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Table 2

Parameters of the maser lines observed with the VLA.

Source Distance Array Peak coordinatesa V LSR,optb L H2Oc Notes
(Mpc) RA Dec. (km s-1) (Jy km s-1) (L)

NGC 3556 12 CnB 11 11 31.46  ±  0.02 +55 40 28.8  ±  0.2 738.2  ±  0.7 0.087  ±  0.004 0.29  ±  0.01
NGC 3556 12 DnA 11 11 31.47  ±  0.01 +55 40 28.7  ±  0.1 737.5  ±  0.1 0.083  ±  0.005 0.28  ±  0.01
Arp 299
– IC 694 42 A 11 28 33.65  ±  0.01 +58 33 46.8  ±  0.1 2996  ±  8 0.16  ±  0.03 6.4  ±  1.2
D 11 28 33.65  ±  0.01 +58 33 46.8  ±  0.1 2988  ±  2 0.46  ±  0.03 19  ±  1
– NGC 3690 A 11 28 30.99  ±  0.01 +58 33 40.7  ±  0.1 3112  ±  8 0.41  ±  0.05 17  ±  2
D 11 28 30.97  ±  0.02 +58 33 40.8  ±  0.2 3112  ±  4 0.55  ±  0.03 22  ±  1
– C+C’-complex A 11 28 30.63  ±  0.01 +58 33 52.4  ±  0.1 3179  ±  18 0.18  ±  0.04 7.5  ±  1.5 tentative
C’ D 11 28 31.35  ±  0.02 +58 33 49.8  ±  0.2 3158  ±  4 0.30  ±  0.04 12  ±  2
C D 11 28 30.65  ±  0.11 +58 33 49.3  ±  0.9 3142  ±  7 0.12  ±  0.03 4.9  ±  1.0 tentative
NGC 4151 13 DnA 12 10 32.58  ±  0.01 +39 24 21.1  ±  0.1 695.6  ±  0.3 0.009  ±  0.002 0.035  ±  0.007 tentative

Notes. 

(a)

Error estimates associated with this quantity are discussed in Sect. 2.4.

(b)

All values obtained by Gaussian fits to the maser line(s) with the exception of NGC 4151 where a Gaussian fit would have been meaningless. In this case, the channel width of the spectrum was taken as a reliable upper limit for the uncertainty in the peak velocity, and the error on the line-integrated intensity has been computed assuming errors of 10 and 20% in the line intensity and width, respectively.

(c)

LH2O/[L] = 0.023  ×  ∫SdV/[Jy km s-1]  ×  D2/ [Mpc2] .

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