The path that surprised me most on EV work was not the radiated field from the inverter itself, but the common-mode current on the high-voltage cable acting as an antenna. The inverter switching edge is fast, the HV cable is long, and if the shield is terminated at only one end, or through a pigtail with significant inductance, the shield current has nowhere clean to return — so it flows on the outside of the shield and radiates, or couples into the low-voltage harness running alongside it. A shield that measures well at DC can be almost useless at the switching harmonics if its termination is poor.
That leads to a practical triage order. First, check the HV cable shield termination: a 360-degree termination at both ends, with low-impedance bonds to the enclosure, is worth more than a thicker shield can. Second, use a current probe on the HV cable, the LV harness and the chassis bond while the inverter is running — the cable carrying the largest common-mode current at the victim frequency is usually the radiating element, and that measurement is much more decisive than a near-field probe alone. Third, look at the busbar and DC-link loop area inside the inverter: a large loop is a magnetic source that a thin enclosure will not stop, so minimising loop area and adding a low-impedance return path often beats adding shielding material.
Also check whether the noise tracks switching frequency or RPM, and which victim band is affected. If the victim is a GNSS or cellular receiver, even a small conducted path through a shared ground can dominate, because the receiver is looking for a signal far below the inverter noise. In that case, filtering the LV harness at the enclosure boundary and separating the HV and LV return paths usually gives more improvement than another layer of shielding on the inverter can.