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Advancements in Eigenstate Preparation Using Random Sampling

A new algorithm improves eigenstate estimation in quantum systems.

― 5 min read


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Estimating the properties of quantum systems made up of many interacting particles is a significant challenge in both traditional and quantum computing. Among these challenges is the task of preparing the eigenstates of these systems, which require knowing their energies and observable properties. Researchers have developed various techniques to tackle these problems, with a focus on Quantum Signal Processing and spectral filter methods being among the most promising.

Background

Quantum systems often exhibit complicated behaviors that require sophisticated mathematical frameworks for accurate description and prediction. Eigenstate preparation is crucial in allowing scientists to understand the fundamental properties of these systems. The energy of a system and the observable properties can provide insights into its behavior and interactions.

The Challenge of Eigenstate Preparation

Preparing the eigenstates of quantum systems can be a difficult task. The difficulty arises from the complexity of the systems themselves and the limitations of the computational resources available. Traditional methods can be inefficient, especially when the system size increases. Quantum computing offers a potential solution to this challenge, because it can perform certain calculations much faster than classical computers.

Quantum signal processing (QSP) is one such method that has shown near-optimal performance for estimating eigenstate properties. However, its implementation is still challenging, especially in the context of noisy intermediate-scale quantum (NISQ) computers, which have limitations regarding the number of qubits and the depth of quantum circuits.

Quantum Computing and Eigenstate Preparation

In quantum computing, algorithms that rely on quantum mechanics can solve problems that are otherwise difficult for classical computers. Quantum algorithms have been developed for various tasks, including eigenstate preparation, that leverage quantum properties to achieve speed improvements.

Techniques Used in Quantum Eigenstate Preparation

Several techniques can be employed to prepare the eigenstates of quantum systems:

  1. Quantum Phase Estimation (QPE): This technique efficiently estimates the phase of an eigenstate by querying the system multiple times. It is based on preparing the eigenstates of the quantum system and measuring their phases to deduce their energies.

  2. Spectral Filter Algorithms: These methods focus on filtering out unwanted eigenstates from a larger set to isolate the one of interest. They do this through the application of specific operators that enhance the measurement of the eigenstate.

  3. Quantum Signal Processing (QSP): QSP techniques utilize the properties of quantum states to optimally estimate eigenstate energies and their corresponding observable properties. This method has shown promise in achieving near-optimal resource requirements.

In recent years, researchers have concentrated on developing methods that minimize the resource requirements for quantum computations while maximizing the precision of the results.

Full-Stack Random Sampling Algorithm

A novel random sampling algorithm has been proposed that combines the strengths of existing techniques while addressing their weaknesses. This new full-stack approach allows for high precision in estimating eigenstate properties while ensuring that the circuit depth remains manageable, a critical factor for practical implementation on existing quantum hardware.

Overview of the Random Sampling Algorithm

The proposed algorithm uses a structured approach to estimate eigenstate properties. It leverages random sampling of quantum operations to effectively prepare the eigenstates and measure their properties. The main steps involve:

  1. Real-Time Evolution: The algorithm simulates the time evolution of the quantum system to create a large enough superposition of states. This superposition contains the target eigenstates, which are the focus of the estimation.

  2. Random Sampling of Operators: Rather than deterministically preparing states, the algorithm samples various operators that act on the quantum states. This random approach helps mitigate the depth of circuits while still providing accurate results.

  3. Error Compensation: The algorithm includes mechanisms to reduce errors associated with the Trotterization process, which approximates the evolution of quantum systems over time.

Advantages of the Proposed Method

The random sampling algorithm presents several advantages over traditional methods:

  • Reduced Circuit Depth: By employing random sampling, the algorithm can achieve results with significantly lower circuit depth, making it more suitable for NISQ devices.

  • Improved Precision: The combination of sophisticated error compensation techniques and random sampling allows for high precision in estimating the properties of eigenstates.

  • Scalability: The method scales well with system size, making it more feasible for larger quantum systems that would otherwise be impractical to study.

Resource Estimation for Quantum Algorithms

When considering the implementation of quantum algorithms, it is essential to analyze the resource requirements, including the number of qubits, the number of operations, and the overall complexity. Resource estimation informs researchers and engineers about the practical limits of their algorithms and helps them optimize them for real-world deployment.

Key Components of Resource Estimation

  1. Qubit Count: This refers to the total number of qubits required to perform the calculations. In many cases, the number of qubits directly influences the depth and complexity of the quantum circuits.

  2. Gate Count: This is a measure of how many gate operations are needed to execute the algorithm. It includes CNOT gates, single-qubit gates, and other operations that manipulate quantum states.

  3. Circuit Depth: This is the number of layers of gates that must be applied in sequence to obtain the final state. A lower circuit depth is desirable as it can significantly reduce the error rates associated with quantum operations.

Comparative Analysis of Methods

When analyzing different quantum algorithms, it is useful to compare their resource requirements. For example, the random sampling algorithm can achieve lower gate counts and circuit depths than traditional QPE-based methods, making it a more practical choice for NISQ devices.

Conclusion

Quantum computing holds the promise of solving complex problems related to quantum systems, including the estimation of eigenstate properties. The proposed random sampling algorithm integrates several techniques to achieve high precision and low circuit depth, making it suitable for current quantum hardware.

By optimizing resource requirements and providing a clear path for practical implementation, this approach contributes significantly to the ongoing efforts in quantum computing research. As technology continues to advance, methods like this will play an essential role in furthering our understanding of quantum systems and their applications across various fields.

Original Source

Title: High-precision and low-depth eigenstate property estimation: theory and resource estimation

Abstract: Estimating the eigenstate properties of quantum many-body systems is a long-standing, challenging problem for both classical and quantum computing. For the task of eigenstate preparation, quantum signal processing (QSP) has established near-optimal query complexity $O( \Delta^{-1} \log(\epsilon^{-1}) )$ by querying the block encoding of the Hamiltonian $H$ where $\Delta$ is the energy gap and $\epsilon$ is the target precision. However, QSP is challenging for both near-term noisy quantum computers and early fault-tolerant quantum computers (FTQC), which are limited by the number of logical qubits and circuit depth. To date, early FTQC algorithms have focused on querying the perfect time evolution $e^{-iHt}$. It remains uncertain whether early FTQC algorithms can maintain good asymptotic scaling at the gate level. Moreover, when considering qubit connectivity, the circuit depth of existing FTQC algorithms may scale suboptimally with system size. Here, we present a full-stack design of a random sampling algorithm for estimating the eigenenergy and the observable expectations on the eigenstates, which can achieve high precision and good system size scaling. The gate complexity has a logarithmic dependence on precision $ {O}(\log^{1+o(1)} (1/\epsilon))$ for generic Hamiltonians, which cannot achieved by methods using Trottersiation to realise $e^{-iHt}$ like in QETU. For $n$-qubit lattice Hamiltonians, our method achieves near-optimal system size dependence with the gate complexity $O(n^{1+o(1)})$. When restricting the qubit connectivity to a linear nearest-neighbour architecture, The method shows advantages in circuit depth, with $O(n^{o(1)})$ for lattice models and $O(n^{2+o(1)})$ for electronic structure problems. We compare the resource requirements (CNOT gates, T gates and qubit numbers) by phase estimation, QSP, and QETU, in lattice and molecular problems.

Authors: Jinzhao Sun, Pei Zeng, Tom Gur, M. S. Kim

Last Update: 2024-06-06 00:00:00

Language: English

Source URL: https://arxiv.org/abs/2406.04307

Source PDF: https://arxiv.org/pdf/2406.04307

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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