build based on ec1a509

dev/.documenter-siteinfo.json

@@ -1 +1 @@
-{"documenter":{"julia_version":"1.9.3","generation_timestamp":"2023-10-31T16:49:55","documenter_version":"1.1.2"}}
+{"documenter":{"julia_version":"1.9.3","generation_timestamp":"2023-11-01T03:44:35","documenter_version":"1.1.2"}}

dev/assets/notebooks/fei2_tutorial.ipynb → dev/assets/notebooks/01_LSWT_SU3_FeI2.ipynb

@@ -3,7 +3,7 @@
   {
    "cell_type": "markdown",
    "source": [
-    "# Case Study: FeI₂\n",
+    "# 1. Multi-flavor spin wave simulations of FeI₂ (Showcase)\n",
     "\n",
     "FeI₂ is an effective spin-1 material with strong single-ion anisotropy.\n",
     "Quadrupolar fluctuations give rise to a single-ion bound state that cannot be\n",
@@ -46,8 +46,8 @@
     "guide. Sunny requires Julia 1.9 or later.\n",
     "\n",
     "From the Julia prompt, load `Sunny`. For plotting, one can choose either\n",
-    "`GLMakie` (a pop-up window) or `WGLMakie` (inline plots for a Jupyter notebook\n",
-    "or VSCode)."
+    "`GLMakie` (a pop-up window) or `WGLMakie` (inline plots for a Jupyter\n",
+    "notebook)."
    ],
    "metadata": {}
   },
@@ -125,7 +125,7 @@
   {
    "cell_type": "markdown",
    "source": [
-    "Observe that `cryst` retains the spacegroup symmetry of the full FeI₂ crystal.\n",
+    "Importantly, `cryst` retains the spacegroup symmetry of the full FeI₂ crystal.\n",
     "This information will be used, for example, to propagate exchange interactions\n",
     "between symmetry-equivalent bonds.\n",
     "\n",
@@ -733,21 +733,15 @@
     "The full SU(_N_) coherent state dynamics, with appropriate quantum correction\n",
     "factors, can be useful to model finite temperature scattering data. In\n",
     "particular, it captures certain anharmonic effects due to thermal\n",
-    "fluctuations. This is the subject of our FeI₂ at Finite Temperature\n",
-    "tutorial.\n",
+    "fluctuations. See our [generalized spin dynamics tutorial](@ref \"3.\n",
+    "Generalized spin dynamics of FeI₂ at finite *T*\").\n",
     "\n",
     "The classical dynamics is also a good starting point to study non-equilibrium\n",
     "phenomena. Empirical noise and damping terms can be used to model [coupling to\n",
     "a thermal bath](https://arxiv.org/abs/2209.01265). This yields a Langevin\n",
-    "dynamics of SU(_N_) coherent states. Our CP² Skyrmion Quench\n",
-    "tutorial shows how this dynamics gives rise to the formation of novel\n",
-    "topological defects in a temperature quench.\n",
-    "\n",
-    "Relative to LSWT calculations, it can take much more time to estimate\n",
-    "$\\mathcal{S}(𝐪,ω)$ intensities using classical dynamics simulation. See the\n",
-    "[SunnyTutorials\n",
-    "notebooks](https://nbviewer.org/github/SunnySuite/SunnyTutorials/tree/main/Tutorials/)\n",
-    "for examples of \"production-scale\" simulations."
+    "dynamics of SU(_N_) coherent states. Our [dynamical SU(_N_) quench](@ref \"5.\n",
+    "Dynamical quench into CP² skyrmion liquid\") tutorial illustrates how a\n",
+    "temperature quench can give rise to novel liquid phase of CP² skyrmions."
    ],
    "metadata": {}
   }

dev/assets/notebooks/powder_averaging.ipynb → dev/assets/notebooks/02_LSWT_CoRh2O4.ipynb

@@ -3,12 +3,12 @@
   {
    "cell_type": "markdown",
    "source": [
-    "# Powder Averaged CoRh₂O₄\n",
+    "# 2. Spin wave simulations of CoRh₂O₄\n",
     "\n",
-    "This tutorial illustrates the calculation of the powder-averaged structure\n",
-    "factor by performing an orientational average. We consider a simple model of\n",
-    "the diamond-cubic crystal CoRh₂O₄, with parameters extracted from [Ge et al.,\n",
-    "Phys. Rev. B 96, 064413](https://doi.org/10.1103/PhysRevB.96.064413)."
+    "This tutorial illustrates the conventional spin wave theory of dipoles. We\n",
+    "consider a simple model of the diamond-cubic crystal CoRh₂O₄, with parameters\n",
+    "extracted from [Ge et al., Phys. Rev. B 96,\n",
+    "064413](https://doi.org/10.1103/PhysRevB.96.064413)."
    ],
    "metadata": {}
   },
@@ -64,21 +64,20 @@
   {
    "cell_type": "markdown",
    "source": [
-    "Construct a `System` with an antiferromagnetic nearest neighbor\n",
-    "interaction `J`. Because the diamond crystal is bipartite, the ground state\n",
-    "will have unfrustrated Néel order. Selecting `latsize=(1,1,1)` is sufficient\n",
-    "because the ground state is periodic over each cubic unit cell. By passing an\n",
-    "explicit `seed`, the system's random number generator will give repeatable\n",
-    "results."
+    "Construct a `System` with quantum spin $S=3/2$ constrained to the\n",
+    "space of dipoles. Including an antiferromagnetic nearest neighbor interaction\n",
+    "`J` will favor Néel order. To optimize this magnetic structure, it is\n",
+    "sufficient to employ a magnetic lattice consisting of a single crystal unit\n",
+    "cell, `latsize=(1,1,1)`. Passing an explicit random number `seed` will ensure\n",
+    "repeatable results."
    ],
    "metadata": {}
   },
   {
    "outputs": [],
    "cell_type": "code",
    "source": [
-    "latsize = (2, 2, 2)\n",
-    "seed = 0\n",
+    "latsize = (1, 1, 1)\n",
     "S = 3/2\n",
     "J = 7.5413*meV_per_K # (~ 0.65 meV)\n",
     "sys = System(cryst, latsize, [SpinInfo(1; S, g=2)], :dipole; seed=0)\n",
@@ -190,7 +189,7 @@
    "outputs": [],
    "cell_type": "code",
    "source": [
-    "qpoints = [[0.0, 0.0, 0.0], [0.5, 0.0, 0.0], [0.5, 0.5, 0.0], [0.0, 0.0, 0.0]]\n",
+    "qpoints = [[0, 0, 0], [1/2, 0, 0], [1/2, 1/2, 0], [0, 0, 0]]\n",
     "path, xticks = reciprocal_space_path(cryst, qpoints, 50)\n",
     "energies = collect(0:0.01:6)\n",
     "is = intensities_broadened(swt, path, energies, formula)\n",