diff --git a/docs/src/index.md b/docs/src/index.md
index 7e80a34..8c070df 100644
--- a/docs/src/index.md
+++ b/docs/src/index.md
@@ -1,6 +1,4 @@
-
-
-
+![Logo](https://github.com/WMD-group/CarrierCapture.jl/blob/master/schematics/Logo.png?raw=true)
A set of codes to compute carrier capture and recombination rates in semiconducting compounds.
This topic has a rich history starting from the work by [Huang and Rhys](http://rspa.royalsocietypublishing.org/content/204/1078/406.short).
@@ -58,7 +56,7 @@ In addition, the alignment of energy surfaces for defects in different charge st
The following examples are provided to illustrate some of the applications of these codes. The input data has been generated from density functional theory (DFT) using [VASP](https://www.vasp.at), but the framework can easily be adapted to accept output from other electronic structure calculators.
-* [SnZn in Cu2ZnSnS4](https://github.com/WMD-group/CarrierCapture.jl/blob/master/example/notebook/Harmonic%20(Sn_Zn).ipynb): Harmonic approximation
+* [Sn-on-Zn in Cu2ZnSnS4](https://github.com/WMD-group/CarrierCapture.jl/blob/master/example/notebook/Harmonic%20(Sn_Zn).ipynb): Harmonic approximation
* [DX-center in GaAs](https://github.com/WMD-group/CarrierCapture.jl/blob/master/example/notebook/Anharmonic%20(DX%20center).ipynb): Anharmonic fitting
@@ -72,9 +70,9 @@ The capture of electrons or holes by point defects in a crystalline materials re
The capture coefficient between an initial and final state for this computational set up is given by (eq. 22 in [Alkauskas and coworkers](https://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.075202)):
-
-
-
+```math
+C_p = V \frac{2\pi}{\hbar} g W_{if}^2 \sum_m w_m \sum_n |\langle \xi_{im}| Q - Q_0 | \xi_{fn}\rangle|^2 \delta (\Delta E + m\hbar\Omega_i -n\hbar\Omega_f )
+```
Here, *V* is the volume of the supercell, *Wif* is the electron-phonon overlap and *ξim* and *ξfn* describe the wavefunctions of the *mth* and *nth* phonons in the initial *i* and final *f* states. The final delta-function term serves to conserve energy and in practice is replaced by a smearing Gaussian of finite width *σ*.
@@ -114,7 +112,7 @@ Here, *V* is the volume of the supercell, *Wif* is the electron-phono
#### Applications of CarrierCapture
-* [Wang et al, Upper efficiency limit of Sb2Se3 solar cells (2024)](https://doi.org/10.1016/j.joule.2024.05.004)
+* [Wang et al, Upper efficiency limit of Sb2Se3 solar cells (2024)](https://doi.org/10.1016/j.joule.2024.05.004)
* [Kavanagh et al, Impact of metastable defect structures on carrier recombination in solar cells (2022)](https://pubs.rsc.org/en/content/articlelanding/2022/fd/d2fd00043a)
@@ -130,6 +128,6 @@ Here, *V* is the volume of the supercell, *Wif* is the electron-phono
* [Kim et al, Anharmonic lattice relaxation during non-radiative carrier capture (2019)](https://journals.aps.org/prb/abstract/10.1103/PhysRevB.100.041202)
-* [Kim et al, Lone-pair effect on carrier capture in Cu2ZnSnS4 solar cells (2019)](https://pubs.rsc.org/en/content/articlehtml/2019/ta/c8ta10130b)
+* [Kim et al, Lone-pair effect on carrier capture in Cu2ZnSnS4 solar cells (2019)](https://pubs.rsc.org/en/content/articlehtml/2019/ta/c8ta10130b)
* [Kim et al, Identification of killer defects in kesterite thin-film solar cells (2018)](https://pubs.acs.org/doi/abs/10.1021/acsenergylett.7b01313)
diff --git a/docs/src/usage.md b/docs/src/usage.md
index 41223c6..1792abb 100644
--- a/docs/src/usage.md
+++ b/docs/src/usage.md
@@ -133,15 +133,14 @@ See [Example](https://github.com/WMD-group/CarrierCapture.jl/blob/master/example
1. Use `fit_pot!` to find a best fit to the [data of `Q` and `E`](#qe_data).
2. Use `solve_pot!` to solve 1D Shrödinger equation for the potential energy surface (PES).
-## 3. Computing capture rates
+## 3. Computing Capture Rates
See [Example](https://github.com/WMD-group/CarrierCapture.jl/blob/master/example/notebook/Anharmonic%20(DX%20center).ipynb).
1. Use `calc_overlap!` to calculate the overlap between phonon wave functions.
2. Use `calc_capt_coeff!` to calculate the capture coefficient as a function of temperature.
-
-# High-Throughput Usage
+# High-throughput Usage
High-throughput usage is possible by preparing files in a similar method to the examples, `useParamScan_Harmonic.jl` and `useParamScan_Anharmonic.jl`. It is recommended that a high-performance computer rather than a personal machine is used, depending on how many calculations are performed. The code can then be run remotely using `nohup julia useParamScan_Harmonic &`.
The steps are as follows,