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Every nonzero finite-dimensional complex inner-product space admits a density operator
Statement
Every nonzero finite-dimensional complex inner-product space admits a density operator; specifically, if , then is a density operator on .
Facts & Assumptions
Given: A nonzero finite-dimensional complex inner-product space , , and the identity endomorphism .
Density operator: on nonzero finite-dimensional , a density operator is a non-negative endomorphism with trace one.
Non-negative and positive operators: non-negative means self-adjoint and having nonnegative quadratic form on every vector.
Real and complex inner-product spaces and their induced length: the inner product is linear in its first argument and positive definite.
The basis-independent trace of an endomorphism of a finite-dimensional vector space: trace of an endomorphism is the matrix trace in any ordered basis.
The trace as the sum of the diagonal entries: matrix trace is the sum of diagonal entries.
Trace is a linear functional on : matrix trace is linear under scalar multiplication and addition.
Finite-dimensional vector space, and its dimension ; infinite-dimensional means having no finite basis: is the finite size of a basis of ; since , .
Proof
Put . The scalar is positive real. The identity is self-adjoint, and for every , by [F3] and [F7]. Thus is non-negative by [F2].
In a basis of with elements, the matrix of is . By [F4]–[F6], its trace is . Therefore is a density operator by [F1].
Depends on
- Density operator
- The basis-independent trace of an endomorphism of a finite-dimensional vector space
- The trace $\operatorname{tr}(A)$ as the sum of the diagonal entries
- Trace is a linear functional on $M_n(F)$
- Finite-dimensional vector space, and its dimension $\dim_F V$; infinite-dimensional means having no finite basis
- Real and complex inner-product spaces and their induced length
- Non-negative and positive operators
Used by
- Bell-state Schmidt decomposition and reduced density Example
- Finite ensemble barycenters are density operators Theorem
Cited to discharge well-definedness by Density operator.
Dependency tree · two levels
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Sources
- John Watrous, The Theory of Quantum Information, §2.1.2 (standard reference, not scraped)
- John Preskill, Quantum Computation, Chapter 2: Foundations I: States and Ensembles (standard reference, not scraped)
- Ronald de Wolf, Quantum Computing: Lecture Notes, §15.1 (standard reference, not scraped)