Docsity
Docsity

Prepare for your exams
Prepare for your exams

Study with the several resources on Docsity


Earn points to download
Earn points to download

Earn points by helping other students or get them with a premium plan


Guidelines and tips
Guidelines and tips

Problem Set 1 - Introduction to Quantum Mechanics II | PHY 4605, Assignments of Physics

Material Type: Assignment; Class: INTRO QUANT MECH 2; Subject: PHYSICS; University: University of Florida; Term: Spring 2005;

Typology: Assignments

Pre 2010

Uploaded on 03/11/2009

koofers-user-ef8-1
koofers-user-ef8-1 🇺🇸

10 documents

1 / 1

Toggle sidebar

Related documents


Partial preview of the text

Download Problem Set 1 - Introduction to Quantum Mechanics II | PHY 4605 and more Assignments Physics in PDF only on Docsity! PHY4605–Introduction to Quantum Mechanics II Spring 2005 Problem Set 3 Jan. 24, 2005 Due: 31 January, 2005 Reading: PH notes Remarks: On problem set 1 too many people had continued difficulty with matrix algebra. To solidify these crucial concepts, here’s more practice. 1. Matrix algebra drill. Given the matrices A =   3 5 −4 5 4 5 3 5   ; B =   1 1 −1 −1 3 −1 −1 2 0   ; C =   −1 2 2 2 2 2 −3 −6 −6   (1) (a) Find the eigenvalues λi and normalized eigenvectors vi, i = 1, 2, 3 for A, B, and C. State the degeneracy of each eigenvalue. (b) Find the determinants of A, B, and C. (c) Recall that, under a change of basis matrices, transform as M → M ′ = Û−1MÛ and vectors as v → v′ = Û−1v. Find Û such that A is brought into diagonal form by a change of basis. How is the matrix of transforma- tion Û related to the eigenvectors of A? Find the transformed eigenvectors Û−1vi. Now answer the same questions for C. (d) Find the inverses of A and B, and state why C is not invertible. (e) Show that the inverse of the 2D matrix represented by M = a01 + ~a · ~σ is M−1 = D−10 (a01−~a ·~σ), with D0 = a20−~a ·~a. Here 1 is the identity matrix in 2D and σx, σy, and σz are the Pauli matrices. [Hint: properties of the Pauli matrices you may find useful: 1) σ2i = 1 for any i; 2) σiσj = i²ijkσk for i 6= j.] 2. Phase shift in a vector potential. (a) Show that the vector potential outside an infinite solenoid containing a flux Φ has the magnitude Φ/2πρ, where ρ is the perpendicular distance from the axis of the solenoid. (b) Show that if ψA satisfies ih̄ ∂ψA ∂t = 1 2m [p− eA(r)]2ψA, then ψA(r, t) = exp ( ie h̄ ∫ r r0 A · ds ) ψA=0(r, t) Apparently ψA depends on an arbitrary initial point r0. Comment on this ambiguity. 1
Docsity logo



Copyright © 2024 Ladybird Srl - Via Leonardo da Vinci 16, 10126, Torino, Italy - VAT 10816460017 - All rights reserved