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Mention in bands.x DOC that calculated p includes the nonlocal potential contribution.
(In other words, the calculated matrix elements are the matrix elements of m*v, not those of the true momentum operator.)
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@ -24,7 +24,8 @@ input_description -distribution {Quantum Espresso} -package PWscf -program bands
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- if (@ref lsigma(i)): file "filband".i, i=1,2,3, with expectation values
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of the spin operator in the noncolinear case
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- file "filband".gnu with bands in eV, directly plottable using gnuplot
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- file @ref filp with matrix elements of p
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- file @ref filp with matrix elements of p (including the nonlocal potential
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contribution i*m*[V_nl,x])
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@b {Structure of the input data:}
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============================
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@ -81,7 +82,11 @@ input_description -distribution {Quantum Espresso} -package PWscf -program bands
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info {
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If .true. matrix elements of the momentum operator p between
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conduction and valence bands are computed and written to file
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specified in @ref filp
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specified in @ref filp.
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The matrix elements include the contribution from the nonlocal
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potential, i*m*[V_nl, x]. In other words, the calculated matrix elements
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are those of the velocity operator i*m*[H, x] times mass, not those of
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the true momentum operator.
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}
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}
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