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Search: Author = G.Baur

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2008BA11      J.Phys.(London) G35, 014028 (2008)

G.Baur, S.Typel

Coulomb dissociation, a tool for nuclear astrophysics

doi: 10.1088/0954-3899/35/1/014028
Citations: PlumX Metrics

2008TY03      Eur.Phys.J. A 38, 355 (2008)

S.Typel, G.Baur

Scaling laws and higher-order effects in Coulomb excitation of neutron halo nuclei

doi: 10.1140/epja/i2008-10864-4
Citations: PlumX Metrics

2007BA39      Prog.Part.Nucl.Phys. 59, 122 (2007)

G.Baur, S.Typel

Direct reactions with exotic nuclei, nuclear structure and astrophysics

doi: 10.1016/j.ppnp.2006.12.002
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2007BA41      Phys.Rev. C 75, 058801 (2007)

G.Baur, K.A.Snover, S.Typel

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
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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
Citations: PlumX Metrics

2005TY02      Nucl.Phys. A759, 247 (2005)

S.Typel, G.Baur

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
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2004BA74      Prog.Theor.Phys.(Kyoto), Suppl. 154, 333 (2004)

G.Baur, S.Typel

Theory of the Trojan-Horse Method

doi: 10.1143/PTPS.154.333
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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
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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
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2004TY01      Phys.Rev.Lett. 93, 142502 (2004)

S.Typel, G.Baur

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
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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
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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
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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
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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
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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
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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
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2001TY01      Phys.Rev. C64, 024601 (2001)

S.Typel, G.Baur

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
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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
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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
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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
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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
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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
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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
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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
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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
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1997BA40      Phys.Rev. C56, 581 (1997)

G.Baur, C.A.Bertulani

Comment on ' Quantum-Mechanical Equivalent-Photon Spectrum for Heavy Ion Physics "

doi: 10.1103/PhysRevC.56.581
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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
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1997TY01      Nucl.Phys. A613, 147 (1997)

S.Typel, H.H.Wolter, G.Baur

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
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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
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1996KA06      J.Phys.(London) G22, 115 (1996)

D.M.Kalassa, G.Baur

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
Citations: PlumX Metrics

1996MU11      Nucl.Phys. A609, 254 (1996)

A.Mundel, G.Baur

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
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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
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1995TY01      Phys.Lett. 356B, 186 (1995)

S.Typel, G.Baur

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
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1994BA04      Phys.Rev. C49, 1127 (1994)

N.Baron, G.Baur

γγ Physics at Relativistic Heavy-Ion Colliders

doi: 10.1103/PhysRevC.49.1127
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1994BB15      J.Phys.(London) G20, 1 (1994)

G.Baur, H.Rebel

Coulomb Dissociation Studies as a Tool of Nuclear Astrophysics

doi: 10.1088/0954-3899/20/1/005
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1994KA25      J.Phys.(London) G20, 1023 (1994)

D.M.Kalassa, G.Baur

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
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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
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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
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1994TY01      Phys.Rev. C49, 379 (1994)

S.Typel, G.Baur

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
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1994TY02      Nucl.Phys. A573, 486 (1994)

S.Typel, G.Baur

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
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1994TY03      Phys.Rev. C50, 2104 (1994)

S.Typel, G.Baur

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
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1993BA40      Nucl.Phys. A561, 628 (1993)

G.Baur, N.Baron

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
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1993NO06      Phys.Rev. C48, 1915 (1993)

J.W.Norbury, G.Baur

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
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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
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1992SH09      Nucl.Phys. A540, 341 (1992)

R.Shyam, P.Banerjee, G.Baur

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
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1991BA36      Nucl.Phys. A530, 267 (1991)

N.Baron, G.Baur, M.Schumacher

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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2209.

1991SH11      Phys.Rev. C44, 915 (1991)

R.Shyam, G.Baur, P.Banerjee

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
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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
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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
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1989BA16      J.Phys.(London) G15, 661 (1989)

G.Baur, N.Baron

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
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1989BA64      Nucl.Phys. A504, 352 (1989)

G.Baur, M.Weber

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
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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
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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)

C.A.Bertulani, G.Baur

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
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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
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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
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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
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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
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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
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1984HO04      Z.Phys. A315, 57 (1984)

B.Hoffmann, G.Baur, J.Speth

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
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1984HO14      Phys.Rev. C30, 247 (1984)

B.Hoffmann, G.Baur

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
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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
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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
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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
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1983TR13      Nucl.Instrum.Methods 214, 21 (1983)

D.Trautmann, F.Rosel, G.Baur

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
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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
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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
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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
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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
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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
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1980LE14      Nucl.Phys. A344, 151 (1980)

H.Lenske, G.Baur

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
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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
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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
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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
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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
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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
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1978BA21      J.Phys.(London) G4, 275 (1978)

G.Baur, F.Roesel, D.Trautmann

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
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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
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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
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1977BA22      Nucl.Phys. A282, 201 (1977)

G.Baur, H.Lenske

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
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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
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1977BA53      Nucl.Phys. A288, 113 (1977)

G.Baur, F.Rosel, D.Trautmann

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
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1977TR09      Nukleonika 22, 485 (1977)

D.Trautmann, G.Baur

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)

G.Baur, M.Pauli, D.Trautmann

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
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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
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1976BA36      Phys.Lett. 63B, 248 (1976)

G.Baur, H.H.Wolter

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
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1975BA61      Nucl.Phys. A252, 77 (1975)

G.Baur, F.Rosel, D.Trautmann

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
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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
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1974BA19      Z.Phys. 267, 103 (1974)

G.Baur, D.Trautmann

On the Theory of Stripping Reactions into the Continuum

NUCLEAR REACTIONS 14N, 16O, 24Mg(d, p); calculated σ(θ).

doi: 10.1007/BF01668636
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1974BA36      Nucl.Phys. A224, 477 (1974)

G.Baur, M.Pauli, D.Trautmann

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
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1974BA46      Phys.Lett. 51B, 205 (1974)

G.Baur, H.H.Wolter

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
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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
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1973BA08      Nucl.Phys. A199, 218 (1973)

G.Baur, D.Trautmann

Sub-Coulomb (d, p) Stripping Theory into the Continuum

doi: 10.1016/0375-9474(73)90344-8
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1973BA43      Nucl.Phys. A208, 261 (1973)

G.Baur, D.Trautmann, V.Zoran

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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