2009
DOI: 10.1088/0022-3727/42/13/135206
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Characterization of an N2flowing microwave post-discharge by OES spectroscopy and determination of absolute ground-state nitrogen atom densities by TALIF

Abstract: A flowing microwave post-discharge source sustained at 2.45 GHz in pure nitrogen has been investigated by optical emission spectroscopy (OES) and two-photon absorption laser-induced fluorescence (TALIF) spectroscopy. Variations of the optical emission along the post-discharge (near, pink and late afterglow) have been studied and the gas temperature has been determined. TALIF spectroscopy has been used in the late afterglow to determine the absolute ground-state nitrogen atomic densities using krypton as a refe… Show more

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Cited by 40 publications
(28 citation statements)
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“…In the particular case of O and CO species, two‐photon absorption LIF (TALIF) is among the most widespread techniques . TALIF is based on a simultaneous absorption of two photons with equal energy, resulting in excitation of the lower atomic (or molecular) state of interest (generally the ground state), which is followed by fluorescence towards a lower intermediate state, according to ITALIF=KnlILAS2ax, where K is a factor taking into account the laser excitation and detection geometry, n l the density of the lower state, I LAS the laser intensity, and a x is branching ratio of the observed fluorescence (including the absorption, collisional depopulation, and spontaneous emission coefficients). It is worth mentioning that two‐photon absorption cross sections are normally few orders of magnitude lower that those corresponding to absorption of a single photon.…”
Section: Experimental Setup and Optical Diagnostic Techniquesmentioning
confidence: 99%
“…In the particular case of O and CO species, two‐photon absorption LIF (TALIF) is among the most widespread techniques . TALIF is based on a simultaneous absorption of two photons with equal energy, resulting in excitation of the lower atomic (or molecular) state of interest (generally the ground state), which is followed by fluorescence towards a lower intermediate state, according to ITALIF=KnlILAS2ax, where K is a factor taking into account the laser excitation and detection geometry, n l the density of the lower state, I LAS the laser intensity, and a x is branching ratio of the observed fluorescence (including the absorption, collisional depopulation, and spontaneous emission coefficients). It is worth mentioning that two‐photon absorption cross sections are normally few orders of magnitude lower that those corresponding to absorption of a single photon.…”
Section: Experimental Setup and Optical Diagnostic Techniquesmentioning
confidence: 99%
“…This expected water contamination is discussed in the 3.1 Section. So far, the electronic features of the Nebulotron plasma setup have not been characterized yet but, as the volume of the plasma is much smaller than for the PAMPRE experiment, with a similar input power (30 W, Table 1), the temperature of neutral gases and the electron density in the Nebulotron setup are expected to be higher than in the PAMPRE plasma (Fridman, 2008, Es-Sebbar et al, 2009, Gries et al, 2009).…”
Section: The Nebulotron Experimentsmentioning
confidence: 99%
“…In the conditions described above for the DC discharge (nN(4S)=2.5±0.27 x 10 13 cm -3 ), the fs-TALIF signals measured inside the discharge yield a SNR746=17.5, SNR744=10, SNR742=5. This corresponds to a detection limit of ~ 10 12 cm -3 , two orders of magnitude lower than previously reported for ns-TALIF 16,17,22 .…”
Section: A Characterization Of the DC Dischargementioning
confidence: 59%