J/A+AS/140/193 Stark broadening of Zn I (Dimitrijevic+, 1999) ================================================================================ Stark broadening of neutral zinc spectral lines Dimitrijevic M.S., Sahal-Brechot S. =1999A&AS..140..193D ================================================================================ ADC_Keywords: Atomic physics Keywords: atomic data - line profiles Abstract: Using the semiclassical perturbation approach, we have calculated electron-, proton- and He II-impact line widths and shifts for 32 Zn I multiplets as a function of temperature and perturber density. Obtained results have been compared with the existing theoretical and experimental data File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file table1.dat 123 594 Stark broadening parameters due to e-, p- and He II-impacts for Zn I for perturber densities 1.E+13cm-3 - 1.E+19cm-3. -------------------------------------------------------------------------------- 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/131/143 : Sc X, Sc XI, Ti XI and Ti XII (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+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: table1.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 7 E7.2 cm-3 N Perturber density 10- 13 A4 --- El [Zn I] Element 16- 21 A6 --- Tr Transition (4) 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 [*] See note (5) 53- 61 E9.3 0.1nm We FWHM for electron impacts (2) 63 A1 --- n_de [*] See note (5) 64- 73 E10.3 0.1nm de Shift for electron impacts (3) 76 A1 --- n_Wp [*] See note (5) 77- 85 E9.3 0.1nm Wp FWHM for proton impacts (2) (6) 88 A1 --- n_dp [*] See note (5) 89- 98 E10.3 0.1nm dp Shift for proton impacts (3) (6) 101 A1 --- n_WHe+ [*] See note (5) 102-110 E9.3 0.1nm WHe+ FWHM for He II-impacts (2) 113 A1 --- n_dHe+ [*] See note (5) 114-123 E10.3 0.1nm dHe+ Shift for He II-impacts (3) -------------------------------------------------------------------------------- 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): In the first part of the Table are singlets and in the second triplets Note (5): An asterisk in this column indicates that 0.10.5 are not given, because in this case the impact approximation is no longer valid -------------------------------------------------------------------------------- Acknowledgements: Dr Milan Dimitrijevic ================================================================================ (End) Patricia Bauer [CDS] 09-Sep-1999