2003
DOI: 10.5194/npg-10-151-2003
|View full text |Cite
|
Sign up to set email alerts
|

Geometric aspects of HF driven Langmuir turbulence in the ionosphere

Abstract: Abstract. The geometric aspects of HF-generated Langmuir turbulence in the ionosphere and its detection by radars are theoretically discussed in a broad approach, including local modelling (damped and driven Zakharov system), basic parametric instabilities, polarization and strength of the driving electric field, and radar configurations. Selected examples of numerical results from the local model are presented and discussed in relation to recent experiments, with emphasis on recent experiments at the EISCAT f… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

5
30
0

Year Published

2005
2005
2020
2020

Publication Types

Select...
8

Relationship

0
8

Authors

Journals

citations
Cited by 27 publications
(35 citation statements)
references
References 59 publications
5
30
0
Order By: Relevance
“…Mjølhus 1990) arcsin sin where . Ray-tracing results for EISCAT parameters (Mjølhus et al 2003) show very similar features as here. Inside the Spitze range, the polarization of the electric field tend to be along the magnetic field as the wave reaches the critical layer, while outside the Spitze, the polarization instead approaches vertical (Mjølhus et al 2003).…”
Section: Full-wave Modeling Of Strong Langmuir Turbulencesupporting
confidence: 77%
“…Mjølhus 1990) arcsin sin where . Ray-tracing results for EISCAT parameters (Mjølhus et al 2003) show very similar features as here. Inside the Spitze range, the polarization of the electric field tend to be along the magnetic field as the wave reaches the critical layer, while outside the Spitze, the polarization instead approaches vertical (Mjølhus et al 2003).…”
Section: Full-wave Modeling Of Strong Langmuir Turbulencesupporting
confidence: 77%
“…These calculations suggest that the maximum turbulence seen by the UHF radar ought to lie at the critical height between the Spitze angle and the vertical, yet the maximum occurs outside the Spitze, at an angle where the pump wave does not reach critical, and, perhaps even more puzzling, at an altitude several km below the maximum height reached by the pump. Mjølhus et al (2003) consider this problem and are unable to suggest an explanation. At positions beyond the Spitze to the south, conditions for strong polarization of the pump electric field along the geomagnetic field are present when the pump wave is propagating downward after reflection.…”
Section: Discussionmentioning
confidence: 99%
“…Stubbe and Hagfors (1997) comment: "One of the shortcomings in the theoretical work appears to be an inappropriate treatment of the low frequency turbulence which depends very sensitively on the direction with respect to the magnetic field, implying that the full angular spectrum rather than a prescribed fixed angular component should be considered." Although Mjølhus et al (2003) have recently addressed this criticism for the theoretical interpretation of incoherent scatter observations of Langmuir turbulence, much remains to be done. Furthermore, this comment applies equally well to experimental results.…”
Section: Discussionmentioning
confidence: 99%
“…The SSA dynamics as a whole conforms to theoretical calculations in the weak-turbulence approximation [59], while the SEE generation process at this stage of pumping has not been given adequate interpretation. Large progress has been achieved in the numerical simulation of the nonlinear stage of SPI within the framework of Zakharov's equation with allowance for the isothermal nature and regular inhomogeneity of the ionospheric plasma, as well as for the geomagnetic field [60]. At the same time, this modeling was performed for a time-constant amplitude of the PW, which disagrees with the experiment data.…”
Section: Initial Stage Of the Action: Striction Parametric Instabilitymentioning
confidence: 99%