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Show that there is no acceptable solution to the Schrodinger equation for the infinite square well with E=0orE<0(This is a special case of the general theorem in Problem 2.2, but this time do it by explicitly solving the Schrodinger equation, and showing that you cannot meet the boundary conditions.)

Short Answer

Expert verified

Ecannot be less than zero because nis squared, also, it cannot be zero because if E=0then this will violate the uncertainty principle.

Step by step solution

01

Significance of the Schrodinger equation

The position of a particular electron is described in space and time using Schrodinger equation in the form of a mathematical expression. It considered the wave nature of the electron.

02

Identification of solution of the Schrodinger equation for infinite square wall

Write equation (2.27).

En=n2π222ma2

Encannot be negative because all the constants are positive or squared (that is., if we take n=±1,±2, the square will kill the negative signs, so Encannot be less than zero).

The other case in this problem when E=0(i.e.,n=0 ) is not accepted because Eis the eigenvalue of the total energy operator (we can think about it as the total energy of the wave function) which cannot be zero because this will violate the uncertainty principle.

Since if E=0this corresponds to zero kinetic energy (because E in the potential energy in the infinite potential well is zero), and zero kinetic energy corresponds to zero momentum, and the particle will rest inside the potential.

The calculation of the minimum kinetic energy by restricting the particle to move in a region of width Δxa(i.e., the length of the well) can be done, then using the uncertainty principle.

The calculation of the minimum uncertainty in the momentum can be done, so the result can beΔp/(2a) , so the minimum kinetic energy is2/(8ma2)where this result qualitatively agrees with the exact value of the ground state.

Thus, Ecannot be less than zero because nis squared, also, it cannot be zero because if E=0then this will violate the uncertainty principle.

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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?

a) Compute x,p,x2,p2, for the states ψ0and ψ1, by explicit integration. Comment; In this and other problems involving the harmonic oscillator it simplifies matters if you introduce the variable ξmωxand the constant α(mωπ)1/4.

b) Check the uncertainty principle for these states.

c) Compute T(the average kinetic energy) and V(the average potential energy) for these states. (No new integration allowed). Is their sum what you would expect?

Evaluate the following integrals:

(a)-3+1(x3-3x2+2x-1)δ(x+2)dx.

(b).0[cos(3x)+2]δ(x-π)dx

(c)_1+1exp(lxl+3)δ(x-2)dx

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.

A particle of mass m is in the potential

V(x)={,(x<0)-32h2ma2,(0xa)0,(x>a)

How many bound states are there?

In the highest-energy bound state, what is the probability that the particle would be found outside the well (x>a)? Answer: 0.542, so even though it is “bound” by the well, it is more likely to be found outside than inside!

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