3. We discussed a perturbative expansion for solving the Schrodinger equation for scat- tering of a particle of energy E = ħ²k²/2m where the first non-trivial approximation (Born approximation) was vy (x) 2m ikx + G(x-x')V (x')eika' dx' with G(xx) the Green's function we discussed in class. Use this to compute the reflection and transmission coefficients as a function of k for scattering off the potential V(x) = Voe-αx² where Vo and a are positive, real constants. 4. Let A, B be operators and as usual define the exponential of an operator by e Σo An/n!. In this problem you will derive some results which are very helpful in dealing with exponentials of operators. These results will be particularly helpful when we discuss the quantum simple harmonic oscillator. They generally go under the name of Baker Campbell Hausdorff or BCH formula. (a) We want to prove a relation expressing eA Be-A as an infinite sum of nested commutators: eA Be-A = 1 1 : B + [A, B] + [A, [A, B}]] + ¸[A, [A, [A, B}]] + … … + + ... To prove this introduce a real parameter A and consider the operator valued function of X f(A)=e^A Be-A By differentiating with respect to A derive a first order differential equation satisfied by f(A). From this equation and the initial condition obeyed by f(0), derive the solution to this first order differential equation as a power series in A. Finally, set = 1 to derive the desired result. Be very careful with the order of operators in this problem. (b) Suppose now that A, B are operators that commute with their commutator, that is such that [A, [A, B]] = [B, [A, B] = 0. Show that [A", B]=nA1A, B] for all positive integers n = 1, 2, 3,.... (c) Assuming still that A, B are operators that commute with their commutator, show that eAB=BAA,B]
3. We discussed a perturbative expansion for solving the Schrodinger equation for scat- tering of a particle of energy E = ħ²k²/2m where the first non-trivial approximation (Born approximation) was vy (x) 2m ikx + G(x-x')V (x')eika' dx' with G(xx) the Green's function we discussed in class. Use this to compute the reflection and transmission coefficients as a function of k for scattering off the potential V(x) = Voe-αx² where Vo and a are positive, real constants. 4. Let A, B be operators and as usual define the exponential of an operator by e Σo An/n!. In this problem you will derive some results which are very helpful in dealing with exponentials of operators. These results will be particularly helpful when we discuss the quantum simple harmonic oscillator. They generally go under the name of Baker Campbell Hausdorff or BCH formula. (a) We want to prove a relation expressing eA Be-A as an infinite sum of nested commutators: eA Be-A = 1 1 : B + [A, B] + [A, [A, B}]] + ¸[A, [A, [A, B}]] + … … + + ... To prove this introduce a real parameter A and consider the operator valued function of X f(A)=e^A Be-A By differentiating with respect to A derive a first order differential equation satisfied by f(A). From this equation and the initial condition obeyed by f(0), derive the solution to this first order differential equation as a power series in A. Finally, set = 1 to derive the desired result. Be very careful with the order of operators in this problem. (b) Suppose now that A, B are operators that commute with their commutator, that is such that [A, [A, B]] = [B, [A, B] = 0. Show that [A", B]=nA1A, B] for all positive integers n = 1, 2, 3,.... (c) Assuming still that A, B are operators that commute with their commutator, show that eAB=BAA,B]
University Physics Volume 3
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ISBN:9781938168185
Author:William Moebs, Jeff Sanny
Publisher:William Moebs, Jeff Sanny
Chapter8: Atomic Structure
Section: Chapter Questions
Problem 101AP: A student in a physics laboratory observes a hydrogen spectrum with a diffraction grating for the...
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