Math Problem Statement

Calculate ln(A) and Exp(iAt) for the matrix A = [[0, 1], [1, 0]] and analyze the quantum state |ψ> in Hilbert space H3 with observable Ô.

Solution

This document includes two main problems related to linear algebra and quantum mechanics.


Problem 1: Matrix Calculations

  1. Problem Statement

    • Given a 2×22 \times 2 matrix A=(0110)A = \begin{pmatrix} 0 & 1 \\ 1 & 0 \end{pmatrix}, you need to:

      • (a) Calculate lnA\ln A using the diagonalization method.
      • (b) Compute exp(iAt)\exp(i A t) using the series expansion method.
    • For the series expansion, the following Taylor series expansions are provided: ex=n=0xnn!,cosx=n=0(1)nx2n(2n)!,sinx=n=0(1)nx2n+1(2n+1)!.e^x = \sum_{n=0}^{\infty} \frac{x^n}{n!}, \quad \cos x = \sum_{n=0}^{\infty} \frac{(-1)^n x^{2n}}{(2n)!}, \quad \sin x = \sum_{n=0}^{\infty} \frac{(-1)^n x^{2n+1}}{(2n+1)!}.

  2. Solution Outline

    • (a) For lnA\ln A: Diagonalize the matrix AA, find the eigenvalues and eigenvectors, and express lnA\ln A in terms of these components.
    • (b) For exp(iAt)\exp(i A t): Use the series expansion for the matrix exponential, incorporating the identity and the matrix AA terms iteratively.

Problem 2: Quantum Mechanics in Hilbert Space H3\mathcal{H}_3

  1. Problem Statement

    • Given an orthonormal basis {e1,e2,e3}\{|e_1\rangle, |e_2\rangle, |e_3\rangle\}, and a quantum state: ψ=i2e1+38(e2e3),|\psi\rangle = \frac{i}{2} |e_1\rangle + \sqrt{\frac{3}{8}} \left( |e_2\rangle - |e_3\rangle \right), answer the following:
      • (a) Show that ψ|\psi\rangle is normalized.
      • (b) Consider an observable O^\hat{O} represented by the matrix (10002i0i2)\begin{pmatrix} -1 & 0 & 0 \\ 0 & 2 & i \\ 0 & -i & 2 \end{pmatrix}. Find possible measurement outcomes for this observable.
      • (c) Calculate the probability of measuring outcome 3 for the observable O^\hat{O}.
      • (d) Determine the state of the system immediately after a measurement records outcome 3.
  2. Solution Outline

    • (a) Verify normalization by calculating ψψ=1\langle \psi | \psi \rangle = 1.
    • (b) Diagonalize O^\hat{O} to find eigenvalues, which represent the possible measurement outcomes.
    • (c) Use the projection of ψ|\psi\rangle onto the eigenvector associated with outcome 3 to compute the probability.
    • (d) After obtaining outcome 3, project ψ|\psi\rangle onto the corresponding eigenvector and normalize.

Would you like me to work through any of these parts in detail?


Follow-up Questions:

  1. What are the eigenvalues and eigenvectors of matrix AA?
  2. How does the series expansion method apply to non-commuting matrices?
  3. Why is diagonalization useful in calculating lnA\ln A?
  4. What physical meaning does normalization of ψ|\psi\rangle carry in quantum mechanics?
  5. How does the probability of an outcome relate to projection operators?

Tip:

For matrix exponentials and logarithms, understanding eigenvalues can simplify calculations significantly.

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Math Problem Analysis

Mathematical Concepts

Matrix logarithms
Matrix exponentials
Series expansion
Hilbert spaces
Quantum mechanics
Eigenvalues and eigenvectors

Formulas

Matrix logarithm: ln(A)
Matrix exponential: Exp(iAt)
Series expansions for e^x, cos(x), and sin(x)
Normalization of quantum states

Theorems

Diagonalization theorem
Spectral theorem for Hermitian operators
Projection operators in quantum mechanics

Suitable Grade Level

Undergraduate level (University)