Add SpinW tutorials 12, 13, 14

examples/02_LSWT_CoRh2O4.jl

@@ -74,7 +74,7 @@ swt = SpinWaveTheory(sys_prim; measure=ssf_perp(sys_prim))
 # path that connects high-symmetry points in reciprocal space.
 
 qs = [[0, 0, 0], [1/2, 0, 0], [1/2, 1/2, 0], [0, 0, 0]]
-path = q_space_path(cryst, qs, 400)
+path = q_space_path(cryst, qs, 500)
 
 # Select [`lorentzian`](@ref) broadening with a full-width at half-maximum
 # (FWHM) of 0.8 meV. Use [`ssf_perp`](@ref) to calculate unpolarized scattering

examples/03_LLD_CoRh2O4.jl

@@ -138,7 +138,7 @@ qs = [[3/4, 3/4,   0],
       [1/4,   1, 1/4],
       [  0,   1,   0],
       [  0,  -4,   0]]
-qpts = q_space_path(cryst, qs, 1000)
+qpts = q_space_path(cryst, qs, 500)
 
 # Calculate ``I(𝐪, ω)`` intensities along this path and plot.
 

examples/07_Dipole_Dipole.jl

@@ -38,7 +38,7 @@ plot_spins(sys_prim; ghost_radius=8, color=[:red, :blue, :yellow, :purple])
 
 qs = [[0,0,0], [0,1,0], [1,1/2,0], [1/2,1/2,1/2], [3/4,3/4,0], [0,0,0]]
 labels = ["Γ", "X", "W", "L", "K", "Γ"]
-path = q_space_path(cryst, qs, 400; labels)
+path = q_space_path(cryst, qs, 500; labels)
 
 measure = ssf_trace(sys_prim)
 swt = SpinWaveTheory(sys_prim; measure)

examples/08_Momentum_Conventions.jl

@@ -66,7 +66,7 @@ for _ in 1:nsamples
     end
     add_sample!(sc, sys)
 end
-path = q_space_path(cryst, [[0,0,-1/2], [0,0,+1/2]], 300)
+path = q_space_path(cryst, [[0,0,-1/2], [0,0,+1/2]], 400)
 res1 = intensities(sc, path; energies=:available, kT)
 
 # Calculate the same quantity with linear spin wave theory at ``T = 0``. Because
@@ -76,7 +76,6 @@ res1 = intensities(sc, path; energies=:available, kT)
 sys_small = resize_supercell(sys, (1,1,1))
 minimize_energy!(sys_small)
 swt = SpinWaveTheory(sys_small; measure=ssf_trace(sys_small))
-path = q_space_path(cryst, [[0,0,-1/2], [0,0,+1/2]], 400)
 res2 = intensities_bands(swt, path)
 
 # This model system has a single magnon band with dispersion ``ϵ(𝐪) = 1 - D/B

examples/spinw_tutorials/SW11_La2CuO4.jl

@@ -2,7 +2,7 @@
 # # SW11 - La₂CuO₄
 #
 # This is a Sunny port of [SpinW Tutorial
-# 11](https://spinw.org/tutorials/15tutorial), originally authored by Sandor
+# 11](https://spinw.org/tutorials/11tutorial), originally authored by Sandor
 # Toth. It calculates the spin wave spectrum of La₂CuO₄.
 
 # Load packages 
@@ -14,7 +14,9 @@ using Sunny, GLMakie
 
 units = Units(:meV, :angstrom)
 latvecs = lattice_vectors(1, 1, 10, 90, 90, 90)
-cryst = Crystal(latvecs, [[0, 0, 0]])
+positions = [[0, 0, 0]]
+types = ["Cu"]
+cryst = Crystal(latvecs, positions; types)
 view_crystal(cryst; dims=2)
 
 # Build a spin system using the exchange parameters from [R. Coldea, Phys. Rev.
@@ -45,9 +47,9 @@ energies = range(0, 320, 400)
 swt = SpinWaveTheory(sys; measure=ssf_perp(sys))
 res = intensities(swt, path; energies, kernel=gaussian(fwhm=35))
 res.energies .*= 1.18
-plot_intensities(res)
+plot_intensities(res; units)
 
 # Plot instantaneous itensities, integrated over ω.
 
 res = intensities_instant(swt, path)
-plot_intensities(res; colorrange=(0,20))
+plot_intensities(res; colorrange=(0,20), units)

examples/spinw_tutorials/SW12_Triangular_easy_plane.jl

@@ -0,0 +1,67 @@
+# # SW12 - Triangular lattice with easy plane
+#
+# This is a Sunny port of [SpinW Tutorial
+# 12](https://spinw.org/tutorials/12tutorial), originally authored by Sandor
+# Toth. It calculates the spin wave dispersion of a triangular lattice model
+# with antiferromagnetic interactions and easy-plane single-ion anisotropy.
+
+# Load packages 
+
+using Sunny, GLMakie
+
+# Build a triangular lattice with arbitrary lattice constant of 3 Å.
+
+latvecs = lattice_vectors(3, 3, 4, 90, 90, 120) 
+cryst = Crystal(latvecs, [[0, 0, 0]])
+
+# Build a system with exchange +1 meV along nearest neighbor bonds.
+
+S = 3/2
+J1 = +1.0
+sys = System(cryst, (3,3,1), [SpinInfo(1; S, g=2)], :dipole)
+set_exchange!(sys, J1, Bond(1, 1, [1, 0, 0]))
+
+# Set an easy-axis anisotropy operator ``+D S_z^2`` using
+# [`set_onsite_coupling!`](@ref). **Important note**: When introducing a
+# single-ion anisotropy in `:dipole` mode, Sunny will automatically include a
+# classical-to-quantum correction factor, as described in the document
+# [Interaction Strength Renormalization](@ref). The present single-ion
+# anisotropy is quadratic in the spin operators, so the prescription is to
+# rescale the interaction strength as ``D → (1 - 1/2S) D``. For purposes of this
+# tutorial, our aim is to reproduce the SpinW result, which requires to "undo"
+# Sunny's classical-to-quantum rescaling factor. Another way to achieve the same
+# thing is to select system mode `:dipole_large_S` instead of `:dipole`.
+
+undo_classical_to_quantum_rescaling = 1 / (1 - 1/2S)
+D = 0.2 * undo_classical_to_quantum_rescaling
+set_onsite_coupling!(sys, S -> D*S[3]^2, 1)
+randomize_spins!(sys)
+minimize_energy!(sys)
+plot_spins(sys; dims=2)
+
+# Plot the spin wave spectrum for a path through ``𝐪``-space.
+
+qs = [[0, 0, 0], [1, 1, 0]]
+path = q_space_path(cryst, qs, 400)
+swt = SpinWaveTheory(sys; measure=ssf_perp(sys))
+res = intensities_bands(swt, path)
+plot_intensities(res)
+
+# To select a specific linear combination of spin structure factor (SSF)
+# components in global Cartesian coordinates, one can use [`ssf_custom`](@ref).
+# Here we calculate and plot the real part of ``\mathcal{S}^{zz}(𝐪, ω)``.
+
+measure = ssf_custom(sys) do q, ssf
+    return real(ssf[3, 3])
+end
+swt = SpinWaveTheory(sys; measure)
+res = intensities_bands(swt, path)
+plot_intensities(res)
+
+# It's also possible to get data for the full 3×3 SSF. For example, this is the
+# SSF for the 7th energy band, at the 10th ``𝐪``-point along the path.
+
+measure = ssf_custom((q, ssf) -> ssf, sys)
+swt = SpinWaveTheory(sys; measure)
+res = intensities_bands(swt, path)
+res.data[7, 10]

examples/spinw_tutorials/SW13_LiNiPO4.jl

@@ -0,0 +1,94 @@
+# # SW13 - LiNiPO₄
+#
+# This is a Sunny port of [SpinW Tutorial
+# 13](https://spinw.org/tutorials/13tutorial), originally authored by Sandor
+# Toth. It calculates the spin wave spectrum of LiNiPO₄.
+
+# Load packages 
+
+using Sunny, GLMakie
+
+# Build an orthorhombic lattice and populate the Ni atoms according to
+# spacegroup 62 (Pnma).
+
+units = Units(:meV, :angstrom)
+a = 10.02
+b = 5.86
+c = 4.68
+latvecs = lattice_vectors(a, b, c, 90, 90, 90)
+positions = [[1/4, 1/4, 0]]
+types = ["Ni"]
+cryst = Crystal(latvecs, positions, 62, setting=""; types)
+view_crystal(cryst)
+
+# Create a system with exchange parameters taken from [T. Jensen, et al., PRB
+# **79**, 092413 (2009)](https://doi.org/10.1103/PhysRevB.79.092413). The
+# corrected anisotropy values are taken from the thesis of T. Jensen. The mode
+# `:dipole_large_S` avoids a [classical-to-quantum rescaling factor](@ref
+# "Interaction Strength Renormalization") of anisotropy strengths, as needed for
+# consistency with the original fits.
+
+S = 3/2
+sys = System(cryst, (1,1,1), [SpinInfo(1, S=1, g=2)], :dipole_large_S)
+Jbc =  1.036
+Jb  =  0.6701
+Jc  = -0.0469
+Jac = -0.1121
+Jab =  0.2977
+Da  =  0.1969
+Db  =  0.9097
+set_exchange!(sys, Jbc, Bond(2, 3, [0, 0, 0]))
+set_exchange!(sys, Jc, Bond(1, 1, [0, 0, -1]))
+set_exchange!(sys, Jb, Bond(1, 1, [0, 1, 0]))
+set_exchange!(sys, Jab, Bond(1, 2, [0, 0, 0]))
+set_exchange!(sys, Jab, Bond(3, 4, [0, 0, 0]))
+set_exchange!(sys, Jac, Bond(3, 1, [0, 0, 0]))
+set_exchange!(sys, Jac, Bond(4, 2, [0, 0, 0]))
+set_onsite_coupling!(sys, S -> Da*S[1]^2 + Db*S[2]^2, 1)
+
+# Energy minimization yields a co-linear order along the ``c`` axis.
+
+randomize_spins!(sys)
+minimize_energy!(sys)
+plot_spins(sys; color=[s[3] for s in sys.dipoles])
+
+# Calculate the spectrum along path [ξ, 1, 0]
+
+swt = SpinWaveTheory(sys; measure=ssf_perp(sys))
+qs = [[0, 1, 0], [2, 1, 0]]
+path = q_space_path(cryst, qs, 400)
+res = intensities_bands(swt, path)
+fig = Figure(size=(768, 300))
+plot_intensities!(fig[1, 1], res; units);
+
+# There are two physical bands with nonvanishing intensity. To extract these
+# intensity curves, we must filter out the additional bands with zero intensity.
+# One way is to sort the data along dimension 1 (the band index) with the
+# comparison operator "is intensity less than ``10^{-12}``". Doing so moves the
+# physical bands to the end of the array axis. Call the [Makie `lines!`
+# function](https://docs.makie.org/stable/reference/plots/lines) to make a
+# custom plot.
+
+data_sorted = sort(res.data; dims=1, by= >(1e-12))
+ax = Axis(fig[1, 2], xlabel="Momentum (r.l.u.)", ylabel="Intensity",
+          xticks=res.qpts.xticks, xticklabelrotation=π/6)
+lines!(ax, data_sorted[end, :]; label="Lower band")
+lines!(ax, data_sorted[end-1, :]; label="Upper band")
+axislegend(ax)
+fig
+
+# Make the same plots along path [0, 1, ξ]
+
+qs =  [[0, 1, 0], [0, 1, 2]]
+path = q_space_path(cryst, qs, 400)
+res = intensities_bands(swt, path)
+fig = Figure(size=(768, 300))
+plot_intensities!(fig[1, 1], res; units)
+
+data_sorted = sort(res.data; dims=1, by=x->abs(x)>1e-12)
+ax = Axis(fig[1, 2], xlabel="Momentum (r.l.u.)", ylabel="Intensity",
+          xticks=res.qpts.xticks, xticklabelrotation=π/6)
+lines!(ax, data_sorted[end, :]; label="Lower band")
+lines!(ax, data_sorted[end-1, :]; label="Upper band")
+axislegend(ax)
+fig

examples/spinw_tutorials/SW14_YVO3.jl

@@ -0,0 +1,69 @@
+# # SW14 - YVO₃
+#
+# This is a Sunny port of [SpinW Tutorial
+# 14](https://spinw.org/tutorials/14tutorial), originally authored by Sandor
+# Toth. It calculates the spin wave spectrum of YVO₃.
+
+# Load packages
+
+using Sunny, GLMakie
+
+# Build an orthorhombic lattice and populate the V atoms according to the
+# pseudocubic unit cell, doubled along the c-axis. The listed spacegroup of the
+# YVO₃ chemical cell is international number 62. It has been observed, however,
+# that the exchange interactions break this symmetry. For this reason, disable
+# all symmetry analysis by selecting spacegroup 1 (P1).
+
+units = Units(:meV, :angstrom)
+a = 5.2821 / sqrt(2)
+b = 5.6144 / sqrt(2)
+c = 7.5283
+latvecs = lattice_vectors(a, b, c, 90, 90, 90)
+positions = [[0, 0, 0], [0, 0, 1/2]]
+types = ["V", "V"]
+cryst = Crystal(latvecs, positions, 1; types)
+
+# Create a system following the model of [C. Ulrich, et al. PRL **91**, 257202
+# (2003)](https://doi.org/10.1103/PhysRevLett.91.257202). The mode
+# `:dipole_large_S` avoids a [classical-to-quantum rescaling factor](@ref
+# "Interaction Strength Renormalization") of anisotropy strengths, as needed for
+# consistency with the original fits.
+
+sys = System(cryst, (2,2,1), [SpinInfo(1, S=1/2, g=2), SpinInfo(2, S=1/2, g=2)], :dipole_large_S)
+Jab = 2.6
+Jc  = 3.1
+δ   = 0.35
+K1  = 0.90
+K2  = 0.97
+d   = 1.15
+Jc1 = [-Jc*(1+δ)+K2 0 -d; 0 -Jc*(1+δ) 0; +d 0 -Jc*(1+δ)]
+Jc2 = [-Jc*(1-δ)+K2 0 +d; 0 -Jc*(1-δ) 0; -d 0 -Jc*(1-δ)]
+set_exchange!(sys, Jab, Bond(1, 1, [1, 0, 0]))
+set_exchange!(sys, Jab, Bond(2, 2, [1, 0, 0]))
+set_exchange!(sys, Jc1, Bond(1, 2, [0, 0, 0]))
+set_exchange!(sys, Jc2, Bond(2, 1, [0, 0, 1]))
+set_exchange!(sys, Jab, Bond(1, 1, [0, 1, 0]))
+set_exchange!(sys, Jab, Bond(2, 2, [0, 1, 0]))
+set_onsite_coupling!(sys, S -> -K1*S[1]^2, 1)
+set_onsite_coupling!(sys, S -> -K1*S[1]^2, 2)
+
+# When using spacegroup P1, there is no symmetry-propagation of interactions
+# because all bonds are considered inequivalent. One can visualize the
+# interactions in the system by clicking the toggles in the
+# [`view_crystal`](@ref) GUI.
+
+view_crystal(sys)
+
+# Energy minimization yields a Néel order with canting
+
+randomize_spins!(sys)
+minimize_energy!(sys)
+plot_spins(sys)
+
+# Plot the spin wave spectrum along a path
+
+swt = SpinWaveTheory(sys; measure=ssf_perp(sys))
+qs = [[0.75, 0.75, 0], [0.5, 0.5, 0], [0.5, 0.5, 1]]
+path = q_space_path(cryst, qs, 400)
+res = intensities_bands(swt, path)
+plot_intensities(res; units)

examples/spinw_tutorials/SW18_Distorted_kagome.jl

@@ -77,7 +77,7 @@ energy_per_site(sys2) # < -0.7834 meV
 # Define a path in q-space
 
 qs = [[0,0,0], [1,0,0]]
-path = q_space_path(cryst, qs, 512)
+path = q_space_path(cryst, qs, 400)
 
 # Calculate intensities for the incommensurate spiral phase using
 # [`SpiralSpinWaveTheory`](@ref). It is necessary to provide the original `sys`,
@@ -93,7 +93,7 @@ plot_intensities(res; units)
 radii = range(0, 2, 100) # (1/Å)
 energies = range(0, 6, 200)
 kernel = gaussian(fwhm=0.05)
-res = powder_average(cryst, radii, 200) do qs
+res = powder_average(cryst, radii, 400) do qs
     intensities(swt, qs; energies, kernel)
 end
 plot_intensities(res; units)

examples/spinw_tutorials/SW19_Different_Ions.jl

@@ -39,7 +39,7 @@ plot_spins(sys)
 
 swt = SpinWaveTheory(sys; measure=ssf_perp(sys))
 qs = [[0,0,0], [1,0,0]]
-path = q_space_path(cryst, qs, 512)
+path = q_space_path(cryst, qs, 400)
 
 # Plot three types of pair correlation intensities