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首页> 外文期刊>The Astrophysical journal >INDUCED COMPTON BACKSCATTERING IN RADIO PULSARS AND RADIO-LOUD ACTIVE GALACTIC NUCLEI
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INDUCED COMPTON BACKSCATTERING IN RADIO PULSARS AND RADIO-LOUD ACTIVE GALACTIC NUCLEI

机译:放射性脉冲和放射性大分子活性银河系引起的康普顿反散射

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摘要

We perform a quantitative numerical calculation of the steady-state radiation spectrum in a slab of cold electrons which is illuminated by unpolarized collimated, high brightness temperature radiation. The process of induced Compton backscattering can dramatically increase the intensity of radiation reflected from the slab over the level predicted by spontaneous scattering when the incident radiation spectrum has a spectral index α > 1 (where the flux density S_v ∝ v~α). In this case, the reflected spectrum has a spectral index α ≥ 1 up to a cutoff at the peak frequency (v_0) of the illuminating radiation spectrum. When the incident spectrum has a spectral index α < 1, the intensity of the reflected radiation is instead strongly reduced and a broad absorption-like feature appears in the reflected spectrum at v approx > v_0. In agreement with previous order of magnitude estimates, we find that induced Compton backscattering limits the brightness temperature at the peak of the transmitted flux density spectrum to (kT_b/m_ec~2)τ_T~2 θ~2 = 1.0, where θ is the opening angle of the beam and τ_T is the Thomson depth of the slab. The polarization of the backscattered flux can be exponentially magnified if the incident radiation has a small net polarization. Induced Compton backscattering also rapidly transfers momentum from the incident radiation beam to the scattering electrons and can significantly enhance the radiation pressure force on the illuminated side of the scattering plasma. Applying these results to a simple spherically symmetric model of a magnetized pulsar wind, we find that the pulsed emission from radio pulsars with P approx < 0.1 P_(-15)~(1/5) s should be obscured by stimulated backscattering. We argue that the electron density along the path of the radio emission must be substantially underdense relative to the predictions of the simplest wind model, perhaps as the result of a large induced radiation pressure force. Stimulated backscattering enhances the reflected flux density from the parsec scale material in the centers of radio-loud active galactic nuclei, and the flux from the reflection nebulae could be as much as a few percent of the total observed flux. The reflected flux density is characterized by S_v ∝ v and strong frequency-dependent polarization.
机译:我们对冷电子平板中的稳态辐射光谱进行定量数值计算,该平板由无偏振的准直高亮度温度辐射照射。当入射辐射光谱的光谱指数α> 1(其中通量密度S_v ∝ v〜α)时,诱导的康普顿反向散射过程可以大大增加板坯反射的辐射强度,使其超过自发散射所预测的水平。在这种情况下,反射光谱具有光谱指数α≥1,直到在照明辐射光谱的峰值频率(v_0)截止为止。当入射光谱的光谱指数α<1时,反射辐射的强度会大大降低,并且在反射光谱中,大约v> v_0处会出现宽的吸收状特征。与先前的数量级估计一致,我们发现感应康普顿反向散射将透射通量密度谱峰值处的亮度温度限制为(kT_b / m_ec〜2)τ_T〜2θ〜2 = 1.0,其中θ为开口光束的角度和τ_T是平板的Thomson深度。如果入射辐射的净极化较小,则后向散射通量的极化可以成倍放大。诱导的康普顿反向散射还将动量从入射辐射束迅速转移到散射电子,并且可以显着增强散射等离子体受照侧的辐射压力。将这些结果应用到磁化脉冲星风的简单球对称模型中,我们发现受激励的反向散射应掩盖P约<0.1 P _(-15)〜(1/5)s的射电脉冲星的脉冲发射。我们认为,相对于最简单的风模型的预测,沿无线电发射路径的电子密度必须实质上较低,这可能是由于较大的感应辐射压力造成的。受刺激的反向散射增强了在放射性大声活跃银河核中心的等距尺度材料的反射通量密度,而来自反射星云的通量可能高达观测到的总通量的百分之几。反射通量密度的特征在于S_v ∝ v和强的频率相关极化。

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