NSR Query Results


Output year order : Descending
Format : Normal

NSR database version of April 27, 2024.

Search: Author = M.P.Rekalo

Found 87 matches.

Back to query form



2004RE14      Phys.Lett. B 591, 225 (2004)

M.P.Rekalo, E.Tomasi-Gustafsson

Possible methods for the determination of the P-parity of the Θ+ -pentaquark in NN-collisions

NUCLEAR REACTIONS 1H(p, X), (n, X), E ≈ threshold; calculated pentaquark production associated polarization observables.

doi: 10.1016/j.physletb.2004.04.041
Citations: PlumX Metrics


2004RE17      Nucl.Phys. A740, 271 (2004)

M.P.Rekalo, E.Tomasi-Gustafsson

Complete experiment in eN-elastic scattering, in presence of two-photon exchange

NUCLEAR REACTIONS 1H(e, e), (e+, e+), E not given; calculated polarization observables, two-photon exchange contributions, form factors, related features.

doi: 10.1016/j.nuclphysa.2004.04.111
Citations: PlumX Metrics


2004RE23      Nucl.Phys. A742, 322 (2004)

M.P.Rekalo, E.Tomasi-Gustafsson

Polarization phenomena in eN elastic scattering, for axial parametrization of two-photon exchange

NUCLEAR REACTIONS 1n, 1H(e, e), (e+, e+), E not given; calculated polarization observables, two-photon exchange contribution.

doi: 10.1016/j.nuclphysa.2004.07.009
Citations: PlumX Metrics


2004RE27      Eur.Phys.J. A 22, 119 (2004)

M.P.Rekalo, E.Tomasi-Gustafsson

Polarization observables in the processes p + p → Θ+ + Σ+ and n + p → Θ+ + Λ0, in the threshold region, for any spin and parity of the Θ+-hyperon

NUCLEAR REACTIONS 1H(p, X), (n, X), E not given; calculated hyperon and pentaquark production polarization observables.

doi: 10.1140/epja/i2004-10026-8
Citations: PlumX Metrics


2004RE28      Eur.Phys.J. A 22, 331 (2004)

M.P.Rekalo, E.Tomasi-Gustafsson

Model-independent properties of two-photon exchange in elastic electron-proton scattering

NUCLEAR REACTIONS 1H(e, e), E not given; calculated two-photon exchange contribution to σ.

doi: 10.1140/epja/i2004-10039-3
Citations: PlumX Metrics


2004TO18      Phys.Rev. C 70, 025202 (2004)

E.Tomasi-Gustafsson, G.I.Gakh, A.P.Rekalo, M.P.Rekalo

Possible method for the determination of the neutron electric form factor based on a measurement of asymmetries for the process 2H(pol)(e(pol), e'n)p

NUCLEAR REACTIONS 2H(polarized e, e'n), E=2.721, 4.232 GeV; calculated polarization observables, dependence on neutron electric form factor. Polarized target.

doi: 10.1103/PhysRevC.70.025202
Citations: PlumX Metrics


2004TO21      Eur.Phys.J. A 21, 469 (2004)

E.Tomasi-Gustafsson, M.P.Rekalo

Exclusive photoproduction of charmed D* vector mesons, γ + N → Yc + (D-bar)*, Yc = Λ+c or Σc

NUCLEAR REACTIONS 1H(γ, X), E ≈ 10-200 GeV; calculated charmed meson production σ, polarization observables.

doi: 10.1140/epja/i2004-10005-1
Citations: PlumX Metrics


2003RE02      Nucl.Phys. A714, 632 (2003)

M.P.Rekalo, E.Tomasi-Gustafsson

Determination of the gVσγ coupling constant through the process γ + N → N + V with circularly polarized photons

NUCLEAR REACTIONS 1H(polarized γ, X), E=1.2, 1.8 GeV; calculated vector meson production associated polarization observables. Polarized target.

doi: 10.1016/S0375-9474(02)01403-3
Citations: PlumX Metrics


2003RE05      Phys.Rev. C 67, 038501 (2003)

M.P.Rekalo, E.Tomasi-Gustafsson

P parity of charmed particles from associative photoproduction of D and D*-mesons

NUCLEAR REACTIONS 1H(polarized γ, X), E=40 GeV; calculated D mesons relative σ(E, θ), polarization correlations, sensitivity to charmed particle parity.

doi: 10.1103/PhysRevC.67.038501
Citations: PlumX Metrics


2003RE06      Eur.Phys.J. A 16, 563 (2003)

M.P.Rekalo, E.Tomasi-Gustafsson

Sensitivity of the pQCD deuteron structure to the nucleon form factors

NUCLEAR REACTIONS 1,2H(e, e), E not given; analyzed form factors, scaling behavior. Perturbative QCD.

doi: 10.1140/epja/i2002-10115-8
Citations: PlumX Metrics


2003RE07      Eur.Phys.J. A 16, 575 (2003)

M.P.Rekalo, E.Tomasi-Gustafsson

Threshold open charm production in nucleon-nucleon collisions

NUCLEAR REACTIONS 1H(p, p'X), (n, n'X), E ≈ threshold; calculated charm production matrix elements. 1H(p, p'X), E ≈ threshold; calculated open charm production σ. D-meson exchange model.

doi: 10.1140/epja/i2002-10123-8
Citations: PlumX Metrics


2003RE13      Phys.Rev. C 67, 044004 (2003)

M.P.Rekalo, E.Tomasi-Gustafsson

The reaction Δ+N → N+N+φ in ion-ion collisions

doi: 10.1103/PhysRevC.67.044004
Citations: PlumX Metrics


2003RE24      Nucl.Phys. A725, 116 (2003)

M.P.Rekalo, E.Tomasi-Gustafsson

The gVσγ coupling constants in hadron electrodynamics

doi: 10.1016/S0375-9474(03)01605-1
Citations: PlumX Metrics


2003RE35      Eur.Phys.J. A 18, 709 (2003)

M.P.Rekalo, E.Tomasi-Gustafsson

Scalar-meson production in nucleon-nucleon collisions near threshold

NUCLEAR REACTIONS 1n, 1H(p, X), E ≈ threshold; calculated scalar-meson production associated matrix elements, polarization observables, related features.

doi: 10.1140/epja/i2003-10060-0
Citations: PlumX Metrics


2003TO26      Yad.Fiz. 66, 2209 (2003); Phys.Atomic Nuclei 66, 2159 (2003)

E.Tomasi-Gustafsson, L.Bimbot, S.Danagoulian, K.Gustafsson, D.Mack, H.Mkrtchyan, M.P.Rekalo

Observation of Coherent π0 Electroproduction on Deuterons at Large Momentum Transfer

NUCLEAR REACTIONS 2H(e, e'π0), E=4.05 GeV; measured pion production σ(Q2, W). Comparison with model predictions.

doi: 10.1134/1.1634323
Citations: PlumX Metrics


2002RE10      Phys.Rev. C65, 035501 (2002)

M.P.Rekalo, J.Arvieux, E.Tomasi-Gustafsson

Neutral Weak Currents in Pion Electroproduction on the Nucleon

NUCLEAR REACTIONS 1H(γ, π0), (γ, π+), E=220-300; calculated σ(θ). 1H(polarized e, e'π0), (polarized e, e'π+), E not given; calculated σ(k2, W), parity violating asymmetry.

doi: 10.1103/PhysRevC.65.035501
Citations: PlumX Metrics


2002RE12      Ann.Phys.(New York) 295, 1 (2002)

M.P.Rekalo, E.Tomasi-Gustafsson, J.Arvieux

Coherent π0 Electroproduction on the Deuteron

NUCLEAR REACTIONS 2H(γ, π0), E=220-300 MeV; 2H(e, e'π0), E=high; calculated σ(θ), form factors, polarization observables. Impulse approximation, η-meson production also discussed.

doi: 10.1006/aphy.2001.6208
Citations: PlumX Metrics


2002RE26      Phys.Rev. C66, 015203 (2002)

M.P.Rekalo, E.Tomasi-Gustafsson

Considerations on Rescattering Effects for Threshold Photo- and Electroproduction of π0 on the Deuteron

NUCLEAR REACTIONS 2H(γ, π0), (e, e'π0), E ≈ threshold; calculated rescattering effects, role of Pauli principle.

doi: 10.1103/PhysRevC.66.015203
Citations: PlumX Metrics


2002RE33      New Journal of Physics 4, 68 (2002)

M.P.Rekalo, E.Tomasi-Gustafsson

Threshold J/ψ production in nucleon-nucleon collisions

NUCLEAR REACTIONS 1H(p, p'X), (n, n'X), E ≈ threshold; calculated J/ψ production matrix elements, polarization, isotopic effects.

doi: 10.1088/1367-2630/4/1/368
Citations: PlumX Metrics


2002TO03      Nucl.Phys. A699, 152c (2002)

E.Tomasi-Gustafsson, M.P.Rekalo

The Nucleon Form Factors in Space-Like and Time-Like Regions

NUCLEAR STRUCTURE 1H; analyzed form factor data, asymptotic behavior.

doi: 10.1016/S0375-9474(01)01485-3
Citations: PlumX Metrics


2002TO13      Fiz.Elem.Chastits At.Yadra 33, 436 (2002); Phys.Part.Nucl. 33, 220 (2002)

E.Tomasi-Gustafsson, M.P.Rekalo

Polarization Phenomena in Hadronic and Nuclear Processes in the Threshold Regime


2001PA43      Eur.Phys.J. A 12, 121 (2001)

N.K.Pak, M.P.Rekalo

General Formalism in Collinear Regime for Pseudoscalar Meson Production in NN Collisions

NUCLEAR REACTIONS 1H(p, X), E not given; calculated matrix element spin structure for meson production.

doi: 10.1007/s100500170045
Citations: PlumX Metrics


2001RE03      Phys.Lett. 500B, 53 (2001)

M.P.Rekalo, E.Tomasi-Gustafsson

Associative Photoproduction of Charmed Particles Near Threshold

NUCLEAR REACTIONS 1H(γ, X), E ≈ 9-200 GeV; calculated charmed particle production σ, σ(θ), beam asymmetry. Effective Lagrangian model.

doi: 10.1016/S0370-2693(01)00016-8
Citations: PlumX Metrics


2001RE10      Phys.Rev. C63, 054001 (2001)

M.P.Rekalo, E.Tomasi-Gustafsson

Polarization Phenomena in the Reaction p + α → p + π0 + α

NUCLEAR REACTIONS 4He(p, pπ0), E not given; calculated spin transfer coefficients, matrix element spin structure; deduced exchanged meson dependence.

doi: 10.1103/PhysRevC.63.054001
Citations: PlumX Metrics


2001RE22      Ukr.J.Phys. 46, 668 (2001)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

The left-right asymmetry in deuteron electrodisintegration beyond quasi-elastic scattering

NUCLEAR REACTIONS 2H(polarized e, e'p), E not given; calculated azimuthal asymmetry, role of final-state interaction, deuteron wave function, other mechanisms.


2001TO12      Phys.Lett. 504B, 291 (2001)

E.Tomasi-Gustafsson, M.P.Rekalo

Search for Evidence of Asymptotic Regime of Nucleon Electromagnetic Form Factors from a Compared Analysis in Space- and Time-Like Regions

NUCLEAR STRUCTURE 1H; analyzed electric and magnetic form factors, asymptotic properties.

doi: 10.1016/S0370-2693(01)00312-4
Citations: PlumX Metrics


2001TO22      Europhys.Lett. 55, 188 (2001)

E.Tomasi-Gustafsson, M.P.Rekalo

Neutron Electric Form Factor at Large Momentum Transfer

NUCLEAR REACTIONS 1,2H(e, e), E=high; analyzed structure functions, analyzing powers. 1n, 1H deduced electric form factor vs momentum transfer. Nonrelativistic impulse approximation.

doi: 10.1209/epl/i2001-00330-9
Citations: PlumX Metrics


2000PA01      Phys.Rev. D61, 017501 (2000)

N.K.Pak, M.P.Rekalo

Polarization Phenomena for Processes p(bar) + p → P + V and Mechanisms of OZI Violations in φ Production

NUCLEAR REACTIONS 1H(p-bar, X), E not given; calculated matrix element spin structure for meson production.

doi: 10.1103/PhysRevD.61.017501
Citations: PlumX Metrics


2000SI11      Nucl.Phys. A663-664, 443c (2000)

I.M.Sitnik, C.F.Perdrisat, E.Tomasi-Gustafsson, L.S.Azhgirey, J.Ball, L.Bimbot, Y.Bisson, M.Boivin, Yu.T.Borzunov, J.L.Boyard, Ph.Courtat, R.Gacougnolle, M.Garcon, L.B.Golovanov, T.Hennino, M.Jones, D.A.Kirillov, R.Kunne, L.V.Malinina, S.Nedev, N.M.Piskunov, V.Punjabi, M.P.Rekalo, J.L.Sans, R.Skowron, E.A.Strokovsky, J.Yonnet

Measurement of the Deuteron Tensor Polarization at the 3He → d + p Vertex Up to Internal Momenta of 0.43 GeV/c

NUCLEAR REACTIONS 1H(polarized 3He, dX), E at 4.60-5.66 GeV/c; measured T20.

doi: 10.1016/S0375-9474(99)00679-X
Citations: PlumX Metrics


2000TA31      Acta Phys.Pol. B31, 2339 (2000)

B.Tatischeff, J.Yonnet, M.P.Rekalo, M.Boivin, M.P.Comets, P.Courtat, R.Gacougnolle, Y.Le Bornec, E.Loireleux, F.Reide, N.Willis

Production of π0, η, ω and Exotic Low Mass Mesons in N-N Scattering

NUCLEAR REACTIONS 1H(polarized p, pX), E=1.5, 1.8, 2.1 GeV; measured light meson production σ(θ), missing mass; deduced resonance features. Comparison with model predictions.


2000TA32      Phys.Rev. C62, 054001 (2000)

B.Tatischeff, J.Yonnet, M.P.Rekalo, M.Boivin, M.P.Comets, P.Courtat, R.Gacougnolle, Y.Le Bornec, E.Loireleux, F.Reide, N.Willis

Light Mesons: π, η, and ω and Exotic Low Mass Meson Production at Intermediate Energies in Nucleon-Nucleon Scattering

NUCLEAR REACTIONS 1H(polarized p, pX), E=1520, 1805, 2100 MeV; measured light meson production σ(θ), σ(E), analyzing powers. Previously unobserved structures in mass spectrum discussed.

doi: 10.1103/PhysRevC.62.054001
Citations: PlumX Metrics


1999ON02      Eur.Phys.J. A 6, 215 (1999)

S.Ong, M.P.Rekalo, J.Van de Wiele

Pion Electroproduction in Parity Violating Elastic ep Scattering Experiment

NUCLEAR REACTIONS 1H(γ, π0), (γ, π+), (e, eπ0), E not given; analyzed σ(θ), related data. 1H(e, eX), E=855 MeV; calculated pion electroproduction contribution in parity violation experiment.

doi: 10.1007/s100500050337
Citations: PlumX Metrics


1999PA42      Phys.Lett. 450B, 433 (1999)

N.K.Pak, M.P.Rekalo

Polarization Phenomena for (p-bar) + p → (Λ-bar) + Λ in Collinear Kinematics as a Test of Polarized Strangeness

NUCLEAR REACTIONS 1H(p-bar, X), E not given; calculated Λ hyperon production associated polarization observables.

doi: 10.1016/S0370-2693(99)00118-5
Citations: PlumX Metrics


1999RE04      Yad.Fiz. 62, No 2, 253 (1999); Phys.Atomic Nuclei 62, 218 (1999)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

Physics of Left-Right Asymmetry in Exclusive Deuteron Electrodisintegration

NUCLEAR REACTIONS 2H(e, e'p), E not given; calculated left-right asymmetry vs angle; deduced sensitivity to kinematic conditions. Relativistic impulse approximation. Comparison with data.


1999RE18      Few-Body Systems 26, 227 (1999)

M.P.Rekalo, J.Arvieux, E.Tomasi-Gustafsson

Polarization Phenomena for Vector-Meson Production Induced by Neutron-Proton Collisions in Collinear Kinematics

NUCLEAR REACTIONS 1H(n, dX), E not given; calculated vector-meson production associated polarization structure functions.

doi: 10.1007/s006010050116
Citations: PlumX Metrics


1999RE19      Phys.Rev. C60, 042202 (1999)

M.P.Rekalo, E.Tomasi-Gustafsson, D.Prout

Search for Evidence of Two-Photon Exchange in New Experimental High Momentum Transfer Data on Electron Deuteron Elastic Scattering

NUCLEAR REACTIONS 2H(e, e), E=high; analyzed σ(θ); deduced possible two-photon exchange contribution.

doi: 10.1103/PhysRevC.60.042202
Citations: PlumX Metrics


1999TO03      Phys.Rev. C59, 1526 (1999)

E.Tomasi-Gustafsson, M.P.Rekalo, R.Bijker, A.Leviatan, F.Iachello

Sensitivity of Tensor Analyzing Power in the Process d + p → d + X to the Longitudinal Isoscalar Form Factor of the Roper Resonance Electroexcitation

NUCLEAR REACTIONS 1H(polarized d, d'X), E at 3.7-9 GeV/c; calculated tensor analyzing power T20(q); deduced resonance contributions. Algebraic collective model.

doi: 10.1103/PhysRevC.59.1526
Citations: PlumX Metrics


1998KO02      Int.J.Mod.Phys. E7, 139 (1998)

H.Koru, M.P.Rekalo

Testing Nucleon Strangeness in Polarization Effects for n + p → d + η

NUCLEAR REACTIONS 1n(p, dX), E not given; calculated η production associated polarization observables; deduced strangeness component related features.

doi: 10.1142/S0218301398000075
Citations: PlumX Metrics


1998PA03      Eur.Phys.J. A 1, 201 (1998)

N.P.Pak, M.P.Rekalo

Manifestations of Hidden Polarized Strangeness of the Nucleon in Polarization Phenomena for the Process p + (p-bar) → P0 + V0

NUCLEAR REACTIONS 1H(p-bar, X), E not given; calculated two-meson production associated polarization observables; deduced strangeness related features.

doi: 10.1007/s100500050049
Citations: PlumX Metrics


1998RE08      Phys.Rev. C57, 2870 (1998)

M.P.Rekalo, E.Tomasi-Gustafsson

Polarization Phenomena for Low Energy d + 3He Collisions

NUCLEAR REACTIONS 3He(polarized d, p), E < 1 MeV; calculated σ(θ), polarization observables.

doi: 10.1103/PhysRevC.57.2870
Citations: PlumX Metrics


1998RE13      Few-Body Systems 23, 187 (1998)

M.P.Rekalo, N.M.Piskunov, I.M.Sitnik

Complete Experiment for d-p and 3He-d Backward Elastic Scattering

NUCLEAR REACTIONS 2H(polarized p, p), 3He(polarized d, d), E not given; calculated polarization observables for backward scattering.

doi: 10.1007/s006010050070
Citations: PlumX Metrics


1998YA08      J.Phys.(London) G24, 1003 (1998)

C.Yalcin, M.P.Rekalo, H.Koru

General Analysis of the Polarization Effects in N + N → d + P Processes

NUCLEAR REACTIONS 1H(polarized n, π0), E not given; calculated polarization effects.

doi: 10.1088/0954-3899/24/5/008
Citations: PlumX Metrics


1998YA10      Nucl.Phys. A635, 387 (1998)

C.Yalcin, M.P.Rekalo, H.Koru

Electromagnetic Form Factors of Electrodisintegration of Light Nuclei Near Threshold

doi: 10.1016/S0375-9474(98)00193-6
Citations: PlumX Metrics


1998YO05      Nucl.Phys. A637, 63 (1998)

J.Yonnet, B.Tatischeff, M.P.Rekalo, N.Willis, M.Boivin, M.P.Comets, P.Courtat, R.Gacougnolle, Y.Le Bornec, E.Loireleux, F.Reide

Analyzing Powers of One and Two Δ Production in Inelastic pp Reactions at Energies between 1.5 and 2.1 GeV

NUCLEAR REACTIONS 1H(polarized p, π+X), E=1520, 1805, 2100 MeV; measured analyzing powers vs θ; deduced Δ production related features.

doi: 10.1016/S0375-9474(98)00221-8
Citations: PlumX Metrics


1997RE06      Z.Phys. A357, 133 (1997)

M.P.Rekalo, J.Arvieux, E.Tomasi-Gustafsson

OZI Violation and Polarization Effects in Nucleon-Nucleon Induced Production of Vector Mesons

NUCLEAR REACTIONS 1H(p-bar, X), E not given; analyzed annihilation into φ-meson related features; deduced OZI-rule violation associated features.

doi: 10.1007/s002180050227
Citations: PlumX Metrics


1997RE09      Phys.Rev. C55, 2630 (1997)

M.P.Rekalo, J.Arvieux, E.Tomasi-Gustafsson

Properties of η-Meson Production in Nucleon-Nucleon Collisions Near Threshold

NUCLEAR REACTIONS 1H, 1n(p, X), E ≤ threshold; calculated η-production ratio, polarization observables, spin-correlation coefficients; deduced S-, P-wave contributions to spin structure.

doi: 10.1103/PhysRevC.55.2630
Citations: PlumX Metrics


1997RE16      Yad.Fiz. 60, No 8, 1361 (1997); Phys.Atomic Nuclei 60, 1228 (1997)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

Polarization Effects in Deuteron Electrodisintegration: T-odd proton polarization

NUCLEAR REACTIONS 2H(e, e'p), E=654-730 MeV; calculated proton polarization vector. Structure functions formalism.


1997RE19      Phys.Rev. C56, 2238 (1997)

M.P.Rekalo, J.Arvieux, E.Tomasi-Gustafsson

Strange Particle Production in Nucleon-Nucleon Collisions Near Threshold

NUCLEAR REACTIONS 1H(p, X), E ≈ threshold; calculated strange particle production associated amplitudes spin structure. Final particles S-, P-wave production assumed.

doi: 10.1103/PhysRevC.56.2238
Citations: PlumX Metrics


1997YA16      Ann.Phys.(New York) 257, 136 (1997)

C.Yalcin, M.P.Rekalo, H.Koru

General Analysis of Polarization Phenomena in Processes of Inclusive and Exclusive Scattering Photons and Electrons by Hadrons

doi: 10.1006/aphy.1997.5678
Citations: PlumX Metrics


1996GA14      Yad.Fiz. 59, No 4, 656 (1996); Phys.Atomic Nuclei 59, 624 (1996)

G.I.Gakh, M.P.Rekalo

Polarization Effects in Diffractive Deuteron Disintegration Induced by High-Energy Pions

NUCLEAR REACTIONS 2H(π, πp), E not given; calculated proton polarization, asymmetry vs θ. Diffractive disintegration, polarized target, one-Pomeron mechanism.


1996RE14      Yad.Fiz. 59, No 6, 996 (1996); Phys.Atomic Nuclei 59, 952 (1996)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

Simplest T-Odd Polarization Observable in the Exclusive Deuteron Electrodisintegration

NUCLEAR REACTIONS 2H(polarized e, e'p), E not given; calculated asymmetry vs θ; deduced different mechanisms contributions. Relativistic impulse approximation.


1996RE23      Phys.Rev. C54, 3125 (1996)

M.P.Rekalo, E.Tomasi-Gustafsson

Polarization Observables in the Process d + p → d + X and Electromagnetic Form Factors of N → N(*) Transitions

NUCLEAR REACTIONS 1H(polarized d, X), E at 4.5, 5.5 GeV/c; calculated T20, vector polarization transfer coefficient vs q. 2H(e, e), E at 4.5, 5.5 GeV/c; analyzed T20 vs q data; deduced nucleonic resonances excitation, 2H magnetic form factors related features.

doi: 10.1103/PhysRevC.54.3125
Citations: PlumX Metrics


1996YA04      Phys.Rev. C53, 2645 (1996)

C.Yalcin, M.P.Rekalo, H.Koru

Isospin Invariance and the Spin Structure of the Amplitude for the Process 3H + 3He → d2H + 4He

NUCLEAR REACTIONS 3He(t, X), E not given; analyzed amplitude spin struture, isospin invariance features for the process t+3He → d2H+α, polarization effects.

doi: 10.1103/PhysRevC.53.2645
Citations: PlumX Metrics


1995GA23      Yad.Fiz. 58, No 3, 553 (1995); Phys.Atomic Nuclei 58, 501 (1995)

G.I.Gakh, M.P.Rekalo

Disintegration of Deuterons in the Scattering of High-Energy Pions in the Diffraction Region

NUCLEAR REACTIONS 2H(π+, π+p), (π-, π-p), E=high; calculated σ, longitudinal to transverse σ (ratio) vs E(np), θ. Diffraction dissociation model, pomeron exchange.


1995RE17      Phys.Lett. 356B, 434 (1995)

M.P.Rekalo, I.M.Sitnik

Study of T-Odd Asymmetry in Backward Elastic dp Scattering as a Method to Identify the Reaction Mechanism

NUCLEAR REACTIONS 1H(polarized d, d), E not given; calculated T-odd asymmetry, backward scattering; deduced sensitivity to mechanism. Polarized target.

doi: 10.1016/0370-2693(95)00754-9
Citations: PlumX Metrics


1994RE08      Yad.Fiz. 57, No 4, 659 (1994); Phys.Atomic Nuclei 57, 698 (1994)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

Unitarization of the e- + d → e- + n + p Amplitude Using NN Scattering Phases

NUCLEAR REACTIONS 2H(e, e'p), E not given; calculated σ(E(e'), θ(e), θp), asymmetry vs θ. Unitarization scheme by using NN scattering phases from data analysis.


1994SI24      Yad.Fiz. 57, No 12, 2170 (1994); Phys.Atomic Nuclei 57, 2089 (1994)

I.M.Sitnik, V.P.Ladygin, M.P.Rekalo

Polarization Phenomena in Backward Elastic Deuteron-Proton Scattering d + p → p + d

NUCLEAR REACTIONS 2H(polarized p, p), E at ≤ 1 GeV/c; calculated spin correlation function vs momentum. Polarized target, impulse approximation.


1993RE10      J.Phys.(London) G19, 1325 (1993)

M.P.Rekalo, I.V.Stoletny

Rescattering Effects in the Reaction γd → dπ0 at Large π0 Production Angles

NUCLEAR REACTIONS 2H(γ, π0), (polarized γ, π0), E ≈ 0.3-1 GeV; analyzed σ(θ), asymmetry vs E. Two different mechanisms.

doi: 10.1088/0954-3899/19/9/011
Citations: PlumX Metrics


1992GA12      Z.Phys. A341, 205 (1992)

V.B.Ganenko, V.A.Gushchin, Yu.V.Zhebrovskij, A.A.Zybalov, L.Ya.Kolesnikov, O.G.Konovalov, Yu.V.Kulish, S.V.Marekhin, M.P.Rekalo, A.L.Rubashkin, P.V.Sorokin, Yu.O.Storozhenko, A.Eh.Tenishev

Polarization Observables Σ, P(y), T1 in the Reaction γ(pol) d → p(pol)n at Photon Energies between 200 and 600 MeV and Dibaryon Resonances

NUCLEAR REACTIONS 2H(polarized γ, p), E=300-600 MeV; measured polarization observables; deduced dibaryon resonances role. Linear beam polarization. Gauge invariant pole model, multipole analysis.

doi: 10.1007/BF01298482
Citations: PlumX Metrics


1992ST12      Yad.Fiz. 55, 2408 (1992); Sov.J.Nucl.Phys. 55, 1338 (1992)

I.V.Stoletny, M.P.Rekalo

Effects of Rescattering of Pions in the Reaction γd → dπ0 and the Problem of Dibaryon Resonances

NUCLEAR REACTIONS 2H(γ, π0), (polarized γ, π0), E ≤ 1 GeV; calculated σ(θ), asymmetry vs θ. Coherent pion production mechanism.


1991RE05      J.Phys.(London) G17, 1643 (1991)

M.P.Rekalo, I.V.Stoletny

Neutron Pion Photoproduction on Deuterons in the Resonance Energy Region

NUCLEAR REACTIONS 2H(polarized γ, π0), E=0.2-0.8 GeV; calculated σ(θ) vs E. Linear beam, vector target polarizations, impulse approximation.

doi: 10.1088/0954-3899/17/11/011
Citations: PlumX Metrics


1990ST31      Yad.Fiz. 52, 723 (1990); Sov.J.Nucl.Phys. 52, 464 (1990)

I.V.Stoletny, M.P.Rekalo

Coherent Photoproduction of π0 Mesons on Deuterons, γd → dπ0

NUCLEAR REACTIONS 2H(polarized γ, π0), (γ, π0), E=0.2-0.8 GeV; calculated σ(θ), asymmetry; deduced pion production mechanism. Impulse approximation.


1989AF02      Ukr.Fiz.Zh. 34, 1773 (1989)

A.V.Afanasev, M.P.Rekalo

Polarization Effects in Deuteron Electrodisintegration Near Threshold

NUCLEAR REACTIONS 2H(e, e'np), (polarized e, e'np), E ≈ threshold; calculated analyzing power. Relativistic impulse approximation. Polarized target.


1989RE05      J.Phys.(London) G15, 1223 (1989)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

Polarization Effects in Deuteron Electrodisintegration and the Neutron Electric Form Factor

NUCLEAR REACTIONS 2H(e, e'p), E not given; calculated neutron electric form factor dependent polarization effect. Polarized target.

doi: 10.1088/0954-3899/15/8/018
Citations: PlumX Metrics


1988AF05      Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 2210 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.11, 130 (1988)

A.V.Afanasev, M.P.Rekalo

Electrosplitting of the Deuteron in the Region of Small Transmitted Energies and Momenta

NUCLEAR REACTIONS 2H(e-, np), E=threshold; calculated breakup form factor vs E(np); deduced structural function, polarization effects features.


1988RE04      Phys.Lett. 205B, 432 (1988)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

Neutron Electric Form Factor in Inelastic Scattering of Polarized Electrons by Polarized Deuterons

NUCLEAR REACTIONS 2H(polarized e, e'p), E not given; calculated σ(θ(e'), E(e'), θp); deduced sensitivity to neutron electric form factor, d wave function. Polarized target.

doi: 10.1016/0370-2693(88)90972-0
Citations: PlumX Metrics


1988RE15      Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 2252 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.11, 173 (1988)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

Tensor Polarization of Target in the Reaction d(pol)(e, np)e' for Investigation of the Spin Structure of the Deuteron Wave Function

NUCLEAR REACTIONS 2H(e, np), E not given; calculated polarization observables following breakup; deduced sensitivity to target wave function.


1988RE16      Ukr.Fiz.Zh. 33, 179 (1988)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

Deuteron Tensor Polarization in the e- + d → e- + p + n Process

NUCLEAR REACTIONS 2H(e, e'p), (e, np), E not given; calculated asymmetries vs Ep, θp; deduced deuteron wave function parametrization. Polarized target. Relativistic impulse approximation.


1987ES03      Yad.Fiz. 45, 410 (1987)

A.S.Esaulov, A.P.Rekalo, M.P.Rekalo, Yu.I.Titov, R.V.Akhmerov, E.M.Smelov

Measurement of the Neutron Magnetic Form Factor in the d(e, e')np Reaction for Momentum Transfers 0.48 ≤ Q2 ≤ 0.83 GeV2

NUCLEAR REACTIONS 2H(e, e'n), E=high; measured σ(θ, E(e')). 1n deduced magnetic moment factor, deuteron wave function dependence.


1987RE06      Yad.Fiz. 45, 777 (1987)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

On a Possibility to Determine the Neutron Charge Form Factor in the d(pol)(e(pol), e')np Reaction

NUCLEAR REACTIONS 2H(polarized e, e'n), E ≤ 1104 MeV; calculated electron scattering assymmetry following breakup; deduced sensitivity to neutron charge form factor. Polarized target, longitudinal beam polarization.


1987RE12      J.Phys.(London) G13, 1209 (1987)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

Inclusive Electrodisintegration of Polarized Deuterons

NUCLEAR REACTIONS 2H(polarized e, e'n), E=449-1104 MeV; calculated σ(E(e'), θ(e)), asymmetry. One-photon approximation, polarized target.

doi: 10.1088/0305-4616/13/10/010
Citations: PlumX Metrics


1987RE13      Ukr.Fiz.Zh. 32, 805 (1987)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

Quasielastic Scattering of Polarized Electrons by Polarized Deuterons in the Process of d(pol)(e(pol), e'p)n

NUCLEAR REACTIONS 2H(polarized e, e'p), E not given; calculated independent asymmetries vs θ. Vector polarized target, longitudinal beam polarization.


1986AK06      Dok.Akad.Nauk SSSR 288, 100 (1986); Sov.Phys.Dokl. 31, 408 (1986)

A.I.Akhiezer, M.P.Rekalo

Polarization Correlations in the Radiative Capture of Nucleons by Deuterons, n+d → 3H+γ and p+d → 3He+γ

NUCLEAR REACTIONS 2H(polarized p, γ), (polarized n, γ), E=slow; calculated reaction amplitude, tensor polarization, σ(θ). Hadronic electromagnetic interaction, polarized target.


1986BA10      Nucl.Phys. A451, 751 (1986)

V.P.Barannik, A.S.Bratashevskij, V.G.Gorbenko, V.A.Gushchin, Yu.V.Zhebrovskij, A.A.Zybalov, S.P.Karasev, L.Ya.Kolesnikov, O.G.Konovalov, Yu.V.Kulish, M.P.Rekalo, A.L.Rubashkin, P.V.Sorokin, Yu.O.Storozhenko, A.Eh.Tenishev

Proton Polarization in Deuteron Disintegration by Linearly Polarized Photons and Dibaryon Resonances

NUCLEAR REACTIONS 2H(polarized γ, p), E=300-500 MeV; measured σ(θ) asymmetry, proton polarization, polarization asymmetry. Linearly polarized beam.

doi: 10.1016/0375-9474(86)90304-0
Citations: PlumX Metrics


1986RE01      Phys.Lett. 166B, 27 (1986)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

A Polarized Deuteron Target in the d(pol)(e(pol), e')np Reaction

NUCLEAR REACTIONS 2H(polarized e, e'), E=449, 557, 865, 1104 MeV; calculated σ(E(e')), asymmetries; deduced neutron electric form factor, deuteron spin structure roles. Polarized target.

doi: 10.1016/0370-2693(86)91148-2
Citations: PlumX Metrics


1986RE09      Ukr.Fiz.Zh. 31, 805 (1986)

M.P.Rekalo

The Polarized Phenomena in Deuteron Photo- and Electrodisintegration near the Threshold

NUCLEAR REACTIONS 2H(γ, n), (e-, n), E ≈ breakup; calculated polarization observables near disintegration threshold.


1986RE16      Izv.Akad.Nauk SSSR, Ser.Fiz. 50, 2001 (1986); Bull.Acad.Sci.USSR, Phys.Ser. 50, No.10, 126 (1986)

M.P.Rekalo, G.I.Gakh, A.P.Korzh

Electron Breakup of Polarized Deuteron with Δ-Isobar Excitation

NUCLEAR REACTIONS 2H(e, e'n), E=0.5-2.5 GeV; calculated σ(E(e'), θn), asymmetry.


1986RE17      Ukr.Fiz.Zh. 31, 1293 (1986)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

Proton Polarization in the d(e(pol), e'p(pol))n Reaction and Electric Form Factor of a Neutron

NUCLEAR REACTIONS 2H(polarized e, e'p), E not given; calculated proton polarization, recoil neutron electric form factor. Relativistic impulse approximation.


1985RE08      Ukr.Fiz.Zh. 30, 662 (1985)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

Relativistic Impulse Approximation and d(e, e')pn Reaction on the Polarized Deuteron Target

NUCLEAR REACTIONS 2H(e, e'p), E=449, 1104 MeV; calculated polarized electron asymmetries. Polarized target, relativistic impulse approximation.


1985RE13      Ukr.Fiz.Zh. 30, 1125 (1985)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

Description of the d(e, e'p)n Reaction in the Framework of Relativistic Impulse Approximation

NUCLEAR REACTIONS 2H(e, e'p), E=500 MeV; calculated σ(θ(e), (θp), E(e')). Relativistic impulse approximation, electrodisintegration.


1985RE14      Yad.Fiz. 42, 393 (1985); Sov.J.Nucl.Phys. 42, 249 (1985)

M.P.Rekalo

Thermal-Neutron Capture by Protons Accompanied by e+e- Pair Production

NUCLEAR REACTIONS 1H(n, e+e-), E=thermal; calculated capture induced pair production electromagnetic form factors.


1984AK01      Dok.Akad.Nauk SSSR 274, 1079 (1984); Sov.Phys.Dokl. 24, 121 (1984)

A.I.Akhiezer, M.P.Rekalo

Radiative Capture of Polarized Deuterons by α Particles

NUCLEAR REACTIONS 4He(polarized d, α), E not given; calculated polarization variables, σ(θ) in capture process.


1984RE01      Ukr.Fiz.Zh. 29, 11 (1984)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

Deuteron Distintegration in the Neutrino Scattering Reaction ν + d → ν + p + n

NUCLEAR REACTIONS 2H(polarized ν, νp), E ≈ breakup; calculated σ(θ(ν), E(ν), θp); deduced beam, target polarization dependences.


1983RE06      Ukr.Fiz.Zh. 28, 481 (1983)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

P-Odd Effects in the Electrodisintegration of the Deuteron in the Reaction e- + d → e- + n + p

NUCLEAR REACTIONS 2H(e-, e-n), (polarized e-, e-n), E=breakup threshold; calculated P-odd role in σ(θ(e), θn), recoil proton polarization, P-odd asymmetries. Polarized target, final state interactions.


1983RE14      Ukr.Fiz.Zh. 28, 1313 (1983)

M.P.Rekalo, G.I.Gakh, A.P.Rekalo

General Structure of the Polarization Characteristics of the Electrodisintegration of the Deuteron

NUCLEAR REACTIONS 2H(polarized e-, p), E ≈ breakup threshold; calculated breakup σ(E(e), θ(e), θp), proton asymmetry; deduced colliding particle polarization state dependence. Vector, tensor polarized target.


1983RE15      Izv.Akad.Nauk SSSR, Ser.Fiz. 47, 2244 (1983)

M.P.Rekalo

Polarization Phenomena in the Process e- + 6Li → e- + 6Li(*) (3.56 MeV)

NUCLEAR REACTIONS 6Li(polarized e, e'), E not given; calculated polarization asymmetry ratio. Hadron, electromagnetic interactions.


1971RE22      Ukr.Fiz.Zh. 16, 1841 (1971)

M.P.Rekalo

Connection of Neutral Vector Meson Photoproduction Processes on Nuclei With the Processes of π- and K-Meson Interaction with Nuclei


Back to query form