With respect to efficiency using vacuum or mica capacitors:
In general, resonant coupling networks (e.g. simple L-C, tapped inductor, pi-networks, L-networks) are characterized by "unloaded Q" and "loaded Q" (after connecting load).
They are designed for a desired value of loaded Q from specified load impedance, and the unloaded Q includes parasitic resistive losses in the inductor(s) and capacitor(s).
The power loss from input to output depends on the ratio between unloaded Q and loaded Q, where higher unloaded Q gives lower loss to the loaded case, since the parasitic losses are lower.
Now, unless you use really crummy capacitors, the unloaded Q for a practical network will be dominated by the Q of the inductor(s), since decent capacitors have Q near 1000, while inductors are typically in the 100s.
(The Jennings vacuum capacitors have unmeasurably high Q, maybe 25,000; the CDE micas I cited above have Q around 2000 in their usable frequency range; and class-I ceramics in doorknob or other high-voltage packages are also > 1000.)
Therefore, you should concentrate on improving inductor Q if efficiency is critical.
I have seen reports that with large RF transmitting coils (air core), Q of 1000 is possible.