Fixed LaTeX compilation. Added microwave field docs.

Author: aibergman

content/conf.py

@@ -84,6 +84,9 @@
     "conf_py_path": conf_py_path,
 }
 
+# Use XeLaTeX for better Unicode support when building PDF
+latex_engine = 'xelatex'
+
 # Intersphinx mapping.  For example, with this you can use
 # :py:mod:`multiprocessing` to link straight to the Python docs of that module.
 # List all available references:

content/detailed-input-background.rst

@@ -70,6 +70,7 @@ Spatially and temporally varying magnetic fields
 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~
 
 - :doc:`stimuli/fields`
+- :doc:`stimuli/microwave_fields`
 
 Spin-polarized currents and torques
 ~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

content/methods/wang-landau.rst

@@ -91,7 +91,7 @@ the total energy window:
 
 .. math::
 
-   \sigma_E = \text{wl_sigma} \times N_{\text{hist}} \times \Delta E
+   \sigma_E = \text{wl\_sigma} \times N_{\text{hist}} \times \Delta E
 
 This broadening helps smooth the DOS and ensures that nearby energy bins are
 updated simultaneously, reducing statistical noise.
@@ -112,8 +112,8 @@ The final energy window is then adjusted by cutoff factors ``wl_lcut`` and ``wl_
 
 .. math::
 
-   E_{\text{min}}^{\text{final}} &= \text{wl_lcut} \times E_{\text{min}} \\
-   E_{\text{max}}^{\text{final}} &= \text{wl_hcut} \times E_{\text{max}}
+   E_{\text{min}}^{\text{final}} &= \text{wl\_lcut} \times E_{\text{min}} \\
+   E_{\text{max}}^{\text{final}} &= \text{wl\_hcut} \times E_{\text{max}}
 
 If ``wl_emin`` and ``wl_emax`` are explicitly provided in the input file, the
 automatic energy window determination is skipped.
@@ -165,7 +165,7 @@ wl_hcut
    Higher cutoff factor for the automatic energy window. The automatically determined :math:`E_{\\text{max}}` is multiplied by this factor to set the final upper bound. Values less than 1.0 reduce the energy window. Default: **0.950**.
 
 wl_sigma
-   Broadening width (in units of the energy window) for the Gaussian kernel applied during DOS updates. The broadening in energy units is :math:`\\sigma_E = \\text{wl_sigma} \\times N_{\\text{hist}} \\times \\Delta E`. Larger values smooth the DOS more aggressively but may reduce fine structure. Default: **0.005**.
+   Broadening width (in units of the energy window) for the Gaussian kernel applied during DOS updates. The broadening in energy units is :math:`\\sigma_E = \\text{wl\\_sigma} \\times N_{\\text{hist}} \\times \\Delta E`. Larger values smooth the DOS more aggressively but may reduce fine structure. Default: **0.005**.
 
 wl_gfac
    Global prefactor applied to the final density of states. Used for rescaling or normalization. Default: **1.0**.

content/observables/correlations.rst

@@ -59,23 +59,23 @@ Proper sampling of :math:`S(\mathbf{q},\omega)` requires careful choice of:
 
    .. math::
 
-      \omega_{\max} = \frac{\pi}{\text{timestep} \times \text{sc_step}}
+      \omega_{\max} = \frac{\pi}{\text{timestep} \times \text{sc\_step}}
 
 2. **Number of temporal samples** ``sc_nstep``: Controls frequency resolution
 
    .. math::
 
-      \Delta \omega = \frac{2\omega_{\max}}{N_{\text{step}}} = \frac{2\pi}{N_{\text{step}} \times \text{timestep} \times \text{sc_step}}
+      \Delta \omega = \frac{2\omega_{\max}}{N_{\text{step}}} = \frac{2\pi}{N_{\text{step}} \times \text{timestep} \times \text{sc\_step}}
 
 3. **Total sampling time**: Determines lowest frequency accessed
 
    .. math::
 
-      t_{\max} = \text{sc_nstep} \times \text{timestep} \times \text{sc_step}
+      t_{\max} = \text{sc\_nstep} \times \text{timestep} \times \text{sc\_step}
 
    .. math::
 
-      \omega_{\min} = \frac{2\pi}{t_{\max}} = \frac{2\pi}{N_{\text{step}} \times \text{timestep} \times \text{sc_step}}
+      \omega_{\min} = \frac{2\pi}{t_{\max}} = \frac{2\pi}{N_{\text{step}} \times \text{timestep} \times \text{sc\_step}}
 
 4. **q-point mesh**: Determines spatial resolution and Brillouin zone coverage
 
@@ -89,10 +89,10 @@ do_sr
    Sample static correlation :math:`G(\mathbf{r})` in real space directly (Y=yes, N=no). When enabled, :math:`C(\mathbf{r},0)` is computed without requiring a q-point mesh.
 
 sc_step
-   Number of MD/MC steps between temporal correlation samples; controls maximum frequency :math:`\omega_{\max} = \pi / (\text{timestep} \times \text{sc_step})`. Default: **10**.
+   Number of MD/MC steps between temporal correlation samples; controls maximum frequency :math:`\omega_{\max} = \pi / (\text{timestep} \times \text{sc\_step})`. Default: **10**.
 
 sc_nstep
-   Number of temporal samples collected for each correlation measurement. Controls frequency resolution :math:`\Delta \omega = 2\pi / (N_{\text{step}} \times \text{timestep} \times \text{sc_step})`. Default: **100**.
+   Number of temporal samples collected for each correlation measurement. Controls frequency resolution :math:`\Delta \omega = 2\pi / (N_{\text{step}} \times \text{timestep} \times \text{sc\_step})`. Default: **100**.
 
 sc_sep
    Number of steps between independent correlation measurements (used when ``do_sc = C``). Default: **1**.

content/stimuli/currents.rst

@@ -55,7 +55,7 @@ In this case:
 
 .. math::
 
-   \mathbf{j} = \text{stt_dens_conv} \times \mathbf{j}_{\text{vec}}
+   \mathbf{j} = \text{stt\_dens\_conv} \times \mathbf{j}_{\text{vec}}
 
 A note is printed at startup indicating that legacy input has been used and
 showing the resulting current density in physical units.

content/stimuli/index.rst

@@ -8,6 +8,7 @@ Apply external driving and thermal control modules.
    :hidden:
 
    fields
+   microwave_fields
    currents
    temperature-3tm
    temperature-gradients