NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = G.Baur Found 109 matches. Showing 1 to 100. [Next]2008BA11 J.Phys.(London) G35, 014028 (2008) Coulomb dissociation, a tool for nuclear astrophysics
doi: 10.1088/0954-3899/35/1/014028
2008TY03 Eur.Phys.J. A 38, 355 (2008) Scaling laws and higher-order effects in Coulomb excitation of neutron halo nuclei
doi: 10.1140/epja/i2008-10864-4
2007BA39 Prog.Part.Nucl.Phys. 59, 122 (2007) Direct reactions with exotic nuclei, nuclear structure and astrophysics
doi: 10.1016/j.ppnp.2006.12.002
2007BA41 Phys.Rev. C 75, 058801 (2007) E0 emission in α + 12C fusion at astrophysical energies NUCLEAR REACTIONS 12C(α, γ), E(cm)< 1.5 MeV; calculated the contribution of E0 emission compared to E1 and E2 emissions.
doi: 10.1103/PhysRevC.75.058801
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
2005TY02 Nucl.Phys. A759, 247 (2005) Electromagnetic strength of neutron and proton single-particle halo nuclei NUCLEAR STRUCTURE 11Be, 15C, 17,23O; calculated neutron separation energies, radius and Woods-Saxon potential depth; analyzed partial and total reduced transition B(E1) probabilities. 8Be, 9C, 12N; calculated proton separation energies, radius and Woods-Saxon potential depth; analyzed partial and total reduced transition B(E1) probabilities. NUCLEAR REACTIONS 7Be, 8B, 11C(p, γ), E=low; calculated zero energy astrophysical S-factors using asymptotic normalisation coefficients. Compared Woods-Saxon and square-well potential models.
doi: 10.1016/j.nuclphysa.2005.05.145
2004BA74 Prog.Theor.Phys.(Kyoto), Suppl. 154, 333 (2004) Theory of the Trojan-Horse Method
doi: 10.1143/PTPS.154.333
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
2004TY01 Phys.Rev.Lett. 93, 142502 (2004) Effective-Range Approach and Scaling Laws for Electromagnetic Strength in Neutron-Halo Nuclei NUCLEAR STRUCTURE 11Be; analyzed B(E1); deduced asymptotic normalization coefficient, spectroscopic factors. Effective-Range approach.
doi: 10.1103/PhysRevLett.93.142502
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
2001TY01 Phys.Rev. C64, 024601 (2001) Higher Order Effects in Electromagnetic Dissociation of Neutron Halo Nuclei NUCLEAR REACTIONS 208Pb(19C, n18C), E=67 MeV/nucleon; 208Pb(11Be, n10Be), E=72 MeV/nucleon; calculated Coulomb dissociation σ(E, θ); deduced role of higher-order effects. Zero-range model for neutron-core interaction, comparisons with data.
doi: 10.1103/PhysRevC.64.024601
2000BA20 Eur.Phys.J. A 7, 55 (2000) G.Baur, C.A.Bertulani, D.Dolci Influence of Damping on the Excitation of the Double Giant Resonance NUCLEAR REACTIONS 208Pb(208Pb, 208Pb'), E=640 MeV/nucleon; calculated GDR, double GDR occupation probabilities, excitation σ following Coulomb excitation; deduced dependence on resonance width, dynamical effects. Coupled channels calculations.
doi: 10.1007/s100500050011
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
1999UT03 Nucl.Phys. (Supplement) A654, 928c (1999) H.Utsunomiya, Y.Tokimoto, T.Yamagata, M.Ohta, Y.Aoki, K.Hirota, K.Ieki, Y.Iwata, K.Katori, S.Hamada, Y.-W.Lui, R.P.Schmitt, S.Typel, G.Baur Excitation of Continuum States in 7Li and Their Decay by Quantum Tunneling NUCLEAR REACTIONS 27Al, 58Ni, 64Zn, 90Zr, 120Sn, 144Sm, 197Au(7Li, tα), E=42 MeV; measured particle spectra, forward-backward asymmetry; deduced E1, E2, higher-order effects in Coulomb breakup.
doi: 10.1016/S0375-9474(00)88575-9
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
1997BA40 Phys.Rev. C56, 581 (1997) Comment on ' Quantum-Mechanical Equivalent-Photon Spectrum for Heavy Ion Physics "
doi: 10.1103/PhysRevC.56.581
1997CA36 Nucl.Phys. A621, 139c (1997) G.Calvi, S.Cherubini, M.Lattuada, S.Romano, C.Spitaleri, M.Aliotta, G.Rizzari, M.Sciuto, R.A.Zappala, V.N.Kondratyev, D.Miljanic, M.Zadro, G.Baur, O.Yu.Goryunov, A.A.Shvedov Indirect Measurement of Nuclear Reaction Cross Sections at Astrophysical Energies NUCLEAR REACTIONS, ICPND 2H(7Li, 2α), E=19, 20 MeV; measured αα-coin; deduced 7Li(p, 2α) reaction σ, astrophysical S-factors vs E. 'Trojan horse' method.
doi: 10.1016/S0375-9474(97)00226-1
1997TY01 Nucl.Phys. A613, 147 (1997) Higher-Order Effects in the Coulomb Dissociation of 8B into 7Be + p NUCLEAR REACTIONS, ICPND 7Be(p, γ), E ≤ 2 MeV; calculated E2, M1 contribution to astrophysical S-factor. 208Pb(8B, p7Be), E=46.5 MeV/nucleon; calculated σ(θ, E(relative)), Coulomb dissociation. Diffraction effects, Glauber theory based simple approximation.
doi: 10.1016/S0375-9474(96)00415-0
1996BA75 Yad.Fiz. 59, No 9, 1568 (1996); Phys.Atomic Nuclei 59, 1509 (1996) G.Baur, R.Broders, M.Dahmen, D.Grzonka, K.Kilian, W.Oelert, K.Rohrich, M.Rook, K.Sachs, T.Sefzick, O.Steinkamp, M.Wolke, M.Chanel, C.Lacroix, P.Lefevre, D.Mohl, G.Molinari Search for Antihydrogen at LEAR
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
1996KA06 J.Phys.(London) G22, 115 (1996) Analytical Cross Sections for the Photodissociation of Loosely Bound Nuclei NUCLEAR STRUCTURE 11Be; calculated dipole strength distribution. Analytic approach. NUCLEAR REACTIONS 9Be(γ, X), E not given; calculated photodissociation σ. Analytic approach.
doi: 10.1088/0954-3899/22/1/010
1996MU11 Nucl.Phys. A609, 254 (1996) Effects of Strong Interaction on the Electromagnetic Dissociation NUCLEAR REACTIONS 208Pb(8B, X), E=51.9 MeV/nucleon; calculated dissociation, E2 σ(θ); deduced strong interaction related features. Eikonal approach.
doi: 10.1016/S0375-9474(96)00294-1
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
1995TY01 Phys.Lett. 356B, 186 (1995) Multiple Electromagnetic Excitation in Fast Peripheral Heavy Ions Collisions NUCLEAR STRUCTURE 11Be; calculated first excited state population σ ratio vs projectile velocity. Multiple electromagnetic excitation, fast peripheral heavy ion collisions.
doi: 10.1016/0370-2693(95)00845-C
1994BA04 Phys.Rev. C49, 1127 (1994) γγ Physics at Relativistic Heavy-Ion Colliders
doi: 10.1103/PhysRevC.49.1127
1994BB15 J.Phys.(London) G20, 1 (1994) Coulomb Dissociation Studies as a Tool of Nuclear Astrophysics
doi: 10.1088/0954-3899/20/1/005
1994KA25 J.Phys.(London) G20, 1023 (1994) Coulomb Dissociation of 9Be: Investigation of higher-order effects NUCLEAR REACTIONS 9Be(γ, n), E=low; calculated photodissociation σ(E(rel)). 8Be(n, n), E=low; calculated σ(E(rel)). 208Pb(9Be, nX), E=30 MeV/nucleon; calculated transition amplitude square vs E(rel); deduced higher-order effects role. Saddle point method.
doi: 10.1088/0954-3899/20/7/003
1994PO02 Phys.Rev.Lett. 72, 1168 (1994) V.Yu.Ponomarev, E.Vigezzi, P.F.Bortignon, R.A.Broglia, G.Colo, G.Lazzari, V.V.Voronov, G.Baur Multiple Excitation of Giant Dipole Resonances in Relativistic Heavy Ion Collisions NUCLEAR REACTIONS 208Pb(136Xe, 136Xe'), E=681 MeV/nucleon; calculated projectile giant resonances associated B(λ) following Coulomb excitation, σ(E). Mean field harmonic vibration, doorway states coupled damping.
doi: 10.1103/PhysRevLett.72.1168
1994PO04 Nucl.Phys. A569, 333c (1994) V.Yu.Ponomarev, E.Vigezzi, P.F.Bortignon, R.A.Broglia, G.Colo, G.Lazzari, V.V.Voronov, G.Baur Microscopic Origin of the Giant Resonance Structure NUCLEAR STRUCTURE 136Xe; calculated B(λ), GDR strength distribution. Microscopic approach. NUCLEAR REACTIONS 208Pb(γ, n), E ≤ 22 MeV; calculated σ(E). 208Pb(136Xe, 136Xe'), E=690 MeV/nucleon; analyzed σ data; deduced model radius parameter. Microscopic approach.
doi: 10.1016/0375-9474(94)90124-4
1994TY01 Phys.Rev. C49, 379 (1994) Higher Order Effects in Electromagnetic Excitation with Fast Projectiles NUCLEAR REACTIONS 208Pb(14O, 14O'), E=70, 87.5 MeV/nucleon; 208Pb(32Cl, 32Cl'), E=70 MeV/nucleon; calculated projectile electromagnetic excitation. 208Pb(136Xe, 136Xe'), E=0.7 GeV/nucleon; calculated σ(θ, E); deduced electromagnetic excitation mechanism influence on one-, two-phonon GDR line shape.
doi: 10.1103/PhysRevC.49.379
1994TY02 Nucl.Phys. A573, 486 (1994) Higher Order Effects in Electromagnetic Dissociation of Fast Particles, a Soluble Model and Application to 11Li NUCLEAR STRUCTURE 11Li; calculated σ(θ(9Li)) following 11Li fragmentation at 28, 800 MeV/nucleon incident energy. Soluble model.
doi: 10.1016/0375-9474(94)90354-9
1994TY03 Phys.Rev. C50, 2104 (1994) Coulomb Dissociation of 8B into 7Be + p: Effects of multiphoton exchange NUCLEAR REACTIONS, ICPND 7Be(p, γ), E ≤ 0.5 keV; calculated astrophysical S-factor; 7Be(p, γ), E ≤ 2 MeV; calculated capture σ(E). 208Pb(8B, p7Be), E=46.5 MeV/nucleon; calculated breakup σ(θ) vs E(relative). Coulomb dissociation of 8B, first-, second-order perturbation, sudden approximation.
doi: 10.1103/PhysRevC.50.2104
1993BA40 Nucl.Phys. A561, 628 (1993) Coherent Photon-Photon Processes in Disruptive and Non-Disruptive Relativistic Heavy-Ion Collisions NUCLEAR REACTIONS 208Pb(208Pb, X), E=relativistic; calculated coherent μ+μ--, e+e--differential production probabilities. Impact parameter formulation, disruptive, nondisruptive relativistic collisions.
doi: 10.1016/0375-9474(93)90069-A
1993NO06 Phys.Rev. C48, 1915 (1993) Explanation of Recent Observations of Very Large Electromagnetic Dissociation Cross Sections. II. Higher Order Corrections NUCLEAR REACTIONS 197Au(12C, X), (20Ne, X), (40Ar, X), (56Fe, X), (139La, X), (197Au, X), (238U, X), (16O, X), (32S, X), E ≥ 0.15 GeV/nucleon; calculated electromagnetic dissociation σ; deduced higher order corrections role. Weizsacker-Williams theory.
doi: 10.1103/PhysRevC.48.1915
1992BA63 Nucl.Phys. A550, 527 (1992) G.Baur, C.A.Bertulani, D.M.Kalassa Higher-Order Electromagnetic Interaction in the Dissociation of Fast Particles NUCLEAR REACTIONS 11Li(γ, X), E ≤ 5 MeV; calculated photo-dissociation σ(E). Pb(11Li, 9Li), E=30 MeV/nucleon; calculated projectile breakup σ(E); deduced higher order electromagnetic interactions role. Classical approach, breakup radius concept.
doi: 10.1016/0375-9474(92)90022-C
1992SH09 Nucl.Phys. A540, 341 (1992) Coulomb Dissociation of 11Li and 11Be in a Direct Fragmentation Model NUCLEAR STRUCTURE A ≈ 25-120; calculated Coulomb part of (11Li, 9Li), (11Be, 10Be) reaction induced fragmentation σ. Post form DWBA. NUCLEAR REACTIONS 197Au(11Li, 9Li), E=29-100 MeV/nucleon; calculated σ(θ), σ(θ(9Li), E(9Li)); deduced 2n-removal mechanism. Post form DWBA.
doi: 10.1016/0375-9474(92)90208-2
1991BA36 Nucl.Phys. A530, 267 (1991) Nuclear Photon Scattering Below and Above the Giant Resonances NUCLEAR REACTIONS 208Pb(γ, γ), E ≤ 50 MeV; calculated σ(θ) vs E, Compton scattering. 208Pb(γ, X), E=20-140 MeV; calculated photoabsorption σ(E). Microscopic operator based matrix elements.
doi: 10.1016/0375-9474(91)90803-E
1991BE09 Nucl.Phys. A526, 751 (1991) C.A.Bertulani, G.Baur, M.S.Hussein Two-Neutron Removal Cross Sections of 11Li Projectiles NUCLEAR REACTIONS 12C, 63Cu, 208Pb, 27Al, 9Be(9Li, X), E=0.8 GeV/nucleon; calculated elastic, inelastic, 2-nucleon removal σ; deduced nuclear, Coulomb interaction interplay. Cluster model, modified RPA calculation comparisons.
doi: 10.1016/0375-9474(91)90442-9
1991KI05 Z.Phys. A339, 489 (1991) J.Kiener, G.Gsottschneider, H.J.Gils, H.Rebel, V.Corcalciuc, S.K.Basu, G.Baur, J.Raynal Investigation of Sequential Break-Up Mode 6Li → 6Li(*) (3+1) → α + d of 156 MeV 6Li Projectiles on 208Pb in the Very Forward Angular Hemisphere NUCLEAR REACTIONS 208Pb(6Li, 6Li), (6Li, 6Li'), E=156 MeV; measured σ(θ), dα-coin following projectile breakup; deduced breakup mechanism.
doi: 10.1007/BF01288432
1991KI07 Phys.Rev. C44, 2195 (1991) J.Kiener, H.J.Gils, H.Rebel, S.Zagromski, G.Gsottschneider, N.Heide, H.Jelitto, J.Wentz, G.Baur Measurements of the Coulomb Dissociation Cross Section of 156 MeV 6Li Projectiles at Extremely Low Relative Fragment Energies of Astrophysical Interest NUCLEAR REACTIONS 208Pb(6Li, dα), E=156 MeV; measured σ(θα, θd, E(dα)); deduced radiative capture σ, astrophysical S-factor. Coincidence measurements with magnetic spectrometer.
doi: 10.1103/PhysRevC.44.2195
1991SH11 Phys.Rev. C44, 915 (1991) Projectile Breakup by Nuclear and Coulomb Fields and Application to Astrophysically Relevant Radiative-Capture Processes NUCLEAR REACTIONS 208Pb(7Li, tα), E=63 MeV; 208Pb(6Li, dα), E=156 MeV; calculated σ(θ); deduced favorable regime for radiative capture astrophysical S-factor extractions. Breakup processes, nuclear, Coulomb contributions interplay.
doi: 10.1103/PhysRevC.44.915
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
1989BA16 J.Phys.(London) G15, 661 (1989) Studies on Multiple Electromagnetic Excitation with Fast Heavy Ions: Scaling properties for the excitation of rotational-vibrational states NUCLEAR REACTIONS 238U(16O, 16O'), (238U, 238U'), E < 100 MeV/nucleon; calculated GDR excitation σ(E). Sudden approximation, collective state coupling.
doi: 10.1088/0954-3899/15/5/018
1989BA64 Nucl.Phys. A504, 352 (1989) The Angular Correlation in the Coulomb Dissociation Method for Radiative Capture Processes of Astrophysical Interest NUCLEAR REACTIONS 208Pb(7Li, tα), E=63 MeV; 208Pb(6Li, dα), E=156 MeV; 208Pb(16O, α12C), E=100 MeV/nucleon; calculated σ(θ, θ(αt), E(αt)), σ(θ, θ(αd), E(αd)), σ(θ, θ(α12C), E(α12C)) following Coulomb excitation into continuum; deduced astrophysical S-factor associated with 6Li breakup.
doi: 10.1016/0375-9474(89)90347-3
1989KI07 Z.Phys. A332, 359 (1989) J.Kiener, H.J.Gils, H.Rebel, G.Baur Observation of Nonresonant Coulomb Break-Up of 156 MeV 6Li Projectiles NUCLEAR REACTIONS 208Pb(6Li, dα), E=156 MeV; measured σ(θ(6Li), θ(αd), E(αd)); deduced projectile breakup mechanism.
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.
1988BE09 Nucl.Phys. A480, 615 (1988) Coincidence Cross Sections for the Dissociation of Light Ions in High-Energy Collisions NUCLEAR REACTIONS 208Pb(d, np), E=200 MeV; calculated dissociation σ(θ); deduced nuclear electromagnetic field roles.
doi: 10.1016/0375-9474(88)90467-8
1986BA50 Nucl.Phys. A458, 188 (1986) G.Baur, C.A.Bertulani, H.Rebel Coulomb Dissociation as a Source of Information on Radiative Capture Processes of Astrophysical Interest NUCLEAR REACTIONS 208Pb(7Be, 3Heα), E=30 MeV/nucleon; 208Pb(16O, 12Cα), E=1000 MeV; calculated virtual photon spectra and kinematical loci; 7Be(γ, α), E ≥ 1.658 MeV; 16O(γ, α), E ≥ 8.162 MeV; calculated σ. Coulomb dissociation mechanism.
doi: 10.1016/0375-9474(86)90290-3
1986BA89 Phys.Lett. 178B, 135 (1986) Breakup Reactions as an Indirect Method to Investigate Low-Energy Charged-Particle Reactions Relevant for Nuclear Astrophysics
doi: 10.1016/0370-2693(86)91483-8
1986GO18 Phys.Rev. C34, 1229 (1986) M.Godlewski, J.Lang, R.Muller, P.A.Schmelzbach, J.Sromicki, L.Jarczyk, A.Strzalkowski, H.Witala, G.Baur Polarization Effects in Sub-Coulomb Breakup of Deuterons NUCLEAR REACTIONS 197Au, 208Pb(polarized d, np), E=9, 10.5, 12 MeV; measured σ(θn, θp, Ep), asymmetry following breakup, tensor analyzing power vs θn, θp, φ. Solid state detector, liquid scintillator. DWBA.
doi: 10.1103/PhysRevC.34.1229
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
1984HO04 Z.Phys. A315, 57 (1984) Effects of Nuclear Polarizability on Isotope Shifts in Electronic Atoms NUCLEAR STRUCTURE 208Pb; calculated s1/2 polarization shift, B(E1). 148,150,152,154Sm; calculated B(E2), rms radii differences. Perturbation theory, nuclear polarizability effect on electronic isotope shifts.
doi: 10.1007/BF01436209
1984HO14 Phys.Rev. C30, 247 (1984) Coulomb Dissociation at Nonrelativistic and Relativistic Energies NUCLEAR REACTIONS, ICPND 208Pb(α, α'), E=96, 172, 480 MeV; calculated σ(θ). 232Th(d, np), E=0.01-10 GeV; 208Pb(d, np), E=0.2=10 GeV; calculated Coulomb dissociation σ(E). DWBA model.
doi: 10.1103/PhysRevC.30.247
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
1980BE11 Nucl.Phys. A343, 221 (1980) U.Bechstedt, H.Machner, G.Baur, R.Shyam, C.Alderliesten, O.Bousshid, A.Djaloeis, P.Jahn Experimental and Theoretical Study of Continuous Proton Spectra from High-Energy Deuteron Induced Reactions NUCLEAR REACTIONS 27Al, 93Nb, 197Au(d, pX), E=80 MeV; measured σ(θp, Ep), integral σ(Ep); deduced reaction mechanism.
doi: 10.1016/0375-9474(80)90651-X
1980FU04 Nucl.Phys. A343, 133 (1980) H.Fuchs, J.A.Nolen, G.J.Wagner, H.Lenske, G.Baur Experimental and Theoretical Study of Line Shapes in 13C(α, α') Inelastic Scattering to Resonant States NUCLEAR REACTIONS 13C(α, α'), E=22, 36 MeV; measured σ(Eα, θ). 13C resonance deduced line shape parameter. Enriched target.
doi: 10.1016/0375-9474(80)90645-4
1980LE14 Nucl.Phys. A344, 151 (1980) The Role of the Coulomb Interaction in Isospin-Violating Direct Nuclear Reactions NUCLEAR REACTIONS 13C(d, t), (d, 3He), E=24-26 MeV; 12C(d, d'), E=24.1-50 MeV; calculated σ(θ). 12C levels deduced isospin mixing effects. Coulomb interaction, target wave function effects, direct reaction mechanism.
doi: 10.1016/0375-9474(80)90436-4
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
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
1978BA11 Phys.Rev. C17, 819 (1978) G.Baur, V.A.Madsen, F.Osterfeld Microscopic Theory of the Imaginary Inelastic Transition Form Factor NUCLEAR REACTIONS 40Ca(n, n'), E=30 MeV; calculated form factor.
doi: 10.1103/PhysRevC.17.819
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
1977BA22 Nucl.Phys. A282, 201 (1977) On the Line Shape in Inelastic Scattering Leading to Resonant States NUCLEAR REACTIONS 25Mg, 16N(p, p'), E=40 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(77)90212-3
1977BA29 Nucl.Phys. A283, 521 (1977) On the Direct Capture to Unbound States NUCLEAR REACTIONS 12C(p, γ); calculated σ for resonances in 13N.
doi: 10.1016/0375-9474(77)90555-3
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
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
1976BA31 Nucl.Phys. A265, 101 (1976) Investigations of the Deuteron Break-up on Heavy Nuclei Above the Coulomb Barrier NUCLEAR REACTIONS 197Au(d, pn), E=9-18 MeV; 208Pb(d, pn), E=11, 17 MeV; calculated σ. DWBA calculations.
doi: 10.1016/0375-9474(76)90118-4
1976BA36 Phys.Lett. 63B, 248 (1976) Sequential Transfer Mechanism in the Elastic Scattering of Nearly Identical Heavy Ions NUCLEAR REACTIONS 30Si(28Si, 28Si), (28Si, 29Si), E=70 MeV; calculated σ(θ).
doi: 10.1016/0370-2693(76)90255-0
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
1975KA24 Nucl.Phys. A250, 364 (1975) D.Kalinsky, D.Melnik, U.Smilansky, N.Trautner, B.A.Watson, Y.Horowitz, S.Mordechai, G.Baur, D.Pelte Nuclear Reactions between Oxygen Isotopes NUCLEAR REACTIONS 16O(17O, 17O), (18O, 18O), E(cm)=12-16, 19-20 MeV; measured σ(θ).
doi: 10.1016/0375-9474(75)90266-3
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
1974BA46 Phys.Lett. 51B, 205 (1974) Multistep Transfer Processes in Inelastic Heavy Ion Reactions NUCLEAR REACTIONS 17O(16O, 16O'), E=22, 24, 28, 32 MeV; calculated σ(θ).
doi: 10.1016/0370-2693(74)90274-3
1974GE01 Nucl.Phys. A219, 253 (1974) C.K.Gelbke, G.Baur, R.Bock, P.Braun-Munzinger, W.Grochulski, H.L.Harney, R.Stock Interference between Inelastic Scattering and Transfer in the Scattering of 16O on 17O NUCLEAR REACTIONS 17O(16O, 16O'), E(lab)=22, 24, 28, 32 MeV; measured σ(θ), for θ(cm)=129° measured σ(E); enriched targets.
doi: 10.1016/0375-9474(74)90065-7
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
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