Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

(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 .

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

(a) Work out the Clebsch-Gordan coefficients for the case s1=1/2,s2=anything. Hint: You're looking for the coefficients A and Bin

|sm=A|1212|s2(m-12)+B|12(-12)|s2(m+12)

such that|sm is an eigenstate of . Use the method of Equations 4.179 through 4.182. If you can't figure out whatSx(2) (for instance) does to|s2m2 , refer back to Equation 4.136 and the line before Equation 4.147. Answer:

;role="math" localid="1658209512756" A=s2+12±m2s2+1;B=±s2+12±m2s2+1

where, the signs are determined bys=s2±1/2 .

(b) Check this general result against three or four entries in Table 4.8.

(a) If you measured the component of spin angular momentum along the x direction, at time t, what is the probability that you would get +h/2?

(b) Same question, but for the ycomponent.

(c) Same, for the z component.

Starting from the Rodrigues formula, derive the orthonormality condition for Legendre polynomials:

-11Pl(x)PI(x)dx=(22l+1)δII.

Hint: Use integration by parts.

Deduce the condition for minimum uncertainty inSx andSy(that is, equality in the expression role="math" localid="1658378301742" σSxσSy(ħ/2)|<Sz>|, for a particle of spin 1/2 in the generic state (Equation 4.139). Answer: With no loss of generality we can pick to be real; then the condition for minimum uncertainty is that bis either pure real or else pure imaginary.

Consider the observablesA=x2andB=Lz .

(a) Construct the uncertainty principle forσAσB

(b) EvaluateσB in the hydrogen stateψn/m .

(c) What can you conclude about<xy>in this state?

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free