[Quantum Information] Quantum teleportation
Quantum teleportation
Notes from RWTH Aachen University course
“Quantum Information” Summer semester 2020
professor: Müller, Markus
Quantum teleportation
Protocol
The Bell state shared by A and B is available
- A:1/√2(|0A0B⟩+|1A1B⟩)
- B:1/√2(|0A0B⟩+|1A1B⟩)
A interacts her qubit with the (unknown) state |ψ⟩
- assume that |ψ⟩=α|0⟩+β|1⟩
A:(α|0⟩+β|1⟩)(1/√2(|0A0B⟩+|1A1B⟩))C1NOTA→1/√2[α|0⟩(|0A0B⟩+|1A1B⟩)+β|1⟩(|0A1B⟩+|1A0B⟩)]H1→1/2[α(|0⟩+|1⟩)(|0A0B⟩+|1A1B⟩)+β(|0⟩−|1⟩)(|0A1B⟩+|1A0B⟩)]=|00A⟩[1/2(α|0B⟩+β|1B⟩)]+|01A⟩[1/2(α|1B⟩+β|0B⟩)]+|10A⟩[1/2(α|0B⟩−β|1B⟩)]+|11A⟩[1/2(α|1B⟩−β|0B⟩)]
A measures the qubits in her procession
A sends the information of measurement outcome via a classical channel
Depending on A's message, B applies operations to his qubit and recover |ψ⟩
A's outcome B's state B's operation |00A⟩ α|0⟩+β|1⟩ |01A⟩ α|1⟩+β|0⟩ X |10A⟩ α|0⟩−β|1⟩ Z |11A⟩ α|1⟩−β|0⟩ X,Z
Discussion
- Does it allow fast-than-light communication?
- No, A needs to send the outcome information via classical channel (limited by the spped of light).
- Does the protocol violate the no-cloning theorem?
- No, at the end of the protocol, only the B's qubit is in the state |ψ⟩
No information of |ψ⟩ is left on A's qubit (only the four basis states.)
- No, at the end of the protocol, only the B's qubit is in the state |ψ⟩
- Importance of quantum teleportation:
- fundamental property of quantum mechanics
- used e.g. in QEC
- measuremnt-based quantum computing
- distribution of quantum information in quantum networks
Readings
Bennett, Charles & Brassard, Gilles & Crépeau, Claude & Jozsa, Richard & Peres, Asher & Wootters, William. (1993). Teleporting an unknown quantum state via dual classical and Einstein-Podolsky-Rosen channels. Physical review letters. 70. 1895-1899. 10.1103/PhysRevLett.70.1895.
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