Table 3: Line parameters of newly detected masers.
Source Adopted Epoch $\int{S{\rm d}V}^{a}$ $V_{\rm LSR,opt}^{a,b}$ $\Delta V_{1/2}^{a}$ Channel rms log  $L_{\rm H_2O}^{d}$ Comments
  distance         widthc      
  (Mpc) (2002) (mJy km s-1) (km s-1) (km s-1) (km s-1) (mJy) ($L_{\odot}$)  
Mrk 1066 48 Mar. 07 $ 696\pm61 $ $3547.2\pm1.4$ $ 38.7\pm04.6$ 1.08 5.3 1.6 see Fig. 1
      $ 169\pm12 $ $3635.9\pm0.1$ $ 2.1\pm00.2$ 1.08 5.3 1.0 see Fig. 1
      $ 171\pm17 $ $3635.9\pm0.1$ $ 1.9\pm00.2$ 0.07 29.7 1.0 see Fig. 2
    Mar. 10 $ 822\pm59 $ $3547.8\pm1.3$ $ 38.3\pm03.4$ 1.08 5.6 1.6 see Fig. 1
      $ 193\pm13 $ $3636.2\pm0.1$ $ 2.1\pm00.2$ 1.08 5.6 1.0 see Fig. 1
      $ 157\pm16 $ $3636.1\pm0.1$ $ 1.2\pm00.2$ 0.07 34.9 0.9 see Fig. 2
    May 03 $ 566\pm16 $ $3552.8\pm7.7$ $ 46.2\pm16.9$ 1.08 15.0 1.5 see Fig. 1
      $ 166\pm33 $ $3635.9\pm0.2$ $ 1.7\pm00.4$ 1.08 15.0 0.9 see Fig. 1
    Sep. 27 $ 143\pm31 $ $3635.2\pm0.2$ $ 2.0\pm00.5$ 1.08 13.7 0.9 see Fig. 1
Mrk 34e 205 Mar. 08 $ \phantom{0}46\pm14 \phantom{0} $ $14661.2\pm0.4$ $ 2.1\pm00.8$ 1.16 5.8 1.6 see Fig. 3
      $ 354\pm52 \phantom{0} $ $14837.6\pm2.3$ $ 31.9\pm05.3$ 1.16 5.8 2.5 see Fig. 3
      $ 417\pm78 \phantom{0} $ $15771.7\pm8.7$ $ 88.2\pm16.2$ 9.29 1.9 2.6 see Fig. 4
    Mar. 17 $ 335\pm57\phantom{0} $ $14840.5\pm2.9$ $ 36.5\pm07.8$ 1.16 5.5 2.5 see Fig. 3
    May 07 $ \phantom{0}77\pm24\phantom{0} $ $14674.9\pm0.8$ $ 5.0\pm01.9$ 1.16 6.6 1.9 see Fig. 3
      $ 323\pm62 \phantom{0} $ $14838.7\pm2.9$ $ 31.2\pm07.6$ 1.16 6.6 2.5 see Fig. 3
      $ 995\pm122 $ $15754.9\pm8.0$ $ 130.4\pm18.4$ 9.30 2.3 3.0 see Fig. 4
    May 09 $ \phantom{0} 67\pm25 \phantom{0} $ $14658.2\pm0.8$ $ 4.7\pm02.2$ 4.67 3.4 1.8 see Fig. 3
      $ 559\pm81 \phantom{0} $ $14837.4\pm3.1$ $ 43.9\pm08.2$ 4.67 3.4 2.7 see Fig. 3
      $ 607\pm92 \phantom{0} $ $15787.2\pm9.6$ $ 115.5\pm19.9$ 18.67 1.4 2.8 see Fig. 4
      $ 117\pm32 \phantom{0} $ $15738.2\pm1.1$ $ 6.9\pm03.0$ 4.67 3.2 2.1 see Fig. 4
      $ 394\pm87 \phantom{0} $ $15803.1\pm4.2$ $ 47.8\pm15.0$ 4.67 3.2 2.6 see Fig. 4
NGC 3556 12 Mar. 12 $ 505\pm72 \phantom{0} $ $738.5\pm1.1 $ $ 15.1\pm2.2 $ 1.06 11.6 0.2 see Fig. 5
    Mar. 15 $ \phantom{0} 99\pm29\phantom{0} $ $738.0\pm0.3 $ $ 2.1\pm0.5 $ 1.06 10.1 -0.5 see Fig. 5
      $ 421\pm78 \phantom{0} $ $740.3\pm1.6 $ $ 17.9\pm4.8 $ 1.06 10.1 0.1 see Fig. 5
    May 05 $ 229\pm35 \phantom{0} $ $737.2\pm0.4 $ $ 4.8\pm0.8 $ 1.06 10.9 -0.1 see Fig. 5
    Sep. 27 $ 329\pm75 \phantom{0} $ $737.1\pm1.1 $ $ 10.0\pm2.9 $ 4.21 6.5 0.0 see Fig. 5
Arp 299 42 Mar. 16 $6210\pm242 $ $3101.8\pm05.1$ $ 260.2\pm11.5$ 4.30 4.8 2.4 see Fig. 6
a Obtained from Gaussian fits.
b See the caption to Fig. 1.
c Channel width of the spectra used for the Gaussian fits. Some of the spectra shown in Figs. 1-7 are smoothed.
d $L_{\rm H_2O}$/[$L_{\odot}$] = 0.023 $\times$ $\int{S {\rm d}V}$/[Jy km s-1] $\times$ D2/[Mpc2].
e To the observations of the high velocity feature (15787 km s-1) from May 9: the first Gaussian fit refers to the smoothed profile shown in Fig. 4; the latter two component fit refers to the unsmoothed spectrum with a channel spacing of 4.7 km s-1.

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