NameTypeR.A. (J2000)Dec
(J2000)
Jet speedν
(GHz)
F
(mJy)
D
(kpc)
δΓθ
(deg)
CI CamHMXRB04:19:42.13+55:59:57.70.15c22.54501.01.011.0183
XTE J1118+480HMXRB11:18:10.7+48:02:12.30.4c2 x 10+05201.9
GRO J1655-40HMXRB16:54:00.13-39:50:44.90.27±0.03c1.634003.10.462.5581
KS 1731-260LMXRB17:34:13.46-26:05:18.6
1E 1740.7-2942LMXRB17:43:54.83-29:44:42.00.7c
XTE J1748-282917:43:54.83-29:44:42.0?4.94108.01.011.4664
GRS 1758-258LMXRB18:01:12.40-25:44:36.1<=0.3c
V4641 SagitariiHMXRB18:19:21.63-25:24:25.840.9c4.94009.67.3122.376.9
V691 CrALMXRB18:25:46.8-37:06:18.52
LS 5039HMXRB18:26:15.0-14:50:54.2>0.15c5.0163.01.041.0968
XTE J1859+226HMXRB18:58:41.58+22:39:29.4?
SS 433HMXRB19:11:49.56+04:58:57.80.26c
GRS 1915+105HMXRB19:15:11.5+10:56:44.90.60c8.665512.50.572.5570
Cygnus X-1HMXRB19:58:21.6+35:12:05.78?1x 10+04152.0
Cygnus X-3HMXRB20:32:25.78+40:57:27.90.48-0.81c15.01050010.03.142.1014
XTE J1720-318LMXRB17:19:58.9-31:45:01.11
Sco X-1LMXRB16:19:55.06-15:38:25.05.0202.81.393.2044

List of the 17 known microquasars observable within the Noto–KM3NeT declination limits. The information on distance (D), observing frequency (ν), and corresponding flux density (Fν) was taken from the study by Distefano et al. (2002). From the same work, we also adopted the values of the Doppler factor (δ), the angle between the jet axis and the observer’s line of sight (θ), and the Lorentz factor (Γ), for the resolved microquasars. For unresolved microquasars, no information is available on Γ, δ, or on the jet size.