2013A&A...556A..14G


Query : 2013A&A...556A..14G

2013A&A...556A..14G - Astronomy and Astrophysics, volume 556A14-14 (2013/8-1)

X-ray emission regimes and rotation sequences in M 35. An updated model of stellar activity evolution on the main sequence.

GONDOIN P.

Abstract (from CDS):

Late-type stars in young open clusters show two kinds of dependence of their X-ray emission on rotation. They also tend to group into two main sub-populations that lie on narrow sequences in diagrams where their rotation periods are plotted against their (B-V) colour indices. A correlation between these two regimes of X-ray emission and the rotation sequences has been recently observed in the M34 open cluster. Sun-like M34 stars also show a drop of their X-ray to bolometric luminosity ratio by about one order of magnitude at a Rossby number of about 0.3. The present study looks for similar connections between X-ray activity and rotation in an other open cluster. The aim is to consolidate a model of X-ray activity evolution on the main sequence and to provide observational constraints on dynamo processes in the interiors of late-type stars. The paper compares XMM-Newton measurements of X-ray stellar emission in M35 with X-ray luminosity distributions derived from rotation period measurements assuming either an X-ray regime transition at a critical Rossby number or a correlation between X-ray emission regimes and rotation sequences. This second hypothesis could account for the low number of M35 stars detected in X-rays. A model of X-ray activity evolution is proposed based on the correlation. One major output is that the transition from saturated to non-saturated X-ray emission occurs at Rossby numbers between about 0.13 and 0.4 for each star depending on its mass and initial period of rotation on the ZAMS. This prediction agrees with observations of stellar X-ray emission in M34. It explains the large range of X-ray luminosities observed among Sun-like stars in young open clusters. I conclude that the correlation between X-ray emission regimes and rotation sequences could be a fundamental property of the early evolution of stellar magnetic activity on the main sequence. I argue that the angular momentum redistribution mechanism(s) responsible for the transition between rotation sequences could result in a changing mixture of dynamo processes occurring side by side, possibly including a turbulent dynamo at high rotation rate and an interface-type dynamo whose efficiency decreases progressively at later stage of stellar evolution when rotation dies away.

Abstract Copyright: ∼

Journal keyword(s): open clusters and associations: general - stars: activity - stars: coronae - stars: evolution - stars: rotation - fields magnetic

Simbad objects: 30

goto Full paper

goto View the references in ADS

Number of rows : 30
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 NGC 752 OpC 01 56 53.7 +37 45 06           ~ 712 0
2 NGC 1039 OpC 02 42 09.1 +42 44 02           ~ 467 0
3 Cl Melotte 20 MGr 03 26 50.6 +48 51 48           ~ 928 0
4 Cl Melotte 22 OpC 03 46 38.0 +24 10 41           ~ 3679 0
5 Cl Melotte 25 OpC 04 30 27.4 +16 46 43           ~ 3309 0
6 Cl* NGC 2168 MMS 126 BY* 06 08 02.0409940447 +24 26 47.393644389   17.4419 16.4237 16.0444   ~ 15 0
7 Cl* NGC 2168 SB 12 Ro* 06 08 09.9699104136 +24 21 00.576948312   15.69 14.71 14.3094   ~ 7 0
8 Cl* NGC 2168 SB 47 Ro* 06 08 12.9127000344 +24 17 47.923768248   17.7342 16.602 16.2443   ~ 12 0
9 Cl* NGC 2168 SB 101 Ro* 06 08 17.7492795384 +24 12 25.515745092   16.21 15.3 14.9758   ~ 10 0
10 Cl* NGC 2168 BSB 5287 MS* 06 08 27.6287518536 +24 12 37.243513944 17.992 17.417 16.339 15.714 15.113 ~ 19 0
11 Cl* NGC 2168 MMS 175 SB* 06 08 37.8915781873 +24 31 45.531079653   16.97 15.817 15.4425 14.634 K1 18 0
12 Cl* NGC 2168 SB 417 Ro* 06 08 42.8742369744 +24 29 38.964967872   16.79 15.78 15.3101   ~ 14 0
13 Cl* NGC 2168 SB 447 Ro* 06 08 45.1039253424 +24 19 56.158529736   15.866 14.886 14.5614   ~ 12 0
14 NGC 2168 394 Ro* 06 09 00.4973483904 +24 11 59.828038332   15.35 14.53 14.201   ~ 12 0
15 Cl* NGC 2168 BSB 5280 Ro* 06 09 01.9194408648 +24 16 34.750572816   17.45 16.405 15.8992 15.060 ~ 8 0
16 Cl* NGC 2168 SB 688 SB* 06 09 02.5177122216 +24 19 51.883324536   17.34 16.28 15.8378   ~ 10 0
17 Cl* NGC 2168 SB 706 MS* 06 09 03.5253817440 +24 17 23.471347920 17.637 17.047 15.951 15.287 14.669 M 19 0
18 NGC 2168 OpC 06 09 07.5 +24 20 15           ~ 604 0
19 Cl* NGC 2168 BSB 5640 * 06 09 08.6435063040 +24 29 46.989276972     19.168   17.100 ~ 4 0
20 Cl* NGC 2168 BSB 5482 Ro* 06 09 13.7588062008 +24 15 47.770452576   19.3946 17.919 17.3643 16.235 ~ 6 0
21 Cl* NGC 2168 MMS 225 MS* 06 09 15.5721098832 +24 10 42.205419696 17.082 16.501 15.467 14.858 14.295 K1 16 0
22 NGC 2168 54 SB* 06 09 21.9900308472 +24 18 49.920797232   16.93 15.85 15.3239   ~ 14 0
23 Cl* NGC 2168 SB 974 MS* 06 09 23.5606951992 +24 31 15.511179180   17.080 15.918 15.271 14.597 ~ 16 0
24 Cl* NGC 2168 BSB 5181 Ro* 06 09 28.7859657984 +24 25 33.063290580 17.001 16.622 15.669 15.115 14.568 ~ 18 0
25 Cl* NGC 2168 MMS 242 MS* 06 09 31.9021095997 +24 10 38.528434966 16.243 15.923 15.014 14.465 13.946 ~ 17 0
26 NGC 2516 OpC 07 58 00.5 -60 46 36           ~ 793 0
27 NGC 2547 OpC 08 10 01.5 -49 12 08           ~ 445 0
28 NGC 2632 OpC 08 39 58.4 +19 36 33           ~ 1733 0
29 IC 2391 OpC 08 41 17.5 -53 03 00           ~ 871 0
30 IC 2602 OpC 10 42 55.9 -64 25 22           ~ 735 0

To bookmark this query, right click on this link: simbad:objects in 2013A&A...556A..14G and select 'bookmark this link' or equivalent in the popup menu