nt - p h / 06 02 08 9 v 1 10 F eb 2 00 6 Relation between concurrence and Berry phase of an entangled state of two spin 1 / 2 particles

نویسنده

  • Banasri Basu
چکیده

In the last few years Berry phase in a single particle system has been studied very well, both theoretically and experimentally. However, the study of Berry phase in an entangled state has become a topic of interest very recently [1, 2, 3, 4, 5]. As entanglement is a striking feature of quantum systems and is a useful resource to realize quantum information, quantum teleportation, quantum cryptography or quantum computation, the study of entangled state has absorbed much attention. We have to be careful about two aspects of Berry phase of an entangled state. One is how it changes due to interparticle interaction [1, 2, 3] and the other is how it affects [4] the biparticle states. The motivation of this letter is to see the effect of the Berry phase on an entangled system of two spin-1/2 particles. As a result we have also found a connection between it and the concurrence (which is the measure of of entanglement) for different spin chains. It is well known that a fermion which is a spin 1/2 particle can be realized when a scalar particle is attached with a magnetic flux quantum. The attachment of the magnetic flux quantum changes the spin and statistics of the scalar particle. The effect of the flux quantum is to induce an appropriate AharanovBohm phase which simulates the statistical phase factor. For one complete rotation the wave function of a fermion acquires an extra geometric phase known as Berry phase besides the dynamical phase. The attachment of magnetic flux quantum to a scalar particle is also equivalent to the motion of a charged particle in the field of a magnetic monopole of strength 2b where b is a half integer or integer. The angular momentum of the particle can be written as

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

منابع مشابه

ar X iv : q ua nt - p h / 01 01 10 6 v 2 4 F eb 2 00 1 Entanglement and Dynamic Stability of Nash Equilibrium in a Symmetric Quantum Game

We present an example of a symmetric quantum game for which a dynamically stable Nash equilibrium becomes unstable when the initial state used to play the quantum game is changed to 'entangled' from 'unentan-gled'. The game is played between two players via the proposed scheme of applying 'identity' and 'Pauli spin flip' operators on the initial state with classical probabilities.

متن کامل

nt - p h / 01 02 03 8 v 1 6 F eb 2 00 1 Quasiprobability and Probability Distributions for Spin 1 / 2 States ∗

We develop a Radon like transformation, in which P quasiprobability distribution for spin 1/2 states is written in terms of the tomographic probability distribution w.

متن کامل

nt - p h / 02 04 01 9 v 1 4 A pr 2 00 2 Squeezing of a coupled state of two spinors

The notion of spin squeezing involves reduction in the uncertainty of a component of the spin vector S below a certain limit. This aspect has been studied earlier [1, 2] for pure and mixed states of definite spin. In this paper, this study has been extended to coupled spin states which do not possess sharp spin value. A general squeezing criterion has been obtained by requiring that a direct pr...

متن کامل

ua nt - p h / 01 02 04 0 v 1 7 F eb 2 00 1 Universal state inversion and concurrence in arbitrary dimensions

Wootters [Phys. Rev. Lett. 80, 2245 (1998)] has given an explicit formula for the entanglement of formation of two qubits in terms of what he calls the concurrence of the joint density operator. Wootters’s concurrence is defined with the help of the superoperator that flips the spin of a qubit. We generalize the spin-flip superoperator to a “universal inverter,” which acts on quantum systems of...

متن کامل

ua nt - p h / 05 08 04 6 v 1 5 A ug 2 00 5 Proper Time for Spin 1 / 2 Particles

We find a quantum mechanical formulation of proper time for spin 1/2 particles within the framework of the Dirac theory. It is shown that the rate of proper time can be represented by an operator called the “tempo operator”, and that the proper time itself be given by the integral of the expectation value of the operator. The tempo operator has some terms involving the Pauli spin matrices, and ...

متن کامل

ذخیره در منابع من


  با ذخیره ی این منبع در منابع من، دسترسی به آن را برای استفاده های بعدی آسان تر کنید

برای دانلود متن کامل این مقاله و بیش از 32 میلیون مقاله دیگر ابتدا ثبت نام کنید

ثبت نام

اگر عضو سایت هستید لطفا وارد حساب کاربری خود شوید

عنوان ژورنال:

دوره   شماره 

صفحات  -

تاریخ انتشار 2006