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QUANTUM NATURE OF CYCLOTRON HARMONICS IN THERMAL SPECTRA OF NEUTRON STARS

机译:中子星热谱中回旋回波的量子性质

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Some isolated neutron stars (NSs) show harmonically spaced absorption features in their thermal soft X-ray spectra. The interpretation of the features as a cyclotron line and its harmonics has been suggested, but the usual explanation of the harmonics as caused by relativistic effects fails because the relativistic corrections are extremely small in this case. We suggest that the features, known as quantum oscillations, correspond to the peaks in the energy dependence of the free-free opacity in a quantizing magnetic field. The peaks arise when the transitions to new Landau levels become allowed with increasing the photon energy; they are strongly enhanced by the square-root singularities in the phase-space density of quantum states in the case when the free (non-quantized) motion is effectively one dimensional. To explore observable properties of these quantum oscillations, we calculate models of hydrogen NS atmospheres with B ~ 1010-1011?G (i.e., electron cyclotron energy E c,e ~ 0.1-1?keV) and T eff = 1-3 MK. Such conditions are thought to be typical for the so-called central compact objects in supernova remnants, such as 1E?1207.4-5209 in PKS 1209-51/52. We show that observable features at the electron cyclotron harmonics form at moderately large values of the quantization parameter, b eff ≡ E c,e /kT eff 0.5-20. The equivalent widths of the features can reach ~100-200 eV; they grow with increasing b eff and are lower for higher harmonics.
机译:一些孤立的中子星(NSs)在其热软X射线光谱中显示出谐波间隔的吸收特征。已经提出将特征解释为回旋加速器线及其谐波,但是由于相对论校正在这种情况下非常小,因此通常无法解释由相对论效应引起的谐波。我们建议这些称为量子振荡的特征对应于量化磁场中自由-不透明的能量依赖性的峰值。当随着光子能量的增加而允许过渡到新的朗道能级时,就会出现峰值。当自由(非量化)运动实际上是一维时,量子态的相空间密度中的平方根奇异性极大地增强了它们。为了探索这些量子振荡的可观察特性,我们计算了B = 1010-1011?G(即电子回旋​​加速器能量E c,e〜0.1-1?keV)和T eff = 1-3 MK的氢NS​​大气的模型。对于超新星遗迹中所谓的中心致密物体,例如PKS 1209-51 / 52中的1E?1207.4-5209,这种条件被认为是典型的。我们表明,在一定范围内,量化参数b eff≡E c,e / kT eff 0.5-20的值较大时,在电子回旋加速器谐波处形成了可观察到的特征。功能的等效宽度可以达到〜100-200 eV;它们随着b eff的增加而增长,而对于高次谐波则更低。

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