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QuantumInfo.ResourceTheory.SteinsLemma

7 declarations

definition

Asymptotic optimal hypothesis testing rate R1(ρ,ϵ)R_1(\rho, \epsilon)

Given a mixed state ρMState(H(i))\rho \in \text{MState}(H(i)) and a tolerance probability ϵ[0,1]\epsilon \in [0, 1], the value R1(ρ,ϵ)R_1(\rho, \epsilon) is defined as the limit inferior of the normalized negative logarithm of the optimal hypothesis testing rate as the number of copies nn tends to infinity: R1(ρ,ϵ)=lim infnlogβϵ(ρrnIsFree)n R_1(\rho, \epsilon) = \liminf_{n \to \infty} \frac{-\log \beta_\epsilon(\rho^{\otimes_r n} \| \text{IsFree})}{n} where ρrn\rho^{\otimes_r n} is the nn-th tensor power of the state ρ\rho within the resource theory, and βϵ(ρrnIsFree)\beta_\epsilon(\rho^{\otimes_r n} \| \text{IsFree}) is the optimal Type II error rate for distinguishing ρrn\rho^{\otimes_r n} from the set of free states IsFree\text{IsFree} given a Type I error bound ϵ\epsilon. The result is an extended non-negative real number in [0,][0, \infty].

definition

Asymptotic relative entropy rate R2(ρ,σ)R_2(\rho, \sigma)

Given a mixed state ρMState(H(i))\rho \in \text{MState}(H(i)) and a sequence of free states σ=(σn)nN\sigma = (\sigma_n)_{n \in \mathbb{N}} (where each σn\sigma_n is a free state for the system index ini^n), the value R2(ρ,σ)R_2(\rho, \sigma) is defined as the limit inferior of the normalized quantum relative entropy between the nn-th tensor power of ρ\rho and σn\sigma_n as nn tends to infinity: R2(ρ,σ)=lim infnD(ρrnσn)n R_2(\rho, \sigma) = \liminf_{n \to \infty} \frac{D(\rho^{\otimes_r n} \parallel \sigma_n)}{n} where D()D(\cdot \parallel \cdot) denotes the quantum relative entropy and ρrn\rho^{\otimes_r n} denotes the nn-th power of the state within the resource theory. The result is an extended non-negative real number in [0,][0, \infty].

definition

A full-rank free mixed state σ1\sigma_1 on HiH_i

The definition specifies σ1\sigma_1 as a quantum mixed state on the finite-dimensional Hilbert space HiH_i. It is chosen (using the axiom of choice) to be a state that is both "free" within a specified resource theory and of full rank, based on the property provided by `FreeStateTheory.free_fullRank`.

definition

Minimum eigenvalue of the state σ1\sigma_1

For a mixed state σ1\sigma_1 on the Hilbert space HiH_i, let its associated density operator be represented by a Hermitian matrix. This definition calculates the minimum eigenvalue of this matrix, expressed as the infimum infkλk\inf_k \lambda_k, where λk\lambda_k are the eigenvalues of the density operator corresponding to σ1\sigma_1.

definition

The sequence cn c_n based on the minimum eigenvalue of σ1 \sigma_1

For a natural number n n , the sequence cn c_n is defined as: cn=log(1λmin(σ1))+log3max(n,1) c_n = \log \left( \frac{1}{\lambda_{\min}(\sigma_1)} \right) + \frac{\log 3}{\max(n, 1)} where λmin(σ1) \lambda_{\min}(\sigma_1) is the minimum eigenvalue of the quantum state σ1 \sigma_1 . This definition corresponds to the sequence cn c_n appearing in equation (S44) of Stein's Lemma, modified to handle the n=0 n=0 case by replacing n n with max(n,1) \max(n, 1) .

theorem

Gap Reduction between Asymptotic Relative Entropy and Hypothesis Testing Rates

Let ρMState(H(i))\rho \in \text{MState}(H(i)) be a mixed state and ϵ(0,1)\epsilon \in (0, 1) be a probability. Let σ=(σn)nN\sigma = (\sigma_n)_{n \in \mathbb{N}} be a sequence of free states where each σnIsFree(in)\sigma_n \in \text{IsFree}(i^n). If the asymptotic relative entropy rate R2(ρ,σ)R_2(\rho, \sigma) is greater than or equal to the asymptotic optimal hypothesis testing rate R1(ρ,ϵ)R_1(\rho, \epsilon), then for any probability ϵ(0,ϵ)\epsilon' \in (0, \epsilon), there exists a sequence of free states σ=(σn)nN\sigma' = (\sigma'_n)_{n \in \mathbb{N}} such that R2(ρ,σ)R1(ρ,ϵ)(1ϵ)(R2(ρ,σ)R1(ρ,ϵ)), R_2(\rho, \sigma') - R_1(\rho, \epsilon) \le (1 - \epsilon') (R_2(\rho, \sigma) - R_1(\rho, \epsilon)), where R1(ρ,ϵ)R_1(\rho, \epsilon) is the limit inferior of the normalized negative logarithm of the optimal Type II error rate, and R2(ρ,σ)R_2(\rho, \sigma) is the limit inferior of the normalized quantum relative entropy D(ρnσn)D(\rho^{\otimes n} \| \sigma_n).

definition

Improver for the gap between R2(ρ,σ)R_2(\rho, \sigma) and R1(ρ,ϵ)R_1(\rho, \epsilon)

Let ρMState(H(i))\rho \in \text{MState}(H(i)) be a mixed state and 0<ϵ<ϵ<10 < \epsilon' < \epsilon < 1 be probabilities. Given a sequence of free states σ=(σn)nN\sigma = (\sigma_n)_{n \in \mathbb{N}} where each σnIsFree(in)\sigma_n \in \text{IsFree}(i^n), the improver function returns a new sequence of free states σ=(σn)nN\sigma' = (\sigma'_n)_{n \in \mathbb{N}} defined as: 1. If R2(ρ,σ)R1(ρ,ϵ)R_2(\rho, \sigma) \ge R_1(\rho, \epsilon), then σ\sigma' is the sequence whose existence is guaranteed by Lemma 7, which satisfies the gap reduction inequality: R2(ρ,σ)R1(ρ,ϵ)(1ϵ)(R2(ρ,σ)R1(ρ,ϵ)). R_2(\rho, \sigma') - R_1(\rho, \epsilon) \le (1 - \epsilon') (R_2(\rho, \sigma) - R_1(\rho, \epsilon)). 2. If R2(ρ,σ)<R1(ρ,ϵ)R_2(\rho, \sigma) < R_1(\rho, \epsilon), the function returns the original sequence σ\sigma. Here, R1(ρ,ϵ)R_1(\rho, \epsilon) denotes the asymptotic optimal hypothesis testing rate and R2(ρ,σ)R_2(\rho, \sigma) denotes the asymptotic relative entropy rate.