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Stabilizer projector rank and code dimension
Statement
Let be a stabilizer subgroup on qubits of rank , and let be its fixed-space projector. Then
In particular, if , then is one-dimensional; for arbitrary it is the -dimensional stabilizer code space.
Facts & Assumptions
Given: An -qubit stabilizer subgroup of rank .
Stabilizer average is the fixed-space projector: is an idempotent whose image is .
Stabilizer labels form an isotropic space of the same rank: , and the identity is the unique element with zero binary label.
The Pauli matrices: in the ordered computational basis, and .
Phase aware n qubit pauli group: for , in the fixed tensor order.
Tensor products of finitely many linear maps: tensor products of operators act factorwise on elementary tensor vectors.
Ordered tensor registers, their inner product, and wire permutations: the ordered computational basis is the lexicographically ordered product basis of the tensor factors, and the zero-qubit register is .
Pauli group on the empty register and Stabilizer subgroup: when , the only stabilizer subgroup element is .
The trace as the sum of the diagonal entries and The basis-independent trace of an endomorphism of a finite-dimensional vector space: trace is the finite sum of diagonal coefficients in a basis.
The trace of an idempotent is its rank as a field scalar: for an idempotent on a finite-dimensional complex space, its trace is its image dimension viewed as a scalar.
A maximal stabilizer label space is self-dual: an isotropic stabilizer label space of dimension satisfies .
Finite commutative-monoid sums are invariant under bijective reindexing, split over disjoint unions, and satisfy the finite Fubini rule: a finite sum indexed by a Cartesian product may be evaluated as iterated finite sums.
Proof
Given: The data in the Statement.
By [F1], [F2], and [F10], and . For , the identity is . In the ordered product basis [F5]–[F6], its trace is a sum over bit words; [F11] factors this finite sum into the product of its one-qubit diagonal sums, each equal to . Thus its trace is . When , [F6]–[F8] give trace . For , every other has nonzero binary label by [F2], hence at least one nonidentity tensor factor. By [F4] that factor is a scalar multiple of , , or . For any tensor Pauli, its trace is the sum over bit words of products of one-qubit diagonal coefficients; [F11] factors this finite sum into the product of the one-qubit traces. By [F3], and are off-diagonal, while has diagonal entries , so the nonidentity factor has trace zero. Hence every such has trace zero. Therefore .
As is idempotent, [F9] gives . Combining with step 1.1 proves the dimension formula, including and .
When , step 2.1 gives a one-dimensional common fixed space, so the space is nonzero and all of its nonzero vectors determine the same ray. This is the existence and uniqueness assertion used in the definition of a pure stabilizer state.
Sources
Watrous Lesson 14 §14.3, printed pp. 420–422 (PDF pp. 426–428), expands commuting stabilizer projectors and computes code-space dimension. De Wolf §20.3, PDF pp. 187–188, gives the rank- stabilizer-state and projector calculation. The local proof keeps the binary-label injectivity, finite tensor trace factorization, and trace-zero cases explicit.
Depends on
- Stabilizer subgroup
- Stabilizer labels form an isotropic space of the same rank
- A maximal stabilizer label space is self-dual
- Stabilizer average is the fixed-space projector
- The Pauli matrices
- Phase aware n qubit pauli group
- Tensor products of finitely many linear maps
- Ordered tensor registers, their inner product, and wire permutations
- The trace $\operatorname{tr}(A)$ as the sum of the diagonal entries
- The basis-independent trace of an endomorphism of a finite-dimensional vector space
- The trace of an idempotent is its rank as a field scalar
- Finite commutative-monoid sums are invariant under bijective reindexing, split over disjoint unions, and satisfy the finite Fubini rule
Used by
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Sources
- John Watrous, Understanding Quantum Information and Computation, Lesson 14 §14.3 (standard reference, not scraped)
- Ronald de Wolf, Quantum Computing: Lecture Notes, §20.3 (standard reference, not scraped)