Bell measurement
|0⟩ -----------------------------------MZ +1 |0⟩ -----------------------------------MZ +1
|0⟩ --H--.----------- -----------.--H--MZ +1 | | |0⟩ -----X----------- -----------X-----MZ +1
|0⟩ --H--.------ ------.--H--MZ +1 | |00⟩ + |11⟩ | |0⟩ -----X------ ------X-----MZ +1
the outcome says which Bell state is measured |0⟩ --H--.------ ------.--H--MZ +1 | |00⟩ + |11⟩ | |0⟩ -----X------ ------X-----MZ +1
|0⟩ --H--.------ ------.--H--MZ +1 | |00⟩ + |11⟩ | |0⟩ -----X------ ------X-----MZ +1
|0⟩ --H--.------ ------.--H--MZ +1 | |01⟩ + |10⟩ | |1⟩ -----X------ ------X-----MZ -1
|1⟩ --H--.------ ------.--H--MZ -1 | |00⟩ - |11⟩ | |0⟩ -----X------ ------X-----MZ +1
|1⟩ --H--.------ ------.--H--MZ -1 | |01⟩ - |10⟩ | |1⟩ -----X------ ------X-----MZ -1
|1⟩ --H--.------ ------.--H--MZ -1 | |01⟩ - |10⟩ | |1⟩ -----X------ ------X-----MZ -1
|1⟩ --H--.----------- -----------.--H--MZ -1 | | |1⟩ -----X----------- -----------X-----MZ -1
|1⟩ -----------------------------------MZ -1 |1⟩ -----------------------------------MZ -1
we can change the measurement basis to {±XZ,±ZX} |0⟩ --H--.----- -----.--H--MZ | |00⟩ + |11⟩ | |0⟩ -----X----- -----X-----MZ
|0⟩ --H--.----- -----.--H--MZ +1 | |0+⟩ + |1-⟩ | |0⟩ -----X--H-- --H--X-----MZ +1
|0⟩ --H--.----- -----.--H--MZ +1 | |0+⟩ + |1-⟩ | |0⟩ -----X--H-- --H--X-----MZ +1 |0+⟩ + |1-⟩ is stabilized by {+XZ,+ZX}
|.⟩ --H--.----- -----.--H--MZ ±1 | ... | |.⟩ -----X--H-- --H--X-----MZ ±1 and so on ..
Applications: Quantum teleportation;
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Can also do a Bell measurement as a Multi-qubit measurement using an ancilla;
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Hardware implementation: Bell measurement with linear optics;