Analysis of the unambiguous state discrimination with unequal a priori probabilities Текст научной статьи по специальности «Физика»

NANOSYSTEMS: PHYSICS, CHEMISTRY, MATHEMATICS, 2019, 10 (4), P. 398-401

Analysis of the unambiguous state discrimination with unequal a priori probabilities

In this paper, we study unambiguous state discrimination regarding advanced attack on phase-coded quantum key distribution protocol. We propose the method of optimal unambiguous state discrimination probability derivation as a function of a priori probabilities for signal states. The expression obtained as an example in case of two signal states explicitly demonstrates the additional term dependent on small deviations from equal a priori probabilities that may take place in real quantum key distribution implementations. Precise estimation of optimal unambiguous state discrimination probability is significant for complete evaluation of quantum key distribution security.

Keywords: quantum key distribution, unambiguous state discrimination.

Received: 13 May 2019

Revised: 28 June 2019

1. Introduction

Throughout the last few decades the field of quantum cryptography has been rapidly developing and advancing. It has emerged with the first papers [1,2] dedicated to the descriptions of protocols which allow secure distribution of a finite bit sequence between legitimate partners, and it is still in the focus of research groups, for instance [3-5]. Not only the protocols are of special interest, but also different types of attacks are studied in order to find successful countermeasures.

In this work we would like to concentrate on zero-error unambiguous state discrimination (USD) attack that is a considerable threat for protocols utilizing weak coherent states. USD attack requires eavesdropper (Eve) tapping into quantum channel of legitimate parties (Alice and Bob), errorlessly measuring the states and resending the modified states to Bob in order to preserve detection statistics [6]. We explore the phase-coded protocol which utilizes several pairs weak coherent states sent with unequal a priori probability. Imperfect state preparation that can result in the sending probabilities' inequality is the immanent part of every practical set-up. For example, quantum random number generator may cause unequal probability of state preparation [7-9]. Hence we examine the influence of unequal a priori probability on the discrimination probability.

USD measurement is subject of research for almost three decades. General approach to discrimination between linearly independent states was introduced in [10,12,13]. The solution for minimum achievable probability of inconclusive outcome for three states was given by [11]. The method of minimizing the probability for N symmetric states was considered in [12]. The special case of equal a priori probabilities for N states was discussed in [13]. Bounds of unambiguous state discrimination probabilities have been studied for the case of N linearly independent states in [14-16]. Several approaches to numerical optimization were proposed as well in [16,17]. Implementations of USD in field of quantum computations also take place, e.g. for purpose of quantum cloning operation [18] or USD between oracle operators [19].

2. Method description

To perform unambiguous discrimination of the N signal states \fi) Eve determines special positive-operator valued measure (POVM). It consists of projection operators Ai which are related to probabilities of successful state discrimination Pi (for each state) and operator A0 that is related to obtaining inconclusive result which is always present due to the nonorthogonality of the states and introduced in order to make the sum of the projection operators satisfy the decomposition of the identity:

A. A. Gaidash, S. S. Medvedeva, G. P. Miroshnichenko

ITMO University, Kronverkskiy, 49, St. Petersburg, 197101, Russia [email protected], [email protected]

PACS 42.50.Dv

DOI 10.17586/2220-8054-2019-10-4-398-401

N

i=0

Extracted from (1) the operator A0 is expressed as:

N

Ao = I-X) A, (2)

i=1

and according to [11] A0 is subject to condition:

det[Ao] = 0. (3)

The latter provides maximal allowed values for probabilities Pi. We specify operators Ai as follows:

Ai = Pi |vi)(vi|, (4)

where |vi) is state that forms biorthogonal basis with the signal states |fi) (i.e. (v/) = Sij, where Sij is Kronecker delta).

Thus one needs to optimize the average probability of USD:

N

P = Y, PiPi, (5)

where pi is a priori probability of sending each state. One may use Lagrange multiplier method in order to do so. Hence, the function to be optimized is P from expression (5) and the following expression is bound [11]:

det Ao = det ^Î — ^N Pi|vi)(vi|j = 0.

(6)

Let us introduce orthogonal basis |uj) obtained by, for instance, Gram-Schmidt process. For simplicity let us denote matrix of the operator A0 (inconclusive result) as A in this orthonormal basis, and operators |vk )(vk | as V (k) respectively.

Thus system of equations is as follows:

d N d

-v^Y^PkPk — ^ det A = 0, (7)

dPn j -, dPn

k = 1

det A = 0,

where A is Lagrange multiplier. Insofar as

^ det(A) = Tr ^adj(A) -L (V — £ Pk V (k)jj = Tr (— adj(A)V(n)) ,

(8)

where, Tr(X) = ^ Xu is trace of arbitrary matrix X, adj(A) is adjoint matrix of matrix A, I is identity matrix,

i

hence

Pn + A Tr(adj(A)V (n)) =0, (9)

det A = 0.

Since sum of pi is equal to unit than Lagrange multiplier is as follows:

A = - Tr (adj(A)£fc V), (10)

and consequently pj is expressed as

p = Tr (adj(A)V(j)) (11)

Pi Tr (adj(A)£k V(k)). (11)

One needs to derive Pi as function pi in order to obtain expression of optimal USD as function of pi.

400

A. A. Gaidash, S. S. Medvedeva, G. P. Miroshnichenko

3. Example

As an example let us consider two signal states. Their overlapping is denoted as B. Thus signal states can be

described in terms of orthonormal basis (obtained by Gram-Schmidt process) as follows:

( -B

l/i> = 1^1 , I/2) =

Vi - b2 VVT-B2,

Considering

|vi> =

i

-B

VVT-s2,

condition (6) may be derived in the following form:

det An = det

= det

1 0 0 1

1 - Pi BPi _VT—B2

1

-B

|v2> =

-B

VVT-B2,

Vi - B2 B2

P -

_vr—B2 1 - B2 _ BPi

V1 - B2 1 - b2 - B2Pi - P2

1 - B2

P2

1 - B2

1 - B2 - Pi - P2 + PiP2

1 - B2

thereby the probability Pi can be denoted as

Lagrange multiplier is as follows:

and probabilities p1 and p2 are as

Pi

i=

Pi

P2

1 - B2 - P2 1 - P2 '

1 - B2 (Pi + P2) - 2'

1 - P2

2 - (Pi + P2)' 1 - Pi

2 - (Pi + P2)"

By substituting expression (15) in expression (17) we find

(1 - P2)2

(1 - P2)2 + B2'

Pi =

and consequently:

P2 = 1 - B

Pi

1 - Pi

1 - B/Pi.

V P2

(12)

(13)

(14)

(15)

(16)

(17)

(18)

(19)

(20)

Taking into account symmetry of expressions (15), (17), (18) with respect to P1 and P2 following expression for P1 is derived analogously:

Pi = 1 - B/P1.

Pi

(21)

By substituting expressions (20) and (21) in (5) we obtain optimized USD probability:

P = Pi( 1 - B^p^ + P2 (1 - By^i) =1 - 2BVp^. (22)

This result has well-known form [11] if p = p1 = p2 = 1. Defining p1 = 1 + Ap and p2 = 1 - Ap, where Ap is considerably small deviation from equal a priori probabilities, we get

0

A

P = 1 - 2B

1 - B + 2B(Ap)2.

(23)

Therefore, the value of P has quadratic term dependent on small deviations from equal a priori probabilities. 4. Discussion and conclusion

In this work we analyze the probability of unambiguous discrimination for arbitrary number of states with unequal a priori probabilities. The proposed method provides system of equations (expressions (11) and (3)) that can be solved in order to find optimized USD probability as function of a priori probabilities. We consider rather simple and well-studied example for two states; the result is the same as in [20]. However, the authors of that paper obtain result only for two states. Concerning the method described in this paper it is unfortunate that the amount of calculations for higher number of states grows rapidly so it might be rather difficult to obtain analytical expressions similar to expression (22).

The results are important mostly in the field of quantum key distribution. In order to achieve certain level of security, one should consider various attacks, estimate probabilities of their success, and apply corresponding counter-measures to them. Thus estimation of optimal USD probability is crucial for bounding Eve's information during, for instance, advanced USD attack [6]. However consideration of an ideal case is not enough in this instance since there is an additional quadratic term related to slightly unequal (e.g. due to the bias in quantum random number generator) a priori probabilities in expression (23) that might provide additional information to Eve. Precise estimation of optimal USD probability is a significant step towards complete evaluation of quantum key distribution security.

Acknowledgements

This work was financially supported by the Ministry of Education and Science of Russian Federation (contract No. 03.G25.31.0229).

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References