论文标题

测试相干无线电发射与热磁星的物理参数之间的缩放关系

Testing a scaling relation between coherent radio emission and physical parameters of hot magnetic stars

论文作者

Das, Barnali, Chandra, Poonam, Shultz, Matt E., Leto, Paolo, Mikulášek, Zdeněk, Petit, Véronique, Wade, Gregg A.

论文摘要

在二十多年前发现了通过热磁星的电子回旋摩泽发射(ECME)的相干无线电发射,但是使ECME有利的物理条件仍然不确定。直到最近,才是经验关系,将ECME的光度与恒星磁场和温度联系起来,它建议解释是什么使热磁星能够产生ECME。然而,这种关系仅14颗恒星获得了。因此,重要的是要检查这种关系是否牢固。为了测试鲁棒性,我们对五个热磁星星进行了无线电观察。这导致发现了另外三颗生产ECME的星星。我们发现,在添加新发现的恒星后,提出的缩放关系仍然有效。但是,我们发现,磁场和有效温度与$ t_ \ mathrm {eff} \ Lessim 16 $ kk(可能是小样本量的工件)相关,从而使ECME亮度与$ t_ \ Mathrm {eff} $之间的拟议连接变得不可靠。通过根据缩放定律的无线电发射来检查经验关系,我们得出的结论是,两种发射都由相同的磁层现象驱动。就像不连贯的排放一样,连贯的无线电排放对后期B和A型星的$ t_ \ mathrm {eff} $无关紧要,但是$ t_ \ mathrm {eff} $似乎对早期b型星星显得很重要,可能是由于吸收率更高,或者是由于更高的吸收而引起的,或者是在降低排放位置的高血浆密度降低生产的作品。

Coherent radio emission via electron cyclotron maser emission (ECME) from hot magnetic stars was discovered more than two decades ago, but the physical conditions that make the generation of ECME favourable remain uncertain. Only recently was an empirical relation, connecting ECME luminosity with the stellar magnetic field and temperature, proposed to explain what makes a hot magnetic star capable of producing ECME. This relation was, however, obtained with just fourteen stars. Therefore, it is important to examine whether this relation is robust. With the aim of testing the robustness, we conducted radio observations of five hot magnetic stars. This led to the discovery of three more stars producing ECME. We find that the proposed scaling relation remains valid after the addition of the newly discovered stars. However we discovered that the magnetic field and effective temperature correlate for $T_\mathrm{eff}\lesssim 16$ kK (likely an artifact of the small sample size), rendering the proposed connection between ECME luminosity and $T_\mathrm{eff}$ unreliable. By examining the empirical relation in light of the scaling law for incoherent radio emission, we arrive at the conclusion that both types of emission are powered by the same magnetospheric phenomenon. Like the incoherent emission, coherent radio emission is indifferent to $T_\mathrm{eff}$ for late-B and A-type stars, but $T_\mathrm{eff}$ appears to become important for early-B type stars, possibly due to higher absorption, or, higher plasma density at the emission sites suppressing the production of the emission.

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