NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = M.V.Mebel Found 22 matches. 2005BO10 J.Radioanal.Nucl.Chem. 264, 101 (2005) M.L.Bonardi, F.Groppi, H.S.Mainardi, V.M.Kokhanyuk, E.V.Lapshina, M.V.Mebel, B.L.Zhuikov Cross section studies on 64Cu with zinc target in the proton energy range from 141 down to 31 MeV NUCLEAR REACTIONS Zn(p, X)64Cu/57Ni/56Ni/52Mn/54Mn/62Zn/65Zn/51Cr/48V/55Co/56Co/57Co/58Co/60Co/66Ga/67Ga/52Fe/59Fe, E ≈ 31-141 MeV; measured production σ. Stacked-foil activation.
doi: 10.1007/s10967-005-0681-1
2003ZH39 Phys.Rev. C 68, 054611 (2003) B.L.Zhuikov, M.V.Mebel, V.M.Kokhanyuk, A.S.Iljinov, A.Yu.Zyuzin, J.S.Vincent Production of high-spin isomers in proton induced reactions at 100-500 MeV on 181Ta NUCLEAR REACTIONS 181Ta(p, xnyp)178mTa/180mHf/177mLu/179mHf/177mHf, E=100-500 MeV; measured high-spin isomer production σ, isomer ratios vs spin; deduced reaction mechanism features. Radiochemical separation.
doi: 10.1103/PhysRevC.68.054611
2001IL04 Yad.Fiz. 64, No 8, 1463 (2001); Phys.Atomic Nuclei 64, 1386 (2001) Induced Nuclear Fission Accompanied by Pion Emission NUCLEAR REACTIONS 238U(p, F), E=150-600 MeV; calculated σ for pion-accompanied fission, pion spectra and angular distributions, fragment mass distributions.
doi: 10.1134/1.1398930
1997ME28 Nucl.Instrum.Methods Phys.Res. A398, 324 (1997) M.V.Mebel, A.S.Iljinov, C.Grandi, G.Reffo, M.Blann Analysis of Isotope Yields and Excitation Functions for Fissile and Non-Fissile Nuclei with CEF and HMS-ALICE Codes NUCLEAR REACTIONS 58,62Ni(p, X), E=80-1000 MeV; 209Bi, 232Th, 238U(p, X), E=150-1800 MeV; calculated fragments isotopic yields. Comparison of computer codes. Comparison with data.
doi: 10.1016/S0168-9002(97)00779-1
1997SC10 Phys.Rev. C55, 2965 (1997) W.Schmid, T.von Egidy, F.J.Hartmann, J.Hoffmann, S.Schmid, D.Hilscher, D.Polster, H.Rossner, A.S.Iljinov, M.V.Mebel, D.I.Ivanov, V.G.Nedorezov, A.S.Sudov, H.Machner, H.S.Plendl, J.Eades, S.Neumaier Neutrons in Coincidence with Fission of 238U Induced by Stopped Antiprotons NUCLEAR REACTIONS 238U(p-bar, F), E at rest; measured fission fragment mass, energy, En, n(fragment)-coin; deduced pre-, post-scission neutron multiplicities. Compound with cascade-evaporation model calculations, dissipative effects in fission.
doi: 10.1103/PhysRevC.55.2965
1997SC27 Z.Phys. A359, 27 (1997) S.Schmid, W.Schmid, F.J.Hartmann, T.von Egidy, D.Hilscher, W.Bohne, P.Figuera, F.Goldenbaum, U.Jahnke, D.Polster, P.Ziem, J.Galin, B.Lott, M.Morjean, A.Peghaire, B.Quednau, K.Gulda, J.Jastrzebski, W.Kurcewicz, L.Pienkowski, G.Pausch, J.Eades, A.S.Iljinov, M.V.Mebel Probability of Fission Induced by 1.2 GeV Antiprotons NUCLEAR REACTIONS 238U, 232Th, 209Bi, 197Au, 165Ho, 119Sn, Ag, 100Mo, 89Y, Cu(p-bar, F), E=1.2 GeV; measured annihilation σ, absolute fission probability vs fragment mass, neutron multiplicity, fission fragment folding angle distributions. Monte Carlo calculations. 4π neutron, particle detectors.
doi: 10.1007/s002180050363
1996KI19 Phys.Rev. C54, 2469 (1996) Y.S.Kim, A.S.Iljinov, M.V.Mebel, P.Hofmann, H.Daniel, T.von Egidy, T.Haninger, F.J.Hartmann, H.Machner, H.S.Plendl, G.Riepe Fission of Heavy Nuclei Induced by Stopped Antiprotons. II. Correlations between Fission Fragments NUCLEAR REACTIONS 238U, 232Th, 209Bi(p-bar, F), E at rest; measured fission(fragment)(fragment)-coin, mass, energy, velocity, folding angle total kinetic energy, momentum, mass loss of fissioning nucleus; deduced correlations between measured quantities, mass loss before and after scission. Intranuclear cascade, evaporation calculations including fission channel.
doi: 10.1103/PhysRevC.54.2469
1995IV01 Z.Phys. A352, 191 (1995) D.I.Ivanov, A.S.Iljinov, M.V.Mebel, V.G.Nedorezov, A.S.Sudov, A.A.Turinge, T.von Egidy, S.Schmid, W.Schmid, H.Rossner, J.Eades Fission Probabilities of Cu, Nb, Ag, Ho, Au and Bi Nuclei Excited by Stopped Antiprotons NUCLEAR REACTIONS Cu, 93Nb, Ag, Ho, 197Au, 209Bi(p-bar, F), E at rest; measured fission probability; deduced fissility minimum near A=100. Liquid drop model interpretation, other data included.
doi: 10.1007/BF01298907
1995VO14 Z.Naturforsch. 50a, 1077 (1995) T.von Egidy, F.J.Hartmann, S.Schmid, W.Schmid, K.Gulda, J.Jastrzebski, W.Kurcewicz, P.Lubinski, L.Pienkowski, A.Trzcinska, D.Hilscher, W.Bohne, F.Goldenbaum, U.Jahnke, D.Polster, H.Rossner, A.S.Iljinov, D.I.Ivanov, M.V.Mebel, V.G.Nedorezov, A.S.Sudov, J.Eades, S.Neumaier Nuclear Physics with Antiprotons NUCLEAR REACTIONS 197Au(p-bar, X), E at rest; 197Au(p-bar, X), E=1.2 GeV; 197Au(p, X), E=1, 6 GeV; compiled, reviewed residuals yields vs mass number. 234U(p-bar, F), E at rest; 234U(p-bar, F), E=fast; measured neutron spectra following fission; deduced absolute fission probabilities.
1994AN40 J.Alloys and Compounds 213/214, 460 (1994) N.V.Antonenko, E.A.Cherepanov, A.S.Iljinov, M.V.Mebel Production of heavy actinides in incomplete fusion reactions NUCLEAR REACTIONS 248Cm(18O, X), E not given; calculated relative yields for Z=98-100 fragments. 248Cm(18O, X)251Fm/252Fm/253Fm/254Fm/255Fm/256Fm/257Fm, E not given; calculated production σ. Phenomenological model.
doi: 10.1016/0925-8388(94)90961-X
1994HO08 Phys.Rev. C49, 2555 (1994) P.Hofmann, A.S.Iljinov, Y.S.Kim, M.V.Mebel, H.Daniel, P.David, T.von Egidy, T.Haninger, F.J.Hartmann, J.Jastrzebski, W.Kurcewicz, J.Lieb, H.Machner, H.S.Plendl, G.Riepe, B.Wright, K.Ziock Fission of Heavy Nuclei Induced by Stopped Antiprotons. I. Inclusive Characteristics of Fission Fragments NUCLEAR REACTIONS 238U, 232Th, 209Bi(p-bar, F), E at rest; measured fission fragment energy, mass, θ; deduced fission fragment total mass, total momentum. Intranuclear cascade, evaporation, fission models.
doi: 10.1103/PhysRevC.49.2555
1994IL03 Yad.Fiz. 57, No 7, 1286 (1994); Phys.Atomic Nuclei 57, 1218 (1994) A.S.Iljinov, M.V.Mebel, H.Daniel, T.von Egidy, F.J.Hartmann, P.Hofmann, Y.S.Kim Antiproton-Induced Nuclear Fission NUCLEAR REACTIONS 209Bi, 238U, 232Th(p-bar, F), E at rest; calculated fission fragment total mass distributions; deduced (p-bar)A annihilation role in fission. Dynamical model including all fission stages.
1994SC07 Nucl.Phys. A569, 689 (1994) W.Schmid, P.Baumann, H.Daniel, T.von Egidy, F.J.Hartmann, P.Hofmann, Y.S.Kim, H.H.Schmidt, A.S.Iljinov, M.V.Mebel, D.Hilscher, D.Polster, H.Rossner Absolute Probabilities of Fission Induced by Stopped Antiprotons NUCLEAR REACTIONS U, 232Th, 197Au, 165Ho(p-bar, X), E at rest; measured absolute fission probabilities, fission(fragment)(fragment)-coin; deduced absolute fission probabilities. Intranuclear cascade model. In-beam semiconductor detector (pin-diode).
doi: 10.1016/0375-9474(94)90380-8
1993BI16 Phys.Rev. C48, 1785 (1993) N.Bianchi, A.Deppman, E.De Sanctis, A.Fantoni, P.Levi Sandri, V.Lucherini, V.Muccifora, E.Polli, A.R.Reolon, P.Rossi, A.S.Iljinov, M.V.Mebel, J.D.T.Arruda-Neto, M.Anghinolfi, P.Corvisiero, G.Gervino, L.Mazzaschi, V.Mokeev, G.Ricco, M.Ripani, M.Sanzone, M.Taiuti, A.Zucchiatti, R.Bergere, P.Carlos, P.Garganne, A.Lepretre Photofissility of 232Th Measured with Tagged Photons from 250 to 1200 MeV NUCLEAR REACTIONS 232Th(γ, F), E=250-1200 MeV; measured photofission σ(E). 232Th deduced photofissility. Tagged photons, parallel plate avalanche detector.
doi: 10.1103/PhysRevC.48.1785
1993VO06 Nucl.Phys. A558, 383c (1993) T.von Egidy, H.Daniel, F.J.Hartmann, P.Hofmann, Y.S.Kim, W.Schmid, H.H.Schmidt, G.Riepe, H.Machner, P.David, H.S.Plendl, A.S.Iljinov, A.S.Botvina, Ye.S.Golubeva, M.V.Mebel, J.Jastrzebski, W.Kurcewicz Antiproton Induced Fission NUCLEAR REACTIONS 209Bi, 232Th, 238U(p-bar, F), E at 105 MeV/c; measured fission fragment mass yield distributions; deduced absolute fission probabilities.
doi: 10.1016/0375-9474(93)90407-O
1992IL02 Nucl.Phys. A539, 263 (1992) A.S.Iljinov, D.I.Ivanov, M.V.Mebel, V.G.Nedorezov, A.S.Sudov, R.Ya.Kezerashvili Fissilities of 238U and 237Np Nuclei Measured with Tagged Photons in the Energy Range 60-240 MeV NUCLEAR REACTIONS 238U, 237Np(γ, F), E=60-240 MeV; measured photon-induced fission σ, fissilities. Cascade evaporation, double-humped barrier model analyses. Natural, enriched targets, tagged photons.
doi: 10.1016/0375-9474(92)90270-T
1992IL04 Nucl.Phys. A543, 517 (1992) A.S.Iljinov, M.V.Mebel, N.Bianchi, E.De Sanctis, C.Guaraldo, V.Lucherini, V.Muccifora, E.Polli, A.R.Reolon, P.Rossi Phenomenological Statistical Analysis of Level Densities, Decay Widths and Lifetimes of Excited Nuclei NUCLEAR STRUCTURE A=20-253; analyzed level densities, decay width, T1/2 data; deduced level density parameters. Phenomenological statistical model.
doi: 10.1016/0375-9474(92)90278-R
1990GU05 Nuovo Cim. 103A, 607 (1990) C.Guaraldo, V.Lucherini, E.De Sanctis, A.S.Iljinov, M.V.Mebel, S.Lo Nigro Excitation Energy Dependence of Photofissility in Preactinide Nuclei NUCLEAR STRUCTURE 197Au, 209Bi; calculated photon-induced fission features, fissility vs excitation energy. Intranuclear cascade model. NUCLEAR REACTIONS 197Au, 209Bi(γ, F), E ≈ 100-300 MeV; calculated photon-induced fission features, fissility vs excitation energy. Intranuclear cascade model.
doi: 10.1007/BF02820532
1989IL01 Phys.Rev. C39, 1420 (1989) A.S.Iljinov, M.V.Mebel, C.Guaraldo, V.Lucherini, E.De Sanctis, N.Bianchi, P.Levi Sandri, V.Muccifora, E.Polli, A.R.Reolon, P.Rossi, S.Lo Nigro Comparison of Fission of Heavy Nuclei Induced by Different Probes NUCLEAR REACTIONS 197Au, 209Bi, U(γ, F), E=200 MeV; 197Au, 209Bi, U(γ, F), E=190 MeV; 197Au, 209Bi, U(π, F), E=80 MeV; analyzed fission data; deduced fissility parameters. Monte Carlo cascade calculations.
doi: 10.1103/PhysRevC.39.1420
1989LU01 Phys.Rev. C39, 911 (1989) V.Lucherini, C.Guaraldo, E.De Sanctis, P.Levi Sandri, E.Polli, A.R.Reolon, A.S.Iljinov, S.Lo Nigro, S.Aiello, V.Bellini, V.Emma, C.Milone, G.S.Pappalardo, M.V.Mebel Au Photofission Cross Section by Quasimonochromatic Photons in the Intermediate Energy Region NUCLEAR REACTIONS 197Au(γ, F), E=100-300 MeV; measured fission yields; deduced fission σ(E), nuclear fissility. Monchromatic photons.
doi: 10.1103/PhysRevC.39.911
1983CH21 J.Phys.(London) G9, 931 (1983) E.A.Cherepanov, A.S.Iljinov, M.V.Mebel Systematics of the Effective Ratio < Γn/Γf > of Neutron Emission and Fission Partial Widths for Transcurium Nuclei NUCLEAR STRUCTURE A ≈ 245-270; analyzed < Γn >/< ΓF >, neutron binding energy, fission barrier systematics. Statistical, liquid drop model, (HI, xn) reaction data input.
doi: 10.1088/0305-4616/9/8/015
1983CH37 J.Phys.(London) G9, 1397 (1983) E.A.Cherepanov, A.S.Iljinov, M.V.Mebel The Energy Dependence of the Neutron Emission-to-Fission Ratio Γ(n)/Γ(f) for Transuranium Nuclei NUCLEAR STRUCTURE 239Pu, 244Cm, 247Bk, 248Cf, 256Md, 258No; analyzed heavy ion induced reaction data; deduced neutron emission probability vs excitation energy, neutron emission, fission partial width ratio, liquid drop, double-humped fission barriers.
doi: 10.1088/0305-4616/9/11/012
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