2017ApJS..230...19B


Query : 2017ApJS..230...19B

2017ApJS..230...19B - Astrophys. J., Suppl. Ser., 230, 19-19 (2017/June-0)

An advanced N-body model for interacting multiple stellar systems.

BROZ M.

Abstract (from CDS):

We construct an advanced model for interacting multiple stellar systems in which we compute all trajectories with a numerical N-body integrator, namely the Bulirsch-Stoer from the SWIFT package. We can then derive various observables: astrometric positions, radial velocities, minima timings (TTVs), eclipse durations, interferometric visibilities, closure phases, synthetic spectra, spectral energy distribution, and even complete light curves. We use a modified version of the Wilson-Devinney code for the latter, in which the instantaneous true phase and inclination of the eclipsing binary are governed by the N-body integration. If all of these types of observations are at one's disposal, a joint χ2 metric and an optimization algorithm (a simplex or simulated annealing) allow one to search for a global minimum and construct very robust models of stellar systems. At the same time, our N-body model is free from artifacts that may arise if mutual gravitational interactions among all components are not self-consistently accounted for. Finally, we present a number of examples showing dynamical effects that can be studied with our code and we discuss how systematic errors may affect the results (and how to prevent this from happening).

Abstract Copyright: © 2017. The American Astronomical Society. All rights reserved.

Journal keyword(s): binaries: close - binaries: eclipsing - methods: numerical - techniques: interferometric - techniques: photometric - techniques: radial velocities - techniques: radial velocities

Simbad objects: 16

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Number of rows : 16
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 * ksi Tau PM* 03 27 10.1405792544 +09 43 57.871023240 3.33 3.66 3.75 3.76 3.85 B9Vn 198 0
2 * lam Tau SB* 04 00 40.8167738514 +12 29 25.239987626 2.66 3.29 3.41 3.44 3.53 B4IV 364 0
3 HD 91962 SB* 10 36 59.9979931102 -08 50 23.512435908   7.87 7.23   6.34 G1V 77 0
4 HD 95660 SB* 11 02 51.9104777040 +30 24 54.702250596   8.43 8.06     F5V 99 1
5 HD 109648 SB* 12 35 59.9179796448 +36 15 28.180878804   9.19 8.8     F5V 62 0
6 HD 144548 EB* 16 07 17.7847898136 -22 03 36.556794720   9.37 8.752   7.868 F7V 70 0
7 V* V907 Sco SB* 17 56 55.5622524456 -34 45 01.218496968   8.75 8.63     B9V 56 0
8 V* V994 Her ** 18 27 45.89332 +24 41 50.6652           B9Vn 70 1
9 KOI-6625 EB* 18 58 20.5286857776 +41 00 34.498680156           F6IV 29 0
10 KOI-6545 EB* 18 58 46.3378826448 +40 29 55.062482712           ~ 24 0
11 KOI-6899 EB* 19 05 06.4737051312 +43 20 20.880322836           ~ 27 0
12 HD 181068 SB* 19 17 08.9786734416 +41 15 53.314415820   8.01 7.09     G8III+G8V+K1V 90 0
13 KOI-6938 RG* 19 20 44.7017781024 +43 43 25.855119624   14.082 12.901     K1IV 50 0
14 KOI-6073 EB* 19 34 09.6670928808 +46 26 14.022392424           ~ 30 0
15 KOI-399 EB* 19 35 51.8565988536 +42 50 14.161269084           ~ 42 0
16 KOI-1351 EB* 19 44 03.4738784784 +42 25 20.095789620       15.815   ~ 24 0

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