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Search: Author = I.Borbely

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2003DO05      Phys.Rev. C 67, 064005 (2003)

P.Doleschall, I.Borbely, Z.Papp, W.Plessas

Nonlocality in the nucleon-nucleon interaction and three-nucleon bound states

NUCLEAR STRUCTURE 3H, 3He; calculated binding energies, effect of nonlocal nucleon-nucleon interaction. Comparison with data.

doi: 10.1103/PhysRevC.67.064005
Citations: PlumX Metrics

2001DO06      Nucl.Phys. A684, 557c (2001)

P.Doleschall, I.Borbely

Phenomenological Nonlocal NN Interactions

doi: 10.1016/S0375-9474(01)00393-1
Citations: PlumX Metrics

2000DO23      Phys.Rev. C62, 054004 (2000)

P.Doleschall, I.Borbely

Properties of the Nonlocal NN Interactions Required for the Correct Triton Binding Energy

NUCLEAR STRUCTURE 2H; calculated binding energy, radius. 3H; calculated binding energy, dependence on deuteron D-state probability. Nonlocal interactions.

doi: 10.1103/PhysRevC.62.054004
Citations: PlumX Metrics

1999DO35      Few-Body Systems 27, 1 (1999)

P.Doleschall, I.Borbely

Phenomenological Non-Local Nucleon-Nucleon Interactions and the Neutron-Deuteron Break-Up Process

NUCLEAR REACTIONS 2H(n, np), E=10.5, 13, 19 MeV; calculated σ(θ), analyzing powers; deduced sensitivity to nucleon-nucleon interaction features. Phenomenological non-local interactions, comparisons with data.

doi: 10.1007/s006010050120
Citations: PlumX Metrics

1992BO12      Phys.Lett. 283B, 19 (1992)

I.Borbely, P.Doleschall

Nucleon Exchange Effects at Low Bombarding Energies for Deuteron-Neutron Scattering

NUCLEAR REACTIONS 2H(n, n), E=low; calculated quartet scattering amplitude; deduced nucleon exchange mechanism role.

doi: 10.1016/0370-2693(92)91418-9
Citations: PlumX Metrics

1990KA17      Z.Phys. A336, 297 (1990)

Sh.S.Kayumov, A.M.Mukhamedzhanov, R.Yarmukhamedov, I.Borbely

Three-Body Coulomb Effects in One-Particle Transfer Reactions

NUCLEAR REACTIONS 2,1H, 3He(d, p), E=1-45 MeV; 2H(3He, d), E=3-35 MeV; 2H(6Li, d), E=10-100 MeV; 9Be(3He, d), E=15-75 MeV; 11B(12C, 11B), E=10-100 MeV; 12C(12C, 11B), E=45-150 MeV; 12C(30P, 29Si), 53Fe(13N, 12C), E=75-150 MeV; calculated Coulomb normalization factors, parameters.

1989BO22      Yad.Fiz. 49, 1309 (1989)

I.Borbely, Sh.S.Kayumov, A.M.Mukhamedzhanov, R.Yarmukhamedov

On Coulomb Renormalization of Pole Singularity of Neutron-Transfer-Reaction Amplitude

NUCLEAR REACTIONS 1,2H, 3He(d, p), E=1-45 MeV; calculated σ(θ) pole residue related Coulomb renormalization factor.

1989BO26      Yad.Fiz. 50, 64 (1989)

I.Borbely, Sh.S.Kayumov, A.M.Mukhamedzhanov, R.Yarmukhamedov

On Coulomb Renormalization of Pole Singularity of Charged-Particle-Transfer-Reaction Amplitude

NUCLEAR REACTIONS 2H(3He, d), E=3-35 MeV; 2H(6Li, d), E=10-100 MeV; 9Be(3He, d), E=15-75 MeV; 11B(12C, 11B), E=10-100 MeV; 12C(12C, 11B), E=45-150 MeV; calculated reaction amplitudes. DWBA, pole mechanism near singularity.

1989BO32      Nucl.Phys. A503, 349 (1989)

I.Borbely, W.Gruebler, B.Vuaridel, V.Konig

Empirical Continuation of Polarization Observables to the Transfer Pole for the Determination of the Deuteron D- to S-State Asymptotic Normalization

NUCLEAR REACTIONS 2H(polarized d, p), E ≈ 5.5-13 MeV; 1H(polarized d, p), E=10 MeV; analyzed polarization observables data. 2H deduced D- to S-state asymptotic normalization. Empirical continuation techniques.

doi: 10.1016/0375-9474(89)90240-6
Citations: PlumX Metrics

1989VU01      Nucl.Phys. A499, 429 (1989)

B.Vuaridel, W.Gruebler, V.Konig, K.Elsener, P.A.Schmelzbach, M.Bittcher, D.Singy, I.Borbely, M.Bruno, F.Cannata, M.D'Agostino

New Constraints on D-State Contributions to the Trinucleon Wave Functions

NUCLEAR REACTIONS 4He(polarized d, 3He), E=32.21-49.7 MeV; measured σ(θ, E), analyzing power vs θ. 3H, 3He deduced ratios of the D- to S-state asymptotic normalization.

doi: 10.1016/0375-9474(89)90538-1
Citations: PlumX Metrics

1988VU01      Nucl.Phys. A484, 34 (1988)

B.Vuaridel, W.Gruebler, V.Konig, K.Elsener, P.A.Schmelzbach, J.Ulbricht, Ch.Forstner, M.Bittcher, D.Singy, M.Bruno, F.Cannata, M.D'Agostino, I.Borbely

Experimental Investigation of Charge Symmetry Breaking Effects in the Reaction 4He(d(pol), 3He)3H between E(d) = 32 and 50 MeV

NUCLEAR REACTIONS 4He(polarized d, 3He), E=32.1-49.7 MeV; measured σ(θ), σ(E), vector, tensor analyzing powers vs θ; deduced charge symmetry breaking effects.

doi: 10.1016/0375-9474(88)90139-X
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0074.

1987VU01      Helv.Phys.Acta 60, 776 (1987)

B.Vuaridel, W.Gruebler, V.Konig, P.A.Schmelzbach, I.Borbely

New Approach for the Determination of the Deuteron D to S State Asymptotic Normalization

NUCLEAR REACTIONS 2H(p, p), E not given; analyzed tensor analyzing power data. 2H deduced D-to S-state asymptotic normalization.

1985BO40      Phys.Lett. 160B, 17 (1985)

I.Borbely, W.Gruebler, V.Konig, P.A.Schmelzbach, A.M.Mukhamedzhanov

Determinationn of the Deuteron S-State Asymptotic Normalization by Continuation of p-d Elastic Cross Section to the Transfer Pole

NUCLEAR REACTIONS 2H(p, p), E=2-46.3 MeV; analyzed σ(θ). 2H deduced S-state asymptotic normalization. Continuation into transfer pole region, correct three-particle state Coulomb effect handling.

doi: 10.1016/0370-2693(85)91459-5
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1984MU11      Izv.Akad.Nauk SSSR, Ser.Fiz. 48, 350 (1984)

A.M.Mukhamedzhanov, I.Borbei, W.Gruebler, V.Konig, P.A.Schmelzbach

Influence of Coulomb Interaction on the Singularities in the Exchange Amplitude and the Nuclear Vertex Constant d → p + n from the Analysis of pd-Angular Distributions

NUCLEAR REACTIONS 2H(p, p), E=3-46.3 MeV; calculated σ(θ); deduced exchange amplitude singularities Coulomb interaction role. Diagrammatic approach.

1982BO06      Phys.Lett. 109B, 262 (1982)

I.Borbely, W.Gruebler, V.Konig, P.A.Schmelzbach, B.Jenny

The Determination of the D-State Asymptotic Normalization of the Deuteron and Triton Wavefunctions by the Continuation of the 2H(d(pol), p)3H Tensor Polarizations

NUCLEAR REACTIONS 2H(polarized d, p), E=6-14 MeV; analyzed tensor polarization data. 2H deduced D-state asymptotic normalization.

doi: 10.1016/0370-2693(82)90431-2
Citations: PlumX Metrics

1982BO22      Phys.Lett. 113B, 443 (1982)

I.Borbely, P.Doleschall

Triton Binding Energy, Asymptotic Normalization Constants and Zero-Range Parameters

NUCLEAR STRUCTURE 3H; calculated binding energy, asymptotic normalization constants. Faddeev calculations, realistic separable interactions.

doi: 10.1016/0370-2693(82)90781-X
Citations: PlumX Metrics

1981BO04      Nucl.Phys. A351, 107 (1981)

I.Borbely, V.Konig, W.Gruebler, B.Jenny, P.A.Schmelzbach

The Asymptotic S- to D-State Ratio of the Deuteron- and Triton-Wave Function Determined by Empirical Continuation of the 2H(d, p)3H Tensor polarization

NUCLEAR REACTIONS 2H(polarized d, p), E=13 MeV; analyzed polarization data. 2,3H deduced asymptotic S- to D-state ratio. Empirical continuation.

doi: 10.1016/0375-9474(81)90547-9
Citations: PlumX Metrics

1977BL11      Fiz.Elem.Chastits At.Yadra 8, 1189 (1977); Sov.J.Part.Nucl. 8, 485 (1977)

L.D.Blokhintsev, I.Borbely, E.I.Dolinskii

Nuclear Vertex Constants

NUCLEAR STRUCTURE 2H, 3H, 3He, 4He, 6Li; reviewed properties of nuclear vertex constants, relation to nuclear wave functions.

1977BO42      Yad.Fiz. 26, 516 (1977); Sov.J.Nucl.Phys. 26, 274 (1977)

I.Borbei, E.I.Dolinskii, A.M.Mukhamedzhanov, V.V.Turovtsev

Effects of the Nuclear Vertex Form Factor in the Peripheral Model

NUCLEAR REACTIONS 18O(p, d), E=17.6 MeV; 19F(p, d), E=18.9 MeV; 19F(d, 3He), E=52 MeV; 14N(p, d), E=30.3 MeV; calculated σ(θ).

1976BO15      Nucl.Phys. A262, 244 (1976)

I.Borbely

Determination of Neutron Separation Vertex Constants of Light Nuclei from (d, p) Reaction Data

NUCLEAR REACTIONS 16O(d, p), E=13.3 MeV; 31P(d, p), E=10.0 MeV; 9Be(p, d), E=17-29 MeV; calculated σ. Singularity subtraction method.

doi: 10.1016/0375-9474(76)90618-7
Citations: PlumX Metrics

1971BO24      Phys.Lett. 35B, 388 (1971)

I.Borbely

Application of the Nonrelativistic Peripheral Model to Reactions between Light Particles

NUCLEAR REACTIONS 2H(d, p), E= 8.1, 13.8, 25.3, 83 MeV; 2H(p, d), E = 3-46 MeV; 2H(n, d), E = 18.3 MeV; calculated σ(θ). Nonrelativistic peripheral model.

doi: 10.1016/0370-2693(71)90400-X
Citations: PlumX Metrics

1971BO50      Phys.Lett. 37B, 243 (1971)

I.Borbely

Comparison of Spectroscopic Information Given by the Peripheral Model and DWBA

NUCLEAR REACTIONS 10B, 12C, 14N, 16O(d, t), 16O(d, p), E=26, 28 MeV; calculated σ(θ), opm, DWBA.

doi: 10.1016/0370-2693(71)90008-6
Citations: PlumX Metrics

1969BO32      Acta Phys.Acad.Sci.Hung. 26, 269 (1969)

I.Borbely, T.Dolinszky, J.Ero, G.Hrehuss

Angular Distributions of the Reaction 12C(d, p)13C below E = 2 MeV

NUCLEAR REACTIONS 12C(d, d), (d, p), E = 0.9-2.0 MeV; measured σ(E), σ(E;Ep, θ); deduced resonance interference. 14N deduced resonances, J, π.

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0659.

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