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The phase kickback phenomenon is a fundamental technique that appears throughout quantum computing. When we apply controlled operations, phases that would normally appear on the target qubit can instead 'kick back' to affect the control qubit. This surprising behavior turns out to be incredibly useful - it's a key ingredient in many quantum algorithms.

By cleverly using phase kickback, we can encode information about an operation into phases that can then be measured, allowing quantum computers to solve certain problems more efficiently than classical computers.

Let's start with the controlled-NOT (CNOT\text{CNOT}) gate. When the target qubit is in the =12(01)|-\rangle = \frac{1}{\sqrt{2}}(|0\rangle - |1\rangle) state, something interesting happens:

PhaseKickback

If we trace through the computation:

  • Initial state: +=12(0+1)12(01)|+\rangle|-\rangle = \frac{1}{\sqrt{2}}(|0\rangle + |1\rangle) \frac{1}{\sqrt{2}}(|0\rangle - |1\rangle)
  • Expanding: 12(0001+1011)\frac{1}{2}(|00\rangle - |01\rangle + |10\rangle - |11\rangle)
  • After CNOT\text{CNOT}: 12(0001+1110)\frac{1}{2}(|00\rangle - |01\rangle + |11\rangle - |10\rangle)

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... continued in the full lesson.

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