NSR Query Results

Output year order : Descending
Format : Normal

NSR database version of April 11, 2024.

Search: Author = V.Fohr

Found 9 matches.

Back to query form

2020DI05      Phys.Lett. B 811, 135962 (2020)

J.Diaz-Cortes, J.Benlliure, J.L.Rodriguez-Sanchez, H.Alvarez-Pol, T.Aumann, C.A.Bertulani, B.Blank, E.Casarejos, D.Cortina-Gil, D.Dragosavac, V.Fohr, A.Gargano, M.Gascon, W.Gawlikowicz, A.Heinz, K.Helariutta, A.Kelic-Heil, S.Lukic, F.Montes, D.Perez-Loureiro, L.Pienkowski, K.-H.Schmidt, M.Staniou, K.Subotic, K.Summerer, J.Taieb, A.Trzcinska

Systematic reduction of the proton-removal cross section in neutron-rich medium-mass nuclei

NUCLEAR REACTIONS ⁹Be(²³⁸U, X)¹³²Sn/¹³¹Sn/¹³¹In/¹²⁸Sn/¹³⁰Sn/¹³⁶Sn, E=950 MeV/nucleon; ⁹Be(¹³²Xe, X)¹¹⁹Sn/¹²⁴Sn/¹²⁶Sn, E=1200 MeV/nucleon; ⁹Be(¹¹⁹Sn, X), (¹²⁴Sn, X), (¹²⁶Sn, X), (¹³⁰Sn, X), (¹³¹Sn, X), (¹³²Sn, X), (¹²⁸Sn, X), (¹³⁶Sn, X), (¹³¹Sn, X), E ∼ 1000 MeV/nucleon; measured reaction products, TOF; deduced single neutron and single proton removal σ. Comparison with the advanced Liege intra-nuclear cascade (INCL) model calculations.

doi: 10.1016/j.physletb.2020.135962
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD8031.

2019PE09      Phys.Rev. C 99, 054606 (2019)

D.Perez-Loureiro, J.Benlliure, J.Diaz-Cortes, J.L.Rodriguez-Sanchez, H.Alvarez-Pol, B.Blank, E.Casarejos, D.Dragosavac, V.Fohr, M.Gascon, W.Gawlikowicz, A.Heinz, K.Helariutta, A.Kelic-Heil, S.Lukic, F.Montes, L.Pienkowski, K-H.Schmidt, M.Staniou, K.Subotic, K.Summerer, J.Taieb, A.Trzcinska

Neutron-rich fragments produced by in-flight fission of ²³⁸U

NUCLEAR REACTIONS ²⁰⁸Pb(²³⁸U, F)⁹⁰Kr/⁹¹Kr/⁹⁴Rb/⁹⁵Rb/⁹⁶Rb/⁹⁷Rb/⁹⁸Rb/⁹⁹Rb/¹⁰⁰Rb/⁹⁶Sr/⁹⁷Sr/⁹⁸Sr/⁹⁹Sr/¹⁰⁰Sr/¹⁰¹Sr/¹⁰²Sr/¹⁰³Sr/⁹⁹Y/¹⁰⁰Y/¹⁰¹Y/¹⁰²Y/¹⁰³Y/¹⁰⁴Y/¹⁰⁵Y/¹⁰⁶Y/¹⁰²Zr/¹⁰³Zr/¹⁰⁴Zr/¹⁰⁵Zr/¹⁰⁶Zr/¹⁰⁷Zr/¹⁰⁸Zr/¹⁰⁹Zr/¹⁰⁴Nb/¹⁰⁵Nb/¹⁰⁶Nb/¹⁰⁷Nb/¹⁰⁸Nb/¹⁰⁹Nb/¹¹⁰Nb/¹¹¹Nb/¹⁰⁷Mo/¹⁰⁸Mo/¹⁰⁹Mo/¹¹⁰Mo/¹¹¹Mo/¹¹²Mo/¹¹³Mo/¹¹⁰Tc/¹¹¹Tc/¹¹²Tc/¹¹³Tc/¹¹⁴Tc/¹¹⁵Tc/¹¹⁶Tc/¹¹⁷Tc/¹¹²Ru/¹¹³Ru/¹¹⁴Ru/¹¹⁵Ru/¹¹⁶Ru/¹¹⁷Ru/¹¹⁸Ru/¹¹⁹Ru/¹¹⁵Rh/¹¹⁶Rh/¹¹⁷Rh/¹¹⁸Rh/¹¹⁹Rh/¹²⁰Rh/¹²¹Rh/¹²²Rh/¹¹⁸Pd/¹¹⁹Pd/¹²⁰Pd/¹²¹Pd/¹²²Pd/¹²³Pd/¹²⁴Pd/¹²⁵Pd/¹²⁰Ag/¹²¹Ag/¹²²Ag/¹²³Ag/¹²⁴Ag/¹²⁵Ag/¹²⁶Ag/¹²⁷Ag/¹²⁸Ag/¹²³Cd/¹²⁴Cd/¹²⁵Cd/¹²⁶Cd/¹²⁷Cd/¹²⁸Cd/¹²⁹Cd/¹³⁰Cd/¹³¹Cd/¹²⁶In/¹²⁷In/¹²⁸In/¹²⁹In/¹³⁰In/¹³¹In/¹³²In/¹³³In/¹³⁴In/¹³⁵In/¹²⁸Sn/¹²⁹Sn/¹³⁰Sn/¹³¹Sn/¹³²Sn/¹³³Sn/¹³⁴Sn/¹³⁵Sn/¹³⁶Sn/¹³⁷Sn/¹³²Sb/¹³³Sb/¹³⁴Sb/¹³⁵Sb/¹³⁶Sb/¹³⁷Sb/¹³⁸Sb/¹³⁹Sb/¹³⁵Te/¹³⁶Te/¹³⁷Te/¹³⁸Te/¹³⁹Te/¹⁴⁰Te/¹⁴¹Te/¹⁴²Te/¹³⁷I/¹³⁸I/¹³⁹I/¹⁴⁰I/¹⁴¹I/¹⁴²I/¹⁴³I/¹⁴⁴I/¹⁴¹Xe/¹⁴²Xe/¹⁴³Xe/¹⁴⁴Xe/¹⁴⁵Xe/¹⁴⁶Xe/¹⁴⁷Xe/¹⁴⁴Cs/¹⁴⁵Cs/¹⁴⁶Cs/¹⁴⁷Cs/¹⁴⁸Cs/¹⁴⁹Cs/¹⁴⁵Ba/¹⁴⁶Ba/¹⁴⁷Ba/¹⁴⁸Ba/¹⁴⁹Ba/¹⁵⁰Ba/¹⁵¹Ba/¹⁴⁸La/¹⁴⁹La/¹⁵⁰La/¹⁵¹La/¹⁵²La/¹⁵³La/¹⁵¹Ce/¹⁵²Ce/¹⁵³Ce/¹⁵⁴Ce/¹⁵²Pr/¹⁵³Pr/¹⁵⁵Pr/¹⁵⁵Nd/¹⁵⁶Nd, E=950 MeV/nucleon; ⁹Be(²³⁸U, F)⁸⁰Ga/⁸⁴Ga/⁷⁹Ge/⁸⁰Ge/⁸²Ge/⁸³Ge/⁸⁴Ge/⁸¹As/⁸²As/⁸³As/⁸⁵As/⁸⁶As/⁸⁷As/⁸⁸As/⁸⁴Se/⁸⁵Se/⁸⁷Se/⁸⁸Se/⁸⁹Se/⁹⁰Se/⁸⁶Br/⁸⁷Br/⁸⁸Br/⁸⁹Br/⁹¹Br/⁹²Br/⁹³Br/⁹⁴Br/⁸⁹Kr/⁹⁰Kr/⁹¹Kr/⁹²Kr/⁹³Kr/⁹⁴Kr/⁹⁵Kr/⁹⁶Kr/⁹⁷Kr/⁹²Rb/⁹³Rb/⁹⁴Rb/⁹⁵Rb/⁹⁶Rb/⁹⁷Rb/⁹⁸Rb/⁹⁹Rb/¹⁰⁰Rb/¹⁰¹Rb/⁹⁴Sr/⁹⁵Sr/⁹⁶Sr/⁹⁷Sr/⁹⁸Sr/⁹⁹Sr/¹⁰⁰Sr/¹⁰¹Sr/¹⁰²Sr/¹⁰³Sr/⁹⁹Zr/¹⁰⁰Zr/¹⁰¹Zr/¹⁰²Zr/¹⁰³Zr/¹⁰⁴Zr/¹⁰⁵Zr/¹⁰⁶Zr/¹⁰⁷Zr/¹⁰⁸Zr/¹⁰⁹Zr/¹⁰²Nb/¹⁰³Nb/¹⁰⁴Nb/¹⁰⁵Nb/¹⁰⁶Nb/¹⁰⁷Nb/¹⁰⁸Nb/¹⁰⁹Nb/¹¹⁰Nb/¹¹¹Nb/¹¹²Nb/¹⁰⁵Mo/¹⁰⁶Mo/¹⁰⁷Mo/¹⁰⁸Mo/¹⁰⁹Mo/¹¹⁰Mo/¹¹¹Mo/¹¹²Mo/¹¹³Mo/¹¹⁴Mo/¹¹⁵Mo/¹⁰⁷Tc/¹⁰⁸Tc/¹⁰⁹Tc/¹¹⁰Tc/¹¹¹Tc/¹¹²Tc/¹¹³Tc/¹¹⁴Tc/¹¹⁵Tc/¹¹⁶Tc/¹¹⁷Tc/¹¹⁸Tc/¹¹⁰Ru/¹¹¹Ru/¹¹²Ru/¹¹³Ru/¹¹⁴Ru/¹¹⁵Ru/¹¹⁶Ru/¹¹⁷Ru/¹¹⁸Ru/¹¹⁹Ru/¹²⁰Ru/¹¹³Rh/¹¹⁴Rh/¹¹⁷Pd/¹¹⁸Pd/¹¹⁹Pd/¹²⁰Pd/¹²¹Pd/¹²²Pd/¹²³Pd/¹²⁴Pd/¹²⁵Pd/¹¹⁸Ag/¹¹⁹Ag/¹²⁰Ag/¹²¹Ag/¹²²Ag/¹²³Ag/¹²⁴Ag/¹²⁵Ag/¹²⁶Ag/¹²⁷Ag/¹²⁸Ag/¹²¹Cd/¹²²Cd/¹²³Cd/¹²⁴Cd/¹²⁵Cd/¹²⁶Cd/¹²⁷Cd/¹²⁸Cd/¹²⁹Cd/¹³⁰Cd/¹³¹Cd/¹³²Cd/¹²³In/¹²⁴In/¹²⁵In/¹²⁶In/¹²⁷In/¹²⁸In/¹²⁹In/¹³⁰In/¹³¹In/¹³²In/¹³³In/¹³⁴In/¹²⁶Sn/¹²⁷Sn/¹²⁸Sn/¹²⁹Sn/¹³⁰Sn/¹³¹Sn/¹³²Sn/¹³³Sn/¹³⁴Sn/¹³⁵Sn/¹³⁶Sn/¹³⁷Sn/¹²⁹Sb/¹³³Te/¹³⁴Te/¹³⁵Te/¹³⁶Te/¹³⁷Te/¹³⁸Te/¹³⁹Te/¹⁴⁰Te/¹⁴¹Te/¹⁴²Te/¹⁴³Te/¹³⁵I/¹³⁶I/¹³⁷I/¹³⁸I/¹³⁹I/¹⁴⁰I/¹⁴¹I/¹⁴²I/¹⁴³I/¹⁴⁴I/¹⁴⁵I/¹³⁷Xe/¹³⁸Xe/¹³⁹Xe/¹⁴⁰Xe/¹⁴¹Xe/¹⁴²Xe/¹⁴³Xe/¹⁴⁴Xe/¹⁴⁵Xe/¹⁴⁶Xe/¹⁴⁷Xe/¹⁴⁰Cs/¹⁴¹Cs/¹⁴²Cs/¹⁴³Cs/¹⁴⁴Cs/¹⁴⁵Cs/¹⁴⁶Cs/¹⁴⁷Cs/¹⁴⁸Cs/¹⁴⁹Cs/¹⁴³Ba/¹⁴⁴Ba/¹⁴⁵Ba/¹⁴⁶Ba/¹⁴⁷Ba/¹⁴⁸Ba/¹⁴⁹Ba/¹⁵⁰Ba/¹⁵¹Ba/¹⁵²Ba/¹⁴⁶La/¹⁴⁷La/¹⁴⁸La/¹⁴⁹La, E=950 MeV/nucleon; measured fission fragments, isotopic distributions of the fission fragments, production σ and yields using zero-degree magnetic spectrometer Fragment Separator at GSI accelerator facilities; deduced mean neutron-to-proton ratio of fission fragments, role of Coulomb and nuclear excitation mechanisms in the neutron excess of the final fragments.

doi: 10.1103/PhysRevC.99.054606
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0955.

2014AY03      Phys.Rev. C 89, 054610 (2014)

Y.Ayyad, J.Benlliure, E.Casarejos, H.Alvarez-Pol, A.Bacquias, A.Boudard, M.Caamano, T.Enqvist, V.Fohr, A.Kelic-Heil, K.Kezzar, S.Leray, D.Mancusi, C.Paradela, D.Perez-Loureiro, R.Pleskac, J.L.Rodriguez-Sanchez, D.Tarrio

Proton-induced fission of ¹⁸¹Ta at high excitation energies

NUCLEAR REACTIONS ¹H(¹⁸¹Ta, F), E=300, 500, 800, 1000 MeV/nucleon; measured energy losses of the tantalum beam particles, and fission products at GSI facility; deduced proton-induced total fission σ(E), Mass, charge, and excitation energy distributions of prefragments, average fission lifetime, temperature dependence of dissipative and transient effects at small deformation. Comparison with previous experimental data, and model calculations using INCL+ABLA, ISABEL+ABLA, and INCL+GEMINI++ statistical model codes. Benchmarking state-of-the-art reaction codes

doi: 10.1103/PhysRevC.89.054610
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1888.

2012BA09      Phys.Rev. C 85, 024904 (2012)

A.Bacquias, V.Fohr, D.Henzlova, A.Kelic-Heil, M.V.Ricciardi, K.-H.Schmidt

Dispersion of longitudinal momentum distributions induced in fragmentation reactions

doi: 10.1103/PhysRevC.85.024904
Citations: PlumX Metrics

2011AY03      J.Korean Phys.Soc. 59, 1852s (2011)

Y.Ayyad, J.Benlliure, E.Casarejos, H.Alvarez-Pol, C.Paradela, D.Perez-Loureiro, D.Tarrio, A.Bacquias, T.Enqvist, V.Fohr, A.Kelic, R.Pleskac, A.Boudard, K.Kezzar, S.Leray

Total Fission Cross Sections in Reactions p+¹⁸¹Ta Investigated in Inverse Kinematics at Relativistic Energies

NUCLEAR REACTIONS ¹H(¹⁸¹Ta, X), E=300, 500, 800, 1000 MeV/nucleon; measured fragments; deduced fission σ; calculated fission σ using INCL4 coupled to ABLA code. Compared with other data and systematics.

doi: 10.3938/jkps.59.1852
Citations: PlumX Metrics

2011FO17      Phys.Rev. C 84, 054605 (2011)

V.Fohr, A.Bacquias, E.Casarejos, T.Enqvist, A.R.Junghans, A.Kelic-Heil, T.Kurtukian, S.Lukic, D.Perez-Loureiro, R.Pleskac, M.V.Ricciardi, K.-H.Schmidt, J.Taieb

Experimental study of fragmentation products in the reactions ¹¹²Sn+¹¹²Sn and ¹²⁴Sn+¹²⁴Sn at 1A GeV

doi: 10.1103/PhysRevC.84.054605
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0908.

2011PE20      Phys.Lett. B 703, 552 (2011)

D.Perez-Loureiro, J.Benlliure, H.Alvarez-Pol, B.Blank, E.Casarejos, D.Dragosavac, V.Fohr, M.Gascon, W.Gawlikowicz, A.Heinz, K.Helariutta, A.Kelic-Heil, S.Lukic, F.Montes, L.Pienkowski, K.-H.Schmidt, M.Staniou, K.Subotic, K.Summerer, J.Taieb, A.Trzcinska

Production of neutron-rich nuclei in fragmentation reactions of ¹³²Sn projectiles at relativistic energies

NUCLEAR REACTIONS Pb(²³⁸U, X)¹³²Sn, E=950 MeV/nucleon; Be(¹³²Sn, X), E not given; measured reaction products; deduced σ. Comparison with code COFRA results.

doi: 10.1016/j.physletb.2011.08.037
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1956.

2010BE24      Nucl.Phys. A834, 467c (2010)

J.Benlliure, D.Dragosavac, D.Perez-Loureiro, H.Alvarez-Pol, B.Blank, E.Casarejos, V.Fohr, M.Gascon, W.Gawlikowicz, A.Heinz, K.Helariutta, S.Lukic, F.Montes, L.Pienkowski, M.Staniou, K.Subotic, K.Summerer, J.Taieb, A.Trzcinska, M.Veselsky

Investigating the radial distributions of medium-mass nuclei

NUCLEAR REACTIONS ⁹Be(¹¹¹Sn, X), (¹¹²Sn, X), (¹¹³Sn, X), (¹¹⁴Sn, X), (¹¹⁵Sn, X), (¹¹⁷Sn, X), (¹¹⁸Sn, X), (¹¹⁹Sn, X), (¹²⁰Sn, X), (¹²¹Sn, X), (¹²³Sn, X), (¹²⁴Sn, X), (¹²⁵Sn, X), (¹²⁶Sn, X), (¹²⁷Sn, X), (¹²⁸Sn, X), (¹²⁹Sn, X), (¹³⁰Sn, X), (¹³¹Sn, X), (¹³²Sn, X), (¹³³Sn, X), (¹³⁴Sn, X), (¹³⁵Sn, X), E not given; measured total σ; analyzed σ, radii dependence, halo nuclei, neutron skin. Calculations using Glauber model optical limit and "black disk". Transmission method with FRS at GSI.

doi: 10.1016/j.nuclphysa.2010.01.066
Citations: PlumX Metrics

2009PE12      Acta Phys.Pol. B40, 863 (2009)

D.Perez-Loureiro, H.Alvarez-Pol, J.Benlliure, B.Blank, E.Casarejos, D.Dragosavac, V.Fohr, M.Gascon, W.Gawlikowicz, A.Heinz, K.Helariutta, A.Kelic, S.Lukic, F.Montes, L.Pienkowski, K.-H.Schmidt, M.Staniou, K.Subotic, K.Summerer, J.Taieb, A.Trzcinska

Production of Medium-Mass Neutron Rich Nuclei from Fragmentation of Fission Residues Around Sn