DOI: 10.5281/zenodo.8253792
title: Data for "Phase transition in Random Circuit Sampling"

description: Purpose

This dataset defines the Random Quantum Circuits (RQCs) used in our paper "Phase transition in Random Circuit Sampling" and lists the bitstrings observed in the experimental executions of the circuits on the Sycamore  processor. See [1] for more details about the experiment. This data upload is modeled after that of [5].

Background

Circuit parameters

RQCs posted here are uniquely identifiedusing the following parameters:



 `n`: number of qubits (69, 70),

 `m`: number of cycles (04, 06, 08, ..., 28, 30),

 `s`: seed for the pseudo-random number generator (000, 001, ..., 595),

 `patches`: the number of patches,

 `p`: sequence of coupler activation patterns (`ABCD`, `ABCDCDAB`),

 `num_sq`: the number of distinct single-qubit gates (3, 8),

 the date on which the data was collected, included in yymmdd format in the filename, and

 `phase_match`: included in the file name if phase matching was performed.


See Figure S25 in [2] and Figure 3 of [1] for the coupler activation patterns and Figure 4 of [1] for illustrations of the patches. Also see code snippets below for visualizing the patches and activation patterns from the provided circuits.When `num_sq` is 8, the single-qubit gates are chosen randomly from \(Z^p X^{1/2} Z^{-p}\), with \(p \in \{-1, -3/4, -1/2, -1/4, 0, 1/4, 1/2, 3/4 \}\), whereas when `num_sq` is 3, they are chosen randomly from among \(\sqrt X\), \(\sqrt Y\), and \(\sqrt W\). Phase matching is described in Appendix C.1 of [1]. Note that circuits which share the same seed `s` share the same initial gate sequence.

Content description

For each RQC there are four files in the dataset: * original RQC specification in QSIM format, named `circuit_\*.qsim`, * derived RQC specificaton as python code using cirq, named `circuit_\*.py`, * derived RQC specification in QASM format, named `circuit_\*.qasm`, * bitstrings observed in experiments, named `measurements_\*.txt`.

The asterisk \* in the names above stands for a string specifying the parameters identifying a RQC. For example,`circuit_n70_m24_s00_patches3_pABCD_num_sq8_221014_phase_match.qasm` contains the definition of the 70-qubit, 24-cycle RQC with PRNG seed 0, 3 patches, a simplifiable sequence of coupler activation patterns (i.e. ABCD), and 8 distinct single-qubit gates, taken on October 14, 2022, with phase matching, in the QASM format.

Files are grouped by parameters `n`, `m`, and `patches` and into compressed tarballs. For example, tarball `n69_m04_patches2.tar.gz` contains all RQCs and measurement files for circuits with 69 qubits, 4 cycles, and 2 patches.

Circuit file formats

QSIM format

First line specifies the number of qubits n. Each subsequent line specifies a single gate and consists of moment number, gate name and one or two qubits as a number in 0..n-1 optionally followed by gate parameters.

The circuits use the following gates: * `x_1_2`: parameter-free, single-qubit pi/2 rotation around the X axis of the Bloch sphere, see equation (45) in section VII of [2], * `y_1_2`: parameter-free, single-qubit pi/2 rotation around the Y axis of the Bloch sphere, see equation (46) in section VII of [2], * `hz_1_2`: parameter-free, single-qubit pi/2 rotation around the X+Y axis of the Bloch sphere, see equation (47) in section VII of [2], * `rz`: single-qubit rotation around the Z axis of the Bloch sphere through the angle specified in radians by the gate's sole parameter, * `fsim`: two-qubit gate corresponding to the composition of the iSWAP and CPHASE gates and taking two parameters in radians: theta (the negative iSWAP angle) and phi (the CPHASE angle), see equation (48) in section VII of [2].

Note that the two-qubit gates executed in our experiments on Sycamore belong to the five-parameter family of two-qubit gates that preserve the number of 0 and 1 states of the qubits. Each such gate can be decomposed into one fsim gate and four rz gates. Therefore, one cycle consisting of one application ofsingle-qubit gates and one application of two-qubit gates is represented in the file using four moments. The first moment contains `x_1_2`, `y_1_2` and `hz_1_2` gates. The other three moments use `rz` and `fsim` gates to describe the two-qubit gates used in the experiments. See section VII in [2] for more details about the Sycamore gates and their decomposition.

Qubits are specified as numbers in 0..n-1 and hence do not directly indicate qubit location on the device.

Python/cirq format

Each python file defines two variables: QUBIT_ORDER and CIRCUIT. The former is a python list object containing `cirq.GridQubit` objects initialized with therow and column of each qubit on the device. The latter is a `cirq.Circuit` object initialized with all gate operations contained in the circuit. The files have been tested using cirq version 1.2.0.dev20230613162638.

The following code snippet illustrates how one can use cirq and our circuit definitions to compute output state amplitudes:

$ python -i circuit_n70_m24_s00_patches3_pABCD_num_sq8_221014_phase_match.py
>>> cirq.final_wavefunction(CIRCUIT, qubit_order=QUBIT_ORDER)
array([ 0.00263724+0.00337646j,  0.0009332 +0.00111853j,
       -0.0007809 +0.00386362j, ...,  0.00574739-0.00027827j,
       -0.00254766+0.00299345j,  0.00396056+0.00312335j], dtype=complex64)

 

See [3] for more details about cirq.

QASM format

Each QASM file has been generated using cirq and specifies the RQC decomposed into CNOT and single-qubit gates. The files have been generated using cirq.

See [4] for more details about the format.

Measurements file format

Each line contains the bitstring obtained in a single execution of the RQC on Sycamore. The first, left-most position corresponds to the qubit 0 in QSIM format and the first qubit in the `QUBIT_ORDER` list in the python/cirq files.

To visualize the patches

After loading `CIRCUIT` from the appropriate `.py` file, the following code snippet can be used to visualize the patches:

import cirq
import matplotlib.pyplot as plt
pairs = set()
for moment in CIRCUIT:
    for op in moment.operations:
        q = op.qubits
        if len(q) > 1:
            assert len(q) == 2
            pairs.add(tuple(sorted(q)))
d = {p:1 for p in pairs}
heatmap = cirq.TwoQubitInteractionHeatmap(d)
_, ax = plt.subplots(figsize=(8, 8))
_ = heatmap.plot(ax)

 

Visualize the activation patterns

The activation pattern sequence can also be visualized in a similar manner. After loading `CIRCUIT` from the appropriate `.py` pyle, the following code snippet can be used to visualize the activation patterns:

import cirq
import matplotlib.pyplot as plt
def has_two_qubit_gates(moment):
    has = False
    for op in moment.operations:
        if len(op.qubits) > 1:
            has = True
            break
    return has

def plot_pairs(moment):
    pairs = set()
    for op in moment.operations:
        q = op.qubits
        if len(q) > 1:
            assert len(q) == 2
            pairs.add( tuple(sorted(q)) )
    d = {p:1 for p in pairs}
    heatmap = cirq.TwoQubitInteractionHeatmap(d)
    _, ax = plt.subplots(figsize=(8, 8))
    _ = heatmap.plot(ax)
    return ax

moments = [_ for _ in CIRCUIT if has_two_qubit_gates(_)]

moment_to_visualize = moments[0] # iterate through this manually

plot_pairs(moment_to_visualize)

 

Content listing

The dataset includes the following tarball files:

n69_m04_patches2.tar.gz (80 files)
n69_m04_patches3.tar.gz (80 files)
n69_m06_patches2.tar.gz (80 files)
n69_m06_patches3.tar.gz (80 files)
n69_m08_patches2.tar.gz (80 files)
n69_m08_patches3.tar.gz (80 files)
n69_m10_patches2.tar.gz (80 files)
n69_m10_patches3.tar.gz (80 files)
n69_m12_patches2.tar.gz (80 files)
n69_m12_patches3.tar.gz (80 files)
n69_m14_patches2.tar.gz (80 files)
n69_m14_patches3.tar.gz (80 files)
n69_m16_patches2.tar.gz (80 files)
n69_m16_patches3.tar.gz (80 files)
n69_m18_patches2.tar.gz (80 files)
n69_m18_patches3.tar.gz (80 files)
n69_m20_patches2.tar.gz (80 files)
n69_m20_patches3.tar.gz (80 files)
n69_m22_patches2.tar.gz (80 files)
n69_m22_patches3.tar.gz (80 files)
n69_m24_patches1.tar.gz (4 files)
n69_m24_patches2.tar.gz (80 files)
n69_m24_patches3.tar.gz (80 files)
n69_m26_patches2.tar.gz (80 files)
n69_m26_patches3.tar.gz (80 files)
n69_m28_patches2.tar.gz (80 files)
n69_m28_patches3.tar.gz (80 files)
n69_m30_patches2.tar.gz (80 files)
n69_m30_patches3.tar.gz (80 files)
n70_m16_patches2.tar.gz (960 files)
n70_m16_patches3.tar.gz (1040 files)
n70_m16_patches9.tar.gz (160 files)
n70_m18_patches2.tar.gz (960 files)
n70_m18_patches3.tar.gz (1040 files)
n70_m18_patches9.tar.gz (160 files)
n70_m20_patches2.tar.gz (960 files)
n70_m20_patches3.tar.gz (1040 files)
n70_m20_patches9.tar.gz (160 files)
n70_m22_patches2.tar.gz (960 files)
n70_m22_patches3.tar.gz (1040 files)
n70_m22_patches9.tar.gz (160 files)
n70_m24_patches1.tar.gz (56 files)
n70_m24_patches2.tar.gz (960 files)
n70_m24_patches3.tar.gz (1040 files)
n70_m24_patches9.tar.gz (160 files)
n70_m26_patches1.tar.gz (4 files)
n70_m26_patches2.tar.gz (880 files)
n70_m26_patches3.tar.gz (960 files)
n70_m26_patches9.tar.gz (160 files)67-qubit data (described below)

 

Additionally, the file  Figures 2 and 3 data.zip contains processed data (9 files in Pickle format) that are shown in Figures 2 and 3 of the paper.

The 67-qubit data files, n67_full.zip, n67_patches2.zip, and n67_patches3.zip are formatted differently. The circuits are savd in .json format and can be loaded with `cirq.read_json()`. The data files are in .npy format and can be opened with numpy.load(). The number of cycles (`m` elsewhere) is indicated after `d` in the filename. The contents of these zip files can be previewed with the "preview" button.

 

 

References

[1] Google AI Quantum and collaborators, "Phase transition in Random Circuit Sampling". arXiv:2304.11119

[2] Google AI Quantum and collaborators, Supplementary information for “Quantum supremacy using a programmable superconducting processor”. arXiv:1910.11333

[3] Cirq: A Python framework for creating, editing, and invoking Noisy Intermediate Scale Quantum (NISQ) circuits, https://github.com/quantumlib/Cirq.

[4] Cross, Andrew W.; Bishop, Lev S.; Smolin, John A.; Gambetta, Jay M. "Open Quantum Assembly Language", arXiv:1707.03429

[5] Martinis, John M. et al. (2022), "Quantum supremacy using a programmable superconducting processor", Dryad, Dataset, https://doi.org/10.5061/dryad.k6t1rj8
description: Data for arXiv:2304.11119