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An electron istrapped in a finite well. How "far" (in eV) is it from being free if the penetration length of its wave function into the classically forbidden region 1nm?

Short Answer

Expert verified

The distance of the electron to set free is 0.038eV.

Step by step solution

01

Identification of given data

The penetration length of the classically forbidden region isL=1nm.

02

Concept/Significance of a potential well

A potential well is a place in aforce field, where the atomic nucleus is located and where the potential is much lower than at a point immediately outside it unless aparticle accumulates a significant amount of energy.

03

Determination of the distance of the electron from being free

The distance of the electron is mathematically presented as:

δ=2mU0-EU0-E=2mδ22

Here, is the reduce planks constant whose value is 1.055×10-34J·s , is the mass of the electron whose value is 9.11×10-31kg , and U0-Eis the distance of the potential well to free the electron.

Replaceall the values in the above equation:

U0-E=2×9.11×10-31kg10-9m21.055×10-34J·s2=6.1×10-21J6.24×1018eV1J=38.064×10-3eV=0.038eV.

Hence, the distance of the electron to set free is 0.038eV.

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Most popular questions from this chapter

Obtain expression (5-23) from equation (5-22). Using cosθ=cos2(12θ)sin2(12θ)andsinθ=2sin(12θ)cos(12θ), first convert the argument of the cotangent fromkLto12kL. Next, put the resulting equation in quadratic form, and then factor. Note thatαis positive by definition.

For the harmonic oscillator potential energy, U=12kx2, the ground-state wave function is ψ(x)=Ae-(mk/2)x2, and its energy is 12k/m.

(a) Find the classical turning points for a particle with this energy.

(b) The Schrödinger equation says that ψ(x) and its second derivative should be of the opposite sign when E > Uand of the same sign when E < U . These two regions are divided by the classical turning points. Verify the relationship between ψ(x)and its second derivative for the ground-state oscillator wave function.

(Hint:Look for the inflection points.)

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(a) Which of the two normalizability requirements is violated by the plane wave, and which by Dirac delta function?

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(c) Rather than an infinitely tall and narrow spike like the Dirac delta function. Consider a function that is 0 everywhere except the narrow region-E<x<+ where its value is a constant B. This too could be normalized, What would be the relationship between s and B, and what would happen to B as s approaches 0? (What we get is not exactly the Dirac delta function, but the distinction involves comparing infinities, a dangerous business that we will avoid.)

(d) As we see, the two "exceptional" functions may be viewed as limits of normalizable ones. In those limits, they are also complementary to each other in terms of their position and momentum uncertainties. Without getting into calculations, describe how they are complementary.

A bound particle of massdescribed by the wave function

ψ(x)=Axe-x2/2b2

What is the most probable location at which to find the particle?

Repeat the exercise 60-62 for the first excited state of harmonic oscillator.

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