论文标题
无线电PULSAR PSR B1451-68中的圆极化:相干模式转变和内部干扰
Circular polarization in radio pulsar PSR B1451-68: coherent mode transitions and intrabeam interference
论文作者
论文摘要
脉冲星B1451-68的无线电发射包含两个相似强度的极化模式,它们产生了两个明确的正交偏振角轨道。当在繁殖球体上观察时,发射由两个通量贴片组成,它们将作为脉冲经度的函数旋转并穿过Stokes V杆,从而导致正交极化模式(OPMS)之间的过渡。此外,在配置文件窗口内,贴片中的功率比率一次。结果表明,子午循环化是由固定四分之一波相滞后的变化模式比产生的相干OPM转变(COMT)引起的。在无线电脉冲星数据中,COMT可能无处不在且难以检测,因为它们在极化部分中不留下痕迹,并且它们的描述是通过与旋转矢量模型相似的方程式描述的。圆形化与较低频率的通量最小值相吻合,要求该轮廓成分是由辐射形成的,其振荡阶段与每个组件90度的经度增加。这些特性可以理解为涉及两对线性正交模式(或两个非正交椭圆形波)的干扰模式。共面振荡的频率依赖性相干叠加可以在脉冲曲线中产生最小值,从而将组件作为单独实体的幻觉。这种负干扰后留下的正交极化信号解释了极化程度的增强,这在剖面成分之间的最小值中通常观察到了极化度。
The radio emission of pulsar B1451-68 contains two polarization modes of similar strength, which produce two clear orthogonal polarization angle tracks. When viewed on a Poincare sphere, the emission is composed of two flux patches that rotate meridionally as function of pulse longitude and pass through the Stokes V poles, which results in transitions between orthogonal polarization modes (OPMs). Moreover, the ratio of power in the patches is inversed once within the profile window. It is shown that the meridional circularization is caused by a coherent OPM transition (COMT) produced by a varying mode ratio at a fixed quarter-wave phase lag. The COMTs may be ubiquitous and difficult to detect in radio pulsar data, because they can leave no trace in polarized fractions and they are described by equation similar to the rotating vector model. The circularization, which coincides with flux minima at lower frequency, requires that profile components are formed by radiation with an oscillation phase which increases with longitude in steps of 90 degrees per component. The properties can be understood as an interference pattern involving two pairs of linear orthogonal modes (or two nonorthogonal elliptic waves). The frequency-dependent coherent superposition of coplanar oscillations can produce the minima in the pulse profile, and thereby the illusion of components as separate entities. The orthogonally polarized signal which is left after such negative interference explains the enhancement of polarization degree which is commonly observed in the minima between profile components.