J/A+AS/131/143 Stark broadening of Sc X & XI, Ti XI & XII (Dimitrijevic+ 1998)
Stark broadening of spectral lines of multicharged ions of astrophysical
interest. XXI: Sc X, Sc XI, Ti XI and Ti XII spectral lines
Dimitrijevic M.S., Sahal-Brechot S.
<Astron. Astrophys. Suppl. Ser. 131, 143 (1998)>
=1998A&AS..131..143D 1998A&AS..131..143D (SIMBAD/NED BibCode)
ADC_Keywords: Atomic physics
Keywords: atomic data - line profiles - plasmas
Abstract:
By using the semiclassical-perturbation formalism, we have calculated
electron-, proton-, and He III-impact line widths and shifts for 4 Sc
X, 10 Sc XI, 4 Ti XI and 27 Ti XII multiplets, significant for
analysis, investigation and modeling of different plasmas in solar and
stellar physics, physics and technology. The results are presented as
a function of temperature and perturber density.
File Summary:
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FileName Lrecl Records Explanations
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ReadMe 80 . This file
table1.dat 123 72 Stark broadening parameters due to e-, p- and
He III-impacts for Sc X
table2.dat 123 264 Stark broadening parameters due to e-, p- and
He III-impacts for Sc XI
table3.dat 123 120 Stark broadening parameters due to e-, p- and
He III-impacts for Ti XI
table4.dat 123 726 Stark broadening parameters due to e-, p- and
He III-impacts for Ti XII
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See also:
VI/98 : Stark broadening of H lines (Stehle+, 1999)
Stark broadening of other elements (Dimitrijevic, Sahal-Brechot, Popovic)
J/A+AS/105/243 : BeI lines (Dimitrijevic+ 1994)
J/A+AS/105/245 : Al XI and Si XII (Dimitrijevic+ 1994)
J/A+AS/107/349 : Ne VIII and Na IX (Dimitrijevic+ 1994)
J/A+AS/109/551 : OIV and OV (Dimitrijevic+ 1995)
J/A+AS/115/351 : C V and P V (Dimitrijevic+, 1996)
J/A+AS/116/359 : Xe II lines (Popovic+, 1996)
J/A+AS/117/127 : solar Mg I lines (Dimitrijevic+, 1996)
J/A+AS/119/369 : Be III and B III (Dimitrijevic+, 1996)
J/A+AS/119/529 : Sr I spectral lines (Dimitrijevic+, 1996)
J/A+AS/120/373 : Sc II, Y II and Zr II Stark width (Popovic+ 1996)
J/A+AS/122/163 : Ba I and Ba II lines (Dimitrijevic+, 1996)
J/A+AS/122/533 : P IV spectral lines (Dimitrijevic+, 1997)
J/A+AS/127/295 : Kr II lines (Popovic+ 1998)
J/A+AS/127/543 : S V lines (Dimitrijevic+ 1998)
J/A+AS/128/203 : Mn, Ga & Ge multiplets (Popovic+ 1998)
J/A+AS/128/359 : Ca IX and Ca X lines (Dimitrijevic+ 1998)
J/A+AS/129/155 : Si XI and Si XIII lines (Dimitrijevic+ 1998)
J/A+AS/130/539 : Na X (Dimitrijevic+ 1998)
J/A+AS/131/141 : O VII and Mg XI (Dimitrijevic+ 1998)
J/A+AS/133/227 : K VIII and K IX (Dimitrijevic+ 1998)
J/A+AS/140/191 : Ca I (Dimitrijevic+ 1999)
J/A+AS/140/193 : Zn I (Dimitrijevic+ 1999)
J/A+A/400/791 : Be III (Dimitrijevic+ 2003)
J/A+A/417/375 : Cd III (Milovanovic+, 2004)
J/A+A/423/397 : Si V (Ben Nessib+, 2004)
J/A+A/425/1147 : Ga I (Dimitrijevic+, 2004)
Byte-by-byte Description of file: table?.dat
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Bytes Format Units Label Explanations
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1- 7 E7.2 cm-3 N Perturber density
10- 14 A5 --- El Element
15- 20 A6 --- Tr Transition
23- 30 F8.1 0.1nm lambda Wavelength
33- 40 E8.2 0.1nm/cm3 C Parameter C (1)
43- 50 F8.0 K T Temperature
52 A1 --- n_We [*] Validity of impact approximation (4)
53- 61 E9.3 0.1nm We FWHM for electron impacts (2)
63 A1 --- n_de [*] Validity of impact approximation (4)
64- 73 E10.3 0.1nm de Shift for electron impacts (3)
76 A1 --- n_Wp [*] Validity of impact approximation (4)
77- 85 E9.3 0.1nm Wp FWHM for proton impacts (2) (5)
88 A1 --- n_dp [*] Validity of impact approximation (4)
89- 98 E10.3 0.1nm dp Shift for proton impacts (3) (5)
101 A1 --- n_WHe++ [*] Validity of impact approximation (4)
102-110 E9.3 0.1nm WHe++ FWHM for He III-impacts (2)
113 A1 --- n_dHe++ [*] Validity of impact approximation (4)
114-123 E10.3 0.1nm dHe++ Shift for He III-impacts (3)
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Note (1): C/FWHM gives an estimate of the maximum perturber density for which
the line may be treated as isolated and tabulated data may be used
Note (2): FWHM denotes Full Width at Half Maximum
Note (3): A positive (resp. negative) shift is towards the red (resp. blue)
Note (4): An asterisk in this column indicates that 0.1<NV<0.5,
(V = collision volume); beware of the fact that the limit of validity
of the impact approximation is attained for the value that follows
Note (5): Values for NV>0.5 are not given, because in this case the impact
approximation is no longer valid
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Acknowledgements: Dr Milan Dimitrijevic
(End) Patricia Bauer [CDS] 17-Feb-1998