2021
DOI: 10.48550/arxiv.2111.08152
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Optimal scaling quantum linear systems solver via discrete adiabatic theorem

Abstract: Recently, several approaches to solving linear systems on a quantum computer have been formulated in terms of the quantum adiabatic theorem for a continuously varying Hamiltonian. Such approaches enabled near-linear scaling in the condition number κ of the linear system, without requiring a complicated variable-time amplitude amplification procedure. However, the most efficient of those procedures is still asymptotically sub-optimal by a factor of log(κ). Here, we prove a rigorous form of the adiabatic theorem… Show more

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Cited by 10 publications
(30 citation statements)
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“…The QSVT framework also provides algorithms for a variety of other linear algebraic routines such as implementing singular-value-threshold projectors [138,188] and matrix-vector multiplication [73]. Alternatively to QLS based on the QSVT, there is a discrete-time adiabatic (Section 3.2.2) approach [117] to the QLSP by Costa et al [99] that has optimal [160] query complexity: linear in κ and logarithmic in 1/ . Since QLS algorithms invert Hermitian matrices, they can also be used to compute the Moore-Penrose pseudoinverse of an arbitrary matrix.…”
Section: Quantum Linear Systemsmentioning
confidence: 99%
See 1 more Smart Citation
“…The QSVT framework also provides algorithms for a variety of other linear algebraic routines such as implementing singular-value-threshold projectors [138,188] and matrix-vector multiplication [73]. Alternatively to QLS based on the QSVT, there is a discrete-time adiabatic (Section 3.2.2) approach [117] to the QLSP by Costa et al [99] that has optimal [160] query complexity: linear in κ and logarithmic in 1/ . Since QLS algorithms invert Hermitian matrices, they can also be used to compute the Moore-Penrose pseudoinverse of an arbitrary matrix.…”
Section: Quantum Linear Systemsmentioning
confidence: 99%
“…These potentially reduce the original HHL's quadratic dependence on sparsity. HHL's query complexity, which is independent of the complexity of Hamiltonian simulation, is O(κ 2 / ) [99].…”
Section: Quantum Linear Systemsmentioning
confidence: 99%
“…Such state preparation methods are efficient, provided that the rate of change of the Hamiltonian is small compared to an appropriate power of the eigenvalue gap [40]. These approaches are widely used in quantum simulation, linear systems and other algorithms [41,42,43,44]. The results of [43,44] show how to implement a discrete version of adiabatic state preparation that does not reduce down to a smooth transition of the eigenstate at the initial time to the eigenstate at the end time.…”
Section: Adiabatic State Preparationmentioning
confidence: 99%
“…These approaches are widely used in quantum simulation, linear systems and other algorithms [41,42,43,44]. The results of [43,44] show how to implement a discrete version of adiabatic state preparation that does not reduce down to a smooth transition of the eigenstate at the initial time to the eigenstate at the end time. This lack of explicit time dependence allows qubitization to be used; whereas prior to this work it was unclear how one could use the technique to perform adiabatic preparation of eigenstates.…”
Section: Adiabatic State Preparationmentioning
confidence: 99%
“…As with classical algorithms, matching the problem to the algorithm is crucial. The first class was pioneered by the Harrow-Hasidim-Lloyd (HHL) algorithm [12], with later improvements [3,8,20,9]. These algorithms are suitable for fault tolerant devices as they rely on subroutines such as Hamiltonian simulation for potentially long times.…”
Section: Introductionmentioning
confidence: 99%