I don't believe this for one second. Think about this... a raw waveform of a squarewave of say 300Hz with raw input would show an emphasis of about 20dB at around 3kHz ? That would mean an overshoot of 10x the amplitude of the 300Hz would be seen. It would in no way even resemble a squarewave at all and the plots do look like squarwaves but with excessive ringing in time and amplitude. In his plots the overshoot/ringing however one looks at it is no more than 6dB so must have been the 'compensated' signal. As the compensation is incorrect the waveform will also be incorrect.
My plot also isn't EQ'ed but is corrected. The electrical output of my rig does not need additional 'compensations' it is built in hardware in the pre-amp.
Maybe you meant something else but that's the way my simple engineering/measurement mind sees it. Not from an academic level.
Can you post a plot of the raw output from a HATS where a squarewave was the input via a headphone ? We may be looking at this from too different angles. I would like to see a 'raw' squarewave from a HATS.
The raw response of the HD600 at 3khz on Tyll's plots was roundabouts of 12-14dB above 300hz (-14~ to -26~):
The relative amplitude of the peak value of his 300hz square wave and the "shelf" of the real square is about .02 to .005 (12dB).
This doesn't seem in strong contrast to me, but perhaps I'm missing something.
Regardless, here's my HD600 in its raw form and with an EQ viewed in frequency response:
And in square waves:
My apologies for the lack of time alignment - I don't deal with ARTA's square wave outputs usually, but they appear to be from its actual time record, so differences in delay due to the EQ being on or off would need to be compensated either with a delaying filter on the "no EQ" measurement or by hand, and it is late and I am lazy. Ehhh it would have bugged me too much. Fixed.
Edit: And now in
smell-o-vision zoomed in scale:
Edit 2: I didn't record this, but much as with multitones, the FFT of a square wave gives a (very limited) approximation of frequency response, in cases where its variation in the band of early harmonics is so extreme that it is more significant than the typical falling amplitude as a function of order.