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NSR database version of April 25, 2024.

Search: Author = E.Kolbe

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2011KO46      J.Korean Phys.Soc. 59, 1174s (2011)

E.Kolbe, A.Vasiliev, H.Ferroukhi

Assessement of the JEFF-3.1.1 Neutron Data Library for FOR CSE of LWR Fuel Storage Pools

doi: 10.3938/jkps.59.1174
Citations: PlumX Metrics

2011VA15      J.Korean Phys.Soc. 59, 2047s (2011)

A.Vasiliev, E.Kolbe, H.Ferroukhi, R.Pittarello

Comparison of Neutron Data Libraries for the Analysis of the "H. B. ROBINSON-2 Pressure Vessel Benchmark" with the MCNPX Code

COMPILATION ⁴⁶Ti, ⁵⁴Fe(n, p), E=1-20 MeV; calculated, evaluated σ, variance using JEFF-3.1.1, ENDF/B-VII.0, IRDF-2002 libraries.

doi: 10.3938/jkps.59.2047
Citations: PlumX Metrics

2008VA12      Ann.Nucl.Energy 35, 2432 (2008)

A.Vasiliev, E.Kolbe, H.Ferroukhi, M.A.Zimmermann, R.Chawla

On the performance of ENDF/B-VII.0 data for fast neutron fluence calculations

doi: 10.1016/j.anucene.2008.07.009
Citations: PlumX Metrics

2007TH10      Int.J.Mod.Phys. E16, 1149 (2007)

F.-K.Thielemann, D.Mocelj, I.Panov, E.Kolbe, T.Rauscher, K.-L.Kratz, K.Farouqi, B.Pfeiffer, G.Martinez-Pinedo, A.Kelic, K.Langanke, K.-H.Schmidt, N.Zinner

The R-process: Supernovae and other sources of the heaviest elements

doi: 10.1142/S0218301307006587
Citations: PlumX Metrics

2005HE02      Phys.Lett. B 606, 258 (2005)

A.Heger, E.Kolbe, W.C.Haxton, K.Langanke, G.Martinez-Pinedo, S.E.Woosley

Neutrino nucleosynthesis

doi: 10.1016/j.physletb.2004.12.017
Citations: PlumX Metrics

2005KE02      Phys.Lett. B 616, 48 (2005)

A.Kelic, N.Zinner, E.Kolbe, K.Langanke, K.-H.Schmidt

Cross sections and fragment distributions from neutrino-induced fission on r-process nuclei

NUCLEAR REACTIONS ²⁰⁰Yb, ^199,215Lu, ^202,214Hf, ¹⁹⁹Ta, ²⁰⁰W, ^201,215Re, ^200,214,226Os, ¹⁹⁹Ir, ²⁰⁰Pt, ²¹⁵Au, ^216,234Hg, ²³³Tl, ²¹⁶Pb, ^231,245Bi, ^215,233At, ²³⁴Rn, ^215,233,261Fr, ^216,230,246Ra, ^215,231Ac, ^230,274Th, ^{216,229,259,275}Pa, ^{216,232,238,246,254,262,270,278,286,294,302}U, ^231,281Np, ²⁸⁶Pu, ^245,275,293Am, ²⁹⁶Cm, ^245,259,297Bk, ^276,300Cf, ³⁰¹Es, ^246,260,304Fm, ³⁰⁷Md, ^276,308No, ^261,313Lr, ³¹⁴Rf, ³²¹Db, ^276,322Sg, ^261,325Bh, ³²⁴Hs, ²⁷⁶Ds, ²⁷⁶Cn(ν, F), (ν, X), (ν, xn), E=spectrum; calculated total, fission, neutron evaporation σ, fission fragment mass distributions.

doi: 10.1016/j.physletb.2005.04.074
Citations: PlumX Metrics

2005PA06      Nucl.Phys. A747, 633 (2005)

I.V.Panov, E.Kolbe, B.Pfeiffer, T.Rauscher, K.-L.Kratz, F.-K.Thielemann

Calculations of fission rates for r-process nucleosynthesis

NUCLEAR STRUCTURE A=250-320; calculated neutron-induced and β-delayed fission rates, related features. Astrophysical implications discussed.

doi: 10.1016/j.nuclphysa.2004.09.115
Citations: PlumX Metrics

2005TH04      Nucl.Phys. A751, 301c (2005)

F.-K.Thielemann, D.Argast, F.Brachwitz, J.L.Fisker, C.Frohlich, R.Hirschi, E.Kolbe, D.Mocelj, T.Rauscher

Nuclear Physics: A Key Ingredient in Astrophysical Modeling

doi: 10.1016/j.nuclphysa.2005.02.111
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2004KO13      Phys.Rev.Lett. 92, 111101 (2004)

E.Kolbe, K.Langanke, G.M.Fuller

Neutrino-Induced Fission of Neutron-Rich Nuclei

NUCLEAR REACTIONS ^{232,240,248,256}Po, ^{228,236,244,252,260}Rn, ^{230,238,246,254,262}Ra, ^{232,240,248,256,264}Th, ^{238,246,254,262,270}U(ν, F), E=spectrum; calculated neutrino-induced fission σ. Astrophysical implications discussed.

doi: 10.1103/PhysRevLett.92.111101
Citations: PlumX Metrics

2004NI17      Nucl.Phys. A746, 513c (2004)

T.Nilsson, J.Aysto, K.Langanke, K.Riisager, G.Martinez-Pinedo, E.Kolbe

Muonic radioactive atoms - a unique probe for nuclear structure

doi: 10.1016/j.nuclphysa.2004.09.139
Citations: PlumX Metrics

2003HE16      Nucl.Phys. A718, 159c (2003)

A.Heger, S.E.Woosley, K.Langanke, E.Kolbe, T.Rauscher, R.D.Hoffman

Nucleosynthesis of heavy elements in massive stars

doi: 10.1016/S0375-9474(03)00708-5
Citations: PlumX Metrics

2003KA20      Phys.Rev. D 67, 076007 (2003)

Y.Kamyshkov, E.Kolbe

Signatures of nucleon disappearance in large underground detectors

NUCLEAR STRUCTURE ¹²C; analyzed decay modes following neutron disappearance, experimental signatures in underground scintillator detectors.

doi: 10.1103/PhysRevD.67.076007
Citations: PlumX Metrics

2003KO50      J.Phys.(London) G29, 2569 (2003)

E.Kolbe, K.Langanke, G.Martinez-Pinedo, P.Vogel

Neutrino-nucleus reactions and nuclear structure

NUCLEAR REACTIONS ¹⁶O(ν, eX), (ν, μ^-X), E=100-500 MeV; calculated σ, σ(θ). ¹²C(ν, μ^-), E=120-240 MeV; calculated σ. ¹⁶O, ⁵⁶Fe, ²⁰⁸Pb(ν, ν'), (ν, ν'n), (ν, ν'p), (ν, ν'X), (ν-bar, e⁺), (ν-bar, e⁺n), (ν-bar, e⁺α), (ν-bar, e⁺X), ¹⁶O, ⁵⁶Fe, ¹³⁸Ba, ²⁰⁸Pb(ν, ep), ¹⁶O(ν, ν'np), (ν, ν'2n), (ν, ν'2p), (ν, ν'nα), (ν, ν'pα), (ν, enpα), (ν-bar, e⁺nα), (ν-bar, e⁺2n), (ν-bar, e⁺np), ¹⁶O, ¹³⁸Ba(ν, enp), (ν, e2p), (ν, epα), ¹⁶O, ⁵⁶Fe, ¹³⁸Ba(ν, eα), ¹⁶O, ⁵⁶Fe(ν, eX), ⁵⁶Fe(ν, ν'α), ⁵⁶Fe, ²⁰⁸Pb(ν, e), (ν-bar, e⁺p), ⁵⁶Fe, ¹³⁸Ba, ²⁰⁸Pb(ν, en), ¹³⁸Ba(ν, e2n), (ν, enα), (ν, e2α), E=spectrum; calculated σ, σ(E).

doi: 10.1088/0954-3899/29/11/010
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2003KO52      Nucl.Phys. A719, 135c (2003)

E.Kolbe

Semileptonic weak interactions in nuclei within continuum RPA

doi: 10.1016/S0375-9474(03)00983-7
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2003SA32      Nucl.Phys. A718, 440c (2003)

J.M.Sampaio, K.Langanke, G.Martinez-Pinedo, E.Kolbe, D.J.Dean

Electron capture rates for core collapse supernovae

NUCLEAR REACTIONS ¹H, ⁷⁰Cu, ⁷²Zn, ⁷⁶Ga, ⁹³Kr(e, ν), E=stellar; calculated neutrino energies, capture rates vs chemical potential, temperature. Implications for supernovae core collapse discussed.

doi: 10.1016/S0375-9474(02)00832-7
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2003ZI02      Eur.Phys.J. A 17, 625 (2003)

N.T.Zinner, K.Langanke, K.Riisager, E.Kolbe

Muon capture on nickel and tin isotopes

NUCLEAR REACTIONS ^{48,50,52,54,56,58,60,62,64,66,68,70,72,74,76,78,80,82,84,86}Ni, ^{100,104,108,112,114,116,118,120,122,124,128,132,136,140,144,148,152,156,160}Sn(μ, X), E at rest; calculated muon capture rates; deduced nuclear structure effects.

doi: 10.1140/epja/i2003-10020-8
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2002BE18      Phys.Rev. C65, 035801 (2002)

D.Belic, C.Arlandini, J.Besserer, J.de Boer, J.J.Carroll, J.Enders, T.Hartmann, F.Kappeler, H.Kaiser, U.Kneissl, E.Kolbe, K.Langanke, M.Loewe, H.J.Maier, H.Maser, P.Mohr, P.von Neumann-Cosel, A.Nord, H.H.Pitz, A.Richter, M.Schumann, F.-K.Thielemann, S.Volz, A.Zilges

Photo-Induced Depopulation of the ¹⁸⁰Ta^m Isomer via Low-Lying Intermediate States: Structure and astrophysical implications

NUCLEAR REACTIONS ^180mTa(γ, γ'), E=0.8-3.1 MeV bremsstrahlung; measured delayed Eγ, Iγ, X-ray spectra; deduced activation yields. ¹⁸⁰Ta deduced intermediate states energies, transition strengths. Astrophysical implications discussed. Comparisons with previous results, model predictions.

RADIOACTIVITY ¹⁸⁰Ta(EC), (β^-); measured T_1/2.

doi: 10.1103/PhysRevC.65.035801
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2001KO04      Phys.Rev. C63, 025802 (2001)

E.Kolbe, K.Langanke

Role of ν-Induced Reactions on Lead and Iron in Neutrino Detectors

NUCLEAR REACTIONS ⁵⁶Fe, ²⁰⁸Pb(ν, e), (ν, eX), (ν, ν'X), E=10-150 MeV; calculated total σ, branching ratios, excitation energy spectra, neutron spectra. Implications for accelerator-based and solar neutrino measurements discussed.

doi: 10.1103/PhysRevC.63.025802
Citations: PlumX Metrics

2001KO38      Eur.Phys.J. A 11, 39 (2001)

E.Kolbe, K.Langanke, K.Riisager

Muon Capture on Neutron-Rich Nuclei

NUCLEAR REACTIONS ^{40,44,48,52,56,60}Ca(μ^-, ν), E at rest; calculated muon capture rates, excitation energy spectra, structure effects.

doi: 10.1007/s100500170094
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2001LA05      Phys.Rev. C63, 032801 (2001)

K.Langanke, E.Kolbe, D.J.Dean

Unblocking of the Gamow-Teller Strength in Stellar Electron Capture on Neutron-Rich Germanium Isotopes

NUCLEAR REACTIONS ^68,72,76Ge(e, ν), E=12-30 MeV; calculated electron capture σ in stellar medium as a function of temperature. Shell Model Monte Carlo calculations, comparison with independent-particle model calculations, effects on core-collapsed supernovae discussed.

NUCLEAR STRUCTURE ^{68,70,72,74,76}Ge; calculated proton and neutron occupation percentages for nuclei in stellar medium as a function of temperature.

doi: 10.1103/PhysRevC.63.032801
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2001LA32      At.Data Nucl.Data Tables 79, 293 (2001)

K.Langanke, E.Kolbe

Neutrino-Induced Charged-Current Reaction Rates for r-Process Nuclei

COMPILATION Z=21-82; calculated neutrino-induced charged-current reaction rates, spallation neutron σ.

doi: 10.1006/adnd.2001.0872
Citations: PlumX Metrics

2001TH08      Prog.Part.Nucl.Phys. 46, 5 (2001)

F.-K.Thielemann, F.Brachwitz, C.Freiburghaus, E.Kolbe, G.Martinez-Pinedo, T.Rauscher, F.Rembges, W.R.Hix, M.Liebendorfer, A.Mezzacappa, K.-L.Kratz, B.Pfeiffer, K.Langanke, K.Nomoto, S.Rosswog, H.Schatz, M.Wiescher

Element Synthesis in Stars

doi: 10.1016/S0146-6410(01)00103-X
Citations: PlumX Metrics

2001TO20      Nucl.Phys. A694, 395 (2001)

J.Toivanen, E.Kolbe, K.Langanke, G.Martinez-Pinedo, P.Vogel

Supernova Neutrino Induced Reactions on Iron Isotopes

NUCLEAR REACTIONS ^{52,53,54,55,56,57,58,59,60}Fe(ν, X), E=2.5-50 MeV; calculated total charged- and neutral-current σ.

doi: 10.1016/S0375-9474(01)00992-7
Citations: PlumX Metrics

2000HE07      Phys.Rev. C61, 055803 (2000)

A.Hektor, E.Kolbe, K.Langanke, J.Toivanen

Neutrino-Induced Reaction Rates for r-Process Nuclei

NUCLEAR REACTIONS ¹²²Zr, ¹²⁴Mo, ¹²⁶Ru, ¹²⁸Pd, ¹³⁰Cd, ¹³²Sn(ν, e), (ν, ν'), E < 40 MeV; calculated excitation functions, neutron emission probabilities. ⁷⁴Fe, ¹²⁴Mo, ¹⁹²Er(ν, e), E not given; calculated multipole contributions to σ. Implications for astrophysical r-process discussed. Other targets considered.

doi: 10.1103/PhysRevC.61.055803
Citations: PlumX Metrics

2000KO57      Phys.Rev. C62, 055502 (2000)

E.Kolbe, K.Langanke, P.Vogel

Muon Capture on Nuclei with N > Z, Random Phase Approximation, and In-Medium Value of the Axial-Vector Coupling Constant

NUCLEAR REACTIONS ^40,44,48Ca, ⁵⁶Fe, ⁹⁰Zr, ²⁰⁸Pb(μ^-, ν), E at rest; calculated muon capture rates. Continuum and standard RPA.

ATOMIC PHYSICS, Mesic-atoms ^40,44,48Ca, ⁵⁶Fe, ⁹⁰Zr, ²⁰⁸Pb(μ^-, ν), E at rest; calculated muon capture rates. Continuum and standard RPA.

doi: 10.1103/PhysRevC.62.055502
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1999KO24      Nucl.Phys. A652, 91 (1999)

E.Kolbe, K.Langanke, P.Vogel

Weak Reactions on ¹²C within the Continuum Random Phase Approximation with Partial Occupancies

NUCLEAR REACTIONS ¹²C(ν, e), (ν, e⁺), E=20-300; ¹²C(μ^-, ν), E not given; calculated σ; ¹²C(ν, μ^-), E not given; calculated σ vs excitation energy; deduced role of partial subshell occupancies. Continuum RPA.

doi: 10.1016/S0375-9474(99)00152-9
Citations: PlumX Metrics

1999KO49      Phys.Rev. C60, 052801 (1999)

E.Kolbe, K.Langanke, G.Martinez-Pinedo

Inclusive ⁵⁶Fe(ν_e, e^-)⁵⁶Co Cross Section

NUCLEAR REACTIONS ⁵⁶Fe(ν, e), E=spectrum; calculated σ(E), total σ. Comparison with data.

doi: 10.1103/PhysRevC.60.052801
Citations: PlumX Metrics

1998KO65      Eur.Phys.J. A 3, 389 (1998)

E.Kolbe, K.Langanke, F.-K.Thielemann

The Role of Strange Sea Quarks on Neutrino-Nucleus Reactions in Superkamiokande and in the Supernova r-Process

NUCLEAR REACTIONS ¹⁶O(ν, ν'X), (ν, ν'n), (ν, ν'p), E < 300 MeV; calculated total σ, γ-emission probability; deduced role of strange component of axial vector form factor. ¹³⁰Cd(ν, ν'n), E not given; calculated total σ vs strange form factor. Implications for astrophysical r-process discussed.

doi: 10.1007/s100500050194
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1997KO04      Nucl.Phys. A613, 382 (1997)

E.Kolbe, K.Langanke, P.Vogel

Comparison of Continuum Random Phase Approximation and the Elementary Particle Model for the Inclusive Muon Neutrino Reaction on ¹²C

NUCLEAR REACTIONS ¹²C(e, e'), E=80.9-148.5 MeV; analyzed σ(θ) vs energy transfer. ¹²C(ν, μ^-), E=135-250 MeV; ¹²C(ν, e^-), E=36-250 MeV; calculated σ(θ), σ vs energy transfer. Continuum RPA.

doi: 10.1016/S0375-9474(96)00417-4
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1997KO38      Z.Phys. A358, 445 (1997)

E.Kolbe, S.Krewald, H.Weigel

Strangeness in the Nucleon and the Ratio of Proton-to-Neutron Neutrino-Induced Quasi-Elastic Yield

NUCLEAR REACTIONS ¹²C(ν, ν'), (ν-bar, ν-bar'), E not given; calculated proton-to-neutron yield ratio. Nucleon electroweak form factors from three flavor pseudoscalar vector meson soliton model.

doi: 10.1007/s002180050353
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1996EN06      Phys.Rev. C54, 2740 (1996)

J.Engel, E.Kolbe, K.Langanke, P.Vogel

Neutrino Induced Transitions between the Ground States of the A = 12 Triad

NUCLEAR REACTIONS ¹²C(ν, e^-), (ν, μ^-)(ν, μ⁺), E ≤ 300 MeV; calculated σ(E); deduced incident spectrum normalization, detector efficiency related features.

doi: 10.1103/PhysRevC.54.2740
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1996KO32      Phys.Rev. C54, 1741 (1996)

E.Kolbe

Differential Cross Sections for Neutrino Scattering on ¹²C

NUCLEAR REACTIONS ¹²C(ν, μ^-), (ν, e^-), E not given; calculated σ(θ). Continuum RPA.

doi: 10.1103/PhysRevC.54.1741
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1995KO40      Phys.Rev. C52, 3437 (1995)

E.Kolbe, K.Langanke, F.-K.Thielemann, P.Vogel

Inclusive ¹²C(ν(μ), μ)¹²N Reaction in the Continuum Random Phase Approximation

NUCLEAR REACTIONS ¹²C(ν, μ^-X), (ν, μ⁺X), (ν-bar, μ⁺X), E not given; ¹²C(ν, e^-), (ν, e⁺), (ν-bar, e^-), (ν-bar, e⁺), E=20-250 MeV; calculated total, partial σ, branching ratios for several exit channels. Continuum RPA.

doi: 10.1103/PhysRevC.52.3437
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1994KO03      Phys.Rev. C49, 1122 (1994)

E.Kolbe, K.Langanke, S.Krewald

Neutrino-Induced Reactions on ¹²C within the Continuum Random Phase Approximation

NUCLEAR REACTIONS ¹²C(ν, μ^-), E=125-300 MeV; calculated σ(E), differential σ. ¹²C(ν, e^-), (ν, ν'), E not given; calculated σ. Different interactions, different mechanisms for production of ν.

doi: 10.1103/PhysRevC.49.1122
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1994KO27      Phys.Rev. C50, 2576 (1994)

E.Kolbe, K.Langanke, P.Vogel

Muon Capture, Continuum Random Phase Approximation, and In-Medium Renormalization of the Axial-Vector Coupling Constant

NUCLEAR REACTIONS ¹⁶O, ⁴⁰Ca, ¹²C(μ^-, ν), E at rest; calculated total capture rates. Continuum RPA.

ATOMIC PHYSICS, Mesic-Atoms ¹⁶O, ⁴⁰Ca, ¹²C(μ^-, ν), E at rest; calculated total capture rates. Continuum RPA.

doi: 10.1103/PhysRevC.50.2576
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1993GA20      Phys.Rev. C48, 1919 (1993)

G.Garvey, E.Kolbe, K.Langanke, S.Krewald

Role of Strange Quarks in Quasielastic Neutrino Scattering

NUCLEAR REACTIONS ¹²C(ν, ν'n), (ν, ν'p), (ν-bar, ν-bar'n), (ν-bar, ν-bar'p), E not given; calculated neutron, proton yield ratio; deduced strange quarks role. Continiuum RPA.

doi: 10.1103/PhysRevC.48.1919
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1992GA14      Phys.Lett. 289B, 249 (1992)

G.T.Garvey, S.Krewald, E.Kolbe, K.Langanke

Strange Quark Contributions to Neutrino Induced Quasielastic Scattering

NUCLEAR REACTIONS ¹²C(ν, ν'n), (ν, ν'p), E=200 MeV; calculated angle integrated σ, proton-to-neutron yield ratio; deduced strange quark axial form factor sensitivity to yield ratio.

doi: 10.1016/0370-2693(92)91214-T
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1992KO06      Phys.Rev. C45, 2464 (1992)

E.Kolbe, K.Langanke, S.Krewald

Comparison of Inelastic Neutrino and Antineutrino Scattering on Nuclei

NUCLEAR REACTIONS ¹²C, ¹⁶O(ν, ν'), (ν-bar, ν-bar'), E=29.8 MeV; calculated inelastic scattering angle integrated σ. Other target nuclei studied. Continuum RPA.

doi: 10.1103/PhysRevC.45.2464
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1992KO07      Nucl.Phys. A540, 599 (1992)

E.Kolbe, K.Langanke, S.Krewald, F.-K.Thielemann

Inelastic Neutrino Scattering on ¹²C and ¹⁶O Above the Particle Emission Threshold

NUCLEAR REACTIONS ¹²C(ν, ν'), E ≈ 20-35 MeV; ¹⁶O(ν, ν'), E ≈ 12-38 MeV; ¹²C(ν-bar, ν-bar'), (ν-bar, e⁺), (ν, e^-), E ≈ 15-40 MeV; ¹⁶O(ν-bar, ν-bar'), (ν-bar, e⁺), (ν, e^-), E ≈ 13-39 MeV; calculated angle integrated σ. Extended continuum RPA theory.

doi: 10.1016/0375-9474(92)90175-J
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1988AL24      Z.Phys. A330, 277 (1988)

T.Altmeyer, E.Kolbe, T.Warmann, K.Langanke, H.J.Assenbaum

On Discrepancies within the Experimental and Theoretical Low Energy ³H(α, γ)⁷Li Cross Sections

NUCLEAR REACTIONS, ICPND ³H(α, γ), E ≈ 50-600 keV; calculated σ(E), S-factor vs E. Resonating group method.

1988KO29      Phys.Lett. 214B, 169 (1988)

E.Kolbe, K.Langanke, H.J.Assenbaum

Microscopic Study of the Low-Energy ⁷Be(p, γ)⁸B Reaction

NUCLEAR REACTIONS, ICPND ⁷Be(p, γ), E < 500 keV; calculated astrophysical S-factor vs E.

doi: 10.1016/0370-2693(88)91462-1
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