2002
DOI: 10.1086/345587
|View full text |Cite
|
Sign up to set email alerts
|

Loop-Top Nonthermal Microwave Source in Extended Solar Flaring Loops

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

5
76
0
6

Year Published

2003
2003
2018
2018

Publication Types

Select...
5
5

Relationship

2
8

Authors

Journals

citations
Cited by 118 publications
(87 citation statements)
references
References 15 publications
5
76
0
6
Order By: Relevance
“…The fast electrons are concentrated at or near the looptop as often seen in flares (e.g., Melnikov et al 2002). Both longitudinal and transverse distributions are well described by Gaussian functions with the parameters listed in Table 1; see also Figure 6, right column.…”
Section: Discussionmentioning
confidence: 73%
“…The fast electrons are concentrated at or near the looptop as often seen in flares (e.g., Melnikov et al 2002). Both longitudinal and transverse distributions are well described by Gaussian functions with the parameters listed in Table 1; see also Figure 6, right column.…”
Section: Discussionmentioning
confidence: 73%
“…Also, the isotropic injection implies strong scattering in the acceleration process. Although the electron accumulation at the looptop can be explained by a trapplus-precipitation model with modest mirror ratios σ < 2, we concluded that the pitch-angle distribution must be wide enough to be divided by the losscone, or else it will result in either a fully trapped (as proposed by Melnikov et al (2002) due to an anisotropic pitch-angle distribution orthogonal do the magnetic field, the so-called pancake distribution) or fully precipitated scenario (as in the classical thick-target model). This requirement can be fulfilled by moderate/strong pitch-angle scattering processes.…”
Section: Pitch-angle Scatteringmentioning
confidence: 77%
“…We suggest that this spatial QPP distribution is not the pulsation mode property, but is connected with the properties of the acceleration and transport of energetic electrons. It was found from the model simulations (Melnikov et al 2002;Gorbikov & Melnikov 2007;Reznikova et al 2009) that the absence of the emission peaks in the LT can be a natural consequence of anisotropic injection of accelerated electrons near to the loop apex predominantly along magnetic field lines. In this case the injected electrons pass quickly though the upper part of the loop with almost zero pitch-angle and, therefore, effectiveness of their gyrosynchrotron emission there is very low.…”
Section: Spatial Distribution Of Qpp and Modulation Depthmentioning
confidence: 99%