2020
DOI: 10.1002/ppap.202000020
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Solution to the perturbation of LIF measurements via photodissociation, OH measurement in atmospheric‐pressure multihollow DBD

Abstract: This study solves the problem of the invasivity of laser-induced fluorescence (LIF) measurements caused by photodissociation. It is shown with the example of OH LIF that the excess signal caused by laser-induced photodissociation can be distinguished from the true LIF signal of the naturally presented species by This is an open access article under the terms of the Creative Commons Attribution License, which permits use, distribution and reproduction in any medium, provided the original work is properly cited.

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Cited by 4 publications
(1 citation statement)
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“…The plasma was generated by a sinusoidal alternate-current (AC), high-voltage (HV) power source with an external signal of frequency ≈ 18 kHz. The operation of MSDBD plasma is possible at different ow rates from 0 to 50 litres per minute (L/min) in ambient air or various gases such as nitrogen, oxygen, argon, and pure water vapour [38][39][40][41][42]. The owing gas serves not only to blow the plasma out of the holes but also to cool the ceramic plate.…”
Section: Plasma Source and Treatment Of Seedsmentioning
confidence: 99%
“…The plasma was generated by a sinusoidal alternate-current (AC), high-voltage (HV) power source with an external signal of frequency ≈ 18 kHz. The operation of MSDBD plasma is possible at different ow rates from 0 to 50 litres per minute (L/min) in ambient air or various gases such as nitrogen, oxygen, argon, and pure water vapour [38][39][40][41][42]. The owing gas serves not only to blow the plasma out of the holes but also to cool the ceramic plate.…”
Section: Plasma Source and Treatment Of Seedsmentioning
confidence: 99%