diff --git a/2022_05_Trieste/Fri.AM.2.BoltzWann/.gitignore b/2022_05_Trieste/Fri.AM.2.BoltzWann/.gitignore
new file mode 100644
index 0000000..2247701
--- /dev/null
+++ b/2022_05_Trieste/Fri.AM.2.BoltzWann/.gitignore
@@ -0,0 +1,18 @@
+out/
+scf.out
+nscf.out
+Si.nnkp
+Si.wout
+pw2wan.out
+Si.amn
+Si.chk
+Si.eig
+Si.mmn
+Si.wpout
+Si_boltzdos.dat
+Si_elcond.dat
+Si_kappa.dat
+Si_seebeck.dat
+Si_sigmas.dat
+Si_tdf.dat
+Si_seebeck_xx_500K.dat
diff --git a/2022_05_Trieste/Fri.AM.2.BoltzWann/Si.nscf b/2022_05_Trieste/Fri.AM.2.BoltzWann/Si.nscf
new file mode 100644
index 0000000..f67d113
--- /dev/null
+++ b/2022_05_Trieste/Fri.AM.2.BoltzWann/Si.nscf
@@ -0,0 +1,93 @@
+Silicon
+ &control
+    calculation        =  'nscf'
+    prefix             =  'si'
+    pseudo_dir         =  '/media/ictpuser/AiiDA/codes/wannier90/pseudo/'
+    outdir             =  'out/'
+    iprint             =   2
+    verbosity          =  'high'
+/
+ &system
+    ibrav              =    2
+    celldm(1)          =   10.2
+    nat                =    2
+    ntyp               =    1
+    ecutwfc            =   25.0
+    nbnd               =   12
+/
+ &electrons
+    conv_thr           =   1.0d-12
+    diagonalization    =  'cg'
+    diago_full_acc     =  .true.
+/
+ATOMIC_SPECIES
+ Si 28 Si.pbe-n-van.UPF
+ATOMIC_POSITIONS {crystal}
+Si  -0.25    0.75   -0.25
+Si   0.00    0.00    0.00
+K_POINTS {crystal}
+64
+  0.00000000  0.00000000  0.00000000  1.562500e-02
+  0.00000000  0.00000000  0.25000000  1.562500e-02
+  0.00000000  0.00000000  0.50000000  1.562500e-02
+  0.00000000  0.00000000  0.75000000  1.562500e-02
+  0.00000000  0.25000000  0.00000000  1.562500e-02
+  0.00000000  0.25000000  0.25000000  1.562500e-02
+  0.00000000  0.25000000  0.50000000  1.562500e-02
+  0.00000000  0.25000000  0.75000000  1.562500e-02
+  0.00000000  0.50000000  0.00000000  1.562500e-02
+  0.00000000  0.50000000  0.25000000  1.562500e-02
+  0.00000000  0.50000000  0.50000000  1.562500e-02
+  0.00000000  0.50000000  0.75000000  1.562500e-02
+  0.00000000  0.75000000  0.00000000  1.562500e-02
+  0.00000000  0.75000000  0.25000000  1.562500e-02
+  0.00000000  0.75000000  0.50000000  1.562500e-02
+  0.00000000  0.75000000  0.75000000  1.562500e-02
+  0.25000000  0.00000000  0.00000000  1.562500e-02
+  0.25000000  0.00000000  0.25000000  1.562500e-02
+  0.25000000  0.00000000  0.50000000  1.562500e-02
+  0.25000000  0.00000000  0.75000000  1.562500e-02
+  0.25000000  0.25000000  0.00000000  1.562500e-02
+  0.25000000  0.25000000  0.25000000  1.562500e-02
+  0.25000000  0.25000000  0.50000000  1.562500e-02
+  0.25000000  0.25000000  0.75000000  1.562500e-02
+  0.25000000  0.50000000  0.00000000  1.562500e-02
+  0.25000000  0.50000000  0.25000000  1.562500e-02
+  0.25000000  0.50000000  0.50000000  1.562500e-02
+  0.25000000  0.50000000  0.75000000  1.562500e-02
+  0.25000000  0.75000000  0.00000000  1.562500e-02
+  0.25000000  0.75000000  0.25000000  1.562500e-02
+  0.25000000  0.75000000  0.50000000  1.562500e-02
+  0.25000000  0.75000000  0.75000000  1.562500e-02
+  0.50000000  0.00000000  0.00000000  1.562500e-02
+  0.50000000  0.00000000  0.25000000  1.562500e-02
+  0.50000000  0.00000000  0.50000000  1.562500e-02
+  0.50000000  0.00000000  0.75000000  1.562500e-02
+  0.50000000  0.25000000  0.00000000  1.562500e-02
+  0.50000000  0.25000000  0.25000000  1.562500e-02
+  0.50000000  0.25000000  0.50000000  1.562500e-02
+  0.50000000  0.25000000  0.75000000  1.562500e-02
+  0.50000000  0.50000000  0.00000000  1.562500e-02
+  0.50000000  0.50000000  0.25000000  1.562500e-02
+  0.50000000  0.50000000  0.50000000  1.562500e-02
+  0.50000000  0.50000000  0.75000000  1.562500e-02
+  0.50000000  0.75000000  0.00000000  1.562500e-02
+  0.50000000  0.75000000  0.25000000  1.562500e-02
+  0.50000000  0.75000000  0.50000000  1.562500e-02
+  0.50000000  0.75000000  0.75000000  1.562500e-02
+  0.75000000  0.00000000  0.00000000  1.562500e-02
+  0.75000000  0.00000000  0.25000000  1.562500e-02
+  0.75000000  0.00000000  0.50000000  1.562500e-02
+  0.75000000  0.00000000  0.75000000  1.562500e-02
+  0.75000000  0.25000000  0.00000000  1.562500e-02
+  0.75000000  0.25000000  0.25000000  1.562500e-02
+  0.75000000  0.25000000  0.50000000  1.562500e-02
+  0.75000000  0.25000000  0.75000000  1.562500e-02
+  0.75000000  0.50000000  0.00000000  1.562500e-02
+  0.75000000  0.50000000  0.25000000  1.562500e-02
+  0.75000000  0.50000000  0.50000000  1.562500e-02
+  0.75000000  0.50000000  0.75000000  1.562500e-02
+  0.75000000  0.75000000  0.00000000  1.562500e-02
+  0.75000000  0.75000000  0.25000000  1.562500e-02
+  0.75000000  0.75000000  0.50000000  1.562500e-02
+  0.75000000  0.75000000  0.75000000  1.562500e-02 
diff --git a/2022_05_Trieste/Fri.AM.2.BoltzWann/Si.pw2wan b/2022_05_Trieste/Fri.AM.2.BoltzWann/Si.pw2wan
new file mode 100644
index 0000000..1be8b0c
--- /dev/null
+++ b/2022_05_Trieste/Fri.AM.2.BoltzWann/Si.pw2wan
@@ -0,0 +1,9 @@
+&inputpp 
+   outdir = 'out/'
+   prefix = 'si'
+   seedname = 'Si'
+   spin_component = 'none'
+   write_mmn = .true.
+   write_amn = .true.
+   write_unk = .false.
+/
diff --git a/2022_05_Trieste/Fri.AM.2.BoltzWann/Si.scf b/2022_05_Trieste/Fri.AM.2.BoltzWann/Si.scf
new file mode 100644
index 0000000..0ceb161
--- /dev/null
+++ b/2022_05_Trieste/Fri.AM.2.BoltzWann/Si.scf
@@ -0,0 +1,28 @@
+Silicon
+ &control
+    calculation     =  'scf'
+    restart_mode    =  'from_scratch'
+    prefix          =  'si'
+    tprnfor         =  .true.
+    pseudo_dir      =  '/media/ictpuser/AiiDA/codes/wannier90/pseudo/'
+    outdir          =  'out/'
+    iprint          =   2
+/
+ &system
+    ibrav           =   2
+    celldm(1)       =  10.2
+    nat             =   2
+    ntyp            =   1
+    ecutwfc         =  25.0
+/
+ &electrons
+    conv_thr        =   1.0d-12
+    diagonalization =  'cg'
+/
+ATOMIC_SPECIES
+ Si  28  Si.pbe-n-van.UPF
+ATOMIC_POSITIONS {crystal}
+Si  -0.25   0.75   -0.25
+Si   0.00   0.00    0.00
+K_POINTS {automatic}
+10 10 10 0 0 0
diff --git a/2022_05_Trieste/Fri.AM.2.BoltzWann/Si.win b/2022_05_Trieste/Fri.AM.2.BoltzWann/Si.win
new file mode 100644
index 0000000..1a3a1a8
--- /dev/null
+++ b/2022_05_Trieste/Fri.AM.2.BoltzWann/Si.win
@@ -0,0 +1,125 @@
+!!! -- Begin of BoltzWann input -- !!!
+boltzwann                    = true
+boltz_calc_also_dos          = true
+boltz_dos_energy_step        = 0.01
+smr_type                     = gauss
+boltz_dos_adpt_smr           = false
+boltz_dos_smr_fixed_en_width = 0.03
+kmesh                        = 40
+boltz_mu_min                 = 5.
+boltz_mu_max                 = 8.
+boltz_mu_step                = 0.01
+boltz_temp_min               = 300.
+boltz_temp_max               = 300.
+boltz_temp_step              = 50
+boltz_relax_time             = 10.
+!! Next variable is commented because 2 is its default value
+!num_elec_per_state          = 2
+!!! --- End of BoltzWann input --- !!!
+
+#restart           = plot
+#bands_plot        = true
+#bands_plot_format = xmgr
+
+num_bands         = 12
+num_wann          = 8
+dis_win_max       = 17.d0
+dis_froz_max      = 6.4d0
+dis_num_iter      = 120
+dis_mix_ratio     = 1.d0
+
+num_iter          = 500
+num_print_cycles  = 50
+
+begin unit_cell_cart
+bohr
+-5.1000 0.0000 5.1000
+ 0.0000 5.1000 5.1000
+-5.1000 5.1000 0.0000
+end unit_cell_cart
+
+begin atoms_frac
+Si   0.00   0.00   0.00
+Si   -0.25  0.75  -0.25
+End atoms_frac
+
+begin projections
+Si : sp3
+end projections
+
+begin kpoint_path
+L 0.50000  0.50000 0.5000 G 0.00000  0.00000 0.0000
+G 0.00000  0.00000 0.0000 X 0.50000  0.00000 0.5000
+X 0.50000 -0.50000 0.0000 K 0.37500 -0.37500 0.0000
+K 0.37500 -0.37500 0.0000 G 0.00000  0.00000 0.0000
+end kpoint_path
+
+
+mp_grid      = 4 4 4
+
+begin kpoints
+  0.00000000  0.00000000  0.00000000
+  0.00000000  0.00000000  0.25000000
+  0.00000000  0.00000000  0.50000000
+  0.00000000  0.00000000  0.75000000
+  0.00000000  0.25000000  0.00000000
+  0.00000000  0.25000000  0.25000000
+  0.00000000  0.25000000  0.50000000
+  0.00000000  0.25000000  0.75000000
+  0.00000000  0.50000000  0.00000000
+  0.00000000  0.50000000  0.25000000
+  0.00000000  0.50000000  0.50000000
+  0.00000000  0.50000000  0.75000000
+  0.00000000  0.75000000  0.00000000
+  0.00000000  0.75000000  0.25000000
+  0.00000000  0.75000000  0.50000000
+  0.00000000  0.75000000  0.75000000
+  0.25000000  0.00000000  0.00000000
+  0.25000000  0.00000000  0.25000000
+  0.25000000  0.00000000  0.50000000
+  0.25000000  0.00000000  0.75000000
+  0.25000000  0.25000000  0.00000000
+  0.25000000  0.25000000  0.25000000
+  0.25000000  0.25000000  0.50000000
+  0.25000000  0.25000000  0.75000000
+  0.25000000  0.50000000  0.00000000
+  0.25000000  0.50000000  0.25000000
+  0.25000000  0.50000000  0.50000000
+  0.25000000  0.50000000  0.75000000
+  0.25000000  0.75000000  0.00000000
+  0.25000000  0.75000000  0.25000000
+  0.25000000  0.75000000  0.50000000
+  0.25000000  0.75000000  0.75000000
+  0.50000000  0.00000000  0.00000000
+  0.50000000  0.00000000  0.25000000
+  0.50000000  0.00000000  0.50000000
+  0.50000000  0.00000000  0.75000000
+  0.50000000  0.25000000  0.00000000
+  0.50000000  0.25000000  0.25000000
+  0.50000000  0.25000000  0.50000000
+  0.50000000  0.25000000  0.75000000
+  0.50000000  0.50000000  0.00000000
+  0.50000000  0.50000000  0.25000000
+  0.50000000  0.50000000  0.50000000
+  0.50000000  0.50000000  0.75000000
+  0.50000000  0.75000000  0.00000000
+  0.50000000  0.75000000  0.25000000
+  0.50000000  0.75000000  0.50000000
+  0.50000000  0.75000000  0.75000000
+  0.75000000  0.00000000  0.00000000
+  0.75000000  0.00000000  0.25000000
+  0.75000000  0.00000000  0.50000000
+  0.75000000  0.00000000  0.75000000
+  0.75000000  0.25000000  0.00000000
+  0.75000000  0.25000000  0.25000000
+  0.75000000  0.25000000  0.50000000
+  0.75000000  0.25000000  0.75000000
+  0.75000000  0.50000000  0.00000000
+  0.75000000  0.50000000  0.25000000
+  0.75000000  0.50000000  0.50000000
+  0.75000000  0.50000000  0.75000000
+  0.75000000  0.75000000  0.00000000
+  0.75000000  0.75000000  0.25000000
+  0.75000000  0.75000000  0.50000000
+  0.75000000  0.75000000  0.75000000
+end kpoints
diff --git a/2022_05_Trieste/Fri.AM.2.BoltzWann/latex/.gitignore b/2022_05_Trieste/Fri.AM.2.BoltzWann/latex/.gitignore
new file mode 100644
index 0000000..d790b0e
--- /dev/null
+++ b/2022_05_Trieste/Fri.AM.2.BoltzWann/latex/.gitignore
@@ -0,0 +1,9 @@
+.vscode
+main.aux
+main.bcf
+main.log
+main.out
+main.pdf
+main.run.xml
+main.blg
+main.bbl
diff --git a/2022_05_Trieste/Fri.AM.2.BoltzWann/latex/fig/dos.pdf b/2022_05_Trieste/Fri.AM.2.BoltzWann/latex/fig/dos.pdf
new file mode 100644
index 0000000..00e1d1b
Binary files /dev/null and b/2022_05_Trieste/Fri.AM.2.BoltzWann/latex/fig/dos.pdf differ
diff --git a/2022_05_Trieste/Fri.AM.2.BoltzWann/latex/fig/seebeck.pdf b/2022_05_Trieste/Fri.AM.2.BoltzWann/latex/fig/seebeck.pdf
new file mode 100644
index 0000000..1a5438f
Binary files /dev/null and b/2022_05_Trieste/Fri.AM.2.BoltzWann/latex/fig/seebeck.pdf differ
diff --git a/2022_05_Trieste/Fri.AM.2.BoltzWann/latex/main.bib b/2022_05_Trieste/Fri.AM.2.BoltzWann/latex/main.bib
new file mode 100644
index 0000000..211d0b1
--- /dev/null
+++ b/2022_05_Trieste/Fri.AM.2.BoltzWann/latex/main.bib
@@ -0,0 +1,32 @@
+@article{Pizzi2014,
+ author = {Pizzi, Giovanni and Volja, Dmitri and Kozinsky, Boris and Fornari, Marco and Marzari, Nicola},
+ date = {2014-01},
+ doi = {10.1016/j.cpc.2013.09.015},
+ issn = {0010-4655},
+ journaltitle = {Comput. Phys. Commun.},
+ keywords = {Maximally-localized Wannier functions, Wannier90, Band interpolation, Band velocities, Thermoelectric properties},
+ number = {1},
+ pages = {422--429},
+ shorttitle = {{BoltzWann}},
+ title = {{BoltzWann}: {A} code for the evaluation of thermoelectric and electronic transport properties with a maximally-localized {Wannier} functions basis},
+ url = {http://www.sciencedirect.com/science/article/pii/S0010465513003160},
+ urldate = {2021-02-03},
+ volume = {185}
+}
+
+@article{Pizzi2014a,
+ author = {Pizzi, Giovanni and Volja, Dmitri and Kozinsky, Boris and Fornari, Marco and Marzari, Nicola},
+ date = {2014-08},
+ doi = {10.1016/j.cpc.2014.05.004},
+ issn = {0010-4655},
+ journaltitle = {Comput. Phys. Commun.},
+ keywords = {Maximally-localized Wannier functions, Wannier90, Band interpolation, Band velocities, Thermoelectric properties},
+ number = {8},
+ pages = {2311--2312},
+ shorttitle = {An updated version of {BoltzWann}},
+ title = {An updated version of {BoltzWann}: {A} code for the evaluation of thermoelectric and electronic transport properties with a maximally-localized {Wannier} functions basis},
+ url = {http://www.sciencedirect.com/science/article/pii/S0010465514001581},
+ urldate = {2021-02-03},
+ volume = {185}
+}
+
diff --git a/2022_05_Trieste/Fri.AM.2.BoltzWann/latex/main.tex b/2022_05_Trieste/Fri.AM.2.BoltzWann/latex/main.tex
new file mode 100644
index 0000000..6e76ec7
--- /dev/null
+++ b/2022_05_Trieste/Fri.AM.2.BoltzWann/latex/main.tex
@@ -0,0 +1,211 @@
+\documentclass[11pt,a4paper]{article}
+
+\usepackage[a4paper,margin=1in,footskip=0.25in]{geometry}
+\usepackage{amsmath}
+\usepackage{amssymb}
+\usepackage{graphicx}
+\usepackage{dcolumn}
+\usepackage{bm}
+\usepackage{cprotect}
+\usepackage{spverbatim}
+
+\usepackage{siunitx}
+
+\usepackage[caption=false]{subfig}
+\usepackage{printlen}
+\usepackage{xspace}
+
+\usepackage{fancyhdr}
+\pagestyle{fancy}
+\fancyhf{}
+\rhead{Wannier 2022 Summer School}
+\lhead{Giovanni Pizzi, Junfeng Qiao}
+\cfoot{\thepage}
+
+\usepackage{tabularx}
+\usepackage{dcolumn}
+\usepackage{booktabs}
+\usepackage[inline]{enumitem}
+
+\usepackage[cache=false]{minted}%
+
+\usepackage{hyperref}
+\usepackage[capitalize]{cleveref}
+
+\usepackage[backend=biber,style=phys]{biblatex}
+\addbibresource{main.bib}
+
+\begin{document}
+
+\definecolor{LightGray}{gray}{0.9}
+\setminted{
+  bgcolor=LightGray, }
+
+\title{Hands-on:\\
+  \textbf{Thermoelectric and electronic transport properties with Wannier90+BoltzWann}}
+
+\author{Giovanni Pizzi}
+\author{Junfeng Qiao}
+
+\date{\today}
+\maketitle
+
+\newcommand{\wan}{\texttt{Wannier90}\xspace}
+\newcommand{\boltzwan}{\texttt{BoltzWann}\xspace}
+\newcommand{\pwx}{\texttt{pw.x}\xspace}
+\newcommand{\ptowx}{\textnormal{\texttt{pw2wannier90.x}}\xspace}
+\newcommand{\wanx}{\textnormal{\texttt{wannier90.x}}\xspace}
+\newcommand{\postwanx}{\textnormal{\texttt{postw90.x}}\xspace}
+
+\section{Outline}
+
+\begin{itemize}
+  \item Obtain MLWFs for the valence and low-lying conduction states of silicon.
+  \item Calculate the electrical conductivity, the Seebeck coefficient and the thermal
+        conductivity in the constant relaxation time approximation using the \boltzwan
+        module\cite{Pizzi2014,Pizzi2014a}.
+\end{itemize}
+
+\section{Input files \& executables}
+\begin{itemize}
+  \item{Directory: \texttt{wannier-tutorials/2022\_05\_Trieste/Fri.AM.2.BoltzWann/}}
+  \item{Input Files}
+  \begin{itemize}
+    \item \texttt{Si.scf}: The \pwx input file for ground state
+          calculation
+    \item \texttt{Si.nscf}: The \pwx input file to obtain Bloch
+          states on a uniform grid
+    \item \texttt{Si.pw2wan}: Input file for \ptowx
+    \item \texttt{Si.win}: The \wanx and \postwanx input file
+  \end{itemize}
+  \item Executables:
+        \begin{itemize}
+          \item \pwx, \ptowx, \wanx, and \postwanx
+          \item Available in \texttt{/media/ictpuser/AiiDA/bin/}
+        \end{itemize}
+\end{itemize}
+
+\section{Steps}
+We will first run the standard Wannierization of silicon, then run the
+\postwanx with \boltzwan related parameters added to the input file.
+\begin{enumerate}
+  \item Run \pwx to obtain the ground state of silicon
+        \begin{minted}{bash}
+pw.x < Si.scf > scf.out
+\end{minted}
+
+  \item Run \pwx to obtain the Bloch states on a uniform k-point grid.
+        \begin{minted}{bash}
+pw.x < Si.nscf > nscf.out
+  \end{minted}
+
+  \item Run \wanx to generate a list of the required overlaps (written into the
+        \texttt{Si.nnkp} file).
+        \begin{minted}{bash}
+wannier90.x -pp Si
+        \end{minted}
+
+  \item Run \ptowx to compute the overlap between Bloch states and the projections for
+        the starting guess (written in the \texttt{Si.mmn} and \texttt{Si.amn} files).
+        \begin{minted}{bash}
+pw2wannier90.x < Si.pw2wan > pw2wan.out
+        \end{minted}
+
+  \item Run \wanx to compute the MLWFs.
+        \begin{minted}{bash}
+wannier90.x Si
+\end{minted}
+
+        Inspect the output file \texttt{Si.wout} and check if the convergence was
+        reached both in the disentanglement and in the Wannierization steps. You may
+        also want to plot the Wannier functions and the interpolated band structure.
+
+  \item Run \postwanx to calculate the transport coefficients.
+        \begin{minted}{bash}
+# serial execution
+postw90.x Si
+# or parallel execution with, e.g. 4 MPI processes
+mpirun -np 4 postw90.x Si
+\end{minted}
+\end{enumerate}
+
+\section{Analysis}
+\begin{itemize}
+\item Inspect the output file \texttt{Si.wpout}. It summarizes the main details of
+the calculation (more details can be obtained by setting a larger value of the
+\texttt{iprint} flag). Check if no warnings are issued. Note that if no special
+flags are passed to \boltzwan, it assumes that the ab-initio calculation did
+not include magnetization effects, and thus it sets to 2 the number of
+electrons per state.
+
+\item Note also that the value of the relaxation time $\tau$ = \SI{10}{fs} in the
+example is set only as a representative value; note also that only the
+electrical and thermal conductivity depend on $\tau$, while the Seebeck
+coefficient is independent of $\tau$.
+
+\item Using your favorite plotting program, plot the \texttt{Si\_boltzdos.dat} file
+to inspect the DOS, e.g. with \texttt{gnuplot}, see \cref{fig:dos}.
+\begin{minted}{gnuplot}
+set xlabel 'E (eV)'
+set ylabel 'DOS (ang^{-3})'
+plot 'Si_boltzdos.dat' w l
+\end{minted}
+\begin{figure}[htb]
+  \centering
+  \includegraphics[width=.7\textwidth]{fig/dos.pdf}
+  \caption{DOS of silicon using \boltzwan module.}
+  \label{fig:dos}
+\end{figure}
+
+\item Using your favorite plotting program, plot columns 1 and 3 of the
+\texttt{Si\_seebeck.dat} file to inspect the $S_{xx}$ component of the Seebeck
+coefficient as a function of the chemical potential $\mu$, at $T$ =
+\SI{300}{K}. For example, with \texttt{gnuplot}, see \cref{fig:seebeck}.
+\begin{minted}{gnuplot}
+set xlabel 'E (eV)'
+set ylabel 'DOS (S_{xx} (V/K))'
+plot 'Si_seebeck.dat' u 1:3 w l
+\end{minted}
+\begin{figure}[htb]
+  \centering
+  \includegraphics[width=.7\textwidth]{fig/seebeck.pdf}
+  \caption{$S_{xx}$ of silicon using \boltzwan module.}
+  \label{fig:seebeck}
+\end{figure}
+\end{itemize}
+
+\subsection{Further ideas}
+
+\begin{itemize}
+  \item Change the interpolation to a $60\times 60\times 60$ mesh and run again
+        \postwanx to check if the results for the transport properties are converged.
+
+  \item Change the \texttt{Si.win} input file so that it calculates the transport
+        coefficients for temperatures from \SIrange{300}{700}{K}, with steps of
+        \SI{200}{K}. Rerun \postwanx and verify that the increase in execution time is
+        neglibile (in fact, most of the time is spent to interpolate the band structure
+        on the $k$ mesh).
+
+        Plot the Seebeck coefficient for the three temperatures $T$ = \SI{300}{K}, $T$
+        = \SI{500}{K} and $T$ = \SI{700}{K}. To do this, you have to filter the
+        \texttt{Si\_seebeck.dat} to select only those lines where the second column is
+        equal to the required temperature. A possible script to select the $S_{xx}$
+        component of the Seebeck coefficient for $T$ = \SI{500}{K} using the
+        \texttt{awk/gawk} command line program is the following:
+        \begin{minted}{bash}
+awk '{if ($2 == 500) {print $1, $3;}}' < Si_seebeck.dat \
+    > Si_seebeck_xx_500K.dat
+\end{minted}
+        Then, you can plot columns 1 and 2 of the output file
+        \verb#Si_seebeck_xx_500K.dat#.
+  \item Try to calculate the Seebeck coefficient as a function of the temperature, for
+        a $n-$doped sample with, e.g., $n$ = \SI{1e18}{cm^{-3}}. Note that to this aim,
+        you need to calculate consistently the value $\mu(T)$ of the chemical potential
+        as a function of the temperature, so as to reproduce the given value of $n$.
+        Then, you have to write a small program/script to interpolate the output of
+        \boltzwan, that you should have run on a suitable grid of $(\mu,T)$ points.
+\end{itemize}
+
+\printbibliography
+
+\end{document}
diff --git a/2022_05_Trieste/Fri.AM.2.BoltzWann/latex/makefile b/2022_05_Trieste/Fri.AM.2.BoltzWann/latex/makefile
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+all: main.tex main.bib
+	lualatex -shell-escape main.tex
+	biber main
+	lualatex -shell-escape main.tex
+
+clean:
+	rm main.aux main.bcf main.log main.out main.pdf main.run.xml main.blg main.bbl
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