Matt Pitkin edited untitled.tex  over 8 years ago

Commit id: 48c4a34e72824441ddb640bbae0c897c4148fa51

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Therefore we can expand out the phase evolution to be  \begin{equation}  \phi(t) \approx 2\pi \sum_{l=0} \frac{f^{(l)}}{(l+1)!} \left(t(1+\dot{\delta}_k \left(t\left(1+\dot{\delta}_k  + \frac{\ddot{\delta}_k}{2}t)-t_0+\delta_k+t_k\right)^{(l+1)}. \frac{\ddot{\delta}_k}{2}t\right)-t_0+\delta_k+t_k\right)^{(l+1)}.  \end{equation}