Bulletin of the American Physical Society
77th Annual Gaseous Electronics Conference
Monday–Friday, September 30–October 4 2024; San Diego, California
Session HT4: Poster Session I (4:00pm-6:00pm)
4:00 PM,
Tuesday, October 1, 2024
Room: Gallery & Great Room 1-4
Abstract: HT4.00052 : Development of a wide bandwidth heterodyne dispersion interferometer for electron density measurement of atmospheric pressure plasmas*
Presenter:
Tomu H Hisakado
(General Atomics - San Diego)
Author:
Tomu H Hisakado
(General Atomics - San Diego)
Collaboration:
T. Hisakado1, T. Akiyama1, D. Vollmer1, A. Palmer1, K. Urabe2, and N. Shirai3
1General Atomics, San Diego, USA
2Kyoto University, Kyoto, Japan
3Hokkaido University, Hokkaido, Japan
A CO2 laser Heterodyne DI (HDI) is being developed to measure the dynamics of the electron density in atmospheric pressure plasmas (APPs) with a high temporal resolution. Laser based interferometry is a common tool for measurement of electron density in plasmas; however, for application to APPs, the phase shift caused by the plasma can often be masked by the large phase shift associated with changes in neutral gas density. A Dispersion Interferometer (DI), whose probe beam is a mixture of the fundamental and the second harmonic components of laser light, potentially overcomes this neutral gas effect. DIs inherently cancel a significant portion of the large phase shifts caused by neutral gas density as well as by mechanical vibration. As a result, DIs can measure the relatively small electron density induced phase shifts even in the presence of vibration and atmospheric conditions. To achieve the necessary bandwidth, a heterodyne approach, as first demonstrated on the DIII-D tokamak fusion device, has been implemented in a CO2 laser heterodyne dispersion interferometer. The HDI is targeted to measure APPs in an electron density range of 1020 to 1024 m-3 with a time resolution of 1 microsecond. The optical system is currently being optimized for APP measurements and the achievable density resolution is being characterized.
*This work is supported by US DOE Contract No. DE-SC0024435. This report was prepared as an account of work sponsored by an agency of the United States Government. Neither the United States Government nor any agency thereof, nor any of their employees, makes any warranty, express or implied, or assumes any legal liability or responsibility for the accuracy, completeness, or usefulness of any information, apparatus, product, or process disclosed, or represents that its use would not infringe privately owned rights. Reference herein to any specific commercial product, process, or service by trade name, trademark, manufacturer, or otherwise does not necessarily constitute or imply its endorsement, recommendation, or favoring by the United States Government or any agency thereof. The views and opinions of authors expressed herein do not necessarily state or reflect those of the United States Government or any agency thereof.
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