The field strength is not related to gap area, rather just the gap.
With two infinite plates, the field strength is V/d, so halving the gap will double the field strength and halve the trigger voltage for a given dielectric.
As you move down to finite electrode radius, the field strength goes up as the radius goes down. However, to a first order you will still get the direct relationship between breakdown voltage and gap.
Having said that, I wonder about your stated "on" resistance for the gap. On resistance is generally inversely related to current, because the plasma channel tends to expand as the current/heating goes up. At the currents in question, I am surprised with your quoted value.
To provide more analysis will require more details on the gap design, including dimensions, gas pressure and source inductance/capacitance. However, you might find this paper informative ARC CURRENT, VOLTAGE, AND RESISTANCE IN A HIGH ENERGY, GAS-FILLED SPARK GAP
Finally, I assume you know that to get to 1MV trigger, you are likely to need very large radius electrode, and insulator structures? Have a look at this answer for more info Spark gap minimum breakdown voltage vs air gap
Additional context
It's worth noting that gaps in this voltage range are often implemented in a stacked multi-stage configuration. The bottom gap commonly has a trigger system, and the upper gaps are designed to trigger as soon as the lower gap fires because of the increased overvoltage. There is also the potential for sync using the UV light from the lower gap (as common in Marx generators), or with external lasers.
Balance across the gaps can be maintained with grading electrodes and corona stabilizers, which leak charge across any intermediate gaps with excessive voltage difference.
These kind of setups can be very compact, and I've seen past descriptions of a pressurized gas gap with 5 stages, which fitted in an 11" gap between two large electrodes, all in a SF6 insulating tank.