Remark:
We elaborate on two ways of checking where a map is actually a representation. This point was discussed a bit in Lecture 1, but since it will be used frequently throughout the course, I would like to emphasise this a bit further:
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(i)
Assume that a rule or formula is given for for every . In order to verify that really is a representation, one needs to either check or show that for all .
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(ii)
Frequently, we will just give the operators for a set of generators of a group . Since every element of can be written as a word in , if is required to be a homomorphism, then there is no choice in the values of for the other group elements : must be the product of the s corresponding to the decomposition of into a product of s. In order for this procedure to give a well-defined homomorphism on all of , it is both necessary and sufficient that the s satisfy the same relations as the s. (This is a general fact about any group homomorphism, not just ones into ).
Compare the phrasing of problems 12 and 13 below!
Problem 12. Verify that is a representation of , where is defined via
Solution: The operators are clearly linear (it is stated in the problem that they are in ), so it remains to check that is a homomorphism. We compute the action of a group product on a vector:
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showing that is indeed a homomorphism.
Problem 13. Writing , let be given by
Show that these operators define a representation of .
Solution: To check that the operators define a representation of , we simply to need to verify that and satisfy the same relations as and . We check this directly:
and
For the other group relation, we have
and
which are equal.
Problem 14.
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(a)
Find the matrices of all the elements of for the permutation
representation , with respect to the basis .
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(b)
Find another basis such that the matrices all take the form
and determine the unknown entries for your basis.
Solution:
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(a)
First note that . We then find the matrices for a generating set of . We have
and
This gives us
As is a homomorphism we can compute the remaining matrices by taking the product of the matrices corresponding to each generator. Thus
By a similar argument we get
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(b)
First we note that for any we have
so we pick to be our first basis element. Furthermore if we have for some then so our matrices will all take the form
We then have a choice for our other two basis vectors. Let and . Then clearly forms a basis of so we just need to compute each of the matrices. We proceed in a similar way to part (a), so
Thus the remaining matrices are
Problem 15. Let and be two representations of a group . Show that is a representation of , where
Remark: this is called the (direct) sum of two representations.
Solution: Given vector spaces , and any , , the map defined by
is in , since for all and ,
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Moreover, if and , then as
Applying this to , we have so it remains to show that is a homomorphism. We compute the image of a product: for all , , , we have
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where we used that and are homomorphisms for the second equality. This shows that is a homomorphism.
Problem 16. Let be a representation of a group . Given a subgroup , show that is a representation of .
Solution:
Since , and we have that for all . It remains to show that is a homomorphism. For any , we have
(the third equality holding since is a homomorphism for ).
Problem 17. Given a group action , let .
a) Show that is a representation of , where for every and , is defined via the formula
b) Show that is a not a representation of , where for every and , is defined via the formula
Solution:
We first verify that is linear: given , , and ,
Next we show that is a homomorphism: given , , and , we have
For part (b), we simply observe that the above calculation gives .
Problem 18. Prove the following:
Prop. 1.11 Let be a finite group and a representation of . Show that for every , there exists such that
Solution:
Since , for each , . By Lagrange’s theorem, hence
hence is a -th root of unity, and may therefore be written as for some .
Problem 19. Find all one-dimensional representations of .
Solution: Let be a one-dimensional vector space. Thus and for some . These numbers must satisfy the group relations, i.e.
Since , we then get that , hence Thus, for any , is a representation, where
is a representation. (This gives four isomporhism classes of one-dimensional representations of .)