What are CP maps in QM good for?

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SUMMARY

Completely Positive (CP) maps are essential in quantum mechanics for mapping density operators between Hilbert spaces. A bounded operator A is considered positive if it satisfies the condition \(\langle x|A|x\rangle \geq 0\) for all vectors |x⟩ in the Hilbert space H. An operator E is classified as completely positive if the tensor product \(I_n \otimes E\) remains a positive operator for all \(n \geq 0\). Understanding CP maps is crucial for identifying entanglement witnesses, as some positive operators are not completely positive.

PREREQUISITES
  • Understanding of Hilbert spaces in quantum mechanics
  • Familiarity with bounded operators and their properties
  • Knowledge of density operators and their significance in quantum states
  • Basic concepts of entanglement in quantum systems
NEXT STEPS
  • Study the properties of Completely Positive maps in quantum mechanics
  • Read "Quantum Computation and Quantum Information" by Nielsen and Chuang
  • Explore the role of entanglement witnesses in quantum information theory
  • Investigate the mathematical framework of positive operators and their applications
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Students and researchers in quantum mechanics, quantum information theorists, and anyone interested in the mathematical foundations of quantum states and operations.

mtak0114
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Hi
I am trying to teach myself quantum mechanics and I have heard a lot about Completely Positive maps but I haven't been able to find anything on them could someone please tell me what they are and what they are good fore?

cheers

Mark
 
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From linear algebra point of view, a bounded operator [tex]A[/tex] acting on a Hilbert space [tex]H[/tex] is said to be positive (P), if for all [tex]|x\rangle\in H[/tex], [tex]\langle x|A|x\rangle\geq0[/tex].
An operator [tex]E[/tex] which maps density operators of a space [tex]H_1[/tex] to [tex]H_2[/tex] is called completely positive (CP). (Now you understand why they are impotent).
Equivalently, [tex]E[/tex] is completely positive, if and only if [tex]I_n\otimes E[/tex] is a positive operator for all [tex]n\geq0[/tex]. [tex]I_n[/tex] is the identity operator. Testing an operator is CP or not is a difficult problem. The operators which are P but not CP can be used as entanglement witnesses.

For more details read Nielsen and Chuang.
 

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