Abstract
The optimality of a class of entanglement witnesses constructed from any permutation \(\pi \) for any \(n\otimes n\) bipartite systems is investigated. A necessary and sufficient condition is presented for such entanglement witnesses to be optimal, and thus, a class of optimal entanglement witnesses constructed by permutations is obtained.
Similar content being viewed by others
Explore related subjects
Discover the latest articles, news and stories from top researchers in related subjects.References
Bruß, D.: Characterizing entanglement. J. Math. Phys. 43, 4237–4251 (2002)
Choi, M.-D.: Completely positive linear maps on complex matrices. Lin. Alg. Appl. 10, 285–290 (1975)
Chruściński, D., Kossakowski, A.: On the structure of entanglement witnesses and new class of positive indecomposable maps. Open Syst. Inf. Dyn. 14, 275–294 (2007)
Ha, K.-C.: Optimal PPTES witnesses for states in \(\mathbb{C}^n\otimes \mathbb{C}^n\). Phys. Rev. A 86, 014304 (2012)
Ha, K.-C., Kye, S.-H.: Optimality for indecomposable entanglement witnesses. Phys. Rev. A 86, 034301 (2012)
Ha, K.-C., Yu, H.: Optimal indecomposable witnesses without extremality as well as spanning property. J. Phys. A Math. Gen. 45, 395307 (2012)
Horodecki, M., Horodecki, P., Horodecki, R.: Separability of mixed states: necessary and sufficient conditions. Phys. Lett. A 223, 1–8 (1996)
Hou, J.-C.: A characterization of positive elementary operators. J. Oper. Theory 39, 43–58 (1998)
Hou, J.-C.: A characterization of positive linear maps and criteria for entangled quantum states. J. Phys. A Math. Theor. 43, 385201 (2010)
Hou, J.-C., Guo, Y.: When different entanglement witnesses detect the same entangled states. Phys. Rev. A 82, 052301 (2010)
Hou, J.-C., Li, C.-K., Poon, Y.-T., Qi, X.-F., Sze, N.-S.: A new criterion and a special class of \(k\)-positive maps. Lin. Alg. Appl. 470, 51–69 (2015)
Hou, J.-C., Qi, X.-F.: Constructing entanglement witnesses for infinite-dimensional systems. Phys. Rev. A 81, 062351 (2010)
Hyllus, P.: Optimal entanglement witnesses for continuous-variable systems. J. Eisert N. J. Phys. 8, 51 (2006)
Jafarizadeh, M.A., Behzadi, N., Akbari, Y.: Entanglement witnesses and characterizing entanglement properties of some PPT states. Eur. Phys. J. D. 55, 197–203 (2009)
Jamiołkowski, A.: Linear transformations which preserve trace and positive semidefiniteness of operators. Rep. Math. Phys. 3, 275–278 (1972)
Lewensetein, M., Kraus, B., Cirac, J.I., Horodecki, P.: Optimization of entanglement witnesses. Phys. Rev. A 62, 052310 (2001)
Qi, X.-F., Hou, J.-C.: Positive finite rank elementary operators and characterizing entanglement of states. J. Phys. A. Math. Theor. 43, 385201 (2011)
Qi, X.-F., Hou, J.-C.: Characterization of optimal entanglement witnesses. Phys. Rev. A 85, 022334 (2012)
Qi, X.-F., Hou, J.-C.: Optimality of a class of entanglement witnesses for \(3\otimes 3\) systems. Int. J. Theor. Phys. 52(10), 3474–3485 (2013)
Qi, X.-F., Hou, J.-C.: Indecomposability of entanglement witnesses constructed from any permutation. Quant. Inf. Comput. 15(5&6), 0478–0488 (2015)
Tóth, G., Gühne, O.: Detecting genuine multipartite entanglement with two local measurements. Phys. Rev. Lett. 94, 060501 (2005)
Zwolak, J.P., Chruściński, D.: Recurrent construction of optimal entanglement witnesses for \(2N\)-qubit systems. Phys. Rev. A 89, 052314 (2014)
Zhao H.-L., Hou J.-C.: Criteria of positivity for linear maps constructed from permutation pairs. arXiv:1302.0175v1
Acknowledgments
The authors wish to give their thanks to the referees for their helpful comments and suggestions to improve the original manuscript. This work was partially completed while the first author was visiting the Institute of Quantum Computation of the University of Waterloo during the academic year 2014–2015, and she would like to thank Professor Bei Zeng for her hospitality. This work is partially supported by National Natural Science Foundation of China (11171249) and Program for the Outstanding Innovative Teams of Higher Learning Institutions of Shanxi.
Author information
Authors and Affiliations
Corresponding author
Appendix: A proof of main theorem
Appendix: A proof of main theorem
Here, we give a proof of the main theorem. Before doing it, let us recall some notions and give several lemmas needed.
Let \(l\), \(k\in \mathbb {N}\) (the set of all natural numbers), and let \(A_{1},\ldots , A_{k}\), \(C_{1},\ldots , C_{l}\in {\mathcal B}(H\), \(K\)). If, for each \(|\psi \rangle \in H\), there exists an \(l\times k\) complex matrix \((\alpha _{ij}(|\psi \rangle ))\) (depending on \(|\psi \rangle \)) such that \(C_{i}|\psi \rangle =\sum _{j=1}^{k}\alpha _{ij}(|\psi \rangle )A_{j}|\psi \rangle \), \(i=1,2,\ldots ,l,\) we say that \((C_{1},\ldots ,C_{l})\) is a locally linear combination of \((A_{1},\ldots ,A_{k})\) and \((\alpha _{ij}(|\psi \rangle ))\) is called a local coefficient matrix at \(|\psi \rangle \). Furthermore, if for every \(|\psi \rangle \in H\), the associated local coefficient matrix \((\alpha _{ij}(|\psi \rangle ))\) can be chosen so that its operator norm \(\Vert (\alpha _{ij}(|\psi \rangle ))\Vert =\sup \{\Vert (\alpha _{ij}(|\psi \rangle )|x\rangle \Vert : |x\rangle \in {\mathbb C}^\mathrm{k}, \Vert |x\rangle \Vert \le 1\}\le 1\), we say that \((C_{1},\ldots ,C_{l})\) is a contractive locally linear combination of \((A_{1},\ldots ,A_{k})\); if there is a matrix \((\alpha _{ij})\) such that \(C_{i}=\sum _{j=1}^{k}\alpha _{ij}A_{j}\) for all \(i\), we say that \((C_{1},\ldots ,C_{l})\) is a linear combination of \((A_{1},\ldots ,A_{k})\) with coefficient matrix \((\alpha _{ij})\) (see [8, 9] for more details).
Lemma 1
([8, 9]) Let \(H\) and \(K\) be complex Hilbert spaces of any dimension and \(\Phi : {\mathcal B}(H)\rightarrow {\mathcal B}(K)\) a linear map defined by \(\Phi (X) =\sum _{i=1}^{k}C_{i}XC_{i}^{\dagger }-\sum _{j=1}^{l}D_{j}XD_{j}^{\dagger }\) for all \(X\in {\mathcal B}(H)\), where \(C_1,\ldots ,C_k; D_1,\ldots , D_l\in {\mathcal B}(H,K)\). Then, \(\Phi \) is positive if and only if \((D_{1},\ldots ,D_{l})\) is a contractive locally linear combination of \((C_{1},\ldots ,C_{k})\). Furthermore, \(\Phi \) is completely positive if and only if \((D_{1},\ldots ,D_{l})\) is a linear combination of \((C_{1},\ldots ,C_{k})\) with a contractive coefficient matrix and, in turn, if and only if there exist \(E_1, E_2, \ldots , E_r\) in \(\mathrm{span}\{C_{1},\ldots ,C_{k}\}\) such that \( \Phi =\sum _{i=1}^r E_i(\cdot )E_i^\dagger .\)
The following lemma comes from [23], which is useful to establish our key lemma, that is, Lemma 3 below, and is also useful in the proof of the main theorem.
Lemma 2
Let \(s,M\) be positive numbers and \(f(u_1,u_2,\ldots ,u_m)\) a function in \(m\)-variable defined by
on the region \(u_i>0\) with \(u_1u_2\ldots u_m=M^m\), \(i=1,2,\ldots ,m\). Then, \(\sup f(u_1,u_2,\ldots ,u_m)=\max \{\frac{m-1}{s}, \frac{m}{s+M}\}.\) Moreover, we have
and
The next lemma is crucial for our purpose.
Lemma 3
Let \(t\) be a fixed number with \(0<t<1\) and \(n\) a positive integer with \(n\ge 2\). Let \(x_1,x_2,\ldots ,x_n\) be any positive numbers with \(\prod _{i=1}^nx_i=1\) and \((x_1,x_2,\ldots ,x_n)\not =(1,1,\ldots ,1)\). Then,
Proof
Let \(f\) be the function in \(n\) variables defined by
If \(n=2\), then for any \(x_1,x_2>0\) with \(x_1x_2=1\) and \((x_1,x_2)\not =(1,1)\), we have
Obviously, the lemma is true.
In the sequel, assume that \(n\ge 3\). Since \((x_1,x_2,\ldots ,x_n)\not =(1,1,\ldots ,1)\), we have \(1-\sum _{i=1}^n\frac{1}{n-t+tx_i}\not =0\), and
where \(t\) is fixed with \(0<t<1\), \(x_1,x_2,\ldots ,x_n\) are any positive numbers with \(\prod _{i=1}^nx_i=1\), and \((x_1,x_2,\ldots ,x_n)\not =(1,1,\ldots ,1)\).
Now fix \(x_1\) and \(x_2\); then \(\prod _{i=3}^nx_i=\frac{1}{x_1x_2}\). Using Lemma 2 with \(s=n-t\), \(M=\frac{t}{\root n-2 \of {x_1x_2}}\) and \(m=n-2\), we obtain
if \(x_1x_2\ge (\frac{tn-3t}{n-t})^{n-2}\); and
if \(x_1x_2<(\frac{tn-3t}{n-t})^{n-2}\).
Assume that \(0<x_1x_2<(\frac{tn-3t}{n-t})^{n-2}\); then Eq. (5) holds. Thus, for any positive numbers \(x_1,x_2\ldots ,x_n\) satisfying \(\prod _{i=1}^nx_i=1\) and \(0<x_1x_2<(\frac{tn-3t}{n-t})^{n-2}\), Eqs. (5) and (3) yield
Define a function
where \(x_1,x_2\) are any positive numbers with \(x_1x_2<(\frac{tn-3t}{n-t})^{n-2}\). To prove that the lemma is true in this case, one only needs to check that \(g(x_1,x_2)\ge 1-t\) for all \(x_{i}>0\) \((i=1,2)\) with \(x_1x_2<(\frac{tn-3t}{n-t})^{n-2}\).
In fact, since the denominator of \(g(x_1,x_2)\) is not zero, a computation shows that
where
Note that \((1-t)(n-t)(n-2+t)\), \(2nt-nt^2+2t^2-3t\) and \(t^2(3-t)\) are all positive. So, \(h(x_1,x_2)>0\) for all positive numbers \(x_1\) and \(x_2\). This implies that the lemma holds whenever \(0<x_1x_2<(\frac{tn-3t}{n-t})^{n-2}\).
Now, consider the case \(x_1x_2\ge (\frac{tn-3t}{n-t})^{n-2}\). In this case, Eq. (4) holds. Combining Eqs. (3–4), for any positive numbers \(x_1,x_2\ldots ,x_n\) with \(\prod _{i=1}^nx_i=1\) and \(x_1x_2\ge (\frac{tn-3t}{n-t})^{n-2}\), we have
Define a function
where \(x_1,x_2,x_3\) are any positive numbers with \(x_1x_2x_3^{n-2}=1\) and \(x_1x_2\ge (\frac{tn-3t}{n-t})^{n-2}\). Still, we only need to check that the minimum of \(g(x_1,x_2,x_3)\) is \(1-t\) on the region \(x_{i}>0\) with \(x_{1}x_{2}x_3^{n-2}=1\) and \(x_1x_2\ge (\frac{tn-3t}{n-t})^{n-2}\).
Also, note that the denominator of \(g(x_1,x_2,x_3)\) is not zero whenever \((x_1,x_2,x_3)\not =(1,1,1)\). A computation shows that
where
Let
By the method of Lagrange multipliers, we have the system
By (i) and (ii), one obtains \((x_2-x_1)(2t-t^2+t^2x_3+\lambda x_3^{n-2})=0,\) which implies that
If \(2t-t^2+t^2x_3+\lambda x_3^{n-2}=0\), by (ii), one gets \(x_3=\frac{t-1}{t}<0\), a contradiction. Hence, we must have \(x_1=x_2\). Thus, (ii) and (iii) become
and
Combining the above two equations and applying (iv), we get
Letting \(y>0\) and \(y=\root n-2 \of {x_1}\), then \(x_1=y^{n-2}\) and \(x_3=y^{-2}\) as \(x_1^2x_3^{n-2}=1\). Replacing \(x_1\) and \(x_3\) by \(y\) in the above equation, one has
Solving the equation, we achieve
Note that \(2nt-4t-nt^2+2t^2\), \(2nt-4t-t^2\) and \(n^2-4n-t^2+4\) are all positive. So, the solution of the above equation is \(y=1\), which implies \(x_1=x_2=x_3=1\). It follows that the function \(h(x_1,x_2,x_3)\) takes its extremum at the point \((1,1,1)\). Moreover, it is easy to check that \((1,1,1)\) is the minimal point of \(h(x_1,x_2,x_3)\). Hence, \(h(x_1,x_2,x_3)\ge h(1,1,1)=0\) for all \(x_{i}>0\) satisfying \(x_{1}x_{2}x_3^{n-2}=1\) and \(x_1x_2\ge (\frac{tn-3t}{n-t})^{n-2}\), \(i=1,2,3\). This implies that the lemma holds whenever \(x_1x_2\ge (\frac{tn-3t}{n-t})^{n-2}\).
Therefore, the inequality in Lemma 3 holds for all \(x_i>0\) (\(i=1,2,\ldots ,n\)) with \(\prod _{i=1}^nx_i=1\) and \((x_1,x_2,\ldots ,x_n)\not =(1,1,\ldots ,1)\). The proof is finished. \(\square \)
Now, we are in a position to give our proof of the main theorem.
Proof of Main Theorem
For \(\pi =(\pi _1)(\pi _2) \ldots (\pi _k)\), with no loss of generality, assume \(l(\pi _j)=n_{j}-n_{j-1}\) and \(\pi _j(n_{j-1}+i)=(n_{j-1}+i+1)\ \mathrm{mod}(n_{j}-n_{j-1})\), \(i=1,2,\ldots ,n_{j}-n_{j-1}\), \(j=1,\ldots ,k\). Here, set \(n_0=0\) and \(n_k=n\).
By a similar approach to that of [18], Theorem 3.2] using Proposition 1, one can prove that the “if” part holds.
In the rest part of this paper, we will show that, if one of the conditions (i–iii) in the theorem is not satisfied, then \(W_{{n,t,\pi }}\) is not optimal, and therefore, the “only if” part holds. To do this, by Proposition 1, one has to find a matrix \(C_0\in M_n({\mathbb C})\) such that the linear map \(A\mapsto \Phi _{n,t,\pi }(A)-C_0AC_0^\dagger \) is positive.
For \(\pi =(\pi _1)(\pi _2)\cdots (\pi _k)\), still assume that \(l(\pi _j)=n_{j}-n_{j-1}\) and \(\pi _j(n_{j-1}+i)=(n_{j-1}+i+1)\ \mathrm{mod}(n_{j}-n_{j-1})\), \(i=1,2,\ldots ,n_{j}-n_{j-1}\) and \(j=1,\ldots ,k\), with \(n_0=0\) and \(n_k=n\). Let \(\Psi _{C_0}\) be the map defined by
for all \(A\in M_n({\mathbb C})\). If \(\Psi _{C_0}\) is positive, by Lemma 1, for any unit vector \(|x\rangle \in {\mathbb C}^n\), there exist scalars \(\{ \alpha _{i}^j\}\), \(\{ \beta _{i}^j\}\), \(\{\delta _i^j\}\), \(\{\gamma _i^j\}\) depending on \(|x\rangle \) such that
and the matrix
is contractive. Note that
and \(\Vert F_x\Vert \le 1\) if and only if \(\Vert F_xF_x^\dag \Vert \le 1 \).
In the sequel, for any unit vector \(|x\rangle \in {\mathbb C}^n\), write \(|x\rangle =(|x_1|e^{i\theta _1},|x_2|e^{i\theta _2},\ldots , |x_n|e^{i\theta _n})^T\). Then, \(\sum _{i=1}^n|x_i|^2=1\). We will complete the proof of the theorem by considering two cases.
Case 1 \(\pi \) is cyclic.
In this case, \(\pi =(\pi _1)\), \(l(\pi )=l(\pi _1)=n\) and \(\pi (i)=(i+1)\) mod \(n\). We will show that, for any \(0<t<1\) and any \(C_0=\mathrm{diag}(c,-c,0,\cdots ,0)\) with \(0<c\le \sqrt{1-t}\), \(\Psi _{C_0}\) is positive, and so \(W_{{n,t,\pi }}\) is not optimal.
In the present case, Eqs. (6–8) can be reduced to
and
where \(\alpha _i=\alpha _i^1\), \(\beta _i=\beta _i^1\),\(\delta _i=\delta _i^1\) and \(\gamma _i=\gamma _i^1\) for \(i=1,2,\ldots ,n\).
Subcase 1.1 \(|x_i|=\frac{1}{\sqrt{n}}\) for all \(i=1,2,\ldots ,n\).
In Eqs. (4\(^\prime \)–5\(^\prime \)), by taking
and
we get
So, \(\sum _{i=1}^n(|\alpha _i|^2+|\beta _i|^2)=1\), \(\sum _{i=1}^n(|\delta _i|^2+|\gamma _i|^2)=\frac{2c^2}{n}\), and \(\sum _{i=1}^n(\alpha _i\overline{\delta _i}+\beta _i\overline{\gamma _i}) =0\). It follows that
which implies that \(\Vert F_xF_x^\dag \Vert \le 1\Leftrightarrow c^2\le \frac{n}{2}.\) Hence,
Subcase 1.2 \(x_i\not =0\) for all \(i=1,2,\ldots ,n\) and \((|x_1|,|x_2|,\ldots ,|x_n|)\not =(\frac{1}{\sqrt{n}},\frac{1}{\sqrt{n}},\ldots ,\frac{1}{\sqrt{n}})\).
Let \(r_i=|\frac{x_i}{x_{i+1}}|^2\) for \(i=1,2,\ldots , n\). Then, \(r_i>0\) with \(\prod _{i=1}^nr_i=1\). Take
and
By Eqs. (4\(^\prime \)–5\(^\prime \)), one gets
and
So,
and
It follows that
Note that \(\Vert F_{x}F_{x}^\dag \Vert \le 1\) if and only if its maximal eigenvalue \(\lambda _{\mathrm{max}}\le 1\). By a calculation, it is easily checked that \(\lambda _{\mathrm{max}}\le 1\) holds if and only if
where \(r_1,r_2,\ldots ,r_n>0\) with \(\prod _{i=1}^nr_i=1\) and \((r_1,r_2,\ldots ,r_n)\not =(1,1,\ldots ,1)\). Let
Replacing \(r_i\) by \(\frac{1}{r_i}\) in \(g(r_1,r_2,\ldots ,r_n)\) gives
Now, applying Lemma 3 to the function \(g\), we see that \(g(r_1,r_2,\ldots ,r_n)\ge 1-t\) holds for all positive numbers \(r_1,r_2,\ldots ,r_n\) with \(\prod _{i=1}^nr_i=1\) and \((r_1,r_2,\ldots ,r_n)\not =(1,1,1\ldots ,1)\). This and Eq. (7) imply
Combining Subcases 1.1–1.2 and by the proof in [8, 9] of Lemma 1, we have proved that, for any matrix \(C_0=\mathrm{diag}(c,-c,0,\cdots ,0)\) with \(0<c^2\le 1-t\), it holds that
Subcase 1.3 There exists at least one \(x_{i_0}=0\) for some \(i_0\in \{1,2,\ldots ,n\}\).
In this case, it is easily seen that there is a sequence of unit vectors
such that \(\lim _{m\rightarrow \infty }|y_m\rangle =|x\rangle \). So, \(\lim _{m\rightarrow \infty }|y_m\rangle \langle y_m|=|x\rangle \langle x|\) under norm topology. Note that \(\Psi _{C_0}(|y_m\rangle \langle y_m|)\ge 0\) for each \(|y_m\rangle \) by Eq. (10) and \(\Psi _{C_0}\) is continuous. It follows that
that is, \(\Psi \) is positive on any rank one projection \(|x\rangle \langle x|\). Hence, \(\Psi _{C_0}\) is positive. Then, by Proposition 1, \(W_{{n,t,\pi }}\) is not optimal whenever \(0<t<1\). The proof of Case 1 is finished.
Case 2 \(\pi \) is not cyclic.
We will prove it by considering five subcases.
Subcase 2.1 \(l=l(\pi _i)=1\) for all \(i=1,2,\ldots ,k\).
In this case, \(\pi =\mathrm{id}\), and so \(\Phi _{n,t,\pi }\) is a completely positive linear map. It follows that \(W_{n,t,\pi }\) is positive which is not an entanglement witness.
Subcase 2.2 \(l(\pi )=2\).
In this case, \(\pi ^2=\mathrm{id}\). By [20], \(W_{\Phi _{n,t,\pi }}=Q_1+Q_2^T\) is decomposable with \(Q_i\ge 0\) and \(Q_i\not =0\), \(i=1,2\). So, \(W_{n,t,\pi }\) is not optimal because \(Q_2^T\) is an entanglement witness [16].
Subcase 2.3 There exists some cycle \(\pi _j\) such that \(2\le l(\pi _j)<l\) with \(l=l(\pi )\ge 3\).
For the simplicity, assume that \(2\le l(\pi _1)<l\). We will prove that, for any \(0<t\le \frac{n}{l}\), by taking \(C_0=\mathrm{diag}(c,-c,0,\cdots ,0)\) with \(0<c\le \sqrt{1-\frac{l(\pi _1)}{n}t}\), \(\Psi _{C_0}\) is positive, and so \(W_{{n,t,\pi }}\) is not optimal for any \(0\le t\le \frac{n}{l}\). Indeed, similar to the argument of Subcase 1.3 in Case 1, one only needs to check whether there exists a coefficient matrix \(F_x\) such that \(\Vert F_x\Vert \le 1\) for those vectors \(|x\rangle =(x_1,x_2,\ldots ,x_n)\) with \(x_i\not =0\), \(i=1,2,\ldots , n\).
Letting \(r_{i}^{j}=|\frac{x_i}{x_{i+1}}|^2\) (\(i=n_{j-1}+1,n_{j-1}+2,\ldots ,n_j\); \(j=1,2,\ldots , k\)), then \(\prod _{i=n_{j-1}+1}^{n_j}r_{i}^{j}=1\). Take \(\alpha _i^j=\frac{\sqrt{n-t}r_{i}^{j}}{t+(n-t)r_{i}^{j+1}}\) for all \(i,j\), \(\delta _1^1=\frac{c\sqrt{n-t}r_1^1}{t+(n-t)r_1^1}\), \(\delta _2^1=\frac{-c\sqrt{n-t}r_2^1}{t+(n-t)r_2^1}\) and \(\delta _i^j=0\) for other \(i,j\). By Eqs. (6–7), one has \(\beta _i^j=\frac{\sqrt{tr_{i}^{j}}e^{i(\theta _i-\theta _{i+1})}}{t+(n-t)r_{i}^{j}}\) for all \(i,j\), \(\gamma _1^1=\frac{c\sqrt{tr_1^1}e^{i(\theta _1-\theta _2)}}{t+(n-t)r_1^1}\), \(\gamma _2^1=\frac{-c\sqrt{tr_2^1}e^{i(\theta _2-\theta _3)}}{t+(n-t)r_2^1}\) and \(\gamma _i^j=0\) for other \(i,j\), and so
where
and \(s=\frac{l(\pi _1)}{n}t\le \frac{l(\pi _1)}{n}\frac{n}{l}=\frac{l(\pi _1)}{l}<1\). So, by taking \(c\) with
and using similar argument to Subcase 1.2, we obtain \(\Vert F_1F_1^\dag \Vert \le \frac{l(\pi _1)}{n}\). Since \(\prod _{i=n_{j-1}+1}^{n_j}r_{i}^{j}=1\), by Lemma 2, one gets
Note that \(n_j-n_{j-1}\le l(\pi )=l\) and \(t\le \frac{n}{l}\), and we see that \(\frac{n_{j}-n_{j-1}-1}{n-t}\le \frac{n_{j}-n_{j-1}}{n}\), and so
This implies that
Subcase 2.4 \(t<\frac{n}{l(\pi )}\).
In this case, there exists some \(\pi _i\) such that \(l(\pi _i)=l(\pi )\), still, without loss of generality, assume \(\pi _1\). By a similar argument to that of the above Subcase 2.3, one can show that \(W_{n,t,\pi }\) is also not optimal.
Subcase 2.5 There exists at least two fixed points.
Without loss of generality, assume that \(l(\pi _1)=l(\pi _2)=1\). Still, only consider the case that \(x_i\not =0\) (\(i=1,2,\ldots ,n\)) for any \(|x\rangle =(x_1,x_2,\ldots ,x_n)\). Let \(C_0=\mathrm{diag}(c,-c,0,\cdots ,0)\). In Eqs. (6–7), by taking \(\alpha _1^1=\alpha _2^2=\frac{\sqrt{n-t}}{n}\), \(\delta _1^1=\frac{c\sqrt{n-t}}{n}\), \(\delta _2^2=\frac{-c\sqrt{n-t}}{n}\) and \(\alpha _i^j=\frac{\sqrt{n-t}r_{i}^{j}}{t+(n-t)r_{i}^{j}}\), \(\delta _i^j=0\) for other \(i,j\), one can obtain \(\beta _1^1=\beta _2^2=\frac{\sqrt{t}}{n}\), \(\gamma _1^1=\frac{c\sqrt{t}}{n}\), \(\gamma _2^2=\frac{-c\sqrt{t}}{n}\) and \(\beta _i^j=\frac{\sqrt{tr_{i}^{j}}e^{i(\theta _i-\theta _{i+1})}}{t+(n-t)r_{i}^{j}}\), \(\gamma _i^j=0\) for other \(i,j\). Thus,
By Eq. (9), we get
This yields \(0<c^2\le \frac{n}{2}\Rightarrow \Vert F_{x}F_{x}^\dag \Vert \le 1\).
Now, combining Subcases 2.1–2.5 and applying Lemma 1, \(\Psi _{C_0}\) is positive, and so \(W_{{n,t,\pi }}\) is not optimal. The proof of Case 2 is finished.
The proof of the main theorem is complete. \(\square \)
Rights and permissions
About this article
Cite this article
Qi, X., Hou, J. Optimality of entanglement witnesses constructed from arbitrary permutations. Quantum Inf Process 14, 2499–2515 (2015). https://doi.org/10.1007/s11128-015-1007-z
Received:
Accepted:
Published:
Issue Date:
DOI: https://doi.org/10.1007/s11128-015-1007-z