Index of /data/ins_data/impact/level3

 Name                          Last modified      Size  
 Parent Directory                                   -   
 LanJian_STEREO_ICME_List.txt  2023-01-13 05:00   84K  
 LanJian_STEREO_SIR_List.txt   2023-01-13 05:00   79K  
 LanJian_STEREO_Shock_List.txt 2023-01-13 05:16   85K  
 SEP_plots.pdf                 2024-03-04 16:23  5.8M  
 SEPs.pdf                      2024-03-04 16:23  124K  
 SEPs_spase_hpevent.txt        2024-03-04 16:24   11K  
 STEREO_Level3_ICME.pdf        2023-01-13 04:54  462K  
 STEREO_Level3_ICME.xls        2023-01-13 04:53  188K  
 STEREO_Level3_SIR.pdf         2023-01-13 04:56  318K  
 STEREO_Level3_SIR.xls         2023-01-13 04:55  206K  
 STEREO_Level3_Shock.pdf       2023-01-13 04:51  408K  
 STEREO_Level3_Shock.xls       2023-01-13 04:51  197K

Original website: https://stereo-dev.epss.ucla.edu/l3_events

Level 3 Results of STEREO IMPACT/PLASTIC
Note: All the dates and times in the following lists are UTC times. All the following lists are not final results. Please check back later for updates.

1. List of Interplanetary Coronal Mass Ejections (ICMEs)

The ICMEs are identified based on inspection of a combination of signatures: an enhancement of total perpendicular pressure (P_t = B²/(2μ₀) + Σ_jn_jkT_perp,_j, where j represents the three major species in the solar wind: protons, electrons and alpha particles, see Russell et al., 2005. Its gradient indicates the force), a stronger than ambient magnetic field, relatively quiet and smooth magnetic field rotations, a declining solar wind speed, a low proton temperature [Jian et al., 2006a, 2013, 2018].

At least three of the above features were required to identify an ICME. The edges of ICMEs were identified from a consensus of available features, usually delimited on sharp changes in plasma and magnetic field properties. For ambiguous events, we checked the SOHO LASCO CME catalog and STEREO SECCHI observations.

2. List of Stream Interaction Regions (SIRs)

The SIRs include corotating interaction regions (CIRs) and transient stream interaction regions. The difference between a CIR and a transient SIR is only that a CIR recurs for two or more solar rotation cycles.

The SIRs are identified based on inspection of the following features: an increase of solar wind speed, a pile-up of total perpendicular pressure (P_t) with gradual decreases at both sides from the P_t peak to the edges of interaction region, velocity deflections, a first-increase and then decrease of proton number density, an enhancement of proton temperature, an increase of the entropy defined as ln(T_p^3/2/N_p) [Siscoe and Intriligator, 1993; Crooker et al., 1996], a compression of the magnetic field. We require the presence of at least 5 signatures, and identify SIRs with careful consideration of the ambient solar wind. For detail, please refer to Jian et al., 2006b, 2013, 2019.

3. List of Interplanetary Shocks

The forward and reverse shocks are identified using 8-Hz magnetic field data. We rotated them into shock normal coordinates to examine the existence of associated shock waves and field changes consistent with the Rankine-Hugoniot relations. The shock normal angle (θ_Bn), field change, and Mach number, are also given in this list.

To confirm, we have also checked the 1-min PLASTIC data. At forward shocks, all of solar wind speed, proton number density, proton temperature, and magnetic field should increase simultaneously. At reverse shocks, solar wind speed increases, while proton number density, proton temperature, and magnetic field all decrease. However, not all shocks have clear signatures in plasma properties. We indicate such shocks in the comments.

4. List of Solar Energetic Proton (SEP) Events Observed by both STA and STB

5. List of PLASTIC Suprathermal Proton Events from University of New Hampshire

Suprathermal Lists

Reference:

Crooker, N.U., M.E. Burton, G.L. Siscoe, S.W. Kahler, J.T. Gosling, and E.J. Smith (1996), Solar wind streamer belt structure, J. Geophys. Res., 101, 24331.

Jian, L., C.T. Russell, J.G. Luhmann, and R.M. Skoug (2006a), Properties of interplanetary coronal mass ejections at one AU during 1995 - 2004, Sol. Phy., 239, 393, doi: 10.1007/s11207-006-0133-2.

Jian, L., C.T. Russell, J.G. Luhmann, and R.M. Skoug (2006b), Properties of stream interaction at one AU during 1995 - 2004, Sol. Phy., 239, 337, doi: 10.1007/s11207-006-0132-3.

Jian, L.K., C.T. Russell, J.G. Luhmann, A.B. Galvin, and K.D.C. Simunac (2013), Solar Wind Observations at STEREO: 2007 - 2011, Amer. Inst. Phys. Proceedings of Solar Wind 13, 1539, 191, doi: 10.1063/1.4811020.

Jian, L.K., C.T. Russell, J.G. Luhmann, and A.B. Galvin (2018), STEREO observations of interplanetary coronal mass ejections in 2007-2016, The Astrophys. J., 885, 114, doi: 10.3847/1538-4357/aab189.

Jian, L.K., J.G. Luhmann, C.T. Russell, and A.B. Galvin (2019), Solar Terrestrial Relations Observatory (STEREO) observations of stream interaction regions in 2007-2016: Relationship with heliospheric current sheets, solar cycle variations, and dual observations, Solar Phys., 294, 31, doi: 10.1007/s11207-019-1416-8.

Russell, C.T., A.A. Shinde, and L. Jian (2005), A new parameter to define interplanetary coronal mass ejections, Adv. Space Res., 35, 2178.

Siscoe, G., and D. Intriligator (1993), Three views of two giant streams: aligned observations at 1 AU, 4.6 AU, and 5.9 AU, Geophys. Res. Lett., 20 (20), 2267. pFad - Phonifier reborn

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