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Kvantna prepletenost v nano sistemih (1) motivacija (2) definicija kvantne prepletenosti (3) statični in leteči kvantni biti (4) prepletenost na zahtevo (5) stabilnost in sesedenje prepletenosti: dvojne kvantne pike kubiti na mreži (kvantni) fazni prehodi (5) povzetek
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Entanglement: quantum phenomenon "When a distinguished but elderly scientist states that something is possible, he is almost certainly right. When he states that something is impossible, he is very probably wrong.“ Arthur C. Clarke
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Entanglement: quantum phenomenon
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Primer uporabe prepletenosti: teleportacija
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D. Bouwmeester et al. Experimental quantum teleportation. Nature, page 575, 1997. Y. Kim et al. Quantum teleportation of a polarization state with a complete bell state measurement. Physical Review Letters, page 1370, 2000. I. Marcikic et al. Long-distance teleportation of qubits at telecommunication wavelengths. Nature, page 509, 2003. R. Ursin et al. Quantum teleportation across the Danube. Nature, page 849, 2004. Primer uporabe prepletenosti: teleportacija
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R. Ursin et al., Nature 430, 849 (2004) Primer uporabe prepletenosti: teleportacija
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A B Ψ original Ψ teleportacija
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A B Ψ Ψ teleportacija
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A B Ψ kopija Ψ Ψ original Ψ “NI kvantnega kloniranja” teleportacija
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A B Meritev: kolaps (sesedenje?) stanja izvor parov EPR razdelitev skupnega para (singleta, npr.) Ψ Ψ naj bo teleportiran teleportacija
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A B izvor parov EPR razdelitev skupnega para (singleta, npr.) teleportacija klasično pošlji izid meritve deluj z unitarnim operatorjem Ψ se pojavi Ψ Meritev: sesedenje stanja
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2 3 teleportacija
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2 3 teleportacija
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1,2 3 teleportacija 1.zavrti okoli x 2.zavrti okoli z 3.počivaj 4.zavrti okoli y “Bellova meritev” ?
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1,2 3 teleportacija
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Quantifying entanglement: E A B two ‘spins’ in a pure state: Destillation of EPR pairs: Consider n such qubits pairs all in the state with E. Then by applying only local operations m singlet pairs can be extracted and E=m/n (for large n).
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Quantifying entanglement: pure states A B two ‘spins’ in a pure state: “1” (or “2”) is also a pure state Entanglement measure E=1 E=0
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A B Quantifying entanglement: mixed states special case: pure states
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Entanglement measure for two d e l o c a l i s e d electrons
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Example: Hubbard model (1D)
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Entanglement measure for two d e l o c a l i s e d electrons A. Ramšak, I. Sega, and J.H. Jefferson PRA 74, 010304(R) (2006)
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Concurrence: numerical examples A B References A. R., I. Sega, and J.H. Jefferson, Phys. Rev. A 74, 010304(R) (2006). A. R., J. Mravlje, R. Žitko, and J. Bonča, Phys. Rev. B 74, 241305(R) (2006). G. Giavaras, J.H. Jefferson, A. R., T.P. Spiller, and C. Lambert, Phys. Rev. B 74, 195341 (2006). J. Mravlje, A. R., and T. Rejec, Phys. Rev. B 73, 241305(R) (2006). D. Gunlycke, J.H. Jefferson, T. Rejec, A. R., D.G. Pettifor, and G.A.D. Briggs, J. Phys.: Condens. Matter 18, S851 (2006). J.H. Jefferson, A. R., and T. Rejec, Europhys. Lett. 75, 764 (2006). S. El Shawish, A. R., and J. Bonča, Phys. Rev. B 75, 205442 (2007). A. R. and J. Mravlje, cond-mat/0701363. M. Habgood, J.H. Jefferson, A. R., D.G. Pettifor, and G.A.D. Briggs, subm. to Phys. Rev. B
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Entanglement measure for two delocalized electrons
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infinite-U Anderson model
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Application: entanglement on demand
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+ Fullerene C 60, C 70, C 82, Sc@C 82, Ce@C 82, Nd@C 82 Sc 2 @C 80, Ce 2 @C 80, Er 3 N@C 80, Sc 3 N@C 80 Nanotubes (diameters 1.36nm and 1.49nm) Gas-Phase Nanotube Filling (300-500 o C): Reality …
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Application: entanglement on demand (I)
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Quasi 1D x
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x T. Rejec and Y. Meir, Nature 2006
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Application: entanglement on demand (I)
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Application: entanglement on demand (II)
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Chan et al, Nanotechnology 15, 609 (2004) Vidan et al, Applied Phys. Lett. 85, 3602 (2004) Electrostatic gates QD Elzerman et al, PRB 67, 16308 (2003) QD Realistic qubit pairs: double quantum dots
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Thermal equilibrium A-B entanglement
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Double quantum dots: entanglement versus the Kondo effect
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Double quantum dots
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Double quantum dot
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J. Mravlje, A. Ramšak, and T. Rejec, Phys. Rev. B 73, 241305(R) (2006)
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Double quantum dots
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spin-qubits charge-qubits
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Double quantum dots
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Zero magnetic field, thermal equilibrium A B
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A B
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A B
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A B see also:
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Zero magnetic field, thermal equilibrium A B see also:
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Double quantum dots: entanglement versus the Kondo effect
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Qubit arrays …
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A B Povzetek
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"Any sufficiently advanced technology is indistinguishable from magic." Arthur C. Clarke
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