deletions | additions       diff --git a/section_Nuclear_Schottky_effect_In__.tex b/section_Nuclear_Schottky_effect_In__.tex  index 96d01fd..c29a04a 100644  --- a/section_Nuclear_Schottky_effect_In__.tex  +++ b/section_Nuclear_Schottky_effect_In__.tex 
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\label{eq:CurieConstant}  \lambda_N = N_A I (I+1) \mu_0 G_N^2 {\mu}_N^2 / 3 k_B  \end{equation}  and we neglect the contribution of effective fields of the dipole and quadrupole moments in Cu in comparison to that from the applied field $H$.   Substituting $g_N = \mathrm{1.5}$ --- the average nuclear g-factor for the two most common Cu isotopes ${}^{63}\mathrm{Cu}$ and ${}^{65}\mathrm{Cu}$ \cite{Leyarovski_1988}--- into Eq.~\ref{eq:CurieConstant} gives a theoretical value $\lambda_{\mathrm{Cu}} = 3.93 \cdot 10^{-12} \textrm{ K}{\textrm{ m}}^3 {\textrm{ mol}}^{-1}$.