Quantum Teleportation
Quantum teleportation is a protocol that transfers an unknown quantum state from one qubit to another using shared entanglement and classical communication, without physically transmitting the qubit.
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What it means
Quantum teleportation, proposed by Bennett et al.in 1993, allows Alice to transfer an unknown quantum state |ψ⟩ to Bob using a pre-shared Bell pair and two classical bits of communication.The protocol consists of three steps: (1) Alice performs a Bell measurement on her unknown qubit and her half of the entangled pair, (2) she sends the two-bit measurement result to Bob via a classical channel, and (3) Bob applies the corresponding Pauli correction (I, X, Z, or XZ) to his half of the entangled pair, recovering the original state |ψ⟩.Crucially, the original state at Alice's location is destroyed in the process (satisfying no-cloning), and the quantum information cannot travel faster than light because the classical bits are required.Everyday analogy
Common misconceptions
- Quantum teleportation does NOT allow faster-than-light communication — classical communication is required to complete the protocol, which is limited to the speed of light.
- Quantum teleportation does NOT transport matter or energy — it transfers only the quantum state (information) from one qubit to another.
Key takeaways
- Quantum teleportation requires a shared entangled pair and two classical bits of communication.
- The original state is destroyed during teleportation, consistent with the no-cloning theorem.
- Teleportation is a key primitive in quantum networking, quantum error correction, and measurement-based quantum computing.
Check your understanding
How many classical bits must Alice send to Bob to complete quantum teleportation of one qubit?
- A.0
- B.1
- C.2
- D.3
Show the answer
Answer: C. 2
Why: Alice must send 2 classical bits encoding her Bell measurement result, which Bob uses to apply the correct Pauli correction to his qubit.
Builds on
Related concepts
Primary source: Bennett et al., Teleporting an unknown quantum state via dual classical and Einstein-Podolsky-Rosen channels, Phys. Rev. Lett. 70, 1895 (1993), doi:10.1103/PhysRevLett.70.1895
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