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NSR database version of April 29, 2024.

Search: Author = H.R.Kissener

Found 20 matches.

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1991GM01      Phys.Rev. C43, 1448 (1991)

M.Gmitro, O.Richter, H.R.Kissener, A.A.Ovchinnikova

Ordinary and Radiative Muon Capture on 14N

NUCLEAR REACTIONS 14N(μ-, γ), E at rest; calculated capture rates, γ-spectra vs coupling constant g(p).

doi: 10.1103/PhysRevC.43.1448
Citations: PlumX Metrics

1990GO20      Nucl.Phys. A516, 15 (1990)

N.G.Goncharova, V.J.Spevak, H.R.Kissener

1(h-bar x Omega) Multipole Excitations of the 15N Nucleus

NUCLEAR REACTIONS 15N(γ, n), (γ, p), (γ, γ'p), (γ, γ'n), E ≈ 10-20 MeV; 15N(π-, γ), E not given; calculated σ(E). 14N, 14C levels deduced Γ, Γp, Γn. 15N deduced M4 transition quenching, multipole excitation form factors. Shell model.

doi: 10.1016/0375-9474(90)90045-N
Citations: PlumX Metrics

1987GO08      Nucl.Phys. A462, 376 (1987)

A.N.Golzov, N.G.Goncharova, H.R.Kissener

Stretched M4 Configurations in 14C and 14N

NUCLEAR REACTIONS 14C, 14N(e, e'), E=196-250 MeV; calculated σ(E(e)), M4 isovector resonance energies, decay branches, partial widths, form factors. Particle-core coupling approach.

doi: 10.1016/0375-9474(87)90554-9
Citations: PlumX Metrics

1987GO09      Nucl.Phys. A462, 367 (1987)

N.G.Goncharova, A.N.Golzov, H.R.Kissener

Partial Photodisintegration Channels of 14C

NUCLEAR REACTIONS 14C(γ, n), E=40 MeV; calculated inclusive, partial σ(E), σ(En); 14C(γ, p), E ≤ 32 MeV; calculated σ(E). 14C deduced GDR branching to final states. Shell model.

doi: 10.1016/0375-9474(87)90553-7
Citations: PlumX Metrics

1983ST04      Phys.Rev. C27, 2771 (1983)

U.Straumann, M.Lebrun, C.J.Martoff, P.Truol, H.R.Kissener, J.P.Perroud, C.Joseph, W.Dahme, K.M.Crowe

M2 States in A = 15: 15N(π-, γ)15C

NUCLEAR REACTIONS 15N(π-, γ), E at rest; measured capture Eγ, Iγ. 15C deduced levels, J, π, T, giant magnetic quadrupole character. Shell model interpretation. Liquid 15NH3 target, high resolution detector.

doi: 10.1103/PhysRevC.27.2771
Citations: PlumX Metrics

1982GM02      Fiz.Elem.Chastits At.Yadra 13, 1230 (1982); Sov.J.Part.Nucl. 13, 513 (1982)

M.Gmitro, H.-R.Kissener, P.Truol, R.A.Eramzhyan

Basic Mechanisms of Radiative Capture of Pions

ATOMIC PHYSICS, Mesic-Atoms 6,7Li, 9Be, 10,11B, 12,13C, 14N, 16,18O, 19F, 20,22Ne, 23Na; compiled pion width data.

NUCLEAR REACTIONS 1,2,3H, 3,4He, 6,7Li, 9Be, 10,11B, 12,13,14C, 14N, 16,18O, 19F, 20Ne, Mg, 32S, 40Ca, 48Ti, 63Cu, 90Zr, Pb, 209Bi(π-, γ), E at rest; compiled γ yield data; deduced reaction mechanism, other processes correlation.

1980ER01      Nucl.Phys. A338, 436 (1980)

R.A.Eramzhyan, M.Gmitro, H.R.Kissener

Giant M2 and Transversal E1 Resonances in Light Nuclei

NUCLEAR REACTIONS 16O, 14N, 13,14C, 7Li, 9Be(e, e'), E=70 MeV; calculated σ(Ee'); deduced giant M2 resonance, configuration, isospin splitting. Shell model.

doi: 10.1016/0375-9474(80)90042-1
Citations: PlumX Metrics

1979DO17      J.Phys.(London) G5, L221 (1979)

G.E.Dogotar, R.A.Eramzhyan, M.Gmitro, H.R.Kissener, E.Tinkova

M2 Giant Resonance in Light Nuclei

NUCLEAR REACTIONS 7Li, 14N, 16O(e, e'), E=70 MeV; 7Li, 14N, 16O(π-, γ), E at rest; calculated σ(E(7Li')); deduced M2 giant resonance strength.

doi: 10.1088/0305-4616/5/12/001
Citations: PlumX Metrics

1979KI11      Nucl.Phys. A326, 289 (1979)

H.R.Kissener, R.A.Eramzhyan

Collective Resonances with Isospin T=2, 1 and 0 in Photoreactions, Low-q Electron Scattering and Radiative Pion Capture in A = 14 Nuclei

NUCLEAR REACTIONS 14C(e, e'), E=70 MeV; calculated σ(θ). 14C(π-, γ), E at rest; calculated yields. 13C, 13N(p, γ), E not given; calculated σ(Eγ). 14C, 14N, 14B deduced collective T=2, 1, 0 resonances.

doi: 10.1016/0375-9474(79)90395-6
Citations: PlumX Metrics

1978KI08      Nucl.Phys. A302, 523 (1978)

H.R.Kissener, G.E.Dogotar, R.A.Eramzhyan, R.A.Sakaev

Excitation of Magnetic Dipole States in 1p Shell Nuclei in Radiative Pion Capture

NUCLEAR STRUCTURE 7,6Li, 11,10B, 13,12C, 14N, 9Be; calculated B(λ).

doi: 10.1016/0375-9474(78)90338-X
Citations: PlumX Metrics

1978KI13      Nucl.Phys. A312, 394 (1978)

H.R.Kissener, G.E.Dogotar, R.A.Eramzhyan, R.A.Sakaev

Spin Dipole Excitations in Radiative Pion Capture on 1p Shell Nuclei

NUCLEAR REACTIONS 6,7Li, 9Be, 11B, 13C, 14N(π-, γ), E=at rest; calculated spin-dipole transitions. 6,7He, 9Li, 11Be, 13B, 14C resonances deduced J, π, total, partial yields.

doi: 10.1016/0375-9474(78)90599-7
Citations: PlumX Metrics

1977DO06      Nucl.Phys. A282, 474 (1977)

G.E.Dogotar, R.A.Eramzhyan, H.R.Kissener, R.A.Sakaev

Partial Transitions in Radiative Pion Capture on Light Atomic Nuclei

NUCLEAR STRUCTURE 7,6He, 13,12B, 11,10Be, 14C, 9Li; calculated partial widths from radiative pion capture.

doi: 10.1016/0375-9474(77)90071-9
Citations: PlumX Metrics

1976BA48      Yad.Fiz. 24, 508 (1976); Sov.J.Nucl.Phys. 24, 264 (1976)

H.W.Barz, I.Birke, H.U.Jager, H.R.Kissener, I.Rotter, J.Hohn

Shell-Model Calculations for the 16O + γ Reaction with and Without Allowance for the Continuous Spectrum

NUCLEAR REACTIONS 16O(γ, n), (γ, p), (γ, X), E ≤ 26 MeV; calculated σ. Shell model.

1974KI03      Nucl.Phys. A219, 601 (1974)

H.R.Kissener, A.Aswad, R.A.Eramzhian, H.U.Jager

Photodisintegration of 13C

NUCLEAR REACTIONS 13C(γ, n); calculated σ(En).

doi: 10.1016/0375-9474(74)90121-3
Citations: PlumX Metrics

1973AS02      Nucl.Phys. A208, 61 (1973)

A.Aswad, H.R.Kissener, H.U.Jager, R.A.Eramzhian

Non-Normal-Parity States in A = 7 and 8 Nuclei

NUCLEAR REACTIONS 7Li(γ, p), (γ, n), E=10-50 MeV; measured nothing, calculated σ(E). 9Be(p, 2p); measured nothing. 8Li calculated levels, S. 7Li(p, γ); measured nothing, calculated σ(Eγ). 8Be calculated levels, J, π.

doi: 10.1016/0375-9474(73)90735-5
Citations: PlumX Metrics

1973KI05      Nucl.Phys. A207, 78 (1973)

H.R.Kissener, R.A.Eramzhian, H.U.Jager

On the Decay of the Photo Resonance in 14N and 14C Nuclei

NUCLEAR REACTIONS 14N, 14C(γ, X); calculated σ(E).

doi: 10.1016/0375-9474(73)90024-9
Citations: PlumX Metrics

1973KI12      Nucl.Phys. A215, 424 (1973)

H.R.Kissener, A.Aswad, H.U.Jager, R.A.Eramzhian

Muon Capture by 14N

NUCLEAR REACTIONS 14N(μ-, ν); calculated muon capture rate. 12,13,14C calculated levels, J, π.

doi: 10.1016/0375-9474(73)90665-9
Citations: PlumX Metrics

1971JA13      Nucl.Phys. A171, 16 (1971)

H.U.Jager, H.R.Kissener, R.A.Eramzhian

Non-Normal Parity States in A = 14 and 13 Nuclei (I). Low-Lying States

NUCLEAR STRUCTURE 14N, 13N, 13C, 13N; calculated non-normal parity states, transition rates, spectroscopic amplitudes. Shell model.

doi: 10.1016/0375-9474(71)90359-9
Citations: PlumX Metrics

1971JA14      Nucl.Phys. A171, 584 (1971)

H.U.Jager, H.R.Kissener, R.A.Eramzhian

Non-Normal Parity States in A = 14 and 13 Nuclei (II). Intermediate-Energy States

NUCLEAR STRUCTURE 14N, 14C, 13C; calculated non-normal parity states, photoabsorption σ. Shell model.

doi: 10.1016/0375-9474(71)90604-X
Citations: PlumX Metrics

1970VA24      Yad.Fiz. 11, 528 (1970); Sov.J.Nucl.Phys. 11, 295 (1970)

V.A.Vartanyan, T.A.Dmitrieva, H.-U.Jager, H.R.Kissener, R.A.Eramzhyan

Partial Transitions in μ- Capture by B11 and N14

NUCLEAR REACTIONS 11B, 14N(μ-, ν), E approx o; calculated partial transition rates.

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Note: The following list of authors and aliases matches the search parameter H.R.Kissener: H.R.KISSENER, K.R.KISSENER