Use equation 8.22 calculate the approximate transmission probability for a particle of energy E that encounters a finite square barrier of height V0 > E and width 2a. Compare your answer with the exact result to which it should reduce in the WKB regime T << 1.

Short Answer

Expert verified

The solution of Transmission probability is T~e-2y.

Step by step solution

01

To Calculate Transmission Probability.

Consider a finite square barrier of height V0>Eand width 2a, we find

γ=1ħ02a2mV0-Edx=2mħ2mV0-EAnd,theprobabilityoftransmissionisTWKBexp-4aħ2mV0-ETherefore,theexactresultisT=11+Ksinh2γWhereK=V02/4EV0-E.Nowrememberthatsinhx=ex-ex/2,thenwefindintheWKBregimey>>1.sinh2y=ey-e-y2e2y4whichleadstoT11+K/4e2yIntheWKBregimeT<<1y>>1,wecanneglecttheoneinthedenominatorandsoweshowthisresultreducestotheWKBtransmissionprobability,T~e-2yWhere,Y=2a/ħ2mV-E

02

Draw the graph.

To draw the graph of the finite square barrier of height V0>Eand width 2a .

For graph, finite square barrier of heightV0>Eand width ,

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

Derive the connection formulas at a downward-sloping turning point, and confirm equation8.50.

ψ(x)={D'|p(x)|exp-1hxx1|p(x')|dx'.ifx<x12D'p(x)sin-1hx1xp(x')dx'+π4.ifx<x1

Consider the case of a symmetrical double well, such as the one pictured in Figure. We are interested in Figure 8.13bound states with E<V(0) .
(a) Write down the WKB wave functions in regions (i) x>x2 , (ii) x1<x<x2 , and (iii) 0<x<x1. Impose the appropriate connection formulas at and (this has already been done, in Equation 8.46, for x2 ; you will have to work out x1 for yourself), to show that


ψ(x)={DPxexp-1hx2xpx'dx'2DPxsin1hx2xpx'dx'+π4DPx2cosθ1hvx1pxdx+sinθe1hvx1pxdx

FIGURE 8.13: Symmetrical double well; Problem 8.15.
Where

θ1hx1x2p(x)dx .

(b) Because v(x) is symmetric, we need only consider even (+)and odd (-)wave functions. In the former case ψ(0)=0 , and in the latter case ψ=(0)=0 . Show that this leads to the following quantization condition:

tanθ=±2ef.

Where

f1h-x1x1p(x)dx

Equation 8.59determines the (approximate) allowed energies (note that Ecomes into 1 and x2, so θ and ϕ are both functions of E ).

(c) We are particularly interested in a high and/or broad central barrier, in which case ϕ is large, and eϕis huge. Equation 8.59 then tells us thatA θmust be very close to a half-integer multiple of π . With this in mind, write localid="1658823154085" (θ=n+1/2)π+o . where localid="1658823172105" ||<<1, and show that the quantization condition becomes

localid="1658823190448" θ=(n+12)πm12e-f.

(d) Suppose each well is a parabola: 16

localid="1658823244259" v(x)={12mω2x+a2,ifx<012mω2x-a2,ifx<0 .

Sketch this potential, find (Equation 8.58 ), and show that

localid="1658823297094" En±=(n+12)hωmhω2πe-f

Comment: If the central barrier were impenetrable localid="1658823318311" (f) , we would simply have two detached harmonic oscillators, and the energies, localid="1658823339386" En=(n+1/2)hω , would be doubly degenerate, since the particle could be in the left well or in the right one. When the barrier becomes finite (putting the two wells into "communication"), the degeneracy is lifted. The even (localid="1658823360600" ψn+) states have slightly lower energy, and the odd ones ψn. have slightly higher energy.
(e) Suppose the particle starts out in the right well-or, more precisely, in a state of the form

localid="1658823391675" ψ(x,0)=12(ψn++ψn)

which, assuming the phases are picked in the "natural" way, will be concentrated in the right well. Show that it oscillates back and forth between the wells, with a period

localid="1658823416179" τ=2π2ωe.

(f) Calculate , for the specific potential in part (d), and show that for , localid="1658823448873" V(0).>>E,ϕ~mωa2/h.

Use the WKB approximation to find the allowed energies (En)of an infinite square well with a “shelf,” of heightV0, extending half-way across

role="math" localid="1658403794484" V(x)={v0,(0<x<a/2)0,(a/2<x<a),(otherwise)

Express your answer in terms ofrole="math" localid="1658403507865" V0andEn0(nπħ)2/2ma2(the nth allowed energy for the infinite square well with no shelf). Assume that, but do not assume that E10>V0. Compare your result with what we got in Section 7.1.2, using first-order perturbation theory. Note that they are in agreement if eitherV0is very small (the perturbation theory regime) or n is very large (the WKB—semi-classical—regime).

As an explicit example of the method developed inProblem 7.15, consider an electron at rest in a uniform magnetic fieldB=B2Kfor which the Hamiltonian is (Equation 4.158):

H=-γB (4.158).

H0=eBzmSz (7.57).

The eigenspinors localid="1656062306189" xaandxbandthecorrespondingenergies,EaandEb, are given in Equation 4.161. Now we turn on a perturbation, in the form of a uniform field in the x direction:

{x+,withenergyE+=-γB0ħ/2x-,withenergyE-=-γB0ħ/2 (4.161).

H'=ebxmSx (7.58).

(a) Find the matrix elements of H′, and confirm that they have the structure of Equation 7.55. What is h?

(b) Using your result inProblem 7.15(b), find the new ground state energy, in second-order perturbation theory.

(c) Using your result inProblem 7.15(c), find the variation principle bound on the ground state energy.

Use appropriate connection formulas to analyze the problem of scattering from a barrier with sloping walls (Figurea).

Hint: Begin by writing the WKB wave function in the form

ψ(x)={1pxAeihxx1px'dx'+Be-ihxr1px'dx',x<x11pxCeihx1'px'dx'+De-1hx1Xpx'dx',X1<X<X21pxFeihx2xpx'dx.x>x2

Do not assume C=0 . Calculate the tunneling probability, T=|F|2/|A|2, and show that your result reduces to Equation 8.22 in the case of a broad, high barrier.

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