4.8 Article

Rodeo Algorithm for Quantum Computing

期刊

PHYSICAL REVIEW LETTERS
卷 127, 期 4, 页码 -

出版社

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevLett.127.040505

关键词

-

资金

  1. U.S. Department of Energy [DE-SC0018638, DE-SC0021152]
  2. Los Alamos National Laboratory
  3. Center for Excellence in Education
  4. U.S. Department of Energy (DOE) [DE-SC0018638, DE-SC0021152] Funding Source: U.S. Department of Energy (DOE)

向作者/读者索取更多资源

The rodeo algorithm can converge to the target eigenvector with exponential accuracy in a finite number of measurements. In addition to preparing eigenvectors, the method can also compute the full spectrum of the Hamiltonian. The speed for eigenstate preparation is exponentially faster than that for phase estimation or adiabatic evolution.
We present a stochastic quantum computing algorithm that can prepare any eigenvector of a quantum Hamiltonian within a selected energy interval [E - epsilon, E + epsilon) . In order to reduce the spectral weight of all other eigenvectors by a suppression factor d, the required computational effort scales as O[vertical bar log delta vertical bar/(p epsilon)], where p is the squared overlap of the initial state with the target eigenvector. The method, which we call the rodeo algorithm, uses auxiliary qubits to control the time evolution of the Hamiltonian minus some tunable parameter E. With each auxiliary qubit measurement, the amplitudes of the eigenvectors are multiplied by a stochastic factor that depends on the proximity of their energy to E. In this manner, we converge to the target eigenvector with exponential accuracy in the number of measurements. In addition to preparing eigenvectors, the method can also compute the full spectrum of the Hamiltonian. We illustrate the performance with several examples. For energy eigenvalue determination with error epsilon, the computational scaling is O[(log epsilon)(2)/(p epsilon)]. For eigenstate preparation, the computational scaling is O(log Delta/p), where. is the magnitude of the orthogonal component of the residual vector. The speed for eigenstate preparation is exponentially faster than that for phase estimation or adiabatic evolution.

作者

我是这篇论文的作者
点击您的名字以认领此论文并将其添加到您的个人资料中。

评论

主要评分

4.8
评分不足

次要评分

新颖性
-
重要性
-
科学严谨性
-
评价这篇论文

推荐

暂无数据
暂无数据