NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = M.Mustafa Found 78 matches. 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
2017SA47 Phys.Rev. C 96, 021301 (2017) B.Saygi, D.T.Joss, R.D.Page, T.Grahn, J.Simpson, D.O'Donnell, G.Alharshan, K.Auranen, T.Back, S.Boening, T.Braunroth, R.J.Carroll, B.Cederwall, D.M.Cullen, A.Dewald, M.Doncel, L.Donosa, M.C.Drummond, F.Ertugral, S.Erturk, C.Fransen, P.T.Greenlees, M.Hackstein, K.Hauschild, A.Herzan, U.Jakobsson, P.M.Jones, R.Julin, S.Juutinen, J.Konki, T.Kroll, M.Labiche, A.Lopez-Martens, C.G.McPeake, F.Moradi, O.Moller, M.Mustafa, P.Nieminen, J.Pakarinen, J.Partanen, P.Peura, M.Procter, P.Rahkila, W.Rother, P.Ruotsalainen, M.Sandzelius, J.Saren, C.Scholey, J.Sorri, S.Stolze, M.J.Taylor, A.Thornthwaite, J.Uusitalo Reduced transition probabilities along the yrast line in 166W NUCLEAR REACTIONS 92Mo(78Kr, 4p), E=380 MeV; measured Eγ, Iγ, γγ-coin correlated with implanted recoils, level half-lives by recoil-distance and differential decay curve method (DDCM) using RITU gas-filled separator, GREAT focal-plane spectrometer, DPUNS plunger system and JURGAM-II array at Jyvaskyla accelerator facility. 166W; deduced levels, J, π, yrast band, B(E2), B(E2) ratios and compared with theoretical predictions for an axially deformed rotor. Systematics of energies and B(E2) values for the first 2+, 4+ and 6+ states in A=160-190 even-A W isotopes.
doi: 10.1103/PhysRevC.96.021301
2016MU11 Nucl.Phys. A956, 43 (2016) M.Mustafa, for the STAR Collaboration Overview of recent results from the STAR experiment
doi: 10.1016/j.nuclphysa.2016.02.023
2013MU03 Nucl.Phys. A904-905, 665c (2013) M.Mustafa, for the STAR Collaboration Measurements of Non-photonic Electron Production and Azimuthal Anisotropy in √ sNN=39, 62.4and200GeV Au + Au Collisions from STAR at RHIC
doi: 10.1016/j.nuclphysa.2013.02.103
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
2011HA30 Nucl.Phys. A862-863, 271c (2011) Quark Number Susceptibility and Thermodynamics in HTL approximation
doi: 10.1016/j.nuclphysa.2011.05.070
2011MU19 Phys.Rev. C 84, 054320 (2011) M.Mustafa, J.Ollier, J.Simpson, M.A.Riley, E.S.Paul, X.Wang, A.Aguilar, M.P.Carpenter, I.G.Darby, D.J.Hartley, R.V.F.Janssens, F.G.Kondev, T.Lauritsen, P.J.Nolan, M.Petri, J.M.Rees, J.P.Revill, S.V.Rigby, C.Teal, J.Thomson, C.Unsworth, S.Zhu, B.G.Carlsson, H.L.Ma, T.Mufti, I.Ragnarsson Diverse collective excitations in 159Er up to high spin NUCLEAR REACTIONS 116Cd(48Ca, 5n), E=215 MeV; measured Eγ, Iγ, γγ-coin, γ(θ) using Gammasphere array. 159Er; deduced levels, J, π, multipolarities, bands, triaxial SD band, configurations, alignment plots, band termination, oblate structures, unpaired band crossings; calculated potential energy surfaces. Comparison with cranked Nilsson-Strutinsky (CNS) calculations. systematics of γ-vibrational states in N=88-94 Er nuclei.
doi: 10.1103/PhysRevC.84.054320
2009AB29 Phys.Rev. C 80, 051903 (2009) Color-singlet clustering of partons and recombination model for hadronization of quark-gluon plasma
doi: 10.1103/PhysRevC.80.051903
2009PA40 Phys.Rev. C 80, 054312 (2009) E.S.Paul, J.P.Revill, M.Mustafa, S.V.Rigby, A.J.Boston, C.Foin, J.Genevey, A.Gizon, J.Gizon, I.M.Hibbert, D.T.Joss, P.J.Nolan, B.M.Nyako, N.J.O'Brien, C.M.Parry, A.T.Semple, S.L.Shepherd, J.Timar, R.Wadsworth, L.Zolnai High-spin states in 127Ce and 129Ce: Further evidence for triaxial nuclear shapes NUCLEAR REACTIONS 100Mo(32S, 5n), (34S, 5n), E=155 MeV; measured Eγ, Iγ, γγ-coin using Euroball and Eurogam arrays. 127,129Ce; deduced levels, J, π, bands, and configurations. Comparison with cranked Woods-Saxon calculations, and with systematics of light odd-N cerium nuclei.
doi: 10.1103/PhysRevC.80.054312
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
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
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
2006MU13 Pramana 66, 669 (2006) Some applications of thermal field theory to quark-gluon plasma
doi: 10.1007/BF02704799
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
2005MU23 Phys.Rev. C 72, 014905 (2005); Erratum Phys.Rev. C 74, 019902 (2006) Energy loss of charm quarks in the quark-gluon plasma: Collisional vs radiative losses
doi: 10.1103/PhysRevC.72.014905
2003MU14 Pramana 60, 711 (2003) Can van Hove singularities be observed in relativistic heavy-ion collisions?
doi: 10.1007/BF02705170
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
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
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
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
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
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
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
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
2000MU14 Phys.Rev. C62, 014902 (2000); Erratum Phys.Rev. C63, 069902 (2001) Bremsstrahlung from an Equilibrating Quark-Gluon Plasma
doi: 10.1103/PhysRevC.62.014902
2000PA34 Int.J.Mod.Phys. E9, 149 (2000) Surface Tension at Finite Temperature in the MIT Bag Model
doi: 10.1016/S0218-3013(00)00008-8
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
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
1999MU25 Eur.Phys.J. C 11, 729 (1999) Hadronic Modes in the Quark Plasma with an Internal Symmetry
doi: 10.1007/s100520050669
1999PA34 Phys.Rev. C60, 034905 (1999) 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
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
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
1997MU07 Phys.Rev. C55, 2005 (1997) Color-Singlet Strangelets at Finite Temperature
doi: 10.1103/PhysRevC.55.2005
1997MU16 Phys.Rev. C56, 420 (1997) 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
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) A Gluon Plasma Giant Resonance at Finite Temperature
doi: 10.1142/S0218301397000305
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
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
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
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
1993MU01 Phys.Rev. C47, 473 (1993) Deuteron Quadrupole Moment and 3S1-3D1 State Properties NUCLEAR STRUCTURE 2H; calculated quadrupole moment, rms matter radius, asymptotic D/S ratio. Nonrelativistic potential models, short range attractive nonlocality.
doi: 10.1103/PhysRevC.47.473
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
1993MU11 Phys.Rev. C48, 929 (1993) Radius and Radial Moments of the Deuteron NUCLEAR STRUCTURE 2H; analyzed (e, d), (e, p) data; deduced rms matter radius, radial moments.
doi: 10.1103/PhysRevC.48.929
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
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
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
1992MU05 J.Phys.(London) G18, 303 (1992) M.M.Mustafa, E.M.Zahran, E.El-Deen, A.M.Sultan Recent Energy Dependent Phaseshift Analysis and Deuteron Interaction Models NUCLEAR STRUCTURE 2H; calculated binding energy, charge radius, quadrupole moment, D-state probability. Deuteron interaction models.
doi: 10.1088/0954-3899/18/2/012
1992MU08 Phys.Rev. C45, 2603 (1992) M.M.Mustafa, E.-S.M.Hassan, M.W.Kermode, E.M.Zahran Extracting a Value of the Deuteron Radius by Reanalysis of the Experimental Data NUCLEAR STRUCTURE 1,2H, 1n; analyzed electric form factors data. 2H deduced rms radius.
doi: 10.1103/PhysRevC.45.2603
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
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
1991BL08 Phys.Rev. C44, R590 (1991) 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
1991KE01 Phys.Rev. C43, 416 (1991) M.W.Kermode, S.A.Moszkowski, M.M.Mustafa, W.van Dijk Nonlocality and the Radius of the Deuteron NUCLEAR STRUCTURE 2H; calculated S-, D-state wave functions; deduced nonlocality effects.
doi: 10.1103/PhysRevC.43.416
1991KE03 J.Phys.(London) G17, 105 (1991) M.W.Kermode, W.van Dijk, D.W.L.Sprung, M.M.Mustafa, S.A.Moszkowski Structure Effects in the Deuteron Wavefunction NUCLEAR STRUCTURE 2H; calculated S-, D-state wave functions, rms radius; deduced nucleon quark structure role.
doi: 10.1088/0954-3899/17/2/004
1991MU17 Few-Body Systems 11, 83 (1991) The Nonlocal Tensor Operator S(N)12(ρ, ρ') NUCLEAR STRUCTURE 2H; calculated matter radius, D-state probability, quadrupole moment vs tensor nonlocality strength.
doi: 10.1007/BF01318553
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
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
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
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
1989MU07 Phys.Scr. 39, 552 (1989) The Root Mean Square Radius of the Deuteron and the Nonlocality of the Nucleon-Nucleon Interaction NUCLEAR STRUCTURE 1H; calculated rms radius; deduced nucleon-nucleon interaction features.
doi: 10.1088/0031-8949/39/5/003
1989MU10 Phys.Scr. 40, 162 (1989) The Quadrupole Moment of the Deuteron and Local Potential Models NUCLEAR STRUCTURE 2H; calculated binding energy, quadrupole moment, D-state probability, asymptotic normalization. Local potential models.
doi: 10.1088/0031-8949/40/2/003
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
1988MU24 Phys.Rev. C38, 2416 (1988) Nucleon-Nucleon Interaction with Nonlocal Tensor Contribution for the 3S1-3D1 State NUCLEAR STRUCTURE 2H; calculated radial wave function, quadrupole moment, D-state probability. Nonlocal tensor term in nucleon-nucleon interaction.
doi: 10.1103/PhysRevC.38.2416
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
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
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
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
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
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
1976MU10 Phys.Rev. C14, 2168 (1976) 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
1975MU03 Phys.Rev. C11, 1059 (1975) 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
1975MU11 Phys.Rev. C12, 1638 (1975) 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
1975MU14 Phys.Lett. 60B, 15 (1975) 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
1974MU08 Phys.Lett. 49B, 405 (1974) 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
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
1973MU16 Phys.Rev. C8, 1924 (1973) 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
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
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
1970MU20 Phys.Rev. C2, 2068 (1970) 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
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