I was looking at the ESM implementation in QE, and note that case iv of Otani 
and Sugino doesn't seem to be implemented (\epsilon_r finite in the bulk on 
both sides)--what is the reason for that?
Does that have anything to do with the expressions for the Hartree energy, 
which I can't find in the original paper?
Niels

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Prof. Niels R. Walet                             Phone:  +44(0)1613063693
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