J/ApJS/165/338     Radio recombination lines in HII regions (Quireza+, 2006)

Radio recombination lines in Galactic H II regions. Quireza C., Rood R.T., Balser D.S., Bania T.M. <Astrophys. J. Suppl. Ser., 165, 338-359 (2006)> =2006ApJS..165..338Q 2006ApJS..165..338Q
ADC_Keywords: H II regions ; Radio lines ; Radial velocities Keywords: H II regions - ISM: abundances - ISM: atoms - ISM: clouds - ISM: evolution - ISM: lines and bands - ISM: structure - nuclear reactions, nucleosynthesis, abundances - radio lines: ISM Abstract: We report radio recombination line (RRL) and continuum observations of a sample of 106 Galactic HII regions made with the NRAO 140 Foot (43m) radio telescope in Green Bank, West Virginia. We believe this to be the most sensitive RRL survey ever made for a sample this large. Most of our source integration times range between 6 and 90 hr, yielding typical rms noise levels of ∼1.0-3.5mK. Our data result from two different experiments performed, calibrated, and analyzed in similar ways. A CII survey was made at the 3.5cm wavelength to obtain accurate measurements of carbon radio recombination lines. When combined with atomic (CI) and molecular (CO) data, these measurements will constrain the composition, structure, kinematics, and physical properties of the photodissociation regions that lie on the edges of HII regions. A second survey was made at the 3.5cm wavelength to determine the abundance of 3He in the interstellar medium of the Milky Way. Together with measurements of the 3He+ hyperfine line, we get high-precision RRL parameters for H, 4He, and C. Here we discuss significant improvements in these data with both longer integrations and newly observed sources. Description: Our spectral line observations were made with the NRAO 140 Foot radio telescope during the following periods: 1996 September and December; 1997 January, August, and September; and 1998 January, June, and July. File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file table1.dat 89 119 Properties of Galactic HII Regions table2.dat 59 119 Hydrogen Radio Recombination Line Parameters table3.dat 59 119 Helium Radio Recombination Line Parameters table4.dat 64 121 Carbon Radio Recombination Line Parameters table5.dat 84 119 Radio Emission Continuum Parameters (Total Power Observing Mode) table6.dat 84 119 Radio Emission Continuum Parameters (Switched Power Observing Mode) -------------------------------------------------------------------------------- See also: J/A+A/397/213 : Galactic HII regions (Paladini+, 2003) J/AJ/130/156 : Galactic radio compact HII regions at 1.4GHz (Giveon+, 2005) J/ApJ/582/756 : Velocities of HII regions (Kolpak+, 2003) Byte-by-byte Description of file: table1.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 12 A12 --- Name Galactic HII region name 14- 16 A3 --- f_Name [a,b ] Note on the observation of Name (G1) 18- 30 A13 --- OName Other name 32- 38 F7.3 deg GLON Galactic longitude 40- 46 F7.3 deg GLAT Galactic latitude 48- 49 I2 h RAh Hour of Right Ascension (B1950) 51- 52 I2 min RAm Minute of Right Ascension (B1950) 54- 57 F4.1 s RAs Second of Right Ascension (B1950) 59 A1 --- DE- Sign of the Declination (B1950) 60- 61 I2 deg DEd Degree of Declination (B1950) 63- 64 I2 arcmin DEm Arcminute of Declination (B1950) 66- 69 F4.1 arcsec DEs Arcsecond of Declination (B1950) 71- 75 F5.1 h Tint Integration time corresponding to the spectral line data 77- 81 F5.2 mK rms Data rms corresponding to the spectral line data 83 A1 --- QF [A-E] Spectral line quality factor (1) 85- 89 A5 --- Survey Survey type (C II or 3He) -------------------------------------------------------------------------------- Note (1): QF is an evaluation of the quality of the parameters measured for the spectra as a whole. It is based on the signal-to-noise ratio, the structure of the baseline, the crowding of spectral lines, and the accuracy of the Gaussian fit to the line shape. A = our best spectra to E = our worse cases. -------------------------------------------------------------------------------- Byte-by-byte Description of file: table[234].dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 12 A12 --- Name Galactic HII region name 14- 16 A3 --- f_Name [a,b ] Note on the observation of Name (G1) 20- 26 F7.2 mK TL ? Peak intensity of antenna temperature 28- 32 F5.2 mK e_TL ? Error in TL 34- 38 F5.2 km/s FWHM ? Line width full width at half maximum 40- 44 F5.2 km/s e_FWHM ? Error in FWHM 46- 51 F6.2 km/s VLSR ? LSR radial velocity (G2) 53- 57 F5.2 km/s e_VLSR ? Error in VLSR 59 A1 --- QF [A-E] Line quality factor (1) 61- 62 A2 --- Morph Spectral line shape morphology (2) 64 A1 --- RF [EGFP] Line reliability factor (3) -------------------------------------------------------------------------------- Note (1): QF is a qualitative evaluation of the quality of the parameters measured for the line from A (best spectra) to E (worse cases). Mostly based in the accuracy of the Gaussian fit to the line shape. Note (2): See text. It indicates the position (velocity) of the C line in the spectra and how distinct it is from the He line as follows: r = resolved sb = semi-blended b = blended Note (3): RF is a qualitative evaluation of the reality of a C line as follows: E = excellent G = good F = fair P = poor -------------------------------------------------------------------------------- Byte-by-byte Description of file: table[56].dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 12 A12 --- Name Galactic HII region name 14- 16 A3 --- f_Name [a,b ] Note on the observation of Name (G1) 18- 23 F6.3 K TC-RA ? Peak continuum intensity of antenna temperature along Right Ascension 25- 29 F5.3 K e_TC-RA ? Error in TC-RA 31- 36 F6.3 K TC-DE ? Peak continuum intensity of antenna temperature along Declination 38- 42 F5.3 K e_TC-DE ? Error in TC-DE 44- 49 F6.3 arcmin PA-RA ? FWHM observed angular size along Right Ascension 51- 55 F5.3 arcmin e_PA-RA ? Error in PA-RA 57- 62 F6.3 arcmin PA-DE ? FWHM observed angular size along Declination 64- 69 F6.3 arcmin e_PA-DE ? Error in PA-DE 71- 76 F6.3 arcmin PA-src ? Geometric mean FWHM observed angular size 78- 82 F5.3 arcmin e_PA-src ? Error in PA-src 84 A1 --- QF [A-E] Continuum quality factor (1) -------------------------------------------------------------------------------- Note (1): See text. QF is an evaluation of the quality of the parameters measured for the continuum scans from A (best spectra) to E (worse cases). It is based on the accuracy of the Gaussian fit to the emission feature, the uncertainty in the baseline models and the contrast between the target source emission and any emission from possible sub-structures or nearby confusing sources. -------------------------------------------------------------------------------- Global notes: Note (G1): Flags as follows: a = M16, M17, NGC 6334, Rosette and S209 were observed at different positions in the 3He survey. b = Observed in the C II survey. c = Observed in the 3He survey. Note (G2): Relative to the Local Standard of Rest. The 140 Foot velocities cited here are in the kinematic LSR frame using the radio definition of the Doppler shift. The kinematic LSR is defined by a Solar motion of 20.0km/s towards (RA,Dec)=(18h,+30deg)[1900.0]. -------------------------------------------------------------------------------- History: From electronic version of the journal
(End) Greg Schwarz [AAS], Patricia Vannier [CDS] 14-Dec-2007
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