One of the most common techniques for integrating ODEs is to using Runge-Kutta methods (of which Euler integration is just a special case). However, these only improve errors due to discretization of time. If you are concerned about errors caused by noise in $\delta$ then I'm not aware of any better methods.
Add Example
For RK4 and using the dynamics $\dot{x}(t) = v(t)$, where the velocity is not dependent on the state, you have
$$
\begin{align}
k_1 &= v(t)
\\
k_2 &= v \left ( t+\frac{\delta}{2} \right )
\\
k_3 &= v \left ( t+\frac{\delta}{2} \right )
\\
k_4 &= v \left ( t+\delta \right )
\\
x(t+\delta) &= x(t) + \frac{h}{6} (k_1 + 2 k_2 + 2 k_3 + k_4)
\end{align}
$$
If you have access to $v(t+\frac{\delta}{2})$ this will provide an improvement over Euler integration. If not, you can probably still get some improvement by assuming $v(t+\frac{\delta}{2}) = \frac{v(t) + v(t+\delta)}{2}$.
Other Option - Kalman Filter
For such a simple system, another option would be to use a Kalman filter. In the case where you only have access to $v(t)$ and $v(t+\delta)$ (no intermediate information) this might work better.