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NSR database version of May 24, 2024.

Search: Author = L.Y.Glozman

Found 52 matches.

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2022GL05      Eur.Phys.J. A 58, 247 (2022)

L.Y.Glozman, O.Philipsen, R.D.Pisarski

Chiral spin symmetry and the QCD phase diagram

doi: 10.1140/epja/s10050-022-00895-4
Citations: PlumX Metrics


2021GL01      Eur.Phys.J. A 57, 182 (2021)

L.Ya.Glozman, C.B.Lang

A finite box as a tool to distinguish free quarks from confinement at high temperatures

doi: 10.1140/epja/s10050-021-00494-9
Citations: PlumX Metrics


2019RO02      Nucl.Phys. A982, 207c (2019)

C.Rohrhofer, Y.Aoki, G.Cossu, H.Fukaya, L.Glozman, S.Hashimoto, C.B.Lang, S.Prelovsek

Observation of approximate SU(2)CS and SU(2nf) symmetries in high temperature lattice QCD

doi: 10.1016/j.nuclphysa.2018.10.037
Citations: PlumX Metrics


2018GL02      Eur.Phys.J. A 54, 117 (2018)

L.Ya.Glozman

Chiralspin symmetry and QCD at high temperature

doi: 10.1140/epja/i2018-12560-0
Citations: PlumX Metrics


2015GL01      Eur.Phys.J. A 51, 27 (2015)

L.Ya.Glozman

SU(4) symmetry of the dynamical QCD string and genesis of hadron spectra

doi: 10.1140/epja/i2015-15027-x
Citations: PlumX Metrics


2008GL04      Nucl.Phys. A807, 38 (2008)

L.Ya.Glozman, A.V.Nefediev

Chiral restoration in excited nucleons versus SU(6)

doi: 10.1016/j.nuclphysa.2008.04.001
Citations: PlumX Metrics


2005BU25      Nucl.Phys. A755, 481c (2005)

T.Burch, C.Gattringer, L.Ya.Glozman, C.Hagen, D.Hierl, R.Kleindl, C.B.Lang, A.Schafer, and the BGR [Bern-Graz-Regensburg] Collaboration

Masses of excited baryons from chirally improved quenched lattice QCD

doi: 10.1016/j.nuclphysa.2005.03.058
Citations: PlumX Metrics


2005GL08      Nucl.Phys. A755, 17c (2005)

L.Ya.Glozman

Parity doublets in the baryon spectrum

doi: 10.1016/j.nuclphysa.2005.03.122
Citations: PlumX Metrics


2004BR20      Nucl.Phys. B(Proc.Supp.) S129/130, 251 (2004)

D.Brommel, P.Crompton, C.Gattringer, L.Ya.Glozman, C.B.Lang, A.Schafer, S.Schafer, for the BGR[Bern-Graz-Regensburg] Collaboration

Low lying nucleons from chirally improved fermions

doi: 10.1016/j.nuclphysbps.2003.12.124
Citations: PlumX Metrics


2004BR25      Phys.Rev. D 69, 094513 (2004)

D.Brommel, P.Crompton, C.Gattringer, L.Ya.Glozman, C.B.Lang, S.Schaefer, A.Schafer

Excited nucleons with chirally improved fermions

doi: 10.1103/PhysRevD.69.094513
Citations: PlumX Metrics


2004GL02      Eur.Phys.J. A 19, 153 (2004)

L.Ya.Glozman

Why the high-lying glueball does not mix with the neighbouring f0

doi: 10.1140/epja/i2003-10136-9
Citations: PlumX Metrics


2003WA30      Eur.Phys.J. A 18, 155 (2003)

R.F.Wagenbrunn, S.Boffi, L.Ya.Glozman, W.Klink, W.Plessas, M.Radici

Relativistic study of nucleon electroweak properties in a constituent-quark model

NUCLEAR STRUCTURE 1n, 1H; calculated form factors, radii, μ. Constituent-quark model.

doi: 10.1140/epja/i2002-10291-5
Citations: PlumX Metrics


2002BO23      Eur.Phys.J. A 14, 17 (2002)

S.Boffi, L.Ya.Glozman, W.Klink, W.Plessas, M.Radici, R.F.Wagenbrunn

Covariant Electroweak Nucleon Form Factors in a Chiral Constituent-Quark Model

NUCLEAR STRUCTURE 1n, 1H; calculated electric, magnetic and pseudoscalar form factors, charge radii. Chiral constituent-quark model.

doi: 10.1007/s10050-002-8784-3
Citations: PlumX Metrics


2002PL01      Nucl.Phys. A699, 312c (2002)

W.Plessas, S.Boffi, L.Ya.Glozman, W.Klink, M.Radici, R.F.Wagenbrunn

Nucleon Properties in a Semirelativistic Chiral Quark Model

NUCLEAR STRUCTURE 1n, 1H; calculated form factors, radii, μ. Goldstone-boson-exchange constituent quark model, comparison with data.

doi: 10.1016/S0375-9474(01)01509-3
Citations: PlumX Metrics


2001GL03      Nucl.Phys. A684, 287c (2001)

L.Ya.Glozman, D.O.Riska

Pion Loop Fluctuations of Constituent Quarks and Baryons

doi: 10.1016/S0375-9474(01)00423-7
Citations: PlumX Metrics


2001GL08      Phys.Lett. 516B, 183 (2001)

L.Ya.Glozman, M.Radici, R.F.Wagenbrunn, S.Boffi, W.Klink, W.Plessas

Covariant Axial Form Factor of the Nucleon in a Chiral Constituent Quark Model

NUCLEAR STRUCTURE 1n, 1H; calculated axial form factor. Chiral constituent quark model.

doi: 10.1016/S0370-2693(01)00915-7
Citations: PlumX Metrics


2001ST05      Nucl.Phys. A683, 359 (2001)

Fl.Stancu, L.Ya.Glozman

The Short-Range Baryon-Baryon Interaction in a Chiral Constituent Quark Model

doi: 10.1016/S0375-9474(00)00461-9
Citations: PlumX Metrics


2001WA12      Nucl.Phys. A684, 284c (2001)

R.F.Wagenbrunn, L.Ya.Glozman, W.Plessas, K.Varga

Extended Goldstone-Boson-Exchange Chiral Quark Model

doi: 10.1016/S0375-9474(01)00422-5
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2000GL01      Phys.Rev. D61, 074008 (2000)

L.Ya.Glozman, K.Varga

Is There Diquark Clustering in the Nucleon ?

doi: 10.1103/PhysRevD.61.074008
Citations: PlumX Metrics


2000GL03      Nucl.Phys. A663-664, 103c (2000)

L.Ya.Glozman

Origins of the Baryon Spectrum

doi: 10.1016/S0375-9474(99)00578-3
Citations: PlumX Metrics


2000GL07      Phys.Lett. 494B, 58 (2000)

L.Ya.Glozman

Chiral Aspects of Baryon Structure in the Quark Model

doi: 10.1016/S0370-2693(00)01170-9
Citations: PlumX Metrics


2000HA10      Nucl.Phys. A665, 353 (2000)

L.Hannelius, D.O.Riska, L.Ya.Glozman

The Strangeness Magnetic Moment of the Proton in the Chiral Quark Model

NUCLEAR STRUCTURE 1H; calculated the strangeness magnetic moment. Comparison with experimental value.

doi: 10.1016/S0375-9474(99)00812-X
Citations: PlumX Metrics


2000SH13      Phys.Lett. 477B, 59 (2000)

K.Shimizu, L.Ya.Glozman

On the Origin of the Short Range NN Repulsion

doi: 10.1016/S0370-2693(00)00230-6
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2000WA08      Nucl.Phys. A666-667, 29c (2000)

R.F.Wagenbrunn, L.Ya.Glozman, W.Plessas, K.Varga

Extension of the GBE Chiral Constituent Quark Model

doi: 10.1016/S0375-9474(00)00006-3
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2000WA11      Nucl.Phys. A663-664, 703c (2000)

R.F.Wagenbrunn, L.Ya.Glozman, W.Plessas, K.Varga

Extended Goldstone-Boson-Exchange Constituent Quark Model

doi: 10.1016/S0375-9474(99)00726-5
Citations: PlumX Metrics


1999GL03      Phys.Lett. 459B, 49 (1999)

L.Ya.Glozman, D.O.Riska

Pionic Fluctuations of Constituent Quarks and the Neutron Charge Radius

NUCLEAR STRUCTURE 1n; calculated contributions to charge radius.

doi: 10.1016/S0370-2693(99)00718-2
Citations: PlumX Metrics


1998GL02      Nucl.Phys. A629, 121c (1998)

L.Ya.Glozman

Baryons, Their Interactions and the Chiral Symmetry of QCD

doi: 10.1016/S0375-9474(97)00675-1
Citations: PlumX Metrics


1998GL04      Nucl.Phys. A631, 469c (1998)

L.Ya.Glozman, W.Plessas, K.Varga, R.F.Wagenbrunn

Light and Strange Baryons in a Chiral Quark Model with Goldstone-Boson-Exchange Interactions

doi: 10.1016/S0375-9474(98)00049-9
Citations: PlumX Metrics


1998GL05      Phys.Rev. C57, 3406 (1998); Comments Phys.Rev. C61, 019803 (1999)

L.Ya.Glozman, Z.Papp, W.Plessas, K.Varga, R.F.Wagenbrunn

Effective Q-Q Interactions in Constituent Quark Models

doi: 10.1103/PhysRevC.57.3406
Citations: PlumX Metrics


1998GL09      Nucl.Phys. A639, 65c (1998)

L.Ya.Glozman

Light and Strange Baryons, Two-Baryon Systems and the Chiral Symmetry of QCD

doi: 10.1016/S0375-9474(98)00252-8
Citations: PlumX Metrics


1997DA05      Nucl.Phys. A616, 555 (1997)

K.Dannbom, L.Ya.Glozman, C.Helminen, D.O.Riska

Baryon Magnetic Moments and Axial Coupling Constants with Relativistic and Exchange Current Effects

NUCLEAR STRUCTURE 1H, 1n; calculated μ. Relativistic, exchange current effects.

doi: 10.1016/S0375-9474(97)00005-5
Citations: PlumX Metrics


1997GL04      Nucl.Phys. A623, 90c (1997)

L.Ya.Glozman, Z.Papp, W.Plessas, K.Varga, R.F.Wagenbrunn

Light and Strange Baryons in a Chiral Constituent-Quark Model

doi: 10.1016/S0375-9474(97)00426-0
Citations: PlumX Metrics


1997ST24      Phys.Rev. C56, 2779 (1997); Erratum Phys.Rev. C59, 1219 (1999)

F.Stancu, S.Pepin, L.Ya.Glozman

Nucleon-Nucleon Interaction in a Chiral Constituent Quark Model

doi: 10.1103/PhysRevC.56.2779
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1996GL02      Nucl.Phys. A603, 326 (1996); Erratum Nucl.Phys. A620, 510 (1997)

L.Ya.Glozman, D.O.Riska

The Charm and Bottom Hyperons in a Chiral Quark Model

doi: 10.1016/0375-9474(96)80005-C
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1996GL03      Phys.Rep. 268, 263 (1996)

L.Ya.Glozman, D.O.Riska

The Spectrum of the Nucleons and the Strange Hyperons and Chiral Dynamics

doi: 10.1016/0370-1573(95)00062-3
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1996KO21      Yad.Fiz. 59, No 5, 833 (1996); Phys.Atomic Nuclei 59, 795 (1996)

A.P.Kobushkin, A.I.Syamtomov, L.Ya.Glozman

Quark-Exchange Effects in Deuteron Breakup at Intermediate Energies

NUCLEAR REACTIONS 1H(polarized d, p), E at ≤ 1 GeV/c; analyzed data; deduced quark exchange effects in deuteron breakup. Microscopic approach.


1995GL02      Phys.Lett. 348B, 270 (1995)

L.Ya.Glozman, A.Faessler

Quark-Exchange Versus Meson-Exchange in d(e, e'p)Δ

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
Citations: PlumX Metrics


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