5.2. QUARK MODEL 285
Table 5.7
mesons I I 3 Q S Jπ m(MeV)
pn π+ 1 1 1 0 0 − ∼ 140
−pn π− 1 -1 -1 0 0 − ∼ 140
nn√−pp
2 π
0 1 0 0 0 0 − ∼ 140
pΛ K+^1212110 − ∼ 495
nΛ K^012 −^12010 − ∼ 495
Λn K
(^01)
2
1
2 0 -1^0
− ∼ 495
Λp K−^12 −^12 -1 -1 0 − ∼ 495
nn+p√p− 2 ΛΛ
6 η^00000
− ∼ 548
nn+p√p+ΛΛ
3 η
′ 0 0 0 0 0 − ∼ 548
In view of the irreducible representations ofSU( 3 ):
3 ⊗ 3 = 8 ⊕ 1 ,
3 ⊗ 3 ⊗ 3 = 10 ⊕ 8 ⊕ 8 ⊕ 1 ,
it is natural to guess the relations (5.2.18) or (5.2.19), i.e.
(5.2.66)
mesons= 3 ⊗ 3 = 8 ⊕ 1 ,
baryons= 3 ⊗ 3 ⊗ 3 = 10 ⊕ 8 ⊕ 8 ⊕ 1.
According to the Physical Explanation5.5, we infer immediately, from (5.2.66), that the
hadrons in the Eightfold Way are composed of three fundamental particles, denoted by
(5.2.67) q 1 , q 2 , q 3
and mesons consist of a fundamental particle and an antiparticle. In a nutshell, baryons
consist of three fundamental particles:
(5.2.68)
mesons=qiqj for 1≤i,j≤ 3 ,
baryons=qiqjqk for 1≤i,j,k≤ 3.
Physicists Gell-Mann and Zweig did this work independentlyin 1964, and presented the
celebrated Quark Model. The three fundamental particles (5.2.67) were termed the up, down
and strange quarks by Gell-Mann, denoted by
q 1 =u, q 2 =d, q 3 =s.
Zweig called these particles the aces.
By using the three quarks(u,d,s)to replace the sakataons(p,n,Λ), we can perfectly
explain all hadrons described by the Eightfold Way, i.e. thehadrons given by (5.2.1)-(5.2.4).
An important step to establish the quark model is to determine the quantum numbers of
quarks, which are introduced in the following several procedures: