(a) A particle of spin1and a particle of spin 2 are at rest in a configuration such that the total spin is 3, and its z component is . If you measured the z component of the angular momentum of the spin-2particle, what values might you get, and what is the probability of each one?

(b) An electron with spin down is in the stateψ510of the hydrogen atom. If you could measure the total angular momentum squared of the electron alone (not including the proton spin), what values might you get, and what is the probability of each?

Short Answer

Expert verified

(a) 2with a probability equal to 1/15 , or with a probability of 8/15 or with a probability of 6/15 .

(b) The total is 3/2 or 1/2 withl(l+1)2=1542 and 342respectively. Also, for 1542the probability is 2/3 , and for 342it is 1/3 .

Step by step solution

01

Definition of Probability

The probability of an event occurring. The proportion of the total number of conceivable outcomes to the number of options in an exhaustive collection of equally likely outcomes that cause a given occurrence.

02

(a) Solve the total spin is 3, and its z  component is ℏ

Expand the composite spin 3,1>from the individual spins. For spin 2, the expected states are as follows,

|2,2>,|2,1>,|2,0>,|2,-1>, and 2,-2>.

Write the possible states for spin 1.

localid="1658127583657" |1,1>,|1,0>,and1,-1>.

The combinations that have a z projection equal to one are needed, so the expansion can be written as follows,

|3,1=α|2,2>|1,-1>+β|2,1>|1,0>+γ|2,0>|1,1

Determine the three expansion coefficients a ,β and γ in the Clebsch-Gordon tables. Then the probabilities are |α|2,|β|2 and γ2.

Return to the Clebsch-Gorden table and using the equation.

|sm=cm1m2mm1+m2=ms1s2s|s1m1>|s2m2>

Write the outcomes using the above information.

|31=115|22>|1-1>+815|21>|(100)+615|2011

Thus, 2 is obtained with a probability equal to 1/15 , orwith a probability of 8/15 or with a probability of 6/15 .

03

(b) Determination of the total angular momentum squared of the electron

Look the table 1×1/2 and write the outcome.

|10|12-12=2334-12+1312-12

So the total is 3/2 or 1/2 with l(l+1)2=1542and 342respectively.

Thus, for 1542the probability is 2/3 , and for 342it is 1/3 .

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Most popular questions from this chapter

(a) Apply S_tolocalid="1656131461017" 10>(Equation4.177), and confirm that you getlocalid="1656131442455" 2h1-1>.

(b) ApplyS+to[00>(Equation4.178), and confirm that you get zero.

(c) Show thatlocalid="1656131424007" 11>andlocalid="1656131406083" 1-1>(Equation4.177) are eigenstates ofS2, with the appropriate eigenvalue

In Problem4.3 you showed that Y21(θ,ϕ)=-15/8πsinθcosθeiϕ. Apply the raising operator to find localid="1656065252558" Y22(θ,ϕ). Use Equation 4.121to get the normalization.

(a) From the definition (Equation 4.46), construct n1(x)andn2(x).

(b) Expand the sines and cosines to obtain approximate formulas forn1(x)androle="math" localid="1656329588644" n2(x), valid whenx1.. Confirm that they blow up at the origin.

Determine the commutator of S2withSZ(1)(whereSS(1)+S(2)) Generalize your result to show that

[S2,S1]=2Ih(S1×S2)

Comment: Because Sz(1)does not commute with S2, we cannot hope to find states that are simultaneous eigenvectors of both. In order to form eigenstates ofS2weneed linear combinations of eigenstates ofSz(1). This is precisely what the Clebsch-Gordan coefficients (in Equation 4.185) do for us, On the other hand, it follows by obvious inference from Equation 4.187that the sumrole="math" localid="1655980965321" S(1)+S(2)does commute withdata-custom-editor="chemistry" S2, which is a special case of something we already knew (see Equation 4.103).

Work out the normalization factor for the spherical harmonics, as follows. From Section 4.1.2we know that

Ylm=BlmeimϕPlmcosθ

the problem is to determine the factor (which I quoted, but did not derive, in Equation 4.32). Use Equations 4.120, 4.121, and 4.130to obtain a recursion

relation giving Blm+1 in terms of Blm. Solve it by induction on to get Blm up to an overall constant Cl, .Finally, use the result of Problem 4.22 to fix the constant. You may find the following formula for the derivative of an associated Legendre function useful:

1-x2dPlmdx=1-x2Plm+1-mxPlm [4.199]

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