Table of Contents
Fetching ...

Fidelity preserving and decoherence for mixed unitary quantum channels

Kai Liu, Deguang Han

Abstract

Distinguishable and non-distinguishable quantum states are fundamental resources in quantum mechanics and quantum technologies. Interactions with the environment often induce decoherence, impacting both the distinguishability and non-distinguishability between quantum states. In this paper, we investigate mixed unitary quantum channels and the conditions under which fidelity, a measure of quantum state closeness, is preserved. More precisely, for quantum channels in the form $Φ(ρ) = \sum_{i=1}^N p_i U_i ρU_i^*$, we analyze their effect on quantum state $|\varphi\rangle$ through the associated purification $|Ψ\rangle$, explore the structure of such quantum channels that preserve either distinguishable or non-distinguishable states and then discuss the challenges of maintaining fidelity, particularly under the influence of phase damping.

Fidelity preserving and decoherence for mixed unitary quantum channels

Abstract

Distinguishable and non-distinguishable quantum states are fundamental resources in quantum mechanics and quantum technologies. Interactions with the environment often induce decoherence, impacting both the distinguishability and non-distinguishability between quantum states. In this paper, we investigate mixed unitary quantum channels and the conditions under which fidelity, a measure of quantum state closeness, is preserved. More precisely, for quantum channels in the form , we analyze their effect on quantum state through the associated purification , explore the structure of such quantum channels that preserve either distinguishable or non-distinguishable states and then discuss the challenges of maintaining fidelity, particularly under the influence of phase damping.

Paper Structure

This paper contains 15 sections, 20 theorems, 91 equations, 5 figures.

Key Result

Theorem 1

gupta2015 Suppose that $\Phi: B(H)\rightarrow B(K)$ is a quantum channel with Kraus representation $\Phi(\rho) = \sum_{j=1}^{r}A_{j}\rho A_{j}^{*}$ for some $A_{j}\in B(H,K)$, $1\leq j\leq r$. Then $\Phi(\rho) = \sum_{j=1}^{m}B_{j}\rho B_{j}^{*}$ for operators $B_{j}\in B(H,K)$, $1\leq j\leq m$ if a

Figures (5)

  • Figure 4.1: Coherence decay for Phase damping channel
  • Figure 4.2: Coherence decay under a rank 2 general phase damping error with relative phase $\theta$ and mix parameter p
  • Figure 4.3:
  • Figure 4.4:
  • Figure 4.5: Quantum circuit for general phase damping.

Theorems & Definitions (32)

  • Theorem 1
  • Theorem 2
  • Lemma 3
  • Lemma 4
  • Theorem 5
  • proof
  • Remark 1
  • Remark 2
  • Lemma 6
  • Proposition 7
  • ...and 22 more