diff --git a/notebooks/RuClExample.ipynb b/notebooks/RuClExample.ipynb
index 505b28b..b1de29e 100644
--- a/notebooks/RuClExample.ipynb
+++ b/notebooks/RuClExample.ipynb
@@ -18,7 +18,7 @@
     "\\end{split}\n",
     "\\end{equation}\n",
     "\n",
-    "The terms $S^{x}_{i}$, $S^{y}_{i}$, and $S^{z}_{i}$ represent the Pauli operators acting on site $i$.  The terms $K_{x}$, $K_{y}$, and $K_{z}$ represent the strength of the Kitaev interaction between two sites in a given direction.  The bold terms $\\bf{S_i}$ $ = [S^x_i, S^y_i, S^z_i]$ are useful for defining the Heisenberg interaction terms with strength $J$.  The terms $\\Gamma$ represent the strength of off-diagonal symmetric exchange interactions between nearest neighboring sites, and the terms $\\Gamma'$ represent the effect of trigonal distortion.  Lastly, the term $A$ represents the effect of single-ion anisotropy.  \n",
+    "The terms $S^{x}_{i}$, $S^{y}_{i}$, and $S^{z}_{i}$ represent the Pauli operators acting on site $i$.  The terms $K_{x}$, $K_{y}$, and $K_{z}$ represent the strength of the Kitaev interaction between two sites in a given direction.  The bold terms ${\\bf{S_i}} = [S^x_i, S^y_i, S^z_i]$ are useful for defining the Heisenberg interaction terms with strength $J$.  The terms $\\Gamma$ represent the strength of off-diagonal symmetric exchange interactions between nearest neighboring sites, and the terms $\\Gamma'$ represent the effect of trigonal distortion.  Lastly, the term $A$ represents the effect of single-ion anisotropy.  \n",
     "\n",
     "The connectivity of the Hamiltonian is defined directionally, as shown in Figure 1 (obtained from [[1]](https://doi.org/10.1038/s41535-019-0203-y)).  As a result of the experiment being performed on the material, we need to include a time-varying Hamiltonian component, corresponding to the time-varying Zeeman terms operating on the material. This Hamiltonian is\n",
     "\\begin{equation}\n",
@@ -30,7 +30,7 @@
     "  H(t) = H_{material} + H_{field}(t)\n",
     "\\end{equation}\n",
     "\n",
-    "<img src=\"EmbeddedFigures/RuclLattice.jpg\" alt=\"RuCl Lattice\" width=\"400\"/>\n",
+    "![RuCl_Latticve](EmbeddedFigures/RuClLattice.jpg)\n",
     "\n",
     "##### Figure 1"
    ]
@@ -910,7 +910,7 @@
     "\n",
     "Once all of this has been done, the state has been prepared and the dynamics may be executed.\n",
     "\n",
-    "<img src=\"EmbeddedFigures/RuCl3_spinstructure.jpeg\" alt=\"RuCl_Spin_Structure\" width=\"800\"/>\n",
+    "![RuCl_Spin_Structure](EmbeddedFigures/RuCl3_spinstructure.jpeg)\n",
     "\n",
     "##### Figure 3"
    ]
@@ -1381,7 +1381,7 @@
    "name": "python",
    "nbconvert_exporter": "python",
    "pygments_lexer": "ipython3",
-   "version": "3.11.5"
+   "version": "3.9.13"
   }
  },
  "nbformat": 4,