Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

arXiv:1310.0966 · Physical Review A

Complete analysis for three-qubit mixed-state discrimination

Donghoon Ha, Younghun Kwon

Published Jun 3, 2013• 44 citations
arXivHTMLPDF

Abstract

In this article, by treating minimum error state discrimination as a complementarity problem, we obtain the geometric optimality conditions. These can be used as the necessary and sufficient conditions to determine whether every optimal measurement operator can be nonzero. Using these conditions and an inductive approach, we demonstrate a geometric method and the intrinsic polytope for $N$-qubit mixed-state discrimination. When the intrinsic polytope becomes a point, a line segment, or a triangle, the guessing probability, the necessary and sufficient condition for the exact solution, and the optimal measurement are analytically obtained. We apply this result to the problem of discrimination to arbitrary three-qubit mixed states with given a priori probabilities and obtain the complete analytic solution to the guessing probability and optimal measurement.

DOI
10.1103/physreva.87.062302

Related papers

Minimum-error discrimination of qubit states: Methods, solutions, and properties

Joonwoo Bae, Won-Young Hwang

We show a geometric formulation for minimum-error discrimination of qubit states that can be applied to arbitrary sets of qubit states given with arbitrary a priori probabilities. In particular, when qubit states are given with equal a priori probabilities, we provide a systematic way of finding optimal discrimination and the complete solution in a closed form. This generally gives a bound to cases when prior probabilities are unequal. Then it is shown that the guessing probability does not depend on detailed relations among the given states, such as the angles between them, but on a property that can be assigned by the set of given states itself. This also shows how a set of quantum states can be modified such that the guessing probability remains the same. Optimal measurements are also characterized accordingly, and a general method of finding them is provided.

arXiv:1204.2313•Physical Review A•Jan 30, 2013•49 citations

Complete analysis to minimum-error discrimination of mixed four qubit states with arbitrary prior probabilities

Donghoon Ha, Younghun Kwon

In this work, we provide a complete analysis to minimum-error discrimination of mixed four qubit states with arbitrary prior probabilities. For the complete anaysis, the most important work to do is to find the necessary and sufficient conditions for the existence of null measurement operator. From the geometric structure of qubit states, we obtain the analytic condition for deciding the existence of a null operator in minimum-error measurement for mixed four qubit states, which also gives the necessary and sufficient conditions for every optimal POVM to have non-zero elements. Using the condition, we completely analyze minimum-error discrimination of mixed four qubit states with arbitrary prior probabilities.

arXiv:2111.07726•Nov 15, 2021•0 citations

Geometric bloch vector solution to minimum-error discriminations of mixed qubit states

Mahdi Rouhbakhsh N., Seyed Arash Ghoreishi

Abstract We investigate minimum-error (ME) discrimination for mixed qubit states using a geometric approach. By analyzing positive operator-valued measure (POVM) solutions and introducing Lagrange operator $$\Gamma $$ Γ , we develop a four-step structured instruction to find $$\Gamma $$ Γ for N mixed qubit states. Our method covers optimal solutions for two, three, and four mixed qubit states, including a novel result for four qubit states. We introduce geometric-based POVM classes and non-decomposable subsets for constructing optimal solutions, enabling us to find all possible answers for the general problem of minimum-error discrimination for N mixed qubit states with arbitrary a priori probabilities.

arXiv:2108.12299•Quantum Information Processing•Aug 24, 2023•5 citations

Analysis of optimal unambiguous discrimination of three pure quantum states

Donghoon Ha, Younghun Kwon

We consider unambiguous discrimination of three pure quantum states. Necessary and sufficient conditions to decide which states should be detected for optimal measurement of unambiguous discrimination are provided in terms of inner products and the geometric phase $\mathrm{\ensuremath{\Phi}}$. We get the optimal measurement and the optimal failure probability when the optimal unambiguous discrimination does not require the detection of every given quantum state. When at least two quantum states are orthogonal to each other, we supply the optimal measurement and optimal failure probability in analytic form. When all three quantum states are not orthogonal to each other and $\mathrm{\ensuremath{\Phi}}\ensuremath{\ne}0$, we find an analytic condition to determine the zero and nonzero elements for an optimal positive operator valued measure. We explain how to determine the solution in a geometric manner. Using the known solution of a case where the mutual inner products are real, we check the necessary and sufficient conditions when $\mathrm{\ensuremath{\Phi}}=\ensuremath{\pi}$ and analyze the property of the singular point when $\mathrm{\ensuremath{\Phi}}=0$ and the relation between the optimal points.

Physical Review A•Jun 9, 2015•25 citations

Algebraic approach to minimum-error discrimination of qubit states

Xin Lü, Shi-Hai Dong

Abstract We introduce a general algebraic approach for qubit state discrimination. The primary challenge in such problems lies in determining the nonzero elements of an optimal positive operator-valued measure (POVM). Our work establishes an explicit algebraic criterion to verify whether an optimal POVM for discriminating arbitrary qubit states contains zero elements. Based on this condition, we propose an exhaustive algorithm to obtain analytical solutions for discriminating any number of mixed qubit states with arbitrary prior probabilities.

Journal of Physics A Mathematical and Theoretical•Mar 3, 2026•0 citations

Optimal discrimination of single-qubit mixed states

Graeme Weir, Stephen Mark Barnett, Sarah Croke

We consider the problem of minimum-error quantum state discrimination for single-qubit mixed states. We present a method which uses the Helstrom conditions constructively and analytically; this algebraic approach is complementary to existing geometric methods, and solves the problem for any number of arbitrary signal states with arbitrary prior probabilities. It has long been known that the minimum-error probability is given by the trace of the Lagrange operator $\mathrm{\ensuremath{\Gamma}}$. The remarkable feature of our approach is the central role played not by $\mathrm{\ensuremath{\Gamma}}$, but by its inverse.

arXiv:1704.01035•Physical Review A•Aug 14, 2017•20 citations
In this article, by treating minimum error state discrimination as a complementarity problem, we obtain the geometric optimality conditions. These can be used as the necessary and sufficient conditions to determine whether every optimal measurement operator can be nonzero. Using these conditions and an inductive approach, we demonstrate a geometric method and the intrinsic polytope for NNN-qubit mixed-state discrimination. When the intrinsic polytope becomes a point, a line segment, or a triangle, the guessing probability, the necessary and sufficient condition for the exact solution, and the optimal measurement are analytically obtained. We apply this result to the problem of discrimination to arbitrary three-qubit mixed states with given a priori probabilities and obtain the complete analytic solution to the guessing probability and optimal measurement.
We show a geometric formulation for minimum-error discrimination of qubit states that can be applied to arbitrary sets of qubit states given with arbitrary a priori probabilities. In particular, when qubit states are given with equal a priori probabilities, we provide a systematic way of finding optimal discrimination and the complete solution in a closed form. This generally gives a bound to cases when prior probabilities are unequal. Then it is shown that the guessing probability does not depend on detailed relations among the given states, such as the angles between them, but on a property that can be assigned by the set of given states itself. This also shows how a set of quantum states can be modified such that the guessing probability remains the same. Optimal measurements are also characterized accordingly, and a general method of finding them is provided.
In this work, we provide a complete analysis to minimum-error discrimination of mixed four qubit states with arbitrary prior probabilities. For the complete anaysis, the most important work to do is to find the necessary and sufficient conditions for the existence of null measurement operator. From the geometric structure of qubit states, we obtain the analytic condition for deciding the existence of a null operator in minimum-error measurement for mixed four qubit states, which also gives the necessary and sufficient conditions for every optimal POVM to have non-zero elements. Using the condition, we completely analyze minimum-error discrimination of mixed four qubit states with arbitrary prior probabilities.
Abstract We investigate minimum-error (ME) discrimination for mixed qubit states using a geometric approach. By analyzing positive operator-valued measure (POVM) solutions and introducing Lagrange operator Γ\Gamma Γ Γ , we develop a four-step structured instruction to find Γ\Gamma Γ Γ for N mixed qubit states. Our method covers optimal solutions for two, three, and four mixed qubit states, including a novel result for four qubit states. We introduce geometric-based POVM classes and non-decomposable subsets for constructing optimal solutions, enabling us to find all possible answers for the general problem of minimum-error discrimination for N mixed qubit states with arbitrary a priori probabilities.
We consider unambiguous discrimination of three pure quantum states. Necessary and sufficient conditions to decide which states should be detected for optimal measurement of unambiguous discrimination are provided in terms of inner products and the geometric phase $\mathrm{\ensuremath{\Phi}}$. We get the optimal measurement and the optimal failure probability when the optimal unambiguous discrimination does not require the detection of every given quantum state. When at least two quantum states are orthogonal to each other, we supply the optimal measurement and optimal failure probability in analytic form. When all three quantum states are not orthogonal to each other and $\mathrm{\ensuremath{\Phi}}\ensuremath{\ne}0$, we find an analytic condition to determine the zero and nonzero elements for an optimal positive operator valued measure. We explain how to determine the solution in a geometric manner. Using the known solution of a case where the mutual inner products are real, we check the necessary and sufficient conditions when $\mathrm{\ensuremath{\Phi}}=\ensuremath{\pi}$ and analyze the property of the singular point when $\mathrm{\ensuremath{\Phi}}=0$ and the relation between the optimal points.
Abstract We introduce a general algebraic approach for qubit state discrimination. The primary challenge in such problems lies in determining the nonzero elements of an optimal positive operator-valued measure (POVM). Our work establishes an explicit algebraic criterion to verify whether an optimal POVM for discriminating arbitrary qubit states contains zero elements. Based on this condition, we propose an exhaustive algorithm to obtain analytical solutions for discriminating any number of mixed qubit states with arbitrary prior probabilities.
We consider the problem of minimum-error quantum state discrimination for single-qubit mixed states. We present a method which uses the Helstrom conditions constructively and analytically; this algebraic approach is complementary to existing geometric methods, and solves the problem for any number of arbitrary signal states with arbitrary prior probabilities. It has long been known that the minimum-error probability is given by the trace of the Lagrange operator $\mathrm{\ensuremath{\Gamma}}$. The remarkable feature of our approach is the central role played not by $\mathrm{\ensuremath{\Gamma}}$, but by its inverse.