The spin-flavor wavefunction of Sigma+

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SUMMARY

The discussion focuses on constructing the spin-flavor wavefunction of the baryon ##\Sigma_+##, starting from the known quark content of the proton, ##uud##. Participants highlight the use of ladder operators to derive baryon octet states and express challenges in determining both the flavor and spin wavefunctions for ##\Sigma_+##. Key references include Jerrold Franklin's work in Phys. Rev. 172, 1807 (1968), which provides insights into simple spin-flavor wavefunctions for baryons, and the importance of SU(3) flavor symmetry in this context.

PREREQUISITES
  • Understanding of baryon octet states and ladder operators
  • Familiarity with SU(3) flavor symmetry
  • Knowledge of spin and flavor wavefunctions for quarks
  • Experience with quantum mechanics, particularly spin-1/2 systems
NEXT STEPS
  • Study Jerrold Franklin's Phys. Rev. 172, 1807 for detailed spin-flavor wavefunctions
  • Learn about the derivation of the proton wavefunction in Thomson's book
  • Explore the implications of mixed symmetric and antisymmetric states in baryon wavefunctions
  • Research the applications of ladder operators in quantum chromodynamics (QCD)
USEFUL FOR

Particle physicists, graduate students in theoretical physics, and researchers interested in baryon structure and quantum chromodynamics.

Xico Sim
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Hi, guys.

If I want to write the spin-flavor wavefunction of ##\Sigma_+## starting only from knowing that the quark content of the proton is ##uud##, how can I procced?
I started by applying the ladder operators in order to get the baryon octet vertexes. I am now having problems with:
  1. determining the flavor wavefunction for the center octet states (including ##\Sigma_+##).
  2. determining the spin wavefunction for ##\Sigma_+##. Even if I suppose that the its spin state is ##|1/2,1/2\rangle##, there is more than one way for this to happen when we combine 3 spin 1/2 quarks...
Does anyone know a text where I can find something like this done in a comprehensive and detailed way? Or, alternatively, can you tell me a way to do it?
 
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Aren't sigma baryons strange ones? Are you using an SU(3) flavor symmetry?
As for the quarks they would be uus ? If you have more than 1 combination then you write them all, as you did for the proton [when you had the mixed symmetric states].
the flavor states can be obtained in a similar way by combining u,u and s.
 
The problem is that I did not understand the derivation of the proton wavefunction also: I found Griffiths, and for that matter every other text I found on the subject, quite confusing. Do you happen to know a place where it is clearly and thoroughly explained?
 
Using Thomson's book I understood the derivation of the proton spin-flavour wavefunction. I will try to apply what I learned to this case.
 
what is confusing?
 
ChrisVer said:
what is confusing?

To make myself clear, I posted my attempt. I arrived at the correct wavefunction, but I have a problem with it: even though it seems symmetric, I would expect it to be only mixed symmetric (only symmetric in 1,2), since ##X## is only symmetric in 1,2 and ##\phi## is completely symmetric...
 

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Why is phi symmetric? aren't you using a uds? I am sorry but I don't see why you wouldn't consider the antisymmetric singlet.
 
ChrisVer said:
I am sorry but I don't see why you wouldn't consider the antisymmetric singlet.

When determining ##X##?
 
when determining Phi...
you should have a symmetric one (in the triplet I=1 combination) : uds + dus
and an antisymmetric one (in the singlet I=0 combination) : uds - dus
they both correspond to I3=0
 
  • #10
Look at look at PR 172, 1807 for simple spin – flavor wave functions for baryons.
 
  • #11
clem said:
Look at look at PR 172, 1807 for simple spin – flavor wave functions for baryons.

What is PR?
 

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