Young tableaux and tensor product

In summary, the conversation discussed working on problems from Georgi's book in Lie algebras in particle physics and being stuck on one involving finding representations in the tensor product (2,1)x(2,1) in su(3) using Young tableaux. The first part was understood and a decomposition was provided, but the second part involved using "standard" Young's tableaux to determine which representations appear symmetrically or antisymmetrically in the tensor product. This was done by considering the permutation of the frames and determining if it was odd or even. An example was given to demonstrate this process.
  • #1
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I am working on all of the problems from Georgi's book in Lie algebras in particle physics (independent study), but I am stuck on one of them. The question is the following:

"Find (2,1)x(2,1) (in su(3) using Young tableaux). Can you determine which representations appear antisymmetrically in the tensor product, and which appear symmetrically?"

I understand the first part, and I get that (diagram - representation - dimension)

xxx (2,1) [15]
x

times

xxx (2,1) [15]
x

=

xxxxxx (4,2) [60]
xx

+

xxxxxx (5,0) [21]
x
x

+

xxxxx (2,3) [42]
xxx

+

xxxxx (3,1) [24]
xx
x

+

xxxx (0,4) [15]
xxxx

+

xxxx (1,2) [15]
xxx
x

+

xxx (0,1) [3]
xxx
xx

+

xxxxx (3,1) [24]
xx
x

+

xxxx (1,2) [15]
xxx
x

+

xxxx (2,0) [6]
xx
xx

I don't quite get the second part. How can one determine from this which representations appear symmetrically or antisymmetrically in the tensor product? Any suggestions?
 
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  • #2
To do part two you need to use the "standard" Young's tableaux, which are obtained by filling in the frames with integers in standard order, left to right and top to bottom. Use primed integers for the second factor. Thus the standard frames for (2,1) x (2,1) are:

1 2 3
4

1' 2' 3'
4'

You decomposed the direct product by starting with the first factor and attaching the squares of the second factor to it in all possible ways. So now in the tableau, consider the permutation 1 ↔ 1', 2 ↔ 2', etc. This is an involution, and therefore either an odd or even permutation. Even means that rep belongs to the symmetric part of the product, odd means it's antisymmetric.

For example, take [42], which was

xxxxx
xxx

The standard tableau is

1 2 3 1' 2'
4 3' 4'

Switching the 1's, 2's and 4's are all even since they only involve horizontal moves. But switching 3 with 3' is a vertical move, hence odd. We conclude therefore that [42] is antisymmetric.
 
Last edited:
  • #3
Awesome! Thanks for the help!
 

Related to Young tableaux and tensor product

1. What is a Young tableau?

A Young tableau is a graphical representation of a permutation in which the numbers 1 through n are arranged in a grid such that each row and column is strictly increasing. It is commonly used in the study of representation theory and combinatorics.

2. How are Young tableaux related to tensor products?

Young tableaux are used to compute the decomposition of a tensor product of representations into irreducible representations. This is known as the Littlewood-Richardson rule.

3. What is the significance of the shape of a Young tableau?

The shape of a Young tableau represents the irreducible representation that is obtained from the tensor product of the corresponding representations. The number of squares in each row represents the dimension of that irreducible representation.

4. How are Young tableaux used in the study of symmetric polynomials?

Young tableaux are used to construct and study symmetric polynomials, which are polynomials that remain unchanged under the permutation of their variables. The shape of a Young tableau is used to determine the degree and coefficients of the symmetric polynomial.

5. Can Young tableaux be extended to other mathematical objects?

Yes, Young tableaux can be extended to other mathematical objects such as Young diagrams, which are used to study partitions and their properties. They can also be extended to Kashiwara-Nakashima tableaux, which are used in the study of crystal bases and representation theory.

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