2009
DOI: 10.1016/j.jastp.2008.09.019
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Introduction to Special Issue on high speed solar wind streams and geospace interactions (HSS–GI)

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Cited by 13 publications
(9 citation statements)
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“…The arrival of high‐speed solar wind streams (HSSs) at the Earth's magnetosphere initiates numerous physical processes, including (1) a sudden onset of magnetospheric convection (e.g., McPherron and Weygand [2006] and compare Figure 5), (2) enhanced density, heating, and transport in the plasma sheet [e.g., Borovsky et al , 1998; Lavraud et al , 2006; Denton and Borovsky , 2008], (3) enhanced particle precipitation [ Longden et al , 2008], (4) flux dropouts/recovery of outer radiation belt electrons [e.g., Paulikas and Blake , 1979; O'Brien et al , 2001; Borovsky and Denton , 2009a], (5) the formation of long‐lived plasmaspheric drainage plumes [ Borovsky and Denton , 2006b, 2008], and (6) an increase in ionospheric heating and the occurrence of F region storms [ Denton et al , 2009b; Sojka et al , 2009]. Many of these processes are interlinked [e.g., Tsurutani et al , 2006; Kavanagh and Denton , 2007; Denton et al , 2009a]. For example, the onset of convection (process 1) causes plasma from the outer plasmasphere to be stripped away into a plasmaspheric plume (process 5), which is implicated in the loss of relativistic electrons from the outer radiation belt (process 4) [ Borovsky and Denton , 2009a].…”
Section: Evolution Of the Outer Electron Radiation Belt During High‐smentioning
confidence: 99%
“…The arrival of high‐speed solar wind streams (HSSs) at the Earth's magnetosphere initiates numerous physical processes, including (1) a sudden onset of magnetospheric convection (e.g., McPherron and Weygand [2006] and compare Figure 5), (2) enhanced density, heating, and transport in the plasma sheet [e.g., Borovsky et al , 1998; Lavraud et al , 2006; Denton and Borovsky , 2008], (3) enhanced particle precipitation [ Longden et al , 2008], (4) flux dropouts/recovery of outer radiation belt electrons [e.g., Paulikas and Blake , 1979; O'Brien et al , 2001; Borovsky and Denton , 2009a], (5) the formation of long‐lived plasmaspheric drainage plumes [ Borovsky and Denton , 2006b, 2008], and (6) an increase in ionospheric heating and the occurrence of F region storms [ Denton et al , 2009b; Sojka et al , 2009]. Many of these processes are interlinked [e.g., Tsurutani et al , 2006; Kavanagh and Denton , 2007; Denton et al , 2009a]. For example, the onset of convection (process 1) causes plasma from the outer plasmasphere to be stripped away into a plasmaspheric plume (process 5), which is implicated in the loss of relativistic electrons from the outer radiation belt (process 4) [ Borovsky and Denton , 2009a].…”
Section: Evolution Of the Outer Electron Radiation Belt During High‐smentioning
confidence: 99%
“…The D ST index typically displays a shallow minimum during an HSS‐driven storm, the relatively low magnitude of which indicates a much less intense ring current than that during a typical CME‐driven storm. On occasion, the low‐intensity D ST signature of some HSS‐driven storms has caused them to be overlooked in storm studies; an omission which has been referred to as the “ D ST mistake” [ Denton et al ., ].…”
Section: Data Sets and Hss Identificationmentioning
confidence: 99%
“…Historically, these intervals have been defined using the Dst index (Piddington, ; Loewe & Prölss, ). Since Dst effectively measures the energy content of the ring current (Sckopke, ), whether it is an appropriate measure for organizing or predicting other space weather disturbances has been discussed (Borovsky & Shprits, ; Denton et al, ). Operational space weather forecast centers use the Kp index (Mayaud, ) to define geomagnetic storm levels (Sharpe & Murray, ).…”
Section: Introductionmentioning
confidence: 99%