Quark Model (Supermultiplet and States questions)

In summary: So the decuplet is a simpler place to start. In summary, Ryder explains how a supermultiplet of ten baryons can be formed by classifying the possible states based on their symmetry under interchange of quark labels. This results in 27 states, with one totally anti-symmetric state and ten symmetric states. These symmetric states correspond to the baryon decuplet and have a spin of 3/2. Ryder also clarifies that the decuplet is symmetric under flavor and that the proton is part of a more complex octet.
  • #1
Elwin.Martin
207
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From Ryder:
"We can now see how a supermultiplet of ten baryons may arise. Baryons are made of three identical fermions, so the possible states may be classified according to their symmetry under interchange of quark labels. Altogether there are 27 states. One of these is totally anti-symmetric: uds+dsu+sud-usd-sdu-dus,
and ten symmetric states:
uuu,
ddd,
sss,
uud+udu+duu,
uus+usu+suu,
udd+ddu+dud,
uss+ssu+sus,
dds+dsd+sdd,
dss+ssd+sds,
uds+dsu+sud+usd+sdu+dus"

I am a little bit lost here, first question:
what is a supermultiplet...? Also, what does he mean by interchange of quark labels?

second question:
How are these states supposed to clearly follow from the existence of 27 states...? I'm not really sure how I'd come up with these states.

For "uud+udu+duu"
(assuming I'm not missing something really obvious) my first thought was "2 up quarks, 1 down...proton"? I feel like I'm missing something obvious here, besides the idea that the terms don't commute (which I'm guessing is part of this). Wait, it said these were non-normalized...normalized would we have 1/sqrt 3(uud+udu+duu) and then the whole thing would just be the different states of a proton? I feel like I'm seriously over simplifying at this point.

Thanks for any and all help,

Elwin
 
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  • #2
Elwin, In Ryder's terminology, a multiplet is a group of particles related to each other under isospin, and a supermultiplet is a group of particles related to each other under SU(3). (Usually, I think, the term 'supermultiplet' is reserved for SU(4) and higher, but Oh well.)

By quark labels he means the flavors u, d, s. There are 27 possible states (33 = 27.)

Each of the 27 states has a certain charge and strangeness. The ten states he's listing form the baryon decuplet, and to form the ten, he takes the states having similar charge and strangeness and forms the symmetric combination. So starting with uus we get uus + usu + suu.

Since the overall symmetry of a fermion state (space, spin, flavor, color) must be antisymmetric, the decuplet is symmetric under spin, i.e. spin 3/2. So uud+udu+duu is not a proton, it's a resonance usually called Δ+, or the "3,3" resonance.
 
  • #3
Bill_K said:
Elwin, In Ryder's terminology, a multiplet is a group of particles related to each other under isospin, and a supermultiplet is a group of particles related to each other under SU(3). (Usually, I think, the term 'supermultiplet' is reserved for SU(4) and higher, but Oh well.)

By quark labels he means the flavors u, d, s. There are 27 possible states (33 = 27.)

Each of the 27 states has a certain charge and strangeness. The ten states he's listing form the baryon decuplet, and to form the ten, he takes the states having similar charge and strangeness and forms the symmetric combination. So starting with uus we get uus + usu + suu.

Since the overall symmetry of a fermion state (space, spin, flavor, color) must be antisymmetric, the decuplet is symmetric under spin, i.e. spin 3/2. So uud+udu+duu is not a proton, it's a resonance usually called Δ+, or the "3,3" resonance.

How do we know that the decuplet won't be antisymmetric under something like color...? Is it because hadrons are colorless? I know it's antisymmetric under space (Pauli exclusion principle). What does it mean to be symmetric under flavor? I know what the flavors are, is it just symmetric because of the additive nature of the states?

Thanks for your help :) Sorry if I'm asking slightly stupid questions
 
  • #4
Elwin, Not at all. Good questions. A hadron is colorless, which means it's a color singlet, i.e. the color part is totally antisymmetric.
The space part is (almost always) L=0, so totally symmetric.
That leaves the spin part and flavor part, which must both have the same symmetry "S". So that (antisymmetric x symmetric x S x S) works out to be antisymmetric overall, for a fermion state.

As I said, the decuplet has a symmetric flavor state, so the spin state must be the same - symmetric also.

Ryder focused on the decuplet because the octet which contains the proton is a bit more complicated to describe. It has "mixed" symmetry (neither totally symmetric nor totally antisymmetric) As likewise the coupling of the three spins to total spin 1/2 is mixed.
 

1. What is the Quark Model?

The Quark Model is a theoretical framework used in particle physics to explain the structure and behavior of subatomic particles. It states that protons and neutrons, which make up the nucleus of an atom, are composed of smaller particles called quarks.

2. What is a supermultiplet in the Quark Model?

A supermultiplet is a group of particles that have similar properties and are believed to be made up of the same type of quarks. In the Quark Model, there are three supermultiplets: baryons, mesons, and leptons.

3. What are the different types of states in the Quark Model?

The different types of states in the Quark Model refer to the different ways that quarks can combine to form particles. These include the ground state, excited states, and hybrid states.

4. How does the Quark Model explain the properties of particles?

The Quark Model explains the properties of particles by assigning each particle a specific combination of quarks. The properties of the particle, such as spin and charge, are determined by the properties of the quarks that make it up.

5. What evidence supports the Quark Model?

The Quark Model has been supported by numerous experiments, including scattering experiments and high-energy particle collisions. Additionally, the predictions made by the Quark Model have been confirmed by the discovery of new particles that fit into the model's framework.

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