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NSR database version of May 22, 2024.

Search: Author = H.G.Miller

Found 52 matches.

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2002TE15      Int.J.Mod.Phys. E11, 573 (2002)

R.Tegen, H.G.Miller

Neutrino Mass from Beta Decay of the Free Neutron

RADIOACTIVITY 1n(β-); calculated β-decay rate, sensitivity to neutrino mass.

doi: 10.1142/S0218301302001101
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1997GO01      Phys.Rev. C55, 2002 (1997)

M.I.Gorenstein, H.G.Miller

Isotopic Asymmetry and Coulomb Interactions in Heavy-Ion Collisions

doi: 10.1103/PhysRevC.55.2002
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1995MA59      Nuovo Cim. 108A, 437 (1995)

M.Marinus, H.G.Miller

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1994GO19      Phys.Rev. C50, 2232 (1994)

M.I.Gorenstein, H.G.Miller, R.M.Quick, S.N.Yang

Electrical Chemical Potential and π-+ Asymmetry in Heavy-Ion Collisions

doi: 10.1103/PhysRevC.50.2232
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1994YE05      Phys.Rev. C50, 807 (1994)

G.D.Yen, H.G.Miller

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1993DA14      Phys.Rev. C48, 2108 (1993)

N.J.Davidson, H.G.Miller

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1992YE02      Phys.Lett. 289B, 1 (1992)

G.D.Yen, H.G.Miller

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1990QU02      Z.Phys. A336, 279 (1990)

R.M.Quick, H.G.Miller

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1986MI02      Nucl.Phys. A448, 236 (1986)

H.G.Miller, E.M.De Lange

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1986QU03      Phys.Rev. C34, 1458 (1986)

R.M.Quick, H.G.Miller

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
Citations: PlumX Metrics


1985MI01      Phys.Lett. 150B, 11 (1985)

H.G.Miller, J.P.Vary

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
Citations: PlumX Metrics


1985MI02      Phys.Lett. 150B, 15 (1985)

H.G.Miller, B.J.Cole

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
Citations: PlumX Metrics


1983MI26      Phys.Lett. 131B, 271 (1983)

H.G.Miller, J.P.Vary

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
Citations: PlumX Metrics


1982MI04      Z.Phys. A304, 273 (1982)

H.G.Miller, H.P.Schroder

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
Citations: PlumX Metrics


1981MI13      Nucl.Phys. A368, 237 (1981)

H.G.Miller, H.P.Schroder

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1974AR08      Z.Phys. 267, 13 (1974)

H.Arenhovel, H.G.Miller

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
Citations: PlumX Metrics


1974MI09      Nucl.Phys. A225, 137 (1974)

H.G.Miller, R.M.Dreizler

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
Citations: PlumX Metrics


1973MI01      Phys.Rev. C7, 1003 (1973)

H.G.Miller, H.Arenhovel

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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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