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At time t = 0 a particle is represented by the wave function

ψ(x,0)={A(x,0),0xa,A(bx)/(ba),axb,0,otherwise,where A, a, and b are (positive) constants.

(a) Normalize ψ(that is, find A, in terms of a and b).

(b) Sketch ψ(x,0), as a function of x.

(c) Where is the particle most likely to be found, at t = 0?.

(d) What is the probability of finding the particle to the left of a? Check your result in the limiting cases b = a and b= 2a.

(e) What is the expectation value of x?

Short Answer

Expert verified

(a)A=3bA=b3.

(c) x=0

(d)P=0a|A|2dx=|A|2a20ax2dx=|A|2a3=abP

(e) X=2a+b4.

Step by step solution

01

(a) Normalizing ψ .

1=|A|2a20ax2dx+|A|2(ba)20b(ba)2dx=|A|21a2x330a+1(ba)2(bx)33ab=|A|2a3+ba3=|A|2b3A=3bA=b3.

02

(b) Sketching ψ(x,0)

03

(c) The particle most likely to be found at,

At x = a.

04

(d) probability of finding the particle.

P=0a|A|2dx=|A|2a20ax2dx=|A|2a3=abP=ba,P=1ifb=aP=1/2ifb=2a.

05

(e) Expectation value of x.

x=x|Ψ|2dx=|A|21a20ax3dx+1(ba)2abx(bx)2dx.

=3b1a2x440a+1(ba)2b2x222bx33+x44ab.

=34b(ba)2[a2(ba)2+2b48b4/3+b42a2b2+8a3b/3a4].

=34b(ba)2b43a2b2+23a3b=14(ba)2(b33a2b+2a3)=2a+b4.

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Most popular questions from this chapter

Consider the first 25 digits in the decimal expansion of π (3, 1, 4, 1, 5, 9, . . .).

(a) If you selected one number at random, from this set, what are the probabilities of getting each of the 10 digits?

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(c) Find the standard deviation for this distribution.

Suppose you add a constantV0 to the potential energy (by “constant” I mean independent ofxas well as t). In classical mechanics this doesn’t change anything, but what about quantum mechanics? Show that the wave function picks up a time-dependent phase factor:exp(-iV0t/h). What effect does this have on the expectation value of a dynamical variable?

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(a) Solids. The lattice spacing in a typical solid is around d=0.3nm. Find the temperature below which the free 18electrons in a solid are quantum mechanical. Below what temperature are the nuclei in a solid quantum mechanical? (Use sodium as a typical case.) Moral: The free electrons in a solid are always quantum mechanical; the nuclei are almost never quantum mechanical. The same goes for liquids (for which the interatonic spacing is roughly the same), with the exception of helium below 4K.

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Why can’t you do integration-by-parts directly on the middle expression in Equation -1.29 pull the time derivative over onto x, note thatx/t=0 , and conclude thatd<x>/dt=0 ?

Suppose you wanted to describe an unstable particle, that spontaneously disintegrates with a lifetime in that case the total probability of finding the particle somewhere should not be constant but should decrease at an exponential rate:

p(t)=-[ψx,t2]dx=e-tt

A crude way of achieving this result is as follows. in equation 1.24 we tightly assumed that is real. That is certainly responsible, but it leads to the conservation of probability enshrined in equation 1.27. What if we assign to in imaginary part

V=V0=iΓ

Where is the true potential energy and is a positive real constant?

  1. Show that now we get

dpdt=2Γhp.

Solve for and find the lifetime of the particle in terms ofΓ

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