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Dielectronic Recombination and Inner-Shell Photoabsorption
Work Week and Workshop 2012 Dielectronic Recombination and Inner-Shell Photoabsorption Tom Gorczyca Oleg Zatsarinny, Jun Fu, Dragan Nikolic, Fatih Hasoglu, Shahin Abdel Naby 1/2/2019
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DR Project N. R. Badnell M. G. O’Mullane H. P. Summers M. S. Pindzola
UK M. S. Pindzola S. D. Loch J. Colgan (LANL) D. M. Mitnik T. W. Gorczyca K. T. Korista M. A. Bautista O. Zatsarinny (DU) D. Nikolić (NINT) J. Fu Shahin Abdel Naby DR Project Z. Altun A. Yumak Turkey 1/2/2019
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Status of the DR Project
Level-resolved DR rate coefficients for H-like through Mg-like isoelectronic sequences have been computed. The state-of-the-art AUTOSTRUCTURE package has been used. For each sequence, calculations were performed up to Zn and we included other heavy ions such as Kr, Mo, and Xe. The Controlled Fusion Atomic Data Center ADAS Atomic data and analysis structure 1/2/2019
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Methodology 1/2/2019
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Updated DR Data Si-like and higher isoelectronic sequences are still needed. CHIANTI- an atomic database for emission lines are updated1. For Fe-ions, the work of Badnell and coworkers up through Mg-like. Fe from Badnell2 work. _________________________ 1K. P. Dere et al, A&A 498, 915 (2009) 2N. R. Badnell, ApJ 651, L73 (2006) 1/2/2019
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DR Rate Coefficient for S3+
At low T, the contributions from 3s23pnl core relaxation is forbidden in LS-coupling. Why DR for IC-coupling is reduced? 1/2/2019
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3s → 3p excitation n=36 IC The reduction in the DR occurs at n=36 for both 3s3p2(2P1/2, 3/2)nℓ which is reflected in DR. Such reduction doesn’t exist in LS coupling 3s3p2 2Pnℓ LS FWHM=1.2 meV 1/2/2019
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DR Rate Coefficient for Fe13+
kT║ = 0.09meV ____ Theory ____ TSR Experiment1 3s23p 2P_{3/1}nl, 3s3p2 4P_{3/2}9f, 3s3p3d5g, 3p23dnl, 3s3d2nl 1 E. W. Schmidt et al, ApJ 641, L (2006). 1/2/2019 ncut ≤ 95, ℓ ≤ 8
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DR Rate Coefficient for Al-like Ions
1/2/2019
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Zn17+ P2+ S3+ Si+ Total ground state RR rate coefficients for the Al-like isoelectronic sequence using AUTOSTRUCTURE package. Curves from Si to Zn are shown from left to right. 1/2/2019
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K-Shell Photoabsorption
R-Matrix (nonperturbative method) Include spectator Auger decay broadening effects T. W. Gorczyca and F. Robicheaux, Phys. Rev. A 60, 1215(1999) Excellent agreement with synchrotron experiments on neutral atoms Ar T. W. Gorczyca and F. Robicheaux, Phys. Rev. A 60, 1215(1999) O T. W. Gorczyca and B. M. McLaughlin, J. Phys. B. 33, L859 (2000) Ne T. W. Gorczyca, Phys. Rev. A61, (2000) C Hasoglu et al., ApJ 724, 1296 (2010) Atomic and ionic photoabsorption calculations are crucial for elemental abundance determinations from X-ray spectra of cosmic sources O A. M. Juett et al., APJ 612, 308 (2004) Ne A. M. Juett et al., APJ 648, 1066 (2006) X-rays from about 0.12 to 12 keV (10 to 0.10 nm wavelength) are classified as "soft" X-rays, and from about 12 to 120 keV (0.01 to 0.10 nm wavelength) as "hard" X-rays, due to their penetrating abilities. 1/2/2019
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←Oxygen Ions (Juett+ 2004) ←Neon Ions (Juett+ 2006)
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Cross Section Results for C-Ions at the K-Edge
Experimental Measurements exist ALS group Beside 1s->2p and 3p resonances For astrophysical use, important K-edge features are present.
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Experimental Comparison: C2+ Photoexcitation
** **K-shell photoionization of Be-like C ions S. W. J. Scully, A. Aguilar, E. D. Emmons, R. A. Phaneuf, M. Halka, D. Leitner, J. C. Levin, M. S. Lubell, R. Püttner, A. S. Schlachter, A. M. Covington, S. Schippers, A. Müller and B. M. McLaughlin J. Phys. B. 38, 1967, 2005
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Modeling the Observed X-Ray Spectra
K-shell Photoabsorption Studies of the Carbon Isonuclear Sequence M. F. Hasoglu, S. A. Abdel-Naby, T. W. Gorczyca, J. J. Drake and B. M. McLaughlin The Astrophysical Journal, 724, 1296, 2010
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K-Shell Photoabsorption for Mg2+
a = const. and dominant as n → ∞ 1/2/2019
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Available Data for K-Shell Photoabsorption in Mg Ions
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Spectator Auger 1/2/2019
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Comparison with Previous Results: Mg2+ - Mg5+
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Comparison with Previous Results: Mg+
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Neutral Magnesium
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http://tesla. physics. wmich
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Fe L-Shell Photoabsorption
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Thank You 1/2/2019
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