even though I have been stating rather clearly that my comments were all unrelated to that, I'll now toss my hat into the ring.
There is a lot of truth to what Brian just said. It also quite obvious that an analysts of the data is subject to interpretation.
When comparing, yep, there is interpretation in comparing. I had really tried to avoid this. Just don't get bent out of shape if I don't agree fully with yours.
I have no issue with the spectral decay posted by John. It's his comments that I find objectionable especially in light of his attitude and his mission against those with subjective analysts (listeners).
I still refuse to get dragged into this part of it. That's between you and John.
Looking at the spectral decay of the M-130, I have to say that it looks great. It looks far better than the vast majority of available woofers. Any resonances or breakup in the top end is well controlled and dies very quickly. You can pick it if you like, but it looks good. Even my competitor that has hated my guts for years came on here and said it looks good.
Yep, it looks pretty good, I've not said it wasn't. In fact, I also tried really hard to do any detailed analysis of the measurements. It's not a full set of them, but we'll have to work with what we have.
So let's look at what John posted. Here are the three woofers that were compared.



The M-130 is the one in the middle.
Looking at the group I'd have to say that they all look very good. Resonances across the board are fairly minor and above the range in which they would be used.
OK, I can agree that far. It does not address the distortion amplification by the breakup for any motor-generated distortion. This, many may not realize, is not controllable whatsoever by the crossover unless it's to reduce the excursion at the low end by using it purely as a midrange so the motor distortion stays low. If it's used in a 2-way, what is there will remain there. It won't matter how low or what order lowpass is used. The motor generated distortion will get through. Any breakup or peaks will amplify the harmonics that coincide with them. This is a fact of the physics.
With that in mind, let's continue.
If I were to pick one with the cleanest spectral decay it would have to be the M-130 by a small margin. The other two have slightly more stored energy in the 4 to 6kHz region and have some slightly longer decay rates. I'd still say that they were good overall. Comparing them to other woofers measured by John I'd say that all three of them were just about as good as any. All good !!!
I have to differ completely, for two reasons. The peak in the M-130 is the highest magnitude as well as the highest Q. Passive crossover limitations make its control more problematic, unless a fairly low Fc or higher order is used with any slightly higher Fc. This makes it the most difficult to control vs. the other two. So for purposes of a crossover, the M-130 comes in third. I might call it a close third, but third it is as I see it.
Now let's look at what John had to say.
About the M-130 (the cleanest of the three): "Breakup node at 5.5kHz with energy storage problem."
Of the other two: "Has smooth breakup node at 8kHz, but does not have serious energy storage" and "Tiny breakup node at 5kHz without much ringing"
I really wanted to avoid all of this, but I can't seem to. OK, considering my first point about the XO and the higher Q, I guess I actually have to agree with him. I've seen far worse, but we're only considering the other two presented in this comparison. Again, it comes down the Q and magnitude. John is spot-on now that I've looked more carefully at the other two.
The cleanest one of the three has a "breakup node at 5.5khz and an energy storage problem" but the other two that had a slightly longer decay time in that range had a "smooth breakup node", "does not have serious energy storage", and "Tiny breakup node at 5kHz without much ringing"?
Once the XO is added, the decay rate is no longer an issue. As John K pointed out some time ago, if you design a XO that traps the peak such a match to a target is achieved, the system decay is simply that of the target. That is, if you can trap a peak and get a good LR2 or LR4, then the system response will be that of an LR2 or LR4. The end result is that if a peak of whatever source, be it breakup or other resonance, is difficult to control to allow a match to a target, it's more of a problem than one that is easier to handle. High Q, high magnitude traps are more problematic when done passively. So this in essence makes the driver a little more limited in application. Not that it's bad, just more limited. Just look at metal cones. They exhibit this, only worse. It doesn't stop Linkwitz from using them. But it takes more care, meaning it's more difficult to do well.
Are you kidding me? Do you really think that this is unbiased driver testing? Or is this something else? Do you understand now. Do you see the obvious?
Obvious? Now that I look closer, no, I don't see what you're implying. Point-by-point I'm starting to agree with John.
Now you have to add the fact that the impact of the motor-generated distortion is out of the hands of the XO designer in a 2-way unless a small closed box is used to limit excursion. All three should have some form of added higher order distortion in their respective peaks areas. The only way to compare that is to make distortion measurements. That is more subject to interpretation since we seldom get to see a large set of test data. Even Linkwitz will point out that his distortion measurements are selective due to the difficulty and time-consuming nature of this testing.
I'm not factoring cost in at all. Yours may still be the best bang-for-the-buck of the three, I don't know. That's a big subjective discussion I will not get dragged into.
Actually, now that I look carefully, John looks to be more objective than I had been lead to believe, at least in reading the quotes supplied here. His abrasive comments and email don't enter into what I see in the drivers.
You pressed me into it. I have to call it as I see it.