I'm new here, so please be gentle...
I've been experimenting with adding an active output stage to my Oktava ML52. I replaced the original transformer with a Jensen JT-34K, which was a major improvement all by itself. I used an Analog Devices AD797 for the active stage. The AD797 is (in Analog's words) an ultra-low-noise, ultra-low-distortion op amp. In general, I've been pleased with the results, though I'm still in experimentation mode.
Some comments based on my experience with this project:
Noise is an overriding concern. Each element in the signal chain affects the noise characteristics of the system, often by interacting with other elements in non-obvious ways. For example, noise optimization for an amplifier like the AN797 consists of balancing voltage noise, current noise, and thermal noise of resistances at the input. The thermal noise is determined (mostly) by resistors in the feedback loop, which also determine gain and input impedance. The gain and input impedance requirements are, in turn, strongly influenced by the characteristics of chosen transformer. All of these things are interdependent, and the relationships can be convoluted. Finding a configuration for optimal (or approximately optimal) performance is a complex problem, enough so that simple rules of thumb about higher turns ratios or higher impedance loads being better can be misleading.
Regarding transformer choice--as mentioned above, the choice of transformer is highly interrelated with other design choices. An earlier post mentioned wisdom from the Royer web site that higher turns ratios are perferred for active ribbon mics. Although I'm reluctant to take issue with the guys at Royer, my own experience is somewhat to the contrary. High-performance audio transformers with high turns ratios are harder to design and build (and thus, more expensive or lower performance) than those with lower turns ratios. One of the advantages of an active ribbon design is that you can use a transformer with a lower turns ratio and either save money or get higher performance, or possibly both. You can make up for the loss in gain with the amplifier, as long as you have noise under control. The JT-34K has a turns ratio of 1:37, which is relatively high. Assuming a ribbon impedance of 1 ohm, the output impedance is about 1.4K ohms. The AD797 has optimum noise performance with input impedances under 1K, best around 500 to 600 ohms. When I can afford it, I want to get a JT-347, with a turns ratio of 1:24. With a 1 ohm ribbon, its output impedance is just less than 600 ohms. Also, its overall performance is significantly better than the JT-34K--lower distortion, higher levels, and flatter frequency response. [Note: the JT-347 is considerably more expensive that the JT-34K, which would seem to contradict my earlier statement. The JT-347 is a much larger, much higher performance transformer than the 34K. I haven't found a transformer with a higher turns ratio that comes close to its specified performance.]
Regarding amplifier--I know that many people prefer discrete designs to integrated op-amps, but I don't share this bias. For this application in particular, even an excellent circuit designer would be hard-pressed to design an amp with better performance than the AN797. Its input noise characteristics are better than most discrete low-noise devices, and it's overall performance as an amp (e.g., THD, gain bandwith product, slew rate) is stellar. The Linear Technologies LT1028 looks like a good alternative candidate. There are, no doubt, others. One drawback: the AD797 requires more current than standard P48 phantom power can supply. A production microphone would require special cabling and an outboard power supply, like older tube mics.
It's also probably worth mentioning that, while the JT-34K can fit (just barely) into the bottom can of the Oktava, there isn't any room left for an active stage, so I've had to use a makeshift enclosure for prototyping. The JT-347 will definitely NOT fit into the Oktava can.
Regarding transformer ringing (mentioned in an earlier post)--with high turns ratio transformers, the inter-winding capacitance in the secondary can be sufficiently high that it forms a self-resonant LC circuit. This resonance can be damped with an RC network across the outputs of the secondary. The Jensen datasheets include information on how to do this, what values to use, etc. This is another case where variations in loading the output of the ribbon/transformer can have a big effect. All the more reason to use a built-in active circuit to optimize the loading and isolate it from the down-stream mic pre.
--Da5id