... Is it because in the working lamp the emission is limited by ballast current and not the electrode ?
Yes, normally the arc heats up the electrode enough (it uses to settle for a 10..15V of the cathode fall). When you add external heating, you may decrease the cathode fall by few volts (to about 7..10V), but that is practically no difference when speaking about the consequent arc current (so the brightness).
The lamp fading is, when the current rises/falls around 5 to 10% of the rated current and when the current is limited by the available OCV (not enough voltage to cause emission by just high electric field; way easier to get on a 120V OCV than on a 230V, just because the same absolute voltage of the cathode fall is double in percentage on 120V, so impacts the current way more severely than on 230V).
Usually when you exceed about 30% of the rated current, usually the amount of generated heat on the cathodes is sufficient to make the system "flip" into the normal hot electrode operation. For less than 10% it usually dies out (10% current means 100..150V cathode fall for the same heating power, that starts to be too much even for the 230V).
These figures are even the base on how the RS starts: Very tiny capacitive glow, then as the electrodes warm up so they support about the 10..20% of the rated current means the lamp gets gradually brighter to that 10..20% level. That goes as fast, as the cathodes are warmed up by the heater winding, so the gradual (few seconds) fade-in is quite well visible. At that point the cathode fall gets enough power to provide way higher heating power, so the further warmup gets way faster, till the current became limited by the ballast. The last section is rather fast, so shows rather immediate (fraction of a second) increase in the brightness from the 20% to full ballast power.