NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = H.G.Miller Found 52 matches. 2010CO08 Eur.Phys.J. A 44, 257 (2010) S.M.M.Coelho, C.Zander, H.G.Miller Gross features of finite nuclei at finite temperatures NUCLEAR STRUCTURE 130Xe; calculated temperature-dependent binding energy using a semi-empirical mass formula.
doi: 10.1140/epja/i2010-10941-y
2008BE34 Eur.Phys.J. A 37, 357 (2008) W.A.Berger, H.G.Miller, D.Waxman Threshold bound states
doi: 10.1140/epja/i2008-10636-0
2005KR17 Eur.Phys.J. A 25, 339 (2005) M.K.G.Kruse, H.G.Miller, A.R.Plastino, A.Plastino, S.Fujita Landau-Ginzburg method applied to finite fermion systems: Pairing in nuclei NUCLEAR STRUCTURE 20Ne, 48Ca, 88Sr, 208Pb; calculated specific heat vs temperature, pairing phase transition features. Landau-Ginzburg method.
doi: 10.1140/epja/i2005-10133-0
2003TE04 Int.J.Mod.Phys. E12, 395 (2003) A.M.Teweldeberhan, H.G.Miller, R.Tegen Generalized Statistics and the Formation of Quark-Gluon Plasma
doi: 10.1142/S0218301303001296
2003TE15 Int.J.Mod.Phys. E12, 669 (2003) A.M.Teweldeberhan, H.G.Miller, R.Tegen κ-Deformed Statistics and the Formation of a Quark-Gluon Plasma
doi: 10.1142/S021830130300148X
2002TE15 Int.J.Mod.Phys. E11, 573 (2002) Neutrino Mass from Beta Decay of the Free Neutron RADIOACTIVITY 1n(β-); calculated β-decay rate, sensitivity to neutrino mass.
doi: 10.1142/S0218301302001101
2001RI06 Eur.Phys.J. A 10, 97 (2001) R.A.Ritchie, H.G.Miller, F.C.Khanna Landau-Ginzburg Treatment of Nuclear Matter at Finite Temperature
doi: 10.1007/s100500170148
1998CO42 Mod.Phys.Lett. A 13, 2705 (1998) B.J.Cole, H.G.Miller, R.M.Quick Quadrupole Deformation in Nuclei at Finite Temperature NUCLEAR MOMENTS 20Ne; calculated intrinsic quadrupole moment, deformation vs temperature. Mean-field approach.
doi: 10.1142/S0217732398002874
1997GO01 Phys.Rev. C55, 2002 (1997) Isotopic Asymmetry and Coulomb Interactions in Heavy-Ion Collisions
doi: 10.1103/PhysRevC.55.2002
1996KH05 Phys.Rev. C54, 1133 (1996) F.C.Khanna, H.G.Miller, R.M.Quick Spontaneous Symmetry Breaking and the Dissipation of Nuclear Collective Degrees of Freedom at Finite Temperature NUCLEAR STRUCTURE 20Ne; calculated collective degrees of freedom dissipation associated critical temperature. Elliott model, spontaneous U(3) symmetry breaking.
doi: 10.1103/PhysRevC.54.1133
1996MI18 Z.Phys. A356, 141 (1996) H.G.Miller, Y.Tzeng, G.D.Yen, N.Canosa, R.Rossignoli, A.Plastino The Minimum Norm Method for the Determination of the Charge Density from Elastic Electron Scattering Data
doi: 10.1007/s002180050160
1995MA59 Nuovo Cim. 108A, 437 (1995) Finite-Size Effects in a Relativistic Fermi Gas Model of Quasi-Elastic Scattering NUCLEAR STRUCTURE 6Li, 12C, 24Mg, 40Ca, 58Ni, 89Y, 119Sn, 181Ta, 208Pb; analyzed (e, e') data; deduced Fermi momentum, mean separation energy, R0(A). Relativistic Fermi gas model, finite-size effects. NUCLEAR REACTIONS 12C, 56Fe(e, e'), E not given; analyzed transverse, longitudinal response function. Relativistic Fermi gas model, finite-size effects.
doi: 10.1007/BF02813601
1994BU25 Yad.Fiz. 57, No 12, 2177 (1994); Phys.Atomic Nuclei 57, 2095 (1994) V.V.Burov, H.G.Miller, M.V.Rzjanin, K.V.Shitikova, G.D.Yen A Microscopic Description of Neutron-Rich Lithium Isotopes NUCLEAR STRUCTURE 6,7,8,9,11Li; calculated rms radii, ground state, monopole energies, compressibilities, form factors, radial densities. Hyperspherical basis.
1994CO13 Phys.Rev. C50, 1913 (1994) B.J.Cole, N.J.Davidson, H.G.Miller Determination of Nuclear Level Densities from Experimental Information
doi: 10.1103/PhysRevC.50.1913
1994DA10 Nucl.Phys. A570, 61c (1994) N.J.Davidson, S.S.Hsiao, J.Markram, H.G.Miller, Y.Tzeng A Semi-Empirical Determination of the Properties of Nuclear Matter
doi: 10.1016/0375-9474(94)90269-0
1994GO19 Phys.Rev. C50, 2232 (1994) M.I.Gorenstein, H.G.Miller, R.M.Quick, S.N.Yang Electrical Chemical Potential and π--π+ Asymmetry in Heavy-Ion Collisions
doi: 10.1103/PhysRevC.50.2232
1994MI05 Nucl.Phys. A570, 217c (1994) H.G.Miller, R.M.Quick, R.R.Rossignoli, G.D.Yen Correlated Finite Temperature Mean Field Approximations NUCLEAR STRUCTURE 20Ne; calculated thermal behavior, specific heat, entropy vs temperature; deduced correlated, mean field approaches comparison.
doi: 10.1016/0375-9474(94)90286-0
1994YE05 Phys.Rev. C50, 807 (1994) Dependence of Nuclear Shape Transformations on the Nuclear Volume NUCLEAR STRUCTURE 24Mg; calculated Hill-Wheeler parameters, many-body level density, effective pressure, energy ensemble average energy, specific heat vs temperature, volume. Constrained Hartree-Fock approximation.
doi: 10.1103/PhysRevC.50.807
1993AL14 Phys.Lett. 314B, 173 (1993) M.S.Allie, F.D.Brooks, D.G.Aschman, A.Buffler, W.A.Cilliers, R.W.Fearick, C.G.L.Henderson, M.J.Oliver, M.R.Nchodu, S.M.Perez, D.Steyn, W.R.McMurray, B.R.S.Simpson, F.D.Smit, H.G.Miller, K.Bharuth-Ram, I.J.van Heerden Differential Cross Section for n-p Radiative Capture at E(n) = 63.4 MeV NUCLEAR REACTIONS 1H(n, γ), E=63.4 MeV; measured Iγ(θ); deduced σ(θ) for 2H(γ, p), E ≈ 34 MeV. Legendre polymonial fits.
doi: 10.1016/0370-2693(93)90445-N
1993DA14 Phys.Rev. C48, 2108 (1993) Nuclear Shell Effects at High Temperatures NUCLEAR STRUCTURE A ≤ 250; calculated local shell effects associated temperature, excitation energy vs mass; deduced single particle spectrum. Semi-empirical method.
doi: 10.1103/PhysRevC.48.2108
1992CA19 Phys.Rev. C45, 3027 (1992) N.Canosa, R.Rossignoli, H.G.Miller Dynamical Dependence of Thermal Phase Transformations in Finite Systems NUCLEAR STRUCTURE 20Ne; calculated specific heat vs temperature. Vary-Yang interaction, continuum effects.
doi: 10.1103/PhysRevC.45.3027
1992PE01 Phys.Rev. C45, 870 (1992) S.M.Perez, R.M.Quick, N.J.Davidson, H.G.Miller, F.Solms Reconstruction of the Spin Dependence of One-Nucleon-Transfer Spectroscopic Sums from Incomplete Information NUCLEAR STRUCTURE 49Ti, 45Sc; calculated f7/2 proton pickup, stripping spectroscopic factors.
doi: 10.1103/PhysRevC.45.870
1992QU02 Nuovo Cim. 105A, 913 (1992) R.M.Quick, B.J.Cole, H.G.Miller Effect of Model Space Size on Finite-Temperature Hartree-Fock Calculations NUCLEAR STRUCTURE 20Ne, 24Mg; calculated energy, entropy, specific heat; deduced model space effects. Finite temperature Hartree-Fock approximation.
doi: 10.1007/BF02730832
1992RO06 Phys.Lett. 277B, 18 (1992) R.Rossignoli, R.M.Quick, H.G.Miller Correlated Finite Temperature Mean Field Approximations NUCLEAR STRUCTURE 20Ne; calculated specific heat, deformation parameter, entropy vs temperature. Correlated finite temperature mean field approximations.
doi: 10.1016/0370-2693(92)90949-5
1992YE02 Phys.Lett. 289B, 1 (1992) Nuclear Shape Transitions at Finite Temperature and Fixed Volume NUCLEAR STRUCTURE 24Mg; calculated energy ensemble averages, specific heats, many body level densities, pressure vs temperature; deduced compression role in shape transition temperature dependence. Hartree-Fock approximation.
doi: 10.1016/0370-2693(92)91352-A
1991QU01 Phys.Lett. 254B, 303 (1991) R.M.Quick, N.J.Davidson, B.J.Cole, H.G.Miller The Observation of Nuclear Shape Transitions at Fixed Angular Momentum NUCLEAR STRUCTURE 24Mg; calculated shapes vs spin, temperature; deduced shape transition features. Cranked finite temperature Hartree-Fock.
doi: 10.1016/0370-2693(91)91159-S
1990CO04 Phys.Rev. C41, 789 (1990) B.J.Cole, H.G.Miller, R.M.Quick Effect of the Continuum on Thermally Induced Phase Transitions in Nuclei NUCLEAR STRUCTURE 20Ne, 16O, 24Mg; calculated specific heat vs temperature. Continuum effects, thermally induced phase transitions.
doi: 10.1103/PhysRevC.41.789
1990QU02 Z.Phys. A336, 279 (1990) Signatures for ' Phase ' Transitions in Finite Systems NUCLEAR STRUCTURE 24Mg; calculated internal energy fluctuation square, specific heat. Phase transitions in finite systems.
1989CO10 Phys.Rev. C40, 456 (1989) B.J.Cole, R.M.Quick, H.G.Miller Shape of 24Mg at Zero and Finite Temperature NUCLEAR STRUCTURE 24Mg; calculated ground state deformation. Hartree-Fock-Rothaan calculations.
doi: 10.1103/PhysRevC.40.456
1989DA22 Nucl.Phys. A505, 300 (1989) N.J.Davidson, R.M.Quick, H.G.Miller Approximations to Angular Momentum Projection in Mean Field Calculations NUCLEAR STRUCTURE 24Mg; calculated probability amplitudes. Mean field approach, constrained Hartree-Fock operators.
doi: 10.1016/0375-9474(89)90375-8
1989MI05 Phys.Rev. C39, 1599 (1989) H.G.Miller, R.M.Quick, B.J.Cole Nuclear Shape Transitions at Finite Temperature NUCLEAR STRUCTURE 24Mg; calculated shapes, quadrupole moment, specific heat vs temperature. Finite temperature mean field approach.
doi: 10.1103/PhysRevC.39.1599
1989MI18 Phys.Rev.Lett. 63, 1922 (1989) H.G.Miller, B.J.Cole, R.M.Quick Evidence for Phase Transitions in Finite Systems NUCLEAR STRUCTURE 20Ne; calculated specific heat vs temperature; deduced phase transition evidence.
doi: 10.1103/PhysRevLett.63.1922
1989QU01 Phys.Rev. C40, 993 (1989) R.M.Quick, H.G.Miller, B.J.Cole Reliability of the Finite Temperature Hartree-Fock Approximation NUCLEAR STRUCTURE 20Ne; calculated internal energy average ensemble. Finite temperature Hartree-Fock approximation.
doi: 10.1103/PhysRevC.40.993
1988SA03 Phys.Rev. C37, 1267 (1988) M.Saraceno, J.P.Vary, G.Bozzolo, H.G.Miller Thermodynamic Coefficients of Hot Nuclei NUCLEAR STRUCTURE 16O, 40Ca; calculated thermodynamic coefficients, binding energy per nucleon, rms radii.
doi: 10.1103/PhysRevC.37.1267
1986MI02 Nucl.Phys. A448, 236 (1986) Approximate Angular Momentum Projection NUCLEAR STRUCTURE 28Si; calculated angular momentum projected matrix elements. Cubic-spline interpolation methods.
doi: 10.1016/0375-9474(86)90089-8
1986MI05 Phys.Lett. 168B, 13 (1986) H.G.Miller, R.M.Quick, G.Bozzolo, J.P.Vary Nuclear Shape Transitions in the Finite-Temperature Hartree-Fock Approximation NUCLEAR STRUCTURE 24Mg; calculated level energies, rms radii, chemical potentials, quadrupole moments vs temperature.
doi: 10.1016/0370-2693(86)91450-4
1986QU03 Phys.Rev. C34, 1458 (1986) Thermal Response of States of Approximate Angular Momentum in the Finite Temperature Restricted Hartree-Fock Approximation NUCLEAR STRUCTURE 24Mg; calculated approximate 8+ angular momentum state thermal response, mass quadrupole moment. Hartree-Fock approximation.
doi: 10.1103/PhysRevC.34.1458
1985MI01 Phys.Lett. 150B, 11 (1985) Spurious Center of Mass Effects in the Finite Temperature Hartree-Fock Approximation NUCLEAR STRUCTURE 16O; calculated center-of-mass thermal excitation. Finite temperature Hartree-Fock.
doi: 10.1016/0370-2693(85)90126-1
1985MI02 Phys.Lett. 150B, 15 (1985) Calculation of Interband Level Spacings in the Constrained Hartree-Fock Approach NUCLEAR STRUCTURE 24Mg; calculated T=0, 8+ levels, interband level spacings. Constrained Hartree-Fock.
doi: 10.1016/0370-2693(85)90127-3
1983MI26 Phys.Lett. 131B, 271 (1983) Spurious Center of Mass Effects in a Dynamically Determined Basis NUCLEAR STRUCTURE 16O; calculated ground state energy. Hartree-Fock method, spurious center-of-mass motion effects reduction by different techniques.
doi: 10.1016/0370-2693(83)90496-3
1982MI04 Z.Phys. A304, 273 (1982) Configuration Mixing Calculations with Basis States Obtained from Ground State Variational Methods NUCLEAR STRUCTURE 20Ne; calculated levels. Configuration mixing, variational method basis states, unprojected, projected Hartree-Fock, reorthogonalization.
doi: 10.1007/BF01414503
1981MI13 Nucl.Phys. A368, 237 (1981) The Calculation of a Rotational Energy Spectrum using the Constrained Hartree-Fock Approach NUCLEAR STRUCTURE 20Ne; calculated levels. Hartree-Fock calculation, angular momentum constraint.
doi: 10.1016/0375-9474(81)90684-9
1978MI09 Phys.Lett. 77B, 119 (1978) H.G.Miller, R.M.Dreizler, G.Do Dang Generation of Basis States via Variational Mehods NUCLEAR STRUCTURE 20Ne; calculated levels.
doi: 10.1016/0370-2693(78)90602-0
1976DO04 Phys.Lett. 62B, 1 (1976) G.Do Dang, K.W.Schmid, R.M.Dreizler, H.G.Miller Low-Lying 0+ States of 16O via Parity-Mixed Hartree-Fock Calculations NUCLEAR STRUCTURE 16O; calculated levels. Hartree-Fock with parity-mixed orbitals.
doi: 10.1016/0370-2693(76)90031-9
1974AR08 Z.Phys. 267, 13 (1974) Contributions to the Electromagnetic Form Factors of the Deuteron from Isobar Configurations NUCLEAR REACTIONS 2H(e, e); measured nothing, calculated form factor.
1974AR21 Phys.Lett. 52B, 303 (1974) H.Arenhovel, W.Fabian, H.G.Miller Interaction Effects in the Photodisintegration of the Deuteron up to 140 MeV NUCLEAR REACTIONS 2H(γ, p), E < 140 MeV; calculated σ.
doi: 10.1016/0370-2693(74)90047-1
1974MI09 Nucl.Phys. A225, 137 (1974) A Microscopic Calculation of Inelastic Electron Scattering to the First 2+ State in Some Even Tin Isotopes NUCLEAR REACTIONS 116,120,124Sn(e, e'), E=150, 250 MeV; calculated σ(θ), deduced form factor.
doi: 10.1016/0375-9474(74)90370-4
1973MI01 Phys.Rev. C7, 1003 (1973) Effect of Isobar Configurations on the Photodisintegration of the Deuteron NUCLEAR REACTIONS 2H(γ, pn) calculated effect of nuclear polarization on σ.
doi: 10.1103/PhysRevC.7.1003
1971MI04 Nucl.Phys. A163, 637 (1971) H.G.Miller, W.Buss, J.A.Rawlins High-Energy Photoneutrons from 12C NUCLEAR REACTIONS 12C(γ, n), E=64 to 128 MeV, θ=30-140°; measured σ(E, En, θ). Natural target.
doi: 10.1016/0375-9474(71)90514-8
1971WI26 Phys.Lett. 36B, 278 (1971) H.T.Williams, H.Arenhovel, H.G.Miller Effect of Baryon Resonance Admixtures on Elastic Electron Deuteron Scattering NUCLEAR REACTIONS 2H(e, e), 0.1 < Q < 50 fm-2; calculated deuteron form factor. Baryon resonance admixture in deuteron wave function.
doi: 10.1016/0370-2693(71)90702-7
1963MI04 Bull.Am.Phys.Soc. 8, No.4, 321, GA17 (1963) H.G.Miller, M.L.Pool, H.D.Spangenberg Radioactivities from a He3 Bombardment of Eu151 NUCLEAR STRUCTURE 151Gd, 151Tb, 152Tb, 153Gd; measured not abstracted; deduced nuclear properties.
1963MI11 Priv.Comm. (July 1963) H.G.Miller, M.L.Pool, H.D.Spangenberg NUCLEAR STRUCTURE 152Tb, 153Gd, 151Gd, 151Tb; measured not abstracted; deduced nuclear properties.
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