this is for holding javascript data
Madeline Horn edited The_fits_for_the.tex
over 8 years ago
Commit id: b5131dc62d3ddf1b650c454f5c55f826bb71b7a4
deletions | additions
diff --git a/The_fits_for_the.tex b/The_fits_for_the.tex
index f261f14..b55cacd 100644
--- a/The_fits_for_the.tex
+++ b/The_fits_for_the.tex
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\begin{equation}
E_n [eV] (Peaks) = (0.1386\pm0.06)n + (11.20\pm0.29)
E_a [eV] (Peaks) &=(0.1386\pm0.06)(0.5) + (11.20\pm0.29)\\
E_a [eV] (Peaks) &=11.1177\pm10.35
\end{split}
\end{equation}
\begin{equation}
E_n [eV] (Dips) = (0.1953\pm0.07)n + (11.02\pm0.31)
E_a [eV] (Dips) &=(0.1953\pm0.07)(0.5) + (11.02\pm0.31)\\
E_a [eV] (Dips) &=11.3593\pm0.38
\end{equation}
The value of $\Delta E_n (0.5)$ for the peaks was found to be $11.1177eV$ and for the dips was found to be $11.3593eV$. These values are consistent with the NIST ASD data for excitation energy of the lowest energy level ($11.6236eV$ and $11.548 eV$). The percent error of the peak values is $3.9\%$ and the percent error of the dip values is $2.8 \%$. Therefore the values found from the linear fit of $\Delta E_{n}$ vs $n$ are consistent with the expected values for Argon.