diff --git a/hugo/content/ex/sim/scatter2d/born-approximation.md b/hugo/content/ex/sim/scatter2d/born-approximation.md
index 1f7c6d9f5e426e8ba5a36e8c7223d3dd376c2933..431bd9ab2244fc4a7a92dc7b5d8f8482009bb1b0 100644
--- a/hugo/content/ex/sim/scatter2d/born-approximation.md
+++ b/hugo/content/ex/sim/scatter2d/born-approximation.md
@@ -1,6 +1,6 @@
 +++
 title = "without DWBA terms"
-weight = 10
+weight = 15
 +++
 
 ## GISAS without DWBA terms
diff --git a/hugo/content/ex/sim/scatter2d/gisas.md b/hugo/content/ex/sim/scatter2d/gisas.md
index 7baddf824cb79b3f11fe1d53a1bde5a79026c33e..b263820058ffdbac8760845c09ea18e9914638cd 100644
--- a/hugo/content/ex/sim/scatter2d/gisas.md
+++ b/hugo/content/ex/sim/scatter2d/gisas.md
@@ -1,6 +1,6 @@
 +++
 title = "GISAS"
-weight = 30
+weight = 10
 +++
 
 ## GISAS simulation example
diff --git a/hugo/content/ex/sim/scatter2d/mc.md b/hugo/content/ex/sim/scatter2d/mc.md
new file mode 100644
index 0000000000000000000000000000000000000000..69d0195cc3cf5c25d92da153f2cb11bfaa0c7642
--- /dev/null
+++ b/hugo/content/ex/sim/scatter2d/mc.md
@@ -0,0 +1,24 @@
++++
+title = "Monte-Carlo"
+weight = 80
++++
+
+## Scattering by large particles with Monte-Carlo integration
+
+Reference: [Monte-Carlo](/ref/sim/setup/options/mc)
+
+This example demonstrates that for large particles (~$1000$ nm) the contribution to the scattered intensity from the form factor oscillates rapidly within one detector bin and analytical calculations (performed for the bin center) give completely a wrong intensity pattern. In this case Monte-Carlo integrations over detector bin should be used.
+
+The simulation generates four plots using different sizes of the particles, (radius $=10$ nm, height $=20$ nm) or (radius $=1$ $\mu$m, height $=2$ $\mu$m), and different calculation methods: analytical calculations or Monte-Carlo integration. The other parameters are identical:
+
+* The sample is made of a monodisperse distribution of cylinders, deposited randomly on a substrate.
+* There is no interference between the scattered waves.
+* The wavelength is equal to 0.1 nm.
+* The incident angles are $\alpha\_i = 0.2 ^{\circ}$ and $\varphi\_i = 0^{\circ}$.
+
+{{< galleryscg >}}
+{{< 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 >}}
+
+{{< show-ex file="scatter2d/LargeParticlesFormFactor.py" >}}
diff --git a/hugo/content/ex/sim/scatter2d/polarized_sans.md b/hugo/content/ex/sim/scatter2d/polarized_sans.md
index 3eba2a187fb3b7bec24fd958eb439335c248f17c..80ed655697b089f6ca3e475d1c1e76e59d02b1c4 100644
--- a/hugo/content/ex/sim/scatter2d/polarized_sans.md
+++ b/hugo/content/ex/sim/scatter2d/polarized_sans.md
@@ -1,6 +1,6 @@
 +++
 title = "Polarized SANS"
-weight = 40
+weight = 45
 +++
 
 ### Polarized SANS
diff --git a/hugo/content/ref/sim/setup/options/mc/index.md b/hugo/content/ref/sim/setup/options/mc/index.md
index 386af4278b62d36a673ed084ea74532b1919044e..7c94acd7603e5fa3b989fe651491df69ac1ca085 100644
--- a/hugo/content/ref/sim/setup/options/mc/index.md
+++ b/hugo/content/ref/sim/setup/options/mc/index.md
@@ -15,20 +15,4 @@ simulation.options().setMonteCarloIntegration(True, n)
 ```
 where `n` is the number of scattering intensity evaluations per pixel.
 
-#### Usage example: large qr
-
-This example demonstrates that for large particles (~$1000$ nm) the contribution to the scattered intensity from the form factor oscillates rapidly within one detector bin and analytical calculations (performed for the bin center) give completely a wrong intensity pattern. In this case Monte-Carlo integrations over detector bin should be used.
-
-The simulation generates four plots using different sizes of the particles, (radius $=10$ nm, height $=20$ nm) or (radius $=1$ $\mu$m, height $=2$ $\mu$m), and different calculation methods: analytical calculations or Monte-Carlo integration. The other parameters are identical:
-
-* The sample is made of a monodisperse distribution of cylinders, deposited randomly on a substrate.
-* There is no interference between the scattered waves.
-* The wavelength is equal to 0.1 nm.
-* The incident angles are $\alpha\_i = 0.2 ^{\circ}$ and $\varphi\_i = 0^{\circ}$.
-
-{{< galleryscg >}}
-{{< 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 >}}
-
-{{< show-ex file="scatter2d/LargeParticlesFormFactor.py" >}}
+Example: [Monte-Carlo](/ex/sim/scatter2d/mc).
\ No newline at end of file