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The wave functions for the ground and first excited states of a simple harmonic oscillator are Aebx2/2andBxebx2/2. Suppose you have two particles occupying these two states.

(a) If distinguishable, an acceptable wave function would berole="math" localid="1659955524302" Aebx12/2Bx2ebx22/2. Calculate the probability that both particles would be on the positive side of the origin and divide by the total probability for both being found over all values ofx1,x2. (This kind of normalizing-as-we-go will streamline things.)

(b) Suppose now that the particles are indistinguishable. Using the±symbol to reduce your work. calculate the same probability ratio, but assuming that their multiparticle wave function is either symmetric or antisymmetric. Comment on your results.

Short Answer

Expert verified

(a) The probability ratio is0.25

(b) The probability for symmetry is0.409and for anti symmetry is0.091

Step by step solution

01

Given information:

The ground state of simple harmonic oscillator is Aebx22.

The first excited state of simple harmonic oscillator is Bxebx22.

02

Concept of probability ratio

(a) The expression for probability ratio is given by,

R=(A20ebx12dx1)(B2x220ebx22dx2)((A2=etx12dx1))(B2x22ebx22dx2)

03

Evaluate probability ratio

(a) The probability ratio is calculated as,

R=A20zebx12dx1B2x220zebx22dx2A2zebx12dx1B2x22webx22dx2

R=A20webx12dx1B2x220webx22dx22A20mebx12dx12Bx220webx22dx2

R=14=0.25

04

Evaluate probability ratio

(b)

The probability ratio is calculated as,

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Most popular questions from this chapter

The general form for symmetric and antisymmetric wave functions isψn(x2)ψn(x2)±ψn(x1)ψn(x2) but it is not normalized.

(a) In applying quantum mechanics, we usually deal with quantum states that are "orthonormal." That is, if we integrate over all space the square of any individual-particle function, such asψn(x2)ψn(x2)±ψn(x1)ψn(x2), we get 1, but for the product of different individual-particle functions, such asψnφ(x)ψn,(x), we get 0. This happens to be true for all the systems in which we have obtained or tabulated sets of wave functions (e.g., the particle in a box, the harmonic oscillator, and the hydrogen atom). Assuming that this holds, what multiplicative constant would normalize the symmetric and antisymmetric functions?

(b) What valueAgives the vectorV=A(x^±y^)unit length?

(c) Discuss the relationship between your answers in (a) and (b)?

(a) To determine the repulsive energy between the two electrons in helium.

(b) To determine the distance of electrons that would have to be separated.

(c) To compare distance with approximate orbit radius in Z=2hydrogen like atom.

Question: Solving (or attempting to solve!) a 4-electron problem is not twice as hard as solving a 2-electrons problem. Would you guess it to be more or less than twice as hard? Why?

The subatomic omega particle has spin s=32. What angles might its intrinsic angular in momentum vector make with the z-axis?

Whether a neutral whole atom behaves as bosons or a fermion is independent of Z, instead depending entirely on the number of the neutrons in its nucleus. Why? What is it about this number that determines whether the atom is a boson or a fermion?

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