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Generators And Relations for Some Classes of Quantum Circuits

Xiaoning Bian

Published Aug 24, 2023• 0 citations
OpenAlex

Abstract

We give three finite presentations in terms of generators and relations for three groups of operators. The operators are frequently used in quantum computation. The result can potentially be used to optimize quantum circuits. Two of the three proofs use the Reidemeister-Schreier theorem. Both the Reidemeister-Schreier theorem and the two proofs using it have been formally verified in the proof assistant Agda. First, we give a finite presentation of the group of 2-qubit Clifford+T operators. The proof applies the Reidemeister-Schreier theorem to a finite presentation of a supergroup of the 2-qubit Clifford+T group that was given by Greylyn. The process generates hundreds of relations. We then simplify them to 20 relations using a Pauli rotation representation as an almost-normal form. Second, we give a finite presentation of U_n (Z[1/2, i]), the group of unitary n × n- matrices with entries in Z[1/2, i]. Amy, Glaudell, and Ross showed that this group is generated by a certain set of two-level matrices, and they also gave an exact synthesis algorithm that converts any element of U_n (Z[1/2, i]) to a word in these generators. We say that a word is in normal form if it is an output of the exact synthesis algorithm. Using what we call semantically guided rewriting, we show that each word in the two-level generators is equivalent to a normal form under the congruence generated by finitely many relations. Third, we give a finite presentation of the group of 3-qubit Clifford+CS operators. Amy, Glaudell, and Ross proved that up to a condition on the determinant, the n-qubit Clifford+CS group is exactly U_(2^n) (Z[1/2, i]). In particular, the 3-qubit Clifford+CS group is a subgroup of U_8 (Z[1/2, i]) of index 2. Using a similar technique as in our first result, we repeatedly apply the Reidemeister-Schreier theorem to the presentation of U_8 (Z[1/2, i]) (from our second result), and then simplify thousands of relations into 17 relations. To do the simplification, we devise an almost-normal form for Clifford+CS operators. We also show that the 3-qubit Clifford+CS group, which is of course infinite, is the amalgamated product of three finite subgroups.

Related papers

Generators and Relations for 3-Qubit Clifford+CS Operators

Xiaoning Bian, Peter Selinger

We give a presentation by generators and relations of the group of 3-qubit Clifford+CS operators. The proof roughly consists of two parts: (1) applying the Reidemeister-Schreier theorem recursively to an earlier result of ours; and (2) the simplification of thousands of relations into 17 relations. Both (1) and (2) have been formally verified in the proof assistant Agda. The Reidemeister-Schreier theorem gives a constructive method for computing a presentation of a sub-monoid given a presentation of the super-monoid. To achieve (2), we devise an almost-normal form for Clifford+CS operators. Along the way, we also identify several interesting structures within the Clifford+CS group. Specifically, we identify three different finite subgroups for whose elements we can give unique normal forms. We show that the 3-qubit Clifford+CS group, which is of course infinite, is the amalgamated product of these three finite subgroups. This result is analogous to the fact that the 1-qubit Clifford+T group is an amalgamated product of two finite subgroups.

arXiv:2306.08530•Electronic Proceedings in Theoretical Computer Science•Aug 23, 2023•2 citations

Generators and Relations for 2-Qubit Clifford+T Operators

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We give a presentation by generators and relations of the group of Clifford+T operators on two qubits. The proof relies on an application of the Reidemeister-Schreier theorem to an earlier result of Greylyn, and has been formally verified in the proof assistant Agda.

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Generators and relations for $U_n(\mathbb Z [\frac{1}{2}, i])$

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Generators and Relations for Real Stabilizers

Justin J. Makary

Real stabilizer operators, which are also known as real Clifford operators, are generated, through composition and tensor product, by the Hadamard gate, the Pauli Z gate, and the controlled-Z gate. We introduce a normal form for real stabilizer circuits and show that every real stabilizer operator admits a unique normal form. Moreover, we give a finite set of relations that suffice to rewrite any Clifford circuit to its normal form. This yields a presentation by generators and relations of the strict spatial monoidal category of real stabilizer operators.

•Aug 20, 2020•0 citations
We give three finite presentations in terms of generators and relations for three groups of operators. The operators are frequently used in quantum computation. The result can potentially be used to optimize quantum circuits. Two of the three proofs use the Reidemeister-Schreier theorem. Both the Reidemeister-Schreier theorem and the two proofs using it have been formally verified in the proof assistant Agda. First, we give a finite presentation of the group of 2-qubit Clifford+T operators. The proof applies the Reidemeister-Schreier theorem to a finite presentation of a supergroup of the 2-qubit Clifford+T group that was given by Greylyn. The process generates hundreds of relations. We then simplify them to 20 relations using a Pauli rotation representation as an almost-normal form. Second, we give a finite presentation of U_n (Z[1/2, i]), the group of unitary n × n- matrices with entries in Z[1/2, i]. Amy, Glaudell, and Ross showed that this group is generated by a certain set of two-level matrices, and they also gave an exact synthesis algorithm that converts any element of U_n (Z[1/2, i]) to a word in these generators. We say that a word is in normal form if it is an output of the exact synthesis algorithm. Using what we call semantically guided rewriting, we show that each word in the two-level generators is equivalent to a normal form under the congruence generated by finitely many relations. Third, we give a finite presentation of the group of 3-qubit Clifford+CS operators. Amy, Glaudell, and Ross proved that up to a condition on the determinant, the n-qubit Clifford+CS group is exactly U_(2^n) (Z[1/2, i]). In particular, the 3-qubit Clifford+CS group is a subgroup of U_8 (Z[1/2, i]) of index 2. Using a similar technique as in our first result, we repeatedly apply the Reidemeister-Schreier theorem to the presentation of U_8 (Z[1/2, i]) (from our second result), and then simplify thousands of relations into 17 relations. To do the simplification, we devise an almost-normal form for Clifford+CS operators. We also show that the 3-qubit Clifford+CS group, which is of course infinite, is the amalgamated product of three finite subgroups.
We give a presentation by generators and relations of the group of 3-qubit Clifford+CS operators. The proof roughly consists of two parts: (1) applying the Reidemeister-Schreier theorem recursively to an earlier result of ours; and (2) the simplification of thousands of relations into 17 relations. Both (1) and (2) have been formally verified in the proof assistant Agda. The Reidemeister-Schreier theorem gives a constructive method for computing a presentation of a sub-monoid given a presentation of the super-monoid. To achieve (2), we devise an almost-normal form for Clifford+CS operators. Along the way, we also identify several interesting structures within the Clifford+CS group. Specifically, we identify three different finite subgroups for whose elements we can give unique normal forms. We show that the 3-qubit Clifford+CS group, which is of course infinite, is the amalgamated product of these three finite subgroups. This result is analogous to the fact that the 1-qubit Clifford+T group is an amalgamated product of two finite subgroups.
Consider the universal gate set for quantum computing consisting of the gates X, CX, CCX, omega^dagger H, and S. All of these gates have matrix entries in the ring Z[1/2,i], the smallest subring of the complex numbers containing 1/2 and i. Amy, Glaudell, and Ross proved the converse, i.e., any unitary matrix with entries in Z[1/2,i] can be realized by a quantum circuit over the above gate set using at most one ancilla. In this paper, we give a finite presentation by generators and relations of U_n(Z[1/2,i]), the group of unitary nxn-matrices with entries in Z[1/2,i].
Generators and relations for Un(Z[12,i])U_n(\mathbb Z [\frac{1}{2}, i])Un​(Z[21​,i])
Consider the universal gate set for quantum computing consisting of the gates X, CX, CCX, ω†H{\omega}{\dagger}Hω†H and S. All of these gates have matrix entries in the ring Z[12,i]\mathbb Z [\frac{1}{2}, i]Z[21​,i], the smallest subring of the complex numbers containing 12\frac{1}{2}21​ and iii. Amy, Glaudell, and Ross proved the converse, i.e., any unitary matrix with entries in Z[12,i]\mathbb Z [\frac{1}{2}, i]Z[21​,i] can be realized by a quantum circuit over the above gate set using at most one ancilla. In this paper, we give a finite presentation by generators and relations of Un(Z[12,i])U_n(\mathbb Z [\frac{1}{2}, i])Un​(Z[21​,i]), the group of unitary n×nn\times nn×n-matrices with entries in Z[12,i]\mathbb Z [\frac{1}{2}, i]Z[21​,i].
Real stabilizer operators, which are also known as real Clifford operators, are generated, through composition and tensor product, by the Hadamard gate, the Pauli Z gate, and the controlled-Z gate. We introduce a normal form for real stabilizer circuits and show that every real stabilizer operator admits a unique normal form. Moreover, we give a finite set of relations that suffice to rewrite any Clifford circuit to its normal form. This yields a presentation by generators and relations of the strict spatial monoidal category of real stabilizer operators.