NSR Query Results

Output year order : Descending
Format : Normal

NSR database version of May 2, 2024.

Search: Author = A.Pape

Found 30 matches.

Back to query form


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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1998BR09      At.Data Nucl.Data Tables 69, 125 (1998)

J.Britz, A.Pape, M.S.Anthony

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
Citations: PlumX Metrics

1997AN07      At.Data Nucl.Data Tables 66, 1 (1997)

M.S.Antony, A.Pape, J.Britz

Coulomb Displacement Energies between Analog Levels for 3 ≤ A ≤ 239

COMPILATION A=3-249; compiled Coulomb displacement energies.

doi: 10.1006/adnd.1997.0740
Citations: PlumX Metrics

1995PA15      J.Phys.(London) G21, 237 (1995)

A.Pape, M.Debeauvais

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
Citations: PlumX Metrics

1994NE07      Nucl.Instrum.Methods Phys.Res. B85, 123 (1994)

M.Nekab, A.Pape, Ch.Heitz

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
Citations: PlumX Metrics

1988AN15      At.Data Nucl.Data Tables 40, 9 (1988)

M.S.Antony, J.Britz, A.Pape

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
Citations: PlumX Metrics

1988PA14      At.Data Nucl.Data Tables 39, 201 (1988)

A.Pape, M.S.Antony

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1986AN07      At.Data Nucl.Data Tables 34, 279 (1986)

M.S.Antony, J.Britz, A.Pape

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
Citations: PlumX Metrics

1986PA02      Phys.Rev.Lett. 56, 1424 (1986)

A.Pape, M.S.Antony

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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)

M.S.Antony, A.Pape

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1978SE08      Phys.Rev. C18, 2007 (1978)

J.C.Sens, S.M.Refaei, A.Pape

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
Citations: PlumX Metrics

1977PA14      Phys.Rev. C15, 1937 (1977)

A.Pape, S.M.Refaei, J.C.Sens

50V Half-Life Limit

RADIOACTIVITY 50V; measured EC, β T1/2.

doi: 10.1103/PhysRevC.15.1937
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1976PA07      Phys.Rev. C13, 2116 (1976)

A.J.Pape, S.S.Markowitz

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0627.

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
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0623.

Back to query form

Note: The following list of authors and aliases matches the search parameter A.Pape: , A.J.PAPE