From 5e387b4654bf5574da0eec92d86710cc96e23451 Mon Sep 17 00:00:00 2001 From: Zheyuan Wu <60459821+Trance-0@users.noreply.github.com> Date: Wed, 18 Jun 2025 23:34:23 -0500 Subject: [PATCH] s --- pages/Math401/Math401_T4.md | 46 +++++++++++++++++++++++++++++++++++++ pages/Math401/_meta.js | 1 + 2 files changed, 47 insertions(+) create mode 100644 pages/Math401/Math401_T4.md diff --git a/pages/Math401/Math401_T4.md b/pages/Math401/Math401_T4.md new file mode 100644 index 0000000..79d7f50 --- /dev/null +++ b/pages/Math401/Math401_T4.md @@ -0,0 +1,46 @@ +# Topic 4: The quantum version of probabilistic concepts + +> In mathematics, on often speaks of non-commutative instead of quantum constructions. + +## Section 1: Generalities about classical versus quantum systems + +In classical physics, we assume that a systema's properties have well-defined values regardless of how we choose to measure them. + +### Basic terminology + +#### Observables + +#### Set of states + +The preparation of a system builds a convex set of states as our initial condition for the system. + +For a collection of $N$ system. Let procedure $N_1=\lambda P_1$ be a preparation procedure for state $P_1$, and $N_2=(1-\lambda) P_2$ be a preparation procedure for state $P_2$. The state of the collection is $N=\lambda N_1+(1-\lambda) N_2$. + +#### Set of effects + +The set of effects is the set of all possible outcomes of a measurement. $\Omega=\{\omega_1, \omega_2, \ldots, \omega_n\}$. Where each $\omega_i$ is an associated effect, or some query problems regarding the system. (For example, is outcome $\omega_i$ observed?) + +#### Registration of outcomes + +A pair of state and effect determines a probability $E_i(P)=p(\omega_i|P)$. By the law of large numbers, this probability shall converge to $N(\omega_i)/N$ as $N$ increases. + +**Quantum states, observables, and effects can be represented mathematically by linear operators on a Hilbert space.** + +## Section 2: Examples of physical experiment in language of mathematics + +### Sten-Gernach experiment + +**State preparation:** Silver tams are emitted from a thermal source and collimated to form a beam. + +**Measurement:** Silver atoms interact with the field produced by the magnet and impinges on the class plate. + +**Registration:** The impression left on the glass pace by the condensed silver atoms. + +## Finite probability spaces in the language of Hilbert space and operators + +> Superposition is a linear combination of two or more states. + +A quantum coin can be represented mathematically by linear combination of $|0\rangle$ and $|1\rangle$.$\alpha|0\rangle+\beta|1\rangle\in\mathscr{H}\cong\mathbb{C}^2$. + +> For the rest of the material, we shall take the $\mathscr{H}$ to be vector space over $\mathbb{C}$. + diff --git a/pages/Math401/_meta.js b/pages/Math401/_meta.js index 10a5ddc..32a5e15 100644 --- a/pages/Math401/_meta.js +++ b/pages/Math401/_meta.js @@ -9,4 +9,5 @@ export default { Math401_T1: "Math 401, Topic 1: Probability under language of measure theory", Math401_T2: "Math 401, Topic 2: Finite-dimensional Hilbert spaces", Math401_T3: "Math 401, Topic 3: Separable Hilbert spaces", + Math401_T4: "Math 401, Topic 4: The quantum version of probabilistic concepts", } \ No newline at end of file