All extracts / Quantum Computing & Security
SOURCE-BASED DEEP DIVE · 1 PDF PAGES

Quantum Logic Gates

Text extracted from the original supplied flyer, organized for web reading. The source PDF remains available to verify equations and diagrams.

Mathematical fidelity: These page images preserve the exact notation and visual layout of the supplied PDF. The optional text extract below is for searching/copying only and may contain transcription errors.

Original pages — equations and symbols preserved

quantum logic gates — original PDF page 1, preserving equations and diagrams
Original PDF · page 1 of 1
Show extracted text (searchable; equations may be imperfect)
Extract · PDF page 1
QUANTUM COMPUTING AND CIRCUIT ARCHITECTURES QUANTUM LOGIC GATES Mathematical Transformations in Multi-Qubit Circuits An axiomatic guide to unitary operations, matrix representations, and universal gate sets.
Extract · PDF page 1
1. MATHEMATICAL FOUNDATIONS OF QUANTUM GATES Quantum gates are mathematical operators that transform a quantum state. Because physical systems must conserve total probability (Postulate 4), every closed-system quantum gate is modeled as a Unitary Matrix U. Unitary Condition: U †U = UU † = I ←→ Consequence: Reversible computation is natively mandatory.
Extract · PDF page 1
2. SINGLE-QUBIT OPERATIONS & THE PAULI GROUP Single-qubit gates manipulate state vectors on the complex Bloch Sphere, mapping transformations on the basis states {|0⟩, |1⟩}. The Pauli Matrices & Hadamard Transformation: 0 1 0 −i 1 0 1 1 1 X = Y = Z = H = √ 1 0 i 0 0 −1 2 1 −1 Superposition Generation: H |0⟩= |0⟩+|1⟩√ = |+⟩ and H |1⟩= |0⟩−|1⟩√ = |−⟩ 2 2 ✦Phase Gates: The S gate diag(1, i) executes a π/2 rotation, while the T gate diag(1, eiπ/4) executes a critical π/4 rotation around the Z-axis.
Extract · PDF page 1
3. MULTI-QUBIT ENTANGLING GATES Multi-qubit systems scale via tensor products (⊗). Controlled gates apply a target transformation conditioned strictly on the state of control qubits. Controlled-NOT (CNOT) Operator: Flips the target qubit if and only if the control qubit is |1⟩. 1 0 0 0  0 1 0 0 |00⟩→|00⟩ |10⟩→|11⟩ CNOT =   Mapping: and 0 0 0 1  |01⟩→|01⟩ |11⟩→|10⟩   0 0 1 0 Controlled-Phase (CZ) Operator: Injects a negative phase factor (−1) if and only if both system qubits occupy the |11⟩state. CZ = diag(1, 1, 1, −1). GENERATING THE 3-QUBIT GHZ STATE Global coherence is built sequentially using a mix of single-qubit and multi-qubit entangling operations: |000⟩+ |111⟩ Circuit Operations: (CNOT2→3)(CNOT1→2)(H ⊗I ⊗I) |000⟩= √ 2
Extract · PDF page 1
4. COMPUTATIONAL UNIVERSALITY A finite set of quantum gates is classified as Universal if any arbitrary unitary operation can be approximated to any desired degree of accuracy ε. 1. The Clifford Set: Consisting of {H, S, CNOT}, this set can efficiently be simulated classically (Gottesman-Knill Theorem). 2. Clifford + T Set: Adding the non-Clifford T gate breaks classical simulatability, yielding absolute universal quantum computational power.
◈ QuantumVerse Hub