Check the uncertainty principle for the wave function in the equation? Equation 2.129.

Short Answer

Expert verified

Uncertainty of the wave equation p2=mαh2

Step by step solution

01

Define the Schrodinger equation

A differential equation that describes matter in quantum mechanics in terms of the wave-like properties of particles in a field. Its answer is related to a particle's probability density in space and time.

02

Determine the uncertainty principle

Ψ(x)=hemαxh2when x0

Ψ(x)=hemαxh2 whenx0

x=2dx=0

x2=x2Ψ2dx=2h20x2e2h2dx

x=h42m2α2

σx=h22

dx=h2emαxh2 for x0

dx=h2emαxh2 for x0

dx=h3θ(x)emαxh2+θ(x)emαxh2

d2Ψdx2=h3δ(x)emαxh2+h2θ(x)emαxh2δ(x)emαxh2+h2θ(x)emαxh2

Here,

δ(x)=δ(x),

f(x)δ(x)=f(0)δ(x)

θ(x)+θ(x)=1

d2Ψdx2=h32δ(x)+h2emαxh2

p=0

p2=h2Ψd2Ψdx2dx

p2=h2mαh3emαxh22δ(x)+mαhemαxh2dx

p2=mαh222mαh20e2mαh2dx

p2=mαh21mαh2h22mα       =mαh2

p2=mαh2

σp=mαh

σxσp=h22mαmαh            =2h2>h2

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Most popular questions from this chapter

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.)

Solve the time-independent Schr ̈odinger equation for a centered infinite square well with a delta-function barrier in the middle:

V(x)={αδ(x)for-a<x<+afor|x|a

Treat the even and odd wave functions separately. Don’t bother to normalize them. Find the allowed energies (graphically, if necessary). How do they compare with the corresponding energies in the absence of the delta function? Explain why the odd solutions are not affected by the delta function. Comment on the limiting cases α → 0 and α → ∞.

Calculate (x),(x2),(p),(p2),σxandσp,for the nth stationary state of the infinite square well. Check that the uncertainty principle is satisfied. Which state comes closest to the uncertainty limit?

Although the overall phase constant of the wave function is of no physical significance (it cancels out whenever you calculate a measurable quantity), the relative phase of the coefficients in Equation 2.17 does matter. For example, suppose we change the relative phase of ψ1andψ2in problem 2.5:ψ(x,0)=A[ψ1x+eiϕψ2x]Where ϕis some constant. Find ψ(x,t),|ψx,t|2, and (x), and compare your results with what you got before. Study the special cases ϕ=π2andϕ=π.

In the ground state of the harmonic oscillator, what is the probability (correct to three significant digits) of finding the particle outside the classically allowed region?

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