hugo: mv all drawings to static/img/draw

hugo/content/ex/sim/gisas-no-dwba-terms/index.md

@@ -15,7 +15,7 @@ In consequence, there are no reflections,
 and therefore the DWBA boils down to the ordinary Born approximation.
 
 {{< galleryscg >}}
-{{< figscg src="CylindersInBA_setup.jpg" width="350px" caption="Real-space model">}}
+{{< figscg src="/img/draw/CylindersInBA_setup.jpg" width="350px" caption="Real-space model">}}
 {{< figscg src="/img/auto/scatter2d/CylindersInBA.png" width="350px" caption="Intensity image">}}
 {{< /galleryscg >}}
 

hugo/content/ex/sim/gisas/_index.md

@@ -11,7 +11,7 @@ we take a standard sample model from module
 a dilute random assembly of monodisperse cylindrical disks on a substrate.
 
 {{< galleryscg >}}
-{{< figscg src="CylindersInDWBA_setup.jpg" width="350px" caption="Real-space model">}}
+{{< figscg src="/img/draw/CylindersInDWBA_setup.jpg" width="350px" caption="Real-space model">}}
 {{< figscg src="/img/auto/scatter2d/Cylinders.png" width="350px" caption="Intensity image">}}
 {{< /galleryscg >}}
 

hugo/content/py/fitting/extended/experiment-at-galaxi/index.md

@@ -8,7 +8,7 @@ weight = 30
 This is an example of a real data fit. We use our own measurements performed at the laboratory diffractometer [GALAXI](http://www.fz-juelich.de/jcns/jcns-2//DE/Leistungen/GALAXI/_node.html) in Forschungszentrum Jülich.
 
 {{< galleryscg >}}
-{{< figscg src="FitGALAXIData_setup.jpg" width="350px" caption="Real-space model">}}
+{{< figscg src="/img/draw/FitGALAXIData_setup.jpg" width="350px" caption="Real-space model">}}
 {{< figscg src="FitGALAXIData.png" width="350px" caption="Fit window">}}
 {{< /galleryscg >}}
 

hugo/content/ref/instr/beam/divergence/index.md

@@ -18,7 +18,7 @@ The DWBA simulation is shown for a standard sample model:
   hence there is no interference between scattered waves.
 
 {{< galleryscg >}}
-{{< figscg src="BeamDivergence_setup.jpg" width="350px" caption="Real-space model">}}
+{{< figscg src="/img/draw/BeamDivergence_setup.jpg" width="350px" caption="Real-space model">}}
 {{< figscg src="/img/auto/scatter2d/BeamDivergence.png" width="350px" caption="Intensity image">}}
 {{< /galleryscg >}}
 

hugo/content/ref/sample/interference/grating/cosine-ripples-at-rect-lattice/index.md

@@ -15,7 +15,7 @@ Scattering from elongated particles positioned in a two-dimensional rectangular
 * The incident angles are $\alpha\_i = 0.3 ^{\circ}$ and $\varphi\_i = 0^{\circ}$.
 
 {{< galleryscg >}}
-{{< figscg src="CosineRipplesAtRectLattice_setup.jpg" width="350px" caption="Real-space model">}}
+{{< figscg src="/img/draw/CosineRipplesAtRectLattice_setup.jpg" width="350px" caption="Real-space model">}}
 {{< figscg src="/img/auto/scatter2d/CosineRipplesAtRectLattice.png" width="350px" caption="Intensity image">}}
 {{< /galleryscg >}}
 

hugo/content/ref/sample/interference/grating/lattice1d/index.md

@@ -15,8 +15,8 @@ In this example we simulate the scattering from infinite 1D repetition of rectan
 * To avoid the problem of rapidly oscillating form factors of long boxes (see [this example](/ref/sim/setup/options/mc) for more details), the simulation is performed in monte carlo integration mode.
 
 {{< galleryscg >}}
-{{< figscg src="Interference1DLattice_setup.jpg" width="200px" caption="Real-space model">}}
-{{< figscg src="Interference1DLattice_sketch.jpg" width="200px" caption="Sketch">}}
+{{< figscg src="/img/draw/Interference1DLattice_setup.jpg" width="200px" caption="Real-space model">}}
+{{< figscg src="/img/draw/Interference1DLattice_sketch.jpg" width="200px" caption="Sketch">}}
 {{< figscg src="/img/auto/scatter2d/Interference1DLattice.png" width="200px" caption="Intensity image">}}
 {{< /galleryscg >}}
 
@@ -27,7 +27,7 @@ In this example we simulate the scattering from infinite 1D repetition of rectan
 
 A one dimensional lattice can be viewed as a chain of particles placed at regular intervals on a single axis. The plot below represents one possible use case, where infinitely long (or very long) boxes are placed at nodes of a 1d lattice to form a grating.
 
-{{< figscg src="particles_at_1d_latice.jpg" width="600px" class="center">}}
+{{< figscg src="/img/draw/particles_at_1d_latice.jpg" width="600px" class="center">}}
 
 See the BornAgain user manual (Chapter 3.4.1, One Dimensional Lattice) for details about the theory.
 

hugo/content/ref/sample/interference/incoherent-ex/index.md

@@ -18,7 +18,7 @@ Scattering from a mixture of cylinders and prisms without interference.
 * The simulation is performed using the Distorted Wave Born Approximation (due to the presence of a substrate).
 
 {{< galleryscg >}}
-{{< figscg src="CylindersAndPrisms_setup.jpg" width="350px" caption="Real-space model">}}
+{{< figscg src="/img/draw/CylindersAndPrisms_setup.jpg" width="350px" caption="Real-space model">}}
 {{< figscg src="/img/auto/scatter2d/CylindersAndPrisms.png" width="350px" caption="Intensity image">}}
 {{< /galleryscg >}}
 

hugo/content/ref/sample/interference/lattice2d/_index.md

@@ -7,7 +7,7 @@ weight = 20
 
 The interference function of a two-dimensional lattice is used to model the scattering from particles positioned at some regular intervals.
 
-{{< figscg src="particles_at_lattice.jpg" width="600px" class="center">}}
+{{< figscg src="/img/draw/particles_at_lattice.jpg" width="600px" class="center">}}
 
 The generated layout, the lattice, is characterised by two basis vectors $a$ and $b$ (in real space) and the angle between these two vectors. The finite size effects and/or divergence of the lattice from an ideal crystal are modelled with the help of two-dimensional decay functions.
 

hugo/content/ref/sample/interference/lattice2d/hexagonal-lattice-with-basis/index.md

@@ -16,7 +16,7 @@ Scattering from two hexagonal close packed layers of spheres.
 * The incident angles are $\alpha\_i = 0.2 ^{\circ}$ and $\varphi\_i = 0^{\circ}$.
 
 {{< galleryscg >}}
-{{< figscg src="HexagonalLatticesWithBasis_setup.jpg" width="350px" caption="Real-space model">}}
+{{< figscg src="/img/draw/HexagonalLatticesWithBasis_setup.jpg" width="350px" caption="Real-space model">}}
 {{< figscg src="/img/auto/scatter2d/HexagonalLatticesWithBasis.png" width="350px" caption="Intensity image">}}
 {{< /galleryscg >}}
 

hugo/content/ref/sample/interference/lattice2d/interference-2d-rotated-square-lattice/index.md

@@ -10,7 +10,7 @@ whose main axes are rotated with respect to the reference cartesian frame.
 
 
 {{< galleryscg >}}
-{{< figscg src="Interference2DRotatedSquareLattice_setup.jpg" width="350px" caption="Real-space model">}}
+{{< figscg src="/img/draw/Interference2DRotatedSquareLattice_setup.jpg" width="350px" caption="Real-space model">}}
 {{< figscg src="/img/auto/scatter2d/Interference2DRotatedSquareLattice.png" width="350px" caption="Intensity image">}}
 {{< /galleryscg >}}
 

hugo/content/ref/sample/interference/lattice2d/spheres-at-hex-lattice/index.md

@@ -14,7 +14,7 @@ and positioned in a hexagonal lattice.
 * The incident angles are $\alpha\_i = 0.2 ^{\circ}$ and $\varphi\_i = 0^{\circ}$.
 
 {{< galleryscg >}}
-{{< figscg src="SpheresAtHexLattice_setup.jpg" width="350px" caption="Real-space model">}}
+{{< figscg src="/img/draw/SpheresAtHexLattice_setup.jpg" width="350px" caption="Real-space model">}}
 {{< figscg src="/img/auto/scatter2d/SpheresAtHexLattice.png" width="350px" caption="Intensity image">}}
 {{< /galleryscg >}}
 

hugo/content/ref/sample/interference/lattice2d/with-basis/index.md

@@ -16,7 +16,7 @@ Scattering from cylinders positioned in a squared centered lattice.
 * The incident angles are $\alpha\_i = 0.2 ^{\circ}$ and $\varphi\_i = 0^{\circ}$.
 
 {{< galleryscg >}}
-{{< figscg src="Interference2DCenteredSquareLattice_setup.jpg" width="350px" caption="Real-space model">}}
+{{< figscg src="/img/draw/Interference2DCenteredSquareLattice_setup.jpg" width="350px" caption="Real-space model">}}
 {{< figscg src="/img/auto/scatter2d/Interference2DCenteredSquareLattice.png" width="350px" caption="Intensity image">}}
 {{< /galleryscg >}}
 

hugo/content/ref/sample/particle/composition/core-shell/index.md

@@ -15,7 +15,7 @@ Scattering from cuboidal core-shell particles.
 * The incident angles are $\alpha\_i = 0.2 ^{\circ}$ and $\varphi\_i = 0^{\circ}$.
 
 {{< galleryscg >}}
-{{< figscg src="CoreShellNanoparticles_setup.jpg" width="350px" caption="Real-space model">}}
+{{< figscg src="/img/draw/CoreShellNanoparticles_setup.jpg" width="350px" caption="Real-space model">}}
 {{< figscg src="/img/auto/scatter2d/CoreShellNanoparticles.png" width="350px" caption="Intensity image">}}
 {{< /galleryscg >}}
 

hugo/content/ref/sample/particle/ff/custom/index.md

@@ -15,7 +15,7 @@ Scattering from a monodisperse distribution of particles, whose form factor is d
 * The incident angles are $\alpha\_i = 0.2 ^{\circ}$ and $\varphi\_i = 0^{\circ}$.
 
 {{< galleryscg >}}
-{{< figscg src="CustomFormFactor_setup.jpg" width="350px" caption="Real-space model">}}
+{{< figscg src="/img/draw/CustomFormFactor_setup.jpg" width="350px" caption="Real-space model">}}
 {{< figscg src="/img/auto/scatter2d/CustomFormFactor.png" width="350px" caption="Intensity image">}}
 {{< /galleryscg >}}
 

hugo/content/ref/sample/particle/positioning/positioning-ex/index.md

@@ -15,7 +15,7 @@ Scattering from a sample containing spherical embedded particles.
 * The incident angles are $\alpha\_i = 0.15 ^{\circ}$ and $\varphi\_i = 0^{\circ}$.
 
 {{< galleryscg >}}
-{{< figscg src="BuriedParticles_setup.jpg" width="350px" caption="Real-space model">}}
+{{< figscg src="/img/draw/BuriedParticles_setup.jpg" width="350px" caption="Real-space model">}}
 {{< figscg src="/img/auto/scatter2d/BuriedParticles.png" width="350px" caption="Intensity image">}}
 {{< /galleryscg >}}
 

hugo/content/ref/sample/particle/rotation/rotation-ex/index.md

@@ -17,7 +17,7 @@ This example illustrates how the in-plane rotation of non-radially symmetric par
 * The incident angles are $\alpha\_i = 0.2 ^{\circ}$ and $\varphi\_i = 0^{\circ}$.
 
 {{< galleryscg >}}
-{{< figscg src="RotatedPyramids_setup.jpg" width="350px" caption="Real-space model">}}
+{{< figscg src="/img/draw/RotatedPyramids_setup.jpg" width="350px" caption="Real-space model">}}
 {{< figscg src="/img/auto/scatter2d/RotatedPyramids.png" width="350px" caption="Intensity image">}}
 {{< /galleryscg >}}
 

hugo/content/ref/sample/roughness/specular/index.md

@@ -14,7 +14,7 @@ roughness is characterized by root-mean-square deviation from the mean surface p
 $\sigma = 1$ nm.
 
 {{< galleryscg >}}
-{{< figscg src="SpecularSimulationWithRoughnessSetup.jpg" width="350px" caption="Real-space model">}}
+{{< figscg src="/img/draw/SpecularSimulationWithRoughnessSetup.jpg" width="350px" caption="Real-space model">}}
 {{< figscg src="/img/auto/specular/SpecularSimulationWithRoughness.png" width="350px" caption="Intensity image">}}
 {{< /galleryscg >}}
 

hugo/content/ref/sim/setup/options/mc/index.md

@@ -27,7 +27,7 @@ The simulation generates four plots using different sizes of the particles, (rad
 * The incident angles are $\alpha\_i = 0.2 ^{\circ}$ and $\varphi\_i = 0^{\circ}$.
 
 {{< galleryscg >}}
-{{< figscg src="LargeParticlesFormFactor_setup.jpg" width="700px" caption="Real-space model">}}
+{{< figscg src="/img/draw/LargeParticlesFormFactor_setup.jpg" width="700px" caption="Real-space model">}}
 {{< figscg src="/img/auto/scatter2d/LargeParticlesFormFactor.png" width="350px" caption="Intensity image">}}
 {{< /galleryscg >}}