10 Problems for Epiphany

10.1 Problems for section 5

Problem 49.
  1. 1.

    Compute exp⁡(X) for X equal to (t00s), (0t−t0), and (0tt0) (where s,t∈ℝ).

  2. 2.

    Let Ea,b be the elementary n×n matrix with 1 in the (a,b)-entry and 0 elsewhere. Compute exp⁡(t⁢Ea,b) for a≠b and a=b.

Problem 50.

Show that

exp⁡(t⁢X)⁢exp⁡(t⁢Y)=exp⁡(t⁢(X+Y)+t22⁢[X,Y]+O⁢(t3))

as t→0, where

[X,Y]=X⁢Y−Y⁢X.
Problem 51.

Let 𝔫 be the ℂ-vector space of strictly upper triangular matrices (0’s on the diagonal) and let N={g∈GLn⁡(ℂ):g=I+X,X∈𝔫}.

In this problem we will see that the restriction of the exponential to 𝔫 is a homeomorphism onto N (i.e. a continuous bijection with continuous inverse).

  1. 1.

    Let X∈𝔫. Show that Xn=0.

  2. 2.

    Show that exp⁡(X)∈N for X∈𝔫.

  3. 3.

    Show that, for g∈N, the logarithm log⁡(g)=∑k=1∞(−1)k+1⁢(g−I)kk is in fact a finite sum (and hence converges).

  4. 4.

    Show that exp|𝔫 and log|N are inverses of each other. Hint: this boils down to an identity of formal power series, which you can actually deduce from the corresponding fact over ℝ.

Problem 52.
  1. 1.

    Using the previous question, fill in the gaps of the proof from the notes that

    exp:𝔤⁢𝔩n,ℂ→GLn⁡(ℂ)

    is surjective.

  2. 2.

    (+) Is the exponential map exp:𝔰⁢𝔩2,ℂ→SL2⁡(ℂ) surjective? What about exp:𝔤⁢𝔩2,ℝ→GL2+⁡(ℝ)?

Problem 53.

Let v∈ℝ3 be a unit vector and let f:ℝ→S⁢O⁢(3) be the map with f⁢(θ) being rotation by θ about the axis v (the angle is measured anticlockwise as you look along the vector from the origin).

Show that f is a one-parameter subgroup and find its infinitesimal generator in terms of v.

Problem 54.

Prove that the Lie algebra of U⁢(n) is

𝔲n={X∈𝔤⁢𝔩n,ℂ:X+X†=0}

and find its (real) dimension. Is it a complex vector space?

Problem 55.

Let Ip,q=(Ip−Iq), where Ik denotes the identity matrix of size k. Let n=p+q. Let

O⁡(p,q)={g∈GLn⁡(ℝ):g⁢Ip,q⁢gT=Ip,q}

be the orthogonal group of signature (p,q). Let SO⁢(p,q)=O⁡(p,q)∩SLn⁡(ℝ). We let 𝔬p,q and 𝔰⁢𝔬p,q be their Lie algebras.

Show that the Lie algebra 𝔬p,q is given by

𝔬⁢(p,q)={X∈Mn⁢(ℝ):X⁢Ip,q+Ip,q⁢XT=0}

and that 𝔰⁢𝔬p,q=𝔬p,q.

Problem 56.
  1. 1.

    Show that the Lie algebras 𝔰⁢𝔬3 and 𝔰⁢𝔲2 are isomorphic. (Later on, we will see a conceptual reason for this).

    Hint: it is enough to find a basis for 𝔰⁢𝔬3 and a basis for 𝔰⁢𝔲2 which satisfy the ‘same’ Lie bracket relations. Try using the basis of 𝔰⁢𝔬3 consisting of infinitesimal generators for rotations around the axes, and a basis for 𝔰⁢𝔲2 related to the quaternions.

  2. 2.

    Show that the Lie algebras 𝔰⁢𝔬2,1 and 𝔰⁢𝔩2,ℝ are isomorphic. See Problem 55 for the definition of 𝔰⁢𝔬2,1.

  3. 3.

    (+) Show that the Lie algebras 𝔰⁢𝔬3,1 and 𝔰⁢𝔩2,ℂ are isomorphic (as real Lie algebras). See Problem 55 for the definition of 𝔰⁢𝔬3,1.

Problem 57.

Show that:

  1. 1.

    If X∈𝔰⁢𝔭2⁢n, then tr⁡(X)=0.

  2. 2.

    (+) Show that, if g∈Sp⁡(2⁢n), then det(g)=1.

Problem 58.

Prove that if G is a Lie group and G0 is the connected component of the identity, then the subgroup G0 is normal.

Problem 59.
  1. 1.

    Give a direct proof that SO⁢(3) is connected, by constructing a path from an arbitrary element of SO⁢(3) to the identity. Hint: every element of SO⁢(3) is rotation by some angle about some axis.

  2. 2.

    Prove by induction on n that S⁢O⁢(n) is connected for all n≥1.

Problem 60.

Show that a general element of SU⁢(2) may be written

(a−b¯ba¯)

for a,b∈ℂ with |a|2+|b|2=1.

Deduce that SU⁢(2) is homeomorphic to the three-sphere S3={v∈ℝ4:|v|=1}.

In other words, write down a bijection SU⁢(2)→S3 with continuous inverse. Don’t worry about checking that the maps are continuous, just write them down. The result of this problem implies that SU⁢(2) is simply-connected, because S3 is.

Problem 61.

Show that, if G is a connected (linear) Lie group with Lie algebra 𝔤, then G is abelian if and only if 𝔤 is (see Definition 5.30). Hint: for the converse, consider the adjoint map G→G⁢L⁢(𝔤).

What goes wrong if G is not connected?

Solution: see Proposition 6.14.

Problem 62.

If 𝔤 is a Lie algebra, let 𝔷 be its centre:

𝔷={X∈𝔤:[X,Y]=0:for all Y∈𝔤.}.

Suppose that G is a connected Lie group with centre Z and Lie algebra 𝔤 with centre 𝔷.

Prove that 𝔷 is the Lie algebra of Z.

You will always have Lie⁡(Z)⊂𝔷 but the reverse inclusion requires that G is connected.

Problem 63.

Solve the exercises in section 5.8

10.2 Problems for section 6

Problem 64.
  1. 1.

    If (ρ,V) is an irreducible finite-dimensional complex representation of 𝔤 and 𝔷 is the centre of 𝔤 (see problem 62), show that there is a linear map α:𝔷→ℂ such that ρ⁢(Z)⁢v=α⁢(Z)⁢v for all Z∈𝔷.

  2. 2.

    For 𝔤=GLn,ℂ, find 𝔷. Find α when V=Λk⁢ℂn, where ℂn is the standard representation and 1≤k≤n. These representations are in fact irreducible, though we haven’t proved that yet; you can just directly show that α exists.

Problem 65.

Prove that, for X,Y∈𝔤⁢𝔩n,

(adX)m⁢(Y)=[X,[X,…,[X,Y]⁢…]]=∑k=0m(mk)⁢Xk⁢Y⁢(−X)m−k.

Hence give a direct proof that exp⁡(adX)=Adexp⁡(X).

Problem 66.

Consider G=U⁢(1).

  1. 1.

    For φ a continuous function on G, we define its integral

    ∫Gφ⁢(g)⁢𝑑g=12⁢π⁢∫02⁢πφ⁢(ei⁢t)⁢𝑑t.

    Note that ∫g1⁢𝑑g=1. Show that

    ∫Gφ⁢(h⁢g)⁢𝑑g=∫Gφ⁢(g⁢h)⁢𝑑g=∫Gφ⁢(g)⁢𝑑g

    for any h∈G.

  2. 2.

    Let (V,ρ) be a finite dimensional representation of G and let (,) be any Hermitian form on V. Define a new Hermitian form by

    (v,w)ρ=∫G(ρ⁢(g)⁢v,ρ⁢(g)⁢w)⁢𝑑g.

    Show that (,)ρ is a G-invariant Hermitian form on V.

  3. 3.

    Conclude that every finite-dimensional representation of U⁢(1) is completely reducible. (This is analogous to Maschke’s theorem for finite groups.)

Problem 67.

Consider the orthogonal group O⁡(2).

  1. 1.

    Show that SO⁢(2) has index 2 in O⁡(2). Deduce that every element in O⁡(2) can be uniquely written as rθ or rθ⁢s with s=(0110) and rθ the matrix for rotation by θ. Show that

    s⁢rθ=r−θ⁢s.
  2. 2.

    Mimic the method we used for dihedral groups to classify all irreducible finite-dimensional representations of O⁡(2).

Problem 68.

Let V be the space of functions on ℂ2 that are polynomials in the coordinates x and y. Consider the (left) action of GL2⁡(ℂ) on V given by

(g⁢φ)⁢(v)=φ⁢(g−1⁢v)

(here, think of v=(xy)∈ℂ2 as a column vector).

Compute the derived action for the “standard” basis of 𝔰⁢𝔩2⁢(ℂ) given by X=(0100), Y=(0010), and H=(100−1). You should get something involving the partial derivatives ∂∂x and ∂∂y.

Problem 69.

Let V=ℂ2 be the standard representation of GL2⁡(ℂ).

  1. 1.

    Show that Λ2⁢(V)≅det as Lie group representations.

  2. 2.

    Show that Λ2⁢(V)≅tr as representations of 𝔤⁢𝔩2⁢(ℂ). (You could just ‘take the derivative’ of part (a), but please do it directly instead.)

  3. 3.

    Find an explicit homomorphism ρ:GL2⁡(ℂ)→GL3⁡(ℂ) corresponding to Sym2⁡(V).

10.3 Problems for section 7

Problem 70.

Let V, W be representations of 𝔰⁢𝔩2,ℂ. Let v and w be two weight vectors of V and W respectively with respective weights α and β. Show that

v⊗w∈V⊗W

is a weight vector with weight α+β, and that if v and w are highest weight vectors then so is v⊗w.

Problem 71.

Let V be a finite-dimensional representation of 𝔰⁢𝔩2,ℂ.

  1. 1.

    What are the weights of the dual representation V∗?

  2. 2.

    Deduce that V≅V∗.

Problem 72.

Let (π,V) be a finite-dimensional representation of 𝔰⁢𝔩2,ℂ. Consider the Casimir element88 8 Conventions differ; it might be more usual to call 1+2⁢𝒞 the Casimir.

𝒞=π⁢(X)⁢π⁢(Y)+π⁢(Y)⁢π⁢(X)+12⁢π⁢(H)2.
  1. 1.

    Show 𝒞 commutes with the action of 𝔰⁢𝔩2,ℂ. Conclude that if V is irreducible then 𝒞 acts as a scalar.

  2. 2.

    What is the scalar for V=Symn⁡(ℂ2), the irreducible representation of highest weight n?

  3. 3.

    Compute the action of 𝒞 on the space V of polynomial functions ϕ on ℂ2, with action the derivative of (g⁢ϕ)⁢(v)=ϕ⁢(g−1⁢v) (see problem 68).

Problem 73.

If λ∈ℂ, show that there is a (possibly infinite dimensional!) representation of 𝔰⁢𝔩2,ℂ with highest weight λ.

Problem 74.

Consider V=Symn⁡(ℂ2), the irreducible representation of highest weight n of 𝔰⁢𝔩2,ℂ. Decompose the following representations into irreducibles, and find highest weight vectors for the irreducible constituents:

  1. 1.

    Sym2⁡(Sym2⁡(ℂ2));

  2. 2.

    Λ2⁢(Sym2⁡(ℂ2));

  3. 3.

    Sym3⁡(ℂ2)⊗Sym2⁡(ℂ2);

  4. 4.

    Sym3⁡(Sym2⁡(ℂ2)).

For the third example, find bases for the irreducible subrepresentations.

Problem 75.
  1. 1.

    For a≥b integers, decompose the representation Syma⁡ℂ2⊗Symb⁡ℂ2 of 𝔰⁢𝔩2,ℂ into irreducibles. (This is known as the Clebsch–Gordan formula).

  2. 2.

    (+) Can you find a general expression for the highest weight vectors for the irreducible subrepresentations? What about for the weight bases?

Problem 76.

Show that the real Lie algebras 𝔰⁢𝔩2,ℝ and 𝔰⁢𝔲2 are not isomorphic. Hint: consider the adjoint action of an arbitrary element of 𝔰⁢𝔲2.

Problem 77.

We have that Symn⁡(ℂ2) is the irreducible representation of SU⁢(2) of dimension n+1. Let χn be its character. Every conjugacy class of SU⁢(2) contains an element of the form

exp⁡(i⁢t⁢H)=(ei⁢t00e−i⁢t).

Show that

χn⁢(exp⁡(i⁢t⁢H))=sin⁡((n+1)⁢t)sin⁡(t).
Problem 78.

Let (ρ,V) be an irreducible representation of 𝔤⁢𝔩2,ℂ, and let Z=(1001).

  1. 1.

    Show that ρ⁢(Z) is a scalar.

  2. 2.

    Show that the restriction of V to 𝔰⁢𝔩2,ℂ is irreducible.

  3. 3.

    Show that for every λ∈ℂ and integer n≥0, there is a unique irreducible representation of 𝔤⁢𝔩2,ℂ of dimension n+1 with ρ⁢(Z)=λ⁢I.

  4. 4.

    Which of these are derivatives of representations of GL2⁡(ℂ)? Hence classify the finite dimensional holomorphic irreducible representations of GL2⁡(ℂ).

Problem 79.
  1. 1.

    Verify the formula

    r2⁢Δ=Jx2+Jy2+Jz2+ℓ2+ℓ

    as operators on 𝒫ℓ.

  2. 2.

    Find the image of the Casimir element from problem 72 under our isomorphism 𝔰⁢𝔩2,ℂ→𝔰⁢𝔬3,ℂ, and compare to part 1.

Problem 80.

Let ℓ≥1.

  1. 1.

    Verify that (x−i⁢y)ℓ is a highest weight vector in ℋℓ.

  2. 2.

    By applying the lowering operator, find weight vectors of weights i⁢(ℓ−1) and i⁢(ℓ−2).

  3. 3.

    Find a basis of weight vectors in ℋℓ when ℓ=1 and ℓ=2 (see example 7.40).

Problem 81.
  1. 1.

    Prove that, for f∈𝒫ℓ,

    Δ⁢(r2⁢f)=r2⁢Δ⁢(f)+2⁢(2⁢ℓ+3)⁢f.
  2. 2.

    Find a similar formula for

    Δ⁢(r2⁢k⁢f)−r2⁢k⁢Δ⁢(f).
  3. 3.

    Use this to give another proof that

    ℋℓ∩r2⁢𝒫ℓ−2={0}.

    (Hint: if f is in the intersection, let f=r2⁢k⁢g, g not divisible by r2).

Problem 82.
  1. 1.

    Let V be the standard — three-dimensional — representation of 𝔰⁢𝔬3. Find a basis of weight vectors for Sym2⁡(V), and decompose it into irreducible subrepresentations.

  2. 2.

    Let ℋ2 be the five-dimensional representation of SO⁢(3). Decompose ℋ2⊗ℋ2 into irreducible representations.

10.4 Problems for section 8

Problem 83.

Verify that

[(a1000a2000a3),Ei⁢j]=(ai−aj)⁢Ei⁢j

and

[E12,E23]=E13.
Problem 84.

Consider, instead of 𝔰⁢𝔩3,ℂ, 𝔰⁢𝔩2,ℂ. What are the roots and root spaces? What is the relation between the weights (as linear functionals on 𝔥) and between the weights defined in section 7?

Problem 85.

Let V=(ℂ3)∗ be the dual of the standard representation, with basis e1∗,e2∗,e3∗ dual to the standard basis.

  1. 1.

    Show that the ei∗ are weight vectors with weights −Li.

  2. 2.

    Find the action of each Ei⁢j on e3∗ and deduce that e3∗ is a highest weight vector with weight −L3.

Problem 86.

Show that a1⁢L1+a2⁢L2+a3⁢L3∈ΛW if and only if a1−a2,a2−a3∈ℤ. Must the ai be integers?

Problem 87.

The root lattice ΛR⊂ΛW is the subgroup of the weight lattice generated by the roots.

  1. 1.

    Draw a picture showing the root lattice inside the weight lattice.

  2. 2.

    Show that ΛR has index three in ΛW (i.e. the quotient ΛW/ΛR has order three).

  3. 3.

    What would the root lattice and weight lattice be for 𝔰⁢𝔩2,ℂ? What is the index in this case?

  4. 4.

    Let V be a finite-dimensional irreducible representation of 𝔰⁢𝔩3,ℂ. Show that any two weights of V differ by an element of the root lattice.

Problem 88.

Find the weights of Sym3⁡(ℂ3) and draw the weight diagram.

Problem 89.

Using weights, or otherwise, show that

ℂ3⊗(ℂ3)∗≅ℂ⊕𝔰⁢𝔩3,ℂ

where ℂ is the trivial representation and 𝔰⁢𝔩3,ℂ is the adjoint representation.

Problem 90.

(non-examinable) Let (ρ,V) be a representation of 𝔰⁢𝔩3,ℂ. As SL3⁡(ℂ) is simply-connected ρ exponentiates to a representation, ρ~, of SL3⁡(ℂ). Let

σ3=(010−100001)∈SL3⁡(ℂ).

Show that, for every weight α, ρ~⁢(σ3) is an isomorphism

Vα→Vs3⁢α.

Here s3⁢(a1⁢L1+a2⁢L2+a3⁢L3)=a1⁢L2+a2⁢L1+a3⁢L3.

Give another proof of Theorem 8.26.

Problem 91.

Let a,b≥0 be integers. Check that

e1a⊗(e3∗)b∈Syma⁡(ℂ3)⊗Symb⁡((ℂ3)∗)

is a highest weight vector with weight a⁢L1−b⁢L3.

Problem 92.

Show that, if V is a finite-dimensional representation of 𝔰⁢𝔩3,ℂ with a unique highest weight vector (up to scalar multiplication), then V is necessarily irreducible.

Deduce that the standard representation, its dual, and the adjoint representation are irreducible.

Problem 93.
  1. 1.

    Find the weights of Sym2⁡(ℂ3)⊗(ℂ3)∗ and draw the weight diagram.

  2. 2.

    Show that

    e12⊗e1∗+e1⁢e2⊗e2∗+e1⁢e3⊗e3∗∈Sym2⁡(ℂ3)⊗(ℂ3)∗

    is a highest weight vector with weight L1.

  3. 3.

    Let v=e12⊗e3∗. Calculate E32⁢E21⁢v and E21⁢E32⁢v and show that they are linearly independent.

  4. 4.

    Show that

    Sym2⁡(ℂ3)⊗(ℂ3)∗≅V(2,1)⊕ℂ3

    and find the weight diagram for V(2,1).

Problem 94.

(harder!) The aim of this problem is to show that, for n≥0,

V(n,0)=Symn⁡(ℂ3).

It suffices to show that Symn⁡(ℂ3) is irreducible with highest weight n⁢L1.

  1. 1.

    Show that Symn⁡(ℂ3) has a basis of weight vectors

    {e1a⁢e2b⁢e3c:a,b,c≥0,a+b+c=n}

    and that these have distinct weights (so, every weight has multiplicity one).

  2. 2.

    Show that e1n is the unique highest weight vector in Symn⁡(ℂ3), up to scalar multiplication.

  3. 3.

    Deduce that Symn⁡(ℂ3) is an irreducible representation with highest weight n⁢L1. See problem 92.

Problem 95.

(monster!) Let V=ℂ3, let W=V∗, and let a,b>0. For v∈V,w∈W, define (v,w)=w⁢(v).

Let

ϕ:Syma⁡(V)⊗Symb⁡(W)→Syma−1⁡(V)⊗Symb−1⁡(W)

be defined by

ϕ⁢((v1⁢…⁢va)⊗(w1⁢…⁢wb))=∑i=1a∑j=1b(vi,wj)⁢(v1⁢…⁢v^i⁢…⁢va)⊗w1⁢…⁢w^j⁢…⁢wb

where v^i means vi is omitted (and similarly for w^j).

  1. 1.

    Show that ϕ is an 𝔰⁢𝔩3,ℂ-homomorphism.

  2. 2.

    Show that Syma⁡(V)⊗Symb⁡(W) has a unique highest weight vector of weight (a−i)⁢L1−(b−i)⁢L3 for each 0≤i≤min⁡(a,b), and no other highest weight vectors.

  3. 3.

    Show that the highest weight vector from the previous part is in ker⁡(ϕ) if and only if i=0.

  4. 4.

    Deduce that ker⁡(ϕ)≅V(a,b) is the irreducible representation of highest weight a⁢L1−b⁢L3.

  5. 5.

    Show that ϕ is surjective, and hence decompose Syma⁡(V)⊗Symb⁡(V∗) into irreducibles.

  6. 6.

    Find the dimension of V(a,b). Find its weights.

This problem is hard! For a solution, see Fulton and Harris, section 13.2, but watch out for the unjustified ’clearly’ just before Claim 13.4.