nLab maximally mixed quantum state

Contents

Context

Quantum systems

quantum logic


quantum physics


quantum probability theory – observables and states


quantum information


quantum technology


quantum computing

Contents

Idea

In quantum information theory, by the maximally mixed state of a quantum systems represented by a finite-dimensional Hilbert space ℋ\mathscr{H} one means the mixed state whose density matrix is a multiple of the identity matrix on ℋ\mathscr{H}.

Hence if (|w⟩) w:W\big(\left\vert w \right\rangle\big)_{w \colon W} is any orthonormal linear basis for ℋ\mathscr{H}, then the maximally mixed state is (in bra-ket notation) given by

1dim(ℋ)∑w|w⟩⟨w|:ℋ⊗ℋ *, \frac{1}{dim(\mathscr{H})} \, \underset{w}{\sum} \left\vert w \right\rangle \left\langle w \right\vert \;\;\colon\;\; \mathscr{H} \otimes \mathscr{H}^\ast \,,

representing the uniform probability distribution on WW.

Properties

Relation to quantum channels

A quantum channel which preserves the maximally mixed state is called a unital quantum channel.

A quantum channel with an environmental representation given by coupling to a maximally mixed state of the environment is called a unistochastic quantum channel or (ambiguously) noisy quantum operation. Such operation on single qbits constitute the “DQC1-model” of quantum computation.

References

See references at unistochastic quantum channel.

Created on September 28, 2023 at 10:44:53. See the history of this page for a list of all contributions to it.