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EMISSION PATTERNS OF SOLAR TYPE III RADIO BURSTS: STEREOSCOPIC OBSERVATIONS

机译:太阳第三类无线电爆炸的发射模式:立体观测

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Simultaneous observations of solar type III radio bursts obtained by the STEREO A, B, and WIND spacecraft at low frequencies from different vantage points in the ecliptic plane are used to determine their directivity. The heliolongitudes of the sources of these bursts, estimated at different frequencies by assuming that they are located on the Parker spiral magnetic field lines emerging from the associated active regions into the spherically symmetric solar atmosphere, and the heliolongitudes of the spacecraft are used to estimate the viewing angle, which is the angle between the direction of the magnetic field at the source and the line connecting the source to the spacecraft. The normalized peak intensities at each spacecraft Rj = Ij /ΣIj (the subscript j corresponds to the spacecraft STEREO A, B, and WIND), which are defined as the directivity factors are determined using the time profiles of the type III bursts. It is shown that the distribution of the viewing angles divides the type III bursts into: (1) bursts emitting into a very narrow cone centered around the tangent to the magnetic field with angular width of ~2° and (2) bursts emitting into a wider cone with angular width spanning from ~ – 100° to ~100°. The plots of the directivity factors versus the viewing angles of the sources from all three spacecraft indicate that the type III emissions are very intense along the tangent to the spiral magnetic field lines at the source, and steadily fall as the viewing angles increase to higher values. The comparison of these emission patterns with the computed distributions of the ray trajectories indicate that the intense bursts visible in a narrow range of angles around the magnetic field directions probably are emitted in the fundamental mode, whereas the relatively weaker bursts visible to a wide range of angles are probably emitted in the harmonic mode.
机译:由STEREO A,B和WIND航天器以低频率从黄道面的不同有利位置获得的太阳III型无线电脉冲的同步观测用于确定其指向性。假定这些脉冲源位于相关活动区域进入球形对称太阳大气的Parker螺旋磁场线上,并在不同频率下估算它们的日经度,并用航天器的日经度来估算视角,即源处的磁场方向与将源连接到航天器的线之间的角度。每个航天器的归一化峰强度Rj = Ij /ΣIj(下标j对应于航天器STEREO A,B和WIND),定义为方向性因子是使用III类爆发的时间曲线确定的。结果表明,视角的分布将III型猝发分为:(1)猝发成一个非常狭窄的圆锥体,围绕着与磁场成2°角宽度的切线,以及(2)猝发发出了一个角锥。锥角范围从〜– 100°到〜100°的较宽圆锥体。所有三个航天器的方向性因子与源的视角的关系图表明,III型发射沿源处螺旋磁场线的切线非常强烈,并且随着视角增加到更高的值而稳定下降。这些发射模式与计算得出的射线轨迹分布的比较表明,在磁场方向周围窄角度范围内可见的强烈脉冲很可能以基本模式发射,而在宽范围内可见的相对较弱的脉冲却以基本模式发射。谐波模式下可能会发射角度。

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