Understanding Two-Qubit States: The Bell States

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SUMMARY

The discussion focuses on the properties of Bell states, which are specific examples of two-qubit states in quantum mechanics. The Bell states form an orthonormal basis for the set of two-qubit states, expressed mathematically as |ψ⟩ = a |00⟩ + b |01⟩ + c |10⟩ + d |11⟩. It is established that the inner product between any two different Bell states is zero, confirming their orthogonality, while the inner product of a Bell state with itself equals one, confirming unit magnitude. This confirms that the four Bell states, namely |ψ⁺⟩, |ψ⁻⟩, |φ⁺⟩, and |φ⁻⟩, indeed form an orthonormal basis.

PREREQUISITES
  • Understanding of quantum mechanics principles
  • Familiarity with qubit representation and notation
  • Knowledge of linear algebra concepts, particularly inner products
  • Basic grasp of orthonormality in vector spaces
NEXT STEPS
  • Study the mathematical representation of quantum states in quantum mechanics
  • Learn about the properties of orthonormal bases in Hilbert spaces
  • Explore the implications of Bell states in quantum entanglement
  • Investigate applications of Bell states in quantum computing and quantum information theory
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Quantum physicists, students of quantum mechanics, and researchers in quantum computing will benefit from this discussion, particularly those interested in the foundational aspects of quantum states and entanglement.

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An example of a two-qubit state is one of the Bell states, for example:

lB> = 1/√2 (l00> + l11>)

In my book it is stated that the Bell states form an orthonormal basis for the set of two qubit states. But what exactly is the general form of a two-qubit state? Is it any vector of the form:

lq> = 1√2 (la>lb> + lc>ld>)

, where la>, lb>, lc> and ld> is any normalized linear combination of l0> and l1>.
If so how can I see that the bell states form an orthonormal basis?
 
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A general two-qubit state can be expressed as:

|\Psi\rangle = a |00\rangle + b|01\rangle + c|10\rangle + d|11\rangle

You can show that the four Bell states form an orthonormal basis by showing that they are all orthogonal to each other and have unit magnitude.
The inner product between any two different bell states is zero,
and the inner product of a bell state with itself is unity.

Alternatively, you can with a bit of algebra, show that
|\Psi\rangle = a' |\psi^{+}\rangle + b'|\psi^{-}\rangle + c'|\phi^{+}\rangle + d'|\phi^{-}\rangle
where
|\psi^{+}\rangle, |\psi^{-}\rangle, |\phi^{+}\rangle, and |\phi^{-}\rangle are the 4 bell states.
 

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