Can an opamp MM phono preamp be blamefree?

Ultima Thule - The design of this headshell , and the way it is mounted in the tonearm tube , is a source of additional resonances . It 's a good idea . But the manufacturing method is bad .
And again - this is a non - removable headshell . And this means that it is no longer possible to connect any other phono preamp to this turntable .
 
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@vsmusic you sound like a broken record. :-)
You 're putting on public display a very funny and flimsy headshell . It is mounted very illiterate . But you must really like it 😉 .
But I like to use good headshells .
And in the headshell that you showed - there are more disadvantages than advantages .
If you make such a headshell at the factory , then it should be like a good factory product ....
Nothing personal .
 
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If you are not into extremely low distortion and want to keep the load on the cartridge as small as possible, you could mount a dual JFET in the headshell. You then have one JFET per stereo channel that you connect with its gate to the cartridge, drain to the centre conductor of the cable, source to ground (cable shield and the other side of the cartridge).

On the other end of the cable, you put a RIAA-equalized transimpedance amplifier per stereo channel, designed to have a DC input voltage high enough to supply the JFET. For minimum distortion at only a small noise penalty, the JFET should be biased a little bit into the triode region.
Yamaha's HA-2 from 1979
https://audio-heritage.jp/YAMAHA/etc/ha-2.html

and HA-3 from 1982
https://audio-heritage.jp/YAMAHA/etc/ha-3.html

are both of this type (headshell-mounted JFETs). There is a general schematic on the HA-2 webpage.

Due to the super short wiring between cartridge and JFET, Yamaha judged that there was no need for any resistive termination at the JFET gates, therefore the input impedance of the HA-2 was specified as being "in excess of 1MΩ".

I subsequently heard that a key reason why Yamaha stopped using this technology in their follow-up phono stages was electric corrosion of the contact points, due to the tonearm leadwires having to supply DC power to the JFETs as well as handing the AC signal.
 
JFET buffers like Marcel described are built into essentially all electret microphone capsules, even very famous ones used for recording. For simple speech applications this is called "plug-in power". Signal voltage levels from an electret are likely comparable to or larger than a MM phono cartridge, so linearity can likely be made good enough. Scott Wurcer has published a lot of work on elaborated versions for DIYers.

Seems no real reason that plug-in power inputs couldn't be supplied along with conventional 47K inputs.

Electret phono cartridges like the MicroAcoustics have capsules loaded with a coupla-K Ohm resistors to differentiate the signal (to simulate the velocity response of magnetic cartridges) and reduce level (again, to simulate a MM).

All good fortune,
Chris
 
Yes I can see electrolytic corrosion being an issue given the pogo-pin style contact interface of most headshells - but that's really an argument for better connector tech to be used I think - even without DC there will be issues of contact reliability that could be fixed - say by taking a leaf from the SpeakOn style connector but dine in miniature.
 
The opamp U6 ("synthesized" input resistance amplifier) uses the current of the first cascade feedback divider. Will the input noise current of U6 add to a noise current of U3? There is another way - you can take a signal from the output of U3 and make a mirror frequency responce.

The noise current of U6 will have very little impact because of the low impedance driving U6 (namely R2), but its noise voltage contributes directly to the input noise voltage of the amplifier.

You can also add a FET op-amp connected as a voltage follower or voltage amplifier, just to drive U6.
 
For cartridges with inductances above about 250 mH, the overall RIAA- and A-weighted noise will still be less than without U6, with 47 kohm across the input. For lower cartridge inductances, it is the other way around.

The simplest way to reduce the effect of U6 on the noise voltage is to replace it with an ultralow voltage noise, ultrahigh current noise model.
 
When a semiconductor manufacturer makes an op-amp with a bipolar input stage with plenty of base contacts and a relatively high tail current, it will have a very low voltage noise as well as a relatively high current noise (due to shot noise and 1/f noise of the high base currents). The current noise will increase further when there is a base current compensation circuit added to it. For obvious reasons, these devices are usually marketed as ultralow voltage noise op-amps and not as ultrahigh current noise op-amps, but they are both.

For U6, ultralow voltage noise is desirable and ultrahigh current noise doesn't matter, as long as it stays below 5 pA/√Hz or so.
 
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LT1028 comes to mind here, with the bias compensation feature described as a nuisance by Douglas Self (but not in this context, IIRC).
And he is right, - a DC input bias compensation is not a compensation of not correlated input noise currents (for example - not correlated Ibase of Q1 4.5 uA and Icollector of Q7 4.5 uA inside LT1028\1128). compensated DC difference is 0, and AC non correlated currents "difference" is 1.41 times bigger.