(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

The raising and lowering operators change the value of m by one unit:

L±flm=(Alm)flm+1, (4.120).

Where Almare constant. Question: What is Alm, if the Eigen functions are to be normalized? Hint: First show thatL±is the Hermitian conjugate of L±(Since LxandLyare observables, you may assume they are Hermitian…but prove it if you like); then use Equation 4.112.

[Refer to Problem 4.59 for background.] In classical electrodynamics the potentials Aandφare not uniquely determined; 47 the physical quantities are the fields, E and B.

(a) Show that the potentials

φ'φ-Λt,A'A+Λ

(whereis an arbitrary real function of position and time). yield the same fields asφand A. Equation 4.210 is called a gauge transformation, and the theory is said to be gauge invariant.

(b) In quantum mechanics the potentials play a more direct role, and it is of interest to know whether the theory remains gauge invariant. Show that

Ψ'eiqΛ/Ψ

satisfies the Schrödinger equation (4.205) with the gauge-transformed potentialsφ'andA', SinceΨ'differs fromψonly by a phase factor, it represents the same physical state, 48and the theory is gauge invariant (see Section 10.2.3for further discussion).

[Refer to. Problem 4.59for background.] Suppose A=B02(X^-yI^) andφ=Kz2, where B0 and Kare constants.

(a) Find the fields E and B.

(b) Find the allowed energies, for a particle of mass m and charge q , in these fields, Answer: E(n1,n2)=(n1+12)ħω1+(n2+12)ħω2,(n1,n2=0,1,2,...)whereω1qB0/mandω22qK/m. Comment: If K=0this is the quantum analog to cyclotron motion;ω1 is the classical cyclotron frequency, and it's a free particle in the z direction. The allowed energies,(n1+12)ħω1, are called Landau Levels.

(a)Derive Equation 4.131 from Equation 4.130. Hint: Use a test function; otherwise you're likely to drop some terms.

(b)Derive Equation 4.132 from Equations 4.129 and 4.131 .Hint : Use Equation 4.112.

(a) Find〈r〉and〈r²〉for an electron in the ground state of hydrogen. Express your answers in terms of the Bohr radius.

(b) Find〈x〉and (x2)for an electron in the ground state of hydrogen.

Hint: This requires no new integration—note that r2=x2+y2+z2,and exploit the symmetry of the ground state.

(c) Find〈x²〉in the state n=2,l=1,m=1. Hint: this state is not symmetrical in x, y, z. Usex=rsinθcosπx=rsinθcosϕ

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