NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = K.D.Schilling Found 60 matches. 2014MA05 Phys.Rev.Lett. 112, 072501 (2014) R.Massarczyk, R.Schwengner, F.Donau, S.Frauendorf, M.Anders, D.Bemmerer, R.Beyer, C.Bhatia, E.Birgersson, M.Butterling, Z.Elekes, A.Ferrari, M.E.Gooden, R.Hannaske, A.R.Junghans, M.Kempe, J.H.Kelley, T.Kogler, A.Matic, M.L.Menzel, S.Muller, T.P.Reinhardt, M.Roder, G.Rusev, K.D.Schilling, K.Schmidt, G.Schramm, A.P.Tonchev, W.Tornow, A.Wagner Nuclear Deformation and Neutron Excess as Competing Effects for Dipole Strength in the Pygmy Region NUCLEAR REACTIONS 124,128,132,134Xe(γ, X), E<12 MeV; measured reaction products, Eγ, Iγ. 124,128,132,134Xe; deduced photoabsorption σ, summed B(E1) strength, nuclear deformation in the region of the pygmy dipole resonance. Nuclear resonance fluorescence experiment, random-phase approximation calculations, comparison with available data.
doi: 10.1103/PhysRevLett.112.072501
2013SC03 Phys.Rev. C 87, 024306 (2013) R.Schwengner, R.Massarczyk, G.Rusev, N.Tsoneva, D.Bemmerer, R.Beyer, R.Hannaske, A.R.Junghans, J.H.Kelley, E.Kwan, H.Lenske, M.Marta, R.Raut, K.D.Schilling, A.Tonchev, W.Tornow, A.Wagner Pygmy dipole strength in 86Kr and systematics of N=50 isotones NUCLEAR REACTIONS 86Kr(γ, γ'), (polarized γ, γ'), E<11.2 MeV; measured Eγ, Iγ, γγ(θ), widths, azimuthal asymmetry, integrated σ. ELBE accelerator facility at HZDR, and HIγS facility at TUNL. 86Kr; deduced levels, PDR, J, π, branching ratios, photoabsorption σ(E), energy-weighted sums of photoabsorption σ. Comparison of photoabsorption σ with that from (γ, n) reaction. NUCLEAR STRUCTURE 86Kr, 88Sr, 90Zr, 92Mo; calculated neutron skin thickness, B(E1), proton and neutron transition densities using QRPA calculations. Comparison with shell-model calculations.
doi: 10.1103/PhysRevC.87.024306
2012MA31 Phys.Rev. C 86, 014319 (2012) R.Massarczyk, R.Schwengner, F.Donau, E.Litvinova, G.Rusev, R.Beyer, R.Hannaske, A.R.Junghans, M.Kempe, J.H.Kelley, T.Kogler, K.Kosev, E.Kwan, M.Marta, A.Matic, C.Nair, R.Raut, K.D.Schilling, G.Schramm, D.Stach, A.P.Tonchev, W.Tornow, E.Trompler, A.Wagner, D.Yakorev Electromagnetic dipole strength of 136Ba below the neutron separation energy NUCLEAR REACTIONS 136Ba(γ, γ'), E at 7.0 MeV/c and 11.4 MeV/c; 136Ba(polarized γ, γ')E=4.7, 5.1, 5.6, 6.1, 6.5, 7.0, 7.5, 8.0, 8.4, 8.7, 9.0, 9.3 MeV; measured Eγ, Iγ, integrated σ(E), photoabsorption σ as a function of excitation energy, γ(θ), γ(lin pol) using Bremsstrahlung facility at ELBE, HZDR, and HIγS facility at TUNL. 136Ba; deduced levels, J, π, widths, pygmy dipole resonances, dipole strength in the quasicontinuum, enhancement of dipole strength. Statistical code used to simulate inelastic transitions and to determine the branching ratios of transitions to ground state. GEANT4 simulations. Comparison with previous experimental studies, and with theoretical calculations using quasiparticle random-phase approximation (QRPA) and relativistic quasiparticle time blocking approximation (RQTBA) approaches. Comparison of photoabsorption σ in 136,138Ba and 139La targets.
doi: 10.1103/PhysRevC.86.014319
2012SC02 Phys.Rev. C 85, 014311 (2012) G.Schramm, R.Massarczyk, A.R.Junghans, T.Belgya, R.Beyer, E.Birgersson, E.Grosse, M.Kempe, Z.Kis, K.Kosev, M.Krticka, A.Matic, K.D.Schilling, R.Schwengner, L.Szentmiklosi, A.Wagner, J.L.Weil Dipole strength in 78Se below the neutron separation energy from a combined analysis of 77Se(n, γ) and 78Se(γ, γ') experiments NUCLEAR REACTIONS 77Se(n, γ), E AP 6 milli-eV, cold neutrons; 78Se(γ, γ'), E<11.5 MeV bremsstrahlung; measured Eγ, Iγ; deduced photoabsorption cross section, level density according to constant-temperature model, dipole strength function. Comparison with simulated spectra from extreme statistical code.
doi: 10.1103/PhysRevC.85.014311
2011BE54 Fizika(Zagreb) B 20, 203 (2011) N.Benouaret, R.Schwengner, G.Rusev, F.Donau, R.Beyer, M.Erhard, E.Grosse, A.R.Junghans, K.Kosev, C.Nair, K.D.Schilling, A.Wagner Investigation of dipole excitations below the giant dipole resonance in 89Y using the ELBE facility NUCLEAR REACTIONS 89Y(γ, γ'), E<13.2 MeV; measured Eγ, Iγ; deduced energy levels, resolved giant dipole resonance strength, σ, level densities, branching ratios. Comparison with available data, QRPA calculations.
2011JU04 J.Korean Phys.Soc. 59, 1593s (2011) A.R.Junghans, E.Altstadt, R.Beyer, E.Birgersson, T.Cowan, A.Ferrari, R.Hannaske, A.Matic, K.D.Schilling, R.Schlenk, S.Schneider, R.Schwengner, A.Wagner, F.-P.Weiss, D.Gehre, E.Grosse The nELBE Neutron Time of Flight Facility NUCLEAR REACTIONS 56Fe(n, n'), E=800-6000 keV; measured En, In using plastic and ELBE TOFi, Eγ, Iγ using BaF2; deduced σ. Compared with other data and ENDFB-VII.
doi: 10.3938/jkps.59.1593
2010ER07 J.Phys.:Conf.Ser. 202, 012014 (2010) M.Erhard, E.Grosse, A.R.Junghans, J.Klug, C.Nair, G.Rusev, K.D.Schilling, R.Schwengner, A.Wagner Photoactivation of the p-nucleus 92Mo with bremsstrahlung at ELBE NUCLEAR REACTIONS 92Mo(γ, p), (γ, n), (γ, α), E=0-16 MeV[from bremsstrahlung];100Mo(γ, n), E=10-17 MeV [from bremsstrahlung]; measured Eγ, Iγ; deduced photoactivation yields using activation method; calculated photoactivation yields using TALYS, NON-SMOKER with different nuclear models. Compared with available data.
doi: 10.1088/1742-6596/202/1/012014
2010MA40 Phys.Rev. C 82, 024314 (2010) A.Makinaga, R.Schwengner, G.Rusev, F.Donau, S.Frauendorf, D.Bemmerer, R.Beyer, P.Crespo, M.Erhard, A.R.Junghans, J.Klug, K.Kosev, C.Nair, K.D.Schilling, A.Wagner Dipole strength in 139La below the neutron-separation energy NUCLEAR REACTIONS 139La(γ, γ'), E=2-10 MeV; measured Eγ, Iγ; deduced levels, integrated cross section, branching ratios, partial widths, level densities as function of spin, and γ-intensity distributions. Comparison with calculations based on quasiparticle-random-phase approximation using an instantaneous-shape sampling (ISS-QRPA).
doi: 10.1103/PhysRevC.82.024314
2010NA12 Phys.Rev. C 81, 055806 (2010) C.Nair, A.R.Junghans, M.Erhard, D.Bemmerer, R.Beyer, E.Grosse, K.Kosev, M.Marta, G.Rusev, K.D.Schilling, R.Schwengner, A.Wagner Dipole strength in 144Sm studied via (γ, n), (γ, p), and (γ, α) reactions NUCLEAR REACTIONS 144Sm(γ, n), (γ, p), (γ, α), E<20 MeV bremsstrahlung; measured Eγ, Iγ, yields, σ(E) using activation method. Comparison with Hauser-Feshbach statistical models calculations using NON-SMOKER code.
doi: 10.1103/PhysRevC.81.055806
2010SC11 Phys.Rev. C 81, 054315 (2010) R.Schwengner, R.Massarczyk, B.A.Brown, R.Beyer, F.Donau, M.Erhard, E.Grosse, A.R.Junghans, K.Kosev, C.Nair, G.Rusev, K.D.Schilling, A.Wagner E1 strength in 208Pb within the shell model NUCLEAR REACTIONS 208Pb(γ, γ'), E=9-15 MeV; measured Eγ, Iγ, γ(θ), linear polarization, integrated cross sections. 208Pb; deduced levels, J, π, widths, B(E1). Comparison with shell model and QRPA calculations.
doi: 10.1103/PhysRevC.81.054315
2009BE03 Phys.Rev. C 79, 014303 (2009) N.Benouaret, R.Schwengner, G.Rusev, F.Donau, R.Beyer, M.Erhard, E.Grosse, A.R.Junghans, K.Kosev, C.Nair, K.D.Schilling, A.Wagner, N.Bendjaballah Dipole strength in 89Y up to the neutron-separation energy NUCLEAR REACTIONS 89Y(γ, γ'), E=3-13 MeV; measured Eγ, Iγ, σ, widths, angular distributions, level densities. 89Y; deduced levels. Comparison with quasiparticle-random-phase approximation predictions. NUCLEAR REACTIONS 88Sr, 90Zr(γ, X), E=5-18 MeV; analyzed data for photoabsorption cross sections. Comparison with quasiparticle-random-phase approximation predictions.
doi: 10.1103/PhysRevC.79.014303
2009RU05 Phys.Rev. C 79, 061302 (2009) G.Rusev, R.Schwengner, R.Beyer, M.Erhard, E.Grosse, A.R.Junghans, K.Kosev, C.Nair, K.D.Schilling, A.Wagner, F.Donau, S.Frauendorf Enhanced electric dipole strength below particle-threshold as a consequence of nuclear deformation NUCLEAR REACTIONS 92,94,96,98,100Mo(γ, γ'), E=4-13 MeV; measured Eγ, Iγ, absolute photoabsorption σ. Comparison with QRPA calculations.
doi: 10.1103/PhysRevC.79.061302
2009SC07 Phys.Rev. C 79, 037303 (2009); Publisher's note Phys.Rev. C 79, 039902 (2009) R.Schwengner, A.Wagner, Y.Fujita, G.Rusev, M.Erhard, D.De Frenne, E.Grosse, A.R.Junghans, K.Kosev, K.D.Schilling Dipole transition strengths in 26Mg NUCLEAR REACTIONS 26Mg(γ, γ'), E=13.0 MeV; measured Eγ, Iγ, γ(θ), cross sections, widths. 26Mg; deduced levels, J, π, B(E1), B(M1).
doi: 10.1103/PhysRevC.79.037303
2008NA05 J.Phys.(London) G35, 014036 (2008) C.Nair, A.R.Junghans, M.Erhard, D.Bemmerer, R.Beyer, P.Crespo, E.Grosse, M.Fauth, K.Kosev, G.Rusev, K.D.Schilling, R.Schwengner, A.Wagner Photodisintegration studies on p-nuclei: the case of Mo and sm isotopes NUCLEAR REACTIONS 92Mo(γ, p), (γ, n), (γ, α), E not given; 144Sm(γ, n), (γ, α), E not given; measured Eγ, Iγ, activation yields. Comparison with model calculations.
doi: 10.1088/0954-3899/35/1/014036
2008NA26 Phys.Rev. C 78, 055802 (2008) C.Nair, M.Erhard, A.R.Junghans, D.Bemmerer, R.Beyer, E.Grosse, J.Klug, K.Kosev, G.Rusev, K.D.Schilling, R.Schwengner, A.Wagner Photoactivation experiment on 197Au and its implications for the dipole strength in heavy nuclei NUCLEAR REACTIONS 197Au(γ, n), E=8.0-15.5 MeV; measured activation yields. Comparison with Hauser Feshbach calculations.
doi: 10.1103/PhysRevC.78.055802
2008RU04 Phys.Rev. C 77, 064321 (2008) G.Rusev, R.Schwengner, F.Donau, M.Erhard, E.Grosse, A.R.Junghans, K.Kosev, K.D.Schilling, A.Wagner, F.Becvar, M.Krticka Low-energy tail of the giant dipole resonance in 98Mo and 100Mo deduced from photon-scattering experiments NUCLEAR REACTIONS 98,100Mo(γ, γ'), E<15 MeV; measured Eγ, Iγ, photoabsorption σ, giant resonances, angular distributions, distribution of mean branching ratios, dipole strength functions; deduced multipolarities. 27Al, 28Si, 56Fe, 63Cu, 70,72,73,74Ge(n, γ), E=thermal; measured Eγ, Iγ. 99,101Mo(γ, n); analyzed cross sections. 97Mo(n, γ), 98Mo(3He, 3He'γ); comparisons.
doi: 10.1103/PhysRevC.77.064321
2008SC20 Phys.Rev. C 78, 064314 (2008) R.Schwengner, G.Rusev, N.Tsoneva, N.Benouaret, R.Beyer, M.Erhard, E.Grosse, A.R.Junghans, J.Klug, K.Kosev, H.Lenske, C.Nair, K.D.Schilling, A.Wagner Pygmy dipole strength in 90Zr NUCLEAR REACTIONS 90Zr(γ, γ'), E=7.9, 9.0, 13.2 MeV; measured Eγ, Iγ.σ, angular distributions, widths; deduced levels, J, π. Comparisons with calculations for 88Sr, 90Zr.
doi: 10.1103/PhysRevC.78.064314
2008WA07 J.Phys.(London) G35, 014035 (2008) A.Wagner, R.Beyer, M.Erhard, E.Grosse, A.R.Junghans, J.Klug, K.Kosev, C.Nair, N.Nankov, G.Rusev, K.D.Schilling, R.Schwengner Photon strength distributions in stable even-even molybdenum isotopes NUCLEAR REACTIONS 92,94,96,98,100Mo(γ, γ'), E not given; measured Eγ, Iγ, photoabsorption cross sections.
doi: 10.1088/0954-3899/35/1/014035
2007DO13 Phys.Rev. C 76, 014317 (2007) F.Donau, G.Rusev, R.Schwengner, A.R.Junghans, K.D.Schilling, A.Wagner Effect of nuclear deformation on the electric-dipole strength in the particle-emission threshold region NUCLEAR STRUCTURE Mo, Sm, Nd; calculated B(E1) and photoabsorption cross section using a deformed oscillator model and a Nilsson plus RPA model.
doi: 10.1103/PhysRevC.76.014317
2007SC36 Phys.Rev. C 76, 034321 (2007) R.Schwengner, G.Rusev, N.Benouaret, R.Beyer, M.Erhard, E.Grosse, A.R.Junghans, J.Klug, K.Kosev, L.Kostov, C.Nair, N.Nankov, K.D.Schilling, A.Wagner Dipole response of 88Sr up to the neutron-separation energy NUCLEAR REACTIONS 88Sr(γ, γ'), E=9.0, 13.2, 16.0 MeV; measured Eγ, Iγ and angular distributions. 88Sr deduced levels, J, π, photon scattering and photoabsortption cross sections.
doi: 10.1103/PhysRevC.76.034321
2007SC39 Nucl.Phys. A788, 331c (2007) R.Schwengner, N.Benouaret, R.Beyer, F.Donau, M.Erhard, S.Frauendorf, E.Grosse, A.R.Junghans, J.Klug, K.Kosev, C.Nair, N.Nankov, G.Rusev, K.D.Schilling, A.Wagner Dipole-strength distributions up to the particle-separation energies and photodissociation of Mo isotopes NUCLEAR REACTIONS 92,98,100Mo(γ, γ'), E≈13.2 MeV bremsstrahlung; measured Eγ, Iγ, angular distributions, photoabsorption σ. 92Mo(γ, n), (γ, p), (γ, α), E≈10-16.5 MeV bremsstrahlung; measured activation yields and compared with QRPA calculations.
doi: 10.1016/j.nuclphysa.2007.01.062
2006ER06 Eur.Phys.J. A 27, Supplement 1, 135 (2006) M.Erhard, A.R.Junghans, R.Beyer, E.Grosse, J.Klug, K.Kosev, C.Nair, N.Nankov, G.Rusev, K.D.Schilling, R.Schwengner, A.Wagner Photodissociation of p-process nuclei studied by bremsstrahlung-induced activation NUCLEAR REACTIONS 197Au, 100Mo(γ, n), 92Mo(γ, n), (γ, p), (γ, α), E ≈ 11.8-14 MeV bremsstrahlung; measured activation yields.
doi: 10.1140/epja/i2006-08-019-4
2006RU06 Phys.Rev. C 73, 044308 (2006) G.Rusev, R.Schwengner, F.Donau, M.Erhard, S.Frauendorf, E.Grosse, A.R.Junghans, L.Kaubler, K.Kosev, L.K.Kostov, S.Mallion, K.D.Schilling, A.Wagner, H.von Garrel, U.Kneissl, C.Kohstall, M.Kreutz, H.H.Pitz, M.Scheck, F.Stedile, P.von Brentano, C.Fransen, J.Jolie, A.Linnemann, N.Pietralla, V.Werner Systematics of magnetic dipole strength in the stable even-mass Mo isotopes NUCLEAR REACTIONS 92Mo(γ, γ'), E=6.0 MeV bremsstrahlung; 98,100Mo(γ, γ'), E ≈ 3.3, 3.8 MeV bremsstrahlung; measured Eγ, Iγ. 92,98,100Mo deduced transitions B(M1), strength distributions. Comparison with quasiparticle RPA model predictions.
doi: 10.1103/PhysRevC.73.044308
2006RU11 Eur.Phys.J. A 27, Supplement 1, 171 (2006) G.Rusev, E.Grosse, M.Erhard, A.Junghans, K.Kosev, K.-D.Schilling, R.Schwengner, A.Wagner Pygmy dipole strength close to particle-separation energies - The case of the Mo isotopes NUCLEAR REACTIONS 92,98,100Mo(γ, γ'), E=14 MeV bremsstrahlung; measured Eγ, Iγ. 91,98,100Mo deduced dipole strength functions.
doi: 10.1140/epja/i2006-08-025-6
2006VO04 Phys.Rev. C 73, 054315 (2006) H.von Garrel, P.von Brentano, C.Fransen, G.Friessner, N.Hollmann, J.Jolie, F.Kappeler, L.Kaubler, U.Kneissl, C.Kohstall, L.Kostov, A.Linnemann, D.Mucher, N.Pietralla, H.H.Pitz, G.Rusev, M.Scheck, K.D.Schilling, C.Scholl, R.Schwengner, F.Stedile, S.Walter, V.Werner, K.Wisshak Low-lying E1, M1, and E2 strength distributions in 124, 126, 128, 129, 130, 131, 132, 134, 136Xe: Systematic photon scattering experiments in the mass region of a nuclear shape or phase transition NUCLEAR REACTIONS 124,126,128,129,130,131,132,134,136Xe(γ, γ'), E=4.1 MeV bremsstrahlung; measured Eγ, Iγ. 124,126,128,129,130,131,132,134,136Xe deduced levels, J, π, branching ratios, B(E1), B(M1).
doi: 10.1103/PhysRevC.73.054315
2005RU14 Phys.Rev.Lett. 95, 062501 (2005) G.Rusev, R.Schwengner, F.Donau, S.Frauendorf, L.Kaubler, L.K.Kostov, S.Mallion, K.D.Schilling, A.Wagner, E.Grosse, H.von Garrel, U.Kneissl, C.Kohstall, M.Kreutz, H.H.Pitz, M.Scheck, F.Stedile, P.von Brentano, J.Jolie, A.Linnemann, N.Pietralla, V.Werner Decay of 1+ States as a New Probe of the Structure of 0+ Shape Isomers NUCLEAR REACTIONS 98,100Mo(γ, γ'), E=3.2-3.8 MeV bremsstrahlung; measured Eγ, Iγ. 98,100Mo deduced levels, J, π, branching ratios, transition probabilities, shape isomer configuration mixing features.
doi: 10.1103/PhysRevLett.95.062501
2005WA31 J.Phys.(London) G31, S1969 (2005) A.Wagner, R.Beyer, M.Erhard, F.Donau, E.Grosse, A.Hartmann, A.R.Junghans, L.Kaubler, K.Kosev, S.Mallion, C.Nair, N.Nankov, G.Rusev, K.D.Schilling, W.Schulze, R.Schwengner The new bremsstrahlung facility at the superconducting electron accelerator ELBE NUCLEAR REACTIONS 92,98,100Mo(γ, γ'), E=13.2 MeV bremsstrahlung; measured Eγ, Iγ. 92,100Mo, 197Au(γ, n), 92Mo(γ, p), (γ, α), E ≈ 11.8-16.5 MeV bremsstrahlung; measured integrated σ.
doi: 10.1088/0954-3899/31/10/112
2002HE26 Nucl.Phys. A712, 207 (2002) C.-M.Herbach, D.Hilscher, V.G.Tishchenko, P.Gippner, D.V.Kamanin, W.von Oertzen, H.-G.Ortlepp, Yu.E.Penionzhkevich, Yu.V.Pyatkov, G.Renz, K.D.Schilling, O.V.Strekalovsky, W.Wagner, V.E.Zhuchko Search for mass-symmetric ternary fission in the reactions 14N(53 AMeV) + 197Au and 232Th NUCLEAR REACTIONS 197Au, 232Th(14N, X), E=53 MeV/nucleon; measured binary and ternary fission fragment yields following incomplete fusion, fragment velocity correlations; deduced anisotropic contribution, stretched scission configuration. Coulomb trajectory calculations.
doi: 10.1016/S0375-9474(02)01242-3
2002KA25 Phys.Rev. C65, 054315 (2002) L.Kaubler, K.D.Schilling, R.Schwengner, F.Donau, E.Grosse, D.Belic, P.von Brentano, M.Bubner, C.Fransen, M.Grinberg, U.Kneissl, C.Kohstall, A.Linnemann, P.Matschinsky, A.Nord, N.Pietralla, H.H.Pitz, M.Scheck, F.Stedile, V.Werner Influence of the N = 50 Neutron Core on Dipole Excitations in 87Rb NUCLEAR REACTIONS 87Rb(γ, γ'), E=4.0 MeV bremsstrahlung; measured Eγ, Iγ. 87Rb deduced levels, J, π, configurations, excitation B(M1), B(E1), widths. Comparison with shell model predictions.
doi: 10.1103/PhysRevC.65.054315
2002RA13 Phys.Rev. C65, 044327 (2002) G.Rainovski, R.Schwengner, K.D.Schilling, A.Wagner, A.Jungclaus, E.Galindo, O.Thelen, D.R.Napoli, C.A.Ur, G.de Angelis, M.Axiotis, A.Gadea, N.Marginean, T.Martinez, Th.Kroll High-Spin Structure of the Spherical Nucleus 90Y NUCLEAR REACTIONS 82Se(11B, 3n), E=37 MeV; measured Eγ, Iγ, γγ-coin, DSA. 90Y deduced high-spin levels, J, π, T1/2, configurations. Comparison with shell model predictions. GASP array.
doi: 10.1103/PhysRevC.65.044327
2001ST14 Phys.Rev. C63, 064315 (2001) E.A.Stefanova, R.Schwengner, G.Rainovski, K.D.Schilling, A.Wagner, F.Donau, E.Galindo, A.Jungclaus, K.P.Lieb, O.Thelen, J.Eberth, D.R.Napoli, C.A.Ur, G.de Angelis, M.Axiotis, A.Gadea, N.Marginean, T.Martinez, Th.Kroll, T.Kutsarova Structure of High-Spin States in 89Sr and 90Sr NUCLEAR REACTIONS 82Se(11B, 3np), (11B, 2np), E=37 MeV; measured Eγ, Iγ, γγ-coin. 89,90Sr deduced high-spin levels, J, π. GASP array. Comparison with shell model calculations.
doi: 10.1103/PhysRevC.63.064315
1998OR05 Nucl.Phys. A642, 407 (1998) H.-G.Ortlepp, W.Wagner, C.-M.Herbach, P.Gippner, K.D.Schilling, Yu.E.Penionzhkevich Fragment Mass Distribution of Fission After Incomplete Fusion in the Reaction 7Li (43A MeV) + 232Th NUCLEAR REACTIONS 232Th(7Li, F), E=43 MeV/nucleon; measured binary fission fragments mass, energy distributions; deduced compound nucleus cooling time, fission dynamics.
doi: 10.1016/S0375-9474(98)00491-6
1995AL05 Nucl.Phys. A583, 465c (1995) A.A.Aleksandrov, I.A.Aleksandrova, M.Andrassy, L.Dietterle, V.N.Doronin, P.Gippner, C.-M.Herbach, D.Hilscher, S.I.Ivanovsky, A.Matthies, D.May, H.-G.Ortlepp, G.Pausch, Yu.E.Penionzhkevich, V.N.Pokrovsky, G.Renz, K.-D.Schilling, D.I.Shishkin, V.E.Shuchko, O.V.Strekalovsky, V.V.Trofimov, and the FOBOS Collaboration First Experiments with FOBOS NUCLEAR REACTIONS 232Th(7Li, X), E=43 MeV/nucleon; measured fission (fragment)(intermediate mass fragment)-coin. Position sensitive avalanche counter, BRAGG ionization chamber, CsI scintillation counter assembly, fission following incomplete fusion.
doi: 10.1016/0375-9474(94)00706-S
1990SC19 Z.Phys. A336, 1 (1990) K.D.Schilling, P.Gippner, W.Seidel, F.Stary, D.Wohlfarth Search for Charged-Particle Emission from Deuterated Palladium Foils NUCLEAR REACTIONS 2H(d, X), E=low; measured cold nuclear fusion associated charged particle emission upper limit. Deuterium loaded Pd electrodes in electrolysis cell.
1989ZO01 Yad.Fiz. 49, 8 (1989) H.Zodan, S.M.Lukyanov, Yu.E.Penionzhkevich, V.S.Salamatin, G.G.Chubarian, K.Heidel, A.Pop, K.D.Schilling, E.Will, P.Gippner, K.Borcha Shell-Structure Manifestation in Characteristics of the Zn + Sn Reaction Products NUCLEAR REACTIONS Ag(64Zn, X), E=300, 335 MeV; 114Sn(64Zn, X), E=315-390 MeV; 116,122Sn(64Zn, X), E=315 MeV; 139La(64Zn, X), E=345, 365 MeV; measured fragment mass, total kinetic energy dependences; deduced shell structure role.
1988GI06 Z.Phys. A330, 433 (1988) P.Gippner, K.D.Schilling, F.Stary, E.Will, K.Heidel, S.M.Lukyanov, Yu.E.Penionzhkevich, V.S.Salamatin, H.Sodan, G.G.Chubarian, R.Schmidt On the Evolution of the Mass Asymmetry in Damped Heavy-Ion Collisions NUCLEAR REACTIONS 114Sn, Ag, 139La(64Zn, X), E < Coulomb barrier; measured total kinetic energy vs fragment mass distribution; deduced structure effects role.
1988KO11 Z.Phys. A330, 189 (1988) R.Kotte, W.D.Fromm, E.Hentschel, H.G.Ortlepp, K.D.Schilling, W.Seidel, F.Stary, G.Zwicker In-Beam Investigation of Ternary Fission NUCLEAR REACTIONS 238U(d, αF), E=13.5 MeV; measured σ(Eα), σ(θα), fission (fragment)(α)(θ), fission fragment mass distribution vs Eα. Natural Uranium target.
1987SC28 Nucl.Instrum.Methods Phys.Res. A257, 197 (1987) K.D.Schilling, P.Gippner, W.Seidel, F.Stary, E.Will, K.Heidel, S.M.Lukyanov, Yu.E.Penionzhkevich, V.S.Salamatin, H.Sodan, G.G.Chubarian The Dubna Double-Arm Time-of-Flight Spectrometer for Heavy-Ion Reaction Products NUCLEAR REACTIONS 232Th(40Ar, X), E=220, 301 MeV; measured binary fragments σ(θ3, θ4), relative yields vs fragment mass. Double-arm tof spectrometer.
doi: 10.1016/0168-9002(87)90739-X
1986GI16 Z.Phys. A325, 335 (1986) P.Gippner, K.D.Schilling, W.Seidel, F.Stary, E.Will, H.Sodan, S.M.Lukyanov, V.S.Salamatin, Yu.E.Penionzhkevich, G.G.Chubarian, R.Schmidt Shell Effects in the Evolution of the Mass Asymmetry in Heavy-Ion Collisions Leading to Composite Systems with Z = 108 NUCLEAR REACTIONS 249Cf(22Ne, X), E=174 MeV; 238U(32S, X), E=192 MeV; 232Th(40Ar, X), E=206, 220, 301 MeV; 208Pb(56Fe, X), E=354 MeV; measured fragment mass distributions, total kinetic energy vs mass distributions; calculated fusion barriers, excitation energies; deduced mass asymmetry evolution shell effect dependence. Correlation spectrometer. Heavy ion collision dynamics.
1984RO06 Nucl.Phys. A417, 1 (1984) H.Rotter, C.Heiser, K.D.Schilling, W.Andrejtscheff, L.K.Kostov, M.K.Balodis Electromagnetic Transition Probabilities in the Doubly Odd N = 91 Nucleus 154Eu NUCLEAR REACTIONS 153Eu(n, γ), E=thermal; measured Eγ, Iγ, γγ(t). 154Eu levels deduced T1/2, B(λ). Enriched target, plastic scintillator, Ge detector. Nilsson-plus-pairing-model calculations.
doi: 10.1016/0375-9474(84)90320-8
1981BR15 Yad.Fiz. 33, 1453 (1981) H.Bruchertseifer, E.Langrok, Yu.A.Muzycka, Yu.Ts.Oganesyan, T.Pavlat, Yu.E.Penionzhkevich, B.I.Pustylnik, K.D.Schilling Study of Reactions followed by α-Particle Emission NUCLEAR REACTIONS 176Lu(22Ne, xnα), E=100-120 MeV; measured Eγ, Iγ; deduced production σ(E) for 191,192,193,194Au, reaction mechanism. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0594. 1980BO34 Izv.Akad.Nauk SSSR, Ser.Fiz. 44, 2234 (1980) K.Borcha, E.Gerlik, R.Kalpakchieva, Yu.Ts.Oganesyan, T.Pavlat, Yu.E.Penionzhkevich, K.D.Schilling, H.Bruchertseifer, E.Langrok Radiation Associated with High Energy α-Particle Escape in Heavy Ion Reactions NUCLEAR REACTIONS 197Au, 181Ta, 232Th(22Ne, α), E=178 MeV; 181Ta(20Ne, α), E=110, 196 MeV; measured σ(Eα, θ). Evaporation model analysis.
1979AN19 Nucl.Phys. A325, 317 (1979) W.Andrejtscheff, K.D.Schilling Transition Probabilities and Deformations in the Doubly Odd Nucleus 152Eu NUCLEAR REACTIONS 151Eu(n, γ), E=thermal; measured γγ(t). 152Eu levels deduced T1/2, B(λ), β. Enriched target. Plastic scintillator, Ge(Li) detector.
doi: 10.1016/0375-9474(79)90020-4
1979DU02 Nucl.Phys. A315, 317 (1979) F.Dubbers, L.Funke, P.Kemnitz, K.D.Schilling, H.Strusny, E.Will, G.Winter, M.K.Balodis High-Spin States of the Doubly Odd Nucleus 178Ta NUCLEAR REACTIONS 176Lu(α, 2n), E=23-27 MeV; measured σ(Eα;Eγ, θ), Eγ, Iγ, γγ-coin, γγ(t), αγ(t). 178Hf(d, 2n), E=13.5 MeV; measured Eγ, Iγ, γγ-coin, E(ce), I(ce). 178Hf(p, n), E=6.7, 10 MeV; measured Eγ, Iγ, γγ(t). 178Ta deduced levels, J, π, T1/2. Enriched targets; Ge(Li), Si(Li) detectors.
doi: 10.1016/0375-9474(79)90614-6
1978AD03 Nucl.Phys. A311, 188 (1978) I.Adam, W.Andrejtscheff, K.Y.Gromov, M.Honusek, V.V.Kuznetsov, H.I.Lizurej, N.Z.Marupov, T.M.Muminov, A.F.Novgorodov, H.U.Siebert, R.R.Usmanov, Y.V.Yushkevich, K.D.Schilling Excited States of the Doubly Odd Deformed Nucleus 160Tm RADIOACTIVITY 160Yb [from Ta, Hf(p, X), E=660 MeV]; measured Eγ, Iγ, E(ce), I(ce), prompt γγ-coin, delayed γγ, γce-coin; deduced ICC, log ft. 160Tm deduced levels, J, π, T1/2, γ-multipolarity, B(λ), quadrupole deformation. Natural Ta, Hf targets, mass-separated isobar sources. Ge(Li), scintillation detectors, β-spectrometers.
doi: 10.1016/0375-9474(78)90509-2
1978AN27 Nukleonika 23, 159 (1978) W.Andrejtscheff, U.Hagemann, L.Kaubler, H.Prade, K.D.Schilling, L.Schneider, F.Stary In-Beam Gamma-Spectroscopic Investigations of Nanosecond Isomers NUCLEAR REACTIONS 143Nd(d, 2n), E=13.5 MeV; 141Pr(α, 2n), E=22.4, 24.4, 27.0 MeV; measured Eγ, γ(t), γγ-coin, I(ce), linear polarization, γ(θ, H, t). 143Pm deduced levels, T1/2, g, δ.
1978SC10 Nucl.Phys. A299, 189 (1978) K.D.Schilling, L.Kaubler, W.Andrejtscheff, T.M.Muminov, V.G.Kalinnikov, N.Z.Marupov, F.R.May, W.Seidel Electromagnetic Transitions in Some Doubly Odd Deformed Nuclei RADIOACTIVITY 156,158Er, 162mHo, 162Yb [from Ta+p, Ep=660 MeV]; measured γce-delay. 156,158,162Ho, 162Tm levels deduced T1/2, B(λ). Natural targets. Plastic scintillators, magnetic lens β-spectrometer. NUCLEAR REACTIONS 160Gd, 162,164Dy, 178Hf(p, n), E=8-10 MeV; 162,164Dy(d, 2n), E=13.5 MeV; 176Lu(α, 2n), E=27 MeV; 159Tb, 165Ho, 185,187Re(n, γ), E=thermal; measured γγ-, dγ-, αγ-delay. 160Tb, 162,164,166Ho, 178Ta, 186,188Re levels deduced T1/2, B(λ). Enriched targets. Plastic, NaI(Tl) scintillators, Ge(Li) detectors.
doi: 10.1016/0375-9474(78)90028-3
1977SC22 J.Phys.(London) G3, 1255 (1977) K.D.Schilling, W.Andrejtscheff, G.Winter Hexadecapole Deformations and E1 Transitions in Odd-A Ho and Tm Nuclei NUCLEAR STRUCTURE 161,163,165Ho, 163,165,167,169,171Tm; calculated B(E1).
doi: 10.1088/0305-4616/3/9/016
1976AN03 Phys.Lett. 60B, 241 (1976) W.Andrejtscheff, K.D.Schilling, G.Winter The Effect of Hexadecapole Deformations on E1 Transition Strengths NUCLEAR STRUCTURE 161,163,165Ho, 165,167,169,171Tm; analyzed B(E1); deduced effect of hexadecapole deformations.
doi: 10.1016/0370-2693(76)90290-2
1976SC19 Nucl.Phys. A265, 58 (1976) K.D.Schilling, L.Kaubler, F.Stary, W.Andrejtscheff Electromagnetic Transitions in Some Odd-Proton Deformed Nuclei NUCLEAR REACTIONS 161Dy, 171Yb(p, n), E=8.5 MeV; 163Dy, 173Yb(p, n), E=8 MeV; measured γγ-delay. 161,163Ho, 171,173Lu levels deduced T1/2, B(λ). Enriched targets. Plastic scintillator, Ge(Li) detector.
doi: 10.1016/0375-9474(76)90115-9
1975AN21 At.Data Nucl.Data Tables 16, 515 (1975) W.Andrejtscheff, K.D.Schilling, P.Manfrass Gamma-Ray Transition Probabilities in Deformed Nuclei (150 < A ≤ 190) COMPILATION A=150-190; compiled Eγ, B(λ), ICC.
doi: 10.1016/0092-640X(75)90023-6
1975FR18 Phys.Scr. 12, 91 (1975) W.D.Fromm, L.Funke, K.D.Schilling Lifetimes of the 11/2- Isomers in Odd-Proton N=82 Nuclei NUCLEAR REACTIONS 144Sm(d, nγ), Ba(d, xnγ), E=13.5 MeV; 141Pr(α, 2nγ), E=27 MeV; measured γ(t). 139La(α, 2nγ), E=27 MeV; measured γγ(t). 145Eu, 139La, 143Pm, 141Pr levels deduced T1/2.
doi: 10.1088/0031-8949/12/1-2/010
1974AN04 Nucl.Phys. A220, 438 (1974) W.Andrejtscheff, P.Manfrass, H.Prade, K.D.Schilling, G.Winter, H.Fuia, R.Ion-Mihai, A.B.Khalikulov, V.A.Morozov, N.Z.Marupov, T.M.Muminov Electromagnetic Transition Probabilities in Odd-Mass Erbium Isotopes RADIOACTIVITY 163,165Tm [from Ta+p, Ep=660 MeV]; measured γce- delay. 163,165Er deduced levels, T1/2. Natural target. NUCLEAR REACTIONS 161,163Dy(α, 2n), Eα=27 MeV; measured Eγ, γγ-delay. 163,165Er deduced levels, J, π, T1/2. Enriched targets.
doi: 10.1016/0375-9474(74)90127-4
1974AN11 Nucl.Phys. A225, 300 (1974) W.Andrejtscheff, P.Manfrass, K.D.Schilling, W.Seidel Electromagnetic Transitions in Some Odd-Neutron Deformed Nuclei NUCLEAR REACTIONS 155,157Gd, 177Hf(α, 2n), Eα=27 MeV; 178Hf(n, γ), E=thermal; measured αγ-, γγ-delay. 157,159Dy, 179W, 179Hf deduced levels, T1/2. Enriched targets, Ge(Li) detectors.
doi: 10.1016/0375-9474(74)90543-0
1974AN31 Izv.Akad.Nauk SSSR, Ser.Fiz. 38, 2161 (1974); Bull.Acad.Sci.USSR, Phys.Ser. 38, No.10, 125 (1974) W.H.Andrejtscheff, H.Winter, W.Seidel, P.Manfrass, H.Prade, K.D.Schilling Transition Probabilities and Band Mixing in Odd-N Deformed Nuclei NUCLEAR STRUCTURE 165Er; calculated levels, J, K, π, band-mixing.
1973SC20 Nucl.Phys. A208, 417 (1973) K.D.Schilling, W.Andrejtscheff, F.Dubbers, P.Manfrass Isomeric E1 and M1 Transitions in 177Ta and in Neighbouring Odd-A Lu and Ta Isotopes NUCLEAR REACTIONS 175Lu(α, 2nγ), Eα=27 MeV; 171,173Yb(d, 2nγ), Ed=13.5 MeV; measured αγ-, dγ-, γγ- delay. 177Ta, 171,173Lu levels deduced T1/2. Ge(Li) detectors. Natural Lu, enriched Yb targets.
doi: 10.1016/0375-9474(73)90385-0
1972AN04 Phys.Lett. 40B, 92 (1972) W.Andrejtscheff, P.Manfrass, K.-D.Schilling A Retarded E1 Transition with ΔK = 1 in 173Hf NUCLEAR REACTIONS 171Yb(α, 2nγ), E not given; measured γγ-delay. 173Hf level deduced T1/2, hindrance factor.
doi: 10.1016/0370-2693(72)90292-4
1972AN06 Nucl.Phys. A190, 489 (1972) W.Andrejtscheff, F.Dubbers, P.Manfrass, K.-D.Schilling Isomeric E1 Transitions with ΔK = 0 in 171,173Lu RADIOACTIVITY 173Hf[from 171Yb(α, 2n)]; measured Xkγ-delay. 173Lu deduced levels T1/2. Enriched targets. NUCLEAR REACTIONS 169Tm(α, 2n), Eα=27 MeV; measured αγ-, γγ-delay. 171Lu deduced levels T1/2.
doi: 10.1016/0375-9474(72)90852-4
1971AN07 Nucl.Phys. A168, 513 (1971) W.Andrejtscheff, K.-D.Schilling, F.Stary, F.Dubbers Lifetimes of Excited States in the 89-Neutron Nucleus 151Sm RADIOACTIVITY 151Pm[from 150Nd(n, γβ-)]; measured βγ-delay, γce-delay. 151Sm levels deduced T1/2. Enriched target.
doi: 10.1016/0375-9474(71)90544-6
1969AN17 Nucl.Phys. A137, 693 (1969) W.Andrejtscheff, F.Dubbers, K.-D.Schilling, F.Stary Lifetime Measurements in 187Re and 189Os RADIOACTIVITY 187W [from 186W(n, γ)]; measured βγ-delay. 189Ir[from 187Re(α, 2n)]; measured γce-delay. 187Re level deduced T1/2. 189Os level deduced T1/2, quadrupole moment.
doi: 10.1016/0375-9474(69)90103-1
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