225 research outputs found
A Depth-Optimal Canonical Form for Single-qubit Quantum Circuits
Given an arbitrary single-qubit operation, an important task is to
efficiently decompose this operation into an (exact or approximate) sequence of
fault-tolerant quantum operations. We derive a depth-optimal canonical form for
single-qubit quantum circuits, and the corresponding rules for exactly reducing
an arbitrary single-qubit circuit to this canonical form. We focus on the
single-qubit universal H,T basis due to its role in fault-tolerant quantum
computing, and show how our formalism might be extended to other universal
bases. We then extend our canonical representation to the family of
Solovay-Kitaev decomposition algorithms, in order to find an
\epsilon-approximation to the single-qubit circuit in polylogarithmic time. For
a given single-qubit operation, we find significantly lower-depth
\epsilon-approximation circuits than previous state-of-the-art implementations.
In addition, the implementation of our algorithm requires significantly fewer
resources, in terms of computation memory, than previous approaches.Comment: 10 pages, 3 figure
A State Distillation Protocol to Implement Arbitrary Single-qubit Rotations
An important task required to build a scalable, fault-tolerant quantum
computer is to efficiently represent an arbitrary single-qubit rotation by
fault-tolerant quantum operations. Traditionally, the method for decomposing a
single-qubit unitary into a discrete set of gates is Solovay-Kitaev
decomposition, which in practice produces a sequence of depth
O(\log^c(1/\epsilon)), where c~3.97 is the state-of-the-art. The proven lower
bound is c=1, however an efficient algorithm that saturates this bound is
unknown. In this paper, we present an alternative to Solovay-Kitaev
decomposition employing state distillation techniques which reduces c to
between 1.12 and 2.27, depending on the setting. For a given single-qubit
rotation, our protocol significantly lowers the length of the approximating
sequence and the number of required resource states (ancillary qubits). In
addition, our protocol is robust to noise in the resource states.Comment: 10 pages, 18 figures, 5 table
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