concept

bell states

The four maximally entangled quantum states of two qubits, forming a basis for quantum information processing.
104 related articles

Description

Bell states are four specific quantum states of two qubits (quantum bits) that are maximally entangled. Entanglement means the two qubits are correlated in a way that cannot be described independently; measuring one instantly determines the state of the other, no matter how far apart they are. The four Bell states form a complete, orthonormal basis for the two-qubit Hilbert space, meaning any two-qubit state can be expressed as a combination of them. They are named after physicist John Bell, who in 1964 formulated inequalities that distinguish quantum entanglement from any classical hidden-variable theory.

History

The concept of entangled states dates back to the Einstein-Podolsky-Rosen paper of 1935, but the specific Bell states were formalized in the context of Bell's theorem in the 1960s. They were later named and used extensively in quantum information theory starting in the 1990s, particularly by Charles Bennett and colleagues.

How it works

A Bell state is created by applying a specific quantum circuit: start with two qubits in a known state (e.g., both |0>), apply a Hadamard gate to the first qubit (putting it in a superposition), then apply a controlled-NOT gate with the first qubit as control and the second as target. This entangles the qubits into one of the four states, such as (|00> + |11>)/√2. The four states differ by relative phases and bit flips. Measuring one qubit in the Bell basis (a measurement that projects onto these states) reveals the entanglement and is a key operation in quantum teleportation and superdense coding.

In practice

Bell states are the foundation of quantum teleportation, quantum cryptography (e.g., BB84 protocol), and superdense coding, which allows transmitting two classical bits using one qubit.

Fun fact

In 2022, the Nobel Prize in Physics was awarded for experiments with entangled photons, including the creation and manipulation of Bell states, confirming their non-classical correlations.

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