How Do Techni-Baryons Transform in SU(N_{TF}) and SU(2)_{spin} Symmetries?

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Discussion Overview

The discussion revolves around the transformation properties of techni-baryons (TCb) under the symmetries of ##SU(N_{TF})## and ##SU(2)_{spin}## within a model featuring ##SU(N_{TC})## techni-color symmetry and a global ##SU(N_{TF})_L \otimes SU(N_{TF})_R## symmetry. Participants explore the implications of these symmetries on the representations of TCb, particularly focusing on the conditions under which certain representations can be obtained or are necessary.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant proposes that TCb must be fully symmetric in spin and techni-flavour due to the antisymmetry in techni-color, suggesting that the TCb transforms under ##SU(2N_{TF})## like a completely symmetric representation.
  • Another participant argues that a representation that reduces to the trivial representation of ##S_{N_{TC}}## is sufficient, rather than requiring total symmetry.
  • There is a discussion about the conditions under which certain representations can be considered trivial after deleting rows with ##N_{TC}## or more boxes from the Young tableaux.
  • Participants question the equivalence of certain cycle representations and discuss the implications of the rules of Young tableaux on the reducibility of representations.
  • References to Georgi's work and the limitations of applying certain rules to ##S_4## representations are mentioned, highlighting the complexity of the representations involved.

Areas of Agreement / Disagreement

Participants express differing views on the necessity of total symmetry in the representations and the conditions under which representations can be considered trivial. There is no consensus on the correct approach to the transformation properties of TCb under the discussed symmetries.

Contextual Notes

Participants note limitations in applying certain rules of Young tableaux to ##S_4## due to the maximum number of boxes in irreducible representations. The discussion also highlights the need to consider the implications of deleting rows in the tableaux and the potential for reducibility of certain representations.

Andrea M.
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Consider a model with an exact ##SU(N_{TC})## techni-color symmetry and a ##SU(N_{TF})_L\otimes SU(N_{TF})_R## global techni-flavour symmetry which is spontaneously broken to the diagonal sub-group ##SU(N_{TF})## by condensates producing techni-pions (TC\pi) and techni-baryons(TCb).
What I'm trying to understand is how the various TCb transform under ##SU(N_{TF})## and ##SU(2)_{spin}##.
Because the wave-function is totally antisymmetric in techni-color we expect that TCb must be fully symmetric in spin and techni-flavour. Following the line of thought of Georgi's chapter 15 I have embedded ##SU(N_{TF})## and ##SU(2)_{spin}## in a ##SU(2N_{TF})##. The TCb transform under this ##SU(2N_{TF})## like a ##N_{TC}## completely symmetric combination, or in Young tableaux notation like a tableaux with ##N_{TC}## horizontal box. Now Georgi says that to understand what representation of ##SU(N_{TF})## and ##SU(2)_{spin}## are contained in the fully symmetric representation of ##SU(2N_{TF})## we must take the tensor product of all tableaux with ##N_{TC}## boxes of ##SU(N_{TF})## and ##SU(2)_{spin}## and see if they contain the fully symmetric representation. The results (see for example Chivukula, R.S. & Walker, T.P., 1989. Technicolor cosmology, Boston, MA: Boston Univ.) should be the following:
-For ##N_{TC}=3##
Schermata 2015-09-07 alle 17.55.43.png


-For ##N_{TC}=4##
Schermata 2015-09-07 alle 17.55.28.png

The problem is that, except for the ##N=3## case, I'm not able to obtain the fully symmetric representation by taking the tensor product of this tableaux.
 
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I don't think we necessarily need to have the totally symmetric representation of ##SU(2N_{TF})##, just a representation that reduces to the trivial representation of ##S_{N_{TC}}##. Any diagram that is trivial after deleting all rows with ##N_{TC}## or more boxes from the diagram will work. The totally symmetric representation for ##SU(2N_{TF}## will work, but so will others.

Looking at the products of the representations in your reference, we have
young1.JPG

where in the middle line we actually have a few copies of the trivial ##S_4## representation appearing. For the missing representations like
young2.JPG

we can see that we don't have enough boxes in the rows to make a trivial ##S_4## representation.
 
fzero said:
I don't think we necessarily need to have the totally symmetric representation of SU(2NTF)SU(2N_{TF}), just a representation that reduces to the trivial representation of SNTCS_{N_{TC}}.

Yes I agree with this.
fzero said:
Any diagram that is trivial after deleting all rows with NTCN_{TC} or more boxes from the diagram will work. The totally symmetric representation for SU(2NTFSU(2N_{TF} will work, but so will others

Why I can delete all the rows with ##N_{TC}## or more boxes?
Am I wrong or the trivial representation of ##S_4## is a Young tableaux with 4 horizontal boxes?
 
Andrea M. said:
Yes I agree with this.

Why I can delete all the rows with ##N_{TC}## or more boxes?
Am I wrong or the trivial representation of ##S_4## is a Young tableaux with 4 horizontal boxes?

Yes it is, but a Young tableaux with 4 horizontal columns of any equal size is also the trivial representation. So I mean delete in the same way that you would if you had a column with ##N## boxes for ##SU(N)##.
 
Could you suggest some reference where this result is derived?
 
Andrea M. said:
Could you suggest some reference where this result is derived?

Georgi discusses the Young tableaux for ##S_n## in sects 1.21-24. The trouble is that we already know that irreps of ##S_4## never have more than 4 boxes so not all of the rules there apply (for instance we can't naively compute the dimension using 8 as the number of boxes). But we can assign ##j##-cycles to the the boxes, so we get 4 2-cycles on 4 objects, which should be easy to show is reducible to 4 1-cycles.
 
fzero said:
But we can assign jj-cycles to the the boxes, so we get 4 2-cycles on 4 objects, which should be easy to show is reducible to 4 1-cycles.

Are you sure? For example the four 2-cycles (12)(23)(14)(23) do not seem to be equivalent to four 1-cycles.
 
Andrea M. said:
Are you sure? For example the four 2-cycles (12)(23)(14)(23) do not seem to be equivalent to four 1-cycles.

The rules of the Young Tableau are that the columns are the ##j##-cycles and that we can't repeat an index in the same row. If we had a valid diagram, we would never repeat an index in any box, but with more than ##n## boxes we have to relax something.

With the above rules we only get elements like (13)(21)(34)(42) that are always reducible.
 

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