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| author | Eugeniy E. Mikhailov <evgmik@gmail.com> | 2021-09-28 21:55:33 -0400 |
|---|---|---|
| committer | Eugeniy E. Mikhailov <evgmik@gmail.com> | 2021-09-28 21:55:33 -0400 |
| commit | 558c60df1f70a98c1e04cc96ad7651290708ae11 (patch) | |
| tree | 9872973bd043b240abc9b5ffb4d2a14d6e9d89a5 | |
| parent | 21777ae181c340b701161598b9ec11aa3fef02fe (diff) | |
| download | manual_for_Experimental_Atomic_Physics-558c60df1f70a98c1e04cc96ad7651290708ae11.tar.gz manual_for_Experimental_Atomic_Physics-558c60df1f70a98c1e04cc96ad7651290708ae11.zip | |
improve precision of the cell length: 3 cm -> 3.0 cm
| -rw-r--r-- | interferometry_new.tex | 2 |
1 files changed, 1 insertions, 1 deletions
diff --git a/interferometry_new.tex b/interferometry_new.tex index 55a855d..ff46295 100644 --- a/interferometry_new.tex +++ b/interferometry_new.tex @@ -183,7 +183,7 @@ Eq.(\ref{old3}), this difference is \begin{equation} \label{delta_n} \Delta n=\Delta m \frac{\lambda_0}{2d_{cell}} \end{equation} -where $d_{cell}=3$~cm is the length of the gas cell. +where $d_{cell}=3.0$~cm is the length of the gas cell. Since the change in the refractive index $\Delta n$ is linearly depends on the air pressure $\Delta p=p_0-p_{fin}$, it is now easy to find out the |