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Q UANTUM C OMMUNICATION P ART 2 Aditi Harish-Chandra Research Institute, India
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O UTLINE Communication Secure Communication Quantum Cryptography Communication Without security Classical info transmission Classical info transmission Quantum state transmission
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DC C APACITY : K NOWN /U NKNOWN Single Sender – Single Receiver Many Senders – Single Receiver Solved
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Dense Coding Network 3
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D ISTRIBUTED DC: T WO RECEIVERS Alice (A 1 ) Alice (A 2 ) Bob (B 1 ) Bob (B 2 )
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D ISTRIBUTED DC: T WO RECEIVERS Alice (A 1 ) Alice (A 2 ) Bob (B 1 ) Bob (B 2 ) LOCC i1i1 i2i2
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D ISTRIBUTED DC: T WO RECEIVERS Alice (A 1 ) Alice (A 2 ) Bob (B 1 ) Bob (B 2 )
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D ISTRIBUTED DC: T WO RECEIVERS Alice (A 1 ) Alice (A 2 ) Bob (B 1 ) Bob (B 2 ) Alices send her particles to Bobs
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D ISTRIBUTED DC: T WO RECEIVERS Bob (B 1 ) Bob (B 2 ) Bobs task: gather info abt i k by LOCC
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D ISTRIBUTED DC: T WO RECEIVERS Bob (B 1 ) Bob (B 2 ) Bobs task: gather info abt i k by LOCC LOCC
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C = Max D ISTRIBUTED DC: T WO RECEIVERS
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C = Max Max LOCC Holevo bound Maximization over all encodings i.e. over all {p i, U i } D ISTRIBUTED DC: T WO RECEIVERS
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C = Max Max LOCC Holevo bound Maximization over all encodings i.e. over all {p i, U i } Badziag, Horodecki, ASD, Sen, PRL’03 D ISTRIBUTED DC: T WO RECEIVERS
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C = Max Max LOCC Holevo bound Maximization over all encodings i.e. over all {p i, U i } Bruss, D’Ariano, Lewenstein, Macchiavello, ASD, Sen, PRL’ 04 D ISTRIBUTED DC: T WO RECEIVERS
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DC C APACITY : K NOWN /U NKNOWN Single Sender – Single Receiver Many Senders – Single Receiver Solved
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DC C APACITY : K NOWN /U NKNOWN Single Sender – Single Receiver Many Senders – Single Receiver Solved Many Senders – Two Receivers
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DC C APACITY : K NOWN /U NKNOWN Single Sender – Single Receiver Many Senders – Single Receiver Solved Many Senders – Two Receivers Partially Solved
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DC C APACITY : K NOWN /U NKNOWN Single Sender – Single Receiver Many Senders – Single Receiver Solved Many Senders – Two Receivers Partially Solved Many Senders – Many Receivers Not Solved
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O UTLINE Communication Secure Communication Quantum Cryptography Communication Without security Classical info transmission Classical info transmission Quantum state transmission
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Quantum Dense Coding Task: Classical info transmission Quantum Dense Coding Task: Classical info transmission Quantum Dense Coding
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Task: Classical info transmission Medium: Quantum State Quantum Dense Coding Task: Classical info transmission Medium: Quantum State Quantum Dense Coding
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Task: Classical info transmission Medium: Quantum State Quantum Dense Coding Task: Classical info transmission Medium: Quantum State Task: quantum state/info transmission Task: quantum state/info transmission Task: Quantum state/info transmission Task: Quantum state/info transmission Quantum Dense Coding
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Task: Classical info transmission Medium: Quantum State Quantum Dense Coding Task: Classical info transmission Medium: Quantum State Task: Quantum state/info transmission Medium: Quantum State Task: Quantum state/info transmission Medium: Quantum State Quantum Dense Coding
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Task: Classical info transmission Medium: Quantum State Task: Classical info transmission Medium: Quantum State Task: Quantum state/info transmission Medium: Quantum State Task: Quantum state/info transmission Medium: Quantum State Quantum Dense Coding Quantum Teleportation
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Bennett, Brassard, Crepeau, Jozsa, Peres, Wootters, PRL 1993
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Q UANTUM T ELEPORTATION Task: Sending arbitrary quantum state
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Q UANTUM T ELEPORTATION Task: Sending
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Q UANTUM T ELEPORTATION Task: Sending
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Q UANTUM T ELEPORTATION Task: Sending Classical: Infinite communication
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Q UANTUM T ELEPORTATION Task: Sending Classical: Infinite communication
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Q UANTUM T ELEPORTATION A in B Alice Bob
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Q UANTUM T ELEPORTATION A in B Alice Bob Alice performs measurements on “in’’ and A
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Q UANTUM T ELEPORTATION A in B Alice Bob After measurement
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Q UANTUM T ELEPORTATION A in B Alice Bob After measurement 2 bits of classical comm. sent by Alice to Bob
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Q UANTUM T ELEPORTATION A in B Alice Bob After measurement Bob performs unitary
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Q UANTUM T ELEPORTATION A in B Alice Bob After measurement State is with Bob
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M ORAL Classical Quantum Vs. Task: sending arbitrary quantum state Infinite classical comm 2 bits of classical comm
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M ORAL Classical Quantum Task: sending arbitrary quantum state Infinite classical comm 2 bits of classical comm Vs.
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I S IT MAGIC ?
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Of course not!
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I S IT MAGIC ? Ingredient: Quantum Mechanics
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I S IT MAGIC ? Entangled states
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W HAT IS ENTANGLEMENT ? Unentangled/Useless states : Entangled/Useful states :
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W HAT IS ENTANGLEMENT ? Unentangled/Useless states : Entangled/Useful states :
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W HAT IS ENTANGLEMENT ? Unentangled/Useless states : Entangled/Useful states :
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Is it just theory ?
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Experiments
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P HOTONS
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143 Km Teleportation
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~100KM
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E NTANGLEMENT S WAPPING Zukowski, Zeilinge, Horne, Ekert, PRL 71, 4287 (’93)
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E NTANGLEMENT S WAPPING Zukowski, Zeilinge, Horne, Ekert, PRL 71, 4287 (’93)
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P HOTONS Photons
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P HOTONS Photons
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IONS
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IONS 14 ions entangled
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ION E NTANGLED S TATES Phys. Rep. 2008
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Quantum Teleportation between Light and Matter
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Quantum Teleportation between Light and Matter
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Quantum Teleportation between Light and Matter Polzik’s group, Nature 443, 557 (’06)
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Quantum Teleportation between Light and Matter Polzik’s group, Nature 443, 557 (’06)
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IONS: T ELEPORTATION
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NMR Entangled states in NMR
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T ELEPORTATION BY NMR
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Nielsen, Knill, Laflamme, Nature 395 (’98)
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O PTICAL L ATTICES
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Entangled states in Optical lattices
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O PTICAL L ATTICES Entangled states in Optical lattices
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O PTICAL L ATTICES Resonating valence bond states in Optical lattices
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T ELEPORTATION : N EUTRAL A TOMS Wu, Yang, Shen, Zheng, J. Phys. B: At. Mol. Opt. Phys. 46, 185502 (’13)
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T ELEPORTATION : S PIN CHAIN 1. Initially the spin chain is in the ground state:
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T ELEPORTATION : S PIN CHAIN 1. Initially the spin chain is in the ground state: 2. Alice places an arbitrary state at her end:
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T ELEPORTATION : S PIN CHAIN 1. Initially the spin chain is in the ground state: 2. Alice places an arbitrary state at her end: 3. The state evolves according to some Hamiltonian:
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T ELEPORTATION : S PIN CHAIN 1. Initially the spin chain is in the ground state: 2. Alice places an arbitrary state at her end: 3. The state evolves according to some Hamiltonian: 4. Bob receives the state after some time. Bose, PRL(’03), Subrahmanyam, PRA (’03)
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Many other systems …….
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Teleportation for arbitrary states
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AB Alice & Bob share a state
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AB
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A in B Task: To send to Bob single copy of is available CdCd
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A in B Allowed operations: LOCC
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A in B Not allowed operations: exchange qubits
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A in B Alice & Bob perform some LOCC, T,
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A in B Alice & Bob perform some LOCC, T, and create at Bob’s side
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A in B Alice & Bob perform some LOCC, T, and create at Bob’s side Check its closeness with
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A in B Quantify closeness: integration over all inputs Teleportation fidelity
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Singlet Fraction: : max singlet fraction from by LOCC Bennett, Divincenzo, Smolin, Wootters, PRA 54, 3824 (’97) MPR Horodeccy, PRA 60, 1888 (’99) M.A. Nielsen, quant-ph/0205035
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Singlet Fraction: : max singlet fraction from by LOCC Horodeccy, PRA 60, 1888 (’99) Nielsen, arXiv: 0205035 Verstreate, Verschele, PRL 90, 097901 (’03)
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Popescu, PRL 72, 797 (’94) Alice & Bob share separable state, then f max =2/3
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T ELE C APACITY : K NOWN /U NKNOWN Single Sender – Single Receiver d d Solved
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Teleportation Network 1
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T ELEPORTATION : M ONOGAMY Alice Debu Charu Nitu........ Bob SendersReceiver
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T ELEPORTATION : M ONOGAMY Alice Debu Charu Nitu........ Bob SendersReceiver Teleportation monogamy Faithful teleportation cannot be freely performed
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T ELEPORTATION : M ONOGAMY Tele mono ineq: Lee and Park, PRA 79, 054309(’09)
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T ELEPORTATION : M ONOGAMY Holds for pure states: Lee and Park, PRA 79, 054309(’09)
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T ELEPORTATION : M ONOGAMY Holds for pure states: Lee and Park, PRA 79, 054309(’09) Follows from monogamy of concurrence squared in 2 d
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T ELEPORTATION : M ONOGAMY Does Not hold for mixed states: Lee and Park, PRA 79, 054309(’09)
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Teleportation Network 2
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T ELEPORTATION N ETWORK Alice (A 1 ) Alice (A 2 ) Bob (B 1 ) Bob (B 2 ) ASD, U. Sen, PRA 81, 012308 (’01)
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T ELEPORTATION N ETWORK Alice (A 1 ) Alice (A 2 ) Bob (B 1 ) Bob (B 2 ) ASD, U. Sen, PRA 81, 012308 (’01)
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T ELEPORTATION N ETWORK Alice (A 1 ) Alice (A 2 ) Bob (B 1 ) Bob (B 2 ) ASD, U. Sen, PRA 81, 012308 (’01) Establish relation between capacity & entanglement
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T ELE C APACITY : K NOWN /U NKNOWN Single Sender – Single Receiver d d Solved
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T ELE C APACITY : K NOWN /U NKNOWN Single Sender – Single Receiver d d Solved Many Senders – single Receiver Not Solved
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T ELE C APACITY : K NOWN /U NKNOWN Single Sender – Single Receiver d d Solved Many Senders – single Receiver Not Solved Many Senders – many Receiver Not Solved
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Single Sender – Single Receiver Many Senders – Single Receiver Solved Many Senders – Two Receivers Many Senders – Many Receivers Partially Solved Not Solved Classical info transmit known/Unknown known/Unknown Quantum info transmission Single Sender – Single Receiver d d Solved Many Senders – Single Receiver Not Solved Many Senders – Many Receivers Not Solved
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QIC@HRI
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