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@ -566,9 +566,9 @@ path, as specified in the PATH environment variable.
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Additional instructions for special machines:
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\begin{tabular}{ll}
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\texttt{./configure ARCH=crayxt4r}& for CRAY XT machines
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\texttt{./configure ARCH=necsx} & for NEC SX machines
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\texttt{./configure ARCH=ppc64-mn}& PowerPC Linux + xlf (Marenostrum)
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\texttt{./configure ARCH=crayxt4r}& for CRAY XT machines \\
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\texttt{./configure ARCH=necsx} & for NEC SX machines \\
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\texttt{./configure ARCH=ppc64-mn}& PowerPC Linux + xlf (Marenostrum) \\
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\texttt{./configure ARCH=ppc64-bg}& IBM BG/P (BlueGene)
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\end{tabular}
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@ -1462,7 +1462,7 @@ variable OMP\_NUM\_THREADS.
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MPI is the well-established, general-purpose parallelization.
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In \qe\ several parallelization levels, specified at run-time
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via command-line options to the executable, are implemented
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with MPI. This is your first choice for execution a parallel
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with MPI. This is your first choice for execution on a parallel
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machine.
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Library OpenMP is a low-effort parallelization suitable for
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@ -2236,7 +2236,7 @@ Second, you can calculate phonons using Density-Functional Perturbation Theory.
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Further processing to calculate Interatomic Force Constants, to add macroscopic
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electric field and impose Acoustic Sum Rules at q=0 may be needed.
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In the following, we will indicate by $q$ the phonon wavevectors,
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whle $k$ will indicate Bloch vectors used for summing over the Brillouin Zone.
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while $k$ will indicate Bloch vectors used for summing over the Brillouin Zone.
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Since version 4.0 it is possible to safely stop execution of
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\ph.x\ code using
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@ -2340,7 +2340,7 @@ For more details, see Example 07.
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\subsection{Distributed Phonon calculations}
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A complete phonon dispersion calculation can be quite long and
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expensive, but it can be spit into a number of semi-independent
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expensive, but it can be split into a number of semi-independent
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calculations, using options \texttt{start\_q}, \texttt{last\_q},
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\texttt{start\_irr}, \texttt{last\_irr}. An example on how to
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distribute the calculations and collect the results can be found
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