Quantum information inequalities via tracial positive linear maps
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We present some generalizations of quantum information inequalities involving tracial positive linear maps between mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16306230&_mathId=si1.gif&_user=111111111&_pii=S0022247X16306230&_rdoc=1&_issn=0022247X&md5=f9007b104c3add9b55801c7ca7f6e76d" title="Click to view the MathML source">CmathContainer hidden">mathCode"><math altimg="si1.gif" overflow="scroll">Cmath>-algebras. Among several results, we establish a noncommutative Heisenberg uncertainty relation. More precisely, we show that if mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16306230&_mathId=si2.gif&_user=111111111&_pii=S0022247X16306230&_rdoc=1&_issn=0022247X&md5=8a1f7b62f1e129dc47a24a8475ca94a4" title="Click to view the MathML source">Φ:A→BmathContainer hidden">mathCode"><math altimg="si2.gif" overflow="scroll">mathvariant="normal">Φ:mathvariant="script">Amathvariant="script">Bmath> is a tracial positive linear map between mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16306230&_mathId=si1.gif&_user=111111111&_pii=S0022247X16306230&_rdoc=1&_issn=0022247X&md5=f9007b104c3add9b55801c7ca7f6e76d" title="Click to view the MathML source">CmathContainer hidden">mathCode"><math altimg="si1.gif" overflow="scroll">Cmath>-algebras, mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16306230&_mathId=si3.gif&_user=111111111&_pii=S0022247X16306230&_rdoc=1&_issn=0022247X&md5=3b4aee1b2704f8ec04f9dbcb8de633be" title="Click to view the MathML source">ρ∈AmathContainer hidden">mathCode"><math altimg="si3.gif" overflow="scroll">ρmathvariant="script">Amath> is a Φ-density element and mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16306230&_mathId=si4.gif&_user=111111111&_pii=S0022247X16306230&_rdoc=1&_issn=0022247X&md5=dbed8a1072cb05337894b69eb53bc605" title="Click to view the MathML source">A,BmathContainer hidden">mathCode"><math altimg="si4.gif" overflow="scroll">A,Bmath> are self-adjoint operators of mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16306230&_mathId=si5.gif&_user=111111111&_pii=S0022247X16306230&_rdoc=1&_issn=0022247X&md5=1ff0654e956a78c29dce004b7de59916" title="Click to view the MathML source">AmathContainer hidden">mathCode"><math altimg="si5.gif" overflow="scroll">mathvariant="script">Amath> such that mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16306230&_mathId=si6.gif&_user=111111111&_pii=S0022247X16306230&_rdoc=1&_issn=0022247X&md5=25e7c2cb63b6bac84c54935d71534d76">lineImage" height="20" width="185" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0022247X16306230-si6.gif">mathContainer hidden">mathCode"><math altimg="si6.gif" overflow="scroll">mathvariant="normal">sp(-iρ12[A,B]ρ12)[m,M]math> for some scalers mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16306230&_mathId=si131.gif&_user=111111111&_pii=S0022247X16306230&_rdoc=1&_issn=0022247X&md5=050285b7163f300282cd833edf6cda8a" title="Click to view the MathML source">0<m<MmathContainer hidden">mathCode"><math altimg="si131.gif" overflow="scroll">0<m<Mmath>, then under some conditions where mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16306230&_mathId=si142.gif&_user=111111111&_pii=S0022247X16306230&_rdoc=1&_issn=0022247X&md5=fadfd7d5195c31aa50f144cfd5c662ae" title="Click to view the MathML source">Km,M(ρ[A,B])mathContainer hidden">mathCode"><math altimg="si142.gif" overflow="scroll">Km,M(ρ[A,B])math> is the Kantorovich constant of the operator mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16306230&_mathId=si10.gif&_user=111111111&_pii=S0022247X16306230&_rdoc=1&_issn=0022247X&md5=61bcfc5c79430e8681c00e84548eedd4">lineImage" height="20" width="88" alt="View the MathML source" title="View the MathML source" src="/sd/grey_pxl.gif" data-inlimgeid="1-s2.0-S0022247X16306230-si10.gif">mathContainer hidden">mathCode"><math altimg="si10.gif" overflow="scroll">-iρ12[A,B]ρ12math> and mathmlsrc">mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0022247X16306230&_mathId=si11.gif&_user=111111111&_pii=S0022247X16306230&_rdoc=1&_issn=0022247X&md5=0ac858277be6d30b24f2d5a03d40cfbb" title="Click to view the MathML source">Vρ,Φ(X)mathContainer hidden">mathCode"><math altimg="si11.gif" overflow="scroll">Vρ,mathvariant="normal">Φ(X)math> is the generalized variance of X. In addition, we use some arguments differing from the scalar theory to present some inequalities related to the generalized correlation and the generalized Wigner–Yanase–Dyson skew information.

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