Self-mode transition, oscillation and inverse hysteresis in ECR discharges
Source abstract
Abstract
Positive and negative feedback of microwave (MW) ECR (electron cyclotron resonance) discharges in cross magnetic field were manipulated by a three-stub coaxial tuner. Unstable ECR discharges in the positive feedback region, such as the self-mode transition between the ordinary (O)-wave mode and extraordinary (X) one, inverse hysteresis, and oscillation, were investigated using a time-resolved MW power meter, high speed camera, and thermocouple. In the positive feedback region, the self-O → X wave mode discharge transition can be driven under the “hot” wall condition, while the counterpart, namely the self-X → O wave mode transition, is observable for the “cold” wall; the inverse hysteresis and oscillation take place at low and moderate gas flow rates, respectively. The mechanism underlying the self-mode transitions and instabilities is the discharge shift due to the gas heating effect. For MW ECR discharges to become stable, as indicated in previous experiments, they should be mismatched in the negative feedback region.
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Research context
OpenAlex topics: Plasma Diagnostics and Applications · Electrostatic Discharge in Electronics · Plasma Applications and Diagnostics
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
Affiliations
School of Physics, Dalian University of Technology 1 , Dalian 16024, China
Bolun Middle School 2 , Dalian 16031, China
NAURA Technology Group Co., Ltd. 3 , Beijing 100176, China
Funding
National Natural Science Foundation of China · Open Funds for Science and Technology on Vacuum Technology and Physics Laboratory, Lanzhou Institute of Physics
References (34)
Show source-provided references
1. ECS Trans. · 2015 · 66 · 14310.1149/06604.0143ecst ↗
2. Jpn. J. Appl. Phys. · 2012 · 51 · 8S110.7567/jjap.51.08hd01 ↗
3. IEEE Trans. Plasma Sci. · 2020 · 48 · 361510.1109/tps.2020.3023732 ↗
4. Phys. Plasmas · 2022 · 29 · 12350610.1063/5.0119550 ↗
5. Phys. Plasmas · 2022 · 29 · 01350110.1063/5.0069638 ↗
6. Phys. Plasmas · 2014 · 21 · 09350210.1063/1.4894476 ↗
7. Trans. JSASS Aerosp. Tech. Jpn. · 2016 · 14 · 13110.2322/tastj.14.pb_131 ↗
8. Phys. Plasmas · 2021 · 28 · 03351010.1063/5.0033067 ↗
9. Plasma Sci. Technol. · 2021 · 23 · 08550610.1088/2058-6272/ac061a ↗
10. Phys. Plasmas · 2023 · 30 · 02350610.1063/5.0124834 ↗
11. J. Vac. Sci. Technol. A · 1990 · 8 · 289310.1116/1.576645 ↗
12. J. Vac. Sci. Technol. A · 1990 · 8 · 290910.1116/1.576648 ↗
13. J. Vac. Sci. Technol. A · 1990 · 8 · 371310.1116/1.576484 ↗
14. J. Vac. Sci. Technol. B · 1991 · 9 · 33910.1116/1.585572 ↗
15. Rev. Sci. Instrum. · 1992 · 63 · 254710.1063/1.1142884 ↗
16. J. Vac. Sci. Technol. A · 1993 · 11 · 288310.1116/1.578663 ↗
17. Rev. Sci. Instrum. · 1994 · 65 · 175310.1063/1.1144872 ↗
18. J. Appl. Phys. · 1997 · 81 · 283910.1063/1.363943 ↗
19. Pramana J. Phys. · 2000 · 54 · 76310.1007/s12043-000-0121-2 ↗
20. Surf. Coat. Technol. · 2000 · 131 · 1210.1016/s0257-8972(00)00771-4 ↗
21. J. Vac. Sci. Technol. A · 2001 · 19 · 244610.1116/1.1387053 ↗
22. Nucl. Instrum. Methods Phys. Res., Sect. A · 2014 · 741 · 9510.1016/j.nima.2013.12.054 ↗
23. Phys. Plasmas · 2008 · 15 · 06350610.1063/1.2931038 ↗
24. Phys. Plasmas · 2012 · 19 · 08350210.1063/1.4743012 ↗
25. See https://imagej.en.softonic.com for version 1.52v.
26. AIP Adv. · 2022 · 12 · 05532510.1063/5.0082813 ↗
27. Plasma Sources Sci. Technol. · 2010 · 19 · 01501110.1088/0963-0252/19/1/015011 ↗
28. Plasma Sources Sci. Technol. · 1995 · 4 · 33210.1088/0963-0252/4/3/002 ↗
29. J. Appl. Phys. · 2008 · 103 · 08330310.1063/1.2905213 ↗
30. Phys. Plasmas · 2022 · 29 · 08450310.1063/5.0107483 ↗
31. Appl. Phys. Lett. · 2014 · 105 · 05410210.1063/1.4892656 ↗
32. J. Vac. Sci. Technol. A · 2005 · 23 · 44010.1116/1.1875252 ↗
33. Appl. Phys. Lett. · 1993 · 62 · 203910.1063/1.109472 ↗
34. J. Phys. D: Appl. Phys. · 2008 · 41 · 03520810.1088/0022-3727/41/3/035208 ↗