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首页> 外文期刊>The Astrophysical journal >Rotation and Activity in Mid-M to L Field Dwarfs
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Rotation and Activity in Mid-M to L Field Dwarfs

机译:中M到L田间矮人的旋转和活动

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We analyze rotation velocities and chromospheric (Hα) activity, derived from high-resolution spectra, in a large sample of mid-M to L field dwarfs. The projected rotation velocity is found to increase from mid-M to L. This is consistent with a lengthening of spin-down timescale with later type, although in the L types the trend may also be a function of the observational bias toward younger objects. From M4 to M8.5 a saturation-type rotation-activity relation is seen, similar to that in earlier types, when activity is measured through either FHα or LHα/Lbol. However, we find that activity saturates at a significantly higher velocity (~10 km s-1) in the M5.5-M8.5 dwarfs than in the M4-M5 ones (4 km s-1). This may result from a change in the dynamo behavior with later type (see also below). We note that the saturation level in Hα emission appears to vary somewhat less with spectral type (from M4 to M8.5) when activity is measured through LHα/Lbol instead of FHα. In M9 and later dwarfs, we observe a drastic drop in activity and a sharp break in the rotation-activity connection: Hα emission levels in these dwarfs are much lower than in earlier types, and often undetectable, in spite of very rapid rotation. This may be caused by the very high resistivities in the predominantly neutral atmospheres of these dwarfs, which would damp the magnetic energy available for supporting a chromosphere. It is also possible that the rapid formation of dust in these cool atmospheres exacerbates this effect, as charged particles are soaked up by (more massive) dust grains. Finally, we note that spectral type determination from low-resolution spectra may be affected by gravity effects: cooler, lower gravity objects may mimic hotter, higher gravity ones. Therefore, it is possible that the few unsaturated fast rotators from M5.5 to M8.5 (whose presence leads us to ascribe a higher saturation velocity to these spectral types, as noted above) may actually be very low mass objects, with lower Teff (and gravity) than their spectral types suggest. If so, their behavior (low activity, fast rotation) would be compatible with that of the cool M9 and later dwarfs (and no change in dynamo behavior would have to be postulated in the M5.5-M8.5 dwarfs). This interpretation is supported by a preliminary analysis of the high-resolution spectra of these anomolous objects. It is also bolstered by the fact that a saturation-type Rossby number-activity relation is seen in the M5.5-M8.5 dwarfs when these anomalous objects are removed from the sample, while the relationship is much weaker when they are included.
机译:我们分析了从高分辨率光谱得出的中M到L场矮的大样本的旋转速度和色球(Hα)活性。发现预计的旋转速度从M中间增加到L。这与后一种类型的旋转时间尺度的延长相一致,尽管在L型中,趋势也可能是对年轻物体的观测偏差的函数。从M4到M8.5,当通过FHα或LHα/ Lbol测量活性时,可以看到与早期类型相似的饱和型旋转-活性关系。但是,我们发现,M5.5-M8.5矮星的活动饱和速度明显高于M4-M5矮星(4 km s-1),饱和速度更高(〜10 km s-1)。这可能是由于发电机类型的变化而导致的,其类型更高(另请参见下文)。我们注意到,当通过LHα/ Lbol而不是FHα测量活性时,Hα发射的饱和水平随光谱类型(从M4到M8.5)的变化似乎较小。在M9及以后的矮星中,我们观察到活动性急剧下降,并且旋转-活动关系急剧中断:这些矮星中的Hα排放水平远低于早期类型,尽管旋转非常快,但通常无法检测到。这可能是由于这些矮星的主要是中性大气中很高的电阻率导致的,这会削弱可用于支撑色球的磁能。由于带电粒子被(更大质量的)尘粒吸收,在这些凉爽的气氛中迅速形成尘埃也可能加剧这种影响。最后,我们注意到低分辨率光谱的光谱类型确定可能会受到重力效应的影响:温度较低,重力较低的物体可能会模拟温度较高,重力较高的物体。因此,从M5.5到M8.5的少数不饱和快速旋转器(如上所述,其存在使我们将较高的饱和速度归因于这些光谱类型)可能实际上是质量很低的物体,而Teff较低(和重力)超出其光谱类型所建议的范围。如果是这样,它们的行为(低活动性,快速旋转)将与凉爽的M9和后来的矮人的行为兼容(并且不必假设M5.5-M8.5矮人的发电机行为将发生变化)。对这些无色物体的高分辨率光谱的初步分析支持了这种解释。当从样品中除去这些异常物体时,在M5.5-M8.5矮星中可以看到饱和型Rossby数-活性关系,这也为这一事实提供了支持,而当将它们包括在内时,该关系就弱得多。

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