Quantum mechanical model for the study of pressure ionization in the superconfiguration approach

The knowledge of plasma equation of state and photoabsorption requires suitable and realistic models for the description of ions. The number of relevant electronic configurations of ions in hot dense plasmas can be immense (increasing with atomic number Z). In such cases, calculations relying on the superconfiguration approximation appear to be among the best statistical approaches to photoabsorption in plasmas. The superconfiguration approximation enables one to perform rapid calculation of averages over all possible configurations representing excited states of bound electrons. We present a thermodynamically consistent model involving detailed screened ions (described by superconfigurations) in plasmas. The density effects are introduced via the ion-sphere model. In the usual approaches, bound electrons are treated quantum mechanically while free electrons are described within the framework of semi-classical Thomas–Fermi theory. Such a hybrid treatment can lead to discontinuities in the thermodynamic quantities when pressure ionization occurs. We propose a model in which all electrons (bound and free) are treated quantum mechanically. Furthermore, resonances are carefully taken into account in the self-consistent calculation of the electronic structure of each superconfiguration. The model provides the contribution of electrons to the main thermodynamic quantities, together with a treatment of pressure ionization, and gives a better insight into the electronic properties of hot dense plasmas.

[1]  J. Pain,et al.  Self-consistent approach for the thermodynamics of ions in dense plasmas in the superconfiguration approximation , 2003 .

[2]  J. Benage,et al.  Possibility of an unequivocal test of different models of the equation of state of aluminum in the coupling regime Gamma approximately 1-50. , 2002, Physical review. E, Statistical, nonlinear, and soft matter physics.

[3]  Thomas Blenski,et al.  A superconfiguration code based on the local density approximation , 2000 .

[4]  A. Grimaldi,et al.  HARTREE-FOCK STATISTICAL APPROACH TO ATOMS AND PHOTOABSORPTION IN PLASMAS , 1997 .

[5]  Perrot,et al.  Equation of state and transport properties of an interacting multispecies plasma: Application to a multiply ionized Al plasma. , 1995, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[6]  Ishikawa,et al.  Pressure ionization in the spherical ion-cell model of dense plasmas and a pressure formula in the relativistic Pauli approximation. , 1995, Physical review. E, Statistical physics, plasmas, fluids, and related interdisciplinary topics.

[7]  Goldstein,et al.  Super-transition-arrays: A model for the spectral analysis of hot, dense plasma. , 1989, Physical review. A, General physics.

[8]  Ichimaru,et al.  Free energies of electron-screened ion plasmas in the hypernetted-chain approximation. , 1986, Physical review. A, General physics.

[9]  D. Liberman Self-consistent field model for condensed matter , 1979 .

[10]  L. Dagens Application de la méthode de l'atome neutre auxiliaire au calcul de l'énergie des métaux simples , 1973 .

[11]  W. Kohn,et al.  CONTINUITY BETWEEN BOUND AND UNBOUND STATES IN A FERMI GAS , 1965 .

[12]  N. Metropolis,et al.  Equations of State of Elements Based on the Generalized Fermi-Thomas Theory , 1949 .

[13]  R. More Pressure Ionization, Resonances, and the Continuity of Bound and Free States , 1985 .