Understanding the baryon wavefunction

In summary, the conversation discusses the concept of symmetry in the quark model and how it applies to combinations of baryon wavefunctions. It is explained that in order for the wavefunction to be antisymmetric under the interchange of two quarks, the combination of flavour and spin must be symmetric. Several examples are given to illustrate this concept, including a three-particle state with one u, one d, and one s quark. The conversation ends with the appreciation of a clear and concise explanation of the concept.
  • #1
gboff21
50
0
If a baryon wavefunction is [itex]\Psi = \psi_{spatial} \psi_{colour} \psi_{flavour} \psi_{spin}[/itex],
and we consider the ground state (L=0) only.
We know that the whole thing has to be antisymmetric under the interchange of two quarks. We know that colour is antisymmetric (always colourless) and spatial is symmetric. Therefore, the combination of flavour and spin has to be symmetric.
That's fine, I understand that. However, I'm very uncertain about what the 'interchange of two quarks' actually means. Interchange how?

For the 'easy' example of |uuu>. How is the flavour symmetric?

Basically, what does it mean to be symmetric in the quark model?
 
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  • #2
In the notation, interchanging two quarks just means changing which quark you write first and which one you write second. Nature does not label them "quark 1" and "quark 2"--all she knows is "there are two quarks"--so any expression you write down had better be agnostic about which quark is "first" and which is "second" (up to an overall minus sign in the case of fermions).

Anyway, the best way to get started is probably with examples. Suppose there were particles composed of two quarks. Here are some flavor-symmetric states:

|uu>, |dd>, (|uu> + |dd>)

Here is a flavor-antisymmetric state:

(|ud> - |du>)

[If you swap the first and second quark, you get (|du> - |ud>), which is the negative of the original state.]

Here is a state without definite flavor symmetry (it is a linear combination of a flavor-symmetric and a flavor-antisymmetric state):

|ud>

[If you swap the first and second quark, you get |du>, which is not a multiple of the original state.]

Here is a three-particle example. What is the only totally symmetric flavor state with one u, one d, and one s quark? It is

(|uds> + |usd> + |dus> + |dsu> + |sud> + |sdu>)

For example, on exchanging the first and second quark you get the state

(|dus> + |sud> + |uds> + |sdu> + |usd> + |dsu>)

which you can verify is the same state as we started with.
 
  • #3
Thank you very much. I've been searching everywhere for a clear concise explanation! The answer is actually quite simple when you know about it!
Thanks again
 

Related to Understanding the baryon wavefunction

1. What is a baryon wavefunction?

A baryon wavefunction is a mathematical representation of the spatial and spin properties of a baryon, which is a type of subatomic particle made up of three quarks. This wavefunction describes the probability distribution of finding the baryon at a certain position and spin state.

2. How is the baryon wavefunction related to the strong nuclear force?

The baryon wavefunction is a fundamental aspect of the theory of quantum chromodynamics (QCD), which describes the behavior of the strong nuclear force. In QCD, the baryon wavefunction is used to calculate the interactions between quarks, which are responsible for the strong force that binds protons and neutrons together in the nucleus.

3. How is the baryon wavefunction different from the electron's wavefunction?

The baryon wavefunction is a multi-dimensional function that describes the properties of three quarks, while the electron's wavefunction is a single-dimensional function that describes the properties of only one particle. Additionally, the baryon wavefunction is subject to the strong nuclear force, while the electron's wavefunction is subject to the electromagnetic force.

4. Can the baryon wavefunction be experimentally observed?

No, the baryon wavefunction itself cannot be directly observed. However, its effects can be observed through experiments that measure the properties of baryons, such as their mass and spin. The accuracy of these measurements can also provide evidence for the validity of the baryon wavefunction model.

5. How does understanding the baryon wavefunction contribute to our understanding of the universe?

The baryon wavefunction is a fundamental aspect of the standard model of particle physics, which explains the behavior of all known particles and their interactions. By understanding the baryon wavefunction, we can better understand the structure and behavior of matter at the subatomic level, and ultimately gain a deeper understanding of the physical laws that govern our universe.

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