Hollow cathode effect
The hollow cathode effect allows electrical conduction at a lower voltage or with more current in a cold-cathode gas-discharge lamp than a similar lamp with a flat cathode.[1] The hollow cathode effect was recognized by Friedrich Paschen in 1916.[2]
A hollow cathode is constructed from a conductive tube, open at one end. The electron emitting surface is in the inside of the tube. Several processes contribute to enhanced performance of a hollow cathode:
- The pendulum effect, where an electron oscillates back and forth in the tube, creating secondary electrons along the way
- The photoionization effect, where photons emitted in the tube cause further ionization
- Stepwise ionization[1]
- Sputtering[3][4]
The hollow cathode effect is utilized in the electrodes for neon signs, in hollow-cathode lamps, and more.
References
- 1 2 Eichhorn, H.; Schoenbach, K. H.; Tessnow, T. (1993). "Paschen’s law for a hollow cathode discharge" (PDF). Applied Physics Letters. 63 (18): 2481–2483. ISSN 0003-6951. doi:10.1063/1.110455. Retrieved June 5, 2017.
- ↑ Paschen, F. (1916). "Bohrs Heliumlinien". Annalen der Physik. 355 (16): 901–940. ISSN 0003-3804. doi:10.1002/andp.19163551603.
- ↑ Bartlow, Robert B.; Griffin, Steven T.; Williams, J. C. (2002). "Axial evolution of the negative glow in a hollow cathode discharge". Analytical Chemistry. 64 (22): 2751–2757. ISSN 0003-2700. doi:10.1021/ac00046a017.
- ↑ Mavrodineanu, R. (1984). "Hollow Cathode Discharges - Analytical Applications" (PDF). Journal of Research of the National Bureau of Standards. 89 (2): 143. ISSN 0160-1741. doi:10.6028/jres.089.009. Retrieved June 14, 2017.
This article is issued from
Wikipedia.
The text is licensed under Creative Commons - Attribution - Sharealike.
Additional terms may apply for the media files.