CatBus;372855 Wrote: 
> I really don't want to add to a thread that's based on such a
> fundamentally flawed assumption, but I do want to address this because
> I never want to give anyone the impression that I am personally
> attacking them, telling them what they can or cannot hear, etc.

This was not directed at anyone on this forum, or anyone specifically.
I talk to a number of industry folk on a daily basis, and
well...........we all were about as frustrated the same amount about
this subject. You would be surprised how often we hear this lodged
against all of us.

How I perceive (key word) how something sounds can not be quantified. I
can measure things that I think can explain it, but not always. THD can
easily be measured, and no one will dispute those results. But how it
is perceived by the listener can not. If you could, no one would listen
to tube amps. (I don't, so there!)

But let's move to jitter, which is the genesis of this. Let me explain
why I know (at least to my satisfaction) that I can. This might be
protracted, so bear with me.

When we first made D/A boxes, we were pleased with the results, but
something was not quite right. The initial test had a 50 cm or so coax
cable. Just for grins, we put in a 1 m cable. Huh, different. What if
we put a different one? Again, different. Not better, just different.

So what caused it?

We poked and piddled, talked to some industry buddies working on the
same type of product. All came to the same conclusion(s). Something did
not sound right, and cables changed that around. One buddy, who did not
have my background or education level, pointed out that you could
listen to the PLL pin on the RX chip, and hear a distorted version of
the music.

Huh. I designed PLLs. Why didn't I think of that first?

Anyway......guess what...............you could hear it!

Wow, what if I listen to it with various cables...........

What if I then measure it with various cables?

Moving ahead a few steps in the measuring process, we found that
everything affected that noise of the PLL pin. Cable length and
impedance, type of TX and RX circuit, you name it.

Not only could we measure it, relative to the "stock" configuration, we
could hear the difference. And it wasn't just me and the rest of the
gang at the shop. We found that *everyone* could hear the difference.
And not just at our shop, on our gear. At anyone's house, and on their
own gear. (OK, we had to stick our D/A in, but we used different
sources.)

So, to test out our latest theory, we made a special D/A box. We took
one input, and applied all of our tricks to it, and left the other one
stock. We schlepped it everywhere that we could. Everyone heard the
difference, and heard the exact same difference. No one, outside of
myself, had any idea what I had done, or what it was supposed to do.

I knew what I had done, and thought that I knew how it would affect the
sound, but all I can really do is speculate. It needed verification.

I was able to do 2 things:

1.) When the return loss on the system was down around -30 dB, there
were no further differences that could be reliably discerned. At this
point, all cables and what not all sounded the same.

2.)I could measure the effect on the jitter on the recovered clock. At
the levels mentioned above, it was not possible to pick out any
differences in the recovered clock's noise.

Mind you, this was before we made any attempt to reduce the jitter by
futzing with the PLL itself. -Even with the horrid amounts of jitter
still in the chain, any listener could hear the reduction of jitter.-

So, we may not have reached the level at which jitter can no longer be
heard, but we have found that even in the presence of large amounts of
jitter that slight reductions could be heard.

So, what was the next step? Build a secondary PLL. Get the jitter down
much lower. Making a unit that could switch back and forth was not
practical, so we took 2 identical units, and rigged one up with the
secondary PLL. With a jitter level that we could measure. And compare
it to the transport clock.

At this point, we found out that the transport clock was not adequate.
(We were shocked by how bad they were.) So, more futzing and measuring.
And listening.

Again, the lower we got the jitter, the better things sounded. Also,
the changes that we made were discernible by anyone. Until we got down
the point that we were running into the limits of our efforts. Yes, as
we got lower to the floor, it became harder to detect the differences.
Not everyone could hear the changes.

Having done this now for over 15 years, I can confidently say that the
jitter does need to be significantly lower than 100 pSec, for a 256 Fs
clock. We initially thought that would be good enough, but we continued
our research and were proven to be wrong. That really wasn't good
enough.

It is indeed important to point out that Gaussian noise affects on
jitter were not as detectable as the data-correlated jitter. So,
lowering the jitter at the transport end had less of an effect than on
the SPDIF end.

Unless the jitter on the transport on the transport was
data-correlated.............which is usually is. But that was easy to
fix: just get the clock out of the filter chip!

So, there you have it. A summary of 15+ years of measuring and
listening. We are confident that we established a level of jitter that
was not discernible. Not by industry pros, insiders, or members of a
secret society. Or folks "in the know" what we were up to. Just the
average Joe who bought high-end gear. No knowledge of what we did, why
we did it, or why it should matter.

All they wanted to know was if I could do that to their gear.

Depended on whether they were worried about the resale value of their
gear. And my unwillingness to even try. I had other stuff I wanted to
do.

Like strap on the ol' feed bag. Later.

Pat


-- 
ar-t

http://www.analogresearch-technology.net
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