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git-svn-id: svn://svn.icms.temple.edu/lammps-ro/trunk@13795 f3b2605a-c512-4ea7-a41b-209d697bcdaa
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@ -860,7 +860,7 @@ variables that have to match the VMD installation on your system.</p>
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source code for individual scripts for comments about what they do.</p>
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<p>Here are screenshots of the vizplotgui_tool.py script in action for
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different visualization package options. Click to see larger images:</p>
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<a data-lightbox="group-c530f122-6019-45af-8a35-e7cdc70ddb55"
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<a data-lightbox="group-default"
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href="_images/screenshot_gl.jpg"
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class=""
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title=""
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@ -870,7 +870,7 @@ different visualization package options. Click to see larger images:</p>
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width="25%"
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height="auto"
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alt=""/>
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</a><a data-lightbox="group-f712591c-ea31-483b-86da-3905db788920"
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</a><a data-lightbox="group-default"
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href="_images/screenshot_atomeye.jpg"
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class=""
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title=""
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@ -880,7 +880,7 @@ different visualization package options. Click to see larger images:</p>
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width="25%"
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height="auto"
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alt=""/>
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</a><a data-lightbox="group-4a2be907-5b47-4889-89de-f686acc6e915"
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</a><a data-lightbox="group-default"
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href="_images/screenshot_pymol.jpg"
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class=""
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title=""
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@ -890,7 +890,7 @@ different visualization package options. Click to see larger images:</p>
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width="25%"
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height="auto"
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alt=""/>
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</a><a data-lightbox="group-e62d1b66-7f66-44c5-ba32-c4396e2529ed"
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</a><a data-lightbox="group-default"
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href="_images/screenshot_vmd.jpg"
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class=""
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title=""
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@ -265,7 +265,7 @@ the processor that owns them. The leftmost diagram is the default
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partitioning of the simulation box across processors (one sub-box for
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each of 16 processors); the middle diagram is after a “grid” method
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has been applied.</p>
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<a data-lightbox="group-1ea1982f-2af8-42b4-be30-2e7feb8e77f5"
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<a data-lightbox="group-default"
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href="_images/balance_uniform.jpg"
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class=""
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title=""
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@ -275,7 +275,7 @@ has been applied.</p>
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width="25%"
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height="auto"
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alt=""/>
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</a><a data-lightbox="group-a4b3cf56-edc0-41c1-a22e-57acb6d303e2"
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</a><a data-lightbox="group-default"
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href="_images/balance_nonuniform.jpg"
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class=""
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title=""
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@ -285,7 +285,7 @@ has been applied.</p>
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width="25%"
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height="auto"
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alt=""/>
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</a><a data-lightbox="group-c0259437-bded-4589-b518-4425480db921"
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</a><a data-lightbox="group-default"
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href="_images/balance_rcb.jpg"
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class=""
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title=""
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@ -182,7 +182,7 @@ position of each atom, fj are atomic scattering factors.</p>
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reciprocal lattice nodes. The mesh spacing is defined either (a) by
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the entire simulation domain or (b) manually using selected values as
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shown in the 2D diagram below.</p>
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<a data-lightbox="group-a30c5cda-68d7-4c1b-a26c-5316847c9103"
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<a data-lightbox="group-default"
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href="_images/saed_mesh.jpg"
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class=""
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title=""
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@ -219,7 +219,7 @@ intersecting Ewald sphere. Diffraction intensities will only be
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computed at the intersection of the reciprocal lattice mesh and a
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<em>dR_Ewald</em> thick surface of the Ewald sphere. See the example 3D
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intestiety data and the intersection of a [010] zone axis in the below image.</p>
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<a data-lightbox="group-8fb8943f-067b-4621-ab85-ef00bd1882fd"
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<a data-lightbox="group-default"
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href="_images/saed_ewald_intersect.jpg"
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class=""
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title=""
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@ -167,7 +167,10 @@ dim = 2 or 3 = dimensionality of the simulation, N = number of atoms
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in the group, k = Boltzmann constant, and T = temperature. Note that
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the velocity of each core or shell atom used in the KE calculation is
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the velocity of the center-of-mass (COM) of the core/shell pair the
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atom is part of.</p>
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atom is part of. Note that atoms that are not core or shell particles
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are also included in the temperature calculation (if they are in the
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specified group-ID); they contribute to the total kinetic energy in
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the usual way.</p>
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<p>A kinetic energy tensor, stored as a 6-element vector, is also
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calculated by this compute for use in the computation of a pressure
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tensor. The formula for the components of the tensor is the same as
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@ -41,7 +41,7 @@ For this compute, core and shell particles are specified by two
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respective group IDs, which can be defined using the
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"group"_group.html command. The number of atoms in the two groups
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must be the same and there should be one bond defined between a pair
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of atoms in the two groups.
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of atoms in the two groups.
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The temperature is calculated by the formula KE = dim/2 N k T, where
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KE = total kinetic energy of the group of atoms (sum of 1/2 m v^2),
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@ -49,7 +49,10 @@ dim = 2 or 3 = dimensionality of the simulation, N = number of atoms
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in the group, k = Boltzmann constant, and T = temperature. Note that
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the velocity of each core or shell atom used in the KE calculation is
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the velocity of the center-of-mass (COM) of the core/shell pair the
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atom is part of.
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atom is part of. Note that atoms that are not core or shell particles
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are also included in the temperature calculation (if they are in the
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specified group-ID); they contribute to the total kinetic energy in
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the usual way.
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A kinetic energy tensor, stored as a 6-element vector, is also
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calculated by this compute for use in the computation of a pressure
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@ -185,7 +185,7 @@ the optional <em>LP</em> keyword.</p>
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reciprocal lattice nodes. The mesh spacing is defined either (a)
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by the entire simulation domain or (b) manually using selected values as
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shown in the 2D diagram below.</p>
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<a data-lightbox="group-1bc3f956-68f0-4615-8f93-ca954d919b33"
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<a data-lightbox="group-default"
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href="_images/xrd_mesh.jpg"
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class=""
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title=""
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@ -341,7 +341,7 @@ variable v equal "(0.2*v_y*ylat * cos(v_xx/xlat * 2.0*PI*4.0/v_x) +
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create_atoms 1 box var v set x xx set y yy
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</pre></div>
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</div>
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<a data-lightbox="group-f4ec1fe6-16bb-4d3a-9ef0-ecf4b57f6ec2"
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<a data-lightbox="group-default"
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href="_images/sinusoid.jpg"
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class=""
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title=""
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@ -220,7 +220,7 @@ from an existing dump file, and using these dump commands in the rerun
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script to generate the images/movie.</p>
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<p>Here are two sample images, rendered as 1024x1024 JPEG files. Click
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to see the full-size images:</p>
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<DIV ALIGN=center><a data-lightbox="group-24b43492-ff03-4c03-99b9-12f1dbf252d5"
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<DIV ALIGN=center><a data-lightbox="group-default"
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href="_images/dump1.jpg"
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class=""
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title=""
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@ -230,7 +230,7 @@ to see the full-size images:</p>
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width="25%"
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height="auto"
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alt=""/>
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</a><a data-lightbox="group-2540cc67-71aa-4053-b959-61451a4e4f0d"
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</a><a data-lightbox="group-default"
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href="_images/dump2.jpg"
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class=""
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title=""
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@ -237,7 +237,7 @@ that owns them. The leftmost diagram is the default partitioning of
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the simulation box across processors (one sub-box for each of 16
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processors); the middle diagram is after a “grid” method has been
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applied.</p>
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<a data-lightbox="group-85269663-2cc5-4073-9d2b-e7fb01db4ec3"
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<a data-lightbox="group-default"
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href="_images/balance_uniform.jpg"
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class=""
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title=""
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@ -247,7 +247,7 @@ applied.</p>
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width="25%"
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height="auto"
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alt=""/>
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</a><a data-lightbox="group-349a1bab-83d0-42b4-85c7-81050f4e3d61"
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</a><a data-lightbox="group-default"
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href="_images/balance_nonuniform.jpg"
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class=""
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title=""
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@ -257,7 +257,7 @@ applied.</p>
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width="25%"
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height="auto"
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alt=""/>
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</a><a data-lightbox="group-c6a44ae9-1930-4d73-95ea-e4e0a56b953a"
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</a><a data-lightbox="group-default"
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href="_images/balance_rcb.jpg"
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class=""
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title=""
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@ -479,7 +479,7 @@ barrier.</p>
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neb_combine.py script run on the dump files produced by the two
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example input scripts in examples/neb. Click on them to see a larger
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image.</p>
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<a data-lightbox="group-5916a3a1-a368-4db3-a9ea-37c4eef93ee3"
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<a data-lightbox="group-default"
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href="_images/hop1.jpg"
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class=""
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title=""
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@ -489,7 +489,7 @@ image.</p>
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width="25%"
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height="auto"
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alt=""/>
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</a><a data-lightbox="group-ec426f39-1525-43c6-a3b4-d2aac49c6e80"
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</a><a data-lightbox="group-default"
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href="_images/hop2.jpg"
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class=""
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title=""
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