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Complex Ionospheric Irregularity Echoes Observed by Low Latitude Long Range Ionospheric Radar 低纬度远程电离层雷达观测的复杂电离层不规则回波
IF 2.9 2区 地球科学 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-12 DOI: 10.1029/2025JA034381
Yuxiao Li, Lianhuan Hu, Guozhu Li, Baiqi Ning, Guofeng Dai, Wenjie Sun, Haiyong Xie, Xiukuan Zhao, Yi Li, Jianfei Liu, Prayitno Abadi, Prasert Kenpankho, Bo Xiong

Using the Low lAtitude long Range Ionospheric raDar (LARID) at Dongfang (19.2°N, 108.8°E), Hainan Island, China, we report a unique case of complex ionospheric irregularities observed on 9 June 2024. The most interesting aspect is the first-time long-range (∼2,000 km) detection of daytime ionospheric irregularities and post-sunset band-like irregularity structures by HF radar at low latitudes. By incorporating VHF radar and global navigation satellite system (GNSS) rate of total electron content index (ROTI) observations, the radio wave propagation modes of the ionospheric irregularity events observed by LARID and evolution of these ionospheric irregularities were analyzed. The daytime ionospheric irregularity echoes observed by LARID over the Indian Ocean exhibited westward drift, evident in both echo patterns and Doppler velocities. These ionospheric echoes were likely backscattered from E region field aligned irregularities by the “downleg” of the 1-hop HF ray path. The post-sunset irregularity echoes observed by LARID over Indian Ocean manifested as a band-like structure. This structure was closely attached to the bottom of ground/sea scatter echoes and showed the same range variation as the ground/sea scatters. GNSS ROTI observation revealed that irregularities primarily appeared south of the magnetic equator and drifted eastward across the eastern longitudes in later hours. Analysis indicates that the displacement of small-scale irregularities within the equatorial plasma bubble event along the magnetic field likely contributed to the band-like irregularity structure observed by LARID and the asymmetric irregularity distribution observed by GNSS.

利用位于海南岛东方站(19.2°N, 108.8°E)的低纬远程电离层雷达(LARID),报告了2024年6月9日观测到的一次复杂电离层异常现象。最有趣的方面是首次在低纬度地区用高频雷达远距离(~ 2000公里)探测到白天电离层不规则和日落后带状不规则结构。结合VHF雷达和全球导航卫星系统(GNSS)总电子含量指数(ROTI)观测数据,分析了LARID观测到的电离层不规则事件的无线电波传播模式和这些电离层不规则事件的演变。LARID在印度洋上空观测到的白天电离层不规则回波在回波模式和多普勒速度上都表现出向西漂移。这些电离层回波很可能是由1跳HF射线路径的“下行”从E区场排列不规则中反向散射而来。LARID在印度洋观测到的日落后不规则回波表现为带状结构。该结构与地/海散射回波的底部紧密相连,并表现出与地/海散射回波相同的距离变化。GNSS ROTI观测显示,不规则现象主要出现在地磁赤道以南,并在随后的几个小时内向东漂移,穿过东经。分析表明,赤道等离子体气泡事件内部的小尺度不规则性沿磁场方向的位移可能导致了LARID观测到的带状不规则结构和GNSS观测到的不对称不规则分布。
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引用次数: 0
Statistical Auroral Absorption Model Parameterized by AE Index 用声发射指数参数化的统计极光吸收模型
IF 2.9 2区 地球科学 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-12 DOI: 10.1029/2025JA034648
R. A. D. Fiori, T. G. Cameron, J. Issa, A. Hupé, L. Huang

Energetic electron precipitation, often in association with enhanced geomagnetic activity, leads to increased D-region ionization in the auroral region causing auroral absorption. A statistical auroral absorption model is presented for high-latitudes (poleward of 50° magnetic latitude) based on data collected from 2010 to 2019 from 13 wide-beam riometers at 30 MHz spanning 53.9°–86.9° magnetic latitude. Hourly maximum absorption values were sorted into bins of 5° magnetic latitude and 1 hr of magnetic local time and parameterized based on the hourly maximum global AE index for 0–100 nT, 100–200 nT, 200–300 nT, 300–400 nT, 400–500 nT, 500–600 nT, 600–800 nT, 800–1,000 nT, and ≥1,000 nT. The model uses spherical cap harmonic analysis with a maximum degree index and order of 12 and 10, respectively. Absorption is characterized by a dawnside enhancement that peaks in the pre-noon sector and spreads toward the midnight sector with increasing geomagnetic activity. The maximum equatorward and poleward extents of absorption >0.5 dB expand at a rate of 1.4°/100 nT and 0.4°/100 nT, respectively. According to this model, >0.5 dB absorption is expected in >10% of the high-latitude region for AE > 500 nT (occurs 23.6% of times), and 40% of the high-latitude region for AE ≥ 1,000 nT (occurs 3.2% of times). The statistical auroral absorption model may be used as a background model as a constraint for modeling instantaneous auroral absorption.

高能电子沉淀,通常与增强的地磁活动相关联,导致极光区d区电离增加,导致极光吸收。基于2010年至2019年在53.9°-86.9°磁纬范围内采集的13个30 MHz宽波束riometer数据,提出了高纬度地区(磁纬50°极向)的统计极光吸收模型。将每小时最大吸收值分为5°磁纬和1小时磁地方时的桶,并根据0-100 nT、100-200 nT、200-300 nT、300-400 nT、400-500 nT、500-600 nT、600-800 nT、800-1,000 nT和≥1,000 nT的每小时最大全球声发射指数进行参数化。模型采用球帽谐波分析,最大度指数为12,阶数为10。吸收的特征是黎明边的增强,在午前部分达到峰值,并随着地磁活动的增加向午夜部分扩散。0.5 dB的最大赤道和极向吸收范围分别以1.4°/100 nT和0.4°/100 nT的速率扩展。根据该模型,对于AE >; 500 nT,高纬度地区>;10%的高纬度地区预计吸收>;0.5 dB(发生的次数为23.6%),对于AE≥1000 nT,高纬度地区40%的高纬度地区预计吸收>;0.5 dB(发生的次数为3.2%)。统计极光吸收模型可用作背景模型,作为模拟瞬时极光吸收的约束。
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引用次数: 0
Global MHD Simulations: Magnetosphere–Ionosphere Coupling Dependence on Conductance Model 全球MHD模拟:磁层-电离层耦合对电导模型的依赖
IF 2.9 2区 地球科学 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-11 DOI: 10.1029/2025JA034675
T. I. Pulkkinen, P. Dredger, M. Liemohn, A. Ridley, G. Tóth, D. Welling, Q. Al Shidi, A. Brenner, S. Hill, A. Mukhopadhyay

Eighty-five geomagnetic storms were simulated with the space weather modeling framework Geospace model using two different ionospheric conductance models. One set used the legacy conductances within the Ridley ionosphere model, while the other set used the newly developed conductance model for extreme events conductance model. As input and other model setup parameters were identical, we use this unique simulation suite to assess the impacts of ionospheric conductance on the ionospheric and magnetotail states during magnetic storms. The results show that higher conductance somewhat improves predictions of ground magnetic disturbances, as measured by the AL index. The cross-polar cap potential was lower for higher ionospheric conductance. In the magnetotail, higher ionospheric conductivity led to slightly lower ring current intensity and weakened Earthward flows, while the tail current magnitude was relatively insensitive to the conductance model. These results are an important step in understanding how the ionosphere impacts the magnetospheric state and the magnetosphere–ionosphere coupling.

利用空间气象模拟框架Geospace模型,采用两种电离层电导模式对85个地磁风暴进行了模拟。一组使用传统的Ridley电离层模型中的电导,另一组使用新开发的极端事件电导模型。由于输入和其他模型设置参数相同,我们使用这个独特的模拟套件来评估磁暴期间电离层电导对电离层和磁尾状态的影响。结果表明,较高的电导在一定程度上改善了对地磁扰动的预测,这是由AL指数测量的。电离层电导越高,极间电帽电位越低。在磁尾中,电离层电导率较高导致环电流强度略低,向地流动减弱,而尾电流大小对电导模型相对不敏感。这些结果是理解电离层如何影响磁层状态和磁层-电离层耦合的重要一步。
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引用次数: 0
Self-Organized Hexagon-Shaped Jets in Rotating Fluid Experiments 旋转流体实验中的自组织六边形射流
IF 2.9 2区 地球科学 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-11 DOI: 10.1029/2025JA034520
S. Espa, G. Lacorata

Self-organization of planetary turbulence in persistent and geometrically well-defined flow features, has been attracting, recently, great scientific interest, thanks also to the spectacular images of Saturn's hexagon provided by the Voyager and Cassini missions. These flow patterns can be replicated in laboratory experiments with shallow rotating fluids, provided some characteristic non-dimensional parameters are suitably set up. In particular, we consider here prograde and retrograde (with respect to the rotation of the tank) hexagonal-shaped jets. Both Eulerian and Lagrangian data, directly reconstructed from the experiments, were analyzed and discussed. Our results are consistent with the conjecture that barotropic instability plays a key role in the genesis and maintenance of the hexagonal shape. We also show that the cross-analysis of experimental results and kinematic simulations on a simplified six-node meandering jet model allows, in principle, to formulate a scenario about the Lagrangian dispersion properties of the hexagon on Saturn in relation to its spatial and temporal characteristic scales.

最近,由于旅行者号和卡西尼号提供的土星六边形的壮观图像,行星湍流在持续和几何上定义明确的流动特征中的自组织吸引了极大的科学兴趣。只要适当设置一些特征的无量纲参数,这些流动模式可以在浅旋转流体的实验室实验中复制。特别地,我们在这里考虑顺行和逆行(相对于坦克的旋转)六边形射流。对直接从实验中重建的欧拉和拉格朗日数据进行了分析和讨论。我们的结果与正压不稳定性在六边形的形成和维持中起关键作用的猜想是一致的。我们还表明,对简化的六节点弯曲射流模型的实验结果和运动学模拟进行交叉分析,原则上可以建立土星上六边形的拉格朗日色散特性与其时空特征尺度的关系。
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引用次数: 0
Whistler Critical Mach Number Concept Revisited 惠斯勒临界马赫数概念重新审视
IF 2.9 2区 地球科学 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-11 DOI: 10.1029/2025JA034905
Michael A. Balikhin, Oleksiy V. Agapitov, Vladimir Krasnoselskikh, Vadim Roytershteyn, Simon N. Walker, Michael Gedalin, Immanuel Christopher Jebaraj, Lucas Colomban
<p>The formation of a collisionless shock is the result of a balance between nonlinear steepening and processes that counteract this steepening. Dispersive shocks are shocks in which dispersive processes counterbalance the front steepening and are formed when the dispersive spatial scale exceeds scales associated with resistive processes. Oblique dispersive shocks are characterized by a phase standing wave precursor adjacent to the magnetic ramp. The whistler critical Mach number <span></span><math> <semantics> <mrow> <msub> <mi>M</mi> <mi>CrW</mi> </msub> </mrow> <annotation> ${M}_{mathit{CrW}}$</annotation> </semantics></math> is defined as the maximum Mach number for which a linear whistler wave can phase stand upstream of the shock front. It was widely accepted that if the Mach number <span></span><math> <semantics> <mrow> <mi>M</mi> </mrow> <annotation> $M$</annotation> </semantics></math> exceeds <span></span><math> <semantics> <mrow> <msub> <mi>M</mi> <mi>CrW</mi> </msub> </mrow> <annotation> ${M}_{mathit{CrW}}$</annotation> </semantics></math>, linear whistler waves propagating along the shock normal are not able to “phase stand” in the upstream flow, and “…the shock will be initiated by a monotonic ramp.” (Kennel et al., 1985, https://doi.org/10.1029/gm034p0001). In this study, we present results of numerical simulations and observations of shocks with <span></span><math> <semantics> <mrow> <mi>M</mi> <mo>></mo> <msub> <mi>M</mi> <mi>CrW</mi> </msub> </mrow> <annotation> $M > {M}_{mathit{CrW}}$</annotation> </semantics></math> that reveal the occurrence of an alternative scenario. For both the shock resulting from kinetic particle-in-cell simulations and that observed by MMS, the propagation direction of the precursor deviates from the shock normal direction. As a result, the velocity of the surface of constant phase along the shock normal exceeds the phase speed of these waves. It is shown that the propagation of the surface of constant phase along the shock normal occurs at a velocity that is nearly equal to the shock speed. Hence, these waves are “phase standing along the shock normal” in spite of <span></span><math> <semantics> <mrow> <mi>M</mi> <mo>></mo> <msub>
无碰撞冲击的形成是非线性陡坡和抵消这种陡坡的过程之间平衡的结果。色散冲击是指色散过程抵消锋面陡坡的冲击,当色散空间尺度超过与阻力过程相关的尺度时形成的冲击。斜色散冲击的特征是在磁斜坡附近有一个相位驻波前体。啸声临界马赫数M CrW ${M}_{mathit{CrW}}$定义为线性啸声波相位位于激波前缘上游的最大马赫数。人们普遍认为,当马赫数M$ M$超过M CrW ${M}_{mathit{CrW}}$时,沿激波法线传播的线性哨声波在上游流动中不能“相驻”;而且“震动将由单调的斜坡引起。”(Kennel et al., 1985, https://doi.org/10.1029/gm034p0001)。在这项研究中,我们提出了M >; M CrW $M > {M}_{mathit{CrW}}$的数值模拟和观测结果,揭示了另一种情况的发生。对于胞内粒子动力学模拟和MMS观察到的激波,前驱体的传播方向都偏离激波法向。因此,沿激波法向的恒相表面速度超过了这些波的相速。结果表明,恒相表面沿激波法向的传播速度几乎等于激波速度。因此,尽管M >; M CrW $M > {M}_{mathit{CrW}}$,这些波是“沿激波法线相立的”。
{"title":"Whistler Critical Mach Number Concept Revisited","authors":"Michael A. Balikhin,&nbsp;Oleksiy V. Agapitov,&nbsp;Vladimir Krasnoselskikh,&nbsp;Vadim Roytershteyn,&nbsp;Simon N. Walker,&nbsp;Michael Gedalin,&nbsp;Immanuel Christopher Jebaraj,&nbsp;Lucas Colomban","doi":"10.1029/2025JA034905","DOIUrl":"https://doi.org/10.1029/2025JA034905","url":null,"abstract":"&lt;p&gt;The formation of a collisionless shock is the result of a balance between nonlinear steepening and processes that counteract this steepening. Dispersive shocks are shocks in which dispersive processes counterbalance the front steepening and are formed when the dispersive spatial scale exceeds scales associated with resistive processes. Oblique dispersive shocks are characterized by a phase standing wave precursor adjacent to the magnetic ramp. The whistler critical Mach number &lt;span&gt;&lt;/span&gt;&lt;math&gt;\u0000 &lt;semantics&gt;\u0000 &lt;mrow&gt;\u0000 &lt;msub&gt;\u0000 &lt;mi&gt;M&lt;/mi&gt;\u0000 &lt;mi&gt;CrW&lt;/mi&gt;\u0000 &lt;/msub&gt;\u0000 &lt;/mrow&gt;\u0000 &lt;annotation&gt; ${M}_{mathit{CrW}}$&lt;/annotation&gt;\u0000 &lt;/semantics&gt;&lt;/math&gt; is defined as the maximum Mach number for which a linear whistler wave can phase stand upstream of the shock front. It was widely accepted that if the Mach number &lt;span&gt;&lt;/span&gt;&lt;math&gt;\u0000 &lt;semantics&gt;\u0000 &lt;mrow&gt;\u0000 &lt;mi&gt;M&lt;/mi&gt;\u0000 &lt;/mrow&gt;\u0000 &lt;annotation&gt; $M$&lt;/annotation&gt;\u0000 &lt;/semantics&gt;&lt;/math&gt; exceeds &lt;span&gt;&lt;/span&gt;&lt;math&gt;\u0000 &lt;semantics&gt;\u0000 &lt;mrow&gt;\u0000 &lt;msub&gt;\u0000 &lt;mi&gt;M&lt;/mi&gt;\u0000 &lt;mi&gt;CrW&lt;/mi&gt;\u0000 &lt;/msub&gt;\u0000 &lt;/mrow&gt;\u0000 &lt;annotation&gt; ${M}_{mathit{CrW}}$&lt;/annotation&gt;\u0000 &lt;/semantics&gt;&lt;/math&gt;, linear whistler waves propagating along the shock normal are not able to “phase stand” in the upstream flow, and “…the shock will be initiated by a monotonic ramp.” (Kennel et al., 1985, https://doi.org/10.1029/gm034p0001). In this study, we present results of numerical simulations and observations of shocks with &lt;span&gt;&lt;/span&gt;&lt;math&gt;\u0000 &lt;semantics&gt;\u0000 &lt;mrow&gt;\u0000 &lt;mi&gt;M&lt;/mi&gt;\u0000 &lt;mo&gt;&gt;&lt;/mo&gt;\u0000 &lt;msub&gt;\u0000 &lt;mi&gt;M&lt;/mi&gt;\u0000 &lt;mi&gt;CrW&lt;/mi&gt;\u0000 &lt;/msub&gt;\u0000 &lt;/mrow&gt;\u0000 &lt;annotation&gt; $M &gt; {M}_{mathit{CrW}}$&lt;/annotation&gt;\u0000 &lt;/semantics&gt;&lt;/math&gt; that reveal the occurrence of an alternative scenario. For both the shock resulting from kinetic particle-in-cell simulations and that observed by MMS, the propagation direction of the precursor deviates from the shock normal direction. As a result, the velocity of the surface of constant phase along the shock normal exceeds the phase speed of these waves. It is shown that the propagation of the surface of constant phase along the shock normal occurs at a velocity that is nearly equal to the shock speed. Hence, these waves are “phase standing along the shock normal” in spite of &lt;span&gt;&lt;/span&gt;&lt;math&gt;\u0000 &lt;semantics&gt;\u0000 &lt;mrow&gt;\u0000 &lt;mi&gt;M&lt;/mi&gt;\u0000 &lt;mo&gt;&gt;&lt;/mo&gt;\u0000 &lt;msub&gt;\u0000 ","PeriodicalId":15894,"journal":{"name":"Journal of Geophysical Research: Space Physics","volume":"131 1","pages":""},"PeriodicalIF":2.9,"publicationDate":"2026-01-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://agupubs.onlinelibrary.wiley.com/doi/epdf/10.1029/2025JA034905","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145964224","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Merging and Dissipation of Intense Equatorial Plasma Bubbles With Large-Scale Mid-Latitude Low Electron Density Regions During the 23–24 April 2023 Geomagnetic Storm 2023年4月23-24日地磁风暴期间赤道强等离子体气泡与中纬度大尺度低电子密度区的合并和耗散
IF 2.9 2区 地球科学 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-09 DOI: 10.1029/2025JA033744
Yuhao Zheng, Chao Xiong, Xinyi Rang, Shunzu Gao, Xingxing Li

The extension of the post-sunset equatorial plasma bubbles (EPBs) to mid-latitudes during geomagnetic storms has been widely reported. However, previous research has primarily focused on the initiation and spatial distribution of these EPBs, while their decay processes remain underexplored. In this study, we provide observations of the evolution and dissipation of intense EPBs during the geomagnetic storm on 23–24 April 2023, using measurements from the Global-scale Observations of the Limb and Disk (GOLD), Swarm, and COSMIC-2 satellites. During the storm main phase, intense EPBs with zonal extents of ∼2–3° and latitudinal extents reaching up to ±35° magnetic latitude (Mlat) were observed between 15°W and 5°W. Simultaneously, very low electron density regions, spanning approximately from ±30° to ±45° Mlat and 420–500 km in altitude, were observed in the mid-latitudes. During the storm, the EPBs were observed to extend gradually poleward and subsequently encountered the low electron density regions. This encounter process, along with the storm-caused electric field dynamics, led to a gradual weakening and diffusion of the EPBs. The airglow images from GOLD showed that EPBs evolved from coherent depletions into structurally diffused forms with embedded filamentary features and eventually merged into the background. Notably, a hemispheric asymmetry in EPB dissipation was observed. In the Northern Hemisphere, EPBs tended to retain their morphology for a longer time, while in the Southern Hemisphere, more rapid dissipation occurred, likely due to differing background plasma conditions and magnetic field configurations in the two hemispheres. These findings reveal a previously uncharacterized feature of EPB dissipation during geomagnetic storms.

在地磁暴期间,日落后赤道等离子体气泡(EPBs)向中纬度地区的延伸已被广泛报道。然而,以往的研究主要集中在这些epb的起始和空间分布上,而它们的衰变过程仍未得到充分的探索。本文利用GOLD卫星、Swarm卫星和COSMIC-2卫星的全球尺度观测资料,对2023年4月23-24日地磁风暴期间强epb的演变和消散进行了观测。在风暴主阶段,在15°W至5°W之间观测到纬向范围为~ 2-3°、纬向范围为±35°磁纬(Mlat)的强强epb。同时,在中纬度地区观测到极低的电子密度区域,大约在±30°到±45°之间,海拔420-500 km。在风暴期间,观测到epb逐渐向极地延伸,随后遇到低电子密度区域。这一遭遇过程,加上风暴引起的电场动力学,导致epb逐渐减弱和扩散。GOLD的气辉图像显示,epb从连贯的耗尽演变为结构上扩散的形式,具有嵌入的丝状特征,并最终融入背景。值得注意的是,EPB的半球不对称消散被观察到。在北半球,epb倾向于在较长时间内保持其形态,而在南半球,耗散速度更快,可能是由于两个半球不同的背景等离子体条件和磁场结构。这些发现揭示了地磁风暴期间EPB耗散的一个以前未被描述的特征。
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引用次数: 0
Merging and Dissipation of Intense Equatorial Plasma Bubbles With Large-Scale Mid-Latitude Low Electron Density Regions During the 23–24 April 2023 Geomagnetic Storm 2023年4月23-24日地磁风暴期间赤道强等离子体气泡与中纬度大尺度低电子密度区的合并和耗散
IF 2.9 2区 地球科学 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-09 DOI: 10.1029/2025JA033744
Yuhao Zheng, Chao Xiong, Xinyi Rang, Shunzu Gao, Xingxing Li

The extension of the post-sunset equatorial plasma bubbles (EPBs) to mid-latitudes during geomagnetic storms has been widely reported. However, previous research has primarily focused on the initiation and spatial distribution of these EPBs, while their decay processes remain underexplored. In this study, we provide observations of the evolution and dissipation of intense EPBs during the geomagnetic storm on 23–24 April 2023, using measurements from the Global-scale Observations of the Limb and Disk (GOLD), Swarm, and COSMIC-2 satellites. During the storm main phase, intense EPBs with zonal extents of ∼2–3° and latitudinal extents reaching up to ±35° magnetic latitude (Mlat) were observed between 15°W and 5°W. Simultaneously, very low electron density regions, spanning approximately from ±30° to ±45° Mlat and 420–500 km in altitude, were observed in the mid-latitudes. During the storm, the EPBs were observed to extend gradually poleward and subsequently encountered the low electron density regions. This encounter process, along with the storm-caused electric field dynamics, led to a gradual weakening and diffusion of the EPBs. The airglow images from GOLD showed that EPBs evolved from coherent depletions into structurally diffused forms with embedded filamentary features and eventually merged into the background. Notably, a hemispheric asymmetry in EPB dissipation was observed. In the Northern Hemisphere, EPBs tended to retain their morphology for a longer time, while in the Southern Hemisphere, more rapid dissipation occurred, likely due to differing background plasma conditions and magnetic field configurations in the two hemispheres. These findings reveal a previously uncharacterized feature of EPB dissipation during geomagnetic storms.

在地磁暴期间,日落后赤道等离子体气泡(EPBs)向中纬度地区的延伸已被广泛报道。然而,以往的研究主要集中在这些epb的起始和空间分布上,而它们的衰变过程仍未得到充分的探索。本文利用GOLD卫星、Swarm卫星和COSMIC-2卫星的全球尺度观测资料,对2023年4月23-24日地磁风暴期间强epb的演变和消散进行了观测。在风暴主阶段,在15°W至5°W之间观测到纬向范围为~ 2-3°、纬向范围为±35°磁纬(Mlat)的强强epb。同时,在中纬度地区观测到极低的电子密度区域,大约在±30°到±45°之间,海拔420-500 km。在风暴期间,观测到epb逐渐向极地延伸,随后遇到低电子密度区域。这一遭遇过程,加上风暴引起的电场动力学,导致epb逐渐减弱和扩散。GOLD的气辉图像显示,epb从连贯的耗尽演变为结构上扩散的形式,具有嵌入的丝状特征,并最终融入背景。值得注意的是,EPB的半球不对称消散被观察到。在北半球,epb倾向于在较长时间内保持其形态,而在南半球,耗散速度更快,可能是由于两个半球不同的背景等离子体条件和磁场结构。这些发现揭示了地磁风暴期间EPB耗散的一个以前未被描述的特征。
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引用次数: 0
Climatology of Medium-Scale Traveling Ionospheric Disturbances Over Continental US Using GNSS TEC From 2012 to 2023 基于GNSS TEC的2012 - 2023年美国大陆中尺度电离层扰动气候学研究
IF 2.9 2区 地球科学 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-08 DOI: 10.1029/2025JA034134
Jing Liu, Shun-Rong Zhang, Anthea J. Coster, Philip J. Erickson, Hanli Liu

Medium-Scale Traveling Ionospheric Disturbances (MSTIDs) have long been a subject of interest in ionospheric research. However, their spatiotemporal variability across regions, local times, seasons, and solar cycles is very complicated and remains not well established. Using Total Electron Content (TEC) data from global GNSS receiver networks processed at MIT Haystack Observatory, we perform a detailed statistical analysis of MSTIDs over the Continental US (CONUS). Differential TEC data every day from 2012 to 2023 are processed using a keogram-based image processing technique to identify MSTID wave properties, including the occurrence, propagation direction, phase speed, wavelength, and period. Focusing on eastern US midlatitudes (80°W, 40°N), we extend comparisons longitudinally and latitudinally across CONUS. Our results reveal significant variability in MSTID occurrence rates and propagation directions, notably linked to solar terminators. MSTID occurrence peaks after summer sunrise (with minor maxima near winter daytime), around summer sunset, and after summer midnight. Occurrence generally correlates positively with solar activity in summer but can become negative after winter midnight. In winter, MSTIDs propagate southeastward in the morning and rotate clockwise to west-northwestward after midnight; in summer, propagation is more variable. Comparisons across the CONUS highlight strong regional differences. Our findings reflect complex drivers behind MSTIDs, including gravity waves, electrodynamic processes, and solar terminators. Their relative influences vary with local time, season, and location. This long-term analysis provides critical insights into MSTID climatology and forms a basis for in-depth investigations of MSTID generation mechanisms.

中尺度行电离层扰动(MSTIDs)一直是电离层研究的热点。然而,它们在区域、地方时、季节和太阳活动周期之间的时空变化非常复杂,尚未得到很好的确定。利用麻省理工学院干草堆天文台处理的全球GNSS接收器网络的总电子含量(TEC)数据,我们对美国大陆(CONUS)的mstid进行了详细的统计分析。从2012年到2023年,每天的TEC差分数据使用基于keogram图像处理技术进行处理,以识别MSTID波的属性,包括发生、传播方向、相速度、波长和周期。关注美国东部中纬度地区(80°W, 40°N),我们将纵向和纬度的比较扩展到整个CONUS。我们的研究结果揭示了MSTID的发生率和传播方向的显著变化,特别是与太阳终止器有关。MSTID的发生高峰在夏季日出之后(冬季白天附近有次要高峰)、夏季日落前后和夏季午夜之后。在夏季,这种现象通常与太阳活动呈正相关,但在冬季午夜之后可能变为负相关。在冬季,mstid在早晨向东南方向传播,午夜后顺时针向西北偏西方向旋转;在夏季,繁殖更加多变。美洲国家间的比较凸显了强烈的地区差异。我们的发现反映了mstid背后复杂的驱动因素,包括重力波、电动力过程和太阳终止器。它们的相对影响因当地时间、季节和地点而异。这一长期分析提供了对MSTID气候学的重要见解,并为深入研究MSTID产生机制奠定了基础。
{"title":"Climatology of Medium-Scale Traveling Ionospheric Disturbances Over Continental US Using GNSS TEC From 2012 to 2023","authors":"Jing Liu,&nbsp;Shun-Rong Zhang,&nbsp;Anthea J. Coster,&nbsp;Philip J. Erickson,&nbsp;Hanli Liu","doi":"10.1029/2025JA034134","DOIUrl":"10.1029/2025JA034134","url":null,"abstract":"<p>Medium-Scale Traveling Ionospheric Disturbances (MSTIDs) have long been a subject of interest in ionospheric research. However, their spatiotemporal variability across regions, local times, seasons, and solar cycles is very complicated and remains not well established. Using Total Electron Content (TEC) data from global GNSS receiver networks processed at MIT Haystack Observatory, we perform a detailed statistical analysis of MSTIDs over the Continental US (CONUS). Differential TEC data every day from 2012 to 2023 are processed using a keogram-based image processing technique to identify MSTID wave properties, including the occurrence, propagation direction, phase speed, wavelength, and period. Focusing on eastern US midlatitudes (80°W, 40°N), we extend comparisons longitudinally and latitudinally across CONUS. Our results reveal significant variability in MSTID occurrence rates and propagation directions, notably linked to solar terminators. MSTID occurrence peaks after summer sunrise (with minor maxima near winter daytime), around summer sunset, and after summer midnight. Occurrence generally correlates positively with solar activity in summer but can become negative after winter midnight. In winter, MSTIDs propagate southeastward in the morning and rotate clockwise to west-northwestward after midnight; in summer, propagation is more variable. Comparisons across the CONUS highlight strong regional differences. Our findings reflect complex drivers behind MSTIDs, including gravity waves, electrodynamic processes, and solar terminators. Their relative influences vary with local time, season, and location. This long-term analysis provides critical insights into MSTID climatology and forms a basis for in-depth investigations of MSTID generation mechanisms.</p>","PeriodicalId":15894,"journal":{"name":"Journal of Geophysical Research: Space Physics","volume":"131 1","pages":""},"PeriodicalIF":2.9,"publicationDate":"2026-01-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://agupubs.onlinelibrary.wiley.com/doi/epdf/10.1029/2025JA034134","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145964079","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Spatial Geographic Variation in Earth's Core Magnetic Field Modifies the Radiation Belt Electron Flux Relationship With Substorms, ULF Waves, and Solar Wind Drivers 地核磁场的空间地理变化改变了辐射带电子通量与亚暴、极低频波和太阳风驱动因素的关系
IF 2.9 2区 地球科学 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-07 DOI: 10.1029/2025JA034702
Laura E. Simms, Mark J. Engebretson

Spatial geographic variability in Earth's core magnetic field, measured at 400 km altitude but corrected for ionospheric and magnetospheric signals, correlates with electron flux levels measured by the RBSP spacecraft. A higher Earth's |B| magnitude results in lower flux over L2-6. Over 20 eV–2 MeV, at L2-4, this negative correlation is as large as −0.21, peaking at the 158 keV electrons, with the strongest effects in the 71 keV–2 MeV electrons. Despite higher L shells being well above the 400 km field measure, statistically significant correlation with the core field was still seen in higher energy 1–2 MeV electrons over L5-6. Adding Earth's geographic |B| variability as a covariate in regression or ARMAX analyses, particularly at lower L shells, results in stronger correlations between electron flux and solar wind, substorm, and ULF wave drivers, with possible nonlinearity in the associations accounted for by taking logs of the variables. At L2, substorms (measured by the SME index), ULF waves, and solar wind velocity show increased correlations with electron flux (30%, 100%, and 175%, respectively) when Earth's |B| is added as a covariate to the ARMAX regression models. Modest increases in correlation of electron flux with these possible drivers were also seen at L3-6. This argues for the addition of Earth's |B| as a covariate in models of electron response to drivers.

地球核心磁场的空间地理变异性是在400公里高度测量的,但对电离层和磁层信号进行了校正,它与RBSP航天器测量的电子通量水平相关。地球的b|等越高,L2-6上空的通量就越低。在20 eV-2 MeV以上,在L2-4处,这种负相关系数高达- 0.21,在158 keV电子处达到峰值,在71 keV - 2 MeV电子处影响最强。尽管高L壳层远高于400 km场测量值,但在L5-6的1-2 MeV高能电子中,仍然可以看到与核心场的统计显著相关性。在回归或ARMAX分析中,特别是在低L壳层,将地球的地理bb|变率作为协变量加入,结果表明电子通量与太阳风、亚风暴和极低频波驱动因素之间存在更强的相关性,并通过对变量取对数来解释关联中可能存在的非线性。在L2,当在ARMAX回归模型中加入地球的b| B|作为协变量时,亚暴(由SME指数测量)、ULF波和太阳风速度与电子通量的相关性增加(分别为30%、100%和175%)。在L3-6也可以看到电子通量与这些可能驱动因素的相关性适度增加。这就支持在电子对驱动的响应模型中加入地球的b|作为协变量。
{"title":"Spatial Geographic Variation in Earth's Core Magnetic Field Modifies the Radiation Belt Electron Flux Relationship With Substorms, ULF Waves, and Solar Wind Drivers","authors":"Laura E. Simms,&nbsp;Mark J. Engebretson","doi":"10.1029/2025JA034702","DOIUrl":"10.1029/2025JA034702","url":null,"abstract":"<p>Spatial geographic variability in Earth's core magnetic field, measured at 400 km altitude but corrected for ionospheric and magnetospheric signals, correlates with electron flux levels measured by the RBSP spacecraft. A higher Earth's |B| magnitude results in lower flux over L2-6. Over 20 eV–2 MeV, at L2-4, this negative correlation is as large as −0.21, peaking at the 158 keV electrons, with the strongest effects in the 71 keV–2 MeV electrons. Despite higher L shells being well above the 400 km field measure, statistically significant correlation with the core field was still seen in higher energy 1–2 MeV electrons over L5-6. Adding Earth's geographic |B| variability as a covariate in regression or ARMAX analyses, particularly at lower L shells, results in stronger correlations between electron flux and solar wind, substorm, and ULF wave drivers, with possible nonlinearity in the associations accounted for by taking logs of the variables. At L2, substorms (measured by the SME index), ULF waves, and solar wind velocity show increased correlations with electron flux (30%, 100%, and 175%, respectively) when Earth's |B| is added as a covariate to the ARMAX regression models. Modest increases in correlation of electron flux with these possible drivers were also seen at L3-6. This argues for the addition of Earth's |B| as a covariate in models of electron response to drivers.</p>","PeriodicalId":15894,"journal":{"name":"Journal of Geophysical Research: Space Physics","volume":"131 1","pages":""},"PeriodicalIF":2.9,"publicationDate":"2026-01-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145963774","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
Debye-Scale Bipolar Structures and Their Role in the Electron Trajectory Instability at the Bow Shock 德拜尺度双极结构及其在弓形激波下电子轨迹不稳定性中的作用
IF 2.9 2区 地球科学 Q2 ASTRONOMY & ASTROPHYSICS Pub Date : 2026-01-07 DOI: 10.1029/2025JA034361
Simon N. Walker, Michael Gedalin, Michael A. Balikhin

A number of mechanisms have been suggested to operate within the terrestrial bow shock to redistribute energy contained in the incoming solar wind flow. The majority of mechanisms involve the generation of turbulence while some are based on particle motion alone. In this paper, we investigate the possible occurrence of the Electron Trajectory Instability, that results from short scale electric field gradients. Spike-like bipolar features in electric field measurements are a commonly observed signature within the terrestrial bow shock. They are usually associated with the passage of electrostatic solitary waves associated with phase space holes in the particle distribution. Using electric field measurements, we compare different interferometric methods to determine the propagation direction, velocity, and spatial scale of these features. Based on these results, it appears that the instability criterion for the Electron Trajectory Instability is fulfilled and the electron trajectories will diverge in the presence of these structures.

许多机制已经被提出在地球弓形激波中运作,以重新分配入射太阳风流中包含的能量。大多数机制涉及湍流的产生,而有些机制仅基于粒子运动。本文研究了由短尺度电场梯度引起的电子轨迹不稳定性的可能发生。电场测量中的尖峰状双极特征是在地面弓形激波中通常观察到的特征。它们通常与粒子分布中与相空间空穴相关的静电孤立波的通过有关。通过电场测量,我们比较了不同的干涉测量方法,以确定这些特征的传播方向、速度和空间尺度。这些结果表明,电子轨迹不稳定的判据已经满足,在这些结构的存在下,电子轨迹将发生发散。
{"title":"Debye-Scale Bipolar Structures and Their Role in the Electron Trajectory Instability at the Bow Shock","authors":"Simon N. Walker,&nbsp;Michael Gedalin,&nbsp;Michael A. Balikhin","doi":"10.1029/2025JA034361","DOIUrl":"10.1029/2025JA034361","url":null,"abstract":"<p>A number of mechanisms have been suggested to operate within the terrestrial bow shock to redistribute energy contained in the incoming solar wind flow. The majority of mechanisms involve the generation of turbulence while some are based on particle motion alone. In this paper, we investigate the possible occurrence of the Electron Trajectory Instability, that results from short scale electric field gradients. Spike-like bipolar features in electric field measurements are a commonly observed signature within the terrestrial bow shock. They are usually associated with the passage of electrostatic solitary waves associated with phase space holes in the particle distribution. Using electric field measurements, we compare different interferometric methods to determine the propagation direction, velocity, and spatial scale of these features. Based on these results, it appears that the instability criterion for the Electron Trajectory Instability is fulfilled and the electron trajectories will diverge in the presence of these structures.</p>","PeriodicalId":15894,"journal":{"name":"Journal of Geophysical Research: Space Physics","volume":"131 1","pages":""},"PeriodicalIF":2.9,"publicationDate":"2026-01-07","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://agupubs.onlinelibrary.wiley.com/doi/epdf/10.1029/2025JA034361","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145963749","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"地球科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
期刊
Journal of Geophysical Research: Space Physics
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