Multispacecraft Observations of the Simultaneous Occurrence of Magnetic Reconnection at High and Low Latitudes During the Passage of a Solar Wind Rotational Discontinuity Embedded in the April 9‐11, 2015 ICME
暂无分享,去创建一个
S. Wing | N. Lugaz | C. Escoubet | C. Farrugia | J. Berchem
[1] S. Wing,et al. Effects from dayside magnetosphere to distant tail unleashed by a bifurcated, non-reconnecting interplanetary current sheet , 2022, Frontiers in Physics.
[2] I. Richardson,et al. Substorm Occurrence and Intensity Associated With Three Types of Solar Wind Structure , 2017 .
[3] C.‐L. Huang,et al. Extreme geomagnetic disturbances due to shocks within CMEs , 2015 .
[4] J. Šimůnek,et al. Analysis of temperature versus density plots and their relation to the LLBL formation under southward and northward IMF orientations , 2015 .
[5] S. Petrinec,et al. Distinguishing between pulsed and continuous reconnection at the dayside magnetopause , 2015, Journal of geophysical research. Space physics.
[6] J. Borovsky,et al. Magnetosphere response to high-speed solar wind streams: A comparison of weak and strong driving and the importance of extended periods of fast solar wind , 2012 .
[7] Jesper Gjerloev,et al. Evaluation of SuperMAG auroral electrojet indices as indicators of substorms and auroral power , 2011 .
[8] Q.‐H. Zhang,et al. Reconnection at high latitudes: antiparallel merging. , 2009, Physical review letters.
[9] M. Dunlop,et al. Reconnection at the dayside magnetopause: Comparisons of global MHD simulation results with Cluster and Double Star observations , 2008 .
[10] J. Borovsky,et al. Differences between CME‐driven storms and CIR‐driven storms , 2006 .
[11] S. Wing,et al. Dawn‐dusk asymmetries, ion spectra, and sources in the northward interplanetary magnetic field plasma sheet , 2005 .
[12] C. Meng,et al. Maps of precipitation by source region, binned by IMF, with inertial convection streamlines , 2004 .
[13] M. Dunlop,et al. Simultaneous Cluster and IMAGE observations of cusp reconnection and auroral proton spot for northward IMF , 2003 .
[14] D. Klumpar,et al. Temporal versus spatial interpretation of cusp ion structures observed by two spacecraft , 2002, Journal of Geophysical Research.
[15] S. Wing,et al. Geosynchronous magnetic field temporal response to solar wind and IMF variations , 2002 .
[16] S. Wing,et al. 2D plasma sheet ion density and temperature profiles for northward and southward IMF , 2002 .
[17] Simon Wing,et al. Double cusp: Model prediction and observational verification , 2001 .
[18] M. Ashour‐Abdalla,et al. The distant tail at 200 RE : Comparison between Geotail observations and the results from a global magnetohydrodynamic simulation , 1998 .
[19] S. Wing,et al. Central plasma sheet ion properties as inferred from ionospheric observations , 1998 .
[20] Mario H. Acuna,et al. THE CLUSTER MAGNETIC FIELD INVESTIGATION , 1997 .
[21] S. Wing,et al. Modeling the entry of magnetosheath electrons into the dayside ionosphere , 1996 .
[22] B. Tsurutani,et al. Interplanetary origin of geomagnetic activity in the declining phase of the solar cycle , 1995 .
[23] S. Wing,et al. A large statistical study of the entry of interplanetary magnetic field Y-component into the magnetosphere , 1995 .
[24] Nancy U. Crooker,et al. Postmodern view of M-regions , 1994 .
[25] W. Feldman,et al. The relationship between interplanetary discontinuities and Alfvén waves: Ulysses observations , 1994 .
[26] C. Russell,et al. Determining the standoff distance of the bow shock: Mach number dependence and use of models , 1994 .
[27] M. Smith,et al. The variation of reconnection rate at the dayside magnetopause and cusp ion precipitation , 1992 .
[28] M. Smith,et al. The statistical cusp: a flux transfer event model , 1992 .
[29] Patrick T. Newell,et al. Mapping the dayside ionosphere to the magnetosphere according to particle precipitation characteristics , 1992 .
[30] B. Tsurutani,et al. Great magnetic storms , 1992 .
[31] Patrick T. Newell,et al. The low‐latitude boundary layer and the boundary plasma sheet at low altitude: Prenoon precipitation regions and convection reversal boundaries , 1991 .
[32] V. Sigillito,et al. The auroral oval position, structure, and intensity of precipitation from 1984 onward: An automated on‐line data base , 1991 .
[33] M. Lockwood,et al. Low-altitude signatures of the cusp and flux transfer events , 1989 .
[34] D. Baker,et al. The SSC on July 29, 1977 and its propagation within the magnetosphere , 1982 .
[35] C. Russell,et al. The thickness of the magnetopause current layer: ISEE 1 and 2 observations , 1982 .
[36] Nancy U. Crooker,et al. Dayside merging and cusp geometry , 1979 .
[37] R. Kaufmann,et al. EXPLORER 12 MAGNETOPAUSE OBSERVATIONS: LARGE-SCALE NONUNIFORM MOTION. , 1969 .
[38] C. P. Escoubet,et al. CLUSTER – SCIENCE AND MISSION OVERVIEW , 1997 .
[39] Manuel Grande,et al. PEACE: A PLASMA ELECTRON AND CURRENT EXPERIMENT , 1997 .
[40] W. J. Burke,et al. Identification and observations of the plasma mantle at low altitude , 1991 .
[41] D. Hardy. Precipitating electron and ion detectors (SSJ/4) for the block 5D/flights 6-10 DMSP satellites: calibration and data presentation , 1984 .