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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?

Short Answer

Expert verified

Total orbital angular momentum isL=2h.

Step by step solution

01

Total spin of two electrons

The total spin of the two electronsSTis

ST=ST(ST+1)h ….(1)

02

total spin quantum number

The quantum number jT is zero jT=0.

The spin quantum number of each electron is s1=s2=12.

By using Hund's rule, we conclude that the total spin quantum number st is given by

ST=s1+s2=12+12ST=1

03

total spin of electrons

By using Eq. (I), we find the total spin of the electrons sT as

ST=sTsT+1h=1.1+1hST=2h

04

The total orbital angular momentum LT

Now, since jT=0, we conclude that the total orbital angular momentum LT must be equal to the total spin ST

LT=ST=2h

Hence the total orbital angular momentum is LT=2h.

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Most popular questions from this chapter

Identify the different total angular momentum states j,mj allowed a 3d electron in a hydrogen atom.

Determine the electronic configuration for phosphorus, germanium and cesium.

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.

Two particles in a box occupy the n=1andn'=2individual-particle states. Given that the normalization constant is the same as in Example8.2(see Exercise 36), calculate for both the symmetric and antisymmetric states the probability that both particles would be found in the left side of the box (i.e., between 0 and13L)?

Question: In nature, lithium exists in two isotopes: lithium-6, with three neutrons in its nucleus, and lithium-7, with four as individual atoms, would these behave as Bosons or as Fermions? Might a gas of either behave as a gas of Bosons? Explain.

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