Consider a potential barrier of height 30eV. (a) Find a width around1.000nmfor which there will be no reflection of 35eVelectrons incident upon the barrier. (b) What would be the reflection probability for 36eVelectrons incident upon the same barrier? (Note: This corresponds to a difference in speed of less than1(1/2)%.

Short Answer

Expert verified

The width is 1.098nmand the reflection probability is0.475.

Step by step solution

01

Definition:

Tunneling defines the penetration of a barrier of high energy by a low-energy wave or particle. For no reflection,E>U. This is called resonant transmission.

E=U0+n2π222mL2

Reflection probability or reflection coefficient is defined as the ratio of the amplitude of the reflected wave to that of the incident wave.

R=sin22m(E+U0)Lsin22m(E+U0)L+4EU0EU0+1

02

Given/known parameters

E=35eVandU=30eV

03

Solution

(a)nL=2m(E-U)π

nL=2×9.1×10-31×35-30×1.6×10-19J/eV3.14×1.05×10-34

nL=3.64×109

If L=1nm,n=3.64. Rounding off to the nearest integral value,n=4.This gives L=1.098nm.

(b)Putting values in reflection formula:

R=sin22×9.1×10-31(36-30)×1.6×10-19×1.0981.05×10-34in22×9.1×10-31(36-30)×1.6×10-19×1.0981.05×10-34+4(3630)3630-1

R=0.475

04

Explanation and Conclusion

For a barrier width of1.098nm,no reflection will take place.

Reflection coefficient for36eVbeam is 0.475. It is quite small, which means the window for resonant transmission can be small.

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Most popular questions from this chapter

Reflection and Transmission probabilities can be obtained from equations (6-12). The first step is substituting -fork'. (a) Why? (b) Make the substitutions and then use definitions of k and α to obtain equation (6-16).

What fraction of a beam of 50eVelectrons would get through a 200V1nm wide electrostatic barrier?

A particle moving in a region of zero force encounters a precipice---a sudden drop in the potential energy to an arbitrarily large negative value. What is the probability that it will “go over the edge”?

Solving the potential barrier smoothness conditions for relationships among the coefficients A,B and Fgiving the reflection and transmission probabilities, usually involves rather messy algebra. However, there is a special case than can be done fairly easily, through requiring a slight departure from the standard solutions used in the chapter. Suppose the incident particles’ energyEis preciselyU0.

(a) Write down solutions to the Schrodinger Equation in the three regions. Be especially carefull in the region0<x<L. It should have two arbitrary constants and it isn’t difficult – just different.

(b) Obtain the smoothness conditions, and from these findR and T.

(c) Do the results make sense in the limitL?

For the E>U0 potential barrier, the reflection, and transmission probabilities are the ratios:

R=B*BA*AT=F*FA*A

Where A, B, and F are multiplicative coefficients of the incident, reflected, and transmitted waves. From the four smoothness conditions, solve for B and F in terms of A, insert them in R and T ratios, and thus derive equations (6-12).

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