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From both theoretical and experimental points of view symmetric states constitute an important class of multipartite states. Still, entanglement properties of these states, in particular those with positive partial transposition (PPT), lack…

Quantum Physics · Physics 2013-07-29 R. Augusiak , J. Tura , J. Samsonowicz , M. Lewenstein

We study extremality in various sets of states that have positive partial transposes. One of the tools we use for this purpose is the recently formulated criterion allowing to judge if a given state is extremal in the set of PPT states.…

Quantum Physics · Physics 2015-05-13 Remigiusz Augusiak , Janusz Grabowski , Marek Kuś , Maciej Lewenstein

Multiqubit positive-partial-transpose (PPT) entangled states play an important role in quantum information theory. We characterize such states of minimum rank in three-qubit system, namely rank four. Depending on whether the Lorentz…

Quantum Physics · Physics 2026-05-20 Yonggang Cheng , Lin Chen

In $3\times 3$ dimensions, entangled mixed states that are positive under partial transposition (PPT states) must have rank at least four. They are well understood. We say that they have rank $(4,4)$ since a state $\rho$ and its partial…

Quantum Physics · Physics 2017-08-23 Leif Ove Hansen , Jan Myrheim

We construct $3\otimes 3$ PPT entangled edge states with maximal ranks, to complete the classification of $3\otimes 3$ PPT entangled edge states by their types. The ranks of the states and their partial transposes are 8 and 6, respectively.…

Quantum Physics · Physics 2015-06-04 Seung-Hyeok Kye , Hiroyuki Osaka

We solve the open question of the existence of four-qubit entangled symmetric states with positive partial transpositions (PPT states). We reach this goal with two different approaches. First, we propose a half-analytical-half-numerical…

Quantum Physics · Physics 2015-06-04 J. Tura , R. Augusiak , P. Hyllus , M. Kuś , J. Samsonowicz , M. Lewenstein

We report here on the results of numerical searches for PPT states with specified ranks for density matrices and their partial transpose. The study includes several bipartite quantum systems of low dimensions. For a series of ranks extremal…

Quantum Physics · Physics 2011-03-28 Jon Magne Leinaas , Jan Myrheim , Per Oyvind Sollid

It is known that entangled mixed states that are positive under partial transposition (PPT states) must have rank at least four. In a previous paper we presented a classification of rank four entangled PPT states which we believe to be…

Quantum Physics · Physics 2013-05-30 Leif Ove Hansen , Andreas Hauge , Jan Myrheim , Per Øyvind Sollid

It is known how to construct, in a bipartite quantum system, a unique low rank entangled mixed state with positive partial transpose (a PPT state) from an unextendible product basis (a UPB), defined as an unextendible set of orthogonal…

Quantum Physics · Physics 2013-05-29 Jon Magne Leinaas , Jan Myrheim , Per Øyvind Sollid

It is known that some two qutrit entangled states of rank 4 with positive partial transpose [PPT] can be built from the unextendible product bases [UPB]. We show that this fact is indeed universal, namely all such states can be constructed…

Quantum Physics · Physics 2015-03-19 Lin Chen , Dragomir Z. Djokovic

We construct a set of PPT (positive partial transpose) states and show that these PPT states are not separable, thus present a class of bound entangled quantum states.

Quantum Physics · Physics 2009-11-13 Shao-Ming Fei , Xianqing Li-Jost , Bao-Zhi Sun

Let E' denote the set of non-normalized two-qutrit entangled states of rank four having positive partial transpose (PPT). We show that the set of SLOCC equivalence classes of states in E', equipped with the quotient topology, is…

Quantum Physics · Physics 2012-10-11 Lin Chen , Dragomir Z. Djokovic

Entangled states with a positive partial transpose (so-called PPT states) are central to many interesting problems in quantum theory. On one hand, they are considered to be weakly entangled, since no pure state entanglement can be distilled…

Quantum Physics · Physics 2019-07-17 Károly F. Pál , Tamás Vértesi

Bipartite entangled quantum states with a positive partial transpose (PPT), i.e., PPT entangled states, are usually considered very weakly entangled. Since no pure entanglement can be distilled from them, they are also called bound…

Quantum Physics · Physics 2021-08-26 Károly F. Pál , Géza Tóth , Erika Bene , Tamás Vértesi

We construct a new class of PPT states for bipartite "d x d" systems. This class is invariant under the maximal commutative subgroup of U(d) and contains as special cases almost all known examples of PPT states. Theses states may be used to…

Quantum Physics · Physics 2009-11-13 Dariusz Chruscinski , Andrzej Kossakowski

The absolutely separable (resp. PPT) states remain separable (resp. positive partial transpose) under any global unitary operation. We present a compact form of the extreme points in the sets of absolutely separable states and PPT states in…

Quantum Physics · Physics 2025-10-28 Zhiwei Song , Lin Chen

The equivalence between absolutely separable states and absolutely positive partial transposed (PPT) states in general remains an open problem in quantum entanglement theory. In this work, we study an analogous question for symmetric…

Quantum Physics · Physics 2025-04-16 Jonathan Louvet , Eduardo Serrano-Ensástiga , Thierry Bastin , John Martin

We study the distinguishability of a particular type of maximally entangled states -- the "lattice states" using a new approach of semidefinite program. With this, we successfully construct all sets of four ququad-ququad orthogonal…

Quantum Physics · Physics 2019-04-03 Zong-Xing Xiong , Mao-Sheng Li , Zhu-Jun Zheng , Chuan-Jie Zhu , Shao-Ming Fei

One of the most important problems in quantum information is the separability problem, which asks whether a given quantum state is separable. We investigate multipartite states of rank at most four which are PPT (i.e., all their partial…

Quantum Physics · Physics 2015-06-12 Lin Chen , Dragomir Z. Djokovic

We show that the length of a qubit-qutrit separable state is equal to the max(r,s), where r is the rank of the state and s is the rank of its partial transpose. We refer to the ordered pair (r,s) as the birank of this state. We also…

Quantum Physics · Physics 2013-01-01 Lin Chen , Dragomir Z. Djokovic
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