NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = A.Pape Found 30 matches. 2010MA03 Int.J.Mod.Phys. E19, 131 (2010) A.Marinov, I.Rodushkin, D.Kolb, A.Pape, Y.Kashiv, R.Brandt, R.V.Gentry, H.W.Miller Evidence for the possible existence of a long-lived superheavy nucleus with atomic mass number A = 292 and atomic number Z ≈ 122 in natural Th ATOMIC MASSES 292122; measured masses and relative abundances using inductively coupled plasma sector field mass spectrometry; deduced superheavy nucleus with A=292, T1/2, long-lived isomeric state.
doi: 10.1142/S0218301310014662
2009MA15 Int.J.Mod.Phys. E18, 621 (2009) A.Marinov, I.Rodushkin, A.Pape, Y.Kashiv, D.Kolb, R.Brandt, R.V.Gentry, H.W.Miller, L.Halicz, I.Segal Existence of long-lived isotopes of a superheavy element in natural Au ATOMIC MASSES 261,265Rg; measured masses and relative abundances using inductively coupled plasma sector field mass spectrometry; deduced T1/2limit for isomeric states of Rg.
doi: 10.1142/S021830130901280X
2009MA19 Phys.Rev. C 79, 049802 (2009) A.Marinov, I.Rodushkin, Y.Kashiv, L.Halicz, I.Segal, A.Pape, R.V.Gentry, H.W.Miller, D.Kolb, R.Brandt Reply to "Comment on `Existence of long-lived isomeric states in naturally-occurring neutron-deficient Th isotopes'"
doi: 10.1103/PhysRevC.79.049802
2007MA57 Phys.Rev. C 76, 021303 (2007) A.Marinov, I.Rodushkin, Y.Kashiv, L.Halicz, I.Segal, A.Pape, R.V.Gentry, H.W.Miller, D.Kolb, R.Brandt Existence of long-lived isomeric states in naturally-occurring neutron-deficient Th isotopes ATOMIC MASSES 211,213,217,218Th; measured masses and relative abundances using inductively coupled plasma sector field mass spectrometry.
doi: 10.1103/PhysRevC.76.021303
2006OU02 Nucl.Instrum.Methods Phys.Res. B249, 73 (2006) S.Ouziane, A.Amokrane, I.Toumert, A.Nourreddine, A.Pape Proton induced L and L-subshell X-ray cross-sections in Sm and Yb at 1-2.5 MeV ATOMIC PHYSICS Sm, Yb(p, X), E=1-2.5 MeV; measured X-ray production σ.
doi: 10.1016/j.nimb.2006.03.082
2003MA29 Yad.Fiz. 66, 1173 (2003); Phys.Atomic Nuclei 66, 1137 (2003) A.Marinov, S.Gelberg, D.Kolb, R.Brandt, A.Pape New Outlook on the Possible Existence of Superheavy Elements in Nature
doi: 10.1134/1.1586428
2003MA81 Int.J.Mod.Phys. E12, 661 (2003) A.Marinov, S.Gelberg, D.Kolb, R.Brandt, A.Pape Coherent Description for Hitherto Unexplained Radioactivities by Super- and Hyperdeformed Isomeric States RADIOACTIVITY 271Hs, 282Fl, 316126(α); calculated α-decay T1/2 from superdeformed and hyperdeformed states.
doi: 10.1142/S0218301303001466
1998BR09 At.Data Nucl.Data Tables 69, 125 (1998) Coefficients of the Isobaric Mass Equation and Their Correlations with Various Nuclear Parameters NUCLEAR STRUCTURE A=1-59; calculated isobaric multiplets mass coefficients. ATOMIC MASSES A=1-59; calculated isobaric multiplets mass coefficients.
doi: 10.1006/adnd.1998.0773
1997AN07 At.Data Nucl.Data Tables 66, 1 (1997) Coulomb Displacement Energies between Analog Levels for 3 ≤ A ≤ 239 COMPILATION A=3-249; compiled Coulomb displacement energies.
doi: 10.1006/adnd.1997.0740
1995PA15 J.Phys.(London) G21, 237 (1995) Symmetrical Break-Ups Among Naturally Occurring Nuclides NUCLEAR STRUCTURE 174Hf, 130Ba; calculated fragment ranges in mica for breakup into 88Kr + 86Kr, 66Ni + 64Ni respectively, analytic superasymmetric fission model.
doi: 10.1088/0954-3899/21/2/010
1994NE07 Nucl.Instrum.Methods Phys.Res. B85, 123 (1994) A Study of the Ionization of Al, Si, S, Sc, Ti and V by Ar Ions in the Range 1-5 MeV NUCLEAR REACTIONS 27Al, Si, S, 45Sc, Ti, V, 31P, Cl, K, Ca(Ar, X), E=1-5 MeV; measured X-ray yields; deduced projectile, target X-ray production σ. ATOMIC PHYSICS 27Al, Si, S, 45Sc, Ti, V, 31P, Cl, K, Ca(Ar, X), E=1-5 MeV; measured X-ray yields; deduced projectile, target X-ray production σ.
doi: 10.1016/0168-583X(94)95798-3
1988AN15 At.Data Nucl.Data Tables 40, 9 (1988) Coulomb Displacement Energies between Analog Levels for 44 ≤ A ≤ 239 NUCLEAR STRUCTURE A=44-239; compiled Coulomb displacement energies.
doi: 10.1016/0092-640X(88)90003-4
1988PA14 At.Data Nucl.Data Tables 39, 201 (1988) Masses of Proton-Rich T(z) < 0 Nuclei via the Isobaric Mass Equation NUCLEAR STRUCTURE A ≤ 117; calculated T(z)<0 nuclei mass. Isobaric multiplet mass equation.
doi: 10.1016/0092-640X(88)90020-4
1988PA18 Phys.Rev. C38, 1952 (1988) A.Pape, M.S.Antony, A.Georgiadis Isovector and Isotensor Coulomb Energies for 61 ≤ A ≤ 209 NUCLEAR STRUCTURE A=61-209; calculated isovector, isotensor states; deduced corresponding Coulomb energies. Isobaric mass equation.
doi: 10.1103/PhysRevC.38.1952
1986AN07 At.Data Nucl.Data Tables 34, 279 (1986) Predicted Masses and Excitation Energies in Higher Isospin Multiplets for 9 ≤ A ≤ 60 COMPILATION A=9-60; compiled mass excesses, T≤6 isospin mutiplet level energies.
doi: 10.1016/0092-640X(86)90005-7
1986PA02 Phys.Rev.Lett. 56, 1424 (1986) Comment on ' Properties of the 208Po(0+, T=22) Double Isobaric Analog State ' NUCLEAR STRUCTURE 208Po; analyzed double IAS excitation data; deduced Coulomb energy systematics compatibility condition.
doi: 10.1103/PhysRevLett.56.1424
1985AN28 At.Data Nucl.Data Tables 33, 447 (1985) M.S.Antony, J.Britz, J.B.Bueb, A.Pape Isobaric Mass Equation for A = 1-45 and Systematics of Coulomb Displacement Energies COMPILATION A=1-45; compiled T=1/2, 1, 3/2, 2 multiplet members mass excesses; deduced isobaric multiplet mass equation coefficients, Coulomb displacement energy systematics.
doi: 10.1016/0092-640X(85)90011-7
1984AN03 Nuovo Cim. 79A, 100 (1984) M.S.Antony, J.Britz, J.B.Bueb, A.Pape Mass Defect of 39Cl from 37Cl(t, p)39Cl: Coulomb displacement energy of the T = 5/2, J(π) = (3/2)+ states in 39Cl-39Ar NUCLEAR REACTIONS 37Cl(t, p), E=3.301 keV; measured σ(Ep), σ(θ); deduced Q. 39Cl deduced ground state mass defect. 39Cl, 39Ar deduced Coulomb displacement energy.
doi: 10.1007/BF02831081
1984AN17 Nuovo Cim. 81A, 414 (1984) M.S.Anthony, J.Britz, J.Bueb, A.Pape Masses of 21F, 25Na and 29Al by (t, p) Reactions and Coulomb Displacement Energies NUCLEAR REACTIONS 19F, 23Na, 27Al(t, p), E=3.3 MeV; measured σ(Ep), Q. 21F, 25Na, 29Al deduced ground state mass defects. 21F, 21Ne, 25Na, 25Mg, 29Al, 29Si deduced Coulomb energy differences, radius parameter.
1984AN18 Phys.Rev. C30, 1286 (1984) Isobaric Mass Systematics for A ≤ 60 NUCLEAR STRUCTURE A=6-60; analyzed spectroscopic information; deduced Coulomb energy systematics, nuclear radii. 8C, 10N, 12O, 14F, 16Ne, 18Na, 20Mg, 22Al, 24Si, 26P, 28S, 30Cl, 32Ar, 34K, 36Ca, 38Sc, 40Ti, 42V, 44Cr, 46Mn, 48Fe, 50Co, 52Ni, 54Cu, 56Zn, 58Ga, 60Ge; deduced Coulomb energies. Isobaric mass multiplet equation.
doi: 10.1103/PhysRevC.30.1286
1983AN15 J.Phys.(London) G9, L245 (1983) M.S.Anthony, J.Britz, J.B.Bueb, A.Pape Mass Defect of 13B and the Isobaric Mass Equation for the A = 13 Quartet NUCLEAR REACTIONS 11B(t, p), E=3.293 MeV; measured σ(Ep) at θ=30°; deduced Q, isobaric mass multiplet equation coefficients. 13B deduced mass defect.
doi: 10.1088/0305-4616/9/11/004
1978SE08 Phys.Rev. C18, 2007 (1978) Search for Simple Configurations in 18F. II. The 17O(p, α0)14N, 17O(P, P1γ)17O, and 17O(p, γ)18F Reactions NUCLEAR REACTIONS 17O(p, α), (p, p'γ), (p, γ), E=1.4-2.8 MeV; measured σ(E, θ); deduced Q. 18F deduced levels, J, π, Γ, T1/2. Enriched target.
doi: 10.1103/PhysRevC.18.2007
1977PA14 Phys.Rev. C15, 1937 (1977) 50V Half-Life Limit RADIOACTIVITY 50V; measured EC, β T1/2.
doi: 10.1103/PhysRevC.15.1937
1977SE12 Phys.Rev. C16, 2129 (1977) J.C.Sens, S.M.Refaei, A.Ben Mohamed, A.Pape Search for Simple Configurations in 18F. I. The 17O(p, p)17O Reaction NUCLEAR REACTIONS 17O(p, p), (p, γ), (p, α), E=1.4-3.0 MeV; measured σ(E, θ). 18O resonances deduced J, π, Γp. Enriched target.
doi: 10.1103/PhysRevC.16.2129
1976PA07 Phys.Rev. C13, 2116 (1976) Radiochemical Study of the 12C(3He, 7Be) Reaction Mechanism at 30 MeV NUCLEAR REACTIONS 12C(3He, 7Be), E ≤ 31 MeV; measured σ(E, E(7Be), θ); deduced reaction mechanisms.
doi: 10.1103/PhysRevC.13.2116
1973SE02 Nucl.Phys. A199, 232 (1973) J.C.Sens, F.Rietsch, A.Pape, R.Armbruster A Spectroscopic Study of 18F (I). The 17O(p, p)17O and 17O(p, α0)14N Reactions NUCLEAR REACTIONS 17O(p, p), 17O(p, α0), E=0.50-1.33 MeV; measured σ(Ep, θ). 18F levels deduced L(p), J, π, p-width, T. Enriched gas target.
doi: 10.1016/0375-9474(73)90547-2
1973SE03 Nucl.Phys. A199, 241 (1973) J.C.Sens, A.Pape, R.Armbruster A Spectroscopic Study of 18F (II). The 17O(p, γ)18F Reaction NUCLEAR REACTIONS 17O(p, γ), E=0.440-1.440 MeV; measured σ(Ep, θ), γγ(θ), Q. 18F deduced levels J, π, level-width, T, multipole admixtures. Enriched target.
doi: 10.1016/0375-9474(73)90548-4
1972CH25 Nucl.Phys. A191, 201 (1972) A.Chevallier, E.Bozek, J.Chevallier, A.Pape, R.Armbruster Etude des Niveaux de 38Ar Formes dans la Reaction 34S(α, γ)38Ar NUCLEAR REACTIONS 34S(α, γ), E=3.6-4.8 MeV; measured σ(E, θ(γ), θ(γγ)). 38Ar levels deduced J, π, γ-width. Enriched target.
doi: 10.1016/0375-9474(72)90602-1
1971CH52 Nucl.Phys. A176, 401 (1971) A.Chevallier, E.Bozek, A.Pape, J.C.Sens, R.Armbruster, M.Langevin, J.Vernotte Etude des Niveaux du 32S Formes au Moyen de la Reaction 28Si(α, γ)32S NUCLEAR REACTIONS 28Si(α, γ), E=4.2-6.0 MeV; measured σ(E, θ), Doppler shift attenuation. 32S deduced levels, J, π, γ-width, T1/2. Enriched target.
doi: 10.1016/0375-9474(71)90278-8
1969VE01 Nucl.Phys. A124, 350(1969) J.Vernotte, M.Langevin, S.Fortier, E.Bozek, A.Chevallier, A.J.Pape, J.C.Sens Desexcitation Similaire de Deux Niveaux Voisins Formes dans la Reaction 28Si(α, γ)32S NUCLEAR REACTIONS 28Si(α, γ), E=3.753, 3.820 MeV; measured σ(Eγ, θ), γγ(θ). 32S levels deduced J, γ-mixing, γ-branching. Natural targets.
doi: 10.1016/0375-9474(69)90359-5
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