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Saturns dayside ultraviolet auroras: Evidence for morphological dependence on the direction of the upstream interplanetary magnetic field

机译:土星的日间紫外线极光:形态依赖上游行星际磁场方向的证据

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摘要

We examine a unique data set from seven Hubble Space Telescope (HST) “visits” that imaged Saturn's northern dayside ultraviolet emissions exhibiting usual circumpolar “auroral oval” morphologies, during which Cassini measured the interplanetary magnetic field (IMF) upstream of Saturn's bow shock over intervals of several hours. The auroras generally consist of a dawn arc extending toward noon centered near ∼15° colatitude, together with intermittent patchy forms at ∼10° colatitude and poleward thereof, located between noon and dusk. The dawn arc is a persistent feature, but exhibits variations in position, width, and intensity, which have no clear relationship with the concurrent IMF. However, the patchy postnoon auroras are found to relate to the (suitably lagged and averaged) IMF Bz, being present during all four visits with positive Bz and absent during all three visits with negative Bz. The most continuous such forms occur in the case of strongest positive Bz. These results suggest that the postnoon forms are associated with reconnection and open flux production at Saturn's magnetopause, related to the similarly interpreted bifurcated auroral arc structures previously observed in this local time sector in Cassini Ultraviolet Imaging Spectrograph data, whose details remain unresolved in these HST images. One of the intervals with negative IMF Bz however exhibits a prenoon patch of very high latitude emission extending poleward of the dawn arc to the magnetic/spin pole, suggestive of the occurrence of lobe reconnection. Overall, these data provide evidence of significant IMF dependence in the morphology of Saturn's dayside auroras.Key Points class="unordered" style="list-style-type:disc">We examine seven cases of joint HST Saturn auroral images and Cassini IMF dataThe persistent but variable dawn arc shows no obvious IMF dependencePatchy postnoon auroras are present for northward IMF but not for southward IMF class="kwd-title">Keywords: Auroral phenomena, Hubble Space Telescope, Saturn, Solar wind dependence class="head no_bottom_margin" id="__sec2title">1. IntroductionIt has long been supposed that the dynamics of the magnetospheres of the gas giant planets are dominated by the rotational flows imposed by ion-neutral collisions in the planetary ionosphere [e.g., ; ]. Nevertheless, this expectation does not exclude the possibility that the interaction with the solar wind at the magnetopause boundary produces significant effects involving the outer magnetosphere and magnetospheric tail [e.g., , ]. For the case of Saturn, the topic of the present paper, the estimates of the dayside reconnection rate based on empirical formulae derived from terrestrial experience, indicates typical voltages as low as ∼25 kV during low-field solar wind rarefaction regions, rising to ∼150 kV during high-field compression regions []. Such rates are thus near negligible in the former case, but competitive with ring current region and outer magnetosphere rotational voltages of a few hundred kilovolts each in the latter (the overall rotational voltage at Saturn however, including the inner magnetosphere, is ∼12 MV) []. These dayside reconnection rates nevertheless imply that the time scale governing the solar wind interaction via open flux production is long. To replenish the tail with a typical ∼30 GWb of open flux would take ∼14 days during solar wind rarefaction regions, reducing to ∼2.5 days during compression regions, such time scales being compatible with the rates at which Saturn's auroral oval is observed to increase in size []. Rapid reductions in open flux at Saturn are then found to be excited by strong impulsive compressions of the magnetosphere by the solar wind, resulting in major poleward expansions of the auroras, which are centered in the dawn sector due to the effect of rapid planetary rotation [; ; ; ]. Similar compression-induced closure events are also sometimes observed at Earth, then centered nearer to midnight [e.g., ].Recent work has emphasized however that beyond the simple scaling assumptions employed by for Saturn and ] for Jupiter, dayside reconnection may differ somewhat between the Earth and the gas giants due to the differing physical conditions occurring in the magnetopause regions on both sides of the boundary. In particular, consideration of the effect of flow shear across the boundary related to the interior planetary rotational flow suggests that reconnection may be favored in the dusk sector, where the flow shear is reduced rather than in the dawn sector where it is maximized [], while effects associated with the plasma pressure gradient across the boundary may often restrict the process to loci, where the magnetospheric and magnetosheath fields are quite closely antiparallel []. In addition, href="#b29" rid="b29" class=" bibr popnode">Lai et al. [2012] have confirmed using Cassini data that Earth-like, few minute, flux transfer events (FTEs) are absent at Saturn; these representing the signature of transient magnetopause reconnection events that make an important contribution to the overall open flux transport into the tail at Earth [e.g., href="#b35" rid="b35" class=" bibr popnode">Milan et al., 2000a]. Nevertheless, in addition to the circumstantial evidence for the occurrence of dayside reconnection noted above concerning variations in the size of Saturn's auroral oval, the signatures of reconnection-related plasma heating and magnetic flux connection across the boundary have been reported in Cassini data by href="#b33" rid="b33" class=" bibr popnode">McAndrews et al. [2008] and href="#b5" rid="b5" class=" bibr popnode">Badman et al. [2013], while the presence of magnetosheath plasma in the dayside cusp exhibiting plasma injection signatures has been reported by href="#b44" rid="b44" class=" bibr popnode">Radioti et al. [2013].In addition to these indicators, href="#b43" rid="b43" class=" bibr popnode">Radioti et al. [2011] have presented evidence in Cassini Ultraviolet Imaging Spectrograph (UVIS) data for reconnection-related auroral features in Saturn's dayside ultraviolet (UV) auroras, taking the form of sequential extended bifurcations in the auroral oval in the noon to dusk sector. We noted above that the dusk sector is favored for reconnection at Saturn due to the reduced flow shear across the boundary, between subcorotating magnetospheric plasma on the inside and antisunward flowing magnetosheath plasma on the outside. The auroral bifurcations are found to recur on ∼1–2 h time scales and endure as discrete features for comparable or longer intervals, so that more than one such feature is often present simultaneously, moving slowly poleward and eastward at ∼15% of rigid corotation [href="#b44" rid="b44" class=" bibr popnode">Radioti et al., 2013]. In the events studied by href="#b43" rid="b43" class=" bibr popnode">Radioti et al. [2011], the largest “arcs” were found to contain ∼2 GWb of magnetic flux, corresponding to ∼10% of the preexisting flux lying poleward of the auroral oval, with the oval boundary at other local times expanding equatorward accordingly as the arcs moved poleward. An overall increase in open flux of ∼6 GWb over a ∼4 h interval (see their Figure href="/pmc/articles/PMC4497471/figure/fig04/" target="figure" class="fig-table-link figpopup" rid-figpopup="fig04" rid-ob="ob-fig04" co-legend-rid="lgnd_fig04">4c) corresponds to a substantial averaged dayside reconnection rate of ∼400 kV in this case, rather larger than the typical values estimated by href="#b24" rid="b24" class=" bibr popnode">Jackman et al. [2004] noted above. Similar auroral structures have also been reported by href="#b4" rid="b4" class=" bibr popnode">Badman et al. [2012] in infrared emissions observed by the Cassini visual and infrared mapping spectrometer (VIMS), but in this case centered nearer to noon.href="/pmc/articles/PMC4497471/figure/fig04/" target="figure" rid-figpopup="fig04" rid-ob="ob-fig04">target="object" href="/pmc/articles/PMC4497471/figure/fig04/?report=objectonly">Open in a separate windowclass="figpopup" href="/pmc/articles/PMC4497471/figure/fig04/" target="figure" rid-figpopup="fig04" rid-ob="ob-fig04">Figure 4Set of projected HST images of Saturn's northern UV aurora from (a) the 2011 campaign (visits H1–H3) and (b) the 2012 campaign (visits I5–I8), during which Cassini was located in the solar wind upstream of Saturn's bow shock over intervals of at least several hours. The top rows of Figures 4a and 4b correspond to the five coadded F125LP filtered images at the start of each visit, while the bottom rows similarly correspond to the five coadded F125LP filtered images at the end of each visit. These are termed the “A” and “B” images, respectively, as marked in the figure. HST visit identifiers are given above each image, together with the date (year-month-day) and UT center time (h:min:s). Beneath this are shown the mean and SD values of the three KSM components of the IMF determined from the lagged 2.5 h intervals of Cassini data associated with the center time of each individual image, together with the corresponding mean and SD values of the IMF clock angle. The images are projected onto a polar grid assuming an auroral height of 1100 km above the 1 bar reference spheroid, the grid being shown by white dotted latitude circles at 10° intervals and white dotted longitude lines at 30° intervals (2 h LT), with noon shown at the bottom and dawn to the left. The images have been truncated somewhat past the dawn-dusk meridian to avoid pixels becoming overstretched on approaching the planetary limb. The same color-coded intensity scale, shown upper right, is employed for all images, saturated red at 40 kR.
机译:我们检查了来自七个哈勃太空望远镜(HST)“访问”的独特数据集,这些数据拍摄了土星在北部白天发出的紫外线,这些紫外线表现出通常的圆极“极光椭圆”形态,在此期间,卡西尼测量了土星向船首弓撞击上方的行星际磁场(IMF)。间隔几个小时。极光通常由朝中午延伸至约15°折中度的黎明弧以及位于中午和黄昏之间的约10°折度中的间歇性斑块形式组成。曙光弧是一个持久特征,但位置,宽度和强度都有变化,与并发IMF没有明显关系。但是,发现零星的下午极光与(适当滞后和平均)IMF Bz有关,在所有四次访问中均以正Bz出现,而在所有三次访问中均以Bz负值出现。这种最连续的形式出现在最强的正Bz情况下。这些结果表明,下午的形式与土星的磁更年期的重新连接和开通通量的产生有关,这与以前在卡西尼紫外成像光谱数据中在该时域观察到的类似解释的分叉极光弧结构有关,这些细节在这些HST图像中尚未得到解决。 。但是,具有负IMF Bz的区间之一表现出一个非常高的纬度发射的午前补丁,将黎明弧的极点延伸到磁极/自旋极,暗示了波瓣重新连接的发生。总体而言,这些数据提供了IMF对土星白天极光形态的显着依赖性的证据。要点 class =“ unordered” style =“ list-style-type:disc”> <!-list-behavior = unordered prefix- word = mark-type = disc max-label-size = 0-> 我们研究了7例联合HST土星极光图像和卡西尼IMF数据 持续但变化多端的黎明弧显示不明显IMF依赖 北向IMF出现零星的下午极光,但南向IMF不存在 class =“ kwd-title”>关键字:极光现象,哈勃太空望远镜,土星,太阳风依赖性 class =“ head no_bottom_margin” id =“ __ sec2title”> 1。引言长期以来,人们一直认为气体巨行星的磁层动力学是由行星电离层中离子中性碰撞所施加的旋转流所决定的。 ]。不过,这种期望并不排除与在磁层顶边界处的太阳风的相互作用产生涉及外磁层和磁层尾部的重大影响的可能性[例如,]。以土星为例,本文的主题是根据从地面经验得出的经验公式估算的日间重新连接率,它表明低场太阳风稀疏区的典型电压低至约25 kV,上升至在高场压缩区域为150 kV []。因此,在前一种情况下,这种速率几乎可以忽略不计,但与后者的环形电流区域和外层电磁层的旋转电压各有几百千伏(但是,包括内层磁层在内的土星的总旋转电压约为12 MV)相抗衡。 []。但是,这些日间重新连接速率暗示着通过开放通量生产来控制太阳风相互作用的时间范围很长。为尾巴补充典型的约30μgbb的开放通量,在太阳风稀疏区需要约14μs天,而在压缩区则要减少至约2.5μs天,这种时间尺度与观测到的土星极光椭圆率增加的速率兼容在尺寸方面 []。后来发现,土星的开放通量的快速减少是由太阳风对磁层的强烈脉冲压缩而激发的,从而导致极光的主要向极膨胀,由于快速的行星自转效应,其中心在黎明区[ ; ; ; ]。有时在地球上也观察到类似的由压缩引起的闭合事件,然后以接近午夜的时间为中心[例如]。但是最近的工作强调,除了土星和木星使用的简单比例假设外,白天的重新连接可能会有所不同。由于在边界两侧的磁层顶区中存在不同的物理条件,因此地球和气体巨人。尤其是,考虑到与内部行星旋转流有关的跨边界流动剪切的影响,表明在黄昏区域,流动剪切减小,而不是在黎明区域,重新连接可能更有利于重新连接[],而与跨边界血浆压力梯度相关的影响通常可能会将过程限制在基因座上,其中磁层和磁石场非常反平行[]。此外,href="#b29" rid="b29" class=" bibr popnode"> Lai等。 [2012 ]已使用卡西尼号数据确认,土星不存在类似于地球的几分钟的磁通量传递事件(FTE);这些代表瞬变的更年期重新连接事件的特征,这些事件对整个开放通量传输到地球尾巴中做出了重要贡献[例如,href="#b35" rid="b35" class=" bibr popnode">米兰等等,2000a ]。然而,除了上面提到的与土星极光椭圆大小变化有关的日间重新连接发生的间接证据外,卡西尼数据还报道了与重新连接有关的等离子体加热和跨边界磁通量连接的特征,href =“#b33” rid =“ b33” class =“ bibr popnode”> McAndrews等。 [2008] 和href="#b5" rid="b5" class=" bibr popnode"> Badman等。 [2013] ,而href="#b44" rid="b44" class=" bibr popnode"> Radioti等人已经报道了在日间尖端出现的磁石浆等离子体具有等离子体注入特征。 [2013] 。除了这些指标外,href="#b43" rid="b43" class=" bibr popnode"> Radioti等。 [2011 ]在卡西尼紫外线成像光谱(UVIS)数据中提供了土星白天紫外线(UV)极光中与重连接相关的极光特征的证据,采取的是中午至黄昏时在极光椭圆中依次扩展的分叉形式部门。我们在上面指出,由于内部边界下的同心层磁层等离子体与外部层的逆日流动的磁石浆等离子体之间的边界流切变减小,因此黄昏区在土星处被重新连接更为有利。发现极光分叉在大约1-2h的时间尺度上重复出现,并以可分离或可比较的间隔出现为离散特征,因此经常同时存在多个这样的特征,在刚性同向旋转的约15%时向极和向东缓慢移动[href="#b44" rid="b44" class=" bibr popnode"> Radioti等人,2013 ]。在href="#b43" rid="b43" class=" bibr popnode"> Radioti等人研究的事件中。 [2011 ]中,最大的“弧”被发现含有约2 GWb的磁通量,相当于先前存在的通量的10%位于极光椭圆的极向,而在其他当地时间的椭圆边界向赤道方向扩展因此,随着电弧向极点移动。在大约4 h的时间内,大约6 GWb的开放通量整体增加(请参见其图href =“ / pmc / articles / PMC4497471 / figure / fig04 /” target =“ figure” class =“ fig-table-link在这种情况下,figpopup“ rid-figpopup =” fig04“ rid-ob =” ob-fig04“ co-legend-rid =” lgnd_fig04“> 4 c)对应于约400 kV的实质平均日间重新连接率,但大于href="#b24" rid="b24" class=" bibr popnode"> Jackman等人估算的典型值。上面提到的[2004 ]。 href="#b4" rid="b4" class=" bibr popnode"> Badman等人也报告了类似的极光结构。 [2012 ]由卡西尼号视觉和红外映射光谱仪(VIMS)观测到的红外辐射,但在这种情况下,中心位置接近中午。<!-fig ft0-> <!-fig mode = art f1 -> href="/pmc/articles/PMC4497471/figure/fig04/" target="figure" rid-figpopup="fig04" rid-ob="ob-fig04"> <!-fig / graphic | fig / alternatives / graphic mode =“ anchored” m1-> target="object" href="/pmc/articles/PMC4497471/figure/fig04/?report=objectonly">在单独的窗口中打开 class="figpopup" href="/pmc/articles/PMC4497471/figure/fig04/" target="figure" rid-figpopup="fig04" rid-ob="ob-fig04">图4 <!-标题a7->(a)2011年运动(访问H1-H3)和(b)2012年运动(访问I5-I8)的土星北部紫外线极光的HST投影图像集,在此期间,卡西尼号至少在几个小时的间隔内位于土星船首冲击的太阳风中。图4a和4b的顶行对应于每次访问开始时的五个共存的F125LP滤波图像,而底行类似地对应于每次访问结束时的五个共存的F125LP滤波图像。如图所示,这些分别称为“ A”和“ B”图像。在每张图片上方都提供了HST访问标识符,以及日期(年-月-日)和UT中心时间(h:min:s)。在此之下显示了IMF的三个KSM分量的平均值和SD值,该值是由卡西尼数据的滞后2.5 h间隔确定的,该间隔与每个单个图像的中心时间相关联,以及IMF时钟角度的相应平均值和SD值。图像投影到极坐标栅格上,假设极高高度在1 bar参考椭球上方1100 km,栅格由以10°间隔的白色虚线纬度圆和以30°间隔的白色虚线经度线(LT 2 h)显示,底部显示中午,左侧显示黎明。为了避免像素在接近行星肢体时过度拉伸,图像已在黎明黄昏子午线后被截断了一些。所有图像均使用相同的颜色编码强度标尺,如右上方所示,在40 kR处饱和红色。

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