scholarly journals Collisional Ionization Equilibrium for Optically Thin Plasmas. I. Updated Recombination Rate Coefficients for Bare through Sodium‐like Ions

2006 ◽  
Vol 167 (2) ◽  
pp. 343-356 ◽  
Author(s):  
P. Bryans ◽  
N. R. Badnell ◽  
T. W. Gorczyca ◽  
J. M. Laming ◽  
W. Mitthumsiri ◽  
...  
1976 ◽  
Vol 31 (6) ◽  
pp. 565-568
Author(s):  
Udit Narain ◽  
N. K. Jain ◽  
Suresh Chandra

The ionization equilibrium of helium is investigated using new ionization and modified dielectronic recombination rate coefficients. The results are discussed in the light of available data


2009 ◽  
Vol 42 (10) ◽  
pp. 105203 ◽  
Author(s):  
Fan-Chang Meng ◽  
Li Zhou ◽  
Min Huang ◽  
Chong-Yang Chen ◽  
Yan-Sen Wang ◽  
...  

2012 ◽  
Vol 10 (H16) ◽  
pp. 606-608 ◽  
Author(s):  
M. A. de Avillez ◽  
D. Breitschwerdt ◽  
A. Asgekar ◽  
E. Spitoni

AbstractUntil recently the dynamical evolution of the interstellar medium (ISM) was simulated using collisional ionization equilibrium (CIE) conditions. However, the ISM is a dynamical system, in which the plasma is naturally driven out of equilibrium due to atomic and dynamic processes operating on different timescales. A step forward in the field comprises a multi-fluid approach taking into account the joint thermal and dynamical evolutions of the ISM gas.


2007 ◽  
Vol 478 (2) ◽  
pp. 513-520 ◽  
Author(s):  
A. J. J. Raassen ◽  
K. A. van der Hucht ◽  
N. A. Miller ◽  
J. P. Cassinelli

1972 ◽  
Vol 14 ◽  
pp. 586-587 ◽  
Author(s):  
M. Landini ◽  
B.C. Monsignori Fossi

Ionization equilibrium calculations, which have a number of astrophysical applications, have been computed by Jordan for the ions of C, N, O, Ne, Mg, Si, S, Fe, and Ni.The aim of this paper is to extend the evaluation to other elements relevant to the investigation of the solar atmosphere. Ions of Na, Al, P, Cl, A, K, Ca, Cr, and Mn have been considered and the ionization balance has been computed for temperature from 104 to 107 K.The computation is performed including collisional ionization, autoionization, radiative recombination and dielectronic recombination.


2005 ◽  
Vol 437 (3) ◽  
pp. 1151-1157 ◽  
Author(s):  
S. Böhm ◽  
A. Müller ◽  
S. Schippers ◽  
W. Shi ◽  
M. Fogle ◽  
...  

1996 ◽  
Vol 171 ◽  
pp. 442-442
Author(s):  
T. Schmutzler ◽  
D. Breitschwerdt

The most puzzling observations concerning the LISM (distance < 100 pc) can be explained by a fast adiabatically cooled gas in the cavity of an old superbubble. The ultrasoft X-ray background and contributions to the C- and M-bands are due to the continuum emission of delayed recombination [1]. In contrast to collisional ionization equilibrium (CIE) models, but consistent with recent observations [2], our model predicts a lack of emission lines and a low emissivity in the EUV range. In the figure below we compare the emissivities resulting from CIE at T = 106 K and those from our model at T = 4.2 × 104 K. The basic feature of our model is a thermally self-consistent approach of the time-dependent evolution.


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