Repeat example 8.6 but assume that the upper state is the 2p12rather than the2p32

Short Answer

Expert verified

The 1s12and 2p12states are both split into two levels.

Step by step solution

01

 Step 1: Concept of the ordering Rule for Z- projection.

The ordering rule for the quantum number of the z-projection of the total angular momentum mjis:mj=-j,-j+1,....,j-1,j

Here Jis the quantum number for the total angular momentum.

02

Determine the state of two levels which is split

The J 's for the1s12 and2p12states are both12since that's what the subscripts of the states are. Consequently, the's are given by:

mj=-12,+12

The 1s12and2p12states are both split into two levels.

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Most popular questions from this chapter

In its ground state, carbon's 2pelectrons interact to produce jT=0. Given Hund's rule. what does this say about the total orbital angular momentum of these electrons?

Exercise 44 gives an antisymmetric multiparticle state for two particles in a box with opposite spins. Another antisymmetric state with spins opposite and the same quantum numbers is ψn(x1)n2(x2)ψnn(x1)ψn(x2)

Refer to these states as 1 and 11. We have tended to characterize exchange symmetry as to whether the state's sign changes when we swap particle labels. but we could achieve the same result by instead swapping the particles' stares, specifically theandin equation (8-22). In this exercise. we look at swapping only parts of the state-spatial or spin.

(a) What is the exchange symmetric-symmetric (unchanged). antisymmetric (switching sign). or neither-of multiparticle states 1 and Itwith respect to swapping spatial states alone?

(b) Answer the same question. but with respect to swapping spin states/arrows alone.

(c) Show that the algebraic sum of states I and II may be written(ψn(x1)ψn'(x2)ψn'(x1)ψn(x2))(+)

Where the left arrow in any couple represents the spin of particle 1 and the right arrow that of particle?

(d) Answer the same questions as in parts (a) and (b), but for this algebraic sum.

(e) ls the sum of states I and 11 still antisymmetric if we swap the particles' total-spatial plus spin-states?


(f) if the two particles repel each other, would any of the three multiparticle states-l. II. and the sum-be preferred?

Explain.

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

Consider Z=19potassium. As a rough approximation assume that each of itsn=1electron s orbits 19 pro. tons and half an electron-that is, on average, half its fellown=1electron. Assume that each of itsn=2electrons orbits 19 protons, two Is electrons. and half of the seven othern=2electrons. Continue the process, assuming that electrons at eachorbit a correspondingly reduced positive charge. (At each, an electron also orbits some of the electron clouds of higher. but we ignore this in our rough approximation.)

(a) Calculate in terms ofa0the orbit radii of hydrogenlike atoms of these effective Z,

(b) The radius of potassium is often quoted at around0.22nm. In view of this, are yourn=1throughn=3radii reasonable?

(c) About how many more protons would have to be "unscreened" to then=4electron to agree with the quoted radius of potassium? Considering the shape of its orbit, should potassium'sn=4electron orbit entirely outside all the lower-electrons?

Exercise 45 refers to state I and II and put their algebraic sum in a simple form. (a) Determine algebraic difference of state I and state II.

(b) Determine whether after swapping spatial state and spin state separately, the algebraic difference of state I and state II is symmetric, antisymmetric or neither, and to check whether the algebraic difference becomes antisymmetric after swapping spatial and spin states both.

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