The compliance is an interesting number, if only because it is frequency dependent. The quoted DL103 compliance is at 100Hz, which is useless for calculating arm effective mass/compliance resonance at around 10Hz.
So a compliance at 10Hz is a much more relevant number in this regard.
As far as I can find, and I failed to find a proof for this, you multiply the 100Hz compliance by 1.7 (root 3?) to get the 10Hz compliance. So for the DL103, you get 8.5 x 10^-3m/N.
This means you need a total effective mass of around 30g to hit the resonance sweet spot at 10Hz.
Now I use an SMEIV arm, which has a rather light effective mass of 10-11g. So the regular DL103 with a total effective mass of 22g, giving a resonance of 11.6Hz. Now I use the heftier Zu Audio DL103, where they take the motor out of the plastic bit, and precision glue it into an aluminium housing. That has a mass of 14g, which with the SMEIV puts the resonance at 11Hz
Because all this is a square root thing, you'd have to add 5g at the headshell to my set up to get to 10Hz, or with the regular DL103, 8g.
I use the SME cartridge spacer (because it is needed anyway for the tall Garrard 401) but that adds a useful 3g, getting my effective mass to 11+14+3 = 28g, putting my resonance at 10.3HZ, which I'm very happy with.
All that is with the SMEIV.
If you had deep enough pockets to go for the SME M2-12R 12" arm, with an effective mass of 18g, that would hit the 30g effective mass sweetspot of 10Hz right on the button with the regular DL103 and DL103R.
Oh - of course you have to add the weight of the cartridge screws too to get the total effective mass!