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首页> 外文期刊>Journal of Geophysical Research, A. Space Physics: JGR >Dayside auroral emissions controlled by IMF: A survey for dayside auroral excitation at 557.7 and 630.0 nm in Ny-Alesund, Svalbard
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Dayside auroral emissions controlled by IMF: A survey for dayside auroral excitation at 557.7 and 630.0 nm in Ny-Alesund, Svalbard

机译:由IMF控制的日间极光发射:斯瓦尔巴特群岛Ny-Alesund在557.7和630.0 nm处的日间极光激发调查

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摘要

A survey of dayside 557.7 and 630.0 nm auroral emission, acquired from the all-sky imagers at the Yellow River Station in Ny-Alesund, Svalbard, shows that the dayside auroral oval could be divided into five auroral active regions: the dawnside (Da, 06:00-07:30 MLT) and duskside (Du, 15:30-17:00 MLT) green aurora sectors, the prenoon (W, 07:30-10:00 MLT) and postnoon (H, 13:00-15:30 MLT) peaks for 557.7 and 630.0 nm auroral emissions, and the midday gap (M, 10:00-13:00 MLT) for green aurora. The 630.0 nm intensities in W, M, and H nearly increase linearly with the Kan-Lee electric field. The 630.0 nm auroral emissions in W and H show a double-peak feature associated with the change of interplanetary magnetic field (IMF) clock angle: one peak at 90° and the other at 270°. The 630.0 nm emission in M, however, is dominantly excited during the clock angle of 90°-270°. It is considered that the 630.0 nm emissions in W/H and M are related to the prenoon/postnoon antiparallel reconnection at the high-latitude magnetopause and the subsolar component reconnection, respectively. Moreover, the 630.0 nm intensity in the dayside oval shows the monotonic increase with the absolute value of the north-south oriented electric field (Ez), but the increasing rate of the intensity in the postnoon (prenoon) oval is larger than that in the prenoon (postnoon) oval when IMF By is negative (positive). Only the 557.7 nm intensity in region M and H/Du increases gradually with the absolute value of negative Ez. These features should be associated with the change of interhemispheric currents produced by Ez.
机译:从斯瓦尔巴特群岛Ny-Alesund的黄河站的全天空成像仪获得的白天557.7和630.0 nm极光发射的调查显示,白天极光椭圆可以分为五个极光活动区域:黎明面(Da, 06:00-07:30 MLT)和黄昏(Du,15:30-17:00 MLT)绿色极光区,下午(W,07:30-10:00 MLT)和下午(H,13:00- 15:30 MLT)达到557.7和630.0 nm极光发射的峰值,绿色极光的午间间隙(M,10:00-13:00 MLT)。 W,M和H的630.0 nm强度几乎随Kan-Lee电场线性增加。 W和H中630.0 nm的极光发射具有双峰特征,这与行星际磁场(IMF)时钟角的变化有关:一个峰值为90°,另一个峰值为270°。然而,在90°-270°的时钟角期间,M的630.0 nm发射主要被激发。可以认为,W / H和M中的630.0 nm发射分别与高纬度停磁和太阳下分量重新连接时的午/后反平行重新连接有关。此外,日椭圆形的630.0 nm强度显示出随着南北向电场(Ez)的绝对值单调增加,但午后(早午)椭圆形的强度增加率大于平时。 IMF By为负(正)时的午前(下午)椭圆形。 M和H / Du区域中只有557.7 nm的强度随着负Ez的绝对值逐渐增加。这些特征应与Ez产生的半球电流变化有关。

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