I use the words "local" and "non-local" only in one proper mathematical meaning, i.e., that local observables in relativistic QFTs commute with the Hamilton density when their space-time arguments are space-like separated, i.e., ##[\hat{O}(x),\hat{\mathcal{H}}(y)]=0## for ##(x-y) \cdot (x-y)<0## (west-coast convention, i.e., ##\eta_{\mu \nu}=\mathrm{diag}(1,-1,-1,-1)##. Thus there cannot be any causal connections between space-like separated events.
For me an observable in Q(F)T has a predetermined value if and only if the system is prepared in a state such that the probability for measuring one of the possible values with 100% probability. Otherwise the value is indetermined before measurement and the state preparation only implies a certain probability for finding each of its possible values and nothing else. In which state the system is after the measurement depends on the construction of the measurement device, i.e., the specific interaction between the measured system and the measurement device. Since these interactions are just usual interactions described by local relativistic QFT there's no faster-than-light causal effect by a local measurement at one place and another space-like separated local measurement at another place. If the two space-like separated local measurements refer to entangled parts of a quantum system, then the observed correlations are not mutually caused by the local measurements but are due to the preparation of the system in the entangled state before any of the two measurements where done. By construction there is no contradiction between relativistic spacetime causality constraints and local relativistic QFT.
To confuse long-ranged correlations and inseparability of entangled systems with causal interactions at a distance is only misleading and contradicts the very foundational construction of local relativistic QFT.