International audienceThe time profile of the lasing signal at 391.4 nm emitted by a weakly ionized gas of nitrogen molecules at low pressure is measured under double excitation with intense femtosecond laser pulses at 800 nm. An abrupt decrease of the emission occurs at the time of arrival of the second pulse. It is explained by a transfer of population from ground to first excited ionic level and by a disruption of coherence, terminating the conditions for lasing in a V-scheme without population inversion
International audienceWe report on a spectral splitting effect of the cavity-less lasing emission of...
International audienceWe report on a spectral splitting effect of the cavity-less lasing emission of...
International audienceDelayed cavity-free forward lasing at the wavelengths of 391 and 428 nm was ob...
International audienceThe time profile of the lasing signal at 391.4 nm emitted by a weakly ionized ...
International audienceThe time profile of the lasing signal at 391.4 nm emitted by a weakly ionized ...
International audienceThe time profile of the lasing signal at 391.4 nm emitted by a weakly ionized ...
International audienceThe time profile of the lasing signal at 391.4 nm emitted by a weakly ionized ...
International audienceThe time profile of the lasing signal at 391.4 nm emitted by a weakly ionized ...
International audienceThe time profile of the lasing signal at 391.4 nm emitted by a weakly ionized ...
We attribute the mechanism of "lasing" action of nitrogen ions pumped by femtosecond IR pulses to a ...
We attribute the mechanism of "lasing" action of nitrogen ions pumped by femtosecond IR pulses to a ...
International audienceWe report on a spectral splitting effect of the cavity-less lasing emission of...
International audienceWe report on a spectral splitting effect of the cavity-less lasing emission of...
International audienceDelayed cavity-free forward lasing at the wavelengths of 391 and 428 nm was ob...
International audienceDelayed cavity-free forward lasing at the wavelengths of 391 and 428 nm was ob...
International audienceWe report on a spectral splitting effect of the cavity-less lasing emission of...
International audienceWe report on a spectral splitting effect of the cavity-less lasing emission of...
International audienceDelayed cavity-free forward lasing at the wavelengths of 391 and 428 nm was ob...
International audienceThe time profile of the lasing signal at 391.4 nm emitted by a weakly ionized ...
International audienceThe time profile of the lasing signal at 391.4 nm emitted by a weakly ionized ...
International audienceThe time profile of the lasing signal at 391.4 nm emitted by a weakly ionized ...
International audienceThe time profile of the lasing signal at 391.4 nm emitted by a weakly ionized ...
International audienceThe time profile of the lasing signal at 391.4 nm emitted by a weakly ionized ...
International audienceThe time profile of the lasing signal at 391.4 nm emitted by a weakly ionized ...
We attribute the mechanism of "lasing" action of nitrogen ions pumped by femtosecond IR pulses to a ...
We attribute the mechanism of "lasing" action of nitrogen ions pumped by femtosecond IR pulses to a ...
International audienceWe report on a spectral splitting effect of the cavity-less lasing emission of...
International audienceWe report on a spectral splitting effect of the cavity-less lasing emission of...
International audienceDelayed cavity-free forward lasing at the wavelengths of 391 and 428 nm was ob...
International audienceDelayed cavity-free forward lasing at the wavelengths of 391 and 428 nm was ob...
International audienceWe report on a spectral splitting effect of the cavity-less lasing emission of...
International audienceWe report on a spectral splitting effect of the cavity-less lasing emission of...
International audienceDelayed cavity-free forward lasing at the wavelengths of 391 and 428 nm was ob...