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Normalization Factor - Introduction to Quantum Mechanics - Exam, Exams of Quantum Mechanics

This is the Exam of Introduction to Quantum Mechanics which includes Wavefunctions Valid, Bound State Solutions, One Bound State, Lowering Operators, State Vector, Arbitrary Complex Number, Energy of Electron, Approximate Energy etc. Key important points are: Normalization Factor, Probability Density, Explicit Time-Dependent, Spherical Harmonics, Determine Matrix, Determine Eigenvalues, Step Operators, Vacuum State, Correction in Energy

Typology: Exams

2012/2013

Uploaded on 03/07/2013

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Download Normalization Factor - Introduction to Quantum Mechanics - Exam and more Exams Quantum Mechanics in PDF only on Docsity! 1 2005 Ph.D. Qualifier, Quantum Mechanics DO ONLY 3 OUT OF 4 OF THE QUESTIONS Problem 1. A particle of mass m in an infinitely deep square well extending between x = 0 and x = L has the wavefunction Ψ(x, t) = A [ sin (πx L ) e−iE1t/~ − 3 4 sin ( 3πx L ) e−iE3t/~ ] , (1) where A is a normalization factor and En = n 2h2/8mL2. (a) Calculate an expression for the probability density |Ψ(x, t)|2, within the well at t = 0. (b) Calculate the explicit time-dependent term in the probability density for t 6= 0. (c) In terms of m, L, and h, what is the repetition period T of the complete probability density? Problem 2. Let us consider the spherical harmonics with l = 1. (a) Determine the eigenvalues for aLz, where a is a constant. (b) Determine the matrix for Lx for the basis set |lm〉 with l = 1 using the fact that L±|lm〉 = ~ √ (l ∓m)(l ±m + 1)|l, m± 1〉. (2) and that the step operators are given by L± = Lx ± iLy. (c) Determine the eigenvalues of aLx for the states with l = 1. (d) Determine the matrix for L2 from the matrices for L+, L−, and Lz. Problem 3. Consider a two-dimensional harmonic oscillator H0 = ~ωxa † xax + ~ωya † yay (3) with ~ωx  ~ωy. The number of excited states is given by N = nx + ny, where a†x|nx〉 = √ nx + 1|nx + 1〉 and a†y|ny〉 = √ ny + 1|ny + 1〉 (a) Express the normalized state with N = 2 with the lowest energy in terms of the step operators and the vacuum state |0〉, i.e. the state with no oscillators excited. The system is now perturbed by H1 = K(a † xay + a † yax). (4) (b) Calculate for the state found in (a): the correction in energy up to first order. (c) Express the correction in energy up to second order. (d) Give the lowest-order correction to the wavefunction. NOTE: The correction term to the wavefunction is given by |ψ1n〉 = ∑ m6=n 〈ψ0m|H1|ψ0n〉 E0n − E0m |ψ0m〉 (5)
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