{ "cells": [ { "cell_type": "code", "execution_count": 1, "id": "4e23ccc6", "metadata": { "execution": { "iopub.execute_input": "2024-10-11T06:14:27.563779Z", "iopub.status.busy": "2024-10-11T06:14:27.563392Z", "iopub.status.idle": "2024-10-11T06:14:27.569506Z", "shell.execute_reply": "2024-10-11T06:14:27.568751Z" }, "nbsphinx": "hidden" }, "outputs": [], "source": [ "# Copyright 2024 Keysight Technologies Inc." ] }, { "cell_type": "raw", "id": "eb70cab2", "metadata": { "raw_mimetype": "text/restructuredtext" }, "source": [ "IQ Distribution experiment\n", "==========================\n", "\n", "This guide shows how to measure the I/Q distribution of both the ground state and\n", "excited state of a qubit using a variable amplitude X pulse followed by a measurement.\n", "\n", "We can use the pre-defined\n", ":py:class:`~keysight.qcs.experiments.IQDistributionExperiment` and our example\n", "calibration set from the experiments library. To start out, we define an\n", "empty :py:class:`~keysight.qcs.channels.ChannelMapper` to instantiate our experiment\n", "for a single qubit." ] }, { "cell_type": "code", "execution_count": 2, "id": "de919c71", "metadata": { "execution": { "iopub.execute_input": "2024-10-11T06:14:27.573026Z", "iopub.status.busy": "2024-10-11T06:14:27.572721Z", "iopub.status.idle": "2024-10-11T06:14:31.107753Z", "shell.execute_reply": "2024-10-11T06:14:31.106896Z" }, "lines_to_next_cell": 2 }, "outputs": [ { "data": { "text/html": [ "\n", "\n", "\n", "\n", "\n", "\n", "\n", "\n", "\n", "\n", "\n", "\n", "\n", "\n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", "
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ValuesArray(name=rx_angles, shape=(1,), dtype=float, unit=none)
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Duration130 ns
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" ] }, "metadata": {}, "output_type": "display_data" } ], "source": [ "iq_experiment.compiled_program.render(\n", " channel_subplots=False,\n", " lo_frequency=5e9,\n", " sweep_index=1,\n", " sample_rate=5e9,\n", ")" ] }, { "cell_type": "raw", "id": "e607370d", "metadata": { "raw_mimetype": "text/restructuredtext" }, "source": [ "To execute this experiment, we can simply run" ] }, { "cell_type": "code", "execution_count": 5, "id": "0bb7c4e8", "metadata": { "execution": { "iopub.execute_input": "2024-10-11T06:14:32.030773Z", "iopub.status.busy": "2024-10-11T06:14:32.030079Z", "iopub.status.idle": "2024-10-11T06:14:32.107725Z", "shell.execute_reply": "2024-10-11T06:14:32.106857Z" } }, "outputs": [], "source": [ "if run_on_hw:\n", " iq_experiment.execute()\n", "else:\n", " # load in a previously executed version of this experiment\n", " iq_experiment = qcs.load(\"IQDistribution.qcs\")" ] }, { "cell_type": "raw", "id": "6fd0db9a", "metadata": { "raw_mimetype": "text/restructuredtext" }, "source": [ "For the purposes of this demonstration, we added a second \"ancilla\" qubit to the\n", "IQ distribution program and connected the physical output channels for our qubit to\n", "the digizer associated with the ancilla to allow us to capture the full pulse\n", "sequence." ] }, { "cell_type": "code", "execution_count": 6, "id": "4eac7a1b", "metadata": { "execution": { "iopub.execute_input": "2024-10-11T06:14:32.111763Z", "iopub.status.busy": "2024-10-11T06:14:32.111418Z", "iopub.status.idle": "2024-10-11T06:14:32.125002Z", "shell.execute_reply": "2024-10-11T06:14:32.124162Z" } }, "outputs": [ { "data": { "text/html": [ "\n", "\n", "\n", "\n", "\n", "\n", "\n", "\n", "\n", "\n", "\n", "\n", "\n", "\n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", " \n", "
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