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On Universal and Fault-Tolerant Quantum Computing
Quantum Physics · Submitted 16 Jun 1999
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim A novel universal and fault-tolerant basis (set of gates) for quantum computation is described.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
A novel universal and fault-tolerant basis (set of gates) for quantum computation is described. Such a set is necessary to perform quantum computation in a realistic noisy environment. The new basis consists of two single-qubit gates (Hadamard and ${\sigma_z}^{1/4}$), and one double-qubit gate (Controlled-NOT). Since the set consisting of Controlled-NOT and Hadamard gates is not universal, the new basis achieves universality by including only one additional elementary (in the sense that it does not include angles that are irrational multiples of $\pi$) single-qubit gate, and hence, is potentially the simplest universal basis that one can construct. We also provide an alternative proof of universality for the only other known class of universal and fault-tolerant basis proposed by Shor and by Kitaev.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | A novel universal and fault-tolerant basis (set of gates) for quantum computation is described. | contribution 1.00 | 0.92 | 0.76 | asserted 1.00 |
| s1 | Such a set is necessary to perform quantum computation in a realistic noisy environment. | background 0.98 | 0.09 | 0.07 | asserted 1.00 |
| s2 | The new basis consists of two single-qubit gates (Hadamard and ${\sigma_z}^{1/4}$), and one double-qubit gate (Controlled-NOT). | contribution 0.92 | 0.86 | 0.23 | asserted 1.00 |
| s3 | Since the set consisting of Controlled-NOT and Hadamard gates is not universal, the new basis achieves universality by including only one additional elementary (in the sense that it does not include angles that are irrational multiples of $\pi$) single-qubit gate, and hence, is potentially the simplest universal basis that one can construct. | interpretation 0.85 | 0.73 | 0.33 | hedged possibility 0.74 |
| s4 | We also provide an alternative proof of universality for the only other known class of universal and fault-tolerant basis proposed by Shor and by Kitaev. | contribution 0.98 | 0.89 | 0.10 | asserted 1.00 |
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The paper
Original abstract
A novel universal and fault-tolerant basis (set of gates) for quantum computation is described. Such a set is necessary to perform quantum computation in a realistic noisy environment. The new basis consists of two single-qubit gates (Hadamard and ${\sigma_z}^{1/4}$), and one double-qubit gate (Controlled-NOT). Since the set consisting of Controlled-NOT and Hadamard gates is not universal, the new basis achieves universality by including only one additional elementary (in the sense that it does not include angles that are irrational multiples of $\pi$) single-qubit gate, and hence, is potentially the simplest universal basis that one can construct. We also provide an alternative proof of universality for the only other known class of universal and fault-tolerant basis proposed by Shor and by Kitaev.
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References
How the literature uses it
31 arXiv papers cite this in 47 sentences
Papers citing it · 37 sentences without a confident label
Uses its method or tool 2 papers
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The original fault-tolerant construction due to Boykin et al. [ref] can be used verbatim as the logical gadget for the $T$ gate in the trap scheme.
Quantum one-time programs · The $π/8$-phase gate · 0.98
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The techniques used in this section are based on cyclotomic polynomials and they were used in the similar context in [ref] .
Universality of beamsplitters · Introduction · 0.99
Cites it as background 8 papers
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The second level is the Clifford Group [ref] , $𝒞^(2)$, which can be generated using the unitaries Hadamard, Phase, and either of Controlled-NOT (C$X$) or Controlled-$Z$ (C$Z$) defined respectively as [equation] The Clifford group in combination with any unitary from a higher level can be used to approximate any unitary operator arbitrarily well [ref] .
Divisible Codes for Quantum Computation · The Clifford Hierarchy · 0.96
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Various methods of decomposing an arbitrary quantum gate into a sequence of gates drawn from a universal, discrete set are known [ref] , and typically require first decomposing the operation into controlled single-qubit unitaries [ref] , and then decomposing the single-qubit unitaries into a circuit of gates from a universal basis [ref] .
A Depth-Optimal Canonical Form for Single-qubit Quantum Circuits · Introduction · 0.94
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A common minimal choice is ${H,CNOT,T}$ [ref] .
Universal Weakly Fault-Tolerant Quantum Computation via Code Switching in the [[8,3,2]] Code · Introduction · 0.80
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