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NSR database version of April 11, 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
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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
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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, 216,229,259,275Pa, 216,232,238,246,254,262,270,278,286,294,302U, 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
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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
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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 232,240,248,256Po, 228,236,244,252,260Rn, 230,238,246,254,262Ra, 232,240,248,256,264Th, 238,246,254,262,270U(ν, F), E=spectrum; calculated neutrino-induced fission σ. Astrophysical implications discussed.

doi: 10.1103/PhysRevLett.92.111101
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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
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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
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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 48,50,52,54,56,58,60,62,64,66,68,70,72,74,76,78,80,82,84,86Ni, 100,104,108,112,114,116,118,120,122,124,128,132,136,140,144,148,152,156,160Sn(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 180Tam 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 T1/2.

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

E.Kolbe, K.Langanke, K.Riisager

Muon Capture on Neutron-Rich Nuclei

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

doi: 10.1007/s100500170094
Citations: PlumX Metrics


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 68,70,72,74,76Ge; 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
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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
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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 52,53,54,55,56,57,58,59,60Fe(ν, X), E=2.5-50 MeV; calculated total charged- and neutral-current σ.

doi: 10.1016/S0375-9474(01)00992-7
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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
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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
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1999KO49      Phys.Rev. C60, 052801 (1999)

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

Inclusive 56Fe(νe, 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
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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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