The main point I wanted to make is going to a 16 ohm driver from an 8 ohm driver doesn't necessarily mean you should scale crossover component values as one might expect.
I suggest working it out with Spice. When I did that a few years back, I found that the R1/R2/C1 network was all that should be changed, and in fact, only R1 and C1 was necessary. R2 stayed the same.
The issue is the loading of the splitter HP filter, the "core" of the crossover. Crossovers greater than first-order are very prone to peaking if the load impedance is increased. This is because the crossover acts like a tank circuit - the load impedance damps the filter, setting the Q of its resonance. As the load impedance is increased, the Q of the filter increases too.
This property of higher-order filters is used to our advantage in CD compensation. Without it, you couldn't make the initial flat shelf before starting 6dB/octave augmentation. Because of that, you can't make a filter that is the conjugate of CD power response using a core splitter that's first-order, it has to be second-order, third-order, or greater. This is fine, because higher-orders are good for other reasons too.
When you load the core filter with R1/R2/C1 as in my crossover, or with a similar network as in yours, this network sets the load. The compression driver is in shunt with that load, but is partially isolated with padding resistors. It's a higher impedance leg that doesn't drop the load impedance "seen" by the core filter very much. Consequently, it doesn't affect the crossover frequency or Q very much.
I don't know what work you guys have done to model your crossovers in Spice, or to measure physical models. I can see you've done some measurements, but wasn't sure how much experience you had with that, especially in regards to the value shift when going to a 16 ohm compression driver. I saw some discussion of scaling values like what is normally done on simpler networks, doubling inductance and halving capacitance. I wanted to point out that isn't the way to go, and to suggest instead that Spice models be used to find the values you needed. For illustration, I showed my crossovers because the work has been done there and because your crossovers are very similar. Their basic topology is the same.
One last thing. I've mentioned Spice a few times here. It was the main tool I used to develop my crossover many years ago. I would strongly suggest downloading and using it when contemplating changes to your crossovers too. You can download the models for my crossover and modify them for your values, if you wish. Spice is an excellent tool for this kind of thing.
You can even import your Spice models into Keith Larson's WTPro system, which will make a digital crossover for acoustic testing. This lets you change crossover component values by editing a Spice description file. You can then make acoustic measurements of a physical loudspeaker. The cool thing that buys you is the ability to do polar measurements and set your null angles on the fly. You can easily modify crossover values between each measurement, trying new configurations in seconds. When you're trying to optimize a speaker not only in axial response but also off-axial, this kind of test/modify/re-test cycle is really great. It is probably the best rapid prototyping tool I've ever used, extremely helpful for optimizing the crossover.