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Introduction to Quantum logic (2)
Yong-woo Choi
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Classical Logic Circuits
Circuit behavior is governed implicitly by classical physics Signal states are simple bit vectors, e.g. X = Operations are defined by Boolean Algebra
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Quantum Logic Circuits
Circuit behavior is governed explicitly by quantum mechanics Signal states are vectors interpreted as a superposition of binary “qubit” vectors with complex-number coefficients Operations are defined by linear algebra over Hilbert Space and can be represented by unitary matrices with complex elements
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Signal state (one qubit)
Corresponsd to Corresponsd to Corresponsd to
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More than one qubit If we concatenate two qubits
We have a 2-qubit system with 4 basis states And we can also describe the state as Or by the vector Tensor product
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Quantum Operations Any linear operation that takes states satisfying
and maps them to states must be UNITARY
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Find the quantum gate(operation)
From upper statement We now know the necessities 1. A matrix must has inverse , that is reversible. 2. Inverse matrix is the same as So, reversible matrix is good candidate for quantum gate
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Quantum Gate One-Input gate: Wire WIRE By matrix Input Wire Output
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Quantum Gate One-Input gate: NOT NOT By matrix Input NOT Gate Output
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Quantum Gate y Two-Input Gate: Controlled NOT (Feynman gate) By matrix
CNOT concatenate y By matrix =
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Quantum Gate 3-Input gate: Controlled CNOT (Toffoli gate) By matrix
=
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Quantum circuit G1 G3 G6 G4 G7 G2 G5 G8 Tensor Product Matrix
multiplication
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