"So does the measured or published spectrum of a real instrument have characteristic clues that indicate which peaks are best created by formants and which are best handled by the resonator block? Are you visually sorting out the fixed-frequency content that is specifically NOT harmonically related to the oscillator? Or is the RESON block set largely by ear after the formant peaks are roughed out?" - pitts8rh
Some violin papers differentiate between the "box" or "air" resonances of the enclosed body, and the remaining resonances of the soundboard, bridge, etc. The former are lower in frequency and more like formants, the latter higher and more densely spaced, and the decay rates of these two distinct groups are also different, giving a 2 stage decay when combined. In one paper they use 9 bandpass biquads below 1.4kHz and a waveguide mesh for the resonances above that, but they mention that fewer biquads can still produce a realistic violin sound. For the D-Lev we're limited to 8 2nd order state variable bandpass formants for the low end, and the resonator provides the top end resonances. Sometimes I stick the 8th formant up in the resonator range (~3kHz), which can help to brighten things up without getting too "zingy" sounding, as the resonator is apt to do when cranked on.
The resonator has it's own 4th order HPF at its input for these sorts of blending purposes. Placing the HPF at the input rather than the output obviously helps with overload, and since the system is linear (and if it is used in a linear fashion) it doesn't matter where we place these things. Varying the harmonic content of the input when synthesizing, say, a drum, can markedly influence the timbre. The "freq" knob controls the total digital delay, and so the macro spacing of the resonances in the spread, and the variability of the micro spacing can be messed with via the "tap" knob (which controls the ratio of main delay to all-pass delay), the "harm" knob (which controls the all-pass feedback), and to some degree the "reson" knob (which controls global feedback & LFP of it, and the phase of that since it is +/-).
For my analysis, I take the lowest octave and do an FFT over the whole thing with various bin sizes to roughly resolve the lower resonant peaks. I then look at the FFT of each note in succession, to see if the harmonics "roller coaster" over them and are therefore real (a one octave gliss - a slow motion chirp, actually - would be a much better stimulus to resolve the resonances). I dial them in to the D-Lev formant bank and do the rest by ear (a miracle hopefully occurs here). The phase of the crossover point can produce the dip you often see in the spectra (the resonator "xmix" knob is +/-), though this is less "scientific" when using the resonator to also do pseudo-stereo, as both phases are employed and the dip will therefore only exist in one channel. Simply not placing formants there can also produce a dip of sorts.
Also, violin resonances - and those of many other instruments - tend to be exponentially placed, and the resonator can only do variations on linear spacing. But using the resonator mainly for the high end seems to work OK, as the ear doesn't seem to be as discerning up there.