Your friends ask: “Why is there an exclusion principle?” Explain in the simplest terms.

Short Answer

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The two electrons cannot have all quantum numbers the same including spin, and cannot be in the same one-electron states.

Step by step solution

01

Introduction.

If a system of particles comprises electrons or a system of protons, then the particles are said to be identical when interchanging any of the two particles of the same kind does not change anything about the system. It means the magnitude-squared of the wave function, which gives the probability density, must remain the same when the coordinates of any two electrons are interchanged.

If the wave function involves a pair of particles each in one of two different one-electron states, interchanging the particles (putting each in the state of the other) and doing it again multiplies the wave function with any spin included. This is possible only if a single exchange of particles multiples the wave function or by or.

For electrons, and other particles with half-integer spins, interchanging the quantum numbers of the two electrons always multiplies the wave function.

02

for electrons and other particles with half-integer spin.

Symbolically, changing the quantum numbers of the two electrons must change the sign,

ψn,n'(rI2r2)=ψn',n(rI2r2)

Here, denotes the first set of one-electron quantum number and n'the second electron’s set of quantum numbers. But if the two electrons have all the same quantum numbers, the wave function becomes role="math" localid="1655379141692" ψn,n(r1r2)and the requirements that exchanging quantum numbers,

ψn,n'(r1,r2)=-ψn.n(r1,r2)

This requires the impossible condition that ψn,n(r1r2)is identically zero.

Conclusion: Therefore, The two electrons cannot have all quantum numbers the same including spin, and cannot be in the same one-electron states.

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Most popular questions from this chapter

The 21cm Line: One of the most important windows to the mysteries of the cosmos is the 21cm line. With it astronomers map hydrogen throughout the universe. An important trait is that it involves a highly forbidden transition that is, accordingly, quite long-lived. But it is also an excellent example of the coupling of angular momentum. Hydrogen's ground state has no spin-orbit interaction—forl=0there is no orbit. However, the proton and electron magnetic moments do interact. Consider the following simple model.

(a) The proton seesitself surrounded by a spherically symmetric cloud of 1s electron, which has an intrinsic magnetic dipole moment/spin that of course, has a direction. For the purpose of investigating its effect the proton, treat this dispersed magnetic moment as behaving effectively like a single loop of current whose radius isa0then find the magnetic field at the middle of the loop in terms of e,,me , μ0anda0.

(b) The proton sits right in the middle of the electron's magnetic moment. Like the electron the proton is a spin12particle, with only two possible orientations in a magnetic field. Noting however, that its spin and magnetic moment are parallel rather than opposite, would the interaction energy be lower with the proton's spin aligned or anti-aligned with that of the electron?

(c) For the protongρ.is 5.6. Obtain a rough value for the energy difference between the two orientations.

(d) What would be the wavelength of a photon that carries away this energy difference?

The angles between S and μSand between L and μLare 180o. What is the angle between J and μJ in a2p32state of hydrogen?

Question: Concisely, why is the table periodic?

The total-spin singlet state for two electrons has one spin up and one down, but one of the triplet states does. too. What is the difference?

Using the general rule for adding angular momenta discussed in Section 8.7 and further in Exercise 66, Find the allowed values ofjTfor three spin 12 fermions. First add two, then add the third.

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