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.

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Most popular questions from this chapter

A hydrogen atom starts out in the following linear combination of the stationary states n=2, l=1, m=1 and n=2, l=1, m=-1.

ψ(r,0)=12(ψ211+ψ21-1)

(a) Constructψ(r,t)Simplify it as much as you can.

(b) Find the expectation value of the potential energy,<V>. (Does it depend on t?) Give both the formula and the actual number, in electron volts.

a) Check that the spin matrices (Equations 4.145 and 4.147) obey the fundamental commutation relations for angular momentum, Equation 4.134.

Sz=h2(100-1)(4.145).Sx=h2(0110),sy=h2(0-ii0)(4.147).[Sx,Sy]=ihSz,[Sy,Sz]=ihSx,[Sz,Sx]=ihSy(4.134).(b)ShowthatthePaulispinmatrices(Equation4.148)satisfytheproductruleσx(0110),σy(0-ii0),σz(100-1)(4.148).σjσk=δjk+io'IjklσI,(4.153).

Wheretheindicesstandforx,y,orz,ando'jklistheLevi-Civitasymbol:+1ifjkl=123,231,or2=312;-1ifjkl=132,213,or321;otherwise.

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) Use the recursion formula (Equation 4.76) to confirm that whenI=n-1 the radial wave function takes the form

Rn(n-1)=Nnrn-1e-r/na and determine the normalization constant by direct integration.

(b) Calculate 200a and <r2> for states of the form ψn(n-1)m·

(c) Show that the "uncertainty" in r(δr) is<r>/2n+1for such states. Note that the fractional spread in decreases, with increasing (in this sense the system "begins to look classical," with identifiable circular "orbits," for large ). Sketch the radial wave functions for several values of, to illustrate this point.

[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.

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