACTIONS 197Au(9Be, 8Be), E=18-26 MeV; calculated inclusive spectra including elastic, inelastic breakup with, without recoil correction.
doi: 10.1016/0375-9474(79)90646-8
1979BU15 Z.Phys. A293, 293 (1979) A.Budzanowski, G.Baur, R.Shyam, J.Bojowald, W.Oelert, G.Riepe, M.Rogge, P.Turek, F.Rosel, D.Trautmann Experimental and Theoretical Study of the Elastic Break-up of the Alpha Particle on 58Ni Nuclei at E = 172.5 MeV NUCLEAR REACTIONS 58Ni(α, tp), E=172.5 MeV; measured tp(θ), σ(Et, θp, θt); deduced reaction mechanism. α-breakup, DWBA theory.
doi: 10.1007/BF01435271
1979SH02 Phys.Rev. C19, 1246 (1979) R.Shyam, G.Baur, F.Rosel, D.Trautmann (α, 3He) Breakup Reaction on Nuclei and the Neutron Momentum Distribution in the α Particle NUCLEAR REACTIONS 62Ni(α, n3He), E=172.5 MeV; 209Bi(α, n3He), E=140 MeV; calculated σ(E(3He), En, θ). Plane-wave spectator model, comparison with DWBA.
doi: 10.1103/PhysRevC.19.1246
1978BA21 J.Phys.(London) G4, 275 (1978) Charged-Particle Transfer Reactions into the Continuum: The Line-Shape of (d, n) and (3He, d) Spectra NUCLEAR REACTIONS 12C(d, n), E=6.3 MeV; 12C(3He, d); calculated σ.
doi: 10.1088/0305-4616/4/2/017
1978BU20 Phys.Rev.Lett. 41, 635 (1978) A.Budzanowski, G.Baur, C.Alderliesten, J.Bojowald, C.Mayer-Boricke, W.Oelert, P.Turek, F.Rosel, D.Trautmann Observation of the α-Particle Breakup Process at Eα(lab) = 172.5 MeV NUCLEAR REACTIONS 58,60,62,64Ni(α, 3He), E=172.5 MeV; measured σ(θ).
doi: 10.1103/PhysRevLett.41.635
1978PA17 Nucl.Phys. A311, 141 (1978) J.Pampus, J.Bisplinghoff, J.Ernst, T.Mayer-Kuckuk, J.Rama Rao, G.Baur, F.Rosel, D.Trautmann Inclusive Proton Spectra from Deuteron Break-up: Theory and Experiment NUCLEAR REACTIONS 27Al, 62Ni, 93Nb, 119Sn, 181Ta(d, pX), E=25.5 MeV; measured continuous spectra of protons, angle-integrated cross sections dσ/dϵ, angular distributions. Solid-state counter telescopes.
doi: 10.1016/0375-9474(78)90506-7
1977BA53 Nucl.Phys. A288, 113 (1977) Effects of the Polarizability in Elastic Scattering below the Coulomb Barrier NUCLEAR REACTIONS 208Pb(d, d), E=5.5-7.5 MeV; calculated polarization effects on σ.
doi: 10.1016/0375-9474(77)90083-5
1977BI09 Helv.Phys.Acta 50, 509 (1977) J.Birchall, E.Baumgartner, H.M.Friess, H.Muhry, F.Rosel, D.Trautmann Scattering of Protons from Argon and Hydrogen at 1 MeV NUCLEAR REACTIONS 40Ar(p, p), E=1.093 MeV; measured σ as function of pressure, beam current. 40Ar(p, p), E=0.992 MeV; reanalyzed σ.
1977SC05 Helv.Phys.Acta 50, 29 (1977) H.Schar, D.Trautmann, E.Baumgartner Bestimmung spektroskopischer Faktoren fur Energieniveaux der Isotope 41,43,45,49Ca mit (d, p)-Reaktionen bei 2.5 MeV Deuteronenenergie NUCLEAR REACTIONS 40,42,44,48Ca(d, p), E=2.5 MeV; measured σ(Ep, θ). 41,43,45,49Ca levels deduced S.
1977ST07 Helv.Phys.Acta 50, 9 (1977) P.Staub, E.Baumgartner, J.X.Saladin, H.Schar, D.Trautmann Bestimmung der spektroskopischen Faktoren mehrerer Energieniveaux der Isotope Ni59, 61, 63, 65 mit (d, p) - Reaktionen bei 2.8 MeV Deuteronenenergie NUCLEAR REACTIONS 58,60,62,64Ni(d, p), E=2.8 MeV; measured σ(Ep, θ). 59,61,63,65Ni levels deduced S.
1977TR08 Nucl.Phys. A291, 221 (1977) A.Traber, D.Trautmann, F.Rosel Estimation of Nuclear Effects in Heavy-Ion Elastic Scattering NUCLEAR REACTIONS 208Pb(16O, 16O); calculated σ(θ), nuclear effects.
doi: 10.1016/0375-9474(77)90207-X
1977TR09 Nukleonika 22, 485 (1977) On the Theory of Direct Reactions with Many Particle Final States NUCLEAR REACTIONS 197Au(d, pn), E=10.5, 12 MeV; 208Pb(d, pn), E=12 MeV; 12C(d, n), E=6.3 MeV; calculated σ(θ).
1976BA25 J.Phys.(London) G2, 171 (1976) Semiclassical Treatment of Sub-Coulomb Transfer Reactions to Resonant States NUCLEAR REACTIONS 208Pb(d, p), E=10 MeV; 208Pb(n, n), (d, np), (9Be, n8Be), 208Pb(17O, n16O), (13C, n12C), E ≈ 55, 70 MeV; calculated σ.
doi: 10.1088/0305-4616/2/3/009
1976GO20 Z.Phys. A278, 139 (1976) U.Gotz, F.Rosel, D.Trautmann, H.Jochim Influence of the Mott-Schwinger Interaction on the Elastic Scattering of Protons NUCLEAR REACTIONS 12C, 208Pb(p, p); calculated Mott-Schwinger interaction, polarizations.
1975BA61 Nucl.Phys. A252, 77 (1975) Resonance Line Shapes in Stripping Reactions into the Continuum NUCLEAR REACTIONS 15N(d, p), E=3.1-3.3 MeV; 208Pb(d, p), E=12 MeV; calculated σ(Ep, θ). 16N, 209Pb calculated resonances.
doi: 10.1016/0375-9474(75)90602-8
1974BA19 Z.Phys. 267, 103 (1974) On the Theory of Stripping Reactions into the Continuum NUCLEAR REACTIONS 14N, 16O, 24Mg(d, p); calculated σ(θ).
doi: 10.1007/BF01668636
1974BA36 Nucl.Phys. A224, 477 (1974) Semiclassical Treatment of Break-up Reactions NUCLEAR REACTIONS 197Au(d, pn), E=12, 10.5 MeV; 208Pb(d, pn), E=9.5 MeV; 208Pb(9Be, n8Be), E=35 MeV; calculated σ(Ed, Ep), σ(En), σ(En, θ(p)), σ(θ(n)).
doi: 10.1016/0375-9474(74)90550-8
1973BA08 Nucl.Phys. A199, 218 (1973) Sub-Coulomb (d, p) Stripping Theory into the Continuum
doi: 10.1016/0375-9474(73)90344-8
1973BA43 Nucl.Phys. A208, 261 (1973) Sub-Coulomb Deuteron Break-up and the Neutron-Nucleus Interaction NUCLEAR REACTIONS 197Au(d, np), E=2-12 MeV; calculated σ(Ed). 208Pb(d, np), E=12 MeV; calculated σ(Ep, θ). Analysis of deuteron breakup on heavy nuclei.
doi: 10.1016/0375-9474(73)90374-6
1973BA51 Nucl.Phys. A211, 333 (1973) Neutron Transfer to Unbound States in Heavy-Ion Reactions NUCLEAR REACTIONS 16O(9Be, 8Be), 208Pb(d, p); calculated σ(θ).
doi: 10.1016/0375-9474(73)90724-0
1973PL02 Nucl.Phys. A206, 513 (1973) G.R.Plattner, R.D.Viollier, D.Trautmann, K.Alder Dispersion Relations and Low-Energy Elastic Scattering of Charged Particles from Nuclei (II). Application to N-4He Scattering NUCLEAR REACTIONS 4He(p, p), (n, n); analyzed forward scattering, Coulomb modified dispersion relation. 4He deduced coupling constants.
doi: 10.1016/0375-9474(73)90082-1
1972AL24 Nucl.Phys. A191, 399 (1972) K.Alder, R.Morf, M.Pauli, D.Trautmann Numerical Investigations within the Semiclassical Transfer Theory
doi: 10.1016/0375-9474(72)90524-6
1972BA70 Nucl.Phys. A191, 321 (1972) The Coulomb Break-up of the Deuteron NUCLEAR REACTIONS 208Pb(d, pn), E=5, 8, 9, 10 MeV; calculated σ(Ep, θ(p), θ(n)). DWBA, Hulthen deuteron wave function.
doi: 10.1016/0375-9474(72)90518-0
1972BB12 Phys.Lett. 42B, 31 (1972) The Deuteron Break-up on Heavy Nuclei Around the Coulomb Barrier NUCLEAR REACTIONS 197Au(d, np), E=12 MeV; calculated σ(Ep, θ(p)).
doi: 10.1016/0370-2693(72)90707-1
1972VI05 Phys.Lett. 40B, 625 (1972) R.D.Viollier, G.R.Plattner, D.Trautmann, K.Alder Forward Dispersion Relations and Low-Energy Elastic Scattering of Charged Particles from Nuclei NUCLEAR REACTIONS 4He(α, α), E < 50 MeV; analyzed forward dispersion relation; deduced charge density distribution.
doi: 10.1016/0370-2693(72)90612-0
1971AL08 Nucl.Phys. A164, 433 (1971) The Mott-Schwinger Polarization in (d, p) Reactions NUCLEAR REACTIONS 208Pb, 209Bi, 238U(d, p), E=8, 10 MeV calculated P(p)(θ). Mott-schwinger potential.
doi: 10.1016/0375-9474(71)90771-8
1971AL20 Ann.Phys.(N.Y.) 66, 884 (1971) On the Diffraction Model of Transfer Reactions NUCLEAR REACTIONS 44Ca(t, p), E=12 MeV; 9Be(17O, 16O), E=11 MeV; calculated σ(θ). Diffraction model.
doi: 10.1016/0003-4916(71)90088-1
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