• Photonics Research
  • Vol. 12, Issue 3, 552 (2024)
Qian-Xi Zhang1, Xiao-Xu Fang1, and He Lu1、2、*
Author Affiliations
  • 1School of Physics, State Key Laboratory of Crystal Materials, Shandong University, Jinan 250100, China
  • 2Shenzhen Research Institute of Shandong University, Shenzhen 518057, China
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    DOI: 10.1364/PRJ.506855 Cite this Article Set citation alerts
    Qian-Xi Zhang, Xiao-Xu Fang, He Lu. Experimental distillation of tripartite quantum steering with an optimal local filtering operation[J]. Photonics Research, 2024, 12(3): 552 Copy Citation Text show less

    Abstract

    Multipartite Einstein-Podolsky-Rosen (EPR) steering admits multipartite entanglement in the presence of uncharacterized verifiers, enabling practical applications in semi-device-independent protocols. Such applications generally require stronger steerability, while the unavoidable noise weakens steerability and consequently degrades the performance of quantum information processing. Here, we propose the local filtering operation that can maximally distill genuine tripartite EPR steering from N copies of three-qubit generalized Greenberger-Horne-Zeilinger states, in the context of two semi-device-independent scenarios. The optimal filtering operation is determined by the maximization of assemblage fidelity. Analytical and numerical results indicate the advantage of the proposed filtering operation when N is finite and the steerability of initial assemblages is weak. Experimentally, a proof-of-principle demonstration of two-copy distillation is realized with the optical system. The advantage of the optimal local filtering operation is confirmed by the distilled assemblage in terms of higher assemblage fidelity with perfectly genuine tripartite steerable assemblages, as well as the greater violation of the inequality to witness genuine tripartite steerable assemblages. Our results benefit the distillation of multipartite EPR steering in practice, where the number of copies of initial assemblages is generally finite.
    σa|xBC=TrA(Ma|x1B1CρABC).

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    σab|xyC=TrAB(Ma|xMb|y1CρABC).

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    S1sDI=1+0.1547ZBZC13(A2ZB+A2ZC+A0XBXCA0YBYCA1XBYCA1YBXC)0,

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    S2sDI=10.1831(A2B2+A2ZC+B2ZC)0.2582(A0B0XCA0B1YCA1B0YCA1B1XC)0,

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    |GGHZ3=cosθ|000+sinθ|111,0θπ4.

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    σ0|0BC=12|θ+0θ+0|,σ1|0BC=12|θ0θ0|,σ0|1BC=12|θ1θ1|,σ1|1BC=12|θ+1θ+1|,σ0|2BC=cos2θ|0000|,σ1|2BC=sin2θ|1111|,

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    Psucc=Tr[(1CF(κ))ρBC(1CF(κ))]=κ2cos2θ+sin2θ,

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    σ˜a|xBC=1Psucc[1CF(κ)]σa|xBC[1CF(κ)].

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    Σa|xdist,N=Psucc1sDI,NΣ˜a|x+Pfail1sDI,NΣa|xGGHZ.

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    F1sDI(Σa|xdist,N,Σa|xGHZ)=minxaf(σa|xdist,N,σa|xGHZ),

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    maximizeF1sDI(Σa|xdist,N,Σa|xGHZ)subject to0κ1.

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    Σa|xdist,2=PsuccΣ˜a|x+(1Psucc)Σa|xGGHZ=(κ2cos2θ+sin2θ)Σ˜a|x+(1κ2)cos2θΣa|xGGHZ.

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    F1sDI(Σa|xdist,2,Σa|xGHZ)=minxaf(σa|xdist,σa|xGHZ)=a=0,1f(σa|0dist,σa|0GHZ)=12+cosθsinθ(cos2θκ2cos2θ+κ)12+cosθsinθ(cos2θ+14cos2θ).

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    CF(κ)=12cos2θ|00|+|11|

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    F1sDIκ=12+cosθsinθ(cos2θ+14cos2θ).

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    F1sDIκ=112(1sin2θ)cos2θ.

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    |GGHZ3=cosθ|HhHABC+sinθ|VvVABC,

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    σ0|0dist=Psuccσ˜0|0+Pfailσ0|0GGHZ=12(κ2cos2θ00κcosθsinθ00000000κcosθsinθ00sin2θ)+(1κ2)cos2θ2(cos2θ00cosθsinθ00000000cosθsinθ00sin2θ)=12(κ2cos2θsin2θ+cos4θ00cosθsinθ(κ+cos2θκ2cos2θ)00000000cosθsinθ(κ+cos2θκ2cos2θ)00sin2θ(1+cos2θκ2cos2θ)),(A1)

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    σ1|0dist=Psuccσ˜1|0+Pfailσ1|0GGHZ=12(κ2cos2θ00κcosθsinθ00000000κcosθsinθ00sin2θ)+(1κ2)cos2θ2(cos2θ00cosθsinθ00000000cosθsinθ00sin2θ)=12(κ2cos2θsin2θ+cos4θ00cosθsinθ(κ+cos2θκ2cos2θ)00000000cosθsinθ(κ+cos2θκ2cos2θ)00sin2θ(1+cos2θκ2cos2θ)),(A2)

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    σ0|1dist=Psuccσ˜0|1+Pfailσ0|1GGHZ=12(κ2cos2θ00iκcosθsinθ00000000iκcosθsinθ00sin2θ)+(1κ2)cos2θ2(cos2θ00icosθsinθ00000000icosθsinθ00sin2θ)=12(κ2cos2θsin2θ+cos4θ00icosθsinθ(κ+cos2θκ2cos2θ)00000000icosθsinθ(κ+cos2θκ2cos2θ)00sin2θ(1+cos2θκ2cos2θ)),(A3)

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    σ1|1dist=Psuccσ˜1|1+Pfailσ1|1GGHZ=12(κ2cos2θ00iκcosθsinθ00000000iκcosθsinθ00sin2θ)+(1κ2)cos2θ2(cos2θ00icosθsinθ00000000icosθsinθ00sin2θ)=12(κ2cos2θsin2θ+cos4θ00icosθsinθ(κ+cos2θκ2cos2θ)00000000icosθsinθ(κ+cos2θκ2cos2θ)00sin2θ(1+cos2θκ2cos2θ)),(A4)

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    σ0|2dist=Psuccσ˜0|2+Pfailσ0|2GGHZ=(κ2cos2θ000000000000000)+(1κ2)cos2θ(cos2θ000000000000000)=(κ2cos2θsin2θ+cos4θ000000000000000),(A5)

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    σ1|2dist=Psuccσ˜1|2+Pfailσ1|2GGHZ=(000000000000000sin2θ)+(1κ2)cos2θ(000000000000000sin2θ)=(000000000000000sin2θ(1+cos2θκ2cos2θ)).(A6)

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    a=0,1f(σa|0dist,σa|0GHZ)=a=0,1f(σa|1dist,σa|1GHZ)=12+cosθsinθ(cos2θκ2cos2θ+κ),a=0,1f(σa|2dist,σa|2GHZ)=κ2cos2θsin2θ+cos4θ2+sin2θ(1+cos2θκ2cos2θ)2.(A7)

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    [a=0,1f(σa|0dist,σa|0GHZ)]2[a=0,1f(σa|2dist,σa|2GHZ)]2=cosθsinθ[(1κ2)cos2θ+κ(1κ2)2cos4θ+(1+κ2)(1κ2)cos2θ+κ2]cosθsinθ[(1κ2)cos2θ+κ(1κ2)2cos4θ+2κ(1κ2)cos2θ+κ2]=0,(A8)

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    F1sDI=12+cosθsinθ(cos2θκ2cos2θ+κ)12+cosθsinθ(cos2θ+14cos2θ),(A9)

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    σ00|00C=σ11|00C=σ01|11C=σ10|11C=14|θ+2θ+2|,σ01|00C=σ10|00C=σ00|11C=σ11|11C=14|θ2θ2|,σ00|01C=σ11|01C=σ00|10C=σ11|10C=14|θ3θ3|,σ01|01C=σ10|01C=σ01|10C=σ10|10C=14|θ+3θ+3|,σ00|02C=σ10|02C=σ00|12C=σ10|12C=σ00|20C=σ01|20C=σ00|21C=σ01|21C=cos2θ2|00|,σ01|02C=σ11|02C=σ01|12C=σ11|12C=σ10|20C=σ11|20C=σ10|21C=σ11|21C=sin2θ2|11|,σ00|22C=cos2θ|00|,σ11|22C=sin2θ|11|,(B1)

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    σ00|00dist=σ11|00dist=σ01|11dist=σ10|11dist=Psuccσ˜00|00+Pfailσ00|00GGHZ=14(κ2cos2θκcosθsinθκcosθsinθsin2θ)+(1κ2)cos2θ4(cos2θcosθsinθcosθsinθsin2θ)=14(κ2cos2θsin2θ+cos4θcosθsinθ(κ+cos2θκ2cos2θ)cosθsinθ(κ+cos2θκ2cos2θ)sin2θ(1+cos2θκ2cos2θ)),(B2)

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    σ01|00dist=σ10|00dist=σ00|11dist=σ11|11dist=Psuccσ˜01|00+Pfailσ01|00GGHZ=14(κ2cos2θκcosθsinθκcosθsinθsin2θ)+(1κ2)cos2θ4(cos2θcosθsinθcosθsinθsin2θ)=14(κ2cos2θsin2θ+cos4θcosθsinθ(κ+cos2θκ2cos2θ)cosθsinθ(κ+cos2θκ2cos2θ)sin2θ(1+cos2θκ2cos2θ)),(B3)

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    σ00|01dist=σ11|01dist=σ00|10dist=σ11|10dist=Psuccσ˜00|01+Pfailσ00|01GGHZ=14(κ2cos2θiκcosθsinθiκcosθsinθsin2θ)+(1κ2)cos2θ4(cos2θicosθsinθicosθsinθsin2θ)=14(κ2cos2θsin2θ+cos4θicosθsinθ(κ+cos2θκ2cos2θ)icosθsinθ(κ+cos2θκ2cos2θ)sin2θ(1+cos2θκ2cos2θ)),(B4)

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    σ01|01dist=σ10|01dist=σ01|10dist=σ10|10dist=Psuccσ˜01|01+Pfailσ01|01GGHZ=14(κ2cos2θiκcosθsinθiκcosθsinθsin2θ)+(1κ2)cos2θ4(cos2θicosθsinθicosθsinθsin2θ)=14(κ2cos2θsin2θ+cos4θicosθsinθ(κ+cos2θκ2cos2θ)icosθsinθ(κ+cos2θκ2cos2θ)sin2θ(1+cos2θκ2cos2θ)),(B5)

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    σ00|02dist=σ10|02dist=σ00|12dist=σ10|12dist=σ00|20dist=σ01|20dist=σ00|21dist=σ01|21dist=Psuccσ˜00|02+Pfailσ00|02GGHZ=12(κ2cos2θ000)+(1κ2)cos2θ2(cos2θ000)=12(κ2cos2θsin2θ+cos4θ000),(B6)

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    σ01|02dist=σ11|02dist=σ01|12dist=σ11|12dist=σ10|20dist=σ11|20dist=σ10|21dist=σ11|21dist=12(000sin2θ)+(1κ2)cos2θ2(000sin2θ)=12(000sin2θ(1+cos2θκ2cos2θ)),(B7)

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    σ00|22dist=(κ2cos2θsin2θ+cos4θ000),σ11|22dist=(000sin2θ(1+cos2θκ2cos2θ)).(B8)

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    a,b{0,1}f(σab|xydist,σab|xyGHZ)={12+cosθsinθ(cos2θκ2cos2θ+κ)x2  and  y2κ2cos2θsin2θ+cos4θ2+sin2θ(1+cos2θκ2cos2θ)2x=2  or  y=2,(B9)

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    [a,b{0,1}f(σab|xydist,σab|xyGHZ)]2[a,b{0,1}f(σab|22dist,σab|22GHZ)]2=cosθsinθ[(1κ2)cos2θ+κ(1κ2)2cos4θ+(1+κ2)(1κ2)cos2θ+κ2]cosθsinθ[(1κ2)cos2θ+κ(1κ2)2cos4θ+2κ(1κ2)cos2θ+κ2]=0.(B10)

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    F2sDI=minx,ya,b{0,1}f(σab|xydist,σab|xyGHZ)=12+cosθsinθ(cos2θκ2cos2θ+κ)12+cosθsinθ(cos2θ+14cos2θ),(B11)

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    Psucc=Tr[CF(κ)ρCCF(κ)]=(κ)2cos2θ+sin2θ,(C1)

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    σ˜ab|xyC=1PsuccCF(κ)σab|xyCCF(κ).(C2)

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    a,bf(σ˜ab|xy,σab|xyGHZ)=12(1+2κsinθcosθ(κ)2cos2θ+sin2θ)x,y(C3)

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    F2sDI(Σ˜ab|xy,Σab|xyGHZ)=12(1+2κsinθcosθ(κ)2cos2θ+sin2θ)1.(C4)

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    CF(κ)=tanθ|00|+|11|.(C5)

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    Qian-Xi Zhang, Xiao-Xu Fang, He Lu. Experimental distillation of tripartite quantum steering with an optimal local filtering operation[J]. Photonics Research, 2024, 12(3): 552
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