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Volumn 77, Issue 4, 2008, Pages

Improved bounds on entropic uncertainty relations

Author keywords

[No Author keywords available]

Indexed keywords

HILBERT SPACES; SYSTEMS ANALYSIS;

EID: 42349096443     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.77.042110     Document Type: Article
Times cited : (81)

References (33)
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    • Notice that the concavity of the entropy functional implies that any inequality of the form 2, while stated only for pure states, remains also valid for general (mixed) states. In what follows, for the sake of brevity, we do not write explicitly the dependence of probability distributions and entropies upon the quantum state of the system.
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    • If only PA =1/ MA, then μB = νB =0 and Eqs. 20 21 22 23 hold like in the previous cases. The analog of Eq. 16 for i=A now imposes that MA =1,2 in order to have non-negativity of the Lagrange multipliers. The solution for MA =1 gives Eq. 30, which is thus proven to be valid in principle for all values of c, while the solution for MA =2 can only hold when c≤1/2. If Pi =1/ Mi for both A and B, a similar reasoning yields Mi =1,2 for i=A,B, and the resulting bounds are clearly nonoptimal.
    • If only PA =1/ MA, then μB = νB =0 and Eqs. 20 21 22 23 hold like in the previous cases. The analog of Eq. 16 for i=A now imposes that MA =1,2 in order to have non-negativity of the Lagrange multipliers. The solution for MA =1 gives Eq. 30, which is thus proven to be valid in principle for all values of c, while the solution for MA =2 can only hold when c≤1/2. If Pi =1/ Mi for both A and B, a similar reasoning yields Mi =1,2 for i=A,B, and the resulting bounds are clearly nonoptimal.


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