We investigate the polarization switching mechanism in ferroelectric-dielectric (FE-DE) stacks and its dependence on the dielectric thickness (TDE). We fabricate HZO-Al2O3 (FE-DE) stack and experimentally demonstrate a decrease in remnant polarization and an increase in coercive voltage of the FE-DE stack with an increase in TDE. Using phase-field simulations, we show that an increase in TDE results in a larger number of reverse domains in the FE layer to suppress the depolarization field, which leads to a decrease in remanent polarization and an increase in coercive voltage. Further, the applied voltagedriven polarization switching suggests domain-nucleation dominant characteristics for low TDE, and domain-wall motioninduced behavior for higher TDE. In addition, we show that the hysteretic charge-voltage characteristics of the FE layer in the FE-DE stack exhibit a negative slope region due to the multi-domain polarization switching in the FE layer. Based on our analysis, the trends in charge-voltage characteristics of the FE-DE stack with respect to different TDE (which are out of the scope of single-domain models) can be described well with multi-domain polarization switching mechanisms.Ferroelectric (FE) hafnium oxide, by virtue of its CMOS process compatibility 1,2 and rich domain dynamics 3,4 , has been identified as one of the most promising candidates for enabling future electronic devices. By integrating doped HfO 2 (as FE) in the gate stack of a transistor (FE-FET), non-volatile memory (NVM) 5-6 , neuron 7 and synaptic 8,9 functionalities have been demonstrated. Such diverse functionalities demand different characteristics of polarization (P) switching in the FE layer. For example, an abrupt P-switching is beneficial for neurons and binary NVMs, while a gradual P-switching is favorable for multi-bit memories and synapses. Therefore, it becomes essential to appropriately design FEFET for application-specific device behavior, for which gate stack optimization plays a key role.