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Benchmarking Quantum Fourier Transform Circuits with the Steane Code

Exploring the performance of quantum circuits using the Steane error correction method.

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Quantum computing is a new field that uses the principles of quantum mechanics to process information. One of the key tasks in quantum computing is the Quantum Fourier Transform (QFT). This operation is essential in many quantum algorithms, including those for factoring numbers and searching databases. Essentially, QFT helps in converting quantum states into a form that makes certain calculations easier.

What is the Steane Code?

The Steane code is a method of Quantum Error Correction. It encodes information about a logical qubit (the basic unit of quantum information) into multiple physical qubits (the actual hardware used to perform calculations). The Steane code is designed to protect quantum information from errors that can occur due to noise and other disturbances in the environment.

This coding uses a total of seven physical qubits to protect a single logical qubit. The distance of the code is three, meaning it can detect and correct for all single-qubit errors. This is important because it ensures that even if one qubit suffers from an error, the overall information can still be retrieved accurately.

The Challenge of Quantum Error Correction

Quantum error correction (QEC) is crucial as quantum computers grow larger. As more qubits are added, the likelihood of errors increases. QEC aims to manage these errors by encoding qubits, applying error-correcting codes, and performing corrections through a process called syndrome extraction.

However, implementing these codes is not straightforward. The aim is to ensure that the error rates of the encoded circuits are lower than those of circuits without encoding. This presents various challenges in the design and execution of quantum circuits.

Benchmarking QFT Circuits

In the context of trapped-ion quantum computers, we can benchmark logical circuits that perform the Quantum Fourier Transform. This involves running tests to determine how well these circuits behave when carrying out QFT.

Benchmarking can be divided into two levels: component-level, which assesses the performance of individual gates, and system-level, which measures the overall execution of quantum circuits. Assessing whether the error rates at the component level translate to the overall performance is essential for confidence in calculations performed on quantum processors.

The Experiment

In our investigation, we used a quantum computing platform that features trapped-ion technology, specifically the Quantinuum H-series quantum computers. These systems allow for precise control of qubit interactions and measurements.

We implemented three-qubit circuits for the QFT using the Steane code. Our goal was to assess how well these circuits performed under various conditions.

Logical Gates and Rotations

To perform the QFT, we needed multiple logical gates. These gates can be categorized as two-qubit gates (which involve interactions between pairs of qubits) and single-qubit rotations (which involve changes to individual qubits).

In our setup, we utilized transversal gates, which are applied in such a way that errors can be more easily managed. Meanwhile, non-Clifford gates, which allow for more complex rotations, were implemented through a process involving teleportation and state preparation.

Benchmarking Logical Gates

The first step involved benchmarking the individual logical components using different methods. One method, randomized benchmarking, was used for the two-qubit gates. This technique helps determine the average performance of a gate over a series of random operations.

In our experiments, we achieved high levels of fidelity for the logical two-qubit gates, indicating that they performed close to their ideal behavior. However, the non-Clifford gate showed lower fidelity, revealing a vulnerability that may impact overall circuit performance.

Implementing the QFT

Next, we implemented the full QFT circuit. This involved two different methods for performing control operations. The first utilized a teleportation gadget, while the second relied on logical mid-circuit measurements. Both methods were tested to see how well they maintained performance when subjected to different states.

The QFT circuit was applied to a set of input states, allowing us to calculate a lower bound on the fidelity of the process. This lower bound helped us assess how accurately the circuit performed in transforming states.

Results of the Experiment

The experimental results showed that the QFT circuits had varying levels of fidelity, depending on the method used and the input states. It was observed that when we accounted for certain measurements, the average fidelity increased. However, even with these adjustments, the fidelity of the encoded QFT circuits remained lower than that of unencoded circuits.

Ultimately, our findings indicated that either a better error-correcting code or a fault-tolerant circuit design would be necessary for our logical circuits to outperform their physical counterparts.

Analysis of Errors

A significant portion of the circuit errors stemmed from the logical non-Clifford gates. While we were able to measure the error rates, the total error observed during the benchmarking exceeded what could be attributed solely to component-level benchmarks. This suggests that there are other sources of error, possibly from memory issues or the way information spreads during operations.

Closing the Gap

To make progress in practical quantum computing, it is crucial to bridge the gap between component-level performance and system-level outcomes. Understanding and reducing the impact of different error sources will pave the way for better designs and ultimately more effective quantum computers.

Future Directions

Research in quantum computing is ongoing, and many areas remain ripe for exploration. This includes identifying the best codes and protocols for specific tasks, as well as developing better error correction methods. Future studies will need to focus not only on improving the technology but also on refining the methodologies used to assess circuit performance.

Overall, the potential for quantum computing remains vast, and with continued effort, we can unlock its capabilities to solve complex problems and enhance our computational power in ways currently unimaginable.

Conclusion

In conclusion, the work on benchmarking logical three-qubit circuits performing the Quantum Fourier Transform offers crucial insights into the workings of quantum error correction and circuit design. The advances made in understanding how individual components perform give a solid foundation for future developments in this field. The lessons learned from this work will guide researchers as they push the boundaries of what is possible with quantum technology, moving ever closer to practical and scalable quantum computing solutions.

Original Source

Title: Benchmarking logical three-qubit quantum Fourier transform encoded in the Steane code on a trapped-ion quantum computer

Abstract: We implement logically encoded three-qubit circuits for the quantum Fourier transform (QFT), using the [[7,1,3]] Steane code, and benchmark the circuits on the Quantinuum H2-1 trapped-ion quantum computer. The circuits require multiple logical two-qubit gates, which are implemented transversally, as well as logical non-Clifford single-qubit rotations, which are performed by non-fault-tolerant state preparation followed by a teleportation gadget. First, we benchmark individual logical components using randomized benchmarking for the logical two-qubit gate, and a Ramsey-type experiment for the logical $T$ gate. We then implement the full QFT circuit, using two different methods for performing a logical control-$T$, and benchmark the circuits by applying it to each basis state in a set of bases that is sufficient to lower bound the process fidelity. We compare the logical QFT benchmark results to predictions based on the logical component benchmarks.

Authors: Karl Mayer, Ciarán Ryan-Anderson, Natalie Brown, Elijah Durso-Sabina, Charles H. Baldwin, David Hayes, Joan M. Dreiling, Cameron Foltz, John P. Gaebler, Thomas M. Gatterman, Justin A. Gerber, Kevin Gilmore, Dan Gresh, Nathan Hewitt, Chandler V. Horst, Jacob Johansen, Tanner Mengle, Michael Mills, Steven A. Moses, Peter E. Siegfried, Brian Neyenhuis, Juan Pino, Russell Stutz

Last Update: 2024-04-12 00:00:00

Language: English

Source URL: https://arxiv.org/abs/2404.08616

Source PDF: https://arxiv.org/pdf/2404.08616

Licence: https://creativecommons.org/licenses/by/4.0/

Changes: This summary was created with assistance from AI and may have inaccuracies. For accurate information, please refer to the original source documents linked here.

Thank you to arxiv for use of its open access interoperability.

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