Let $(\mathcal A, \tau)$ be a $C^*$-dynamical system and let $\omega$ be a state on $\mathcal A$.
Is the following true, and if yes, why?
$$ |\omega(\tau_t(A)| \le \|A\| \quad \forall t \in \mathbb R, A \in \mathcal A $$
I have a hunch why it should be true for a concrete example.
If the dynamics is given by a Hamiltonian $H$, that is
$$ \tau_t(A) := e^{itH} A e^{-itH} \,,$$
then the result follows from the formula
$$ \omega(B^*AB) \le \omega(B^*B)\|A\| $$
replacing $B$ with $e^{-itH}$.
However, even in this concrete example, I am not sure if $e^{-itH}$ belongs to the algebra $\mathcal A$, given that the Hamiltonian $H$ is already in the algebra. I think it has to do with the fact that $\mathcal A$ is a Banach space by definition. Therefore, the convergent exponential series should have a limit point in the algebra. Right?
Nevertheless, this is just a hunch with a concrete example. I would like to know the more general theorem stated above.