|
|
|
BVA resonators are designed primarily to
minimize stresses due to the mounting structure and the instabilities due to
the electrodes (see “Stresses on a Quartz Resonator Plate” and subsequent
pages in the next chapter). The BVA2
structure shown above consists of three quartz plates of the same angles of
cut and azimuthal orientation. The
resonator plate is the plate “C” in the
center. The active part of plate C is
separated from the outer inactive part near the edges by means of cutouts,
and the active area is connected to the inactive area by means of small
quartz bridges. The outside plates D1
and D2 contact the C plate only outside the cutouts. The electrodes, deposited onto the center
areas of D1 and D2, are separated from the active area of the resonator by
means of small, 5m to 50 m, gaps.
|
|
The best resonator short term stability
measurements reported to date have been obtained with BVA resonators, i.e., sy(t) of parts in 1014
at the flicker floor (see chapter 4).
|
|
|
|
|
|
R. J. Besson, “A New
‘Electrodeless’ Resonator Design,” Proc. 31st Ann. Symp. on Frequency
Control,” pp. 147-152, 1977
|
|
|
|
R. J. Besson, J-J
Boy, M. M. Maurey, “BVA Resonators and Oscillators: A Review. Relation with
Space Requirements and Quartz Material Characterization,” Proc. 1995 IEEE
Int’l Frequency Control Symposium, pp. 590-599, 1995
|