Thanks for the comment, Dr. Gilmore, that's a very good point. One thing about the cascode CCS (constant current source) on my SRX Plus (modded SRX) is the output voltage drifts about 40-50 volts as it warms up, also the final value may vary by a few volts with different turn-on/turn-off cycles, presumably due to thermal issues. Thermal stability is very significant for practical amplifiers.
In terms of the LL, my copy of the prototype schematic courtesy of Dewey, Cheatem and Howe , uses the same topology as figure 3A discussed in my previous post, but substitutes a MOSFET for a BJT as the device that has the large voltage swings in the output CCS. Here is what Jung has to say a few paragraphs earlier in his introductory remarks in the section discussing the one VBE current source shown in figure 3A:
"Of course, higher-voltage parts should be used when appropriate. While exotic and super-high-gain parts aren't necessary for very good performance from these circuits, LOW CAPACITANCE DEVICES DEFINITELY ARE PREFERRED (<10pf), A CRITICAL POINT IF SUBSTITUTING [emphasis added]."
The reason is that high capacitance devices cause the effective impedance to decrease at high frequencies, degrading the performance of the current source. Given that MOSFETs have a relatively high shunt capacitance, this means that performance of the LL output current source is likely to be even worse than the BJT version that Jung cited as a design to avoid. Now the "fixed" version of the LL uses a low-capacitance BJT for the MOSFET, which is better, but.... the SRM323, which shares a very similar topology, uses the LED and BJT CCS on the output, which is significantly better than the CCS of the "fixed LL." You can't say that Dr. Gilmore and spritzer didn't warn us about this when the LL came out, although they didn't go into it in the infinite gory detail that I just did.
Now, one of the advantages of a cascode MOSFET CCS such as the SRX Plus uses, is that the upper device shields the lower device from voltage variations, so that the lower device, which sets the current, sees nearly constant voltage regardless of the voltage variations across the cascode pair. This means that the effective capacitance of the cascode is very low, so its performance is preserved to high frequencies. For example, Pimm measured a cascode DN2540 pair as having an effective capacitance of < 0.2 pf! By comparison a single DN2540 measured about 32 pf.
ADDENDUM:
I got a look at the production schematic courtesy of spritzer's LL Mk I thread elsewhere on this site. The output current source is identical to the Dewey, Cheatem and Howe version with the exception of a protection zener added to the MOSFET in the production version, so same lousy performance.