1988
DOI: 10.1007/bf00148592
|View full text |Cite
|
Sign up to set email alerts
|

Observations and interpretation of solar flares at microwave frequencies

Abstract: The physical processes responsible for microwave emission in solar flares are outlined, and examples of how microwave observations have been interpreted in terms of physical parameters are described. Selected results obtained during Solar Cycle 21 with the microwave observatories dedicated to synoptic observations of the Sun are summarized. The status and future plans for these facilities at Bern and in Japan are presented. Also discussed are the instrument capabilities required at microwave frequencies to ach… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
7
0

Year Published

1990
1990
1993
1993

Publication Types

Select...
7
1

Relationship

0
8

Authors

Journals

citations
Cited by 22 publications
(7 citation statements)
references
References 62 publications
(6 reference statements)
0
7
0
Order By: Relevance
“…This examines the relationship of 9 type III bursts with energetic (>~ 100 keV) electrons (see the review by Crannell et al, 1988).…”
Section: Introductionmentioning
confidence: 99%
“…This examines the relationship of 9 type III bursts with energetic (>~ 100 keV) electrons (see the review by Crannell et al, 1988).…”
Section: Introductionmentioning
confidence: 99%
“…Maser emission occurs in narrow bands close to the cyclotron frequency Q = eB/m e and its harmonics sCl and its coherence can account for the high brightness temperatures associated with the observed microwave bursts (Melrose and Dulk 1982a, b;Crannell et al 1988). Due to spatial gradients in the field, the waves quickly propagate out of the region in which they can be amplified, thereby producing elementary bursts of short duration (Melrose and Dulk 1984).…”
Section: (A) the Loss-lone-driven Cyclotron Masermentioning
confidence: 99%
“…1. Introduction Millisecond bursts of microwave emission observed during some solar flares are found to exhibit characteristic properties of high brightness temperatures (up to ~ 10 18 K), high degrees of circular polarisation (up to ~ 100%), narrow bandwidths (-1%) and fine temporal structure (1-10 ms) (Slottje 1978(Slottje , 1980Crannell et al 1988). The emission mechanism most widely invoked to account for these properties of microwave spike bursts is the loss-cone-driven electron cyclotron maser (e.g., Wu and Lee 1979;Melrose and Dulk 1982a,b;Melrose et al 1984;Dulk 1985;McKean et al 1989).…”
mentioning
confidence: 99%
“…For example, the range of required magnetic fields for the thick‐target model was smaller than for the thin‐target and multithermal models, suggesting that this might be the better model [ Lu and Petrosian , 1989]. However, some correlations seem to depend on the duration of the x‐ray event [ Kosugi et al , 1988], such that the thick‐target model was preferred for the impulsive flares, while extended flares were better represented by electrons trapped in the corona.…”
Section: Energy Input: the Impulsive Phasementioning
confidence: 99%