TY - JOUR
T1 - Influence of VUV illumination on breakdown mechanics
T2 - Pre-ionization, direct photoionization, and discharge initiation
AU - Stephens, J.
AU - Fierro, A.
AU - Dickens, J.
AU - Neuber, A.
PY - 2014/8/13
Y1 - 2014/8/13
N2 - A microdischarge (MD) vacuum ultraviolet (VUV) light source is fired onto a N2-NO (99.92 : 0.08%) target gas. The minor gas constituent, NO, was chosen for its ionization potential (9.23eV) and photoionization cross-section (1.410-18cm2) at the wavelength of interest (121.6nm, 10.2eV). The result is a plasma generated entirely by volume photoionization in a N2-NO background. Using a very low electric field amplitude, charge carriers are drifted though the photoplasma at picoampere levels, serving as a non-invasive diagnostic. Using a simple one-dimensional fluid approximation for the low electric field condition, theoretical predictions of photoplasma current were found to be in meaningful agreement with experimental data. The impact of direct photoionization and pre-ionization on nanosecond timescale high voltage breakdown yielded two primary observations: (1) a significant reduction in the formative delay time necessary for spark formation, and (2) almost complete elimination of the statistical delay time. Again utilizing one-dimensional fluid approximations, reasonable agreement between experimental and simulated breakdown voltage was observed. Utilizing the same VUV source to illuminate a HV spark gap biased to about 95% self-breakdown voltage revealed that direct volume photoionization alone was insufficient to trigger breakdown of the high voltage gap. However, permitting electrode illumination, the same source was found to be capable of triggering breakdown in the undervoltaged gap, albeit with a large temporal jitter.
AB - A microdischarge (MD) vacuum ultraviolet (VUV) light source is fired onto a N2-NO (99.92 : 0.08%) target gas. The minor gas constituent, NO, was chosen for its ionization potential (9.23eV) and photoionization cross-section (1.410-18cm2) at the wavelength of interest (121.6nm, 10.2eV). The result is a plasma generated entirely by volume photoionization in a N2-NO background. Using a very low electric field amplitude, charge carriers are drifted though the photoplasma at picoampere levels, serving as a non-invasive diagnostic. Using a simple one-dimensional fluid approximation for the low electric field condition, theoretical predictions of photoplasma current were found to be in meaningful agreement with experimental data. The impact of direct photoionization and pre-ionization on nanosecond timescale high voltage breakdown yielded two primary observations: (1) a significant reduction in the formative delay time necessary for spark formation, and (2) almost complete elimination of the statistical delay time. Again utilizing one-dimensional fluid approximations, reasonable agreement between experimental and simulated breakdown voltage was observed. Utilizing the same VUV source to illuminate a HV spark gap biased to about 95% self-breakdown voltage revealed that direct volume photoionization alone was insufficient to trigger breakdown of the high voltage gap. However, permitting electrode illumination, the same source was found to be capable of triggering breakdown in the undervoltaged gap, albeit with a large temporal jitter.
KW - breakdown
KW - gas discharge
KW - microdischarge
KW - photoionization
KW - vacuum ultraviolet
UR - http://www.scopus.com/inward/record.url?scp=84904694796&partnerID=8YFLogxK
U2 - 10.1088/0022-3727/47/32/325501
DO - 10.1088/0022-3727/47/32/325501
M3 - Article
AN - SCOPUS:84904694796
SN - 0022-3727
VL - 47
SP - 325501
JO - Journal of Physics D: Applied Physics
JF - Journal of Physics D: Applied Physics
IS - 32
M1 - 325501
ER -