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Asymmetric multipartite GHZ
 states and Bell inequalities
                 Darwin Gosal
              phydg@nus.edu.sg


        National University of Singapore
Talk Outline

  Generalized GHZ states
Talk Outline

  Generalized GHZ states
  Gisin’s theorem
Talk Outline

  Generalized GHZ states
  Gisin’s theorem
  Bell inequalities
Talk Outline

  Generalized GHZ states
  Gisin’s theorem
  Bell inequalities
  Numerical method
Talk Outline

  Generalized GHZ states
  Gisin’s theorem
  Bell inequalities
  Numerical method
  Discussion and conclusions
Generalized GHZ states

              1        1
        |ψ = √ |000 + √ |111
               2        2
Generalized GHZ states

                 1        1
           |ψ = √ |000 + √ |111
                  2        2


     |ψ = cos α|0, . . . , 0 + sin α|1, . . . , 1
Gisin’s Theorem

Any pure non-product state of two particles
violates the CHSH inequalities.
Physics Letters A 162, 15 (1992)
Gisin’s Theorem

Any pure non-product state of two particles
violates the CHSH inequalities.
Physics Letters A 162, 15 (1992)




Can Gisin’s theorem be generalized to
N-qubit states?
Bell inequalities

   Clauser-Horne-Shimony-Holt inequality
Bell inequalities

   Clauser-Horne-Shimony-Holt inequality
   Clauser-Horne inequality
Bell inequalities

   Clauser-Horne-Shimony-Holt inequality
   Clauser-Horne inequality
   Werner-Wolf-Zukowski-Brukner
   correlation-function
WZB correlation-functions

      1
 ρ =    3
          (1 + a · λ ⊗ I ⊗ I + I ⊗ b · λ ⊗ I + I ⊗ I ⊗ c · λ
     N
            (AB)                      (AC)
   +      Tkl λk ⊗ λl ⊗ I +        Tkl λk ⊗ I ⊗ λl
         k,l                            k,l

                (BC)                                (ABC)
    +          Tkl     I ⊗ λ k ⊗ λl +         k,l,m Tklm    λk ⊗ λ l ⊗ λ m
         k,l
WZB correlation-functions

      1
 ρ =    3
          (1 + a · λ ⊗ I ⊗ I + I ⊗ b · λ ⊗ I + I ⊗ I ⊗ c · λ
     N
            (AB)                      (AC)
   +      Tkl λk ⊗ λl ⊗ I +        Tkl λk ⊗ I ⊗ λl
         k,l                            k,l

                (BC)                                (ABC)
    +          Tkl     I ⊗ λ k ⊗ λl +         k,l,m Tklm    λk ⊗ λ l ⊗ λ m
         k,l
WZB correlation-functions

            sin 2α ≤ 2(1−N )/2
for odd N
WZB correlation-functions

                sin 2α ≤ 2(1−N )/2
for odd N



                               √
            F < 1 − 1/(sin(2α) 2N −1 )
2-particle correlations based on CHSH

All multi-particle entangled states violates local
realism provided post-selections are allowed
Popescu and Rohrlich PLA 166, 293 (1992)
2-particle correlations based on CHSH

All multi-particle entangled states violates local
realism provided post-selections are allowed
Popescu and Rohrlich PLA 166, 293 (1992)


                                   1
          Fthr   =1−               √
                     1 + sin2 (2α)( 2N −1−k − 1)
Numerical method

Using linear optimization method, we have
necessary and sufficient conditions for the
existance of a classical description of the given
correlations.
          ρ = (1 − F )|ψ ψ| + F ρnoise
Numerical method

Using linear optimization method, we have
necessary and sufficient conditions for the
existance of a classical description of the given
correlations.
          ρ = (1 − F )|ψ ψ| + F ρnoise


                            1
where the white noise is   2N I
Numerical method

Using linear optimization method, we have
necessary and sufficient conditions for the
existance of a classical description of the given
correlations.
               ρ = (1 − F )|ψ ψ| + F ρnoise


                                1
where the white noise is       2N I
PRL 85, 4418; PRA 66, 032103
Result (3-qubit GHZ state)

        0.5
         0.5
                   Numerical
                     WWZB
                     CHSH
        0.4
         0.4


        0.3
         0.3
    F
        0.2
         0.2


        0.1
         0.1


          0
          0
               0
               0           π/16
                             6    π/8
                                   12       3π/16
                                              18    π/4
                                                     24
                                        α
Conclusions

  WWZB inequalities cannot detect
  (N − k)-particle correlations
Conclusions

  WWZB inequalities cannot detect
  (N − k)-particle correlations
  CHSH inequalities is not equivalent with CH
  inequality for three qubits
Conclusions

  WWZB inequalities cannot detect
  (N − k)-particle correlations
  CHSH inequalities is not equivalent with CH
  inequality for three qubits
  Gisin’s theorem hold for odd number of qubit
  in the GHZ states
Questions ???

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Asymmetric multipartite GHZ states and Bell inequalities

  • 1. Asymmetric multipartite GHZ states and Bell inequalities Darwin Gosal phydg@nus.edu.sg National University of Singapore
  • 2. Talk Outline Generalized GHZ states
  • 3. Talk Outline Generalized GHZ states Gisin’s theorem
  • 4. Talk Outline Generalized GHZ states Gisin’s theorem Bell inequalities
  • 5. Talk Outline Generalized GHZ states Gisin’s theorem Bell inequalities Numerical method
  • 6. Talk Outline Generalized GHZ states Gisin’s theorem Bell inequalities Numerical method Discussion and conclusions
  • 7. Generalized GHZ states 1 1 |ψ = √ |000 + √ |111 2 2
  • 8. Generalized GHZ states 1 1 |ψ = √ |000 + √ |111 2 2 |ψ = cos α|0, . . . , 0 + sin α|1, . . . , 1
  • 9. Gisin’s Theorem Any pure non-product state of two particles violates the CHSH inequalities. Physics Letters A 162, 15 (1992)
  • 10. Gisin’s Theorem Any pure non-product state of two particles violates the CHSH inequalities. Physics Letters A 162, 15 (1992) Can Gisin’s theorem be generalized to N-qubit states?
  • 11. Bell inequalities Clauser-Horne-Shimony-Holt inequality
  • 12. Bell inequalities Clauser-Horne-Shimony-Holt inequality Clauser-Horne inequality
  • 13. Bell inequalities Clauser-Horne-Shimony-Holt inequality Clauser-Horne inequality Werner-Wolf-Zukowski-Brukner correlation-function
  • 14. WZB correlation-functions 1 ρ = 3 (1 + a · λ ⊗ I ⊗ I + I ⊗ b · λ ⊗ I + I ⊗ I ⊗ c · λ N (AB) (AC) + Tkl λk ⊗ λl ⊗ I + Tkl λk ⊗ I ⊗ λl k,l k,l (BC) (ABC) + Tkl I ⊗ λ k ⊗ λl + k,l,m Tklm λk ⊗ λ l ⊗ λ m k,l
  • 15. WZB correlation-functions 1 ρ = 3 (1 + a · λ ⊗ I ⊗ I + I ⊗ b · λ ⊗ I + I ⊗ I ⊗ c · λ N (AB) (AC) + Tkl λk ⊗ λl ⊗ I + Tkl λk ⊗ I ⊗ λl k,l k,l (BC) (ABC) + Tkl I ⊗ λ k ⊗ λl + k,l,m Tklm λk ⊗ λ l ⊗ λ m k,l
  • 16. WZB correlation-functions sin 2α ≤ 2(1−N )/2 for odd N
  • 17. WZB correlation-functions sin 2α ≤ 2(1−N )/2 for odd N √ F < 1 − 1/(sin(2α) 2N −1 )
  • 18. 2-particle correlations based on CHSH All multi-particle entangled states violates local realism provided post-selections are allowed Popescu and Rohrlich PLA 166, 293 (1992)
  • 19. 2-particle correlations based on CHSH All multi-particle entangled states violates local realism provided post-selections are allowed Popescu and Rohrlich PLA 166, 293 (1992) 1 Fthr =1− √ 1 + sin2 (2α)( 2N −1−k − 1)
  • 20. Numerical method Using linear optimization method, we have necessary and sufficient conditions for the existance of a classical description of the given correlations. ρ = (1 − F )|ψ ψ| + F ρnoise
  • 21. Numerical method Using linear optimization method, we have necessary and sufficient conditions for the existance of a classical description of the given correlations. ρ = (1 − F )|ψ ψ| + F ρnoise 1 where the white noise is 2N I
  • 22. Numerical method Using linear optimization method, we have necessary and sufficient conditions for the existance of a classical description of the given correlations. ρ = (1 − F )|ψ ψ| + F ρnoise 1 where the white noise is 2N I PRL 85, 4418; PRA 66, 032103
  • 23. Result (3-qubit GHZ state) 0.5 0.5 Numerical WWZB CHSH 0.4 0.4 0.3 0.3 F 0.2 0.2 0.1 0.1 0 0 0 0 π/16 6 π/8 12 3π/16 18 π/4 24 α
  • 24. Conclusions WWZB inequalities cannot detect (N − k)-particle correlations
  • 25. Conclusions WWZB inequalities cannot detect (N − k)-particle correlations CHSH inequalities is not equivalent with CH inequality for three qubits
  • 26. Conclusions WWZB inequalities cannot detect (N − k)-particle correlations CHSH inequalities is not equivalent with CH inequality for three qubits Gisin’s theorem hold for odd number of qubit in the GHZ states