Unfortunately that approach degrades the phase noise floor due to crystal 
dissipation limitations as well as degrading the phase  noise in the flicker 
region due to the crystal itself,Not only is a clean (harmonic and subharmonic 
free) sine wave desirable so is  low phase noise.Thermal drift of the crystal 
filter phase shift will also be problematic.Cascaded low Q filters suffer less 
from this  than a single high Q filter.
A low pass filter combined with series resonant shunt traps will have fewer 
issues with phase instability at 10MHz than using a 10MHz bandpass filter.

Bruce
 

     On Wednesday, 4 February 2015 9:53 AM, "Fuqua, Bill L" <wlfuq...@uky.edu> 
wrote:
   

   Push-Push Jfet amplifier with parallel inputs and a  Toroid output 
transformer, no secondary along with a
simple filter using a 10 MHz series resonate crystal connected to one drain and 
an adjustable capacitor connected
to the other would work fine. You connect the other ends of the two together 
and a loading resistor to ground.
  The capacitor is used to neutralize or null out the shunt capacitance of the 
crystal so that a capacitive path 
for the other frequencies , 5, 15, 20, etc is eliminated. Then follow up with 
your linear class A amplifier.
  The loading on the output of the crystal filter will determine it's Q and is 
not real critical, but should be
perhaps around 10-100 times the series resistance of the crystal. Since most 
readily available crystals
are not exactly on frequency a lower Q, higher R would be desired, but that 
will not greatly affect the 
5 MHz or undesired harmonic attenuation.  Perhaps one or two kHz bandpass would 
be just about right.
 Just don't overdrive the crystal. Also, for the price of $1 or less you may 
get 10 or so for further experimentation.
This combination of doubler and crystal filter should provide a very nice 
sinewave output
73
Bill wa4lav
 
 
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