The motor has four shaded poles, so it is not quite synchronous, instead slipping slightly with the braking effect and stylus drag. Personally I think stylus drag is tiny compared to the eddy current brake, which could explain why these decks are valued for their ’drive’ when playing heavily modulated passages.
I’ve seen this rationale applied before in the past and it is counter-intuitive to me. The concept is if you load the drive/platter with torque (either through an eddy brake or thick bearing lubrication), then small dynamic changes in torque will be "swamped" by the static torque load and will therefore go unnoticed. If the speed is stable with whatever static load is placed on it, the system is in balance and dynamic loads will still disturb that balance proportionate to the amplitude of the dynamic load, not in ratio of the dynamic to static load. The only way this makes sense is if the torque load/rotor angle is not linear, which it is not-torque is proportional to the sine of the rotor/field angle, but the relationship is very nearly linear at the lower end of the torque curve. So unless you are applying a static load that is very near the stall torque (close to 90° rotor/field angle where the slope starts to flatten) it’s difficult to see how this could have any benefit. I suspect the improvement in sound that some report with thicker bearing oils is due to mechanical damping and not to speed stability.