2009
DOI: 10.1016/j.chaos.2008.04.054
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Bell’s inequalities for three-qubit entangled states with white noise

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Cited by 3 publications
(3 citation statements)
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“…In our description of the PBI monomers as qubits, we write their associated observables in terms of the Pauli matrices A i = cos θ i σ z + sin θ i σ x , and B i = cos φ i σ z + sin φ i σ x , i = 1, 2, 3. Other observables in terms of combinations with σ y can also be defined [43]. However, as the states explored in this section have a matrix structure with their anti-diagonal elements identically zero, observables in terms of σ x plus σ y do not exhibit any violation.…”
Section: B Pbi Trimer Nonlocal Statesmentioning
confidence: 99%
“…In our description of the PBI monomers as qubits, we write their associated observables in terms of the Pauli matrices A i = cos θ i σ z + sin θ i σ x , and B i = cos φ i σ z + sin φ i σ x , i = 1, 2, 3. Other observables in terms of combinations with σ y can also be defined [43]. However, as the states explored in this section have a matrix structure with their anti-diagonal elements identically zero, observables in terms of σ x plus σ y do not exhibit any violation.…”
Section: B Pbi Trimer Nonlocal Statesmentioning
confidence: 99%
“…One of the well-know Bell type expressions for tripartite systems is Mermin inequality, which can be expressed as [9]:…”
Section: A New Bell Expressionmentioning
confidence: 99%
“…shows that quantum theory is non-local. Here, the violation factor and amount of violation in Mermin inequality are both 2 and the maximum white noise tolerance calculated is 0.5 [9]. Now let's consider the following inequality for a tripartite system…”
Section: A New Bell Expressionmentioning
confidence: 99%