deletions | additions       diff --git a/We_expect_the_transmission_data__.tex b/We_expect_the_transmission_data__.tex  index 63c3723..84f1848 100644  --- a/We_expect_the_transmission_data__.tex  +++ b/We_expect_the_transmission_data__.tex 
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T(\omega)=(\frac{\Gamma}{2}^{2})*(\frac{A}{(\omega-\omega_{0})^{2}+\frac{\Gamma}{2}^{2}})  \end{equation}  Thus the transition frequency of the different peaks should theoretically be given by, $\omega_{1},\cdots,\omega_{6}$. The offset accounts for the background Gaussian distribution, which the Lorentzian functions are superimposed onto.  \par In order to measure transition frequency, we must first convert oscilloscope time to a frequency. We can do this by plotting a graph of $\frac{\delta t}{\delta \omega}$ versus ratio number. number (Figure 12).  Since we expect the width of the peaks on the transmission graph to be the same, \begin{equation}\label{eq3}  \frac{t_{2}-t_{1}}{\omega_{2}-\omega_{1}}=\frac{t_{3}-t_{2}}{\omega_{3}-\omega_{2}}=\cdots  \end{equation}