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

Quarks carry spin 1/2. Three quarks bind together to make a baryon (such as the proton or neutron); two quarks (or more precisely a quark and an antiquark) bind together to make a meson (such as the pion or the kaon). Assume the quarks are in the ground state (so the orbital angular momentum is zero).

(a) What spins are possible for baryons?

(b) What spins are possible for mesons?

Short Answer

Expert verified

(a) Spin 12or 32

(b) Spin 1 or 0

Step by step solution

01

Definition of baryon and meson

The subatomic particles having large mass and are the combination of three quarks are known as baryons.

The existence quark and an antiquark in a subatomic particle are termed Meson

02

(a) Determination of possible spins for baryon

Combine two quarks,12and12.

Spin 1 (If they are parallel),

12+12or-12+-12

Zero (If they are antiparallel),

role="math" localid="1658124052031" 12+-12or12+-12

Combine the result with the third quark for the case to get spin1, 12 and1.

32(if they are parallel),

12+1or-12-1

12(if they are antiparallel),

role="math" localid="1658123797200" -12+1or12-1

For the case to get zero, only 12 is there only.

Thus, the possible spins for baryons are 12and 32.

03

(b) Determination of possible spins for mesons

Combine two quarks, 12 and 12.

Spin 1 (if they are parallel),

12+12or-12+-12

Zero (if they are antiparallel),

12+-12or12+-12

Thus, the possible spins for mesons are 1 and 0.

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

Coincident spectral lines. 43According to the Rydberg formula (Equation 4.93) the wavelength of a line in the hydrogen spectrum is determined by the principal quantum numbers of the initial and final states. Find two distinct pairs{ni,nf} that yield the same λ. For example,role="math" localid="1656311200820" {6851,6409} and{15283,11687}will do it, but you're not allowed to use those!

(a) Construct the spatial wave function (ψ)for hydrogen in the state n=3,I=2,m=1.Express your answer as a function of r,θ,ϕ,anda(the Bohr radius) only—no other variables (p,z,etc.) or functions (p,v,etc.), or constants (A,c0,etc.), or derivatives, allowed (π is okay, and e, and 2, etc.).

(b) Check that this wave function is properly normalized, by carrying out the appropriate integrals over, θ,andϕ.

(c) Find the expectation value of rsin this state. For what range of s (positive and negative) is the result finite?

The fundamental commutation relations for angular momentum (Equation 4.99) allow for half-integer (as well as integer) eigenvalues. But for orbital angular momentum only the integer values occur. There must be some extra constraint in the specific formL=r×p that excludes half-integer values. Let be some convenient constant with the dimensions of length (the Bohr radius, say, if we're talking about hydrogen), and define the operators

q112[x+a2/ħpy];p112[px-(ħ/a2)y];q212[x-(a2/ħ)py];p212[px-(ħ/a2)y];

(a) Verify that [q1,q2]=[p1,p2]=0;[q1,p1]=[p2,q2]=iħ. Thus the q's and the p's satisfy the canonical commutation relations for position and momentum, and those of index 1are compatible with those of index 2 .

(b) Show that[q1,q2]=[p1,p2]Lz=ħ2a2(q12-q22)+a22ħ(p12-p22)

(c) Check that , where each is the Hamiltonian for a harmonic oscillator with mass and frequency .

(d) We know that the eigenvalues of the harmonic oscillator Hamiltonian are , where (In the algebraic theory of Section this follows from the form of the Hamiltonian and the canonical commutation relations). Use this to conclude that the eigenvalues of must be integers.

(a) Construct the wave function for hydrogen in the state n=4,I=3,m=3. Express your answer as a function of the spherical coordinates r,θandϕ.

(b) Find the expectation value of role="math" localid="1658391074946" rin this state. (As always, look up any nontrivial integrals.)

(c) If you could somehow measure the observable Lx2+Ly2on an atom in this state, what value (or values) could you get, and what is the probability of each?

(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.

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