DocumentCode :
1911941
Title :
Plasma column from laser filamentation in air as a virtual radio-frequency antenna
Author :
Point, G. ; Brelet, Y. ; Houard, Aurelien ; Carbonnel, J. ; Arantchouk, Leonid ; Prade, Bernard ; Andre, Yves-Bernard ; Mysyrowicz, A.
Author_Institution :
Lab. d´Opt. Appl., Ecole Polytech., Palaiseau, France
fYear :
2013
fDate :
12-16 May 2013
Firstpage :
1
Lastpage :
1
Abstract :
Summary form only given. Plasma antennas, where plasma replaces metal as the conducting element, have long been known and used [1]. However, most designs use low-pressure plasmas confined inside solid dielectric vessels. We experimentally demonstrated a functional plasma antenna in air, which brings about many advantages like tunability in a large frequency range (100 MHz-1 GHz), stealth when de-activated and quick reconfiguration capabilities [2]. This antenna is based on the low-density (ne ≈ 1016 cm-3) plasma column created by an ultrashort laser pulse (700 fs, 300 mJ @ 800 nm) undergoing filamentation in atmospheric air. However, such plasma has a very short lifetime (less than 1 ns). To deal with this problem, we used the filament to guide a high-voltage electric discharge generated by a compact Tesla coil (output voltage of 350 kV), extending the plasma lifetime to at least 100 ns [3]. Radio-frequency (RF) power was then injected in the plasma by means of an inductive coupler in the form of a hollow metallic cylindrical cavity, fed by a 35 W solid-state RF amplification chain. Radio emission was then detected by means of a remote patch antenna with a 100 MHz-1 GHz bandwidth (figure 1-(a)). As shown in the example given in figure 1-(b), when the coupler is excited at 990 MHz and no plasma is present, there is no signal observed at this frequency (black curve), whereas a clear emission peak appears when the laser guided discharge is generated (red curve). RF energy coupling in the plasma has consequently been achieved, which resulted in the plasma column behaving as an emitting antenna. It is worth to note that the emission level from a copper rod with a length similar to that of the plasma is approximately equal to four times the plasma signal strength, demonstrating the applicability of this technology in real situations.
Keywords :
antennas in plasma; copper; high-frequency discharges; plasma light propagation; plasma production by laser; Cu; RF energy coupling; atmospheric air; black curve; clear emission peak; compact Tesla coil; conducting element; copper rod; emission level; emitting antenna; energy 300 mJ; frequency 100 MHz to 1 GHz; frequency 990 MHz; functional plasma antenna; high-voltage electric discharge; hollow metallic cylindrical cavity; inductive coupler; laser filamentation; laser guided discharge; low-density plasma column; low-pressure plasma confinement; plasma lifetime; plasma signal strength; power 35 W; quick reconfiguration capabilities; radio emission; radio-frequency power; remote patch antenna; solid dielectric vessels; solid-state RF amplification chain; stealth; time 100 ns; time 700 fs; tunability; ultrashort laser pulse; virtual radio-frequency antenna; voltage 350 kV; wavelength 800 nm; Antennas; Coils; Couplers; Discharges (electric); Lasers; Plasmas; Radio frequency;
fLanguage :
English
Publisher :
ieee
Conference_Titel :
Lasers and Electro-Optics Europe (CLEO EUROPE/IQEC), 2013 Conference on and International Quantum Electronics Conference
Conference_Location :
Munich
Print_ISBN :
978-1-4799-0593-5
Type :
conf
DOI :
10.1109/CLEOE-IQEC.2013.6800823
Filename :
6800823
Link To Document :
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