As Fig. 39-8 suggests, the probability density for the region X>L in the finite potential well of Fig. 39-7 drops off exponentially according toψ2(x)=Ce-2kx , where C is a constant. (a) Show that the wave functionψ(x) that may be found from this equation is a solution of Schrödinger’s equation in its one-dimensional form. (b) Find an expression for k for this to be true.

Short Answer

Expert verified

a) It is proved that the wave functionψx is a solution of Schrödinger’s equation in its one-dimensional form.

b) The expression of isk=2πh2mU-E .

Step by step solution

01

Describe Schrodinger's equation

Schrodinger's equation in the finite potential well at is given by,

d2ψdx2+8π2mh2(E-U)ψ=0........(1)

02

Show that the wave function ψ(x) is a solution of Schrödinger’s equation in its one-dimensional form(a)

Consider the given wave function.

ψ2x=Ce-2kxψx=Ce-kx

Substituteψx=Ce-kx in equation (1).

d2dx2Ce-kx+8π2mh2E-Uψ=0Cddx-ke-kx+8π2mh2E-Uψ=0Ck2e-kx+8π2mh2E-Uψ=0k2ψ+8π2mh2E-Uψ=0

Therefore, it is proved that the wave functionψx is a solution of Schrödinger’s equation in its one-dimensional form.

03

Find an expression for k for this to be true(b)

Consider the following equation.

k2ψ+8π2mh2E-Uψ=0

Simplify the above equation for .

k2ψ=8π2mh2U-Eψk2=8π2mh2U-Ek=2πh2mU-E

Therefore, the expression of is k=2πh2mU-E.

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Most popular questions from this chapter

Verify that the combined value of the constants appearing in Eq. 39-33 is 13.6eV

A muon of charge -eand massm=207me(wheremeis the mass of an electron) orbits the nucleus of a singly ionized helium atom (He+). Assuming that the Bohr model of the hydrogen atom can be applied to this muon–helium system, verify that the energy levels of the system are given by

E=-11.3eVn2

Consider a conduction electron in a cubical crystal of a conducting material. Such an electron is free to move throughout the volume of the crystal but cannot escape to the outside. It is trapped in a three-dimensional infinite well. The electron can move in three dimensions so that its total energy is given by

E=h28L2m(n12+n22+n32)

in whichare positive integer values. Calculate the energies of the lowest five distinct states for a conduction electron moving in a cubical crystal of edge length L=0.25μm.

As Fig. 39-8 suggests, the probability density for the region

0 < x < L for the finite potential well of Fig. 39-7 is sinusoidal, being given by

ψ2(x)=Bsin2kx , in which B is a constant. (a) Show that the wave function ψ(x)

may be found from this equation is a solution of Schrodinger’s equation in its one-dimensional form. (b) Express an equation for that makes this true.

Figure 39-26 indicates the lowest energy levels (in electronvolts) for five situations in which an electron is trapped in a one-dimensional infinite potential well. In wells B, C, D, and E, the electron is in the ground state. We shall excite the electron in well A to the fourth excited state (at 25 eV). The electron can then de-excite to the ground state by emitting one or more photons, corresponding to one long jump or several short jumps. Which photon emission energies of this de-excitation match a photon absorption energy (from the ground state) of the other four electrons? Give then values.

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