@pindac
Prove this wrong - Weight of overall structure and an assembly of enabling parts that is compatible with commonly used geometry for Cartridge Set Up, is all that is required to get the optimal performance from a modern design Optical Read Cartridge
DS Audio optical cartridges in many ways are similar to conventional MM and MC cartridges. They all have a stylus, cantilever and armature, which should be familiar to any audiophile. They share the same geometry for ideal set up, requiring the stylus rake angle, vertical tracking force, azimuth, zenith and vertical and horizontal tracking angles to be optimised. DS Audio cartridge weights are remarkably similar: 7.7, 7.7, 7.9, 7.9, 7.7 and 7.7 grams from the top down in my list posted above. The difference is probably paint! Optimal tracking force is 2.1 grams for all current DS Audio cartridges.
The same sorts of styli trace the recorded groove as conventional cartridges. A major consideration here is the effective tip mass measured at the stylus. The best tracking requires the lowest tip mass, which can accelerate the fastest to "hug the groove". Anything added to the basic stylus / cantilever / armature adversely affects the trackability. In LOMC designs, the ART1000 goes to extremes to minimise the added mass, with two tiny coils mounted just above the stylus. Current DS Audio cartridges add two 'sails' of extremely light beryllium on the cantilever just behind the stylus. Most MM and MC designs have relatively massive magnets and coils at the other end of the armature.
The idea of Diamond - Boron - Aluminium having an influence on the Optical Read makes no sense to myself, how are shadows being read influenced for the better by different materials used as the conduit for energy transfer?
The shape of the stylus is important in DS Audio optical cartridges, like in any cartridge. Probably of equal importance is the mass and rigidity of the cantilever. Lithium, beryllium and boron are the lightest metals, with aluminium about twice as dense as boron. Lithium is highly reactive, and beryllium is brittle and toxic.
The real question is how quickly does the position of the beryllium shades change in response to groove modulation.
Carbon is just one up from boron in the periodic table, and in its diamond form, is the hardest naturally occurring substance known to man. Techniques for growing large diamonds from vapour have allowed DS Audio to grow a single diamond to form both the stylus and cantilever in its top model, Presumably this improves rigidity and reduces resonances.
Energy transfer from the stylus to magnet and coil structures is what drives the signal in conventional cartridges. The signal corresponds to the acceleration of the stylus.
Question - An Optical Sensor has zero similarity to an Analogue Sensor when it comes down to an Ambient Kinetic Energy transferring through the Structure that enables the sensors to function
With optical cartridges, there is no energy transferred from the stylus. Instead external power drives Light Emitting Diodes (infra red actually) and the signal is generated by photoelectric sensors, all housed in the cartridge body. The signal is dependent on the position of the beryllium shades, so a completely different equaliser stage is needed. Weight and geometry are far from the entire story!