Hi

As long as we are beating up on the poor old SC for mode issues:

We have an C mode ( = the one that normally gets used in a precision oscillator)

We have a B mode ( = the “thermometer” mode that gets used in some MCXO’s)

Hmmm …. why did they start with B … hmmm ….

Well yes indeed there *is* an A mode. For a given overtone it’s *above* the B 
mode.
Exactly why they are lettered high to low … at least they are in order.

Page 3-15 in:

Quartz Resonator & Oscillator Tutorial - Time and Frequency ...tf.nist.gov › 
sim › 2010_Seminar › vig3 
<https://www.google.com/url?sa=t&rct=j&q=&esrc=s&source=web&cd=2&ved=2ahUKEwiYxa7Z-vbnAhWJlnIEHaTSCAkQFjABegQIARAB&url=https%3A%2F%2Ftf.nist.gov%2Fsim%2F2010_Seminar%2Fvig3.ppt&usg=AOvVaw0LXXz8jKe0sNHtk3Cj18ok>

Gives a nice plot of how it fits in. Why mention it? Well it’s the answer to 
the next up
question “why is the oscillator passband so tight?” ( = you have to kill a very 
close mode just above
the 3rd OT C mode and a closer than you would think mode below it). 

Bob

> On Feb 29, 2020, at 6:30 AM, Bernd Neubig <[email protected]> wrote:
> 
> You are right. As I am usually stating in my crystal seminars: "You are 
> ordering a crystal with one particular frequency, but the manufacturer 
> supplies with the crystals free of charge a bunch of additional frequencies, 
> which are not mentioned on the marking."
> 
> There is a multitude of spurious in real crystals:
> 1. So-called an-harmonic spurious resonances, which are all above the desired 
> frequency. For plano-convex crystals, as the usual high-precision  overtone 
> crystals at 5 MHz or 10 MHz, there are two or three (at least) very strong 
> spuriii about 100 kHz ~ 200 kHz above. In poorly designed crystals these 
> modes could be as strong or even stronger than the main mode.
> 2. The other overtones including the fundamental mode with their an-harmonics 
> are also always present. Higher overtones usually have higher resistance than 
> the main mode, but the fundamental mode of a 3rd overtone could have a lower 
> resistance than the desired 3rd OT. The B-Mode is a temperature sensor mode 
> with -30 ppm/K f(T) slope
> 3. SC-cut crystals have a strong "B-mode only 9% above the main mode, which 
> has comparable or even lower resistance than the desired "C-mode".
> 4. And finally there are the higher overtones of the low frequency vibration 
> modes such as face-shear mode etc. Those can interfere with the main mode 
> within a small temperature interval and will cause frequency dips and 
> activity dips ("band breaks")
> 
> If you try to build an oscillator with overtone crystals you must always 
> include a kind of trap or other selective circuits to allow only the desired 
> overtone to work. For an oscillator using a SC-cut crystal you need to add 
> additional selectivity to avoid operation at (or jumping to) the B-mode. This 
> could be very tricky.
> 
> Best regards
> Bernd
> 
> 
> -----Ursprüngliche Nachricht-----
> Von: time-nuts [mailto:[email protected]] Im Auftrag von Dana 
> Whitlow
> Gesendet: Samstag, 29. Februar 2020 00:47
> 
> Many crystals possess spurious modes not terribly far from the desired Hi-Q 
> mode.
> Since the spurious mode(s) are lower Q, oscillation on one of these can build 
> up faster than oscillation in the desired mode, driving the sustaining 
> amplifier into compression before the desired oscillating mode really gets 
> going.  This will leave only the fastest-growing mode as the winner.  This is 
> not speculation- I've seen it happen.
> 
> My point is that just building an oscillator with an unknown crystal has no 
> assurance of running where  you really want it to, thus leading you astray.
> Discovering all these
> modes is a big part of the benefit of studying the crystal with a VNA or 
> similar instrument before building anything.  Forewarned is forearmed- you 
> then have a better chance of building an oscillator that does what you want 
> it to do.
> 
> Dana
> 
> 
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