4 edition of **Theory of bound states and ionization equilibrium in plasmas and solids** found in the catalog.

Theory of bound states and ionization equilibrium in plasmas and solids

Werner Ebeling

- 41 Want to read
- 14 Currently reading

Published
**1976**
by Akademie-Verlag in Berlin
.

Written in English

- Bound states (Quantum mechanics),
- Ionization.,
- Plasma (Ionized gases),
- Solids.

**Edition Notes**

Statement | von Werner Ebeling, Wolf Dietrich Kraeft, Dietrich Kremp. |

Series | Ergebnisse der Plasmaphysik und der Gaselektronik ;, Bd. 5 |

Contributions | Kraeft, Wolf Dietrich, joint author., Kremp, Dietrich, joint author. |

Classifications | |
---|---|

LC Classifications | QC174.17.B6 E2 |

The Physical Object | |

Pagination | viii, 164 p. : |

Number of Pages | 164 |

ID Numbers | |

Open Library | OL4629642M |

LC Control Number | 77460977 |

Improvements will arise from a better representation for the reduction factor ~,,, as well as from better quantum-mechanical results with allowance for statistical fluctuations from ion to ion. REFERENCES I. W. Ebeling, W. D. Kraeft, and D. Kremp, Theory of Bound States and Ionization Equilibrium in Plasmas and Solids, Akademie, Berlin (). by: 6. An Introduction to the Atomic and Radiation Physics of Plasmas; If this is the first time you use this feature, you will be asked to authorise Cambridge Core to connect with your account. 8 - Discrete Bound States: Many-Electron Atoms and Ions pp Get by: 3.

plasmas. e 2). Study of the ionization equilibrium in a strongly coupl i medium. 3). Setting up a scheme appropriate for the study of the energy levels and of the ionization potential of atom and ions in a strongly coupled plasma medium. 1). The kinetics of two- or sulti-component strongly coupled plasmas. Previous investigation derives d the SAHA equation for a plasma in equilibrium applying the free-bound concept valid for an isolated electron-io pair. In ounr investigation of the "adapted free-bound model" (I) we have shown that due to the free-boun interactiod n the demarcatio ben-tween free and bound states is shifted by A%= e2/r0. We study.

Definition. Plasma is a state of matter in which an ionized gaseous substance becomes highly electrically conductive to the point that long-range electric and magnetic fields dominate the behaviour of the matter. The plasma state can be contrasted with the other states: solid, liquid, and gas.. Plasma is an electrically neutral medium of unbound positive and negative particles (i.e. the. Abstract. A new approach to the theoretical computation of the equation of state of dense plasmas and liquid metals is presented. The method uses the author's complete solution of Saha's equation, modified by a correction to the ionization potentials that is based on Ecker and Weizel's solutions of the Schrodinger equations for an electron in a Debye field.

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PDF | On Jan 1,Werner Ebeling and others published Theory of Bound States and Ionization Equilibrium in Plasmas and Solids | Find, read and cite all the research you need on ResearchGate. Additional Physical Format: Online version: Ebeling, Werner, Theory of bound states and ionization equilibrium in plasmas and solids.

Berlin: Akademie-Verlag, W. Ebeling, W. Kraeft and D. Kremp; Theory of Bound States and Ionization Equilibrium in Plasmas and Solids, Akademie-Verlag Berlin () Google Scholar [4] W. Ebeling, W. Kraeft and D.

Kremp; Invited lecture Nonideal Plasmas, held at the International Conference on the Physics of Ionized Gases (ICPIG), Berlinp. 73 Google ScholarAuthor: D. Kremp, W. Kraeft, M. Schlanges. Ebeling, W. Kraeft, D.

Kremp, “Theory of Bound States and Ionisation Equilibrium in Plasmas and Solids,” Akademie-Verlag, Berlin (); Extended Russ Author: D. Beule, W. Ebeling, A. Förster. Calculation of the physical properties of reacting plasmas depends on knowing the state of ionization and/or the state occupation numbers.

Simple methods have often been used to estimate ionization balance in plasmas, but they are not adequate for understanding a variety of new experimental and observational measurements.

Theoretical methods to determine the ionization state of partially Cited by: Cite this chapter as: Klimontovich Y.L., Kremp D., Schlanges M.

() Bound States in the Quantum Kinetic Theory of Gases and Plasmas. In: Transport Properties of Dense : Yu. Klimontovich, D. Kremp, M. Schlanges.

H.W. Drawin, P. Felenbok: Data for Plasmas in Local Thermodynamic Equlibrium (Gauthier-Villars, Paris ) Google Scholar [] W. Ebeling, W.D. Kraeft, D. Kremp: Theory of Bound States and Ionization Equilibrium in Plasmas and Solids (Akademie-Verlag, Berlin ) Google Scholar. The result that bound states, except possibly those near the plasma continuum edge, are unshifted allows great simplification in atomic data calculations.

It means that we can use isolated atom bound state energy levels and standard line broadening theory to calculate bound-bound and bound free absorption by: 1.

Especially, one may mention that giant planets consist mainly of ionized dense hydrogen. Also the electron-hole plasma in optically excited semiconductors represents a dense plasma.

Moreover, for many purposes it is also necessary to know transport and optical properties of dense : W. Kraeft, D. Kremp. Plasma Chemistry PLASMA AS THE FOURTH STATE OF MATTER Although the term chemistry in the title of the book does not require a special introduction, the term plasma probably does.

Plasma is an ionized gas, a distinct fourth state of matter. “Ionized” means that at least one electron is not bound to an atom or molecule, convertingFile Size: KB. A consistent model for the equilibrium thermodynamic functions of partially ionized flibe plasma with Coulomb corrections W.

Kremp, and D. Kraeft, Theory of Bound States and Ionization Equilibrium in Plasmas and Solids (Akademie-Verlag “Ionization equilibrium and partition functions of high-temperature weakly nonideal flibe gas Cited by: Starting from the results of a recently developed quantum statistical theory of low density electron-ion-plasmas in thermal equilibrium, the equation of state is derived for the temperature region.

The consequences of the deviation of the two particle bound state behaviour from that in dilute plasmas are nonideality effects which lead to modifications of the chemical equilibrium, i.e., of the mass action law, and of the recombination and ionization processes under nonequlibrium : Wolf-Dietrich Kraeft, Manfred Klaus Kilimann, Dietrich Kremp.

Physica A () North-Holland, Amsterdam EQUATION OF STATE AND IONIZATION EQUILIBRIUM FOR NONIDEAL PLASMAS D. KREMP Wilhelm -Pieck-Universitdt Rostock, Sektion Physik, Universitdtsplatz 3, Rostock, DDR W.D. KRAEFT Ernst-Moritz-Arndt-Universitdt, Sektion PhysiklElektronik Domstr.

l0a, Greifswald, DDR and A.J.D. LAMBERT Technische Hogeschool Cited by: [12] Ebeling W., Kraeft W.D., Kremp D.

Theory of Bound States and Ionization Equilibrium in Plasmas and Solids / Akademic–Verlag: Berlin, ). [13] Iosilevskiy I. Generalized “cold curve” and thermodynamics of a substance at the zero-temperature limit // inCited by: 2.

ELSEVIER Physica A () Adiabatic equation of state and ionization equilibrium of dense plasma Dieter Beule a, Werner Ebeling a., Andreas Frrster b, 1 a Institut fiir Physik, Humboldt-Universitgit zu Berlin, InvalidenstrafleD-lOll5 Berlin, Germany b Department of Physics, University of Tokyo, HongoBunkyo-ku, TokyoJapan Received 2 December Abstract We Cited by: 9.

It is presently noted that, in an up-to-date version of the quantum statistics of Coulomb systems with bound states, the discrete energy states of the Bethe-Salpeter equation have to be introduced.

The quantum theory of bound states in plasmas is compared with the classical theory of ion association in electrolytes. Book Search tips Selecting this option will search all publications across the Scitation platform Selecting this option will Reaction and diffusion in dense nonideal plasmas Physics of Fluids B: Plasma W.-D.

Kraeft, and D. Kremp, Theory of Bound States and Ionization Equilibrium in Plasmas and Solids (Akademie-Verlag, Berlin Cited by: The system of excited levels also move to the ionization limit, entering the continuum (Mott effect), therefore, the number of bound levels progressively reduces as the Debye length decreases, up to a critical value of last existence of the only 1 s state, below which bound states are not admitted and the plasma is fully : Gianpiero Colonna, Annarita Laricchiuta.

The influence of a constant uniform magnetic field on the ionization equilibrium and the thermodynamic properties of a nondegenerate partially ionized hydrogen plasma is .Book Search tips Selecting this option will search all publications across the Scitation platform Selecting this option will search all Influence of excited states on the energy loss of fast ions in a hydrogen plasma W.

D. Kraeft, and D. Kremp, Theory of Bound States and Ionization Equilibrium in Plasmas and Solids, (Akademie, Berlin Cited by: 2.

Ebeling, W. et al. Theory of Bound States and Ionization Equilibrium in Plasmas and Solids (Akademie-Verlag, Berlin); extended edition in Russian (Mir Publishers, Moscow).

Ebeling, W. et al. PhysicaCited by: