Physics 471: Integrals with Delta Functions & Bound State Energy in Double Delta Potential, Assignments of Quantum Physics

Problem set 7 for physics 471, fall 2003. It includes integrals with delta functions, evaluation of wave functions for a repulsive delta function potential, and determination of bound state energy in a double delta function potential. Students are expected to apply boundary conditions, construct s matrices, and analyze solutions.

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Uploaded on 07/23/2009

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Physics 471 Problem Set 7 Fall 2003
23. Evaluate the following integrals
(a)
−∞
dx (x24x+1)δ(x24) .
(b)
π
0
dx sin3(x)δcos(x)1
2.
24. For the repulsive δ-function potential V(x)=αδ(x), with α>0, consider a wave function
of the form
ψ(x)=AIeikx +BIeikx for x<0
AIIeikx +BII eikx for x>0.
(a) Apply the boundary conditions at x= 0 and construct the Smatrix which relates
(BI,B
II)to(AI,A
II).
(b) Show that Sis unitary, i.e. that SS=1.
(c) Show that det Shas the form e.
25. A particle of mass mmoves in the double δ-function potential
V(x)=¯h2λ
2ma (δ(xa)+δ(x+a)) ,
where aand λare positive constants. Because V(x)=V(x), the wave functions can be
chosen to be even or odd functions of x.
(a) Find the transcendental equation that determines the bound state energy in the case
when the wave function is even, i.e. ψ(x)=ψ(x). Hint: Analyze the solutions with
E<0 in the regions x<a,a<x<aand x>a. Use the finiteness at x→±∞
and the symmetry under x→−xto reduce the number of coefficients to two, and
then apply the boundary conditions at x=a. Is there always a bound state?
(b) Find the corresponding transcendental equation for the case when the solution satis-
fies ψ(x)=ψ(x). Is there always a bound state in this case?
26. Griffiths Problem 3.9.

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Physics 471 Problem Set 7 Fall 2003

  1. Evaluate the following integrals

(a) (^) ∫ ∞ −∞

dx (x^2 − 4 x + 1)δ(x^2 − 4).

(b) (^) ∫ π 0

dx sin^3 (x)δ

( cos(x) −

) .

  1. For the repulsive δ-function potential V (x) = αδ(x), with α > 0, consider a wave function of the form ψ(x) =

{ AI e ikx^ + BI e −ikx^ for x < 0 AII e −ikx^ + BII e ikx^ for x > 0

(a) Apply the boundary conditions at x = 0and construct the S matrix which relates (BI , BII ) to (AI , AII ). (b) Show that S is unitary, i.e. that SS†^ = 1. (c) Show that det S has the form e iα.

  1. A particle of mass m moves in the double δ-function potential

V (x) = −

¯h^2 λ 2 ma

(δ(x − a) + δ(x + a)) ,

where a and λ are positive constants. Because V (x) = V (−x), the wave functions can be chosen to be even or odd functions of x.

(a) Find the transcendental equation that determines the bound state energy in the case when the wave function is even, i.e. ψ(x) = ψ(−x). Hint: Analyze the solutions with E < 0in the regions x < −a, −a < x < a and x > a. Use the finiteness at x → ± ∞ and the symmetry under x → −x to reduce the number of coefficients to two, and then apply the boundary conditions at x = a. Is there always a bound state? (b) Find the corresponding transcendental equation for the case when the solution satis- fies ψ(x) = −ψ(−x). Is there always a bound state in this case?

  1. Griffiths Problem 3.9.