2006
DOI: 10.1007/s11207-006-2068-z
|View full text |Cite
|
Sign up to set email alerts
|

Density Depletion in a Coronal Flux Tube Associated With Solar Radio Emission

Abstract: A discussion, which is motivated by recent study of solar radio emission, is presented to address the issue under what conditions the depletion of plasma density in a flux tube in the corona may take place. Two particular situations are of interest: One is that density is depleted due to the presence of beams of energetic particles, and the other is attributed to magnetic compression. The scenario discussed appears to be consistent with the occurrence type III solar radio bursts.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
12
0

Year Published

2009
2009
2015
2015

Publication Types

Select...
6

Relationship

0
6

Authors

Journals

citations
Cited by 10 publications
(12 citation statements)
references
References 30 publications
0
12
0
Order By: Relevance
“…This was first reported by Benson et al [1980], who studied ISIS‐1 data, and confirmed by many subsequent articles [e.g., Benson , 1985; Roux et al , 1993; Strangeway et al , 1998; Janhunen et al , 2002]. Recently, Wu et al [2006] have addressed the depletion of plasma density in a flux tube in the corona. They suggested that density depletion may also take place under conditions peculiar to active regions where solar flares occur annergetic particles are generated.…”
Section: Numerical Simulationsmentioning
confidence: 54%
See 1 more Smart Citation
“…This was first reported by Benson et al [1980], who studied ISIS‐1 data, and confirmed by many subsequent articles [e.g., Benson , 1985; Roux et al , 1993; Strangeway et al , 1998; Janhunen et al , 2002]. Recently, Wu et al [2006] have addressed the depletion of plasma density in a flux tube in the corona. They suggested that density depletion may also take place under conditions peculiar to active regions where solar flares occur annergetic particles are generated.…”
Section: Numerical Simulationsmentioning
confidence: 54%
“…A commonly accepted argument is that in a low‐ β plasma β (1 ≫ β ≪ m e /m i ), such as solar corona and auroral regions, a small perturbation of the ambient magnetic field in a flux tube can result in considerable density change because of pressure balance. Density depletion may also take place under conditions peculiar to active regions where solar flares occur and energetic particles are generated [ Wu et al , 2006]. Two possible theories are that density is depleted because of the presence of beams of energetic particles, and the other is attributed to magnetic compression.…”
Section: Introductionmentioning
confidence: 99%
“…On the basis of ECME, a model was explored for coronal type III bursts near the active region Yoon et al 2002). According to this model, the radio emissions are produced inside a magnetic flux tube with density depletion (Duncan 1979;Wu et al 2006) and propagate in the magnetic flux tube until they arrive at a point where the frequencies of the excited waves are equal to the local exterior cutoff frequency. With this model, some longstanding problems from observations of type III bursts can be naturally resolved.…”
Section: Introductionmentioning
confidence: 99%
“…The basic idea developed from observations that F/H waves with identical frequencies have overlapping source regions, as discussed previously in Section 2. In this more recent theory, we extend Duncan's notion by considering that, in the corona, there are density-depleted flux tubes in which the plasma density is much lower than the density of the exterior plasma (A model theory was proposed by Wu et al [27] to explain the origin of such density depletion). Several essential points were considered by Wu et al [23]: (i) waves emitted inside the duct have frequencies close to the local electron gyro frequency and/or second harmonic; (ii) the frequencies of the emitted waves are lower than the cutoff frequencies of the outside plasma so that the radiation cannot exit the duct; (iii) however, when an emitted wave propagates to a sufficiently high altitude where the cutoff frequency of the exterior plasma drops to a value lower than the wave frequency, it exits the duct and becomes visible; and (iv) it is therefore expected that waves having the same frequencies, regardless of where they are originated, exit at the same altitude.…”
Section: A Scenario Without Recourse To the Plasma Hypothesismentioning
confidence: 76%