Microscopic mechanism that initiates vacuum RF breakdown on copper · revision history
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Accepted · first revision · record
- Title
- Microscopic mechanism that initiates vacuum RF breakdown on copper
- Plain
- Breakdowns start at small spots on a polished copper surface, but which process lights the spark (electrons pulled out by the field, crystal defects moving to the surface, local melting) is not agreed.
- Precise
- In Cu accelerating structures at 3-30 GHz, breakdown occurs at surface fields $eE_{s} \sim 2-3\,\mathrm{MeV}/\mathrm{cm}$, and Fowler-Nordheim fits of dark current give field-enhancement factors $\beta \sim 30-100$ although no protrusions of matching height are observed. Identify the sequence of processes (dislocation-driven surface roughening, field-emission heating of emitters, neutral evaporation, plasma ignition) that turns an intact surface into an arc, with a model that predicts the threshold field and its dependence on hardness and crystal structure of the metal.
- Settled by
- In-situ imaging of breakdown sites before and after the event together with a model that reproduces measured thresholds for at least two metals of different crystal structure.
- Kind
- phenomenon
- Answer type
- mechanism
- References
- (empty)
- Literature status
- open
- Status note
- (empty)
- Posed since
- (empty)