You could use a cap, or not.
Normally, a large-value resistor is used to drop the excess voltage. A typical value might be ~220kΩ.
You could look at that resistor as half a voltage divider. The only problem is the other half of the divider has non-linear components, including a diode and charging pulses for the bias cap, so it's harder than normal to calculate the needed value of resistor to drop voltage.
If you're having to experiment with an unknown/untested circuit, maybe you should use a 1MΩ linear pot in place of the 220kΩ resistor, and wire the pot as a rheostat. Adjust til you get proper bias circuit operation.
You could use a cap instead of a resistor to drop the voltage. It's not really blocking anything, because it takes its input voltage from the PT secondary. Therefore it is on the opposite side of the rectifier from the B+ voltage, and there should be no d.c. present.
Instead, what it does is form a capacitive voltage divider with the bias cap. A small-value cap looks like a bigger impedance (at a given frequency) than a larger-value cap. So using two caps as a voltage divider, the a.c. is divided by the impedance of the caps, while the d.c. present at input, "ground" and the junction of the caps are all isolated form each other.
The value of the capacitive divider is that it divides a.c. while leaving d.c. unaffected (or blocked). You'll also occasionally see capacitive divider in parallel with resistive dividers in voltmeters/o'scopes, to ensure parasitic components of the resistive divider don't cause differing results at different frequencies.
A far less important benefit in your case is the physical heat dissipated by the caps will be very much less than the heat dissipated by a resistive divider, because the voltage and current are not in-phase.
So in your case, you could use either. It will probably be easier to dial in the bias circuit operation with a dropping resistor rather than a cap-divider (you'd have to have a lot of cap values on hand to substitute to find the best value).