4.18. Lecture 18

4.18.1. Visualising weights

Shortly we will prove that, if (ρ,V)(\rho,V) is a finite dimensional representation of 𝔰𝔩3,\mathfrak{sl}_{3,\mathbb{C}}, then its weights are integer linear combinations of the LiL_{i}. In other words, they lie in the weight lattice

ΛW={a1L1+a2L2+a3L3|a1,a2,a3}.\Lambda_{W}=\{a_{1}L_{1}+a_{2}L_{2}+a_{3}L_{3}\,|\,a_{1},a_{2},a_{3}\in\mathbb% {Z}\}.

We want to visualise this in a way that treats L1,L2,L3L_{1},L_{2},L_{3} symmetrically. Noticing that they sum to zero, we regard them them as the position vectors of the vertices an equilateral triangle with unit side length, centred on the origin. The weight lattice ΛW\Lambda_{W} is then the set of vertices of equilateral triangles tiling the plane. For any representation (ρ,V)(\rho,V), its weight diagram is then obtained by circling the weights that occur in that representation.

Example 4.18.1.

We draw the weight diagram for the standard representation, in Figure 4.1.

Refer to caption
Figure 4.1. Weights for 3\mathbb{C}^{3}.
Example 4.18.2.

We draw the weight diagram for the adjoint representation in Figure 4.2. Note that in this case the dimension of the weight space for the weight 0 is two. We say the weight has multiplicity two, and indicate this on the weight diagram by circling the weight twice. If the multiplicity was much higher, we would need another method (like writing the multiplicity next to the circle as a number).

Refer to caption
Figure 4.2. Weights for the adjoint representation.

4.18.2. Representations and weights

Firstly, we recall from above that any finite-dimensional representation of 𝔰𝔩3,\mathfrak{sl}_{3,\mathbb{C}} is completely reducible. This is Theorem 3.14.7 from the previous section, that we proved using the unitary trick.

Theorem 4.18.3.

Let (ρ,V)(\rho,V) be a finite-dimensional representation of 𝔰𝔩3,\mathfrak{sl}_{3,\mathbb{C}}. Then:

  1. (i)

    There is a basis of VV consisting of weight vectors.

  2. (ii)

    Every weight of VV is in the weight lattice ΛW\Lambda_{W}.

We may combine these two into the single equality

V=αΛWVα.V=\bigoplus_{\alpha\in\Lambda_{W}}V_{\alpha}.
Proof.

Consider the embedding ι12:𝔰𝔩2,𝔰𝔩3,\iota_{12}:\mathfrak{sl}_{2,\mathbb{C}}\rightarrow\mathfrak{sl}_{3,\mathbb{C}} embedding a 2×22\times 2 matrix into the ‘top left’ of a 3×33\times 3 matrix:

ι12:(abca)(ab0ca0000).\iota_{12}:\begin{pmatrix}a&b\\ c&-a\end{pmatrix}\longmapsto\begin{pmatrix}a&b&0\\ c&-a&0\\ 0&0&0\end{pmatrix}.

This is a Lie algebra homomorphism, and ρι12\rho\circ\iota_{12} is a representation of 𝔰𝔩2,\mathfrak{sl}_{2,\mathbb{C}}. We know from the 𝔰𝔩2,\mathfrak{sl}_{2,\mathbb{C}} theory that

(ρι12)(H)=ρ(110)=ρ(H12)(\rho\circ\iota_{12})(H)=\rho\begin{pmatrix}1&&\\ &-1&\\ &&0\end{pmatrix}=\rho(H_{12})

is diagonalisable with integer eigenvalues. If 𝐯V{\bf v}\in V is a weight vector with weight a1L1+a2L2+a3L3a_{1}L_{1}+a_{2}L_{2}+a_{3}L_{3}, then it is an eigenvector for ρ(ι12(H))\rho(\iota_{12}(H)) with eigenvalue a1a2a_{1}-a_{2}. Thus a1a2a_{1}-a_{2} is an integer.

Now, there is another embedding ι23\iota_{23} putting a 2×22\times 2 matrix in the ‘bottom right’ corner. The same argument then shows that ρ(H13)\rho(H_{13}) is diagonalisable with integer eigenvalues, which shows that a2a3a_{2}-a_{3} is an integer for every weight.

Thus every weight is in the weight lattice. Moreover, ρ(H12)\rho(H_{12}) and ρ(H23)\rho(H_{23}) are diagonalisable, and they commute with each other since H12H_{12} and H23H_{23} commute and ρ\rho is a Lie algebra homomorphism. A theorem from linear algebra states that commuting, diagonalisable matrices are simultaneously diagonalisable. It follows that there is a basis of VV consisting of simultaneous eigenvectors for ρ(H12)\rho(H_{12}) and ρ(H23)\rho(H_{23}). Since H12H_{12} and H23H_{23} span 𝔥\mathfrak{h}, this is a basis of weight vectors. ∎

Remark 4.18.4.

There is a third homomorphism

ι23:(abca)(a0b000c0a).\iota_{23}:\begin{pmatrix}a&b\\ c&-a\end{pmatrix}\longmapsto\begin{pmatrix}a&0&b\\ 0&0&0\\ c&0&-a\end{pmatrix}.

We have ι23(H)=H23\iota_{23}(H)=H_{23}.

Note that, for i<ji<j, ιij(X)=Eij\iota_{ij}(X)=E_{ij} and ιij(Y)=Eji\iota_{ij}(Y)=E_{ji}, so EijE_{ij} and EjiE_{ji} will play the role of raising and lowering operators.

Remark 4.18.5.

We could also prove Theorem 4.18.3 by exponentiating ρ\rho to a representation of SL3()\operatorname{SL}_{3}(\mathbb{C}) and considering the action of the subgroup of diagonal matrices with entries in U(1)U(1), which is compact (isomorphic to U(1)U(1)). Compare the proof of the statement that the weights of representations of 𝔰𝔩2,\mathfrak{sl}_{2,\mathbb{C}} are integers (a combination of Theorem 3.13.9(ii) and Theorem 3.14.7).

4.18.3. Tensor constructions

We record how the various linear algebra constructions we know about interact with the theory of weights. If (ρ,V)(\rho,V) is a representation of 𝔤\mathfrak{g} then we consider its weights as a multiset

{α1,,αn}\{\alpha_{1},\ldots,\alpha_{n}\}

where n=dimVn=\dim V and each α𝔥\alpha\in\mathfrak{h}^{*} is written in this list dimVα\dim V_{\alpha} — the multiplicity of α\alpha — times.

Suppose that (σ,W)(\sigma,W) is another representation of 𝔤\mathfrak{g} with multiset of weights

{β1,,βm}.\{\beta_{1},\ldots,\beta_{m}\}.
Proposition 4.18.6.

Suppose that V,W,αi,βjV,W,\alpha_{i},\beta_{j} are as above. Then:

  1. (i)

    The weights of VV^{*} are {α1,,αn}\{-\alpha_{1},\ldots,-\alpha_{n}\}.

  2. (ii)

    The weights of VWV\otimes W are

    {αi+βj| 1in,1jm}.\{\alpha_{i}+\beta_{j}\,|\,1\leq i\leq n,1\leq j\leq m\}.
  3. (iii)

    The weights of Symk(V)\operatorname{Sym}^{k}(V) are

    {αi1++αik| 1i1i2ikn}.\{\alpha_{i_{1}}+\ldots+\alpha_{i_{k}}\,|\,1\leq i_{1}\leq i_{2}\leq\ldots\leq i% _{k}\leq n\}.
  4. (iv)

    The weights of Λk(V)\Lambda^{k}(V) are

    {αi1++αik| 1i1<i2<<ikn}.\{\alpha_{i_{1}}+\ldots+\alpha_{i_{k}}\,|\,1\leq i_{1}<i_{2}<\ldots<i_{k}\leq n\}.
Proof.

This is similar to the proof of Proposition 3.12.11 in the 𝔰𝔩2,\mathfrak{sl}_{2,\mathbb{C}} case and thus is left as an exercise (Problem 4.18.4). ∎

4.18.4. Exercises

.

Problem 49. Show that a1L1+a2L2+a3L3ΛWa_{1}L_{1}+a_{2}L_{2}+a_{3}L_{3}\in\Lambda_{W} if and only if a1a2,a2a3a_{1}-a_{2},a_{2}-a_{3}\in\mathbb{Z}. Must the aia_{i} be integers?

Problem 50. The root lattice ΛRΛW\Lambda_{R}\subseteq\Lambda_{W} is the subgroup of the weight lattice generated by the roots.

  1. (a)

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

  2. (b)

    Show that ΛR\Lambda_{R} has index three in ΛW\Lambda_{W} (i.e. the quotient ΛW/ΛR\Lambda_{W}/\Lambda_{R} has order three).

  3. (c)

    What would the root lattice and weight lattice be for 𝔰𝔩2,\mathfrak{sl}_{2,\mathbb{C}}? What is the index in this case?

  4. (d)

    Let VV be a finite-dimensional irreducible representation of 𝔰𝔩3,\mathfrak{sl}_{3,\mathbb{C}}. Show that any two weights of VV differ by an element of the root lattice.

Problem 51. Prove Proposition 4.18.6

Problem 52. Find the weights of Sym3(3)\operatorname{Sym}^{3}(\mathbb{C}^{3}) and draw the weight diagram.

Problem 53. Using weights, or otherwise, show that

3(3)𝔰𝔩3,\mathbb{C}^{3}\otimes(\mathbb{C}^{3})^{*}\cong\mathbb{C}\oplus\mathfrak{sl}_{3% ,\mathbb{C}}

where \mathbb{C} is the trivial representation and 𝔰𝔩3,\mathfrak{sl}_{3,\mathbb{C}} is the adjoint representation.