Eightfold way (physics)

In the original eightfold way, the mesons were organized into octets and singlets. This is one of the finer points of differences between the eightfold way and the quark model it inspired, which suggests the mesons should be grouped into nonets (groups of nine).

The pseudo-scalar meson octet.

The eightfold way organizes eight of the lowest spin-0 mesons into an octet.[1][6] They are:

• 
  K⁰
  ,
  K⁺
  ,
  K⁻
  and
  K⁰
  kaons
• 
  π⁺
  ,
  π⁰
  , and
  π⁻
  pions
• 
  η
  

Diametrically opposite particles in the diagram are anti-particles of one-another while particles in the center are their own anti-particle.

The chargeless, strangeless eta prime meson was originally classified by itself as a singlet:

• 
  η′
  

Under the quark model later developed, it is better viewed as part of a meson nonet, as previously mentioned.

The J = 1/ 2  baryon octet.

The eightfold way organizes the spin-1/ 2  baryons into an octet. They consist of

• neutron (n) and proton (p)
• 
  Σ⁻
  ,
  Σ⁰
  , and
  Σ⁺
  sigma baryons
• 
  Λ⁰
  , the strange lambda baryon
• 
  Ξ⁻
  and
  Ξ⁰
  xi baryons

The J = 3/ 2  baryon decuplet.

The organizational principles of the eightfold way also apply to the spin-3/ 2  baryons, forming a decuplet.

• 
  Δ⁻
  ,
  Δ⁰
  ,
  Δ⁺
  , and
  Δ⁺⁺
  delta baryons
• 
  Σ^∗−
  ,
  Σ^∗0
  , and
  Σ^∗+
  sigma baryons
• 
  Ξ^∗−
  and
  Ξ^∗0
  xi baryons
• 
  Ω⁻
  omega baryon

However, one of the particles of this decuplet had never been previously observed when the eightfold way was proposed. Gell-Mann called this particle the
Ω⁻
and predicted in 1962 that it would have a strangeness −3, electric charge −1 and a mass near 1680 MeV/c². In 1964, a particle closely matching these predictions was discovered[7] by a particle accelerator group at Brookhaven. Gell-Mann received the 1969 Nobel Prize in Physics for his work on the theory of elementary particles.

Historically, quarks were motivated by an understanding of flavour symmetry. First, it was noticed (1961) that groups of particles were related to each other in a way that matched the representation theory of SU(3). From that, it was inferred that there is an approximate symmetry of the universe which is parametrized by the group SU(3). Finally (1964), this led to the discovery of three light quarks (up, down, and strange) interchanged by these SU(3) transformations.

The eightfold way may be understood in modern terms as a consequence of flavor symmetries between various kinds of quarks. Since the strong nuclear force affects quarks the same way regardless of their flavor, replacing one flavor of quark with another in a hadron should not alter its mass very much, provided the respective quark masses are smaller than the strong interaction scale—which holds for the three light quarks. Mathematically, this replacement may be described by elements of the SU(3) group. The octets and other hadron arrangements are representations of this group.

There is an abstract three-dimensional vector space:

${\displaystyle {\text{up quark}}\rightarrow {\begin{pmatrix}1\\0\\0\end{pmatrix}},\qquad {\text{down quark}}\rightarrow {\begin{pmatrix}0\\1\\0\end{pmatrix}},\qquad {\text{strange quark}}\rightarrow {\begin{pmatrix}0\\0\\1\end{pmatrix}}}$

and the laws of physics are approximately invariant under applying a determinant-1 unitary transformation to this space (sometimes called a flavour rotation):

${\displaystyle {\begin{pmatrix}x\\y\\z\end{pmatrix}}\mapsto A{\begin{pmatrix}x\\y\\z\end{pmatrix}},\quad {\text{where }}A{\text{ is in }}SU(3)}$

Here, SU(3) refers to the Lie group of 3×3 unitary matrices with determinant 1 (special unitary group). For example, the flavour rotation

${\displaystyle A={\begin{pmatrix}~\;~0&1&0\\-1&0&0\\~\;~0&0&1\end{pmatrix}}}$

is a transformation that simultaneously turns all the up quarks in the universe into down quarks and vice versa. More specifically, these flavour rotations are exact symmetries if only strong force interactions are looked at, but they are not truly exact symmetries of the universe because the three quarks have different masses and different electroweak interactions.

This approximate symmetry is called flavour symmetry, or more specifically flavour SU(3) symmetry.

Assume we have a certain particle—for example, a proton—in a quantum state ${\displaystyle |\psi \rangle }$. If we apply one of the flavour rotations A to our particle, it enters a new quantum state which we can call ${\displaystyle A|\psi \rangle }$. Depending on A, this new state might be a proton, or a neutron, or a superposition of a proton and a neutron, or various other possibilities. The set of all possible quantum states spans a vector space.

Representation theory is a mathematical theory that describes the situation where elements of a group (here, the flavour rotations A in the group SU(3)) are automorphisms of a vector space (here, the set of all possible quantum states that you get from flavour-rotating a proton). Therefore, by studying the representation theory of SU(3), we can learn the possibilities for what the vector space is and how it is affected by flavour symmetry.

Since the flavour rotations A are approximate, not exact, symmetries, each orthogonal state in the vector space corresponds to a different particle species. In the example above, when a proton is transformed by every possible flavour rotation A, it turns out that it moves around an 8 dimensional vector space. Those 8 dimensions correspond to the 8 particles in the so-called "baryon octet" (proton, neutron,
Σ⁺
,
Σ⁰
,
Σ⁻
,
Ξ⁻
,
Ξ⁰
,
Λ
). This corresponds to an 8-dimensional ("octet") representation of the group SU(3). Since A is an approximate symmetry, all the particles in this octet have similar mass.[8]

Every Lie group has a corresponding Lie algebra, and each group representation of the Lie group can be mapped to a corresponding Lie algebra representation on the same vector space. The Lie algebra ${\displaystyle {\mathfrak {su}}}$(3) can be written as the set of 3×3 traceless Hermitian matrices. Physicists generally discuss the representation theory of the Lie algebra ${\displaystyle {\mathfrak {su}}}$(3) instead of the Lie group SU(3), since the former is simpler and the two are ultimately equivalent.