What about doing the same as with a car motor? Make the mount softer so that the resonance is at much lower rpm.
This is the germ of a good idea (in terms of passive methods) but there are two other variables at play, and varying just one is as likely to hinder as help!
Namely, mass and damping. We can draw an equivalent circuit with inductance, capacitance and resistance in terms of spring constant, mass and dashpot. When the ratio sqrt(L/C) = R, it's critically damped. Moreover, the amplitude of displacement (amount it shakes) will be proportional to that times the applied force (i.e., the mechanical impedance, and Ohm's law).
So, just making the spring weaker, lowers the frequency, but also increases the amplitude at that frequency. The force may be lower too (we're dealing with an unbalanced load, so the force is proportional to the unbalanced mass times frequency), which would be a wash. Essentially the damping is a ratio of masses (unbalanced to sprung mass), so the only thing you can really do is increase mass.
Damping is a little harder to do -- in mechanics, we are flush with reactances (masses and springs), and resistance is kind of hard to come by. Typically we have lossy materials and viscous fluids that mix a bit of both.
Examples:
- Rubber shock dampers: really more springy than lossy, but at least having a fairly low Q -- much like ferrite beads.
- Acoustic absorbers, damping mats, etc.: dissipates free waves, or flexing or stretching energy, in a dense yet porous matrix that has significant viscosity or friction (squishy rubber, fibrous materials), or traps a fluid which does (the gas inside open-cell foam or fibrous materials).
- Dashpots, shocks: viscous loss in a fluid, usually a restricted range of motion (like linear or rotating motion, not free motion or wave energy).
The other drawback is, the range of densities and elasticities isn't all that great, so we can rarely absorb/reflect/filter vibration in a single stage, or even two stages; a stack of alternating high-density and high-elastic materials is needed to act as a lowpass filter (a distributed one at that, because it's very easy to get into acoustic modes -- a consequence of the relatively low speed of sound in materials).
Which is to say: if you can't dampen the oscillation by resistance, or brute-force mass, you may have to let it be, and add springs to isolate that motion from the rest of the rig, which in turn has some mass which the springs work against; and the whole suspension needs to be well damped so it doesn't get super bouncy at some (even lower) frequency.
As for active means -- anywhere you can attach a transducer, you can apply cancellation of some sort. But doing it at such high frequencies may not be easy. There are many degrees of freedom. Just for an unbalanced load: you could use a subwoofer / mass driver to cancel linear motion in one direction -- but you need a pair to oppose both axes. And that's if the rotational axis is fixed and known. You need three in general, but even worse than that, you probably need six (in balanced pairs) to ensure you aren't making a rotating moment instead of a linear displacement! And now you have a six channel controller with interactions between all channels and some kind of transfer function or control program to run it, and... yeah, it quickly gets complicated.

Personally, I prefer to stick to electrical circuits, where I can place a (one dimensional) transmission line, more-or-less wherever I please, as opposed to a dozen propagation modes in every solid...

Tim