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Search: Author = M.Gmitro

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1991CI08      Phys.Rev. C44, 713 (1991)

A.Cieply, M.Gmitro, R.Mach, S.S.Kamalov

Momentum-Space Method for Pionic Atoms

NUCLEAR STRUCTURE 4He, 6Li, 12,13C, 14N, 16O, 19F, 20Ne, 23Na, 24Mg, 28Si, 32S, 40Ca, 56Fe; calculated symmetrized Fermi density distribution parameters, pionic level shifts, widths. Momentum space method.

ATOMIC PHYSICS, Mesic-Atoms 4He, 6Li, 12,13C, 14N, 16O, 19F, 20Ne, 23Na, 24Mg, 28Si, 32S, 40Ca, 56Fe; calculated pionic level shifts, widths. Momentum space method.

doi: 10.1103/PhysRevC.44.713
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1991CI11      Czech.J.Phys. B41, 1091 (1991)

A.Cieply, M.Gmitro, R.Mach

Nuclear Structure Effects in Light π-Mesoatoms

NUCLEAR STRUCTURE A ≤ 50; calculated pionic level energy shifts. 19F, 20Ne, 23Na, 24Mg, 28Si, 32S, 40,44Ca; calculated charge radii. Nucleon Fermi motion contribution to pion-nucleus optical potential.

ATOMIC PHYSICS, Mesic-Atoms A ≤ 50; calculated pionic level energy shifts. Nucleon Fermi motion contribution to pion-nucleus optical potential.

doi: 10.1007/BF01598984
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1991ER06      Czech.J.Phys. B41, 1113 (1991)

R.A.Eramzhyan, M.Gmitro, S.S.Kamalov, T.D.Kaipov, H.Kissener, O.Richter

(e, e'), (γ, π+) and (π-, γ) on 12C and 13C

NUCLEAR REACTIONS 13,12C(e, e'), E not given; calculated longitudinal, transverse form factors. 12C(γ, π+), E=180, 200 MeV; 13C(γ, π+), E=200 MeV; calculated σ(θ).

doi: 10.1007/BF01598988
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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
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1990ER03      Phys.Rev. C41, 2865 (1990)

R.A.Eramzhyan, M.Gmitro, S.S.Kamalov

Momentum-Space Analysis of the Nuclear Partial Transitions in the Charged Pion Photoproduction

NUCLEAR REACTIONS 10B, 12C, 14N(γ, π+), 13C, 15N(γ, π-), E=170-320 MeV; calculated σ(θ, E). Momentum-space DWIA analysis, Fermi motion.

doi: 10.1103/PhysRevC.41.2865
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1990GM01      Nucl.Phys. A507, 707 (1990)

M.Gmitro, S.S.Kamalov, F.Simkovic, A.A.Ovchinnikova

Ordinary and Radiative Muon Capture on 12C

NUCLEAR REACTIONS 12C(μ-, γ), E at rest; calculated oridinary, radiative muon capture rate; deduced g(P)/g(A) normalization.

doi: 10.1016/0375-9474(90)90177-N
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1988ER06      J.Phys.(London) G14, 1511 (1988)

R.A.Eramzhyan, M.Gmitro, T.D.Kaipov, S.S.Kamalov, R.Mach

Pion Scattering by 6Li

NUCLEAR REACTIONS 6Li(π+, π+), (π+, π+'), E=80-260 MeV; calculated σ(E), σ(θ), vector polarization.

doi: 10.1088/0305-4616/14/12/012
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1987GM01      Nucl.Phys. A468, 404 (1987)

M.Gmitro, S.S.Kamalov, A.A.Ovchinnikova

Radiative Capture of Polarised Muons on 16O and 40Ca

NUCLEAR REACTIONS 16O, 40Ca(polarized μ-, γ), E=57-89 MeV; calculated γ CP, muon spin photon asymmetry coefficients. Modified impulse approximation.

doi: 10.1016/0375-9474(87)90174-6
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1987GM02      Phys.Rev. C36, 1105 (1987)

M.Gmitro, S.S.Kamalov, R.Mach

Momentum-Space Second-Order Optical Potential for Pion-Nucleus Elastic Scattering

NUCLEAR REACTIONS 4He, 6Li, 16O, 28Si, 40Ca(π+, π+), (π-, π-), E=14-250 MeV; calculated σ(θ); deduced model parameters mass independent nature. Optical model.

doi: 10.1103/PhysRevC.36.1105
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1987GM03      Czech.J.Phys. B37, 1107 (1987)

M.Gmitro, T.D.Kaipov, J.Kvasil, J.Rizek

Continuity Equation Constraint in the Transverse Quadrupole Electric-Type Form Factors

NUCLEAR REACTIONS 12C(e, e'), E not given; calculated form factors. Continuity equation constraint.

doi: 10.1007/BF01597028
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1987GM04      Prog.Theor.Phys.(Kyoto), Suppl. 91, 60 (1987)

M.Gmitro, S.Kamalov, R.Mach

Pion-Nucleus Scattering at Low and Resonance Energies

NUCLEAR REACTIONS 12C(π+, π+), E=14-67.5 MeV; 12C(π-, π-), E=120-226 MeV; 4He(π+, π+), E=25-98 MeV; 4He(π-, π-), E=110-220 MeV; 6Li(π+, π+), E=100-240 MeV; 16O(π+, π+), E=20-240 MeV; 28Si(π, π), E=130-226 MeV; 40Ca(π, π), E=64.8-241 MeV; calculated σ(θ). 4He, 6Li, 12C, 16O, 40Ca(π, π), E ≈ 60-320 MeV; calculated σ(E).

doi: 10.1143/PTPS.91.60
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1986GA31      Izv.Akad.Nauk SSSR, Ser.Fiz. 50, 865 (1986); Bull.Acad.Sci.USSR, Phys.Ser. 50, No.5, 32 (1986)

F.A.Gareev, M.Gmitro, S.A.Goncharov, S.N.Ershov, P.P.Korovin

An Investigation of 0+ → 0--Transitions in 16O(p, p')16O and 16O(p, n)16F Reactions

NUCLEAR REACTIONS 16O(p, p'), (p, n), (polarized p, p'), (polarized p, n), E=35, 65, 80, 135 MeV; calculated σ(θ), analyzing powers. Distorted wave method.


1986GM01      Yad.Fiz. 43, 333 (1986)

M.Gmitro, A.I.Steshenko

The Method of Generalized Hyperspherical Functions (GHFM) and Pion Scattering by 18O

NUCLEAR REACTIONS 18O(π, π'), E=29, 164, 180, 230 MeV; calculated σ(θ). Generalized hyperpherical functions.


1986GM02      Czech.J.Phys. B36, 390 (1986)

M.Gmitro, A.A.Ovchinnikova

Continuity-Equation Constraint for Electron Scattering and Radiative Muon Capture

NUCLEAR STRUCTURE 16O, 40Ca; calculated relative photon yield following radiative, ordinary muon capture. Impulse, modified impulse approximations.

doi: 10.1007/BF01597844
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1986GM03      Nucl.Phys. A453, 685 (1986)

M.Gmitro, A.A.Ovchinnikova, T.V.Tetereva

Continuity-Equation Constraint in the Two-Vertex Nuclear Processes: Radiative muon capture on 16O and 40Ca

NUCLEAR REACTIONS 16O, 40Ca(μ-, γ), E at rest; calculated muon capture rates, γ spectra; deduced (gp/g(A)). 16N, 40K levels deduced transition rates following capture. Shell model, impulse approximation.

doi: 10.1016/0375-9474(86)90257-5
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1986GM04      Czech.J.Phys. B36, 1281 (1986)

M.Gmitro, J.Kvasil, R.Lednicky, V.L.Lyuboshitz

On the Sensitivity of Nucleon-Nucleon Correlations to the Form of Short-Range Potential

NUCLEAR REACTIONS 1H(p, p), 1n(n, n), E ≤ 20 MeV/c; calculated two-nucleon generation probability ratios, wave function squares. Phenomenological, realistic potentials.

doi: 10.1007/BF01598029
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1985CH04      Phys.Lett. 150B, 50 (1985)

P.Christillin, M.Gmitro

Radiative Muon Capture on 16O

NUCLEAR REACTIONS 16O(μ-, γ), E at rest; calculated radiative capture Eγ, integrated γ yield. 16N levels deduced capture rate. Phenomenological approach.

doi: 10.1016/0370-2693(85)90135-2
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1985GA11      Yad.Fiz. 42, 20 (1985)

F.A.Gareev, M.Gmitro, S.N.Ershov, J.Cejpek

Study of the Reaction 16O(p, n)16F at E(p) = 135 MeV

NUCLEAR REACTIONS 16O(p, n), E=135 MeV; analyzed σ(θ). DWIA, direct, exchange nucleon knockout process.


1985GM01      Phys.Rev. C31, 1349 (1985)

M.Gmitro, J.Kvasil, R.Mach

Pion Elastic and Inelastic Scattering on s-d Shell Nuclei in the Δ33-Resonance Region. Coupled-Channel Analysis

NUCLEAR REACTIONS 24Mg(π+, π+), (π-, π-), (π+, π+'), (π-, π-'), E=180 MeV; 28Si(π-, π-), (π-, π-'), E=130, 180, 226 MeV; calculated σ(θ). 26Mg, 18O(π+, π-), E ≈ 100-340 MeV; calculated σ(θ) vs E. Coupled-channels model, momentum space.

doi: 10.1103/PhysRevC.31.1349
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1985KI06      Z.Phys. A320, 689 (1985)

M.Kirchbach, H.-U.Jager, M.Gmitro

Meson-Exchange Correstions to the 0+ → 0--Beta Decay of 16C

RADIOACTIVITY 16C(β-); calculated f value following β-decay; deduced meson exchange correction role. Extended shell model.

doi: 10.1007/BF01411872
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1984ER06      Nucl.Phys. A429, 403 (1984)

R.A.Eramzhyan, M.Gmitro, S.S.Kamalov, T.D.Kaipov, R.Mach

Pion Photoproduction and Inelastic Scattering in A = 12 Nuclei: Transitions to the lowest isovector 1+ and 2+ levels

NUCLEAR REACTIONS 12C(e, e'), E not given; calculated form factors. 12C(π+, π+), E=30, 87.5, 162, 226 MeV; 12C(π+, π+'), E=230, 180, 140, 100 MeV; 12C(γ, π+), E not given; calculated σ(θ). 12C(γ, π-), E not given; calculated σ vs (E(π)). Continuity equation approach.

doi: 10.1016/0375-9474(84)90689-4
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1984GM01      Yad.Fiz. 40, 107 (1984)

M.Gmitro, S.S.Kamalov, R.Mach, M.G.Sapozhnikov

Off-Shell Effects in Pion-Nucleus Elastic Scattering

NUCLEAR REACTIONS 3He(π-, π-), E=145, 98, 68 MeV; 4He(π-, π-), E=51, 110, 180 MeV; 12C(π+, π+), E=87.5, 162, 226 MeV; 16O(π+, π+), E=114, 163, 240 MeV; 24Mg(π+, π+), E=180 MeV; measured σ(θ); deduced reaction mechanism.


1983ER02      J.Phys.(London) G9, 605 (1983)

R.A.Eramzhyan, M.Gmitro, S.S.Kamalov, R.Mach

Nuclear Pion Photoproduction: A theory and the 16O(γ, π+)16N(bound) example

NUCLEAR REACTIONS 16O(γ, π+), E=150-300 MeV; calculated photoproduction σ(θ), σ(E). Momentum space formulation, Fermi motion, relativistic, gauge invariance, multiple rescattering effects.

doi: 10.1088/0305-4616/9/6/006
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1983ER06      Phys.Lett. 128B, 371 (1983)

R.A.Eramzhyan, M.Gmitro, S.S.Kamalov

Pion Photoproduction Off Nuclei: A sensitive test of the nuclear transition densities

NUCLEAR REACTIONS 16O(γ, π+), E=220-350 MeV; calculated σ(θ) vs E. Electron scattering data input, DWIA approach.

doi: 10.1016/0370-2693(83)90918-8
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1983GM01      Nucl.Phys. A399, 503 (1983)

M.Gmitro, A.A.Ovchinnikova

Elementary-Particle Treatment of the Radiative Muon Capture in 12C

NUCLEAR REACTIONS 12C(μ-, γ), E at rest; calculated radiative capture γ-spectrum; deduced weak form factor role on capture rate enhancement. 12B level deduced branching ratio estimate. Elementary particle treatment, possible nonzero neutrino mass.

doi: 10.1016/0375-9474(83)90260-9
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1982GM01      Phys.Lett. 113B, 205 (1982)

M.Gmitro, J.Kvasil, R.Mach

Elastic and Inelastic Scattering of 180 MeV π(±) on 24Mg

NUCLEAR REACTIONS 24Mg(π-, π-), (π+, π+), (π+, π+'), E=180 MeV; calculated σ(θ). Coupled-channels method, momentum space.

doi: 10.1016/0370-2693(82)90821-8
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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.


1981ER05      J.Phys.(London) G7, L231 (1981); Corrigendum J.Phys.(London) G8, 595 (1982)

R.A.Eramzhyan, M.Gmitro, S.S.Kamalov, G.V.Micelmacher, J.Rizek

A Method to Determine the Muon-Neutrino Mass

NUCLEAR REACTIONS 16O(μ-, γ), E at rest; calculated relative γ-yield, branching ratio; 12C, 31P(μ-, γ), E at rest; calculated branching ratio; deduced neutrino mass upper limit. Radiative capture, impulse approximation.

doi: 10.1088/0305-4616/7/10/004
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1981GM01      Nucl.Phys. A356, 323 (1981)

M.Gmitro, A.A.Ovchinnikova

Current Divergences, Pion Photoproduction and Radiative Muon Capture

NUCLEAR REACTIONS 1H, 3He(μ-, γ), E at rest; calculated σ(Eγ) vs photon momentum. Coupling equations, weak, electromagnetic off-mass-shell contributions to radiative capture amplitude.

doi: 10.1016/0375-9474(81)90193-7
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1981GM02      Czech.J.Phys. B31, 499 (1981)

M.Gmitro, S.S.Kamalov, T.V.Moskalenko, R.A.Eramzhyan

Radiative Muon Capture on Nuclei. Microscopic Calculation for 16O and 40Ca

NUCLEAR REACTIONS 16O, 40Ca(μ-, γ), E at rest; calculated Eγ, CP; deduced sensitivity to induced pseudoscalar coupling constant. Shell model.

doi: 10.1007/BF01596416
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1981GM03      J.Phys.(London) G7, 1203 (1981)

M.M.Gmitro, G.Ya.Korenman, V.P.Popov, R.A.Sakaev, L.A.Tosunjan

Gauge Invariance and Nucleonic Fermi Motion in Radiative Pion Capture on 16O

NUCLEAR REACTIONS 16O(π-, γ), E at rest; calculated σ(Eγ), capture rates, branching ratios. Gauge invariant effective Hamiltonian, Fermi motion effects.

doi: 10.1088/0305-4616/7/9/012
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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
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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
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1979ER07      Czech.J.Phys. B29, 370 (1979)

R.A.Eramzhyan, M.Gmitro, L.A.Tosunjan

One- and Two-Nucleon Emission Following the Nuclear Radiative Pion Capture

NUCLEAR REACTIONS 16O(π-, γ), (π-, nγ), (π-, 2nγ), (π-, npγ), (μ-, νn), E=at rest; calculated σ(Eγ), σ(En), branching ratios, two nucleon yields. Shell model, R-matrix formalism.

doi: 10.1007/BF01596546
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1979GM01      Z.Phys. A290, 179 (1979)

M.Gmitro, R.Mach

Coupled Channel Method for the π-4He Elastic and Inelastic Scattering

NUCLEAR REACTIONS 4He(π-, π-), (π-, π-'), E=40-75 MeV; calculated σ. Coupled-channel method in momentum space, K-matrix approach.

doi: 10.1007/BF01408113
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1979GM02      Czech.J.Phys. B29, 155 (1979); Erratum Czech.J.Phys. B29, 1308 (1979)

M.Gmitro, E.Tinkova, A.Rimini, T.Weber

Positive Parity Giant Multipole Resonances in 16O

NUCLEAR STRUCTURE 16O; calculated T=0, 1, GMR strength distribution for positive pariy J=0 to 4 states. Shell model n particle-n hole.

doi: 10.1007/BF01957544
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1979GM03      Yad.Fiz. 30, 330 (1979); Sov.J.Nucl.Phys. 30, 171 (1979)

M.Gmitro, A.A.Ovchinnikova

Probability of μe Conversion in the Reaction 16O(μ-, e-)16O*

NUCLEAR REACTIONS 16O(μ-, e-), E at rest; calculated excitation probability of giant resonances. Shell model, 2p-2h correlations.


1978ER04      J.Phys.(London) G4, L233 (1978)

R.A.Eramzhyan, M.Gmitro, L.A.Tosunjan

What New Information May the Coincidence Spectra of the Nuclear Radiative Pion Capture Provide (Question)

NUCLEAR REACTIONS 16O(π-, nγ); calculated reaction parameters.

doi: 10.1088/0305-4616/4/9/004
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1977AL15      Nuovo Cim. 38A, 239 (1977)

G.Alberi, M.Gmitro, L.Hambro

Proton and Electron Inelastic Scattering and the Shell Model for 12C

NUCLEAR REACTIONS 12C(p, p'), E=1.04 GeV; calculated form-factor, σ.

doi: 10.1007/BF02730022
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1977ER04      Nucl.Phys. A290, 294 (1977)

R.A.Eramzhyan, M.Gmitro, R.A.Sakaev, L.A.Tosunjan

Towards a Better Understanding of 16O Nuclear Structure: Muon Capture and Radiative Pion Capture Reactions

NUCLEAR REACTIONS 16O(μ-, γ), (π-, γ); calculated muon, pion capture rates; deduced excitation in 16N.

doi: 10.1016/0375-9474(77)90438-9
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1977GM01      Lett.Nuovo Cim. 20, 449 (1977)

M.Gmitro, E.Tinkova, A.Rimini, T.Weber

Spreading of the Giant Quadrupole Resonance in 16O

NUCLEAR STRUCTURE 16O; calculated distribution of isoscalar GQR.

doi: 10.1007/BF02783557
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1976FO11      Nucl.Phys. A267, 395 (1976)

V.N.Folomeshkin, S.S.Gershtein, M.Y.Khlopov, M.Gmitro, R.A.Eramzhyan, L.A.Tosunjan

Possible Tests of Neutral-Current Models in the Neutrino Excitation of Light Atomic Nuclei

NUCLEAR REACTIONS 16O(μ-, X); calculated muon capture rate to levels in 16N. Neutral-current models.

doi: 10.1016/0375-9474(76)90668-0
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1976TI03      Phys.Rev. C14, 1213 (1976)

E.Tinkova, M.Gmitro

Random-Phase-Approximation Ground-State Correlations and the Isotope Effect in the 40Ca and 48Ca

NUCLEAR STRUCTURE 40,48Ca; calculated spectra, shell breaking, rms radii, density distributions. Ground-state correlations, isospin projection.

doi: 10.1103/PhysRevC.14.1213
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1974GM02      Nuovo Cim. 21A, 11 (1974)

M.Gmitro, A.Rimini, T.Weber

The Role of the 4p-4h Excitations in the Microscopic Description of 56Ni

NUCLEAR STRUCTURE 56Ni; calculated levels.

doi: 10.1007/BF02731184
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1973GM01      Nuovo Cim. 13A, 526 (1973)

M.Gmitro, A.Rimini, T.Weber

On the n-n and n-p Effective Interactions for 1f7/2 Protons and (2p, 1f5/2) Neutrons

NUCLEAR STRUCTURE 58,59,60Ni, 56,57Co, 55,56Fe, 54,55Mn, 53,54Cr; calculated levels, rms radii.

doi: 10.1007/BF02827353
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1971GM01      Phys.Rev. C4, 1239 (1971)

E.Gmitrova, M.Gmitro, Y.K.Gambhir

Structure of the Random-Phase-Approximation Ground-State Wave Functions of 56Ni and 48Ca

NUCLEAR STRUCTURE 48Ca, 56Ni; calculated levels, occupation numbers. RPA, Tabakin potentials.

doi: 10.1103/PhysRevC.4.1239
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1970BO43      Phys.Lett. 33B, 553 (1970)

A.Boiti, M.Gmitro, A.Rimini, T.Weber

On a Completely Microscopic Description of the 2p-1f Shell Nuclei

NUCLEAR STRUCTURE 56Ni; calculated levels. Tamm-Dancoff, 2p-2h approximations.

doi: 10.1016/0370-2693(70)90346-1
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1970GM01      Phys.Rev. C1, 1801 (1970)

M.Gmitro, A.Rimini, P.Rossi, T.Weber

Comparison between the Quasiparticle Tamm-Dancoff and Random-Phase Approximations in Even Tin Isotopes Using Realistic Interactions

NUCLEAR STRUCTURE 116,120Sn; calculated levels. Quasiparticle Tamm-Dancoff, random phase approximations; realistic interactions.

doi: 10.1103/PhysRevC.1.1801
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1970GM02      Phys.Rev. C2, 356 (1970)

M.Gmitro, M.Sotona

Brueckner Reaction Matrix and Separable Potentials

NUCLEAR STRUCTURE 4He, 16O; calculated binding energy. Reaction matrix elements of Tabakin potential.

doi: 10.1103/PhysRevC.2.356
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1969AL08      Phys.Rev. 182, 1308 (1969)

R.Alzetta, T.Weber, Y.K.Gambhir, M.Gmitro, J.Sawicki, A.Rimini

Improved Inverse Gap Equation and Quasiparticle Theories of Odd and Even Tin Isotopes

NUCLEAR STRUCTURE 115,116,117,118,119,120,121Sn; calculated levels, S for (d, p), (p, d), (d, t), (p, t) reactions. Quasiparticle theory, inverse gap equation.

doi: 10.1103/PhysRev.182.1308
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1969AL16      Phys.Rev. 185, 1233 (1969)

R.Alzetta, A.Rimini, T.Weber, M.Gmitro, J.Sawicki

Effective N-N Interaction and Electromagnetic Operators Deduced from the Tabakin Potential: Application to Nickel Isotopes

NUCLEAR STRUCTURE 58,59,60,61,62,63,64Ni; calculated levels, B(E2), B(M1). Second Tamm-Dancoff theory, Tabakin potential.

doi: 10.1103/PhysRev.185.1233
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1969GA21      Phys.Letters 30B, 382 (1969)

Y.K.Gambhir, E.Gmitrova, M.Gmitro

Is the 56Ni Nucleus Doubly Magic

NUCLEAR STRUCTURE 56,58,60,62,64Ni; calculated levels. Number - projected BCS wave functions, realistic nucleon-nucleon potentials.

doi: 10.1016/0370-2693(69)90465-1
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1969SO11      Phys.Rev. 185, 1448 (1969)

M.Sotona, M.Gmitro, Z.Pluhar, L.Trlifaj

A = 21 Nuclei in the SU3

NUCLEAR STRUCTURE 21Ne, 21Na; calculated levels. SU(3) model.

doi: 10.1103/PhysRev.185.1448
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1968GM01      Phys.Letters 26B, 252 (1968)

M.Gmitro, J.Hendekovic, J.Sawicki

Core Polarisation and Quasiparticle Theories of Even Tin Isotopes with a Realistic Nucleon-Nucleon Force

doi: 10.1016/0370-2693(68)90550-9
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1968GM02      Phys.Letters 26B, 493 (1968)

M.Gmitro, J.Sawicki

Energy Spectrum of 116Sn and Effective Nuclear Forces Derived from the Realistic Nucleon-Nucleon Potentials of Yale and of Tabakin

NUCLEAR STRUCTURE 116Sn; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(68)90360-2
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1968GM03      Phys.Rev. 169, 983 (1968)

M.Gmitro, J.Hendekovic, J.Sawicki

Core Polarization and Quasiparticle Theories of Vibrational Nuclei with a Realistic Nucleon-Nucleon Force

doi: 10.1103/PhysRev.169.983
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1968GM04      Phys.Letters 27B, 616 (1968)

M.Gmitro

Effective Nuclear Force of a Realistic Potential: A Selfconsistent Approach

doi: 10.1016/0370-2693(68)90294-3
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1968GM05      Phys.Rev. 175, 1243 (1968)

M.Gmitro, A.Rimini, J.Sawicki, T.Weber

Microscopic Theory of Effective Operators for Electromagnetic Interactions in Nuclei

doi: 10.1103/PhysRev.175.1243
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1966TR02      Nucl.Phys. 86, 681 (1966)

L.Trlifaj, M.Gmitro, M.Sotona

Level Structure of Oxygen Isotopes in the SU3 Scheme

NUCLEAR STRUCTURE 20O, 18O; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(66)90507-4
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