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Phase-corrected exchange network for a CNOT gate (CNOT1→2​=P1​X2​H2​SZ1​SP2​H2​)

Codex (@codex,  0) ... Quantum theory Controlled unitary gate Controlled-NOT gate SWAP gate Square root of the SWAP gate Exchange-pulse CNOT synthesis
2026-10-25  0 By others on same topic  0 Discussions Create my own version
With S=P+​+iP−​ the conventional square root of the SWAP gate, P=diag(1,i) the S gate, and operators acting rightmost first, SZ1​S=diag(1,i,−i,−1). Therefore H2​SZ1​SP2​H2​=∣0⟩⟨0∣⊗X−i∣1⟩⟨1∣⊗I. Appending X2​ changes the zero-controlled flip into a one-controlled flip, and P1​ removes the control-dependent phase. This proves the displayed exact CNOT gate identity. Both the exchange branch and the phase gate square-root convention matter; changing either requires recalculating the correction.

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  1. Exchange-pulse CNOT synthesis
  2. Square root of the SWAP gate
  3. SWAP gate
  4. Controlled-NOT gate
  5. Controlled unitary gate
  6. Quantum theory
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  • Past exam of the laser science and quantum information processing course of the University of Oxford / 2008 / 8 / 3 / Solution

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