Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

Question: Find the probability current, J (Problem 1.14) for the free particle wave function Equation 2.94. Which direction does the probability flow?

Short Answer

Expert verified

The probability current(J) is

j=^km|A|2

Step by step solution

01

The probability current density (J)

The required formula of probability current density(J) is,

role="math" localid="1657786971189" J=i2m(ΨΨ'x-Ψ*Ψx)

Where y is the wave function of the particle and complex conjugate of yisy°.

02

Compute probability current density

Equation 2.94from the chapter is

Ψk(X,t)=Aeikxjkk22m2

ψ'=Aeikkm22m2?,

Thus, it can written that,

J=i2mΨΨ*x-Ψ*Ψx

=i×2m|A|2eikx-xk22mt(-ik)e-ikx-ak22mt-ekxxk2t2mt(ik)ekx-mk22mt

J=i2m|A|2(-2ik)

J=km|A|2

It flows in the positive (x)direction.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A particle in the infinite square well has the initial wave function

ψ(X,0)={Ax,0xa2Aa-x,a2xa

(a) Sketch ψ(x,0), and determine the constant A

(b) Findψ(x,t)

(c) What is the probability that a measurement of the energy would yield the valueE1 ?

(d) Find the expectation value of the energy.

If two (or more) distinct44solutions to the (time-independent) Schrödinger equation have the same energy E . These states are said to be degenerate. For example, the free particle states are doubly degenerate-one solution representing motion to the right. And the other motion to the left. But we have never encountered normalizable degenerate solutions, and this is no accident. Prove the following theorem: In one dimension45 there are no degenerate bound states. Hint: Suppose there are two solutions, ψ1and ψ2with the same energy E. Multiply the Schrödinger equation for ψ1by ψ2and the Schrödinger equation for ψ2by ψ1and subtract, to show that ψ2dψ1/dx-ψ2dψ1/dxis a constant. Use the fact that for normalizable solutions ψ0at±to demonstrate that this constant is in fact zero.Conclude that ψ2s a multiple of ψ1and hence that the two solutions are not distinct.

For the wave function in Example 2.2, find the expectation value of H, at time t=0 ,the “old fashioned way:

H=Ψ(x,0)H^Ψ(x,0)dx.

Compare the result obtained in Example 2.3. Note: BecauseH is independent of time, there is no loss of generality in usingt=0

In this problem we explore some of the more useful theorems (stated without proof) involving Hermite polynomials.

a. The Rodrigues formula says thatHn(ξ)=(1)neξ2(d)neξ2

Use it to derive H3 and H4 .

b. The following recursion relation gives you Hn+1 in terms of the two preceding Hermite polynomials: Hn+1(ξ)=2ξHn(ξ)2nHn1(ξ)

Use it, together with your answer in (a), to obtain H5 and H6 .

(c) If you differentiate an nth-order polynomial, you get a polynomial of

Order (n-1). For the Hermite polynomials, in fact,

dHn=2nHn1(ξ)

Check this, by differentiatingH5and H6.

d. Hn(ξ)is the nth z-derivative, at z = 0, of the generating function exp(z2+2ξz)or, to put it another way, it is the coefficient ofznn! in the Taylor series expansion for this function: ez2+2ξz=n=0znn!Hn(ξ)

Use this to obtain H0,H1and H2.

Normalize ψ(x)the equation 2.151, to determine the constants D and F.

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free