vault backup: 2026-07-30 14:49:26

This commit is contained in:
Benjamin Neumann
2026-07-30 14:49:26 +02:00
parent 439161caff
commit 5aafe8898d
3 changed files with 13 additions and 2 deletions
+2 -1
View File
@@ -216,6 +216,8 @@
}, },
"active": "25f5b25d5eca7203", "active": "25f5b25d5eca7203",
"lastOpenFiles": [ "lastOpenFiles": [
"SS2026/Quantum Computing/Bernstein-Vazirani/Anhänge/Pasted image 20260730144713.png",
"SS2026/Quantum Computing/Bernstein-Vazirani/Anhänge",
"SS2026/Quantum Computing/Introduction to Quantum Computing.md", "SS2026/Quantum Computing/Introduction to Quantum Computing.md",
"SS2026/Quantum Computing/Anhänge/Introduction-to-Quantum-Computing.pdf", "SS2026/Quantum Computing/Anhänge/Introduction-to-Quantum-Computing.pdf",
"SS2026/Quantum Computing/Bernstein-Vazirani/Bernstein-Vazirani Algorithm.md", "SS2026/Quantum Computing/Bernstein-Vazirani/Bernstein-Vazirani Algorithm.md",
@@ -242,7 +244,6 @@
"SS2026/Quantum Computing/6. Composite Systems/Anhänge", "SS2026/Quantum Computing/6. Composite Systems/Anhänge",
"SS2026/Quantum Computing/6. Composite Systems", "SS2026/Quantum Computing/6. Composite Systems",
"SS2026/Quantum Computing/5. Partial observing and measuring/Anhänge", "SS2026/Quantum Computing/5. Partial observing and measuring/Anhänge",
"SS2026/Quantum Computing/5. Partial observing and measuring",
"SS2026/Quantum Computing/1. Introduction/Introduction to Quantum physics.md", "SS2026/Quantum Computing/1. Introduction/Introduction to Quantum physics.md",
"SS2026/Quantum Computing/2. Probabilistic systems/Probabilistic Systems.md", "SS2026/Quantum Computing/2. Probabilistic systems/Probabilistic Systems.md",
"SS2026/Quantum Computing/3. Quantum Systems/Quantum Systems.md", "SS2026/Quantum Computing/3. Quantum Systems/Quantum Systems.md",
Binary file not shown.

After

Width:  |  Height:  |  Size: 10 KiB

@@ -2,4 +2,14 @@ The first quantum algorithm we will look at is the Bernstein-Vazirani algorithm.
Given a secret s $\in \{0,1\}^n$ and the function f : $\{0,1\}^n \rightarrow \{0,1\}$ defined as f(x) = x * s Given a secret s $\in \{0,1\}^n$ and the function f : $\{0,1\}^n \rightarrow \{0,1\}$ defined as f(x) = x * s
\* denotes the inner product of two bitstrings here \* denotes the inner product of two bitstrings here
For Bitstrings x and y of length n the inner product x * y is For Bitstrings x and y of length n the inner product x * y is $x_1y_1 + ... + x_ny_n$ mod 2
The goal is to find the secret s using as few queries of f as possible.
So as few evaluations of f as possible.
We will look at a quantum algorithm that will find s with only one evaluation of f.
![[Pasted image 20260730144713.png]]
The top wire consists of n qubits in state 0. $\ket{0}^n = \ket{0} \otimes ... \otimes \ket{0}$
The bottom wire is in state 1.
Both wires together are in state $\ket{0^n1} = \ket{0}^n \$