A Derivation of recovery channel for bit flip error

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The discussion focuses on deriving the recovery channel for a bit flip error channel, specifically how to reach the final result from the initial definitions. The recovery channel R is expressed in terms of operators A_i and B_j, which are identified as the bit flip operator σ_x. By substituting these operators into the recovery channel equation, the derivation simplifies to a sum over the combined effects of the bit flip operations. Ultimately, the final result shows that the recovery channel can be expressed as a sum involving the bit flip operator applied to the state ρ. This derivation clarifies the relationship between the recovery channel and the bit flip error channel.
steve1763
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I have found a derivation of the recovery channel for a bit flip error (using the derivation of the Knill-Laflamme condition), but dont quite understand it.
In general, if R is the recovery channel of an error channel ε, with state ρ, then
Screenshot 2021-07-27 at 15.18.43.png

and according to these lecture slides, we get the final result highlighted in red for a bit flip error channel. I am simply asking how one reaches this final result. Thank you (a full-ish derivation can be found at https://orion.math.iastate.edu/ytpoon/publication/qecc1.pdf on pages 6-7, but for some reason i still don't understand how one gets to the final answer).

Screenshot 2021-07-27 at 15.20.15.png
 
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To get the final result, we start by applying the definition of recovery channel:\begin{align}R(\rho) &= \sum_i A_i \rho A_i^\dagger \\&= \sum_i A_i \rho A_i^\dagger \sum_j B_j \rho B_j^\dagger \\&= \sum_{i,j} A_i \rho A_i^\dagger B_j \rho B_j^\dagger\end{align}Now, for a bit flip error channel, we have $A_i = \sigma_x^i$ and $B_j = \sigma_x^j$. Substituting these values into the equation above gives us\begin{align}R(\rho) &= \sum_{i,j} \sigma_x^i \rho \sigma_x^{i\dagger} \sigma_x^j \rho \sigma_x^{j\dagger} \\&= \sum_{i,j} \sigma_x^i \rho \sigma_x^i \sigma_x^j \rho \sigma_x^j \\&= \sum_{i,j} \sigma_x^{i+j} \rho \sigma_x^{i+j} \\&= \sum_k \sigma_x^k \rho \sigma_x^k\end{align}where $k = i + j$. This is the final result.
 
For the quantum state ##|l,m\rangle= |2,0\rangle## the z-component of angular momentum is zero and ##|L^2|=6 \hbar^2##. According to uncertainty it is impossible to determine the values of ##L_x, L_y, L_z## simultaneously. However, we know that ##L_x## and ## L_y##, like ##L_z##, get the values ##(-2,-1,0,1,2) \hbar##. In other words, for the state ##|2,0\rangle## we have ##\vec{L}=(L_x, L_y,0)## with ##L_x## and ## L_y## one of the values ##(-2,-1,0,1,2) \hbar##. But none of these...

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