NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = P.Egelhof Found 72 matches. 2023ZH34 Phys.Rev. C 108, 014614 (2023) J.T.Zhang, P.Ma, Y.Huang, X.L.Tu, P.Sarriguren, Z.P.Li, Y.Kuang, W.Horiuchi, T.Inakura, L.Xayavong, Y.Sun, K.Kaneko, X.Q.Liu, K.Yue, C.J.Shao, Q.Zeng, B.Mei, P.Egelhof, Yu.A.Litvinov, M.Wang, Y.H.Zhang, X.H.Zhou, Z.Y.Sun Matter radius of 78Kr from proton elastic scattering at 153 MeV NUCLEAR REACTIONS 1H(78Kr, p), E=152 MeV/nucleon; measured Ep, Ip; deduced σ(θ). 78Kr; deduced point-matter radius, neutron skin thickness. Glauber model analysis. Comparison of the obtained σ to FRESCO calculations with the phenomenological OMP parameters (KD03). Collision in Cooler Storage Ring of the Heavy Ion Research Facility in Lanzhou (HIRFL-CSR) with molecular hydrogen-gas target. MICRON double-sided Si-strip detector (DSSD) used to measure the recoil protons.
doi: 10.1103/PhysRevC.108.014614
2021DO02 Nucl.Phys. A1008, 122154 (2021) A.V.Dobrovolsky, G.A.Korolev, S.Tang, G.D.Alkhazov, G.Colo, I.Dillmann, P.Egelhof, A.Estrade, F.Farinon, H.Geissel, S.Ilieva, A.G.Inglessi, Y.Ke, A.V.Khanzadeev, O.A.Kiselev, J.Kurcewicz, L.X.Chung, Yu.A.Litvinov, G.E.Petrov, A.Prochazka, C.Scheidenberger, L.O.Sergeev, H.Simon, M.Takechi, V.Volkov, A.A.Vorobyov, H.Weick, V.I.Yatsoura Nuclear matter distributions in the neutron-rich carbon isotopes 14-17C from intermediate-energy proton elastic scattering in inverse kinematics NUCLEAR REACTIONS 1H(12C, 12C), (14C, 14C), (15C, 15C), (16C, 16C), (17C, 17C), E ∼ 700 MeV/nucleon; measured reaction products. 12,14,15,16,17C; deduced total and core matter distributions, rms radii. Comparison with available data, fragment separator FRS at GSI.
doi: 10.1016/j.nuclphysa.2021.122154
2021DU19 Phys.Rev. C 104, 034621 (2021) S.Dubey, A.Echler, P.Egelhof, P.Grabitz, W.Lauterfeld, M.Mutterer, S.Stolte, A.Blanc, U.Koster, O.Serot, G.Kessedjian, S.Kraft-Bermuth, P.Scholz, S.Bishop, J.M.Gomez-Guzman, F.Gonnenwein Isotopic distributions of thermal-neutron-induced fission fragments of near-symmetric fission of 239, 241Pu determined using calorimetric low-temperature detectors NUCLEAR REACTIONS 239,241Pu(n, F)89Se/89Br/90Br/91Br/89Kr/90Kr/91Kr/92Kr/93Kr/94Kr/95Kr/89Rb/90Rb/91Rb/92Rb/93Rb/94Rb/95Rb/96Rb/97Rb/90Sr/91Sr/92Sr/93Sr/94Sr/95Sr/96Sr/97Sr/98Sr/99Sr/100Sr/93Y/94Y/95Y/96Y/97Y/98Y/99Y/100Y/101Y/102Y/96Zr/97Zr/98Zr/99Zr/100Zr/101Zr/102Zr/103Zr/104Zr/105Zr/98Nb/99Nb/100Nb/101Nb/102Nb/103Nb/104Nb/105Nb/106Nb/101Mo/102Mo/103Mo/104Mo/105Mo/106Mo/107Mo/108Mo/109Mo/104Tc/105Tc/106Tc/107Tc/108Tc/109Tc/110Tc/111Tc/112Tc/106Ru/107Ru/108Ru/109Ru/110Ru/111Ru/112Ru/109Rh/110Rh/111Rh/112Rh/112Pd/113Rh/113Pd, E=thermal; measured particle energies, and isotopic distributions for the light fission fragments in A=89-112, Z=36-45 asymmetric to symmetric fission region using calorimetric low-temperature detectors (CLTDs) and the LOHENGRIN spectrometer of the ILL, Grenoble high flux reactor; deduced fractional independent yields, independent yields, charge polarization as a function of the secondary mass, local proton odd-even effect versus nuclear charge number Z, virtual shell effect near Z=44, in analogy to the effect of the Z=50 shell in the complementary heavy fragment group of 239,241Pu. Comparison with previous experimental data.
doi: 10.1103/PhysRevC.104.034621
2021LI49 Phys.Rev. C 104, 034315 (2021) X.Liu, P.Egelhof, O.Kiselev, M.Mutterer Nuclear matter density distributions of the neutron-rich 6, 8He isotopes from a sum-of-Gaussian analysis of elastic proton scattering data at intermediate energies NUCLEAR REACTIONS 1H(6He, p), (8He, p), E≈700 MeV/nucleon; analyzed experimental differential cross sections from GSI using sum-of-Gaussians (SOG) method based on Glauber multiple-scattering theory; deduced scattering amplitude parameters. 6,8He; deduced rms point nuclear matter radii, radial density distributions, neutron halo in 8He; discussed core rearrangement by adding the valence neutrons to an α-like core to form 6He and 8He.
doi: 10.1103/PhysRevC.104.034315
2020DU13 Phys.Rev. C 102, 044602 (2020) S.Dubey, A.Echler, P.Egelhof, P.Grabitz, W.Lauterfeld, M.Mutterer, S.Stolte, A.Blanc, U.Koster, O.Serot, G.Kessedjian, S.Kraft-Bermuth, P.Scholz, F.Gonnenwein Precise 92Rb and 96Y yields for thermal-neutron-induced fission of 235U and 239, 241Pu determined using calorimetric low-temperature detectors NUCLEAR REACTIONS 235U, 239,241Pu(n, F), E=thermal neutrons from high-flux reactor at ILL-Grenoble; measured fission fragments using the LOHENGRIN mass spectrometer; deduced fractional independent yields per A=92 and A=96, independent yields per fission of A=92 and 96 isotopes of 92Rb, 92Sr, 92Kr, 96Rb, 96Sr, 96Y and 96Zr, and cumulative yields. Comparison with previous experimental results, and with data in evaluated libraries: JENDL-4.0, JEFF-3.3, and ENDF/B-VIII.0, and with GEF theoretical calculations. Relevance to reducing nuclear data uncertainties in the computation of reactor antineutrino spectra by the summation method. Discussed problem of 92Rb β- decay to 92Sr ground-state in the context of discrepancies between previous measurements for fission yields.
doi: 10.1103/PhysRevC.102.044602
2020LI38 Phys.Lett. B 809, 135776 (2020) X.Liu, P.Egelhof, O.Kiselev, M.Mutterer Variance in the radial distribution of nuclear matter between 56Ni and 58Ni inferred from a model-independent Sum-of-Gaussian analysis of elastic proton scattering data NUCLEAR REACTIONS 1H(56Ni, p), (58Ni, p), E=400 MeV/nucleon; measured reaction products, Ep, Ip; deduced σ(t), nuclear matter density distributions, rms point matter radii.
doi: 10.1016/j.physletb.2020.135776
2019DO05 Nucl.Phys. A989, 40 (2019) A.V.Dobrovolsky, G.A.Korolev, A.G.Inglessi, G.D.Alkhazov, G.Colo, I.Dillmann, P.Egelhof, A.Estrade, F.Farinon, H.Geissel, S.Ilieva, Y.Ke, A.V.Khanzadeev, O.A.Kiselev, J.Kurcewicz, X.C.Le, Yu.A.Litvinov, G.E.Petrov, A.Prochazka, C.Scheidenberger, L.O.Sergeev, H.Simon, M.Takechi, S.Tang, V.Volkov, A.A.Vorobyov, H.Weick, V.I.Yatsoura Nuclear-matter distribution in the proton-rich nuclei 7Be and 8B from intermediate energy proton elastic scattering in inverse kinematics NUCLEAR REACTIONS 1H(7Be, 7Be), E=701 MeV/nucleon;1H(8B, x), E=702 MeV/nucleon; measured reaction products. 7Be, 8B; deduced σ, dσ/dt, σpp, σpn, parameters using fit to the data, nuclear matter density distribution, nuclear matter radii for both 7Be and 8B. Compared with other calculations and published measurements.
doi: 10.1016/j.nuclphysa.2019.05.012
2019YU04 Phys.Rev. C 100, 054609 (2019); Erratum Phys.Rev. C 102, 049901 (2020) K.Yue, J.T.Zhang, X.L.Tu, C.J.Shao, H.X.Li, P.Ma, B.Mei, X.C.Chen, Y.Y.Yang, X.Q.Liu, Y.M.Xing, K.H.Fang, X.H.Li, Z.Y.Sun, M.Wang, P.Egelhof, Yu.A.Litvinov, K.Blaum, Y.H.Zhang, X.H.Zhou Measurement of 58Ni(p, p)58Ni elastic scattering at low momentum transfer by using the HIRFL-CSR heavy-ion storage ring NUCLEAR REACTIONS 1H(58Ni, p), E=95 MeV/nucleon; measured Ep, Ip, E(x-ray), I(x-ray), absolute differential σ(θ) using a single-sided silicon detector (SSSD) detector at the Cooler Storage Ring (CSRe) at the Heavy Ion Research Facility in Lanzhou (HIRFL-CSR); deduced nuclear matter rms value. Comparison with KDO3 and LC08 optical model calculations, and with previous experimental results.
doi: 10.1103/PhysRevC.100.054609
2018KO13 Phys.Lett. B 780, 200 (2018) G.A.Korolev, A.V.Dobrovolsky, A.G.Inglessi, G.D.Alkhazov, P.Egelhof, A.Estrade, I.Dillmann, F.Farinon, H.Geissel, S.Ilieva, Y.Ke, A.V.Khanzadeev, O.A.Kiselev, J.Kurcewicz, X.C.Le, Yu.A.Litvinov, G.E.Petrov, A.Prochazka, C.Scheidenberger, L.O.Sergeev, H.Simon, M.Takechi, S.Tang, V.Volkov, A.A.Vorobyov, H.Weick, V.I.Yatsoura Halo structure of 8B determined from intermediate energy proton elastic scattering in inverse kinematics NUCLEAR REACTIONS 1H(8B, p), E=0.7 GeV/nucleon; measured reaction products, Ep, Ip. 8B; deduced σ(θ), root-mean-square (rms) matter and halo radii. Comparison with available data.
doi: 10.1016/j.physletb.2018.03.013
2017CH45 Phys.Lett. B 774, 559 (2017) L.X.Chung, C.A.Bertulani, P.Egelhof, S.Ilieva, D.T.Khoa, O.A.Kiselev The dominance of the ν(0d5/2)2 configuration in the N = 8 shell in 12Be from the breakup reaction on a proton target at intermediate energy NUCLEAR REACTIONS 1H(12Be, X)11Be, E=700.5 MeV/nucleon; measured reaction products; deduced σ(p). Distorted wave impulse approximation (DWIA) analysis.
doi: 10.1016/j.physletb.2017.09.068
2017ZA09 Phys.Rev. C 96, 034617 (2017) J.C.Zamora, T.Aumann, S.Bagchi, S.Bonig, M.Csatlos, I.Dillmann, C.Dimopoulou, P.Egelhof, V.Eremin, T.Furuno, H.Geissel, R.Gernhauser, M.N.Harakeh, A.-L.Hartig, S.Ilieva, N.Kalantar-Nayestanaki, O.Kiselev, H.Kollmus, C.Kozhuharov, A.Krasznahorkay, Th.Kroll, M.Kuilman, S.Litvinov, Yu.A.Litvinov, M.Mahjour-Shafiei, M.Mutterer, D.Nagae, M.A.Najafi, C.Nociforo, F.Nolden, U.Popp, C.Rigollet, S.Roy, C.Scheidenberger, M.von Schmid, M.Steck, B.Streicher, L.Stuhl, M.Thurauf, T.Uesaka, H.Weick, J.S.Winfield, D.Winters, P.J.Woods, T.Yamaguchi, K.Yue, J.Zenihiro Nuclear-matter radius studies from 58Ni (α, α) experiments at the GSI Experimental Storage Ring with the EXL facility NUCLEAR REACTIONS 4He(58Ni, α), (58Ni, α'), E=100, 150 MeV/nucleon; measured scattered α-particles, differential σ(θ, E) using stored ion beams and a UHV compatible detection system with a double-sided silicon strip detector (DSSD) at the heavy-ion experimental storage ring (ESR) at GSI facility; deduced optical model potential parameters, probability density distribution, point-density distributions of 58Ni, nuclear-matter radius, and compared with Skyrme-Hartree-Fock calculation (SHF), half-density radius, diffuseness of a Fermi-shape, rms radius, total-matter distribution, point-matter distribution. Comparison with experimental data.
doi: 10.1103/PhysRevC.96.034617
2016ZA08 Phys.Lett. B 763, 16 (2016) J.C.Zamora, T.Aumann, S.Bagchi, S.Bonig, M.Csatlos, I.Dillmann, C.Dimopoulou, P.Egelhof, V.Eremin, T.Furuno, H.Geissel, R.Gernhauser, M.N.Harakeh, A.-L.Hartig, S.Ilieva, N.Kalantar-Nayestanaki, O.Kiselev, H.Kollmus, C.Kozhuharov, A.Krasznahorkay, Th.Kroll, M.Kuilman, S.Litvinov, Yu.A.Litvinov, M.Mahjour-Shafiei, M.Mutterer, D.Nagae, M.A.Najafi, C.Nociforo, F.Nolden, U.Popp, C.Rigollet, S.Roy, C.Scheidenberger, M.von Schmid, M.Steck, B.Streicher, L.Stuhl, M.Thurauf, T.Uesaka, H.Weick, J.S.Winfield, D.Winters, P.J.Woods, T.Yamaguchi, K.Yue, J.Zenihiro First measurement of isoscalar giant resonances in a stored-beam experiment NUCLEAR REACTIONS 4He(58Ni, α'), E=100 MeV/nucleon; measured reaction products, Eα, Iα. 58Ni; deduced σ(θ, E), monopole contribution of the energy-weighted sum rule (EWSR).
doi: 10.1016/j.physletb.2016.10.015
2015CH51 Phys.Rev. C 92, 034608 (2015) L.X.Chung, O.A.Kiselev, D.T.Khoa, P.Egelhof Elastic proton scattering at intermediate energies as a probe of the 6, 8He nuclear matter densities NUCLEAR REACTIONS 1H(6He, p), E=717 MeV/nucleon; 1H(8He, p), E=674 MeV/nucleon; 4He(p, p), E=702 MeV; analyzed σ(θ) data from GSI experiments using Glauber multiple scattering model (GMSM) and several phenomenological parametrizations of the nuclear matter density. 6,8He; deduced nuclear matter radii and densities, structure of 6He in terms of the core and dineutron halo radii.
doi: 10.1103/PhysRevC.92.034608
2015DO10 Phys.Scr. T166, 014007 (2015) D.T.Doherty, P.J.Woods, Y.A.Litvinov, M.A.Najafi, S.Bagchi, S.Bishop, M.Bo, C.Brandau, T.Davinson, I.Dillmann, A.Estrade, P.Egelhof, A.Evdokimov, A.Gumberidze, M.Heil, C.Lederer, S.A.Litvinov, G.Lotay, N.Kalantar-Nayestanaki, O.Kiselev, C.Kozhuharov, T.Kroll, M.Mahjour-Shafiei, M.Mutterer, F.Nolden, N.Petridis, U.Popp, R.Reifarth, C.Rigollet, S.Roy, M.Steck, T.Stohlker, B.Streicher, S.Trotsenko, M.v.Schmid, X.L.Yan, J.C.Zamora Nuclear transfer reaction measurements at the ESR-for the investigation of the astrophysical 15O(α, γ)19Ne reaction NUCLEAR REACTIONS 1H(20Ne, d), E=50 MeV/nucleon; measured reaction products; deduced energy levels, J, π. Comparison with available data.
doi: 10.1088/0031-8949/2015/T166/014007
2012IL01 Nucl.Phys. A875, 8 (2012) S.Ilieva, F.Aksouh, G.D.Alkhazov, L.Chulkov, A.V.Dobrovolsky, P.Egelhof, H.Geissel, M.Gorska, A.Inglessi, R.Kanungo, A.V.Khanzadeev, O.A.Kiselev, G.A.Korolev, X.C.Le, Yu.A.Litvinov, C.Nociforo, D.M.Seliverstov, L.O.Sergeev, H.Simon, V.A.Volkov, A.A.Vorobyov, H.Weick, V.I.Yatsoura, A.A.Zhdanov Nuclear-matter density distribution in the neutron-rich nuclei 12, 14Be from proton elastic scattering in inverse kinematics NUCLEAR REACTIONS 1H(12Be, 12Be), (14Be, 14Be), E=700 MeV/nucleon; measured recoil Ep, Ip(θ) using time-projection chamber; deduced σ, σ(E), scattering amplitudes, nuclear matter radii, halo nuclei, matter density parameters; calculated σ, σ(E) using Glauber theory. Inverse kinematics scattering with secondary radioactive beam, FRS fragment separator.
doi: 10.1016/j.nuclphysa.2011.11.010
2011KI49 Nucl.Instrum.Methods Phys.Res. A 641, 72 (2011) O.A.Kiselev, F.Aksouh, A.Bleile, O.V.Bochkarev, L.V.Chulkov, D.Cortina-Gil, A.V.Dobrovolsky, P.Egelhof, H.Geissel, M.Hellstroem, N.B.Isaev, B.G.Komkov, M.Matos, F.V.Moroz, G.Muenzenberg, M.Mutterer, V.A.Mylnikov, S.R.Neumaier, V.N.Pribora, D.M.Seliverstov, L.O.Sergueev, A.Shrivastava, K.Suemmerer, H.Weick, M.Winkler, V.I.Yatsoura A new experimental approach to investigate intermediate energy proton elastic scattering and breakup reactions on exotic nuclei in inverse kinematics NUCLEAR REACTIONS 1H(6He, 6He), 1H(8He, 8He), 6,8He(p, p), E=4.3-5.3 GeV; measured products, 6He, Eπ, Iπ; deduced σ(θ). Data were imported from EXFOR entry O1908.
doi: 10.1016/j.nima.2011.03.046
2006DO02 Nucl.Phys. A766, 1 (2006) A.V.Dobrovolsky, G.D.Alkhazov, M.N.Andronenko, A.Bauchet, P.Egelhof, S.Fritz, H.Geissel, C.Gross, A.V.Khanzadeev, G.A.Korolev, G.Kraus, A.A.Lobodenko, G.Munzenberg, M.Mutterer, S.R.Neumaier, T.Schafer, C.Scheidenberger, D.M.Seliverstov, N.A.Timofeev, A.A.Vorobyov, V.I.Yatsoura Study of the nuclear matter distribution in neutron-rich Li isotopes NUCLEAR REACTIONS 1H(6Li, 6Li), (8Li, 8Li), (9Li, 9Li), (11Li, 11Li), E=700 MeV/nucleon; measured, analyzed small-angle elastic scattering σ(θ). 6,8,9,11Li deduced radii, matter distributions.
doi: 10.1016/j.nuclphysa.2005.11.016
2005CH50 Nucl.Phys. A759, 43 (2005) L.V.Chulkov, F.Aksouh, A.Bleile, O.V.Bochkarev, D.Cortina-Gil, A.V.Dobrovolsky, P.Egelhof, H.Geissel, M.Hellstrom, N.B.Isaev, O.A.Kiselev, B.G.Komkov, M.Matos, F.N.Moroz, G.Munzenberg, M.Mutterer, V.A.Mylnikov, S.R.Neumaier, V.N.Pribora, D.M.Seliverstov, L.O.Sergeev, A.Shrivastava, K.Summerer, S.Yu.Torilov, H.Weick, M.Winkler, V.I.Yatsoura Quasi-free scattering with 6, 8He beams NUCLEAR REACTIONS 1H(6He, p), (6He, np), (6He, pα), E=717 MeV/nucleon; 1H(8He, p), (8He, np), (8He, pα), E=671 MeV/nucleon; measured recoil proton spectra, σ(E, θ). 6,8He deduced cluster configurations, spectroscopic factors.
doi: 10.1016/j.nuclphysa.2005.05.148
2005KI21 Eur.Phys.J. A 25, Supplement 1, 215 (2005) O.A.Kiselev, F.Aksouh, A.Bleile, O.V.Bochkarev, L.V.Chulkov, D.Cortina-Gil, A.V.Dobrovolsky, P.Egelhof, H.Geissel, M.Hellstrom, N.B.Isaev, B.G.Komkov, M.Matos, F.V.Moroz, G.Munzenberg, M.Mutterer, V.A.Mylnikov, S.R.Neumaier, V.N.Pribora, D.M.Seliverstov, L.O.Sergueev, A.Shrivastava, K.Summerer, H.Weick, M.Winkler, V.I.Yatsoura Investigation of nuclear matter distribution of the neutron-rich He isotopes by proton elastic scattering at intermediate energies NUCLEAR REACTIONS 1H(6He, p), (8He, p), E ≈ 700 MeV/nucleon; measured recoil proton spectra, σ(E, θ). 6,8He deduced nuclear matter density distributions, charge radii, cluster configurations, spectroscopic factors.
doi: 10.1140/epjad/i2005-06-156-3
2003EG01 Phys.Scr. T104, 151 (2003) P.Egelhof, O.Kisselev, G.Munzenberg, S.R.Neumaier, H.Weick Nuclear Structure Studies by Direct Reaction Experiments with Stored Radioactive Beams
doi: 10.1238/Physica.Topical.104a00151
2003EG03 Nucl.Phys. A722, 254c (2003) Probing the halo structure of exotic nuclei by direct reactions with radioactive beams NUCLEAR REACTIONS 1H(8Li, 8Li), (9Li, 9Li), (11Li, 11Li), E ≈ 700 MeV; measured σ(E, θ). 8,9,11Li deduced matter density distributions.
doi: 10.1016/S0375-9474(03)01374-5
2002AL26 Nucl.Phys. A712, 269 (2002) G.D.Alkhazov, A.V.Dobrovolsky, P.Egelhof, H.Geissel, H.Irnich, A.V.Khanzadeev, G.A.Korolev, A.A.Lobodenko, G.Munzenberg, M.Mutterer, S.R.Neumaier, W.Schwab, D.M.Seliverstov, T.Suzuki, A.A.Vorobyov Nuclear matter distributions in the 6He and 8He nuclei from differential cross sections for small-angle proton elastic scattering at intermediate energy NUCLEAR REACTIONS 1H(α, α), (6He, 6He), (8He, 8He), E ≈ 0.7 GeV/nucleon; analyzed small-angle elastic scattering σ(θ). 6,8He deduced density distributions, radii. Comparison with model predictions, previous results.
doi: 10.1016/S0375-9474(02)01273-3
2002EG02 Eur.Phys.J. A 15, 27 (2002) P.Egelhof, G.D.Alkhazov, M.N.Andronenko, A.Bauchet, A.V.Dobrovolsky, S.Fritz, G.E.Gavrilov, H.Geissel, C.Gross, A.V.Khanzadeev, G.A.Korolev, G.Kraus, A.A.Lobodenko, G.Munzenberg, M.Mutterer, S.R.Neumaier, T.Schafer, C.Scheidenberger, D.M.Seliverstov, N.A.Timofeev, A.A.Vorobyov, V.I.Yatsoura Nuclear-matter distributions of halo nuclei from elastic proton scattering in inverse kinematics NUCLEAR REACTIONS 1H(6Li, 6Li), (8Li, 8Li), (9Li, 9Li), (11Li, 11Li), (6He, 6He), (8He, 8He), E ≈ 700 MeV/nucleon; measured σ(θ). 6,8He, 6,8,9,11Li deduced radii. Comparison with previous results, model predictions.
doi: 10.1140/epja/i2001-10219-7
2002NE19 Nucl.Phys. A712, 247 (2002) S.R.Neumaier, G.D.Alkhazov, M.N.Andronenko, A.V.Dobrovolsky, P.Egelhof, G.E.Gavrilov, H.Geissel, H.Irnich, A.V.Khanzadeev, G.A.Korolev, A.A.Lobodenko, G.Munzenberg, M.Mutterer, W.Schwab, D.M.Seliverstov, T.Suzuki, N.A.Timofeev, A.A.Vorobyov, V.I.Yatsoura Small-angle proton elastic scattering from the neutron-rich isotopes 6He and 8He, and from 4He, at 0.7 GeV in inverse kinematics NUCLEAR REACTIONS 1H(α, α), (6He, 6He), (8He, 8He), E ≈ 0.7 GeV/nucleon; measured small-angle elastic scattering σ(θ); deduced integral elastic σ, total and reaction σ. Halo nuclei.
doi: 10.1016/S0375-9474(02)01274-5
2001EG02 Prog.Part.Nucl.Phys. 46, 307 (2001) P.Egelhof, for the IKAR Collaboration Nuclear Matter Distributions of Neutron-Rich Halo Nuclei from Intermediate Energy Elastic Proton Scattering in Inverse Kinematics NUCLEAR REACTIONS 1H(α, α'), (6He, 6He'), (8He, 8He'), (6Li, 6Li'), (9Li, 9Li'), (11Li, 11Li'), E ≈ 700 MeV/nucleon; measured σ(E, θ). 4,6,8He, 6,9,11Li deduced matter radii, halo features.
doi: 10.1016/S0146-6410(01)00136-3
2001TO18 Nucl.Phys. A690, 298c (2001) M.Tomaselli, S.Fritzsche, A.Dax, P.Egelhof, C.Kozhuharov, T.Kuhl, D.Marx, M.Mutterer, S.R.Neumaier, W.Nortershauser, H.Wang, H.-J.Kluge Microscopic Model for Charge and Matter Distributions of Nuclei NUCLEAR STRUCTURE 5,6,7,9,11Li; calculated charge and matter density distributions, radii. Interacting microscopic clusters. Comparison with data.
doi: 10.1016/S0375-9474(01)00963-0
2000TO11 Phys.Rev. C62, 067305 (2000) M.Tomaselli, M.Hjorth-Jensen, S.Fritzsche, P.Egelhof, S.R.Neumaier, M.Mutterer, T.Kuhl, A.Dax, H.Wang Matter and Charge Distributions of 6He and 5, 6, 7, 9Li within the Dynamic-Correlation Model NUCLEAR STRUCTURE 6He, 5,6,7,9Li; calculated matter and charge distributions, radii, halo features. Dynamic-correlation model.
doi: 10.1103/PhysRevC.62.067305
2000TO13 Hyperfine Interactions 127, 95 (2000) M.Tomaselli, P.Egelhof, S.R.Neumaier, M.Mutterer, T.Kuhl, A.Dax, F.Schmitt, S.Fritzsche Microscopic calculations of matter and charge distributions of exotic nuclei within the Dynamic-Correlation Model NUCLEAR STRUCTURE 6He, 5,6,7,8Li; calculated matter and charge distributions, radii. Dynamic-correlation model. NUCLEAR REACTIONS 6He(p, p), E not given; calculated σ(θ). Comparison with data.
doi: 10.1023/A:1012658609988
1999EG02 Pramana 53, 365 (1999) Nuclear Structure Studies on Halo Nuclei by Direct Reactions with Radioactive Beams NUCLEAR REACTIONS 1H(α, α), (6He, 6He), (8He, 8He), E ≈ 700 MeV/nucleon; measured σ(θ). 4,6,8He deduced matter densities, radii.
doi: 10.1007/s12043-999-0002-2
1998BO02 Eur.Phys.J. A 1, 15 (1998) O.V.Bochkarev, L.V.Chulkov, P.Egelhof, H.Geissel, M.S.Golovkov, H.Irnich, Z.Janas, H.Keller, T.Kobayashi, G.Kraus, G.Munzenberg, F.Nickel, A.A.Ogloblin, A.Ozawa, A.Piechaczek, E.Roeckl, W.Schwab, K.Summerer, T.Suzuki, I.Tanihata, K.Yoshida Evidence for a Neutron Skin in 20N NUCLEAR REACTIONS C(20Mg, X), (20Na, X), (20Ne, X), (20F, X), (20O, X), (20N, X), E=950 MeV/nucleon; measured interaction, charge-changing σ; deduced projectile matter, charge radii. 20N deduced evidence for neutron skin.
1997AL09 Phys.Rev.Lett. 78, 2313 (1997) G.D.Alkhazov, M.N.Andronenko, A.V.Dobrovolsky, P.Egelhof, G.E.Gavrilov, H.Geissel, H.Irnich, A.V.Khanzadeev, G.A.Korolev, A.A.Lobodenko, G.Munzenberg, M.Mutterer, S.R.Neumaier, F.Nickel, W.Schwab, D.M.Seliverstov, T.Suzuki, J.P.Theobald, N.A.Timofeev, A.A.Vorobyov, V.I.Yatsoura Nuclear Matter Distributions in 6He and 8He from Small Angle p-He Scattering in Inverse Kinematics at Intermediate Energy NUCLEAR REACTIONS 1H(α, α), (6He, 6He), (8He, 8He), E=674-699 MeV/nucleon; measured absolute differential σ; deduced model parameters. 6,8He deduced nuclear matter radii.
doi: 10.1103/PhysRevLett.78.2313
1997ME20 Nucl.Phys. A626, 451c (1997) H.J.Meier, P.Egelhof, W.Henning, A.von Kienlin, G.Kraus, A.Weinbach Low Temperature Bolometers for Experiments with Cooled Heavy Ion Beams from Storage Rings NUCLEAR REACTIONS Pb(20Ne, 20Ne'), E=100 MeV/nucleon; measured σ(E(20Ne)); deduced giant resonance excitation probability. Pb deduced giant resonance E, Γ. Low temperature calorimeter.
doi: 10.1016/S0375-9474(97)00569-1
1996CH24 Nucl.Phys. A603, 219 (1996) L.Chulkov, G.Kraus, O.Bochkarev, P.Egelhof, H.Geissel, M.Golovkov, H.Irnich, Z.Janas, H.Keller, T.Kobayashi, G.Munzenberg, F.Nickel, A.Ogloblin, A.Ozawa, S.Patra, A.Piechaczek, E.Roeckl, W.Schwab, K.Summerer, T.Suzuki, I.Tanihata, K.Yoshida Interaction Cross Sections and Matter Radii of A = 20 Isobars NUCLEAR REACTIONS 12C(20Ne, X), (20O, X), (20F, X), (20Na, X), (20Mg, X), E ≤ 1 GeV/nucleon; measured interaction σ; deduced matter rms radii. 20O, 20Ne, 20F, 20Na, 20Mg deduced nucleon distribution rms radii differences. Secondary beams from 9Be(36Ar, X), (40Ar, X) reactions.
doi: 10.1016/0375-9474(96)00160-1
1996ME20 Nucl.Instrum.Methods Phys.Res. A370, 259 (1996) J.Meier, L.Chulkov, P.Egelhof, C.Fischer, W.Henning, A.von Kienlin, G.Kirchner, G.Kraus, A.Weinbach Application of Low Temperature Calorimeters for the Detection of Energetic Heavy Ions NUCLEAR REACTIONS 208Pb(20Ne, 20Ne'), E=100 MeV/nucleon; measured energy spectra. Calorimetric low temperature detectors.
doi: 10.1016/0168-9002(95)01104-8
1995KR17 Phys.Scr. T56, 114 (1995) G.Kraus, P.Egelhof, C.Fischer, H.Geissel, A.Himmler, F.Nickel, G.Munzenberg, W.Schwab, A.Weiss, J.Friese, A.Gillitzer, H.J.Korner, M.Peter, W.Henning, J.P.Schiffer, B.A.Brown, J.V.Kratz, L.Chulkov, M.Golovkov, A.Ogloblin The 56Ni B(E2, 01+ → 21+) Value - a Good Test for the Shell-Model Off Stability ( Question ) NUCLEAR REACTIONS 1H(56Ni, p), E=101 MeV/nucleon; measured energy, spectra; deduced elastic σ(θ). 56Ni level deduced β, B(E2). Inverse kinematics, coupled-channels, shell model analyses. NUCLEAR STRUCTURE 40,42,44,46,48Ca, 50Ti, 52Cr, 54Fe, 56,58,60,62,64Ni; calculated 2+ → 0+ transition B(λ). Shell model.
doi: 10.1088/0031-8949/1995/T56/019
1995NE04 Nucl.Phys. A583, 799c (1995) S.Neumaier, G.D.Alkhazov, M.N.Andronenko, T.Beha, K.-H.Behr, A.Brunle, K.Burkard, A.V.Dobrovolsky, P.Egelhof, C.Fischer, G.E.Gavrilov, H.Geissel, V.I.Iatsoura, H.Irnich, A.V.Khanzadeev, G.A.Korolev, A.A.Lobodenko, P.Lorenzen, G.Munzenberg, M.Mutterer, F.Nickel, W.Schwab, D.M.Seliverstov, P.Singer, T.Suzuki, J.P.Theobald, N.A.Timofeev, A.A.Vorobyov Study of the Nucleon Density Distribution of 6He and 8He by Proton Elastic Scattering in Inverse Kinematics NUCLEAR REACTIONS 1H(α, α), E=699 MeV/nucleon; 1H(6He, 6He), E=717 MeV/nucleon; 1H(8He, 8He), E=674 MeV/nucleon; measured differential σ vs four momentum transfer. 8He deduced neutron skin evidence.
doi: 10.1016/0375-9474(94)00761-B
1994KR16 Phys.Rev.Lett. 73, 1773 (1994) G.Kraus, P.Egelhof, C.Fischer, H.Geissel, A.Himmler, F.Nickel, G.Munzenberg, W.Schwab, A.Weiss, J.Friese, A.Gillitzer, H.J.Korner, M.Peter, W.F.Henning, J.P.Schiffer, J.V.Kratz, L.Chulkov, M.Golovkov, A.Ogloblin, B.A.Brown Proton Inelastic Scattering on 56Ni in Inverse Kinematics NUCLEAR REACTIONS 1H(56Ni, 56Ni'), E=101 MeV/nucleon; measured recoil proton spectra. 56Ni level deduced B(λ). Inverse kinematics.
doi: 10.1103/PhysRevLett.73.1773
1992WO09 Z.Phys. A341, 137 (1992) H.J.Wollersheim, P.Egelhof, H.Emling, J.Gerl, W.Henning, R.Holzmann, R.Schmidt, R.S.Simon, N.Martin, G.Eckert, Th.W.Elze, K.Stelzer, R.Kulessa, G.Duchene, B.Haas, J.C.Merdinger, J.P.Vivien, J.de Boer, E.Hauber, K.Kaiser, P.von Brentano, R.Reinhardt, R.Wirowski, R.Julin, C.Fahlander, I.Thorslund, H.Kluge Evidence for a Two-Phonon Octupole Vibrational State in 208Pb NUCLEAR REACTIONS 206,208Pb(208Pb, X), E=1290 MeV; measured (particle)(particle)γ-coin, (particle)γ(θ), directional correlations; 206Pb(208Pb, 208Pb'), E=1290 MeV; measured σ(θ). 208Pb deduced level, possible J, π, octupole character, dynamical deformation parameter.
doi: 10.1007/BF01298473
1991KR12 Z.Phys. A340, 339 (1991) G.Kraus, P.Egelhof, H.Emling, E.Grosse, W.Henning, R.Holzmann, H.J.Korner, J.V.Kratz, R.Kulessa, Ch.Schiessl, J.P.Schiffer, W.Wagner, W.Walus, H.J.Wollersheim Investigation of the (d, p)-Reaction on 136,132Xe in Inverse Kinematics NUCLEAR REACTIONS 2H(132Xe, p), (136Xe, p), (132Xe, d), E=5.87 MeV/nucleon; measured σ(θ). 133,137Xe levels deduced l, J, π, spectroscopic factors.
doi: 10.1007/BF01294683
1991SP03 Z.Phys. A339, 265 (1991) K.-H.Speidel, J.Cub, U.Reuter, F.Passek, H.-J.Wollersheim, N.Martin, P.Egelhof, H.Emling, W.Henning, R.S.Simon, R.Schmidt, H.-J.Simonis, N.Gollwitzer Large Electron Polarization of H-Like 20Ne-Ions Traversing Gd Foils at Very High Velocities NUCLEAR REACTIONS 197Au(20Ne, 20Ne'), E=5.9 MeV/nucleon; measured (particle)γ-coin, (particle)γ(θ) following Coulomb excitation; deduced transient magnetic fields for 20Ne ions in Gd host.
doi: 10.1007/BF01284063
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
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
1989WA11 Nucl.Phys. A493, 224 (1989) K.Wallmeroth, G.Bollen, A.Dohn, P.Egelhof, U.Kronert, M.J.G.Borge, J.Campos, A.Rodriguez Yunta, K.Heyde, C.de Coster, J.L.Wood, H.-J.Kluge Nuclear Shape Transition in Light Gold Isotopes RADIOACTIVITY 185,186,187,188,189m,189,190,191,192,193,195Au; measured hfs, isotope shifts; deduced μ, rms charge radii, deformation parameters β2. Resonance ionization mass spectroscopy, on-line isotope separator. NUCLEAR MOMENTS 197Au; measured hfs; deduced μ, rms charge radius, deformation parameter. Resonance ionization mass spectroscopy, on-line isotope separator.
doi: 10.1016/0375-9474(89)90396-5
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.
1988BO08 Nucl.Phys. A477, 399 (1988) W.Boeglin, P.Egelhof, I.Sick, J.M.Cavedon, B.Frois, D.Goutte, V.Meot, P.Leconte, X.H.Phan, S.K.Platchkov, S.Williamson, M.Girod Electron Scattering from Transitional Nuclei NUCLEAR REACTIONS 188,190,192Os, 194,196Pt(e, e'), E=200, 500 MeV; measured σ(E(e')), σ(θ). 190,188,192Os, 194,196Pt levels deduced transition charge densities.
doi: 10.1016/0375-9474(88)90349-1
1987BO06 Phys.Lett. 186B, 285 (1987) W.Boeglin, P.Egelhof, I.Sick, J.M.Cavedon, B.Frois, D.Goutte, X.H.Phan, S.K.Platchkov, S.Williamson, M.Girod Electron Scattering from Transitional Nuclei NUCLEAR REACTIONS 188,190,192Os, 194,196Pt(e, e), (e, e'), E=200, 500 MeV; measured σ(θ), transition charge densities. HFB calculations.
doi: 10.1016/0370-2693(87)90296-6
1987BO59 Hyperfine Interactions 38, 793 (1987) G.Bollen, P.Dabkiewicz, P.Egelhof, T.Hilberath, H.Kalinowsky, F.Kern, H.Schnatz, L.Schweikhard, H.Stolzenberg, R.B.Moore, H.-J.Kluge, G.M.Temmer, G.Ulm, and the ISOLDE Collaboration First Absolute Mass Measurements of Short-Lived Isotopes RADIOACTIVITY 77Rb(β+), (EC); measured T1/2. On-line mass separator, Penning trap ion confinement. ATOMIC MASSES 39K, 85,87,77Rb, 133Cs; analyzed data; deduced mass measurement accuracies.
doi: 10.1007/BF02394875
1987WA06 Phys.Rev.Lett. 58, 1516 (1987) K.Wallmeroth, G.Bollen, A.Dohn, P.Egelhof, J.Gruner, F.Lindenlauf, U.Kronert, J.Campos, A.Rodriguez Yunta, M.J.G.Borge, A.Venugopalan, J.L.Wood, R.B.Moore, H.-J.Kluge Sudden Change in the Nuclear Charge Distribution of very Light Gold Isotopes RADIOACTIVITY 185,186,187,188,189,189m,190Au; measured isotope shifts, hfs. 185,186,187,188,189,189m,190Au deduced charge radii, μ, deformation parameters. Resonance ionization mass spectrometry.
doi: 10.1103/PhysRevLett.58.1516
1987WA23 Hyperfine Interactions 34, 21 (1987) K.Wallmeroth, G.Bollen, M.J.G.Borge, J.Campos, A.Dohn, P.Egelhof, J.Gruner, H.-J.Kluge, U.Kronert, F.Lindenlauf, R.B.Moore, A.Rodriguez, A.Venugopalan, J.L.Wood, and the ISOLDE Collaboration Nuclear Shape Transition in Neutron-Deficient Gold Isotopes RADIOACTIVITY 189,189m,188,187,186,185Au; measured hfs, isotope shift; deduced hyperfine constants, μ. 189,188,187,186,185Au deduced rms charge radii, shape transition characteristics.
doi: 10.1007/BF02072675
1986JO05 Helv.Phys.Acta 59, 185 (1986) J.Jourdan, M.Baumgartner, S.Burzynski, P.Egelhof, A.Klein, M.A.Pickar, G.R.Plattner, W.D.Ramsay, H.W.Roser, I.Sick, J.Torre P-D(pol) Radiative Capture and the 3He D-State NUCLEAR REACTIONS 1H(polarized d, γ), E=29.2, 45.3 MeV; measured tensor analyzing power vs θ; deduced reaction mechanism. 3He deduced E1 contribution, D-state component. Faddeev calculations.
1986JO06 Nucl.Phys. A453, 220 (1986) J.Jourdan, M.Baumgartner, S.Burzynski, P.Egelhof, R.Henneck, A.Klein, M.A.Pickar, G.R.Plattner, W.D.Ramsay, H.W.Roser, I.Sick, J.Torre p-d(pol) Radiative Capture and the 3He D-State NUCLEAR REACTIONS 1H(polarized d, γ), E=29.2, 45.3 MeV; measured tensor analyzing power A(θ=90°).
doi: 10.1016/0375-9474(86)90011-4
1985JO05 Phys.Lett. 162B, 269 (1985) J.Jourdan, M.Baumgartner, S.Burzynski, P.Egelhof, A.Klein, M.A.Pickar, G.R.Plattner, W.D.Ramsay, H.W.Roser, I.Sick, J.Torre 1H + 2H(pol) Radiative Capture and the 3He D-State NUCLEAR REACTIONS 1H(polarized d, γ), E=29.2, 45.3 MeV; measured tensor analyzing power for θ=96°; deduced 3He D-state role. Faddeev calculations.
doi: 10.1016/0370-2693(85)90920-7
1985WE08 Phys.Rev.Lett. 55, 480 (1985) A.Weller, P.Egelhof, R.Caplar, O.Karban, D.Kramer, K.-H.Mobius, Z.Moroz, K.Rusek, E.Steffens, G.Tungate, K.Blatt, I.Koenig, D.Fick Electromagnetic Excitation of Aligned 7Li Nuclei NUCLEAR REACTIONS 58Ni, 120Sn(polarized 7Li, 7Li), E=8-16 MeV; measured analyzing power vs θ. 7Li level deduced quadrupole moment, B(E2), nuclear polarizability tensor moments.
doi: 10.1103/PhysRevLett.55.480
1984KO25 Z.Phys. A318, 135 (1984) I.Koenig, D.Fick, S.Kossionides, P.Egelhof, K.-H.Mobius, E.Steffens Polarized Recoil Nuclei from Nuclear Reactions Induced by Polarized Lithium Ions NUCLEAR REACTIONS 9Be(polarized 7Li, 8Be), 7Li(polarized 7Li, 5Li), (polarized 6Li, 5Li), E ≈ 9-20 MeV; measured recoil nucleus β-asymetry; deduced 8Li vector polarization vs E. 11B, 19F(polarized 6Li, 5Li), E=18 MeV; measured recoil nucleus β-asymmetry; deduced 12B, 12F vector polarization.
doi: 10.1007/BF01413462
1984MO06 Nucl.Phys. A417, 498 (1984) Z.Moroz, K.Rusek, P.Egelhof, S.Kossionides, K.-H.Mobius, G.Tungate, E.Steffens, G.Grawert, I.Koenig, D.Fick The Interaction of Polarized 7Li with 12C at 21.1 MeV NUCLEAR REACTIONS 12C(polarized 7Li, 7Li), E=21.1 MeV; measured σ(θ), iT11(θ), T20(θ), T21(θ), T22(θ); deduced optical model parameters. 12C(polarized 7Li, 6Li), E=21.1 MeV; measured σ(θ), T20(θ), T21(θ), T22(θ). Optical model analysis.
doi: 10.1016/0375-9474(84)90409-3
1984VO05 Phys.Lett. 136B, 232 (1984) H.P.von Arb, F.Dittus, H.Heeb, H.Hofer, F.Kottmann, S.Niggli, R.Schaeren, D.Taqqu, J.Unternahrer, P.Egelhof Measurement of the Lifetime and Quenching Rate of Metastable 2S Muonic Helium Ions ATOMIC PHYSICS, Mesic-Atoms 4He; measured muonic E(K X-ray), I(K X-ray), 2S-state T1/2, quenching rate.
doi: 10.1016/0370-2693(84)91152-3
1984WE12 Nucl.Instrum.Methods 220, 425 (1984) A Large Solid Angle Ionization Chamber with Ring Counter Geometry NUCLEAR REACTIONS 58Ni(polarized 7Li, 7Li), E=9.5 MeV; 120Sn(polarized 7Li, 7Li), E=12.2 MeV; 208Pb(polarized 7Li, 7Li), E=17.5 MeV; measured Coulomb scattered 7Li spectra; deduced optimum conditions for tensor analyzing power measurements. Large solid angle ionization chamber.
doi: 10.1016/0167-5087(84)90305-3
1983RU09 Nucl.Phys. A407, 208 (1983) K.Rusek, Z.Moroz, R.Caplar, P.Egelhof, K.-H.Mobius, E.Steffens, I.Koenig, A.Weller, D.Fick Spin-Orbit Potentials for Elastic Scattering of Polarized 6Li Ions from 12C and 58Ni NUCLEAR REACTIONS 12C(polarized 6Li, 6Li), E=9, 19.2 MeV; measured iT11(θ), σ(θ), ratio to σ(Rutherford) vs (θ), T20(θ). Optical model analysis. 58Ni(polarized 6Li, 6Li), E=20 MeV; measured σ(θ), ratio to σ(Rutherford) vs (θ), iT11(θ), T20(θ). Optical, diffraction model analyses.
doi: 10.1016/0375-9474(83)90315-9
1982MO13 Nucl.Phys. A381, 294 (1982) Z.Moroz, P.Zupranski, R.Bottger, P.Egelhof, K.-H.Mobius, G.Tungate, E.Steffens, W.Dreves, I.Koenig, D.Fick The Interaction of Aligned 7Li with 58Ni NUCLEAR REACTIONS 58Ni(polarized 7Li, 7Li), E=14.2, 18, 20.3, 22 MeV; measured σ(θ), T20, T21, T22 vs θ, spin-independent analyzing power vs θ. 58Ni(polarized 7Li, 7Li'), E=20.3 MeV; measured σ(θ), T20(θ), spin-dependent analyzing power vs θ. 7Li deduced spectroscopic deformation. Diffraction, optical, DWBA models.
doi: 10.1016/0375-9474(82)90145-2
1982MO17 Z.Phys. A306, 335 (1982) K.-H.Mobius, R.Bottger, P.Egelhof, Z.Moroz, E.Steffens, G.Tungate, I.Koenig, D.Fick The Influence of the Spectroscopic Deformation of Li-Isotopes on Their Interaction with 51V NUCLEAR REACTIONS, ICPND 51V(polarized 6Li, X), (polarized 7Li, X)55Fe/56Fe/52Cr/53Cr/55Mn, (polarized 7Li, 7Li), E=10-20 MeV; 51V(polarized 6Li, 6Li), E=9.8, 12, 14 MeV; measured Eγ, Iγ, reaction σ, elastic σ, tensor analyzing power vs E, θ; deduced production σ(E) for residuals, entrance channel effects. 7Li deduced spectroscopic deformation. Sharp cutoff model.
1981KO42 Fizika(Zagreb) 13, Suppl.No.1, 9 (1981) S.Kossionides, K.-H.Mobius, R.Bottger, P.Egelhof, Z.Moroz, E.Steffens, G.Tungate, W.Dreves, I.Koenig, D.Fick Deformation Dependence of the Cross Section of 7Li(pol) Induced Reactions NUCLEAR REACTIONS 51V(polarized 7Li, X), (polarized 7Li, 7Li), E(cm)=8.5-17.5 MeV; measured σ(reaction), analyzing power vs E. 51V(polarized 7Li, p), (polarized 7Li, t), E=12, 20 MeV; measured σ(θ), analyzing power vs θ; deduced projectile deformation effects. Activation technique.
1981MO05 Nucl.Instrum.Methods 179, 541 (1981) Z.Moroz, R.Bottger, P.Egelhof, K.-H.Mobius, G.Tungate, E.Steffens, W.Dreves, D.Fick Determination of the Alignment of a 7Li Beam by Means of the Doppler-Shift Method NUCLEAR REACTIONS 181Ta(polarized 7Li, 7Li'), E=20 MeV; measured Coulomb excitation σ(θ), Doppler broadened Eγ, Iγ. 7Li deduced alignment t20.
doi: 10.1016/0029-554X(81)90180-4
1981MO08 Phys.Rev.Lett. 46, 1064 (1981) K.-H.Mobius, R.Bottger, P.Egelhof, Z.Moroz, E.Steffens, G.Tungate, W.Dreves, I.Koenig, D.Fick Influence of the Static Deformation of 7Li on the 7Li-51V Total Reaction Cross Section NUCLEAR REACTIONS 51V(polarized 7Li, X), (polarized 7Li, 7Li), E=10-20 MeV; measured σ(reaction), T20(reaction) vs E, σ(quasielastic), T20(quasielastic) vs θ; deduced projectile static deformation effects. Sharp cutoff model.
doi: 10.1103/PhysRevLett.46.1064
1981TU01 Phys.Lett. 98B, 347 (1981) G.Tungate, R.Bottger, P.Egelhof, K.-H.Mobius, Z.Moroz, E.Steffens, W.Dreves, I.Koenig, D.Fick Elastic Scattering of Vector Polarized 7Li on 58Ni NUCLEAR REACTIONS 58Ni(polarized 7Li, 7Li), E=20.3 MeV; measured vector analyzing power iT11(θ), σ(θ); deduced optical model parameters. Optical, folding model analyses.
doi: 10.1016/0370-2693(81)90922-9
1980EG03 Phys.Rev.Lett. 44, 1380 (1980) P.Egelhof, W.Dreves, K.-H.Mobius, E.Steffens, G.Tungate, P.Zupranski, D.Fick, R.Bottger, F.Roesel Determination of the Electric Quadrupole Moment of 7Li by Coulomb Scattering of an Aligned 7Li Ions NUCLEAR REACTIONS 58Ni(polarized 7Li, 7Li), (polarized 7Li, 7Li'), E=10 MeV; 208Pb(polarized 7Li, 7Li), (polarized 7Li, 7Li'), E=22 MeV; measured Coulomb scattering T20(θ). 7Li deduced quadrupole moment.
doi: 10.1103/PhysRevLett.44.1380
1980TU03 Phys.Lett. B95, 35 (1980) G.Tungate, R.Bottger, P.Egelhof, K.-H.Mobius, Z.Moroz, E.Steffens, W.Dreves, D.Fick, D.M.Brink, T.F.Hill Investigation of the 58Ni(7Li, 6Li)59Ni Reaction with Vector Polarized 7Li NUCLEAR REACTIONS 58Ni(polarized 7Li, 6Li), E=20.3 MeV; measured σ(θ), vector analyzing power vs θ; deduced transferred neutron polarization effects.
doi: 10.1016/0370-2693(80)90393-7
1980ZU01 Phys.Lett. 91B, 358 (1980) P.Zupranski, W.Dreves, P.Egelhof, K.-H.Mobius, E.Steffens, G.Tungate, D.Fick Dependence of Deformed Heavy Ion (7Li) Scattering on the Orientation of the Alignment Axis NUCLEAR REACTIONS 58Ni(polarized 7Li, 7Li), E=14.22 MeV; measured σ(θ), tensor analyzing powers; deduced quadrupole moment alignment, shape effects.
doi: 10.1016/0370-2693(80)90995-8
1979EG01 Phys.Lett. 84B, 176 (1979) P.Egelhof, J.Barrette, P.Braun-Munzinger, W.Dreves, C.K.Gelbke, D.Kassen, E.Steffens, W.Weiss, D.Fick Vector Analyzing Power in the Elastic Scattering of 6Li by 4He NUCLEAR REACTIONS 4He(polarized 6Li, 6Li), E=15.1-22.7 MeV; measured σ(θ), A(θ); deduced spin orbit effects in optical model.
doi: 10.1016/0370-2693(79)90277-6
1978DR07 Phys.Lett. 78B, 36 (1978) W.Dreves, P.Zupranski, P.Egelhof, D.Kassen, E.Steffens, W.Weiss, D.Fick Shape Effects in Heavy Ion (Li) Elastic Scattering NUCLEAR REACTIONS 58Ni(6Li, 6Li), (7Li, 7Li), E(cm)=12.7 MeV; 12,13C(6Li, 6Li), (7Li, 7Li), E=9 MeV; measured σ(θ).
doi: 10.1016/0370-2693(78)90341-6
1978MA13 Phys.Lett. 74B, 187 (1978) M.Makowska-Rzeszutko, P.Egelhof, D.Kassen, E.Steffens, W.Weiss, D.Fick, W.Dreves, K.-I.Kubo, T.Suzuki Transfer Reactions Initiated on 12C by Vector Polarized 6Li NUCLEAR REACTIONS 12C(polarized 6Li, d), (polarized 6Li, α), E=20.0 MeV; measured A(θ).
doi: 10.1016/0370-2693(78)90549-X
1976WE10 Phys.Lett. 61B, 237 (1976) W.Weiss, P.Egelhof, K.D.Hildenbrand, D.Kassen, M.Makowska-Rzeszutko, D.Fick, H.Ebinghaus, E.Steffens, A.Amakawa, K.I.Kubo Elastic Scattering of Vector Polarized 6Li NUCLEAR REACTIONS 12C(polarized 6Li, 6Li), E=20, 22.8 MeV; 16O, 28Si, 58Ni(polarized 6Li, 6Li), E=22.8 MeV; measured σ(θ), analyzing power A(θ).
doi: 10.1016/0370-2693(76)90138-6
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