fixed some typos

Author: f-wilsch

assets/css/style.scss

@@ -3,6 +3,11 @@
 
 @import "jekyll-theme-minimalist";
 
+.table-wrapper {
+  overflow-x: auto;
+  width: 100%;
+}
+
 .img-circle {
     -webkit-border-radius: 8px;
     -moz-border-radius: 8px;

index.md

@@ -4,10 +4,12 @@ katex: true
 ---
 # HighPT
 
-`HighPT` (pronounced /haɪpt/) is a `Mathematica` package for the analysis of high-energy semileptonic transitions at hadron colliders. It allows to compute high-$p_T$ tail observables for semileptonic processes, i.e. Drell-Yan cross sections, for dilepton and monolepton final states at the LHC. 
+`HighPT` (pronounced *"hyped"*) is a `Mathematica` package for the analysis of high-energy semileptonic transitions at hadron colliders. It allows to compute high-$p_T$ tail observables for semileptonic processes, i.e. Drell-Yan cross sections, for dilepton and monolepton final states at the LHC. 
 
 The `HighPT` code is publicly available in the GitHub repository: [https://github.com/HighPT/HighPT](https://github.com/HighPT/HighPT)
 
+---
+
 ## Models
 
 `HighPT` can calculate the high-$p_T$ observables either within the Standard Model Effective Field Theory (SMEFT) or in explicit New Physics (NP) models, which allows for an assesment of a wide range of NP scenarios.

mediators.md

@@ -9,6 +9,8 @@ The currently implemented mediators comprise all leptoquarks. The available medi
 
 ### The currently available mediators and their masses:
 
+<div class="table-wrapper" markdown="block">
+
 | Mediator | `HighPT` label | Quantum numbers | 1&nbsp;TeV | 2&nbsp;TeV | 3&nbsp;TeV | 4&nbsp;TeV | 5&nbsp;TeV |
 | -------- | -------------- | --------------- | ----- | ----- | ----- | ----- | ----- |
 | $S_1$ | `"S1"` | $(\boldsymbol{\bar{3}},\boldsymbol{1},1/3)$ | ✓ | ✓ | ✓ | soon | soon |
@@ -20,4 +22,6 @@ The currently implemented mediators comprise all leptoquarks. The available medi
 | $V_2$ | `"V2"` | $(\boldsymbol{\bar{3}},\boldsymbol{2},5/6)$ | ✓ | ✓ | ✓ | soon | soon |
 | $\tilde{V}_2$ | `"V2t"` | $(\boldsymbol{\bar{3}},\boldsymbol{2},-1/6)$ | ✓ | ✓ | ✓ | soon | soon |
 | $S_3$ | `"S3"` | $(\boldsymbol{\bar{3}},\boldsymbol{3},1/3)$ | ✓ | ✓ | ✓ | soon | soon |
-| $U_3$ | `"U3"` | $(\boldsymbol{3},\boldsymbol{3},2/3)$ | ✓ | ✓ | ✓ | soon | soon |
+| $U_3$ | `"U3"` | $(\boldsymbol{3},\boldsymbol{3},2/3)$ | ✓ | ✓ | ✓ | soon | soon |
+
+</div>