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Table A.3

6.7 GHz methanol masers as tracers of spiral arms.

Glon Glat V m V p Ref. D σ D Ref. Mark Ref. R 8.5 D 8.5 R 8.3 D 8.3 R BB93 D BB93
(°) (°) km s-1 km s-1 kpc kpc kpc kpc kpc kpc kpc kpc
(1) (2) (3) (4) (5) (6) (7) (8) (9) (10) (11) (12) (13) (14) (15) (16)

0.212 0.000 45.5 49.2 pmb05 ,174302844 pmb05
0.315 0.200 20.5 18.0 pmb05 ,174392845 pmb05
0.340 0.000 37.5 37.0 pmb05 ,174322835 pmb05
0.393 0.034 26.5 28.7 pmb05
0.496 0.188 5.0 0.8 pmb05 ,174292823 pmb05
0.530 0.180 2.0 7.0 pmb05 ,174302822 pmb05
0.546 0.851 14.0 14.0 pmb05 ,174702853 pmb05
... ... ... ... ... ... ... ... ... ... ... ... ... ... ... ...

Notes. A portion of this table is shown here. The entire version will be available as a machine-readable form at the CDS and at the authors’ webpage. Colums 1 and 2 are the Galactic longitude and latitude; Cols. 3 and 4 list the median velocity and the peak velocity of the maser lines, the reference is listed in Col. 5; Cols. 68 list the photometric or trigonometric distance, its uncertainty and the reference when available; Col. 9 is the note for the kinematic distance ambiguity; the reference is shown in Col. 10; Cols. 11 and 12 list the distance to the GC and the distance to the Sun, the kinematic distances when adopted are calculated with a flat rotation curve with the IAU standard R0 = 8.5 kpc and Θ0 = 220 km s-1 and the standard solar motions; Cols. 13 and 14 are the same as Cols. 11 and 12 except with fundamental parameters R0 = 8.3 kpc and Θ0 = 239 km s-1 (Brunthaler et al. 2011) and the solar motions of Schönrich et al. (2010); Cols. 15 and 16 are the same as Cols. 11 and 12, except with the rotation curve of Brand & Blitz (1993).

Reference. ab09: Anderson & Bania (2009); bdc01: Blum et al. (2001); bbs+08: Bartkiewicz et al. (2008) brm+09: Brunthaler et al. (2009); bph+06: Busfield et al. (2006); cmr+75: Caswell et al. (1975); chr+14: Choi et al. (2014); dlr+11: Dzib et al. (2011); dwbw80: Downes et al. (1980); gcf+12: Green et al. (2012); gm11: Green & McClure-Griffiths (2011); hbc+07: Hirota et al. (2007); hbc+07b: Honma et al. (2007); hhk+11: Honma et al. (2011); irm+13: Immer et al. (2013); kns+11: Kurayama et al. (2011); kjb+03: Kolpak et al. (2003); mrm+09: Moscadelli et al. (2009); msh+11: Motogi et al. (2011); mdf+11: Moisés et al. (2011); mcr+11: Moscadelli et al. (2011); mdf+11: Moisés et al. (2011); nnh+11: Niinuma et al. (2011); okh+10: Oh et al. (2010); oah+13: Olmi et al. (2014); pmg08: Pandian et al. (2008); pmg09: Pandian et al. (2009); pmb05: Pestalozzi et al. (2005); rjh+09: Roman-Duval et al. (2009); rbr+10: Rygl et al. (2010); rbs+12: Rygl et al. (2012); rmb+09: Reid et al. (2009a); swa+04: Sewilo et al. (2004); syby87: Solomon et al. (1987); srm+09: Sanna et al. (2009); shr+10: Sato et al. (2010a); sxc+14: Sun et al. (2014); sh10: Stead & Hoare (2010); uhl12: Urquhart et al. (2012); wam82: Wink et al. (1982); wxm+12: Wu et al. (2012); wsr+14: Wu et al. (2014); xrzm06: Xu et al. (2006); xlh+08: Xu et al. (2008); xrm+09: Xu et al. (2009); xmr+11: Xu et al. (2011); xlr+13: Xu et al. (2013); zzr+09: Zhang et al. (2009).

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