Two Kraus representations: How to check if they're the same TPCPM?

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Discussion Overview

The discussion revolves around the methods for determining whether two Kraus representations yield the same trace-preserving completely positive map (TPCPM). Participants explore various approaches to this problem, which is rooted in the theoretical framework of quantum mechanics and operator algebra.

Discussion Character

  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants note that the Kraus representation theorem states a map is a TPCPM if it can be expressed in an operator sum representation, emphasizing that this representation is not unique.
  • One participant suggests that working out the image of a suitable spanning set of matrices could help determine if two representations are the same.
  • Another participant mentions two methods for checking equivalence: one involves the previously mentioned image of a spanning set, while the other requires finding a unitary matrix that relates the operators of the two representations.
  • It is noted that both methods can be time-consuming, leading to a query about potentially more efficient approaches.
  • A further suggestion is made to take the difference of the operators and simplify it to zero using a fixed set of generators, although this is acknowledged as not easy for arbitrary Kraus representations.
  • Some participants indicate that there is often a preferred representation with physical significance, which may alleviate the need to question equivalence.

Areas of Agreement / Disagreement

Participants express differing views on the efficiency and practicality of the methods discussed, with no consensus on a singular best approach to determine the equivalence of Kraus representations.

Contextual Notes

Participants acknowledge that the complexity of the methods may depend on the specific characteristics of the Kraus representations being analyzed, and that the discussion does not resolve the challenges associated with arbitrary representations.

Ameno
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Hi

According to the Kraus representation theorem, a map \mathcal{E}: \text{End}(\mathcal{H}_A) \rightarrow \text{End}(\mathcal{H}_B)
is a trace-preserving completely positive map if and only if it can be written in an operator sum representation \mathcal{E}: \rho \mapsto \sum_k A_k \rho A_k^\dagger with \sum_k A_k^\dagger A_k = \text{Id}
This operator sum representation is not unique. For example, \rho \mapsto (1-p)\rho + p \sigma_x \rho \sigma_x
and \rho \mapsto (1-2p)\rho + 2pP_+\rho P_+ + 2pP_-\rho P_-
where \sigma_x is the Pauli x-operator and P_+, P_- is the projector to the \sigma_z eigenspace with eigenvalue +1, -1,
are two operator-sum representations of the same trace-preserving completely positive map.

My question is: Given two such operator-sum representations, what is the easiest way to find out whether the two representations give the same TPCPM or not?
 
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Ameno said:
According to the Kraus representation theorem, a map
\mathcal{E}: \text{End}(\mathcal{H}_A) \rightarrow \text{End}(\mathcal{H}_B)
is a trace-preserving completely positive map if and only if it can be written in an operator sum representation
\mathcal{E}: \rho \mapsto \sum_k A_k \rho A_k^\dagger
with
\sum_k A_k^\dagger A_k = \text{Id}
This operator sum representation is not unique. [...]

My question is: Given two such operator-sum representations, what is the easiest way to find out whether the two representations give the same TPCPM or not?

Working out the image of a suitable spanning set of matrices, I guess.
 
Well, there are two ways I know how one can do this. One is what you have just written, the other one is to check if there is a unitary matrix s.t.
N_a = U_{\mu a}M_\mu
where the N's and M's are the operators of two operator-sum representations.
I find that both require a lot of time to work out in practice, so I wonder if there is a more efficient way to do that.
 
Ameno said:
Well, there are two ways I know how one can do this. One is what you have just written, the other one is to check if there is a unitary matrix s.t.
N_a = U_{\mu a}M_\mu
where the N's and M's are the operators of two operator-sum representations.
I find that both require a lot of time to work out in practice, so I wonder if there is a more efficient way to do that.

You can also take the difference and simplify it to zero by expressing the operators involved in terms of a fixed set of generators for which you know all algebraic relations.

None of the methods is easy when the Kraus representations are arbitrary. But usually there is a preferred representation with a physical meaning, and when this is used consistentl;y, the question of equivalence doesn't arise.
 

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