electron density perturbation
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2019 ◽  
Vol 37 (4) ◽  
pp. 341-345
Author(s):  
Narender Kumar ◽  
Ram Kishor Singh ◽  
R. Uma ◽  
R. P. Sharma

AbstractA scheme of phase-matched terahertz generation by beating two co-propagating lasers in magnetized plasma, in the presence of a magnetosonic wave (MSW), is developed. The beat frequency ponderomotive force of the lasers imparts an oscillatory drift to electrons. The electron drift velocity couples with the electron density perturbation associated with the MSW to produce an irrotational nonlinear current $\left(\nabla \times {\vec J}\;{}^{\rm NL}\ne 0\right)$. The beat current density resonantly excites a THz (Terahertz) radiation when the phase-matching conditions are satisfied. The MSW mediates the phase matching. At 9.6 and 10.6 µm wavelengths, and background magnetic field of 285 kG, one may achieve normalized THz wave amplitude of the order of 10−3 and one obtains the ratio of THz power to pump power of the order of 10−6.


2014 ◽  
Vol 32 (9) ◽  
pp. 1145-1152 ◽  
Author(s):  
C. H. Lin ◽  
J. T. Lin ◽  
C. H. Chen ◽  
J. Y. Liu ◽  
Y. Y. Sun ◽  
...  

Abstract. This paper presents a two-dimensional structure of the shock wave signatures in ionospheric electron density resulting from a rocket transit using the rate of change of the total electron content (TEC) derived from ground-based GPS receivers around Japan and Taiwan for the first time. From the TEC maps constructed for the 2009 North Korea (NK) Taepodong-2 and 2013 South Korea (SK) Korea Space Launch Vehicle-II (KSLV-II) rocket launches, features of the V-shaped shock wave fronts in TEC perturbations are prominently seen. These fronts, with periods of 100–600 s, produced by the propulsive blasts of the rockets appear immediately and then propagate perpendicularly outward from the rocket trajectory with supersonic velocities between 800–1200 m s−1 for both events. Additionally, clear rocket exhaust depletions of TECs are seen along the trajectory and are deflected by the background thermospheric neutral wind. Twenty minutes after the rocket transits, delayed electron density perturbation waves propagating along the bow wave direction appear with phase velocities of 800–1200 m s−1. According to their propagation character, these delayed waves may be generated by rocket exhaust plumes at earlier rocket locations at lower altitudes.


2011 ◽  
Vol 54 (6) ◽  
pp. 737-746 ◽  
Author(s):  
Jing LIU ◽  
Wei-Xing WAN ◽  
Jian-Ping HUANG ◽  
Xue-Min ZHANG ◽  
Shu-Fan ZHAO ◽  
...  

2000 ◽  
Vol 18 (1) ◽  
pp. 56-64 ◽  
Author(s):  
A. J. Stocker ◽  
N. F. Arnold ◽  
T. B. Jones

Abstract. Characteristic signatures are often observed in HF radar range-time-intensity plots when travelling ionospheric disturbances (TIDs) are present. These signatures, in particular the variation of the F-region skip distance, have been synthesised using a ray tracing model. The magnitude of the skip variation is found to be a function of the peak electron density perturbation associated with the TID and radar frequency. Examination of experimental observations leads to an estimate of the peak electron density perturbation amplitude of around 25% for those TIDs observed by the CUTLASS radar system. The advantage of using the skip variation over the radar return amplitude as an indicator of density perturbation is also discussed. An example of a dual radar frequency experiment has been given. The investigation of the effect of radar frequency on the observations will aid the optimisation of future experiments..Key words. Ionosphere (auroral ionosphere; ionosphere -atmosphere interactions; ionospheric disturbances)


2000 ◽  
Author(s):  
Eiji Takahashi ◽  
Keisuke Katsura ◽  
Eisuke Miura ◽  
Noboru Yugami ◽  
Yasushi Nishida ◽  
...  

1996 ◽  
Vol 76 (19) ◽  
pp. 3566-3569 ◽  
Author(s):  
J. R. Marquès ◽  
J. P. Geindre ◽  
F. Amiranoff ◽  
P. Audebert ◽  
J. C. Gauthier ◽  
...  

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