Modify eqs to render in ssh_model.ipynb

docs/source/tutorials/ssh_model.ipynb

@@ -16,18 +16,21 @@
    "source": [
     "Using a Microwave channel, the interaction Hamiltonian is given by\n",
     "\n",
-    "```{math}\n",
+    "$$\n",
     "H = \\sum_{i=1}^N \\sum_{j<i} C_{ij} (\\sigma_i^+ \\sigma_j^- + \\sigma_i^- \\sigma_j^+)\n",
-    "```\n",
+    "$$\n",
     "where \n",
-    "{math}`C_{ij} = \\frac{C_3(1-3\\cos^2\\theta_{ij})}{R_{ij}^3}`.\n",
-    "Here {math}`R_{ij}` is the distance between qubits {math}`i` and {math}`j`, {math}`R_{ij}=|\\textbf{x}_i-\\textbf{x}_j|`, and {math}`\\theta_{ij}` is the angle between {math}`\\textbf{x}_i-\\textbf{x}_j` and the magnetic field.\n",
+    "$$\n",
+    "C_{ij} = \\frac{C_3(1-3\\cos^2\\theta_{ij})}{R_{ij}^3}\n",
+    "$$\n",
+    "\n",
+    "Here $R_{ij}$ is the distance between qubits $i$ and $j$, $R_{ij}=|\\textbf{x}_i-\\textbf{x}_j|$, and $\\theta_{ij}$ is the angle between $\\textbf{x}_i-\\textbf{x}_j$ and the magnetic field.\n",
     "See the [Pulser docs](https://pulser.readthedocs.io/en/stable/tutorials/xy_spin_chain.html) for more information.\n",
     "\n",
     "By appropriate choice of the qubit geometry we can approximate the [SSH model](https://en.wikipedia.org/wiki/Su%E2%80%93Schrieffer%E2%80%93Heeger_model) for hard bosons.\n",
     "For example, when \n",
     "$$ \\theta_{ij} = \\cos^{-1}\\sqrt{1/3}$$\n",
-    "there will be no interaction between qubits {math}`i` and {math}`j`. We use this to model the SSH model below.\n"
+    "there will be no interaction between qubits $i$ and $j$. We use this to model the SSH model below.\n"
    ]
   },
   {
@@ -193,7 +196,7 @@
  ],
  "metadata": {
   "kernelspec": {
-   "display_name": "qse",
+   "display_name": "env_qse",
    "language": "python",
    "name": "python3"
   },
@@ -207,7 +210,7 @@
    "name": "python",
    "nbconvert_exporter": "python",
    "pygments_lexer": "ipython3",
-   "version": "3.11.11"
+   "version": "3.12.11"
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  "nbformat": 4,