2015
DOI: 10.1007/s11207-015-0800-2
|View full text |Cite
|
Sign up to set email alerts
|

Reconstruction of Helio-Latitudinal Structure of the Solar Wind Proton Speed and Density

Abstract: The modeling of the heliosphere requires continuous three-dimensional solar wind data. The in-situ out-of-ecliptic measurements are very rare, so that other methods of solar wind detection are needed. We use the remote-sensing data of the solar wind speed from observations of interplanetary scintillation (IPS) to reconstruct spatial and temporal structures of the solar wind proton speed from 1985 to 2013. We developed a method of filling the data gaps in the IPS observations to obtain continuous and homogeneou… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

6
42
0

Year Published

2015
2015
2022
2022

Publication Types

Select...
7

Relationship

2
5

Authors

Journals

citations
Cited by 52 publications
(48 citation statements)
references
References 104 publications
(200 reference statements)
6
42
0
Order By: Relevance
“…The lowenergy ENA flux varies with changes in the SW dynamic pressure over the course of the solar cycle, which is generally in phase with the sunspot number, whereas the high-energy Figure 9. Heliolatitude vs.time map of the SW speed reconstructed from interplanetary scintillation (IPS) data and OMNI data, as described in Sokół et al (2015). Figure 10.…”
Section: Discussionmentioning
confidence: 99%
See 2 more Smart Citations
“…The lowenergy ENA flux varies with changes in the SW dynamic pressure over the course of the solar cycle, which is generally in phase with the sunspot number, whereas the high-energy Figure 9. Heliolatitude vs.time map of the SW speed reconstructed from interplanetary scintillation (IPS) data and OMNI data, as described in Sokół et al (2015). Figure 10.…”
Section: Discussionmentioning
confidence: 99%
“…Because the SW dynamic pressure is regarded as an SW invariant with heliolatitude (McComas et al . 2008), we use the dynamic pressure calculated from the ecliptic OMNI-2 archive (King & Papitashvili 2005) as a proxy for P 1 au in the polar regions (see also thediscussion in Sokół et al 2013 andSokół et al 2015). The upper plot is for the north pole,and the lower isfor the south pole.…”
Section: Correlation Of 1 Au Dynamic Pressure With Ena-derived Plasmamentioning
confidence: 99%
See 1 more Smart Citation
“…The solar wind energy flux and density at 1 AU show a coherent decay with time (peak to basin ratio of~2) up to early 2010 and a recovery in both quantities thereafter (e.g. Figure 9 in [41]). This, as expected (e.g.…”
Section: Global Ena Emissions Over Solar Cycles 23 and 24mentioning
confidence: 96%
“…Recent studies [41] have undertaken a significant effort to calculate the solar wind parameters as a function of time for the in-ecliptic solar wind data at 1 AU from the OMNI database. The solar wind energy flux and density at 1 AU show a coherent decay with time (peak to basin ratio of~2) up to early 2010 and a recovery in both quantities thereafter (e.g.…”
Section: Global Ena Emissions Over Solar Cycles 23 and 24mentioning
confidence: 99%