Nuclear Science References (NSR)

NUCLEAR REACTIONS ²H(e, e'X), E=4 GeV; calculated meson-, quark-exchange contributions (amplitude)² vs Ep; deduced quark degrees of freedom exploration possibility in Δ production.

doi: 10.1016/0370-2693(95)00135-8
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1995WA22 Nucl.Phys. A594, 263 (1995)

G.Wagner, L.Ya.Glozman, A.J.Buchmann, A.Faessler

Constituent Quark Model Calculation for a Possible J(P) = 0^-, T = 0 Dibaryon

doi: 10.1016/0375-9474(95)00351-Z
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1994GL01 Phys.Rev. C49, 1149 (1994); Erratum Phys.Rev. C53, 2560 (1996)

L.Ya.Glozman, E.I.Kuchina

Baryon-Baryon Components in the Deuteron as Quark-Exchange Currents

NUCLEAR STRUCTURE ²H; calculated different baryon-baryon components effective number. Quark exchange currents.

doi: 10.1103/PhysRevC.49.1149
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1994GL02 J.Phys.(London) G20, 93 (1994)

L.Ya.Glozman, U.Straub, A.Faessler

The d(e, e'p)Δ Process as an Example of Quark-Exchange Currents in Leading Order

NUCLEAR REACTIONS ²H(e, e'X), E not given; calculated off-shell disintegration d → ΔΔ amplitude; deduced quark exchange role.

doi: 10.1088/0954-3899/20/1/010
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1994GL03 J.Phys.(London) G20, L49 (1994)

L.Ya.Glozman, A.Buchmann, A.Faessler

Constituent Quark Model and a Possible J(p) = 0^-, T = 0 Dibaryon

doi: 10.1088/0954-3899/20/5/001
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1994ZH21 Nucl.Phys. A578, 573 (1994)

Z.-Y.Zhang, A.Faessler, U.Straub, L.Ya.Glozman

The Baryon-Baryon Interaction in a Modified Quark Model

doi: 10.1016/0375-9474(94)90761-7
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1993GL04 Phys.Rev. C48, 389 (1993)

L.Ya.Glozman, V.G.Neudatchin, I.T.Obukhovsky

Exclusive Process ²H(e, e'p)N(*) as a Tool for Investigation of the Quark Structure of the Deuteron

NUCLEAR REACTIONS ²H(e, e'p), E not given; calculated spectroscopic factors, momentum distributions, various baryon-baryon channels. ²H deduced quark structure. Exclusive reaction, nonrelativistic quark model.

doi: 10.1103/PhysRevC.48.389
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1992GL01 Phys.Rev. C45, R17 (1992)

L.Ya.Glozman, V.I.Kukulin, V.N.Pomerantsev

Deep Attractive NN Potential as a Potential for the N(1440)-N System

NUCLEAR STRUCTURE ²H; calculated N(1440)-N component momentum distribution. Deep attractive NN-potential.

doi: 10.1103/PhysRevC.45.R17
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1990GL08 Phys.Lett. 252B, 23 (1990)

L.Ya.Glozman, V.G.Neudatchin, I.T.Obukhovsky, A.A.Sakharuk

The d(e, e'p)N(*) Process as a Tool for the Study of the 6q-Structure of the Deuteron

NUCLEAR REACTIONS ²H(e, e'p), E not given; calculated excited spectator nucleon related momentum distributions. Six-quark deuteron wave function.

doi: 10.1016/0370-2693(90)91073-K
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1989GL01 Z.Phys. A332, 339 (1989)

L.Ya.Glozman, N.A.Burkova, E.I.Kuchina

Elastic and Inelastic Magnetic Form Factors of Deuteron in the Model of Orthogonal Coupled Channels

NUCLEAR STRUCTURE ²H; calculated form factors. Orthogonal coupled channels.

NUCLEAR REACTIONS ²H(e, n), E ≈ threshold; calculated electrodisintegration σ(θn, En) vs momentum transfer. Orthogonal coupled channels.

1988BU06 Yad.Fiz. 47, 983 (1988)

N.A.Burkova, L.Ya.Glozman, M.A.Zhusupov, V.G.Neudachin

On Three-Cluster Fragmentation Mechanism of Light Nuclei A(γ, b₁b₂)A-b by 60-100-MeV Photons

NUCLEAR REACTIONS ¹⁶O(γ, 2d), ¹²C(γ, pd), E=60-100 MeV; calculated σ(E₁, θ₁, θ₂), σ(Ep, θp, θd); deduced fragmentation mechanism.

1988GL01 Phys.Lett. 200B, 406 (1988)

L.Ya.Glozman, N.A.Burkova, E.I.Kuchina, V.I.Kukulin

Nucleonic, Mesonic and Quark Degrees of Freedom in the Description of Electromagnetic Processes in the Two-Nucleon System

NUCLEAR REACTIONS ²H(e, e'p), E=300-700 MeV; calculated double differential σ. Consistent semi-microscopic model.

doi: 10.1016/0370-2693(88)90143-8
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1984GL02 Phys.Lett. 136B, 315 (1984)

L.Ya.Glozman, V.I.Kukulin, V.G.Neudatchin

Investigation of the ⁶Li(π⁺, pp)⁴He Process within the Three-Body Problem with Forbidden States

NUCLEAR REACTIONS ⁶Li(π⁺, 2p), E=70 MeV; calculated recoil α momentum distribution. Three-body problem, forbidden states, intermediate isobar absorption mechanism.

doi: 10.1016/0370-2693(84)92010-0
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1984GL09 Nucl.Phys. A430, 589 (1984)

L.Ya.Glozman, V.I.Kukulin, V.G.Neudatchin

A Study of the ⁶Li(π⁺, pp)⁴He Reaction within the Three-Body Problem

NUCLEAR REACTIONS ⁶Li(π⁺, 2p), E=70 MeV; calculated σ(θp₁, θp₂, Ep₁). Three-body model, symmetrical coplanar kinematics.

doi: 10.1016/0375-9474(84)90096-4
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1984GL11 Pisma Zh.Eksp.Teor.Fiz. 40, 33 (1984); JETP Lett.(USSR) 40, 759 (1984)

L.Ya.Glozman, V.G.Neudachin

Microscopic Approach to Direct Cluster Absorption of γ Rays

NUCLEAR REACTIONS ¹⁶O(γ, 2d), E not given; calculated σ(θ₁, θ₂, E₁). Direct cluster absorption, microscopic approach.

1983GL05 J.Phys.(London) G9, 1033 (1983)

L.Ya.Glozman, Yu.M.Tchuvilsky

Multicluster Fractional Parentage Coefficients

NUCLEAR STRUCTURE ¹⁶O; calculated three-body breakup multi-cluster fractional parentage coefficients. Translationally invariant shell model, harmonic oscillator basis.

doi: 10.1088/0305-4616/9/9/009
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Note: The following list of authors and aliases matches the search parameter L.Y.Glozman: , L.Y.GLOZMAN