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Advances in Mathematical Physics
Volume 2016 (2016), Article ID 7213197, 5 pages
http://dx.doi.org/10.1155/2016/7213197
Research Article

Virtual Correlations in Single Qutrit

1Moscow Institute of Physics and Technology, Institutskii per. 9, Dolgoprudny, Moscow Oblast 141700, Russia
2P.N. Lebedev Physical Institute, Russian Academy of Sciences, Leninskii Prospect 53, Moscow 119991, Russia

Received 19 June 2016; Revised 14 September 2016; Accepted 21 September 2016

Academic Editor: Giorgio Kaniadakis

Copyright © 2016 Alexey A. Strakhov and Vladimir I. Man’ko. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract

We construct the positive invertible map of the mixed states of a single qutrit onto the antisymmetrized bipartite qutrit states (quasifermions). It is shown that using this one-to-one correspondence between qutrit states and states of two three-dimensional quasifermions one may attribute hidden entanglement to a single mixed state of qutrit.

1. Introduction

Quantum entanglement [1] is one of the most valuable nonclassical resources in quantum information science. By virtue of entanglement the protocols of superdense coding [2] and quantum teleportation [3] were discovered. Entangled states are essential in quantum computing [4, 5] and are used in various cryptography protocols [6, 7]. Entangled states are also used in more applied areas of physics such as quantum metrology [8, 9].

Naturally it is hard to prepare and maintain maximally entangled states. In order to control the amount of entanglement in quantum systems several measures were proposed. In case of bipartite pure states an entropy of entanglement [10] was proved to be an asymptotic measurement of distillating maximally entangled states by means of local operations and classical communication (LOCC) from the supply of initial pure states and vice versa. The case of mixed states is more complicated. In particular for mixed states the following measures were introduced: the asymptotic entanglement of formation and distillation [11] and the relative entropy of entanglement [12]. However, all of them include variational step and thus are generally hardly calculable (notable exceptions are mixed qubit states fully characterized by concurrence [13]). From the Peres-Horodecki criterion [14, 15] the notions of negativity and logarithmical negativity [1618] emerged. They are relatively easy calculable and the latter provides an upper bound of distillable entanglement. Negativity will be used further in the paper.

Recently several attempts to study quantum correlations of noncomposite qudit systems were conducted [1923]. The physical realization of such systems is convenient with nonlinear quantum circuits on Josephson junctions [24, 25]. This paper is an attempt to study correlations between different degrees of freedom in qutrit via the invertible map to a bipartite system of antisymmetrized states of qutrits (as the dimension of them is odd we shall call them quasifermions). The source of correlations in such case would be antisymmetrization, that is, restriction to the subspace of the whole tensor product space of two qutrits. Actually using the same method one can construct an isomorphism between six-dimensional noncomposite qudit and two indistinguishable four-dimensional fermions. Correlations between particles and modes in the systems of indistinguishable particles were recently studied [2630]. For mixed states of indistinguishable four-dimensional fermions obtained by the isomorphism discussed in the present paper both the dualization concurrence and Slater number will show that the states are separable in the sense of antisymmetrized fermionic subspace. However, we would like to emphasize that due to the virtuality of the division of the noncomposite system into bipartite quasifermion system it is not necessary to treat these quasifermions as indistinguishable particles. One might view correlations resulting from antisymmetrization as internal correlations between different degrees of freedom of the initial qudit. Thus one might treat the initial six-dimensional mixed state as a fully separable state of indistinguishable fermions or as an entangled state of distinguishable particles. The present paper will be about analyzing negativity of qutrit viewed as an antisymmetrized biqutrit state. An open question in such approach is operating with the corresponding virtual subsystems.

2. Partial Trace in Matrix Representation

The state of a subsystem of a quantum system is defined by an operation called partial trace, taking mean value over states of another subsystem: where and are basis vectors of the subsystem and is basis vectors of the subsystem . Despite the explicit choice of basis vectors of space , partial trace is invariant with respect to unitary transformations of .

Let us consider a space and choose a lexicographically ordered basis , . Then an arbitrary state will be presented as matrix:Formula (1) then might be represented by square block matrices whose sizes are determined by the numbers of dimensions of spaces and :where is a state of the first subsystem and is a state of the second subsystem . Partial traces in matrix form will be constantly used further in this paper.

3. Qutrit as Quasifermionic System

Let us pick a basis in an arbitrary three-dimensional state space . The general mixed state of qutrit is described by a density operator : , in matrix form:

Now we will consider a system of two three-dimensional quasifermions, antisymmetrized qutrits. Mathematically it is an exterior product, that is, the quotient of the tensor product by the subspace generated by elements, of two three-dimensional spaces: . Let us pick orthonormal basis vectors in as . Then in the normalized basis of the exterior product an arbitrary pure state looks as follows:

We will further omit the symbol of tensor product. Thus we see that the space is isomorphic to qutrit space . The general form of density operator on space is , so we can introduce an isomorphism between sets of mixed states and by equalizing matrix elements for all .

As we already mentioned, is a state in antisymmetrized subspace of the tensor product space . Let us observe this state in context of the whole space . It is easy to verify that its matrix representation is as follows: Now using the partial trace operation, introduced in the previous section, we are able to obtain single three-dimensional quasifermionic states: The map is a completely positive trace-preserving (CPTP) map. It is obvious because the map is an isomorphism and expanding to is simply adding extra dimensions to Hilbert space which do not participate in constructing of the state ; that is, the spectrum of is equal to the spectrum of and hence of . The partial trace is obviously a CPTP map, so the whole map is CPTP. Despite such trivial construction of reduced states in general their spectrum is different from because their construction was out of quasifermionic antisymmetric subspace .

4. Correlations between Different Degrees of Freedom of Qutrit

The well-known Peres-Horodecki criterion or PPT criterion is a necessary condition for a mixed state to be separable. It states that if the density operator of a bipartite system is separable then partial transpose of one of the subsystems is positive. The partial transpose of the second subsystem of in matrix form is the following: It can be easily verified that has negative values for various states; that is, it is an entangled state. Actually, with the aid of entanglement monotone called negativity it is possible to show that this state is always entangled.

The entanglement monotone is nonnegative linear functional over state with two main properties:(1)The monotone is a convex functional: .(2)The functional is an entanglement monotone, that is, it does not increase on average under local quantum operations and classical communication (LOCC).

Most of the entanglement monotones, like distillability monotones and monotones of formation, are immensely difficult to compute. The more easily countable measure of entanglement is called negativity monotone. It is defined as follows: where is a trace norm. In case of Hermitian operators it is just a sum of modules of negative eigenvalues.

Now it is possible to show that in case of initial pure states their negativity is and in case of maximally chaotic state . More formally, one can use another more convenient entanglement monotone for pure states : the entropy of the subsystem In our case if the initial state and then the density matrices of quasifermion subspaces are as follows: A simple technical calculation shows that nonzero eigenvalues of this matrix are This means that the entanglement measure of is for all initial pure states . Thus the negativities of all pure states are also equal to each other. En elementary calculation for an arbitrary pure state shows that .

The previous considerations about pure states negativities prove that for two different mixed states with equal coefficients and negativities are equal to each other. Thus to analyze all mixed states it is enough to consider a general density matrix: The partial transpose of then will be the following: Its negative eigenvalues are the negative solutions of the third-order equation: Careful analysis shows that for every distribution there is only one negative solution. The infimum of negativity is situated at maximally chaotic state and is equal to .

5. Conclusions

In this paper the simplest nontrivial case of quantum correlations inside qutrit was analyzed. It was demonstrated that for arbitrary mixed qutrit state the negativity is nonzero for corresponding virtual bipartite system of antisymmetrized qutrits. Thus the correlations between the degrees of freedom of qutrit emerge. These considerations could be generalized for qudits with more degrees of freedom in a straightforward manner.

Competing Interests

The authors declare that there are no competing interests regarding the publication of this paper.

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