Bulletin of the American Physical Society
65th Annual Meeting of the APS Division of Plasma Physics
Monday–Friday, October 30–November 3 2023; Denver, Colorado
Session NP11: Poster Session V:
MFE:DIII-D and conventional tokamaks I;Heating and energetic particles;ITER, HBT-EP, and tokamak control
HED: Measurements and analysis in HED plasmas
Fundamental: Fundamental processes in plasmas
Mini Conference:Experiments in Lab and Space
MFE: Measurement and diagnostics techniques
9:30 AM - 12:30 PM
Wednesday, November 1, 2023
Room: Plaza ABC
Abstract: NP11.00137 : Opacity calculations: including more and more states
Presenter:
Jean-Christophe Pain
(French Alternative Energies and Atomic Energy Commission)
Author:
Jean-Christophe Pain
(French Alternative Energies and Atomic Energy Commission)
Firstly, we propose to start from global approaches and refine them, either by combining statistical approaches such as Unresolved Transition Arrays, Spin-Orbit Split Arrays or Super Transition Arrays (STA), with Detailed Line Accouting (DLA) calculations [1], or by revealing the underlying structure of the spectra as in the Configurationally-Resolved Super Transition Array (CRSTA) [2] or Partially-Resolved (PR)-CRSTA [3] approaches.
In a second step, we try to go the other way, starting with detailed calculations and including (even in an approximate manner) more spectral features. In multiply-charged ion plasmas, a significant number of electrons may occupy high-energy orbitals. These Rydberg electrons, when they act as spectators, are responsible for a huge number of satellites of X-ray absorption or emission lines, yielding a broadening of the red wing of the resonance lines. We suggest to model the perturbation induced by the Rydberg spectators as a partial DLA calculation, their effect being included through a shift and width, expressed in terms of the canonical partition functions, which are key-ingredients of the STA model [4].
[1] G. Hazak and Y. Kurzweil, High Energy Density Phys. 8, 280 (2012).
[2] Y. Kurzweil and G. Hazak, Phys. Rev. E 94, 053210 (2016).
[3] J.-C. Pain, F. Gilleron and T. Blenski, Laser Part. Beams 33, 201 (2015).
[4] J.-C. Pain and F. Gilleron, High Energy Density Phys. 15, 30 (2015).
Follow Us |
Engage
Become an APS Member |
My APS
Renew Membership |
Information for |
About APSThe American Physical Society (APS) is a non-profit membership organization working to advance the knowledge of physics. |
© 2024 American Physical Society
| All rights reserved | Terms of Use
| Contact Us
Headquarters
1 Physics Ellipse, College Park, MD 20740-3844
(301) 209-3200
Editorial Office
100 Motor Pkwy, Suite 110, Hauppauge, NY 11788
(631) 591-4000
Office of Public Affairs
529 14th St NW, Suite 1050, Washington, D.C. 20045-2001
(202) 662-8700