vault backup: 2026-07-30 15:04:27
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"SS2026/Quantum Computing/Introduction to Quantum Computing.md",
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"SS2026/Quantum Computing/8. Ket Notation/Anhänge/Pasted image 20260730101012.png",
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"SS2026/Quantum Computing/8. Ket Notation/Anhänge/Pasted image 20260730101012.png",
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"SS2026/Quantum Computing/8. Ket Notation/Anhänge",
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"SS2026/Quantum Computing/8. Ket Notation/Anhänge",
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"SS2026/Quantum Computing/8. Ket Notation",
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"SS2026/Quantum Computing/8. Ket Notation",
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"SS2026/Quantum Computing/4. Observing and measuring/Observing probabilistic and measuring quantum systems.md",
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"SS2026/Quantum Computing/5. Partial observing and measuring/Partial observing and measuring systems.md",
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"SS2026/Quantum Computing/5. Partial observing and measuring/Partial observing and measuring systems.md",
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"SS2026/Quantum Computing/6. Composite Systems/Composite Systems.md",
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"SS2026/Quantum Computing/6. Composite Systems/Composite Systems.md",
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@@ -12,4 +12,10 @@ We will look at a quantum algorithm that will find s with only one evaluation of
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The top wire consists of n qubits in state 0. $\ket{0}^n = \ket{0} \otimes ... \otimes \ket{0}$
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The top wire consists of n qubits in state 0. $\ket{0}^n = \ket{0} \otimes ... \otimes \ket{0}$
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The bottom wire is in state 1.
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The bottom wire is in state 1.
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Both wires together are in state $\ket{0^n1} = \ket{0}^n \$
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Both wires together are in state $\ket{0^n1} = \ket{0}^n \otimes \ket{1}$
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First, we apply the Hadamard gate on all qubits.
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The resulting state is calculated as follows:
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![[Pasted image 20260730145119.png]]
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