Abstract

The accurate evaluation of diagonal unitary operators is often the most resource-intensive element of quantum algorithms such as real-space quantum simulation and Grover search. Efficient circuits have been demonstrated in some cases but generally require ancilla registers, which can dominate the qubit resources. In this paper, we give a simple way to construct efficient circuits for diagonal unitaries without ancillas, using a correspondence between Walsh functions and a basis for diagonal operators. This correspondence reduces the problem of constructing the minimal-depth circuit within a given error tolerance, for an arbitrary diagonal unitary in the basis, to that of finding the minimal-length Walsh-series approximation to the function f(x). We apply this approach to the quantum simulation of the classical Eckart barrier problem of quantum chemistry, demonstrating that high-fidelity quantum simulations can be achieved with few qubits and low depth.

Highlights

  • Walsh FunctionsThe Paley-ordered Walsh functions are defined on the continuous interval 0 ≤ x < 1 as [12]. = δjl

  • The accurate evaluation of diagonal unitary operators is often the most resource-intensive element of quantum algorithms such as real-space quantum simulation and Grover search

  • We point out a correspondence between Walsh functions and a basis for diagonal operators that gives a simple way to construct efficient circuits for diagonal unitaries without ancillas

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Summary

Walsh Functions

The Paley-ordered Walsh functions are defined on the continuous interval 0 ≤ x < 1 as [12]. = δjl. The Paley-ordered Walsh functions are defined on the continuous interval 0 ≤ x < 1 as [12]. ETih-ethsebciotndineqthuealidtyyasdhiocwesxtphaantsitohne, k= functional form is the same whether x is continuous or discrete, the only difference being the number of bits in the expansion of x. This makes Walsh series useful for representing discretely sampled continuous functions. For Walsh functions up to order 2n, it is the group Z⊗2 n, which is formed by a basis for diagonal operators on n qubits.

Walsh Operators
OPTIMAL CIRCUIT CONSTRUCTIONS
EFFICIENT CIRCUITS FOR DIAGONAL UNITARIES
QUANTUM SIMULATION EXAMPLE
Real-space algorithm
Simulation
Error analysis
Findings
CONCLUSION
Full Text
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