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NSR database version of May 19, 2024.

Search: Author = M.G.Mustafa

Found 63 matches.

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2018IK01      Phys.Rev. C 98, 034915 (2018)

A.Ikbal Sheikh, Z.Ahammed, P.Shukla, M.G.Mustafa

Effect of the chromo-electromagnetic field fluctuations on heavy quark propagation in a deconfined hadronic medium at energies available at the CERN Large Hadron Collider

doi: 10.1103/PhysRevC.98.034915
Citations: PlumX Metrics


2011GR03      Phys.Rev. C 83, 014908 (2011)

C.Greiner, N.Haque, M.G.Mustafa, M.H.Thoma

Low-mass dilepton rate from the deconfined phase

doi: 10.1103/PhysRevC.83.014908
Citations: PlumX Metrics


2011HA30      Nucl.Phys. A862-863, 271c (2011)

N.Haque, M.G.Mustafa

Quark Number Susceptibility and Thermodynamics in HTL approximation

doi: 10.1016/j.nuclphysa.2011.05.070
Citations: PlumX Metrics


2009AB29      Phys.Rev. C 80, 051903 (2009)

R.Abir, M.G.Mustafa

Color-singlet clustering of partons and recombination model for hadronization of quark-gluon plasma

doi: 10.1103/PhysRevC.80.051903
Citations: PlumX Metrics


2008QI02      Phys.Rev.Lett. 100, 072301 (2008)

G.-Y.Qin, J.Ruppert, C.Gale, S.Jeon, G.D.Moore, M.G.Mustafa

Radiative and Collisional Jet Energy Loss in the Quark-Gluon Plasma at the BNL Relativistic Heavy Ion Collider

doi: 10.1103/PhysRevLett.100.072301
Citations: PlumX Metrics


2007CH52      Phys.Rev. C 75, 064908 (2007)

P.Chakraborty, M.G.Mustafa, M.H.Thoma

Energy gain of heavy quarks by fluctuations in a quark-gluon plasma

doi: 10.1103/PhysRevC.75.064908
Citations: PlumX Metrics


2006CH53      Phys.Rev. D 74, 094002 (2006)

P.Chakraborty, M.G.Mustafa, M.H.Thoma

Wakes in the quark-gluon plasma

doi: 10.1103/PhysRevD.74.094002
Citations: PlumX Metrics


2006MU13      Pramana 66, 669 (2006)

M.G.Mustafa

Some applications of thermal field theory to quark-gluon plasma

doi: 10.1007/BF02704799
Citations: PlumX Metrics


2005MU03      Phys.Rev. C 71, 017901 (2005)

M.G.Mustafa, M.H.Thoma, P.Chakraborty

Screening of a moving parton in the quark-gluon plasma

doi: 10.1103/PhysRevC.71.017901
Citations: PlumX Metrics


2005MU23      Phys.Rev. C 72, 014905 (2005); Erratum Phys.Rev. C 74, 019902 (2006)

M.G.Mustafa

Energy loss of charm quarks in the quark-gluon plasma: Collisional vs radiative losses

doi: 10.1103/PhysRevC.72.014905
Citations: PlumX Metrics


2003MU14      Pramana 60, 711 (2003)

M.G.Mustafa, M.H.Thoma

Can van Hove singularities be observed in relativistic heavy-ion collisions?

doi: 10.1007/BF02705170
Citations: PlumX Metrics


2003PA26      Pramana 60, 1083 (2003)

D.Pal, A.Sen, M.G.Mustafa, D.K.Srivastava

The extent of strangeness equilibration in quark gluon plasma

doi: 10.1007/BF02707035
Citations: PlumX Metrics


2002PA11      Phys.Rev. C65, 034901 (2002)

D.Pal, A.Sen, M.G.Mustafa, D.K.Srivastava

Evolution of Strangeness in a Equilibrating and Expanding Quark-Gluon Plasma

doi: 10.1103/PhysRevC.65.034901
Citations: PlumX Metrics


2002TA23      Nucl.Instrum.Methods Phys.Res. B196, 215 (2002)

F.Tarkanyi, F.Ditroi, S.Takacs, M.Al-Abyad, M.G.Mustafa, Yu.Shubin, Y.Zhuang

New data and evaluation of 3He-induced nuclear reactions on Cu

NUCLEAR REACTIONS Cu(3He, X)66Ga/67Ga/63Zn/65Zn, E ≈ 3-36 MeV; measured production σ. Stacked-foil activation, comparison with previous results.

doi: 10.1016/S0168-583X(02)01286-7
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4109.


2001SZ02      Nucl.Instrum.Methods Phys.Res. B174, 47 (2001)

F.Szelecsenyi, F.Tarkanyi, S.Takacs, A.Hermanne, M.Sonck, Yu.Shubin, M.G.Mustafa, Y.Zhuang

Excitation Function for the natTi(p, x)48V Nuclear Process: Evaluation and new measurements for practical applications

NUCLEAR REACTIONS Ti(p, X)48V, E=6-18 MeV; Cu(p, X)62Zn/63Zn/65Zn, E=6-18 MeV; Ni(p, X)57Ni, E=15-18 MeV; measured σ. Stacked-foil activation, comparisons with previous results.

doi: 10.1016/S0168-583X(00)00516-4
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4083.


2001TA08      Nucl.Instrum.Methods Phys.Res. B174, 235 (2001)

S.Takacs, F.Szelecsenyi, F.Tarkanyi, M.Sonck, A.Hermanne, Yu.Shubin, A.Dityuk, M.G.Mustafa, Y.Zhuang

New Cross-Sections and Intercomparison of Deuteron Monitor Reactions on Al, Ti, Fe, Ni and Cu

NUCLEAR REACTIONS 27Al(d, X)22Na/24Na, E=13-50 MeV; Ti(d, X)48V, E=7-50 MeV; Fe(d, X)56Co, E=10-50 MeV; Ni(d, X)61Cu, E=10-50 MeV; Cu(d, X)65Zn, E=5-50 MeV; measured σ. Stacked foil activation method. COmparisons with previous results, model predictions. Recommended values given.

doi: 10.1016/S0168-583X(00)00589-9
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4081.


2000DI15      Nucl.Instrum.Methods Phys.Res. B168, 337 (2000)

F.Ditroi, F.Tarkanyi, M.A.ALi, L.Ando, S.-J.Heselius, Yu.Shubin, Y.Zhuang, M.G.Mustafa

Investigation of 3He-Induced Reactions on Natural Ti for Nuclear Analytical and Radionuclide Production Purposes

NUCLEAR REACTIONS Ti(3He, X)43Sc/44mSc/46Sc/47Sc/48Sc/48V/48Cr/49Cr/51Cr, E=2-36 MeV; measured excitation functions. Stacked-foil activation technique. Comparisons with previous results. Application to wear measurement discussed.

doi: 10.1016/S0168-583X(99)01200-8
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4091.


2000MU02      Phys.Lett. 472B, 402 (2000)

M.G.Mustafa, A.Schafer, M.H.Thoma

Gluon Condensate and Non-Perturbative Quark-Photon Vertex

doi: 10.1016/S0370-2693(99)01441-0
Citations: PlumX Metrics


2000MU03      Phys.Rev. C61, 024902 (2000)

M.G.Mustafa, A.Schafer, M.H.Thoma

Nonperturbative Dilepton Production from a Quark-Gluon Plasma

doi: 10.1103/PhysRevC.61.024902
Citations: PlumX Metrics


2000MU14      Phys.Rev. C62, 014902 (2000); Erratum Phys.Rev. C63, 069902 (2001)

M.G.Mustafa, M.H.Thoma

Bremsstrahlung from an Equilibrating Quark-Gluon Plasma

doi: 10.1103/PhysRevC.62.014902
Citations: PlumX Metrics


2000PA34      Int.J.Mod.Phys. E9, 149 (2000)

L.Paria, A.Abbas, M.G.Mustafa

Surface Tension at Finite Temperature in the MIT Bag Model

doi: 10.1016/S0218-3013(00)00008-8
Citations: PlumX Metrics


2000TA18      Nucl.Instrum.Methods Phys.Res. B168, 144 (2000)

F.Tarkanyi, F.Szelecsenyi, S.Takacs, A.Hermanne, M.Sonck, A.Thielemans, M.G.Mustafa, Yu.Shubin, Y.Zhuang

New Experimental Data, Compilation and Evaluation for the natCu(α, x)66Ga, natCu(α, x)67Ga and natCu(α, x)65Zn Monitor Reactions

NUCLEAR REACTIONS Cu(α, X)66Ga/67Ga/65Zn, E=7-40 MeV; measured σ. Stacked-foil activation technique. Comparisons with previous results.

doi: 10.1016/S0168-583X(99)00877-0
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD4085.


1999MU24      Nucl.Phys. A661, 653c (1999)

M.G.Mustafa, A.Schafer, M.H.Thoma

Gluon Condensate, Quark Propagation, and Dilepton Production in the Quark-Gluon Plasma

doi: 10.1016/S0375-9474(99)85110-0
Citations: PlumX Metrics


1999MU25      Eur.Phys.J. C 11, 729 (1999)

M.G.Mustafa, A.Sen, L.Paria

Hadronic Modes in the Quark Plasma with an Internal Symmetry

doi: 10.1007/s100520050669
Citations: PlumX Metrics


1999PA34      Phys.Rev. C60, 034905 (1999)

D.Pal, M.G.Mustafa

Soft Electromagnetic Radiations from an Equilibrating Quark-Gluon Plasma

NUCLEAR REACTIONS 197Au(197Au, X), E=high; calculated bremsstrahlung dileptons transverse, invariant mass distributions, soft photons transverse momenta from equilibrating quark-gluon plasma.

doi: 10.1103/PhysRevC.60.034905
Citations: PlumX Metrics


1998MU03      Phys.Rev. C57, 889 (1998); Erratum Phys.Rev. C57, 3499 (1998)

M.G.Mustafa, D.Pal, D.K.Srivastava

Propagation of Charm Quarks in Equilibrating Quark-Gluon Plasma

NUCLEAR REACTIONS 197Au(197Au, X), E=high; calculated quark-gluon plasma charm quark propagation related features; deduced drag, diffusion coefficients. Parton cascade model.

doi: 10.1103/PhysRevC.57.889
Citations: PlumX Metrics


1998MU13      Phys.Lett. 428B, 234 (1998); Erratum Phys.Lett. 438B, 450 (1998)

M.G.Mustafa, D.Pal, D.K.Srivastava, M.Thoma

Radiative Energy-Loss of Heavy Quarks in a Quark-Gluon Plasma

doi: 10.1016/S0370-2693(98)00429-8
Citations: PlumX Metrics


1997MU07      Phys.Rev. C55, 2005 (1997)

M.G.Mustafa, A.Ansari

Color-Singlet Strangelets at Finite Temperature

doi: 10.1103/PhysRevC.55.2005
Citations: PlumX Metrics


1997MU16      Phys.Rev. C56, 420 (1997)

M.G.Mustafa, A.Ansari

Deformed Strangelets at Finite Temperature

NUCLEAR STRUCTURE A ≤ 100; calculated baryon energy per particle vs deformation parameter; deduced color-singlet strangelets stability related features. Massless quarks confined in axially symmetric quadrupole shape deformable bag.

doi: 10.1103/PhysRevC.56.420
Citations: PlumX Metrics


1997MU35      Acta Phys.Hung.N.S. 5, 387 (1997)

B.Muller, M.G.Mustafa, D.K.Srivastava

Expanding Quark-Gluon Plasmas

NUCLEAR REACTIONS 197Au(197Au, X), E=high; calculated quark-gluon plasma features.


1997PA37      Int.J.Mod.Phys. E6, 633 (1997)

L.Paria, M.G.Mustafa, A.Abbas

A Gluon Plasma Giant Resonance at Finite Temperature

doi: 10.1142/S0218301397000305
Citations: PlumX Metrics


1997SR01      Phys.Lett. 396B, 45 (1997)

D.K.Srivastava, M.G.Mustafa, B.Muller

Chemical Equilibration of an Expanding Quark-Gluon Plasma

NUCLEAR REACTIONS 197Au(197Au, X), E=relativistic; calculated transversely expanding quark-gluon plasma constant energy density contours, other aspects; deduced chemical equilibration related features.

doi: 10.1016/S0370-2693(97)00090-7
Citations: PlumX Metrics


1997SR02      Phys.Rev. C56, 1064 (1997)

D.K.Srivastava, M.G.Mustafa, B.Muller

Expanding Quark-Gluon Plasmas: Transverse flow, chemical equilibration, and electromagnetic radiation

NUCLEAR REACTIONS 197Au(197Au, X), E ≥ 100 GeV/nucleon; calculated energy density of expanding quark-gluon plasma, other features; deduced evolution vs initial conditions, post-quark-gluon plasma implications. Self screened parton cascade model based inital conditions, parton plasma explanations.

doi: 10.1103/PhysRevC.56.1064
Citations: PlumX Metrics


1994MU06      Phys.Rev. C49, 2602 (1994)

M.G.Mustafa, M.Blann, G.Peilert, A.Botvina

Comparison of Fast Cascade Plus Statistical Models for Heavy Ion Induced Multifragmentation Reactions

NUCLEAR REACTIONS 197Au(36Ar, X), E=35-110 MeV/nucleon; calculated neutron, proton kinetic energy, neutron multiplicity averaged up to time t. Fast cascade plus statistical models.

doi: 10.1103/PhysRevC.49.2602
Citations: PlumX Metrics


1993BO15      Z.Phys. A345, 297 (1993)

A.Botvina, I.N.Mishustin, M.Blann, M.G.Mustafa, G.Peilert, H.Stocker, W.Greiner

Mechanisms of Fragment Production in Heavy-Ion Reactions at Intermediate Energies

NUCLEAR STRUCTURE 100Ru; calculated total excitation energy, entropy per nucleon vs temperature, fragment charge yields. Three models of nuclear disintegration.

doi: 10.1007/BF01280837
Citations: PlumX Metrics


1993MU10      Phys.Rev. C48, 588 (1993)

M.G.Mustafa, M.Blann, A.V.Ignatyuk

Realistic Level Densities in Fragment Emission at High Excitation Energies

NUCLEAR STRUCTURE 100Ru; calculated fragment (Z ≤ 14) yields; deduced level density models dependence.

doi: 10.1103/PhysRevC.48.588
Citations: PlumX Metrics


1993PA13      Z.Phys. A345, 343 (1993)

V.Paar, D.K.Sunko, S.Brant, M.G.Mustafa, R.G.Lanier

Gaussian Polynomial Method for Spin-Dependent Level Density and New Formula for Spin Distribution

NUCLEAR STRUCTURE 114Cd, 244Am; calculated level density, spin distributions. Gaussian polynomial generating function method.

doi: 10.1007/BF01282895
Citations: PlumX Metrics


1993WE02      Phys.Rev. C47, 248 (1993)

H.I.West, Jr., R.M.Nuckolls, B.Hudson, B.Ruiz, R.G.Lanier, M.G.Mustafa

Bromine and Iodine Excitation-Function Measurements with Protons and Deuterons at 3-17 MeV

NUCLEAR REACTIONS, ICPND 81,79Br, 127I(p, n), (d, 2n), E=threshold-17 MeV; measured σ(E); deduced suitable level density prescription. Exciton preequilibrium model, microscopic breakup fusion approach for (d, 2n) reactions. Stacked foil technique.

doi: 10.1103/PhysRevC.47.248
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0151.


1992MU01      Phys.Rev. C45, 1078 (1992)

M.G.Mustafa, M.Blann, A.V.Ignatyuk, S.M.Grimes

Nuclear Level Densities at High Excitations

NUCLEAR STRUCTURE 20Ne, 40Ca, 100Ru; calculated level densities. Fermi gas formulas, thermodynamic methods, shell model single particle levels.

doi: 10.1103/PhysRevC.45.1078
Citations: PlumX Metrics


1992PE08      Phys.Rev. C46, 1457 (1992)

G.Peilert, J.Konopka, H.Stocker, W.Greiner, M.Blann, M.G.Mustafa

Dynamical Treatment of Fermi Motion in a Microscopic Description of Heavy Ion Collisions

NUCLEAR REACTIONS Zr, Pb, 27Al(p, xn), E=80-800 MeV; analyzed σ(θ, En). Quantum molecular dynamics model.

doi: 10.1103/PhysRevC.46.1457
Citations: PlumX Metrics


1991BL06      Phys.Rev. C44, 431 (1991)

M.Blann, M.G.Mustafa, G.Peilert, H.Stocker, W.Greiner

Expectations of Fragment Decay from Highly Excited Nuclei

NUCLEAR STRUCTURE 100Ru; calculated primary, cluster yields for deexcitation cascade; deduced excitation energy dependence. Statistical model.

doi: 10.1103/PhysRevC.44.431
Citations: PlumX Metrics


1991BL08      Phys.Rev. C44, R590 (1991)

M.Blann, M.G.Mustafa

Multifragmentation for 36Ar + 238U Treated as Statistical Dynamic Interaction Processes

NUCLEAR REACTIONS 238U(36Ar, X), E=35 MeV/nucleon; calculated exclusive multi-fragment multiplicities. Fast cascade, Boltzmann master equation.

doi: 10.1103/PhysRevC.44.R590
Citations: PlumX Metrics


1991WE02      Phys.Rev. C43, 1352 (1991)

H.I.West, Jr., M.G.Mustafa, R.G.Lanier, H.O'Brien

Interpretation of Ion-Range Recoil Data Obtained from Activated-Foil Measurements of Nuclear Excitation Functions

NUCLEAR REACTIONS 89Y, 48Ti, 52Cr(p, n), (d, 2n), 89Y(p, 2n), 47Ti(d, n), 48Ti(d, 2n), 46,47,48Ti(t, n), (t, 2n), (t, 3n), 48Ti(t, α), 50Cr(d, α), E ≤ 40 MeV; measured recoil ion ranges vs projectile energy; deduced σ(recoil ion θ); deduced breakup, pickup, multi-step mechanisms roles. Activated foil method.

doi: 10.1103/PhysRevC.43.1352
Citations: PlumX Metrics


1990LA11      Phys.Rev. C42, R479 (1990)

R.G.Lanier, H.I.West, Jr., M.G.Mustafa, J.Frehaut, A.Adam, C.A.Philis

Effects of Nuclear Deformation on 151,153Eu(p, n)151,153Gd Reactions

NUCLEAR REACTIONS, ICPND 151,153Eu(p, n), E=5-12 MeV; measured σ(E); deduced target shape difference role.

doi: 10.1103/PhysRevC.42.R479
Citations: PlumX Metrics


1990MA42      Phys.Rev. C42, 683 (1990)

R.C.Mastroleo, T.Udagawa, M.G.Mustafa

Calculations of Complete Fusion, Incomplete Fusion, and Direct Reaction Cross Sections for Deuteron-Induced Reactions

NUCLEAR REACTIONS 93Nb(d, p), E=15, 25.5 MeV; calculated σ(Ep, θp), angle integrated σ. Microscopic breakup-fusion, direct-reaction theories.

doi: 10.1103/PhysRevC.42.683
Citations: PlumX Metrics


1990MA58      Phys.Lett. 245B, 329 (1990)

R.C.Mastroleo, T.Udagawa, M.G.Mustafa

Dynamical Calculations of Linear Momentum Transfer in α-Induced Reactions

NUCLEAR REACTIONS, ICPND 59Co(α, X), E=80 MeV; calculated reaction σ for X=n, p, d, 3He, t, 2p, 2n, α. Dynamical model.

doi: 10.1016/0370-2693(90)90653-N
Citations: PlumX Metrics


1988MU18      Phys.Rev. C38, 1624 (1988)

M.G.Mustafa, H.I.West, Jr., H.O'Brien, R.G.Lanier, M.Benhamou, T.Tamura

Measurements and a Direct-Reaction - Plus - Hauser-Feshbach Analysis of 89Y(p, n)89Zr, 89Y(p, 2n)88Zr, and 89Y(p, pn)88Y Reactions up to 40 MeV

NUCLEAR REACTIONS, ICPND 89Y(p, n), (p, 2n), (p, np), E=4.59-39.56 MeV; measured σ(E); deduced reaction mechanism. Foil activation method. Hauser-Feshbach calculation, one-, two-step direct reactions, preequilibrium model analyses.

doi: 10.1103/PhysRevC.38.1624
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0403.


1987FO02      Nucl.Sci.Eng. 95, 128 (1987)

K.A.Foland, R.J.Borg, M.G.Mustafa

The Production of 38Ar and 39Ar by 14-MeV Neutrons on 39K

NUCLEAR REACTIONS 39K(n, p), (n, np), E ≈ 14 MeV; measured residual production σ. Mass spectrometric techniques.

doi: 10.13182/NSE87-A20423
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset13109.


1987MU08      Phys.Rev. C35, 2077 (1987)

M.G.Mustafa, T.Tamura, T.Udagawa

Direct-Reaction Plus Statistical-Model Analysis of the 52Cr(d, 2n)52gMn, 52mMn Reaction

NUCLEAR REACTIONS, ICPND 52Cr(d, 2n), E=8-20 MeV; calculated residual production σ(E), isomer ratios. Direct reaction plus statistical model analyses.

doi: 10.1103/PhysRevC.35.2077
Citations: PlumX Metrics


1987WE05      Phys.Rev. C35, 2067 (1987)

H.I.West, Jr., R.G.Lanier, M.G.Mustafa

52Cr(p, n)52gMn, 52mMn and 52Cr(d, 2n)52gMn, 52mMn Excitation Functions

NUCLEAR REACTIONS, ICPND Cr(p, X)52Mn/52mMn, 52Cr(p, n), E=6-27 MeV; 52Cr(d, 2n), E=8-20 MeV; measured residual production σ(E), isomer ratios. Activation method. Statistical model calculations.

doi: 10.1103/PhysRevC.35.2067
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0336.


1985MC03      Phys.Rev.Lett. 54, 1995 (1985)

M.A.McMahan, L.G.Moretto, M.L.Padgett, G.J.Wozniak, L.G.Sobotka, M.G.Mustafa

Mass-Asymmetric Barriers from Excitation Functions for Complex-Fragment Emission

NUCLEAR REACTIONS Ag(3He, X), E(cm) ≈ 40-140 MeV; measured σ(E) for X=α, Li, Be, C, B, N, O, Ne, F, Na; deduced emission barriers, level density parameter ratios.

doi: 10.1103/PhysRevLett.54.1995
Citations: PlumX Metrics


1982MU04      Phys.Rev. C25, 2524 (1982)

M.G.Mustafa, P.A.Baisden, H.Chandra

Equilibrium Shapes and Fission Barriers of Rotating Nuclei with a Macroscopic Two-Center Model

NUCLEAR STRUCTURE 50V, 97Rh, 153Tb, 176Os; calculated equilibrium shapes, fission barriers, critical (L). Rotating nuclei, macroscopic two center model.

doi: 10.1103/PhysRevC.25.2524
Citations: PlumX Metrics


1982WI08      Phys.Rev. C26, 1531 (1982)

J.F.Wild, E.K.Hulet, R.W.Lougheed, P.A.Baisden, J.H.Landrum, R.J.Dougan, M.G.Mustafa

Unusually Low Fragment Energies in the Symmetric Fission of 259Md

RADIOACTIVITY 259No(EC), (α) [from 248Cm(18O, 3nα)]; measured α-decay T1/2. 259Md(SF) [from 259No(EC-decay)]; measured T1/2, (fragment)(fragment)-coin; deduced SF-decay upper limit, fragment mass, total kinetic energy distributions.

doi: 10.1103/PhysRevC.26.1531
Citations: PlumX Metrics


1976MU10      Phys.Rev. C14, 2168 (1976)

M.G.Mustafa

Strongly Damped Heavy-Ion Collisions: Microscopic Calculation of the Kinetic-Energy Loss in Rapid Stretching

NUCLEAR REACTIONS 209Bi, 232Th(40Ar, X), (84Kr, X), (136Xe, X); calculated internal excitation in strongly damped collisions.

doi: 10.1103/PhysRevC.14.2168
Citations: PlumX Metrics


1975MU03      Phys.Rev. C11, 1059 (1975)

M.G.Mustafa

Transition from Mass Asymmetry to Symmetry in the Spontaneous Fission of Fm Isotopes

RADIOACTIVITY, Fission 252,256,258,264Fm(SF); calculated shell corrections, potential energy surfaces.

doi: 10.1103/PhysRevC.11.1059
Citations: PlumX Metrics


1975MU11      Phys.Rev. C12, 1638 (1975)

M.G.Mustafa, K.Kumar

Effects of Rotation on the Stability of Nuclei under Fission and the Possibility of Fusion in Heavy-Ion Reactions

NUCLEAR STRUCTURE 208Pb, 240Pu, 298Fl; calculated rotational effects in compound nuclei following fission, fusion.

doi: 10.1103/PhysRevC.12.1638
Citations: PlumX Metrics


1975MU14      Phys.Lett. 60B, 15 (1975)

M.G.Mustafa

A New Mechanism for the Kinetic Energy Loss in Strongly Damped Heavy-Ion Collisions

NUCLEAR REACTIONS 209Bi(84Kr, X); calculated interaction, energy loss. Microscopic model.

doi: 10.1016/0370-2693(75)90515-8
Citations: PlumX Metrics


1974MU08      Phys.Lett. 49B, 405 (1974)

M.G.Mustafa, K.Kumar

Angular Momentum Dependence of Moments of Inertia and Fission Barriers Of 240Pu

NUCLEAR STRUCTURE 240Pu; calculated moments of inertia.

doi: 10.1016/0370-2693(74)90619-4
Citations: PlumX Metrics


1973MU03      Phys.Rev. C7, 1519 (1973)

M.G.Mustafa, U.Mosel, H.W.Schmitt

Asymmetry in Nuclear Fission

NUCLEAR STRUCTURE 202Pb, 210Po, 236U, 248Cm, 252,258,264Fm calculated potential energies based on two-center model with asymmetric deformations.

doi: 10.1103/PhysRevC.7.1519
Citations: PlumX Metrics


1973MU16      Phys.Rev. C8, 1924 (1973)

M.G.Mustafa, H.W.Schmitt

Potential-Energy Surface for the Fission of the Superheavy Nucleus 298X

NUCLEAR REACTIONS 298Fl(n, F), (p, F); calculated potential energy surface.

doi: 10.1103/PhysRevC.8.1924
Citations: PlumX Metrics


1972MU06      Phys.Rev.Lett. 28, 1536 (1972)

M.G.Mustafa, U.Mosel, H.W.Schmitt

Asymmetric Fission in the Two-Center Model

NUCLEAR STRUCTURE 252,258,264Fm, 236U; calculated 4-dimensional potential energy surfaces. 2-center model.

doi: 10.1103/PhysRevLett.28.1536
Citations: PlumX Metrics


1971MU21      Nucl.Phys. A178, 9 (1971)

M.G.Mustafa, H.W.Schmitt, U.Mosel

Dipole Excitations in Fission Fragments

NUCLEAR REACTIONS, Fission 235U(n, F), E=thermal; calculated fragment dipole excitations at scission points.

doi: 10.1016/0375-9474(71)90180-1
Citations: PlumX Metrics


1970MU20      Phys.Rev. C2, 2068 (1970)

M.G.Mustafa, F.B.Malik

Evidence of E2 and M1 Transitions in High-Energy Photonuclear Reactions in O16

NUCLEAR REACTIONS 16O(γ, n), (γ, p), E=20-50 MeV; calculated σ(E;θ), P; deduced E2, M1 transition interference.

doi: 10.1103/PhysRevC.2.2068
Citations: PlumX Metrics


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