Abstract
We show an equivalence relation between different types of continuity of the generalized discord function (GDF) that leads to the continuity of the generalized quantum discord (GQD) in the finite-dimensional case. We extend the definition of the GQD to the case where the GDF is optimized over the set of all states with zero quantum discord and prove its continuity by showing that this set is topologically compact. However, for an unmeasured subsystem with infinite dimension, we find that this set is no longer compact while the set of locally measured states is shown to maintain this property in the space of Hilbert-Schmidt (HS) operators. This allows us to prove the continuity of the GQD when the GDF is jointly continuous in the infinite case. As an application, we obtain that the geometric discord is continuous (HS topology) and has the zero set given by the zero quantum discord set in the infinite-dimensional case as a consequence of our previous results.
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Einstein, A., Podolsky, B., Rosen, N.: Can quantum-mechanical description of physical reality be considered complete? Phys. Rev. 47, 777 (1935)
Schrödinger, E.: Discussion of probability relations between separated systems. Math. Proc. Camb. Philosophi. Soc. 31(4), 555 (1935)
Bell, J.S.: On the einstein podolsky rosen paradox. Physics 1(3), 195 (1964)
Bennett, C.H., Brassard, G.: Quantum cryptography: Public key distribution and coin tossing. In: Proceedings of IEEE International Conference on Computers, Systems and Signal Processing (1984)
Feynman, R.P.: Simulating physics with computers. Int. J. Theor. Phys. 21, 467 (1982)
Deutsch, D.: Quantum theory, the church-turing principle and the universal quantum computer. Proc. R. Soc. A 400, 97 (1985)
Bennett, C.H., Brassard, G., Crépeau, C., Jozsa, R., Peres, A., Wootters, W.K.: Teleporting an unknown quantum state via dual classical and einstein-podolsky-rosen channels. Phys. Rev. Lett. 70, 1895 (1993)
Bennett, C.H., Wiesner, S.J.: Communication via one- and two-particle operators on einstein-podolsky-rosen states. Phys. Rev. Lett. 69, 2881 (1992)
Ekert, A.K.: Quantum cryptography based on bell’s theorem. Phys. Rev. Lett. 67, 661 (1991)
Ollivier, H., Zurek, W.H.: Quantum discord: a measure of the quantumness of correlations. Phys. Rev. Lett. 88, 017901 (2001)
Henderson, L., Vedral, V.: Classical, quantum and total correlations. J. Phys. A 34, 6899 (2001)
Shor, P.W.: Algorithms for quantum computation: discrete logarithms and factoring. In: Proceedings 35th Annual Symposium on Foundations of Computer Science, IEEE Computer Society Press (1994)
Grover, L.K.: A fast quantum mechanical algorithm for database search. In: Proceedings, 28th Annual ACM Symposium on the Theory of Computing, p. 212 (1996)
Knill, E., Laflamme, R.: Power of one bit of quantum information. Phys. Rev. Lett. 81, 5672 (1998)
Datta, A., Shaji, A., Caves, C.M.: Quantum discord and the power of one qubit. Phys. Rev. Lett. 100, 050502 (2008)
Streltsov, A., Kampermann, H., Bruß, D.: Quantum cost for sending entanglement. Phys. Rev. Lett. 108, 250501 (2012)
Dakić, B., et al.: Quantum discord as resource for remote state preparation. Nature Phys. 8, 666 (2012)
Horodecki, P., Tuziemski, J., Mazurek, P., Horodecki, R.: Can communication power of separable correlations exceed that of entanglement resource? Phys. Rev. Lett. 112, 140507 (2014)
Madhok, V., Datta, A.: Interpreting quantum discord through quantum state merging. Phys. Rev. A 83, 032323 (2011)
Modi, K., Brodutch, A., Cable, H., Paterek, T., Vedral, V.: The classical-quantum boundary for correlations: Discord and related measures. Reviews of Modern Physics 84, 1655 (2012)
Donald, M.J., Horodecki, M.: Continuity of relative entropy of entanglement. Phys. Lett. A 264, 257 (1999)
Christandl, M., Winter, A.: Squashed entanglement: an additive entanglement measure. J. Math. Phys. 45, 829 (2004)
Alicki, R., Fannes, M.: Continuity of quantum conditional information. J. Phys. A Math. General 37, L55 (2004)
Guo, Y.: Any entanglement of assistance is polygamous. Quantum Inf. Process. 17, 222 (2018)
Guo, Y., Hou, J., Wang, Y.: Concurrence for infinite-dimensional quantum systems. Quantum Inf. Process. 12, 2641 (2013)
Brodutch, A., Modi, K.: Criteria for measures of quantum correlations. Quantum Inf. Comput. 12, 721 (2012)
Dakić, B., Vedral, V., Brukner, Č.: Necessary and sufficient condition for nonzero quantum discord. Phys. Rev. Lett. 105, 190502 (2010)
Rossignoli, R., Canosa, N., Ciliberti, L.: Generalized entropic measures of quantum correlations. Phys. Rev. A 82, 052342 (2010)
Datta, A.: Quantum discord between relatively accelerated observers. Phys. Rev. A 80, 052304 (2009)
Brown, E.G., Cormier, K., Martin-Martinez, E., Mann, R.B.: Vanishing geometric discord in noninertial frames. Phys. Rev. A 86, 032108 (2012)
Tian, Z., Jing, J.: Measurement-induced-nonlocality via the unruh effect. Ann. Phys. 333, 76 (2013)
Ferraro, A., Aolita, L., Cavalcanti, D., Cucchietti, F.M., Acín, A.: Almost all quantum states have nonclassical correlations. Phys. Rev. A 81, 052318 (2010)
Guo, Y., Hou, J.: A class of separable quantum states. J. Phys. A Math. Theor. 45, 505303 (2012)
Bera, A., Das, T., Sadhukhan, D., Roy, S.S., De Sen, A., Sen, U.: Quantum discord and its allies: a review of recent progress. Rep. Progr. Phys. 81, 024001 (2018)
Zhou, T., Cui, J., Long, G.L.: Measure of nonclassical correlation in coherence-vector representation. Phys. Rev. A 84, 062105 (2011)
Carrijo, T.M., Avelar, A.T.: Weak quantum correlation quantifiers with generalized entropies. Quantum Inf. Process. 18, 308 (2019)
Guo, Z., Cao, H., Chen, Z.: Distinguishing classical correlations from quantum correlations. J. Phys. A Math. Theor. 45, 145301 (2012)
Luo, S.: Using measurement-induced disturbance to characterize correlations as classical or quantum. Phys. Rev. A 77, 022301 (2008)
Guo, J.-L., Lin-Wang, G.-L. Long: Measurement-induced disturbance and thermal negativity in 1d optical lattice chain. Ann. Phys. 330, 192 (2013)
Luo, S., Fu, S.: Measurement-induced nonlocality. Phys. Rev. Lett. 106, 120401 (2011)
Guo, Y., Li, X., Li, B., Fan, H.: Quantum correlation induced by the average distance between the reduced states. Int. J. Theor. Phys. 54, 2022 (2015)
Maziero, J., Celeri, L.C., Serra, R.M.: Symmetry aspects of quantum discord. arXiv:1004.2082 [quant-ph] (2010)
Feng-Jian, J., Hai-Jiang, L., Xin-Hu, Y., Ming-Jun, S.: A symmetric geometric measure and the dynamics of quantum discord. Chin. Phys. B 22, 040303 (2013)
Singh, U., Pati, A.K.: Quantum discord with weak measurements. Ann. Phys. 343, 141 (2014)
Rulli, C.C., Sarandy, M.S.: Global quantum discord in multipartite systems. Phys. Rev. A 84, 042109 (2011)
Dieguez, P.R., Angelo, R.M.: Weak quantum discord. Quantum Inf. Process. 17, 194 (2018)
Luo, S., Fu, S.: Geometric measure of quantum discord. Phys. Rev. A 82, 034302 (2010)
Acknowledgements
We thank the Brazillian agencies CNPq (GRANT PQ#312723/2018-0, INCT-IQ #465469/2014-0), FAPEG (GRANT PRONEX #201710267000503, PRONEN #201710267000540), CAPES(PROCAD2013) for partial support and CAPES/FAPEG(GRANT DOCFIX #201810267001518) for the fellowship of T. M. Carrijo.
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Appendices
Appendix
Lemma 1
Let \(C\subset \mathbb {R}^{p}\) be a compact convex set. The function \(F:C\rightarrow \mathbb {R}\) is continuous if, and only if, there exists a continuous function \(g:[0,1]\rightarrow \mathbb {R}\), with \(g(0)=0\), such that \(|F(x)-F((1-r)x+ry)|\le g(r)\) for all \(x,y\in C\) with \(r\in [0,1]\).
Proof
First, we suppose that F is continuous. Let \(g:[0,1]\rightarrow \mathbb {R}\) be defined as \(g(r)\equiv \sup _{(x,y)\in C\times C}|F(x)-F((1-r)x+ry)|\). Set \(H(x,y,r)\equiv x\), \(J(x,y,r)\equiv (1-r)x+ry\) and \(G(x,y,r)=|F\circ H(x,y,r)-F\circ J(x,y,r)|\). Then \(G=|.|\circ (F\circ H-F\circ J)\). Using, as a metric on \(C\times C\times [0,1]\), the function \(d((x,y,r),(x',y',r'))\equiv \Vert x-x'\Vert +\Vert y-y'\Vert +|r-r'|\), it is easy to see that H and J are continuous, implying that G is continuous on \(C\times C\times [0,1]\). The set \(C\times C\) is compact in the product topology induced by the metric \(d((x,y),(x',y'))\equiv \Vert x-x'\Vert +\Vert y-y'\Vert \). Then \(g(r)=\sup _{(x,y)\in C\times C}G(x,y,r)\) is a continuous function. Thus for all \(x,y\in C\) and \(r\in [0,1]\),
Now, suppose that Eq. (23) is valid with a continuous function \(g:[0,1]\rightarrow \mathbb {R}\) such that \(g(0)=0\). First, we prove the continuity of F on the relative interior of C, relint(C), and then prove the continuity on the relative boundary of C: relbd(C). Here, we define a metric on \({{\,\mathrm{Aff}\,}}(C)\subseteq \mathbb {R}^{n}\) by the function \(d(x,y)\equiv \Vert x-y\Vert \), where \(\Vert \cdot \Vert \) is the norm on \(\mathbb {R}^{n}\). As the relative interior of any nonempty convex set is nonempty, \(\exists x\in \) relint(C). Then, \(\exists \delta '>0\) such that \(B_{\delta '}(x)\subseteq C\), where \(B_{\delta '}(x)\equiv \{w\in {{\,\mathrm{Aff}\,}}(C):\Vert w-x\Vert <\delta '\}\). As g is continuous and \(g(0)=0\), for any \(\epsilon >0\), there is \(r\in (0,1)\) such that \(g(r)<\epsilon \). Defining \(\delta \equiv r\delta '<\delta '\), for any \(y\in B_{\delta }(x)\in C\) we have \(z\equiv (1-r^{-1})x+r^{-1}y\in {{\,\mathrm{Aff}\,}}(C)\) and \(\Vert z-x\Vert =r^{-1}\Vert x-y\Vert <\delta '\), implying that \(z\in B_{\delta '}(x)\). This means that for any \(y\in B_{\delta }(x)\), we can find \(z\in C\) such that \(y=(1-r)x+rz\). By the continuity of g and \(g(0)=0\), for any \(\epsilon >0\) there is \(r\in (0,1)\) such that \(g(r)<\epsilon \). If \(x\in \) relint(C), by the previous considerations, there is \(\delta >0\) such that \(B_{\delta }(x)\subset C\) and for any \(y\in B_{\delta }(x)\) we can find \(z\in C\) where \(y=(1-r)x+rz\). Then,
Thus F is continuous on \({{\,\mathrm{relint}\,}}(C)\). Now, we prove the continuity of F on relbd(C). For any \(\epsilon \in (0,1)\) (we can put an upper bound on \(\epsilon \) w.l.o.g), there exists \(0<r<\epsilon /3\) such that \(g(r)<\epsilon /3\). With such r, for any \(x\in \) relbd(C), we can choose an arbitrary \(z\in \) relint(C) and define \(z_{x}\equiv (1-r)x+rz\in \) intrel(C). As F is continuous on \({{\,\mathrm{relint}\,}}(C)\),
For any \(y\in B_{\delta ''}(x)\cap C\) and defining \(z_{y}\equiv (1-r)y+rz\in C\), we have
Using Proposition (26),
Then
which proves that F is continuous on \({{\,\mathrm{relbd}\,}}(C)\cup {{\,\mathrm{relint}\,}}(C)=C\).\(\square \)
Appendix
Lemma 2
The set \(\mathcal {P}^{B}\subset H^{\oplus n}\) is compact.
Proof
Let’s define the set \(\tilde{\mathcal {P}}^{B}\). The operator \(\tilde{X}^{B}\in H_{B}^{\oplus n}\), where \(H_{B}\) is the space of hermitian operators on \(\mathcal {H}_{B}\), is an element of \(\tilde{\mathcal {P}}^{B}\) if, and only if, Eq. (29) is satisfied for any k, l:
where \(\tilde{\Pi _{k}}\) projects \(\tilde{X}^{B}=\bigoplus _{l}\tilde{X}^{B}_{l}\) on its kth component \(\tilde{\Pi _{k}}(\tilde{X}^{B})\equiv \tilde{X}^{B}_{k}\). Eq. (29) implies that the elements of \(\tilde{\mathcal {P}}^{B}\) have the form \(\tilde{P}^{B}=\bigoplus _{l} \tilde{P}^{B}_{l}\) such that \(\{\tilde{P}^{B}_{l}:l\in \{1,\ldots ,n\}\}\) is a set of rank one orthogonal projections with \(\sum _{k}\tilde{P}^{B}_{l}=\mathbb {1}^{B}\). As \(\Vert \tilde{P}^{B}_{l}\Vert _{2}=1\), we have \(\Vert \tilde{P}^{B}\Vert =\sum _{l}\Vert \tilde{P}^{B}_{l}\Vert _{2}=n\), implying that \(\tilde{\mathcal {P}}^{B}\) is a bounded set. Suppose \((\tilde{P}^{B,m})_{m\in \mathbb {N}}\) is a convergent sequence in \(H_{B}^{\oplus n}\) such that \(\tilde{P}^{B,m}\in \tilde{\mathcal {P}}^{B}\) for any m. If \(\lim _{m\rightarrow \infty }\tilde{P}^{B,m}=\tilde{X}^{B}\), by the continuity of the functions \(F_{k}\), \(G_{k,l}\) and J, we have \(F_{k}(\tilde{X}^{B})=0\), \(G_{k,l}(\tilde{X}^{B})=0\) and \(J(\tilde{X}^{B})=0\) by Eq. (29), which implies that \(\tilde{X}^{B}\in \tilde{\mathcal {P}}^{B}\). It means that \(\tilde{\mathcal {P}}^{B}\) is a closed set and, as it is also bounded, we conclude that \(\tilde{\mathcal {P}}^{B}\) is compact. Now, consider the function \(L:H_{B}^{\oplus n}\rightarrow H^{\oplus n}\) given by \(L(\tilde{X}^{B})\equiv X^{B}=\bigoplus _{l}\mathbb {1}^{A}\otimes \tilde{X}^{B}_{l}\). As L is a linear function, it is continuous, which implies that \(L(\tilde{\mathcal {P}}^{B})=\mathcal {P}^{B}\) is a compact set.\(\square \)
Appendix
Lemma 3
The function \(\tilde{\mathcal {K}}_{k}:H\times H^{\oplus n}\rightarrow \mathbb {R}\) defined as \(\tilde{\mathcal {K}}_{k}(X,Y)\equiv \Vert {{\,\mathrm{Tr}\,}}_{B}(\Pi _{k}(Y)X\) \(\Pi _{k}(Y))\Vert _{1}\) \(\times \Arrowvert {{\,\mathrm{Tr}\,}}_{B}(X)-{{\,\mathrm{Tr}\,}}_{B}(\Pi _{k}(Y)X\Pi _{k}(Y))/\Vert {{\,\mathrm{Tr}\,}}_{B}(\Pi _{k}(Y)X\Pi _{k}(Y))\Vert _{1}\Arrowvert ^{2}_{2}\) if \(\Vert {{\,\mathrm{Tr}\,}}_{B}(\Pi _{k}(Y)\) \(X\Pi _{k}(Y))\Vert _{1}\ne 0\) and \(\tilde{\mathcal {K}}_{k}(X,Y)=0\) if \(\Vert {{\,\mathrm{Tr}\,}}_{B}(\Pi _{k}(Y)X\Pi _{k}(Y))\Vert _{1}=0\), is jointly continuous in the product topology of \(H\times H^{\oplus n}\).
Proof
Defining \(f_{B}(X,Y)\equiv {{\,\mathrm{Tr}\,}}_{B}(YXY)\) and \(\Pi ^{\beta }_{k}(X,Y)\equiv (X,\Pi _{k}(Y))\), we have \(f_{B}\circ \Pi ^{\beta }_{k}(X,\) Y) \(={{\,\mathrm{Tr}\,}}_{B}(\Pi _{k}(Y)X\Pi _{k}(Y))\). As \(f_{B}\) is jointly continuous and \(\Pi _{k}\) is linear, then \(f_{B}\circ \Pi ^{\beta }_{k}\) is jointly continuous. For any point \((X,Y)\in H\times H^{\oplus n}\) such that \(\Vert {{\,\mathrm{Tr}\,}}_{B}(\Pi _{k}(Y)X\Pi _{k}(Y))\Vert _{1}\ne 0\), \(1/\Vert {{\,\mathrm{Tr}\,}}_{B}(\Pi _{k}(Y)X\Pi _{k}(Y))\Vert _{1}\) is jointly continuous. As \(\tilde{\mathcal {K}}_{k}\) is composition of jointly continuous functions, \(\tilde{\mathcal {K}}_{k}\) also has this property for any point \((X,Y)\in H\times H^{\oplus n}\) such that \(\Vert {{\,\mathrm{Tr}\,}}_{B}(\Pi _{k}(Y)X\Pi _{k}(Y))\Vert _{1}\ne 0\).
Now, suppose that (X, Y) is a point such that \(\Vert {{\,\mathrm{Tr}\,}}_{B}(\Pi _{k}(Y)X\Pi _{k}(Y))\Vert _{1}=0\). For arbitrary \(\delta _{x}>0\) and \(\delta _{y}>0\), suppose that \(\Vert X-X'\Vert _{1}<\delta _{x}\) and \(\Vert Y-Y'\Vert _{1}<\delta _{y}\), where \(X,X'\in H\) and \(Y,Y'\in H^{\oplus n}\). Define \(\Delta X\equiv X'-X\) and \(\Delta Y\equiv Y'-Y\). By \(|\tilde{\mathcal {K}}_{k}(X+\Delta X,Y+\Delta Y)-\tilde{\mathcal {K}}_{k}(X,Y)|=|\tilde{\mathcal {K}}_{k}(X+\Delta X,Y+\Delta Y)|\), we have
By the equivalence of norms, there exists a constant c such that, for any \(Z\in H_{A}\), \(\Vert Z\Vert _{2}\le c\Vert Z\Vert _{1}\). Defining \(Z^{B}\equiv {{\,\mathrm{Tr}\,}}_{B}(\Pi _{k}(Y+\Delta Y)(X+\Delta X)\Pi _{k}(Y+\Delta Y)) \), we have
Equations (30) and (31) imply that
As \(Tr_{B}\) is a bounded linear operator, there exists \(M>0\) such that \(\Vert {{\,\mathrm{Tr}\,}}_{B}(XYZ)\Vert _{1}\le M\Vert XYZ\Vert _{1}\le M\Vert X\Vert _{1}\Vert Y\Vert _{1}\Vert Z\Vert _{1}\). By the same argument, there exists \(N>0\) such that \(\Vert \Pi _{k}(Y)\Vert _{1}\le N\Vert Y\Vert _{1}\). In Inequality (32), the “\(\ldots \)” represents several terms with the form \(\Vert {{\,\mathrm{Tr}\,}}_{B}(X'Y'Z')\Vert _{1}\), such that at least one variable is \(\Delta X\) or \(\Pi _{k}(\Delta Y)\). By these considerations and knowing that \(\Vert {{\,\mathrm{Tr}\,}}_{B}(\Pi ^{B}(Y)X\Pi ^{B}(Y))\Vert _{1}=0\), there exists a constant R such that
where \(S>0\) is a constant. Clearly, Inequality (33) implies that \(\tilde{\mathcal {K}}_{k}\) is jointly continuous.\(\square \)
Lemma 3 implies that:
Corollary 3
The function \(\tilde{\mathcal {K}}:D(\mathcal {H})\times \mathcal {P}^{B}\rightarrow \mathbb {R}_{\ge 0}\) defined as \(\tilde{\mathcal {K}}(\rho ,P^{B})\equiv \sum _{k}\tilde{\mathcal {K}}_{k}(\rho ,P^{B})\), where \(D(\mathcal {H})\times \mathcal {P}^{B}\subset H\times H^{\oplus n}\), is jointly continuous.
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Carrijo, T.M., Avelar, A.T. On the continuity of quantum correlation quantifiers. Quantum Inf Process 19, 214 (2020). https://doi.org/10.1007/s11128-020-02709-2
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DOI: https://doi.org/10.1007/s11128-020-02709-2