Concerning very loud needles, it is widely acknowledged that the "loud tone effect" descends from the improved thickness of the metal shaft of the needle, which is also shorter in some cases. This gives less flexibility to the groove-needle-diaphragm chain, hence the louder sound.
This makes sense (and is probably the actual reason) but leaves me puzzled concerning those super-loud needles that bear added masses. It may be conjectured that the body of the mass implicitly strengthens the needle's shaft just as in the case of a "thicker" needle, but I have to disagree with this. As it can be seen in drawings or actual images of these needles, the mass is very flattened and positioned towards the tip, as lower as it can go without scratching the record. There is then a negligible "reinforcement" effect on the shaft, if any:


Moreover, I recently came across a type of needle that I never saw before and that confirms that the effect is given preminently by the presence and position of the added mass. The latter is made with a wounded spring (as much as in a low-tone wounded piano string, and possibly with the same or similar machinery) which, being flexible by definition, can't add any stiffness to the needle's shaft:

I really can't understand on which principle this type of needles work. The only serious hypothesis I can conjecture is that the mass may induce a vibrational node point somewhere along the needle-diaphragm path, which in turn, perhaps for a local resonance point induced at the diaphragm, or for the generation of added harmonics, may have the effect of amplifying its vibrations.
Has any historical document, commercial paper or well written article surfaced lately, that can shed any light?