Let $W$ be a one dimensional Brownian motion and define, $$ X_t=W_{(\text{exp}(\beta t)-1)}\\ \hat{W}_t=\frac{1}{\sqrt{\beta}}\int_0^te^{-\frac{\beta s}{2}}dX_s $$
Show that $\hat{W}_t$ is a local martingale in its natural filtration and compute its quadratic variation.
To show that it's a local martingale, is it just straight forward differentiation on $\hat{W}_t$ like below,
$$ d\hat{W}_t=\frac{1}{\sqrt{\beta}}e^{-\frac{\beta t}{2}}dW_{(\text{exp}(\beta t)-1)} $$
I came up with a solution involving properties of time change as follows...
Let $\theta(t)=\int_0^t\xi^2ds$, which we assume is finite.
Then the stochastic integral $Y_t=\int_0^t\xi dW_s$ exists, and $Y_t$ is a Gaussian process with independent increments.
The variance of $Y_t-Y_s$ is given by,
$$ \begin{align} Var\left[Y_t-Y_s\right]&=\mathbb{E}\left[\left(Y_t-Y_s\right)^2\right]-\mathbb{E}\left[Y_t-Y_s\right]^2\\ &=\mathbb{E}\left[\left(\int_0^t \xi dW_s - \int_0^s\xi dW_u \right)^2\right]-0\\ &=\mathbb{E}\left[\left(\int_s^t \xi dW_u \right)^2\right]\\ &=\mathbb{E}\left[\left(\int_s^t \xi^2du \right)^2\right]\\ &=\theta(t)-\theta(s)\\ &=\mathbb{E}\left[\left( W_{\theta(t)}-W_{\theta(s)} \right)^2\right]\\ \end{align} $$
So $Y_t$ has the same distribution as time changed Brownian Motion $W_{\theta(t)}$. From the definition of $Y_t$ we have,
$$ Y_t=\int_0^t\xi dW_s=\int_0^t\sqrt{\theta'(s)}dB_s \sim W_{\theta(t)} $$
For our problem, $ \theta(t) = e^{\beta t}-1$ , and $\sqrt{\theta'(t)}=\sqrt{\beta}e^{\frac{\beta t}{2}}$
From this we finally have,
$$ \hat{W}_t=\frac{1}{\sqrt{\beta}}\int_0^t e^{-\frac{bs}{2}}\sqrt{\beta} e^{\frac{bs}{2}}dW_s=\int_0^t dW_s $$
Which is a martingale.
For quadratic variation, we know that $\langle \hat{W}\rangle_t$ is the process such that $ \hat{W}_t^2 - \langle W\rangle_t$ is a martingale. Therefore,
$$ \begin{align} \mathbb{E}\left[ \hat{W}_t^2 - \langle \hat{W}\rangle_t \right] &= 0\\ \Rightarrow\mathbb{E}\left[ \langle \hat{W}\rangle_t \right] &= \mathbb{E}\left[ \hat{W}_t^2 \right]\\ &= \mathbb{E}\left[ \left(\int_0^t dW_s \right)^2\right]\\ &= \mathbb{E}\left[ \left(\int_0^t 1^2 ds \right)^2\right]\\ \Rightarrow \langle \hat{W}\rangle_t = t \end{align} $$
This shows that $\langle \hat{W}\rangle_t $ is a Brownian Motion in its natural filtration.