diff --git a/examples.ipynb b/examples.ipynb
index 6d16ae9beb806b0ac93463b91a5581fc91e94beb..5204573080aa52bd46cf3c80582c715b0217c9d5 100644
--- a/examples.ipynb
+++ b/examples.ipynb
@@ -69,7 +69,7 @@
        "$\\displaystyle \\text{Chern Character:} \\\\ \\begin{array}{l} \\mathrm{ch}_{0} = 3 \\\\ \\mathrm{ch}_{1} = 2 \\ell^{1} \\\\ \\mathrm{ch}_{2} = -2 \\ell^{2} \\end{array}$"
       ],
       "text/plain": [
-       "<pseudowalls.chern_character.Chern_Char object at 0x7f679c692150>"
+       "<pseudowalls.chern_character.Chern_Char object at 0x7f25db3a9990>"
       ]
      },
      "execution_count": 2,
@@ -100,7 +100,7 @@
        "$\\displaystyle \\text{Chern Character:} \\\\ \\begin{array}{l} \\mathrm{ch}_{0} = 29 \\\\ \\mathrm{ch}_{1} = 13 \\ell^{1} \\\\ \\mathrm{ch}_{2} = -\\frac{3}{2} \\ell^{2} \\end{array}$"
       ],
       "text/plain": [
-       "<pseudowalls.chern_character.Chern_Char object at 0x7f67924d6810>"
+       "<pseudowalls.chern_character.Chern_Char object at 0x7f25d1953e20>"
       ]
      },
      "execution_count": 3,
@@ -256,59 +256,59 @@
    ]
   },
   {
-   "cell_type": "code",
-   "execution_count": 8,
-   "id": "712b7324",
+   "cell_type": "markdown",
+   "id": "8de156d1",
    "metadata": {},
-   "outputs": [],
    "source": [
-    "from plots_and_expressions import \\\n",
-    "r_upper_bound_all_q, Delta, nu, n, R\n",
-    "# Delta: symbol for Δ(v)\n",
-    "# n: symbol for denominator for β_(v)\n",
-    "# R : symbol for chern_0(v)\n",
-    "# nu : ..."
+    "$\\renewcommand\\nu\\ell$\n",
+    "Redefine \\nu to $\\nu$ in latex\n",
+    "$\\let\\originalDelta\\Delta$\n",
+    "$\\renewcommand\\Delta{\\originalDelta(v)}$\n",
+    "Redefine \\Delta in latex to be $\\Delta$"
    ]
   },
   {
    "cell_type": "code",
-   "execution_count": 9,
-   "id": "5814dd1d",
-   "metadata": {
-    "scrolled": true
-   },
+   "execution_count": 8,
+   "id": "712b7324",
+   "metadata": {},
    "outputs": [
     {
      "data": {
       "text/html": [
-       "<html>\\(\\displaystyle \\frac{{\\left(R + \\frac{\\Delta n^{2}}{\\nu^{2}}\\right)}^{2} \\nu^{2}}{4 \\, \\Delta n^{2}}\\)</html>"
+       "<html>\\(\\displaystyle \\frac{1}{2} \\, R + \\frac{\\Delta n^{2}}{4 \\, \\nu^{2}} + \\frac{R^{2} \\nu^{2}}{4 \\, \\Delta n^{2}}\\)</html>"
       ],
       "text/latex": [
-       "$\\displaystyle \\frac{{\\left(R + \\frac{\\Delta n^{2}}{\\nu^{2}}\\right)}^{2} \\nu^{2}}{4 \\, \\Delta n^{2}}$"
+       "$\\displaystyle \\frac{1}{2} \\, R + \\frac{\\Delta n^{2}}{4 \\, \\nu^{2}} + \\frac{R^{2} \\nu^{2}}{4 \\, \\Delta n^{2}}$"
       ],
       "text/plain": [
-       "1/4*(R + Delta*n^2/nu^2)^2*nu^2/(Delta*n^2)"
+       "1/2*R + 1/4*Delta*n^2/nu^2 + 1/4*R^2*nu^2/(Delta*n^2)"
       ]
      },
-     "execution_count": 9,
+     "execution_count": 8,
      "metadata": {},
      "output_type": "execute_result"
     }
    ],
    "source": [
-    "r_upper_bound_all_q"
+    "from plots_and_expressions import main_theorem1, Delta, nu, R, n\n",
+    "# Delta: symbol for Δ(v)\n",
+    "# n: symbol for denominator for β_(v)\n",
+    "# R : symbol for chern_0(v)\n",
+    "# nu : ...\n",
+    "main_theorem1.corollary_r_bound"
    ]
   },
   {
    "cell_type": "code",
-   "execution_count": 10,
+   "execution_count": 9,
    "id": "43aa5f56",
    "metadata": {},
    "outputs": [],
    "source": [
     "def corrolary_bound(example):\n",
     "    return (\n",
-    "        r_upper_bound_all_q.expand()\n",
+    "        main_theorem1.corollary_r_bound\n",
     "        .subs(Delta==example.bgmlv)\n",
     "        .subs(nu==1)\n",
     "        .subs(R==example.chern.ch[0])\n",
@@ -322,7 +322,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 11,
+   "execution_count": 10,
    "id": "5baed51c",
    "metadata": {},
    "outputs": [
@@ -338,7 +338,7 @@
        "53838.5009765625"
       ]
      },
-     "execution_count": 11,
+     "execution_count": 10,
      "metadata": {},
      "output_type": "execute_result"
     }
@@ -349,7 +349,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 12,
+   "execution_count": 11,
    "id": "fcc15f60",
    "metadata": {},
    "outputs": [
@@ -365,7 +365,7 @@
        "37.515625"
       ]
      },
-     "execution_count": 12,
+     "execution_count": 11,
      "metadata": {},
      "output_type": "execute_result"
     }
@@ -384,7 +384,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 13,
+   "execution_count": 12,
    "id": "ef8f09ff",
    "metadata": {},
    "outputs": [],
@@ -436,7 +436,7 @@
   },
   {
    "cell_type": "code",
-   "execution_count": 14,
+   "execution_count": 13,
    "id": "9cd102ac",
    "metadata": {},
    "outputs": [
@@ -462,7 +462,7 @@
        "       [0, 0, 4, 3, 8, 25, 12, 15, 19, 6, 5, 4, 3]], dtype=object)"
       ]
      },
-     "execution_count": 14,
+     "execution_count": 13,
      "metadata": {},
      "output_type": "execute_result"
     }
@@ -474,7 +474,7 @@
  ],
  "metadata": {
   "kernelspec": {
-   "display_name": "SageMath 9.8",
+   "display_name": "SageMath 9.7",
    "language": "sage",
    "name": "sagemath"
   },
@@ -488,7 +488,7 @@
    "name": "python",
    "nbconvert_exporter": "python",
    "pygments_lexer": "ipython3",
-   "version": "3.11.3"
+   "version": "3.10.8"
   }
  },
  "nbformat": 4,