{
 "cells": [
  {
   "cell_type": "markdown",
   "id": "283fddbe",
   "metadata": {},
   "source": [
    "# IBM Optimizations using Cirq"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "b7609ea0",
   "metadata": {},
   "source": [
    "[![Open in Colab](https://colab.research.google.com/assets/colab-badge.svg)](https://colab.research.google.com/github/Infleqtion/client-superstaq/blob/main/docs/source/optimizations/ibm/ibmq_compile_css.ipynb) [![Launch Binder](https://mybinder.org/badge_logo.svg)](https://mybinder.org/v2/gh/Infleqtion/client-superstaq/HEAD?labpath=docs/source/optimizations/ibm/ibmq_compile_css.ipynb)"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "55320d7b",
   "metadata": {},
   "source": [
    "Below is a brief tutorial on Superstaq optimizations for IBM Quantum superconducting qubit devices. For more information on IBM Quantum, visit their website [here](https://www.ibm.com/quantum)."
   ]
  },
  {
   "cell_type": "markdown",
   "id": "cc148463",
   "metadata": {},
   "source": [
    "## Imports and API Token\n",
    "\n",
    "This example tutorial notebook uses `cirq-superstaq`, our Superstaq client for Cirq; you can try it out by running `pip install cirq-superstaq[examples]`:"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 1,
   "id": "032904b0",
   "metadata": {},
   "outputs": [],
   "source": [
    "try:\n",
    "    import cirq\n",
    "    import cirq_superstaq as css\n",
    "    import qiskit\n",
    "except ImportError:\n",
    "    print(\"Installing cirq-superstaq[examples]...\")\n",
    "    %pip install --quiet 'cirq-superstaq[examples]'\n",
    "    print(\"Installed cirq-superstaq[examples].\")\n",
    "    print(\"You may need to restart the kernel to import newly installed packages.\")\n",
    "    import cirq\n",
    "    import cirq_superstaq as css\n",
    "    import qiskit\n",
    "\n",
    "import numpy as np"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "ea70f3e9",
   "metadata": {},
   "source": [
    "To interface Superstaq via Cirq, we must first instantiate a service with `cirq_superstaq.Service()`. We then supply a Superstaq API token by either providing the API token as an argument to `cirq_superstaq.Service()` or by setting it as an environment variable (see more details [here](https://superstaq.readthedocs.io/en/latest/get_started/basics/basics_css.html#Set-up-access-to-Superstaq%E2%80%99s-API))"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 2,
   "id": "972b9908",
   "metadata": {},
   "outputs": [],
   "source": [
    "# Provide your Superstaq API key using the \"api_key\" argument\n",
    "service = css.Service()"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "80e1d5e7",
   "metadata": {},
   "source": [
    "## Single Circuit Compilation\n",
    "\n",
    "Let us start by creating an example Cirq circuit that we will then compile and optimize for the 127-qubit IBM Quantum `brisbane` processor."
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 3,
   "id": "06be41c6",
   "metadata": {},
   "outputs": [
    {
     "data": {
      "text/html": [
       "<pre style=\"overflow: auto; white-space: pre;\">0: ───@────────────────@───│───M───\n",
       "      │                │   │   │\n",
       "1: ───X───Rz(0.413π)───X───│───M───</pre>"
      ],
      "text/plain": [
       "0: ───@────────────────@───│───M───\n",
       "      │                │   │   │\n",
       "1: ───X───Rz(0.413π)───X───│───M───"
      ]
     },
     "execution_count": 3,
     "metadata": {},
     "output_type": "execute_result"
    }
   ],
   "source": [
    "# Create a two-qubit cirq circuit\n",
    "qubits = cirq.LineQubit.range(2)\n",
    "theta = np.random.uniform(0, 4 * np.pi)\n",
    "circuit = cirq.Circuit(\n",
    "    cirq.CNOT(qubits[0], qubits[1]),\n",
    "    cirq.Rz(rads=theta)(qubits[1]),\n",
    "    cirq.CNOT(qubits[0], qubits[1]),\n",
    "    css.barrier(*qubits),\n",
    "    cirq.measure(qubits[0], qubits[1]),\n",
    ")\n",
    "\n",
    "# Visualize circuit\n",
    "circuit"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "e204bac3",
   "metadata": {},
   "source": [
    "We will now compile the above circuit to IBM's `brisbane` processor and visualize the differences by drawing the compiled circuit. "
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 4,
   "id": "e921bf6e",
   "metadata": {},
   "outputs": [
    {
     "data": {
      "text/html": [
       "<pre style=\"overflow: auto; white-space: pre;\">4: ───Rz(0.5π)───X───────────────AceCR+-(Z side)───Rz(0.5π)────X───────AceCR+-(Z side)───────│───M(&#x27;q(0),q(1)&#x27;)───\n",
       "                                 │                                     │                     │   │\n",
       "5: ───Rz(π)──────X^0.5───Rz(π)───AceCR+-(X side)───Rz(1.59π)───X^0.5───AceCR+-(X side)───X───│───M────────────────</pre>"
      ],
      "text/plain": [
       "4: ───Rz(0.5π)───X───────────────AceCR+-(Z side)───Rz(0.5π)────X───────AceCR+-(Z side)───────│───M('q(0),q(1)')───\n",
       "                                 │                                     │                     │   │\n",
       "5: ───Rz(π)──────X^0.5───Rz(π)───AceCR+-(X side)───Rz(1.59π)───X^0.5───AceCR+-(X side)───X───│───M────────────────"
      ]
     },
     "execution_count": 4,
     "metadata": {},
     "output_type": "execute_result"
    }
   ],
   "source": [
    "# Compile with qscout compile\n",
    "compiler_output = service.ibmq_compile(circuit, target=\"ibmq_brisbane_qpu\")\n",
    "\n",
    "# Call circuit from the compiler output to get the corresponding output circuit\n",
    "output_circuit = compiler_output.circuit\n",
    "\n",
    "# Visualize the compiled circuit\n",
    "output_circuit"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "57bf81d5",
   "metadata": {},
   "source": [
    "The resulting output is now a circuit compiled to `brisbane`'s native operations. With Superstaq compilation, you can also observe the gates and gate times for the compiled circuit using Qiskit’s timeline drawer (see [Qiskit Timeline Visualizations Documentation](https://docs.quantum.ibm.com/api/qiskit/qiskit.visualization.timeline_drawer)) by running the following:"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 5,
   "id": "bd85d98b",
   "metadata": {},
   "outputs": [
    {
     "data": {
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      "text/plain": [
       "<Figure size 3000x300 with 1 Axes>"
      ]
     },
     "execution_count": 5,
     "metadata": {},
     "output_type": "execute_result"
    }
   ],
   "source": [
    "# The pulse gate circuit is obtained via the `pulse_gate_circuit` attribute\n",
    "pulse_circuit = compiler_output.pulse_gate_circuit\n",
    "\n",
    "custom_style = {\"formatter.general.fig_width\": 30, \"formatter.general.fig_unit_height\": 1}\n",
    "style = qiskit.visualization.timeline.IQXStandard(**custom_style)\n",
    "\n",
    "qiskit.visualization.timeline_drawer(pulse_circuit, idle_wires=False, style=style)"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "ebd51e12",
   "metadata": {},
   "source": [
    "## Multiple Circuits Compilation\n",
    "\n",
    "All the functionalities we have seen so far can also be used on a multiple-circuit input as well. To illustrate this, let us create a different example two-qubit circuit: a Bell-state circuit."
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 6,
   "id": "afe9537a",
   "metadata": {},
   "outputs": [
    {
     "data": {
      "text/html": [
       "<pre style=\"overflow: auto; white-space: pre;\">0: ───H───@───M───\n",
       "          │   │\n",
       "1: ───────X───M───</pre>"
      ],
      "text/plain": [
       "0: ───H───@───M───\n",
       "          │   │\n",
       "1: ───────X───M───"
      ]
     },
     "execution_count": 6,
     "metadata": {},
     "output_type": "execute_result"
    }
   ],
   "source": [
    "# Create second circuit\n",
    "bell_circuit = cirq.Circuit(\n",
    "    cirq.H(qubits[0]), cirq.CNOT(qubits[0], qubits[1]), cirq.measure(qubits[0], qubits[1])\n",
    ")\n",
    "\n",
    "# Visualize second circuit\n",
    "bell_circuit"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "b63696a1",
   "metadata": {},
   "source": [
    "By passing multiple circuits as a list to the `ibmq_compile` endpoint, we can compile all of them individually with a single call to the endpoint. This will return all the corresponding compiled circuits and pulse gate circuits back as a list, like so:  "
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 7,
   "id": "31699457",
   "metadata": {},
   "outputs": [],
   "source": [
    "# Create list of circuits\n",
    "circuit_list = [circuit, bell_circuit]\n",
    "\n",
    "# Compile list of circuits\n",
    "compiler_output_list = service.ibmq_compile(circuit_list, \"ibmq_brisbane_qpu\")\n",
    "\n",
    "# The list of compiled output circuits is stored in the `circuits` attribute instead of `circuit`. Likewise for\n",
    "# pulse gate circuits.\n",
    "output_circuits = compiler_output_list.circuits\n",
    "pulse_gate_circuits = compiler_output_list.pulse_gate_circuits"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 8,
   "id": "2de5dbe1",
   "metadata": {},
   "outputs": [
    {
     "name": "stdout",
     "output_type": "stream",
     "text": [
      "Compiled circuit 1 \n",
      "\n"
     ]
    },
    {
     "data": {
      "text/html": [
       "<pre style=\"overflow: auto; white-space: pre;\">4: ───Rz(1.5π)───X^0.5───Rz(π)──────AceCR+-(Z side)───Rz(0.5π)───X^0.5───Rz(1.59π)───X^0.5───AceCR+-(Z side)───Rz(1.5π)───X^0.5───Rz(0.5π)───│───M────────────────\n",
       "                                    │                                                        │                                               │   │\n",
       "5: ───Rz(π)──────X^0.5───Rz(0.5π)───AceCR+-(X side)──────────────X^0.5───────────────────────AceCR+-(X side)───Rz(0.5π)───X^0.5───Rz(0.5π)───│───M(&#x27;q(0),q(1)&#x27;)───</pre>"
      ],
      "text/plain": [
       "4: ───Rz(1.5π)───X^0.5───Rz(π)──────AceCR+-(Z side)───Rz(0.5π)───X^0.5───Rz(1.59π)───X^0.5───AceCR+-(Z side)───Rz(1.5π)───X^0.5───Rz(0.5π)───│───M────────────────\n",
       "                                    │                                                        │                                               │   │\n",
       "5: ───Rz(π)──────X^0.5───Rz(0.5π)───AceCR+-(X side)──────────────X^0.5───────────────────────AceCR+-(X side)───Rz(0.5π)───X^0.5───Rz(0.5π)───│───M('q(0),q(1)')───"
      ]
     },
     "execution_count": 8,
     "metadata": {},
     "output_type": "execute_result"
    }
   ],
   "source": [
    "# Visualize the first compiled circuit\n",
    "print(\"Compiled circuit 1 \\n\")\n",
    "output_circuits[0]"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 9,
   "id": "81996430",
   "metadata": {},
   "outputs": [
    {
     "data": {
      "image/png": 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      "text/plain": [
       "<Figure size 3000x300 with 1 Axes>"
      ]
     },
     "execution_count": 9,
     "metadata": {},
     "output_type": "execute_result"
    }
   ],
   "source": [
    "# Visualize the pulse gate circuit for the first compiled circuit\n",
    "qiskit.visualization.timeline_drawer(pulse_gate_circuits[0], idle_wires=False, style=style)"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 10,
   "id": "39c2b1d9",
   "metadata": {},
   "outputs": [
    {
     "name": "stdout",
     "output_type": "stream",
     "text": [
      "Compiled circuit 2 \n",
      "\n"
     ]
    },
    {
     "data": {
      "text/html": [
       "<pre style=\"overflow: auto; white-space: pre;\">4: ───Rz(0.5π)───X^0.5───AceCR+-(Z side)───Rz(0.5π)───X^0.5───│───M────────────────\n",
       "                         │                                    │   │\n",
       "5: ──────────────────────AceCR+-(X side)───Rz(0.5π)───X^0.5───│───M(&#x27;q(0),q(1)&#x27;)───</pre>"
      ],
      "text/plain": [
       "4: ───Rz(0.5π)───X^0.5───AceCR+-(Z side)───Rz(0.5π)───X^0.5───│───M────────────────\n",
       "                         │                                    │   │\n",
       "5: ──────────────────────AceCR+-(X side)───Rz(0.5π)───X^0.5───│───M('q(0),q(1)')───"
      ]
     },
     "execution_count": 10,
     "metadata": {},
     "output_type": "execute_result"
    }
   ],
   "source": [
    "# Visualize the second compiled circuit\n",
    "print(\"Compiled circuit 2 \\n\")\n",
    "output_circuits[1]"
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 11,
   "id": "7fb554e4",
   "metadata": {},
   "outputs": [
    {
     "data": {
      "image/png": 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      "text/plain": [
       "<Figure size 3000x300 with 1 Axes>"
      ]
     },
     "execution_count": 11,
     "metadata": {},
     "output_type": "execute_result"
    }
   ],
   "source": [
    "# Visualize the pulse gate circuit for the second compiled circuit\n",
    "qiskit.visualization.timeline_drawer(pulse_gate_circuits[1], idle_wires=False, style=style)"
   ]
  },
  {
   "cell_type": "markdown",
   "id": "501f2692",
   "metadata": {},
   "source": [
    "## Using the Superstaq Simulator\n",
    "\n",
    "Lastly, we will show (a) how to submit a circuit to a backend and (b) how to simulate circuit execution. Simulation is available to free trial users, and can be done by passing the `\"dry-run\"` method parameter when calling `create_job()` on the Superstaq service."
   ]
  },
  {
   "cell_type": "code",
   "execution_count": 12,
   "id": "39643374",
   "metadata": {},
   "outputs": [
    {
     "name": "stdout",
     "output_type": "stream",
     "text": [
      "{'11': 504, '00': 496}\n"
     ]
    }
   ],
   "source": [
    "# Create job that submits to IBM Quantum backend\n",
    "job = service.create_job(\n",
    "    bell_circuit,\n",
    "    repetitions=1000,\n",
    "    target=\"ibmq_brisbane_qpu\",\n",
    "    method=\"dry-run\",  # Specify \"dry-run\" as the method to run Superstaq simulation\n",
    ")\n",
    "\n",
    "# Get the counts from the measurement\n",
    "print(job.counts(0))"
   ]
  }
 ],
 "metadata": {
  "kernelspec": {
   "display_name": "Python 3 (ipykernel)",
   "language": "python",
   "name": "python3"
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  "language_info": {
   "codemirror_mode": {
    "name": "ipython",
    "version": 3
   },
   "file_extension": ".py",
   "mimetype": "text/x-python",
   "name": "python",
   "nbconvert_exporter": "python",
   "pygments_lexer": "ipython3",
   "version": "3.9.16"
  }
 },
 "nbformat": 4,
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