2014ApJ...794..144R


Query : 2014ApJ...794..144R

2014ApJ...794..144R - Astrophys. J., 794, 144 (2014/October-3)

Generalized investigation of the rotation-activity relation: favoring rotation period instead of Rossby number.

REINERS A., SCHUSSLER M. and PASSEGGER V.M.

Abstract (from CDS):

Magnetic activity in Sun-like and low-mass stars causes X-ray coronal emission which is stronger for more rapidly rotating stars. This relation is often interpreted in terms of the Rossby number, i.e., the ratio of rotation period to convective overturn time. We reconsider this interpretation on the basis of the observed X-ray emission and rotation periods of 821 stars with masses below 1.4 M☉. A generalized analysis of the relation between X-ray luminosity normalized by bolometric luminosity, LX/Lbol, and combinations of rotational period, P, and stellar radius, R, shows that the Rossby formulation does not provide the solution with minimal scatter. Instead, we find that the relation LX/Lbol∝P –2 R –4 optimally describes the non-saturated fraction of the stars. This relation is equivalent to LX∝P –2, indicating that the rotation period alone determines the total X-ray emission. Since LX is directly related to the magnetic flux at the stellar surface, this means that the surface flux is determined solely by the star's rotation and is independent of other stellar parameters. While a formulation in terms of a Rossby number would be consistent with these results if the convective overturn time scales exactly as Lbol–1/2, our generalized approach emphasizes the need to test a broader range of mechanisms for dynamo action in cool stars.

Abstract Copyright: ∼

Journal keyword(s): dynamo - stars: activity - stars: magnetic field

Simbad objects: 20

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Number of rows : 20
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 * alf Per V* 03 24 19.3700924 +49 51 40.245455 2.64 2.27 1.79     F5Ib 870 1
2 Cl Melotte 22 OpC 03 46 38.0 +24 10 41           ~ 3679 0
3 Cl Melotte 25 OpC 04 30 27.4 +16 46 43           ~ 3309 0
4 V* V1005 Ori BY* 04 59 34.8342878424 +01 47 00.669818328   11.48 10.107 9.603 8.239 M0Ve 371 0
5 G 99-49 PM* 06 00 03.5042217306 +02 42 23.592579736   12.97 11.31 10.92 8.43 M3.5Ve 170 0
6 NGC 2516 OpC 07 58 00.5 -60 46 36           ~ 793 0
7 NGC 2547 OpC 08 10 01.5 -49 12 08           ~ 445 0
8 NGC 2632 OpC 08 39 58.4 +19 36 33           ~ 1733 0
9 IC 2391 OpC 08 41 17.5 -53 03 00           ~ 871 0
10 HD 81809 ** 09 27 46.8088908054 -06 04 17.008787302           G1.5IV-V 322 0
11 V* AD Leo PM* 10 19 36.2808181226 +19 52 12.010446571   10.82 9.52 9.19   dM3 1469 1
12 IC 2602 OpC 10 42 55.9 -64 25 22           ~ 735 0
13 V* DS Leo BY* 11 02 38.3420210088 +21 58 01.700013360 12.246 11.049 9.572 8.638 7.634 M1.0Ve 269 0
14 V* GL Vir PM* 12 18 59.3997287457 +11 07 33.773236317   15.68 13.90 13.55   M4.5Ve 191 0
15 Wolf 461 PM* 13 00 33.5221795982 +05 41 07.996620384   15.12   13.041   M4.5Ve 156 0
16 BD+13 2618 RS* 13 00 46.5566863405 +12 22 32.677229903 12.314 11.233 9.750 8.785 7.653 M0V 383 1
17 NAME Proxima Centauri PM* 14 29 42.9461331854 -62 40 46.164680672 14.21 12.95 11.13 9.45 7.41 M5.5Ve 1483 0
18 CD-38 11343 Er* 16 56 48.56771 -39 05 38.1219 13.803 12.806 11.332 10.143 8.773 M3Ve+M4Ve 50 0
19 Ross 868 PM* 17 19 54.2077697528 +26 30 03.068999297   12.98 11.336 11.060 8.420 M3.5V 169 0
20 G 24-16 Er* 20 29 48.3179167836 +09 41 20.590506834       12.728   M4.5V 164 0

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