equation (5-33). The twosolutionsare added in equal amounts. Show that if we instead added a different percentage of the two solutions. It would not change the important conclusion related to the oscillation frequency of the charge density.

Short Answer

Expert verified

The frequency of the time-dependent wave function is the same as it was before

Step by step solution

01

Identification of given data

The sum of the two different solutions is Aψnxe-iEn/t+Bψme-iEm/t

02

Concept/significance of oscillation frequency 

The frequency of an oscillation is the number of oscillations that occur once per unit time or once per second. The frequency of an oscillation can be calculated as the inverse of the time of oscillation.

03

Explanation of the adding different percentages of the two solutions 

The wave function of the particle is mathematically presented as:

ψx,t=Aψnxe-iEn/t+Bψme-iEm/t

Multiply the wave function with its complex conjugate as shown below.

ψx,tψ*x,t=Aψnxe-iEn/t+Bψmxe-iEm/tAψnxeiEn/t+BψmeiEm/t=A2ψn2x+B2ψm2x+e-iEn-Em/t+e-iEm-En/t=A2ψn2x+B2ψm2x+2ABψnxψmxcosEn-Emt

Hence, the frequency of the time-dependent wave function is the same as it was before.

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Most popular questions from this chapter

Consider the delta well potential energy:

U(x)={0x0-x=0

Although not completely realistic, this potential energy is often a convenient approximation to a verystrong, verynarrow attractive potential energy well. It has only one allowed bound-state wave function, and because the top of the well is defined as U = 0, the corresponding bound-state energy is negative. Call its value -E0.

(a) Applying the usual arguments and required continuity conditions (need it be smooth?), show that the wave function is given by

ψ(x)=(2mE0h2)1/4e-(2mE0/)|x|

(b) Sketch ψ(x)and U(x) on the same diagram. Does this wave function exhibit the expected behavior in the classically forbidden region?

The harmonic oscillator potential energy is proportional to x2, and the energy levels are equally spaced:

En(n+12). The energy levels in the infinite well become farther apart as energy increases: Enn2.Because the functionlimb|x/L|bis 0 for|x|<Land infinitely large for|x|>L. the infinite well potential energy may be thought of as proportional to |x|.

How would you expect energy levels to be spaced in a potential well that is (a) proportional to |x|1and (b) proportional to -|x|-1? For the harmonic oscillator and infinite well. the number of bound-state energies is infinite, and arbitrarily large bound-state energies are possible. Are these characteristics shared (c) by the |x|1well and (d) by the-|x|-1well? V

In the harmonic oscillators eave functions of figure there is variation in wavelength from the middle of the extremes of the classically allowed region, most noticeable in the higher-n functions. Why does it vary as it does?

For a total energy of 0, the potential energy is given in Exercise 96. (a) Given these, to what region of the x-axis would a classical particle be restricted? Is the quantum-mechanical particle similarly restricted? (b) Write an expression for the probability that the (quantum-mechanical) particle would be found in the classically forbidden region, leaving it in the form of an integral. (The integral cannot be evaluated in closed form.)

The particle has E=0.

(a) Show that the potential energy for x>0is given by

U(x)=-2am1x+2a22m

(b) What is the potential energy for x<0?

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