Entanglement: Bell and GHZ States

Intermediate Quantum Entanglement
Created by Pavel · 11.03.2026 at 14:32 UTC

Entangled states are not products of separate qubit states: the vector lives in the joint space, so correlations can be stronger than shared classical randomness alone. Bell and GHZ templates—Hadamard plus CNOT fan-out—are the usual starting points.

More entangling depth is not always better; noise accumulates, so hardware-aware layout matters as much as circuit diagrams. [1], [2].


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Tasks
Question 1

Which circuit fragment is canonical for creating a Bell state from |00>?

Hint

Create superposition first, then correlate.

Question 2

In a Bell state, a single-qubit measurement outcome is typically:

Hint

Local vs joint behavior.

Question 3

How many basis terms appear in the ideal 3-qubit GHZ superposition?

Hint

Only all-zeros and all-ones terms.

Question 4

Which pair best distinguishes entanglement from simple classical correlation?

Hint

Look for separability/coherence language.

Question 5

Provide the two computational-basis strings that define GHZ(3).

Hint

All equal bits.

Question 6

In an ideal Bell state $\frac{|00\rangle + |11\rangle}{\sqrt{2}}$, what is $P(\text{two measurements are equal})$?

Hint

Only 00 and 11 appear.

Question 7

Which statement best captures why Bell-state correlations are non-classical?

Hint

Focus on separability and coherence.

Question 8

In noisy hardware, which change most directly threatens useful entanglement in deep circuits?

Hint

Depth and coherence time trade off.

Question 9

Implement bell_correlation_probability() -> float returning the ideal probability that two Z-measurements on the Bell state $(|00\rangle+|11\rangle)/\sqrt2$ agree (both 00 or both 11).

Hint

Only 00 and 11 have amplitude; they are mutually exclusive.

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Card Info
  • Topic: Quantum Entanglement
  • Difficulty: Intermediate
  • Completed: 0 users
Creator
Pavel
Pavel