2011ApJ...733..122D


Query : 2011ApJ...733..122D

2011ApJ...733..122D - Astrophys. J., 733, 122 (2011/June-1)

On the distribution of orbital eccentricities for very low-mass binaries.

DUPUY T.J. and LIU M.C.

Abstract (from CDS):

We have compiled a sample of 16 orbits for very low-mass stellar (<0.1 M) and brown dwarf binaries, including updated orbits for HD 130948BC and LP 415-20AB. This sample enables the first comprehensive study of the eccentricity distribution for such objects. We find that very low-mass binaries span a broad range of eccentricities from near-circular to highly eccentric (e ~ 0.8), with a median eccentricity of 0.34. We have examined potential observational biases in this sample, and for visual binaries we show through Monte Carlo simulations that if we choose appropriate selection criteria then all eccentricities are equally represented ( ≲ 5% difference between input and output eccentricity distributions). The orbits of this sample of very low-mass binaries show some significant differences from their solar-type counterparts. They lack a correlation between orbital period and eccentricity, and display a much higher fraction of near-circular orbits (e < 0.1) than solar-type stars, which together may suggest a different formation mechanism or dynamical history for these two populations. Very low-mass binaries also do not follow the e 2 distribution of Ambartsumian, which would be expected if their orbits were distributed in phase space according to a function of energy alone (e.g., the Boltzmann distribution). We find that current numerical simulations of very low-mass star formation do not completely reproduce the observed properties of our binary sample. The cluster formation model of Bate agrees very well with the overall e distribution, but the lack of any high-e (>0.6) binaries at orbital periods comparable to our sample suggests that tidal damping due to gas disks may play too large of a role in the simulations. In contrast, the circumstellar disk fragmentation model of Stamatellos & Whitworth predicts only high-e binaries and thus is highly inconsistent with our sample. These discrepancies could be explained if multiple formation processes are responsible for producing the field population.

Abstract Copyright:

Journal keyword(s): binaries: close - binaries: general - binaries: visual - brown dwarfs - infrared: stars - stars: low-mass - techniques: high angular resolution

Simbad objects: 32

goto Full paper

goto View the references in ADS

Number of rows : 32
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 LP 881-64 ** 00 24 44.1774908692 -27 08 25.263232614   17.18 15.338 13.502 11.403 M5.5/6Ve+M8.5Ve+M9/9.5V 139 0
2 LP 349-25 LM* 00 27 56.0057038615 +22 19 32.635434516   18.6   16.0   M8Ve 73 0
3 * tet Per PM* 02 44 11.9866154103 +49 13 42.414669174 4.62 4.62 4.11 3.67 3.37 F8V 405 0
4 2MASS J03202839-0446358 LM* 03 20 28.3630482681 -04 46 36.396685568           M8.5+T5 44 0
5 Cl* Melotte 22 PPL 15 LM* 03 48 04.6585327824 +23 39 30.318163560         17.91 M6.5 102 0
6 LP 415-20 LM* 04 21 49.5764748384 +19 29 08.566062612           M7+M9.5 45 0
7 V* DF Tau TT* 04 27 02.7932020080 +25 42 22.453341516 11.97 12.25 11.42 10.31 9.14 M3Ve 500 1
8 NAME Taurus Complex SFR 04 41.0 +25 52           ~ 4416 0
9 V* GW Ori Or* 05 29 08.3928710640 +11 52 12.666457092   10.83 10.10 9.52   G5/8Ve 351 0
10 NAME Orion Nebula Cluster OpC 05 35.0 -05 29           ~ 2331 0
11 V* V2384 Ori EB* 05 35 21.8473218600 -05 46 08.571352260       19.21 17.28 M7 99 1
12 LP 206-11 ** 07 11 11.518536 +43 29 56.66532   16.7 15.90 15.746 11.92 M5.5V 38 0
13 LSPM J0746+2000 BD* 07 46 42.50553 +20 00 31.9757       17.9 15.034 L0+L1.5 184 1
14 2MASS J08503593+1057156 BD* 08 50 35.93400 +10 57 15.6168       22.466 20.349 L6.5+L8.5 78 0
15 * sig02 UMa ** 09 10 23.54597 +67 08 02.4642   5.29 4.80     F7V 171 0
16 2MASSW J0920122+351742 BD* 09 20 12.23664 +35 17 42.9684           L5.5+L9 46 0
17 [NC98] Cha HA 8 SB* 11 07 46.0912894776 -77 40 08.918309388   22.2 20.1   15.61 ~ 43 1
18 LP 732-94 LM* 11 21 49.1708652037 -13 13 08.693807585     19.57     M8.5V 131 0
19 2MASSI J1426316+155701 LM* 14 26 31.6133387736 +15 57 01.066079268       18.320 15.819 M9V 30 0
20 HD 130948 BY* 14 50 15.8109853464 +23 54 42.634220112   6.456 5.867     F9IV-V 285 0
21 BD+16 2708B SB* 14 54 29.4185719182 +16 06 08.616294953           M8.5 137 0
22 2MASSI J1534498-295227 BD* 15 34 49.84080 -29 52 27.4188           T4.5+T5 66 0
23 LSR J1610-0040 LM* 16 10 28.9498230750 -00 40 53.964223684       17.51 14.81 sdM6.5 52 0
24 * sig CrB RS* 16 14 40.85557 +33 51 30.9497           F6V+G0V 493 0
25 2MASSW J1728114+394859 BD* 17 28 11.50056 +39 48 59.3100           L5+L6.5 56 0
26 LSPM J1750+4424 LM* 17 50 12.9048979032 +44 24 04.388509332   21.0   18.8   M6.5+M8.5 21 0
27 2MASSI J1847034+552243 SB* 18 47 03.4341091776 +55 22 43.458679704   18.7   16.4   M6+M7 13 0
28 2MASS J21321145+1341584 BD* 21 32 11.45376 +13 41 58.4124           L4.5+L8.5 22 0
29 2MASS J21402931+1625183 ** 21 40 29.3219106816 +16 25 18.097174704         15.36 M8+M9.5 32 0
30 * eps Ind B BD* 22 04 10.5951812451 -56 46 58.239102418     24.12 20.8 15.60 T1V+T6V 163 1
31 2MASSW J2206228-204705 SB* 22 06 22.8297746064 -20 47 06.597790152     19.788 17.452 14.877 M8.0V 45 0
32 2MASS J22521073-1730134 BD* 22 52 10.7512306563 -17 30 13.889743018         17.9 L4.5+T3.5 56 0

To bookmark this query, right click on this link: simbad:objects in 2011ApJ...733..122D and select 'bookmark this link' or equivalent in the popup menu