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

Use the WKB approximation to find the allowed energies of the harmonic oscillator.

Consider the quantum mechanical analog to the classical problem of a ball (mass m) bouncing elastically on the floor.
(a) What is the potential energy, as a function of height x above the floor? (For negative x, the potential is infinite x - the ball can't get there at all.)
(b) Solve the Schrödinger equation for this potential, expressing your answer in terms of the appropriate Airy function (note that Bi(z) blows up for large z, and must therefore be rejected). Don’t bother to normalize ψ(x).
(c) Using g=9.80m/s2and m=0.100kg , find the first four allowed energies, in joules, correct to three significant digits. Hint: See Milton Abramowitz and Irene A. Stegun, Handbook of Mathematical Functions, Dover, New York (1970), page 478; the notation is defined on page 450.
(d) What is the ground state energy, in ,eV of an electron in this gravitational field? How high off the ground is this electron, on the average? Hint: Use the virial theorem to determine <x> .

About how long would it take for a (full) can of beer at room temperature to topple over spontaneously, as a result of quantum tunneling? Hint: Treat it as a uniform cylinder of mass m, radius R, and height h. As the can tips, let x be the height of the center above its equilibrium position (h/2) .The potential energy is mgx, and it topples when x reaches the critical value X0=R2+(h/2)2-h/2. Calculate the tunneling probability (Equation
8.22), for E = 0. Use Equation 8.28, with the thermal energy ((1/2)mv2=(1/2)kBT)to estimate the velocity. Put in reasonable numbers, and give your final answer in years.

Te-2T,withγ1h0a|px|dx... (8.22).

tau=2r1Ve2T (8.28).

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).

Consider a particle of massm in the n th stationary state of the harmonic oscillator (angular frequency ω ).

(a) Find the turning point, x2 .
(b) How far (d) could you go above the turning point before the error in the linearized potential reaches 1%? That is, if V(x2+d)-VIin(x2+d)V(x2)=0.01 what is ?
(c) The asymptotic form of Ai(z) is accurate to 1% as long as localid="1656047781997" z5. For the din part (b), determine the smallest nsuch thatαd5 . (For any n larger than this there exists an overlap region in which the liberalized potential is good to 1% and the large-z form of the Airy function is good to 1% .)

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