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A particle in the infinite square well has the initial wave function

ψ(X,0)={Ax,0xa2Aa-x,a2xa

(a) Sketch ψ(x,0), and determine the constant A

(b) Findψ(x,t)

(c) What is the probability that a measurement of the energy would yield the valueE1 ?

(d) Find the expectation value of the energy.

Short Answer

Expert verified

a) and the value for A 12a3

b) ψx,t=46π22an=1,3,5...-1n-121n2sinnπaxe-Entħ

c) The probability is 96π4=0.985534.

d) The value for expectation energy H=6ħ2ma2 .

Step by step solution

01

Define the graph of the wave function

A wave function is a mathematical representation of a particle's quantum state in terms of momentum, time, location, and spin. The Greek letter psi is used to represent a wave function ψ.

02

Graph of ψ(x,0)  .

a)

The graph for the function is:

03

Normalize the value of A

The wave function is

1=A20a2x2dx+A2a2aa-x2dx1=A2x330a2-a-x33a2a1=A23a38+a381=A2a312A=23a3

Therefore the value of A is 23a3.

04

Find the value for ψ(x,t)

(b)

Using the given function ψx,t=n=1cnψnxe-iEnt/ħwhere,

ψnx=2asinnπax

and

En=n2π2ħ22ma2

Now find the complex constant as:

cn=2a×23aa0a2×sinnπaxdx+a2aa-xsinnπaxdxcn=26a2anπ2sinnπax-xanπcosnπax0a2+a-anπcosnπaxa2a-anπ2sinnπax-axnπcosnπaxa2a

cn=26a2anπ2sinnπaa2x-a22nπcosnπ2-a2nπcosnπ+a2cos2-anπ2sinnπa+a22nπcosnπa2cosacn=26a22a2nπ2sinnπ2cn=0,ifniseven-1n-12462,ifnisodd

So, The wave function is ψx,t=46π22an=1,3,5...-1n-121n2sinnπaxe-Entħ

Where, En=n2π2ħ2ma2.

05

Now, find the value of particle energy P1 .

(c)

The probability can be calculated as,

c12=-1n-1/246nπ22=46nπ22=96π4=0.985534

Thus, the required probability is 0.985534 .

06

Now find the value for the expectation value (H)

(d)

Calculate the expectation value of energy as,

H=cn2En=96π4π2ħ2ma211+132+152+172+....=48π2ħ8π2ma2=6ħ2ma2

Hence, the expectation value of the energy is 6ħ2ma2 .

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Most popular questions from this chapter

A particle of mass m in the infinite square well (of width a) starts out in the left half of the well, and is (at t=0) equally likely to be found at any point in that region

(a) What is its initial wave function, ψ(x,0)? (Assume it is real. Don’t forget to normalize it.)

(b) What is the probability that a measurement of the energy would yield the valuesπ2h22ma2?

Solve the time-independent Schrodinger equation with appropriate boundary conditions for the “centered” infinite square well: V(x)=0(for-a<x<+a), V(x)=α(otherwise). Check that your allowed energies are consistent with mine (Equation 2.30), and confirm that your ψ'scan be obtained from mine (Equation 2.31) by the substitution x → (x + a)/2 (and appropriate renormalization). Sketch your first three solutions, and compare Figure 2.2. Note that the width of the well is now 2a.

Consider the double delta-function potentialV(x)=-α[δx+a+δx-a]Whereand are positive constants

(a) Sketch this potential.

(b) How many bound states does it possess? Find the allowed energies, forα=ħ/maand forα=ħ2/4ma, and sketch the wave functions.

In Problem 2.7 (d), you got the expectation value of the energy by summing the series in Equation 2.39, but 1 warned you (in footnote 15 not to try it the "old fashioned way,"<H>=Ψ(x,0)*HΨ(x,0)dx, because the discontinuous first derivative ofΨ(x.0)renders the second derivative problematic. Actually, you could have done it using integration by parts, but the Dirac delta function affords a much cleaner way to handle such anomalies.

(a) Calculate the first derivative of Ψ(x.0)(in Problem 2.7), and express the answer in terms of the step function, θ(x-c1/2)defined in Equation (Don't worry about the end points-just the interior region

(b) Exploit the result of Problem 2.24(b) to write the second derivative of Ψ(x,0)in terms of the delta function.

(c) Evaluate the integral Ψ(x,0)*HΨ(x,0)dxand check that you get the same answer as before.

This is a strictly qualitative problem-no calculations allowed! Consider the "double square well" potential (Figure 2.21). Suppose the depth V0and the width a are fixed, and large enough so that several bound states occur.

(a) Sketch the ground state wave function Ψ1and the first excited state localid="1658211858701" Ψ2(i) for the case b = 0 (ii) forbaand (iii) for ba

(b) Qualitatively, how do the corresponding energies(E1andE2)and vary, as b goes from 0 to ? Sketch E1(b)and E2(b)on the same graph.

(c) The double well is a very primitive one-dimensional model for the potential experienced by an electron in a diatomic molecule (the two wells represent the attractive force of the nuclei). If the nuclei are free to move, they will adopt the configuration of minimum energy. In view of your conclusions in (b), does the electron tend to draw the nuclei together, or push them apart? (Of course, there is also the internuclear repulsion to consider, but that's a separate problem.)

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