2015
DOI: 10.1016/j.jksus.2015.02.008
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Design and construction of prototype transversely excited atmospheric (TEA) nitrogen laser energized by a high voltage electrical discharge

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Cited by 5 publications
(12 citation statements)
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“…The amplitude decreases and falls to zero within 0.5 ms; then maximum amplitude achieved after 6.5 ms which falls again to zero after 0.5 ms as shown in Fig.9.At the highestamplitudeof voltage waveform, the potential difference across the transmission line is maximum, consequently strong electric fieldcreated across the Blumlein transmission line.Subsequently, when the amplitude falls, the strength of electric field decreases across the Blumlein transmission line, so as potential difference as well. Such behavior of voltage in the Blumlein transmission line practically generates the coherent ultraviolet pulses in the air in the form of TEA Nitrogen Laser as reported [8][9][10][11]13]. The simulated voltage waveform variation across the Blumlein transmission lineshown in Fig.…”
Section: Simulation Of Pulsed High Voltage DC Source and Blumlein Tramentioning
confidence: 75%
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“…The amplitude decreases and falls to zero within 0.5 ms; then maximum amplitude achieved after 6.5 ms which falls again to zero after 0.5 ms as shown in Fig.9.At the highestamplitudeof voltage waveform, the potential difference across the transmission line is maximum, consequently strong electric fieldcreated across the Blumlein transmission line.Subsequently, when the amplitude falls, the strength of electric field decreases across the Blumlein transmission line, so as potential difference as well. Such behavior of voltage in the Blumlein transmission line practically generates the coherent ultraviolet pulses in the air in the form of TEA Nitrogen Laser as reported [8][9][10][11]13]. The simulated voltage waveform variation across the Blumlein transmission lineshown in Fig.…”
Section: Simulation Of Pulsed High Voltage DC Source and Blumlein Tramentioning
confidence: 75%
“…Further applications, thinfilm deposition for non-linear optical purposes [5],Te-doped Ge-Se thin films crystallization [6], andcategorization of change in phase of chalcogenide thin films [7]. The development and optimization of TEA nitrogen laser based on the Blumlein circuit [8], time-dependent inductance and resistance of free running spark gap of Blumlein based nitrogen laser for various resistive phase periods described [9,10]. The oscillatory behavior of power, current and the voltage across the laser discharge channel has observed [9].…”
Section: Introductionmentioning
confidence: 99%
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“…In Blumlein, the discharge in the laser tube reaches to the peak value of V0(Applied voltage) whereas in C-to-C the voltage is reached to only H. Golnabi and A. Ashrafi in 1994 also studied the electrical properties of nitrogen laser constructed using Blumlein and C-to-C discharge circuits and concluded that Blumlein is more efficient [3]. Blumlein discharge circuit is employed to generate nitrogen laser at 0 to 5 bar pressure [4], and transversally electrical excitation at atmospheric (TEA) pressure nitrogen laser was reported [5,6,7,8]. Adolf J. Schwab in 1976 [9] presented the design of nitrogen laser using Blumlein discharge with the efficiency of 0.2-0.4% which is far better than that produced from C-to-C discharge system by K.A.…”
Section: Introductionmentioning
confidence: 99%