Ref. 302, similarly discusses how initializing in a squeezed state can affect polariton dynamics. In that work, a LiF molecular is coupled to a cavity, described by the quantum Rabi model Hamiltonian (Eq. 82). Fig. presents the dynamical progression (illustrated by the black arrows) of the polariton system in the position representation (with photonic coordinate q c as the y-axis and nuclear coordinate R as the x-axis) when the initial photonic condition is set to be either a coherent state or a squeezed state. The coherent state exhibits the standard oscillator behavior that is a "trade- mark" of these states. The squeezed coherent states, on the other hand, evolve in a "breathing" manner, where the expectation value of the photonic coordinate remains constant but the uncertainty oscillates. Fig. presents how the excited state final population changes as a function of the quantum phase term in α, ϕ, and the phase term of ξ, θ, for squeezed states of a constant r = |α| = 1. Further, Fig. presents that if α is held as a constant, varying r and θ can also dramatically change the excited state final population. These theoretical investigations with squeezed coherent states demonstrate how using these minimal uncertainty states (quantum photonic states) can affect polariton dynamics. In these examples, the reactivity of the LiF molecule changes due to the photonic state introduced in the cavity, showing how for a given cavity-molecule system the dynamics can be altered by introducing different photonic states. If can be realized experimentally, this will be a prime example of using tuning knobs in quantum optics to control chemistry.