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\sigma_N,
\label{surf}$$ where $\epsilon_N$ is the energy per nucleon and the star indicates that the surface tension is calculated in the center-of-mass frame. The symmetry energy is the difference between the binding energy per nucleon of symmetric matter and pure neutron matter. In order to calculate the effective surface tension at $T=0$, one has to add the binding energy of asymmetric matter into the thermal energy. The total energy per nucleon in symmetric matter is given by $$E_N = \frac{\epsilon_N}{1+\frac{\epsilon_N}{f_\pi^2}},$$ where $\epsilon_N$ is the energy per nucleon in symmetric matter. One sees that even for symmetric matter the asymmetry energy is needed. The total surface tension of the nucleon gas is then $$\sigma = \sigma_N + \sigma^*.$$ One expects the effective nucleon surface tension in the center-of-mass frame to be less than the free nucleon surface tension: $
\sigma_{\rm eff.} \approx \sigma_N/2.
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