Yes. Since $Z$ and $\xi$ are independent, we may write $$X_t = \int_{-\infty}^\infty \mathbb E[g(\xi, z)| \mathcal F^W_t] \, d\mu_Z,$$ as can be seen by, say, taking the regular conditional expectation with respect to $Z$. We recognize that $Y^z_t: = \mathbb E[g(\xi, z)| \mathcal F_t^W]$ is a closable martingale with respect to the Brownian filtration. According to the results [here](https://mathoverflow.net/questions/402811/when-is-every-levy-martingale-of-a-process-a-continuous-martingale) and [here](https://math.stackexchange.com/questions/4011101/stopping-time-w-r-t-brownian-filtration-is-predictable), $Y^z_t$ is in fact continuous for every $z$. By the boundedness of $g$, $Y^z_t$ is also uniformly bounded. Now the rest of the proof is analysis - we claim that $X_t$, being the average of continuous bounded functions is also continuous almost surely. To see this, let $$\phi(z, \delta, \omega) := \sup_{s, t; |s - t| < \delta} |Y_t^z (\omega) - Y_s^z (\omega)|$$ be a uniform modulus of continuity for $Y^z$, and let $M > 0$ be a uniform bound for $|g|$. By continuity of $Y^z_t$, we have for $\mu_z \times \mathbb P$-a.e. $(z, \omega)$ that $\lim_{\delta\to 0} \phi(z, \delta, \omega) = 0$. In other words, writing $E_{\varepsilon, \delta, \omega} := \{z \, | \, \phi(z, \delta, \omega) \leq \varepsilon\}$, we have that for every $\varepsilon > 0$, and $\mathbb P$-a.e. $\omega$ that $\mu_Z(E_{\varepsilon, \delta, \omega}) \to 1$ as $\delta \to 0^+$. Now let $\varepsilon > 0$ be arbitrary, and fix $\omega$ in the full measure set as above. Pick $\delta$ such that $\mu_z (E_{\varepsilon/2, \delta, \omega}) > 1 - \frac{\varepsilon}{2M}$. We then compute, for all $s, t$ with $|s - t| < \delta$, $$|X_t (\omega) - X_s (\omega)|$$ $$= |\int_{-\infty}^\infty Y^z_t (\omega) - Y^z_s (\omega)\, d\mu_Z|$$ $$\leq \int_{-\infty}^\infty |Y^z_t (\omega) - Y^z_s (\omega)| \, d\mu_Z$$ $$ = \int_{E_{\varepsilon/2, \delta, \omega}} |Y^z_t (\omega) - Y^z_s (\omega)| \, d\mu_Z + \int_{E^c_{\varepsilon/2, \delta, \omega}} \mathbb |Y^z_t (\omega) - Y^z_s (\omega)| \, d\mu_Z$$ $$ < \frac{\varepsilon}{2} + M \frac{\varepsilon}{2M} = \varepsilon$$ and we conclude since $\varepsilon$ was arbitrary.