Implement Päivi's suggestions except the Applications part.
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@ -1040,8 +1040,7 @@ matrix method for multilayer calculations.},
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number = {1}
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number = {1}
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}
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}
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@article{vakevainen_plasmonic_2014-1,
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@article{vakevainen_plasmonic_2014,
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ids = {vakevainen\_plasmonic\_2014},
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title = {Plasmonic {{Surface Lattice Resonances}} at the {{Strong Coupling Regime}}},
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title = {Plasmonic {{Surface Lattice Resonances}} at the {{Strong Coupling Regime}}},
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author = {V{\"a}kev{\"a}inen, A. I. and Moerland, R. J. and Rekola, H. T. and Eskelinen, A.-P. and Martikainen, J.-P. and Kim, D.-H. and T{\"o}rm{\"a}, P.},
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author = {V{\"a}kev{\"a}inen, A. I. and Moerland, R. J. and Rekola, H. T. and Eskelinen, A.-P. and Martikainen, J.-P. and Kim, D.-H. and T{\"o}rm{\"a}, P.},
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year = {2014},
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year = {2014},
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@ -491,6 +491,67 @@ These are compatibility macros for the (...)-old files:
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\end_layout
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\end_layout
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\begin_layout Title
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\begin_layout Title
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Multiple-scattering
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\begin_inset Formula $T$
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\end_inset
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-matrix simulations for nanophotonics: symmetries and periodic lattices
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\end_layout
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\begin_layout Author
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Marek Nečada
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\begin_inset Foot
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status open
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\begin_layout Plain Layout
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\begin_inset CommandInset href
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LatexCommand href
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target "marek@necada.org"
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type "mailto:"
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literal "false"
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\end_inset
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\end_layout
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\end_inset
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, Päivi Törmä
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\begin_inset Foot
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status open
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\begin_layout Plain Layout
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\begin_inset CommandInset href
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LatexCommand href
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target "paivi.torma@aalto.fi"
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type "mailto:"
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literal "false"
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\end_inset
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\end_layout
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\end_inset
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\end_layout
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\begin_layout Address
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Department of Applied Physics, Aalto University School of Science, P.O.
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Box 15100, FI-00076 Aalto, Finland
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\end_layout
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\begin_layout Standard
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\begin_inset Note Note
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status open
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\begin_layout Plain Layout
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Alternative titles:
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\end_layout
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\begin_layout Itemize
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Many-particle
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Many-particle
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\begin_inset Formula $T$
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\begin_inset Formula $T$
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\end_inset
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\end_inset
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@ -499,18 +560,6 @@ Many-particle
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modes
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modes
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\end_layout
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\end_layout
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\begin_layout Standard
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Alternative titles:
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\end_layout
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\begin_layout Itemize
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Multiple-scattering
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\begin_inset Formula $T$
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\end_inset
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-matrix simulations for nanophotonics: symmetries and periodic lattices.
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\end_layout
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\begin_layout Itemize
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\begin_layout Itemize
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Many-particle
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Many-particle
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\begin_inset Formula $T$
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\begin_inset Formula $T$
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@ -527,6 +576,11 @@ Many-particle
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-matrix simulations in finite and infinite systems of electromagnetic scatterers
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-matrix simulations in finite and infinite systems of electromagnetic scatterers
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\end_layout
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\end_layout
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\end_inset
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\end_layout
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\begin_layout Standard
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\begin_layout Standard
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\begin_inset Note Note
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\begin_inset Note Note
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status open
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status open
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@ -610,9 +664,6 @@ The T-matrix multiple scattering method (TMMSM) can be used to solve the
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retaining a good level of accuracy while using relatively few degrees of
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retaining a good level of accuracy while using relatively few degrees of
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freedom, largely surpassing other methods in the number of scatterers it
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freedom, largely surpassing other methods in the number of scatterers it
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can deal with.
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can deal with.
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\end_layout
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\begin_layout Abstract
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Here we extend the method to infinite periodic structures using Ewald-type
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Here we extend the method to infinite periodic structures using Ewald-type
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lattice summation, and we exploit the possible symmetries of the structure
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lattice summation, and we exploit the possible symmetries of the structure
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to further improve its efficiency, so that systems containing tens of thousands
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to further improve its efficiency, so that systems containing tens of thousands
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@ -636,10 +687,6 @@ Should I mention also the cross sections formulae in abstract / intro?
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\end_inset
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\end_inset
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\end_layout
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\begin_layout Abstract
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We release a modern implementation of the method, including the theoretical
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We release a modern implementation of the method, including the theoretical
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improvements presented here, under GNU General Public Licence.
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improvements presented here, under GNU General Public Licence.
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\end_layout
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\end_layout
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@ -289,6 +289,11 @@ wide false
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sideways false
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sideways false
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status open
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status open
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\begin_layout Plain Layout
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\align center
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\begin_inset Note Note
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status open
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\begin_layout Plain Layout
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\begin_layout Plain Layout
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\align center
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\align center
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\begin_inset Graphics
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\begin_inset Graphics
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@ -305,6 +310,11 @@ status open
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\end_inset
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\end_inset
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\end_layout
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\end_inset
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\begin_inset Caption Standard
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\begin_inset Caption Standard
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\begin_layout Plain Layout
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\begin_layout Plain Layout
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@ -361,6 +371,11 @@ status open
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\end_layout
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\end_layout
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\begin_layout Plain Layout
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\align center
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\begin_inset Note Note
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status open
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\begin_layout Plain Layout
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\begin_layout Plain Layout
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\align center
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\align center
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\begin_inset Graphics
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\begin_inset Graphics
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@ -370,6 +385,11 @@ status open
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\end_inset
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\end_layout
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\end_inset
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\end_layout
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\end_layout
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\begin_layout Plain Layout
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\begin_layout Plain Layout
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@ -570,6 +590,11 @@ wide false
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sideways false
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sideways false
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status open
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status open
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\begin_layout Plain Layout
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\align center
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\begin_inset Note Note
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status open
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\begin_layout Plain Layout
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\begin_layout Plain Layout
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\align center
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\align center
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\begin_inset Graphics
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\begin_inset Graphics
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@ -579,6 +604,11 @@ status open
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\end_inset
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\end_inset
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\end_layout
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\end_inset
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\end_layout
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\end_layout
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\begin_layout Plain Layout
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\begin_layout Plain Layout
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@ -690,6 +720,11 @@ wide false
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sideways false
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sideways false
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status open
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status open
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\begin_layout Plain Layout
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\align center
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\begin_inset Note Note
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status open
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\begin_layout Plain Layout
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\begin_layout Plain Layout
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\align center
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\align center
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\begin_inset Graphics
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\begin_inset Graphics
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@ -699,6 +734,11 @@ status open
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\end_inset
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\end_layout
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\end_inset
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\end_layout
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\begin_layout Plain Layout
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\begin_layout Plain Layout
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@ -2139,7 +2139,7 @@ If we assume that
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is chosen to represent the (rough) maximum tolerated magnitude of the summand
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is chosen to represent the (rough) maximum tolerated magnitude of the summand
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with regard to target accuracy.
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with regard to target accuracy.
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This adjustment means that, in worst-case scenario, with growing wavenumber
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This adjustment means that, in the worst-case scenario, with growing wavenumber
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one has to include an increasing number of terms in the long-range sum
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one has to include an increasing number of terms in the long-range sum
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in order to achieve a given accuracy, the number of terms being proportional
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in order to achieve a given accuracy, the number of terms being proportional
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to
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to
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