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# How to Contribute | ||
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## Contributor License Agreement | ||
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## Code reviews | ||
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All submissions, including submissions by project members, require review. We | ||
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## Community Guidelines | ||
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This project follows | ||
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# qsim and qsimh | ||
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Quantum circuit simulators qsim and qsimh. These simulators were used for cross | ||
entropy benchmarking in | ||
[[1]](https://www.nature.com/articles/s41586-019-1666-5). | ||
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[[1]](https://www.nature.com/articles/s41586-019-1666-5), F. Arute et al, | ||
"Quantum Supremacy Using a Programmable Superconducting Processor", | ||
Nature 574, 505, (2019). | ||
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## qsim | ||
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qsim is a Schrödinger full state-vector simulator. It computes all the $$2^n$$ | ||
amplitudes of the state vector, where $$n$$ is the number of qubits. | ||
Essentially, the simulator performs matrix-vector multiplications repeatedly. | ||
One matrix-vector multiplication corresponds to applying one gate. | ||
The total runtime is proportional to $$g2^n$$, where $$g$$ is the number of | ||
2-qubit gates. To speed up the simulator, we use gate fusion | ||
[[2]](https://arxiv.org/abs/1601.07195), single precision arithmetic, AVX/FMA | ||
instructions for vectorization and OpenMP for multi-threading. | ||
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[[2]](https://arxiv.org/abs/1601.07195) M. Smelyanskiy, N. P. Sawaya, | ||
A. Aspuru-Guzik, "qHiPSTER: The Quantum High Performance Software Testing | ||
Environment", arXiv:1601.07195 (2016). | ||
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## qsimh | ||
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qsimh is a hybrid Schrödinger-Feynman simulator | ||
[[3]](https://arxiv.org/abs/1807.10749). The lattice is split into two parts | ||
and the Schmidt decomposition is used to decompose 2-qubit gates on the | ||
cut. If the Schmidt rank of each gate is $$m$$ and the number of gates on | ||
the cut is $$k$$ then there are $$m^k$$ paths. To simulate a circuit with | ||
fidelity one, one needs to simulate all the $$=m^k$$ paths and sum the results. | ||
The total runtime is proportional to $$(2^{n_1} + 2^{n_2})m^k$$, where $$n_1$$ | ||
and $$n_2$$ are the qubit numbers in the first and second parts. Path | ||
simulations are independent of each other and can be trivially parallelized | ||
to run on supercomputers or in data centers. Note that one can run simulations | ||
with fidelity $$F < 1$$ just by summing over a fraction $$F$$ of all the paths. | ||
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A two level checkpointing scheme is used to improve performance. Say, there | ||
are $$k$$ gates on the cut. We split those into three parts: $$p+r+s=k$$, where | ||
$$p$$ is the number of "prefix" gates, $$r$$ is the number of "root" gates and | ||
$$s$$ is the number of "suffix" gates. The first checkpoint is executed after | ||
applying all the gates up to and including the prefix gates and the second | ||
checkpoint is executed after applying all the gates up to and including the | ||
root gates. The full summation over all the paths for the root and suffix gates | ||
is performed. | ||
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If $$p>0$$ then one such simulation gives $$F\approx 1/m^p$$ (for all the | ||
prefix gates having the same Schmidt rank m). One needs to run $m^p$ | ||
simulations with different prefix paths and sum the results to get $$F = 1$$. | ||
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[[3]](https://arxiv.org/abs/1807.10749) I. L. Markov, A. Fatima, S. V. Isakov, | ||
S. Boixo, "Quantum Supremacy Is Both Closer and Farther than It Appears", | ||
arXiv:1807.10749 (2018). | ||
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## C++ Usage | ||
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The code is basically designed as a library. The user can modify sample | ||
aplications in [apps](apps) to meet their own needs. The usage of sample | ||
applications is described in [docs](docs/usage.md). | ||
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### Input format | ||
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Circuit input format is described in [docs](docs/input_format.md). | ||
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### Sample Circuits | ||
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A number of sample circuits are provided in | ||
circuits. | ||
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### Unit tests | ||
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Unit tests are located in [tests](tests). The Google test framework is used. | ||
Paths to Google test include files and to Google test library files should be | ||
edited in [tests/make.sh](tests/make.sh). | ||
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## Cirq Usage | ||
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[Cirq](https://github.com/quantumlib/cirq) is a framework for modeling and | ||
invoking Noisy Intermediate Scale Quantum (NISQ) circuits. | ||
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To run qsim on Google Cirq circuits, or just to call the simulator from Python, | ||
see [docs](docs/cirq_interface.md). | ||
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## Authors | ||
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Sergei Isakov (Google): qsim and qsimh simulators, Vamsi Krishna Devabathini | ||
(Google): Cirq interface. | ||
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## Disclaimer | ||
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This is not an officially supported Google product. |
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# Copyright 2019 Google LLC. All Rights Reserved. | ||
# | ||
# Licensed under the Apache License, Version 2.0 (the "License"); | ||
# you may not use this file except in compliance with the License. | ||
# You may obtain a copy of the License at | ||
# | ||
# https://www.apache.org/licenses/LICENSE-2.0 | ||
# | ||
# Unless required by applicable law or agreed to in writing, software | ||
# distributed under the License is distributed on an "AS IS" BASIS, | ||
# WITHOUT WARRANTIES OR CONDITIONS OF ANY KIND, either express or implied. | ||
# See the License for the specific language governing permissions and | ||
# limitations under the License. | ||
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#!/bin/bash | ||
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g++ -O3 -mavx2 -mfma -fopenmp -lgomp -o qsim1 qsim1.cc | ||
g++ -O3 -mavx2 -mfma -fopenmp -lgomp -o qsim2 qsim2.cc | ||
g++ -O3 -mavx2 -mfma -fopenmp -lgomp -o qsim3 qsim3.cc | ||
g++ -O3 -mavx2 -mfma -fopenmp -lgomp -o qsimh1 qsimh1.cc | ||
g++ -O3 -mavx2 -mfma -fopenmp -lgomp -o qsimh2 qsimh2.cc |
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