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;
-
Can also do a Bell measurement as a Multi-qubit measurement using an ancilla;
-
Hardware implementation: Bell measurement with linear optics;