Spin Algebra for a spin operator ‘J’: ‘Isospin operator ‘I’ follows this same algebra Isospin is also additive. Two particles with Isospin I a and I b will give a total Isospin I = I a + I b Last Time: By defining I + = I 1 + iI 2 and I - = I 1 - iI 2 we could ‘Raise’ and ‘Lower’ the third component of isospin: I - |i,m> = [i(i+1)-m(m-1)] 1/2 |i,m-1> I + |i,m> = [i(i+1)-m(m+1)] 1/2 |i,m+1> NOTICE: I + |1/2,-1/2> = I + |d> = |u> (or -|d-bar>) All part of what we called SU(2)
Concept Developed Before the Quark Model Only works because M(up) M(down) Useful concept in strong interactions only Often encountered in Nuclear physics From SU(2), there is one key quantum number I 3 Up quark Isospin = 1/2; I 3 = 1/2 Anti-up quark I = 1/2; I 3 = -1/2 Down quark I = 1/2; I 3 = -1/2 Anti-down quark I = 1/2; I 3 = 1/2
I3I3 0 1/2 -1/2 1 Graphical Method of finding all the possible combinations: 1). Take the Number of possible states each particle can have and multiply them. This is the total number you must have in the end. A spin 1/2 particle can have 2 states, IF we are combining two particles: 2 X 2 = 4 total in the end. 2) Plot the particles as a function of the I 3 quantum numbers.
I3I3 0 1/2 -1/2 1 Graphical Method of finding all the possible combinations: I3I3 0 1/2 -1/2 1 I3I3 0 1/2 -1/2 1 Triplet Singlet Group A Group B Sum
Graphical Method of finding all the possible combinations: We have just combined two fundamental representations of spin 1/2, which is the doublet, into a higher dimensional representation consisting of a group of 3 (triplet) and another object, the singlet. What did we just do as far as the spins are concerned? Quantum states: Triplet I = |I, I 3 > |1,1> = |1/2,1/2> 1 |1/2,1/2> 2 |1,0> = 1/ 2 (|1/2,1/2> 1 |1/2,-1/2> 2 + |1/2,-1/2> 1 |1/2,1/2> 2 ) |1,-1> = |1/2,-1/2> 1 |1/2,-1/2> 2 Singlet |0,0> = 1/ 2 (|1/2,1/2> 1 |1/2,-1/2> 2 - |1/2,-1/2> 1 |1/2,1/2> 2 )
Quantum states: Triplet I = 1 |I, I 3 > |1,1> = |1/2,1/2> 1 |1/2,1/2> 2 = -|ud> |1,0> = 1/2(|1/2,1/2> 1 |1/2,-1/2> 2 + |1/2,-1/2> 1 |1/2,1/2> 2 ) = 1/2(|uu> - |dd>) |1,-1>= |1/2,-1/2> 1 |1/2,-1/2> 2 = |ud> Singlet|0,0>=1/2(|1/2,1/2> 1 |1/2,-1/2> 2 - |1/2,-1/2> 1 |1/2,1/2> 2 =1/2(|uu> + |dd>) Reminder: u = |1/2,1/2> u-bar or d = |1/2,-1/2> Must choose either quark-antiquark states, or q-q states. We look for triplets with similar masses. MESONs fit the bill! +, 0, - and +, 0, - (q-qbar pairs). 0, 0, and 0 are singlets. WARNING: Ask about |1,0> minus sign or read Burcham & Jobes pgs. 361 and 718
But quarks are also in groups of 3 so we’d like to see that structure too: I3I3 0 1/2 -1/2 1 I3I3 0 1/2 -1/2 1 I3I3 0 1/2 -1/2 1 3/2 -3/2 s a
Isospins of a few baryon and meson states: