RA (ICRS) DEC
|
ℓ b
|
Distance [kpc] |
2.4±0.4 7±1 |
dellaValle1994 Saikia2022Casares2023 |
---|---|---|
Distance to the plane (z) [kpc] |
0.29±0.05 0.9±0.1 |
dellaValle1994 Saikia2022Casares2023 |
Orbital period (Porb) [h] | 6.7±0.2 | Casares2023 |
Peak X-ray flux [erg s-1 cm-2] [keV] |
1.97E-08 [2-10] |
Revnivtsev1998a |
Outburst magnitude (AB) | V∼16.6 | dellaValle1994 |
Quiescent magnitude (AB) | i’=21.39±0.05 | dellaValle1994Casares2023Saikia2022 |
E(B-V) [mag] | 0.9 | dellaValle1994 |
Strictly speaking it is not a dynamical BH but there is either a robust mass function or mass determination suggesting the presence of a BH
N Oph 1993 is too faint (r=23.2±0.1; Casares2023) to perform a dynamical study with current instrumentation. However, Casares2023 derived the dynamical parameters below using the FWHM (Hα) - K2 relation (Casares2015) using time-resolved spectroscopy. It had another outburst on December 2016 (Negoro2016a) |
Orbital period [h] | 6.7±0.2 | Casares2023 |
---|---|---|
Star's spectral type | M0-5V ~ K6 |
Chaty2002a Casares2023 |
Star's radial velocity amplitude (K2) [km/s] | 521±52 | Casares2023 |
Mass function 'f(M1)' [M☉] | 4±1 | Casares2023 |
BH mass (M1) [M☉] | 6.4+3.2-2.0 | Casares2023 |
Mass ratio (q=M2/M1) | ≤0.25 | Casares2023 |
Inclination angle (i) [deg] | 61±15 | Casares2023 |
|
|||
---|---|---|---|
V∼16.6 | |||
dellaValle1994Casares2023Saikia2022 |
|||
B≥21.3 | V≥21.0 | R≥20.06 | |
r=23.2±0.1 | i’=21.39±0.05 | ||
Click to enlarge in new tab/window
Orientation: North up, East left.
Object marked
Click to enlarge in new tab/window
BA=17.80 | VA=16.24 | RA=15.06 |
BB=17.48 | VB=15.72 | RB=14.66 |
BC=15.48 | VC=13.82 | RC=12.76 |
BD=16.99 | VD=15.92 | RD=15.26 |
BE=15.07 | VE=13.86 | RE=13.06 |