4.20. Lecture 20

4.20.1. Irreducible representations of ๐”ฐโข๐”ฉ3,โ„‚\mathfrak{sl}_{3,\mathbb{C}}.

We are now in a position to state the main theorem of ๐”ฐโข๐”ฉ3,โ„‚\mathfrak{sl}_{3,\mathbb{C}}-theory.

Theorem 4.20.1.

For every pair a,ba,b of non-negative integers, there is a unique (up to isomorphism) irreducible finite-dimensional representation V(a,b)V^{(a,b)} of ๐”ฐโข๐”ฉ3,โ„‚\mathfrak{sl}_{3,\mathbb{C}} with a highest weight vector of weight aโขL1โˆ’bโขL3aL_{1}-bL_{3}.

Note that the highest weights occurring in the theorem are exactly the dominant elements of the weight lattice.

Since every irreducible finite-dimensional representation does have a highest weight, necessarily dominant, every irreducible representation is isomorphic to V(a,b)V^{(a,b)} for some integers a,bโ‰ฅ0a,b\geq 0.

Example 4.20.2.

We have already seen some examples:

  1. (i)
    โ€‹

    The standard representation โ„‚3\mathbb{C}^{3} is irreducible with highest weight L1L_{1}, therefore

    V(1,0)=โ„‚3.V^{(1,0)}=\mathbb{C}^{3}.
  2. (ii)
    โ€‹

    The dual to the standard representation is irreducible with highest weight L3L_{3}, and so

    V(0,1)=(โ„‚3)โˆ—.V^{(0,1)}=(\mathbb{C}^{3})^{*}.
  3. (iii)
    โ€‹

    The adjoint representation ๐”ค\mathfrak{g} is irreducible with highest weight L1โˆ’L3L_{1}-L_{3}, and so

    V(1,1)=๐”ค.V^{(1,1)}=\mathfrak{g}.
  4. (iv)
    โ€‹

    The symmetric square Sym2โก(โ„‚3)\operatorname{Sym}^{2}(\mathbb{C}^{3}) has highest weight 2โขL12L_{1} with highest weight vector ๐ž12{\bf e}_{1}^{2}.

4.20.2. Proof of theorem 4.20.1

Lemma 4.20.3.

Let (ฯ,V)(\rho,V) be a finite-dimensional representation of ๐”ฐโข๐”ฉ3,C\mathfrak{sl}_{3,C}. Let ๐ฏโˆˆV{\bf v}\in V be a highest weight vector of weight ฮฑ\alpha, and let

W={ฯ(Yn)ฯ(Ynโˆ’1)โ€ฆฯ(Y1)๐ฏ|nโ‰ฅ0,Yiโˆˆ{E21,E32}.W=\{\rho(Y_{n})\rho(Y_{n-1})\ldots\rho(Y_{1}){\bf v}\,|\,n\geq 0,Y_{i}\in\{E_{% 21},E_{32}\}.

Then

  1. (i)
    โ€‹

    WW is a subrepresentation of VV

  2. (ii)
    โ€‹

    Wฮฑ=โŸจ๐ฏโŸฉW_{\alpha}=\left\langle{\bf v}\right\rangle i.e. ๐ฏ{\bf v} is the unique weight vector in WW of weight ฮฑ\alpha, up to scaling.

  3. (iii)
    โ€‹

    WW is irreducible.

Proof.

o

  1. (i)
    โ€‹

    Let

    Wn={ฯโข(Ym)โขฯโข(Ymโˆ’1)โขโ€ฆโขฯโข(Y1)โข๐ฏ|nโ‰ฅmโ‰ฅ0,Yiโˆˆ{E21,E32}}.W_{n}=\{\rho(Y_{m})\rho(Y_{m-1})\ldots\rho(Y_{1}){\bf v}\,|\,n\geq m\geq 0,Y_{% i}\in\{E_{21},E_{32}\}\}.

    Then

    W=โ‹ƒn=0โˆžWn.W=\bigcup_{n=0}^{\infty}W_{n}.

    Firstly, it is clear that ฯโข(E21)\rho(E_{21}) and ฯโข(E32)\rho(E_{32}) take WnW_{n} to Wn+1W_{n+1}, and so preserve WW. Since

    ฯโข(E31)=ฯโข([E32,E21])=[ฯโข(E32),ฯโข(E21)]\rho(E_{31})=\rho([E_{32},E_{21}])=[\rho(E_{32}),\rho(E_{21})]

    we see that ฯโข(E31)\rho(E_{31}) also preserves WW.

    Secondly, every ฯโข(Ym)โขฯโข(Ymโˆ’1)โขโ€ฆโขฯโข(Y1)โข๐ฏ\rho(Y_{m})\rho(Y_{m-1})\ldots\rho(Y_{1}){\bf v} is a weight vector (by the fundamental weight calculation, Lemmaย 4.19.1) and so an eigenvector for all ฯโข(H)\rho(H), Hโˆˆ๐”ฅH\in\mathfrak{h}. Thus ฯโข(H)\rho(H) preserves each WnW_{n} (and hence also WW).

    Finally, we show that ฯโข(E12)\rho(E_{12}) preserves WnW_{n}. A similar proof then applies for ฯโข(E23)\rho(E_{23}), and then ฯโข(E13)\rho(E_{13}) preserves WW by the same argument as for ฯโข(E31)\rho(E_{31}). We prove the statement for ฯโข(E12)\rho(E_{12}) by induction on nn.

    For n=0n=0, W0=โŸจ๐ฏโŸฉW_{0}=\left\langle{\bf v}\right\rangle. Since ๐ฏ{\bf v} is a highest weight vector, ฯโข(E12)โข๐ฏ=0\rho(E_{12}){\bf v}=0 and so ฯโข(E12)โข(W0)โІW0\rho(E_{12})(W_{0})\subseteq W_{0}.

    Suppose that the claim is true for nn. Consider ๐ฐ=ฯโข(Yn+1)โขโ€ฆโขฯโข(Y1)โข๐ฏโˆˆWn+1{\bf w}=\rho(Y_{n+1})\ldots\rho(Y_{1}){\bf v}\in W_{n+1} with Yiโˆˆ{E21,E32}Y_{i}\in\{E_{21},E_{32}\}. We must show that ฯโข(E12)โข๐ฐโˆˆWn+1\rho(E_{12}){\bf w}\in W_{n+1}. Suppose first that Yn+1=E21Y_{n+1}=E_{21}. Then, as [E12,E21]=H12โˆˆ๐”ฅ[E_{12},E_{21}]=H_{12}\in\mathfrak{h}, we have

    ฯโข(E12)โข๐ฐ\displaystyle\rho(E_{12}){\bf w} =ฯโข(E12)โขฯโข(E21)โขฯโข(Yn)โขโ€ฆโขฯโข(Y1)โข๐ฏ\displaystyle=\rho(E_{12})\rho(E_{21})\rho(Y_{n})\ldots\rho(Y_{1}){\bf v}
    =ฯโข(E21)โขฯโข(E12)โขฯโข(Yn)โขโ€ฆโขฯโข(Y1)โข๐ฏ+ฯโข(H12)โขฯโข(Yn)โขโ€ฆโขฯโข(Y1)โข๐ฏ\displaystyle=\rho(E_{21})\rho(E_{12})\rho(Y_{n})\ldots\rho(Y_{1}){\bf v}+\rho% (H_{12})\rho(Y_{n})\ldots\rho(Y_{1}){\bf v}
    โˆˆฯโข(E21)โขฯโข(E12)โขWn+ฯโข(H12)โขWn\displaystyle\in\rho(E_{21})\rho(E_{12})W_{n}+\rho(H_{12})W_{n}
    โІฯโข(E21)โขWn+Wn\displaystyle\subseteq\rho(E_{21})W_{n}+W_{n}
    by the induction hypothesis and the fact that WnW_{n} is preserved by ๐”ฅ\mathfrak{h}
    โІWn+1+Wn\displaystyle\subseteq W_{n+1}+W_{n}
    =Wn+1,\displaystyle=W_{n+1},

    as required. The proof in the case Yn+1=E32Y_{n+1}=E_{32} is similar, using that [E12,E32]=0[E_{12},E_{32}]=0.

  2. (ii)
    โ€‹

    Note that if ฮฒ\beta the weight of ฯโข(Yn)โขฯโข(Ymโˆ’1)โขโ€ฆโขฯโข(Y1)โข๐ฏ\rho(Y_{n})\rho(Y_{m-1})\ldots\rho(Y_{1}){\bf v}, with nn and YiY_{i} as in the lemma, then a calculation using the fundamental weight calculation, as in the proof of lemma 4.19.7, shows that

    lโข(ฮฒ)=lโข(ฮฑ)โˆ’nl(\beta)=l(\alpha)-n

    and so ฮฒโ‰ ฮฑ\beta\neq\alpha if n>0n>0. Since these vectors span WW, ๐ฏ{\bf v} is the unique (up to scalar) weight vector in WW of weight ฮฑ\alpha.

  3. (iii)
    โ€‹

    Suppose that WW is reducible. By complete reducibility (Theoremย 3.14.7) we have

    W=UโŠ•Uโ€ฒW=U\oplus U^{\prime}

    for U,Uโ€ฒU,U^{\prime} non-zero proper subrepresentations of WW. We must have ๐ฏ=๐ฎ+๐ฎโ€ฒ{\bf v}={\bf u}+{\bf u}^{\prime} for unique ๐ฎโˆˆU{\bf u}\in U, ๐ฎโ€ฒโˆˆUโ€ฒ{\bf u}^{\prime}\in U^{\prime}. The unicity implies that ๐ฎ{\bf u} and ๐ฎโ€ฒ{\bf u}^{\prime} are both weight vectors of weight ฮฑ\alpha so, by part (ii), either ๐ฎ=0{\bf u}=0 or ๐ฎโ€ฒ=0{\bf u}^{\prime}=0. Without loss of generality let ๐ฏ=๐ฎโˆˆU{\bf v}={\bf u}\in U. But then all ฯโข(Yn)โขโ€ฆโขฯโข(Y1)โข๐ฏโˆˆU\rho(Y_{n})\ldots\rho(Y_{1}){\bf v}\in U as UU is a subrepresentation, so W=UW=U contradicting that UU is a proper subrepresentation.

โˆŽ

Remark 4.20.4.

It follows that WW as in Lemma 4.20.3 is actually the subrepresentation generated by ๐ฏ{\bf v}, that is, the span of all vectors obtained by applying arbitrary elements of ๐”ฐโข๐”ฉ3,โ„‚\mathfrak{sl}_{3,\mathbb{C}} some number of times. The content of the lemma is then that it suffices to apply only E21E_{21} and E32E_{32}.

Proof of Theoremย 4.20.1.

First we show the existence. Let a,bโˆˆโ„คโ‰ฅ0a,b\in\mathbb{Z}_{\geq 0}. Consider

V=Symaโก(โ„‚3)โŠ—Symbโก((โ„‚3)โˆ—).V=\operatorname{Sym}^{a}(\mathbb{C}^{3})\otimes\operatorname{Sym}^{b}((\mathbb% {C}^{3})^{*}).

This has a highest weight vector ๐ฏ=๐ž1aโŠ—(๐ž3โˆ—)b{\bf v}={\bf e}_{1}^{a}\otimes({\bf e}_{3}^{*})^{b} of weight aโขL1โˆ’bโขL3aL_{1}-bL_{3}. Let WW be the representation generated by ๐ฏ{\bf v}. Then WW is irreducible by 4.20.3(iii), and has a highest weight vector ๐ฏ{\bf v} of weight aโขL1โˆ’bโขL3aL_{1}-bL_{3}. Thus we can take V(a,b)=WV^{(a,b)}=W.

Next we show the uniqueness. Suppose that V,WV,W are two irreducible representations with highest weight vectors ๐ฏ{\bf v} and ๐ฐ{\bf w}, respectively, of weight aโขL1โˆ’bโขL3aL_{1}-bL_{3}. Let UโІVโŠ•WU\subseteq V\oplus W be the representation generated by ๐ฎ=(๐ฏ,๐ฐ){\bf u}=({\bf v},{\bf w}). Then UU is irreducible by 4.20.3(iii). The projection VโŠ•Wโ†’VV\oplus W\to V sending (๐ฏโ€ฒ,๐ฐโ€ฒ)({\bf v}^{\prime},{\bf w}^{\prime}) to ๐ฏโ€ฒ{\bf v}^{\prime} restricts to a homomorphism Uโ†’VU\to V which sends ๐ฎ{\bf u} to ๐ฏ{\bf v}. This is therefore a non-zero homomorphism between irreducible representations, and so must be an isomorphism. Thus Uโ‰…VU\cong V. Similarly Uโ‰…WU\cong W, and so Vโ‰…WV\cong W as required. โˆŽ

In fact, it is possible to give an explicit description of the irreducible representations.

Theorem 4.20.5.

Let a,bโ‰ฅ0a,b\geq 0 and V=โ„‚3V=\mathbb{C}^{3}. Define

ฯ•:Symaโก(V)โŠ—Symbโก(Vโˆ—)โ†’Symaโˆ’1โก(V)โŠ—Symbโˆ’1โก(Vโˆ—)\phi:\operatorname{Sym}^{a}(V)\otimes\operatorname{Sym}^{b}(V^{*})\to% \operatorname{Sym}^{a-1}(V)\otimes\operatorname{Sym}^{b-1}(V^{*})

to be the map

(๐ฏ1โขโ€ฆโข๐ฏa)โŠ—(ฮป1โขโ€ฆโขฮปb)โŸผโˆ‘i=1aโˆ‘j=1bฮปjโข(๐ฏi)โข(๐ฏ1โขโ€ฆโข๐ฏ^iโขโ€ฆโข๐ฏa)โŠ—(ฮป1โขโ€ฆโขฮปj^โขโ€ฆโขฮปb).({\bf v}_{1}\ldots{\bf v}_{a})\otimes(\lambda_{1}\ldots\lambda_{b})\longmapsto% \sum_{i=1}^{a}\sum_{j=1}^{b}\lambda_{j}({\bf v}_{i})({\bf v}_{1}\ldots\hat{{% \bf v}}_{i}\ldots{\bf v}_{a})\otimes(\lambda_{1}\ldots\hat{\lambda_{j}}\ldots% \lambda_{b}).

Then ฯ•\phi is a surjective ๐”ฐโข๐”ฉ3,โ„‚\mathfrak{sl}_{3,\mathbb{C}}-homomorphism, and its kernel is the irreducible representation with highest weight aโขL1โˆ’bโขL3aL_{1}-bL_{3}.

Proof.

This is Problemย 4.7. โˆŽ

4.20.3. Exercises

.

Problemย 57. Show that, if VV is a finite-dimensional representation of ๐”ฐโข๐”ฉ3,โ„‚\mathfrak{sl}_{3,\mathbb{C}} with a unique highest weight vector (up to scalar multiplication), then VV is necessarily irreducible.

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

Problemย 58.

  1. (a)
    โ€‹

    Find the weights of Sym2โก(โ„‚3)โŠ—(โ„‚3)โˆ—\operatorname{Sym}^{2}(\mathbb{C}^{3})\otimes(\mathbb{C}^{3})^{*} and draw the weight diagram.

  2. (b)
    โ€‹

    Show that

    ๐ž12โŠ—๐ž1โˆ—+๐ž1โข๐ž2โŠ—๐ž2โˆ—+๐ž1โข๐ž3โŠ—๐ž3โˆ—โˆˆSym2โก(โ„‚3)โŠ—(โ„‚3)โˆ—{\bf e}_{1}^{2}\otimes{\bf e}_{1}^{*}+{\bf e}_{1}{\bf e}_{2}\otimes{\bf e}_{2}% ^{*}+{\bf e}_{1}{\bf e}_{3}\otimes{\bf e}_{3}^{*}\in\operatorname{Sym}^{2}(% \mathbb{C}^{3})\otimes(\mathbb{C}^{3})^{*}

    is a highest weight vector with weight L1L_{1}.

  3. (c)
    โ€‹

    Let ๐ฏ=๐ž12โŠ—๐ž3โˆ—{\bf v}={\bf e}_{1}^{2}\otimes{\bf e}_{3}^{*}. Calculate E32โขE21โขvE_{32}E_{21}v and E21โขE32โขvE_{21}E_{32}v and show that they are linearly independent.

  4. (d)
    โ€‹

    Show that

    Sym2(โ„‚3)โŠ—(โ„‚3)โˆ—โ‰…V(2,1)โŠ•โ„‚3\operatorname{Sym}^{2}(\mathbb{C}^{3})\otimes(\mathbb{C}^{3})^{*}\cong V^{(2,1% })\oplus\mathbb{C}^{3}

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

Problemย 59. (harder!)

Refer to caption
Figure 4.7. Weights for Symnโก(โ„‚3)\operatorname{Sym}^{n}(\mathbb{C}^{3}).

The aim of this problem is to show that, for nโ‰ฅ0n\geq 0,

V(n,0)=Symnโก(โ„‚3).V^{(n,0)}=\operatorname{Sym}^{n}(\mathbb{C}^{3}).

It suffices to show that Symnโก(โ„‚3)\operatorname{Sym}^{n}(\mathbb{C}^{3}) is irreducible with highest weight nโขL1nL_{1}.

  1. (a)
    โ€‹

    Show that Symnโก(โ„‚3)\operatorname{Sym}^{n}(\mathbb{C}^{3}) has a basis of weight vectors

    {๐ž1aโข๐ž2bโข๐ž3c|a,b,cโ‰ฅ0,a+b+c=n}\{{\bf e}_{1}^{a}{\bf e}_{2}^{b}{\bf e}_{3}^{c}\,|\,a,b,c\geq 0,a+b+c=n\}

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

  2. (b)
    โ€‹

    Show that ๐ž1n{\bf e}_{1}^{n} is the unique highest weight vector in Symnโก(โ„‚3)\operatorname{Sym}^{n}(\mathbb{C}^{3}), up to scalar multiplication.

  3. (c)
    โ€‹

    Deduce that Symnโก(โ„‚3)\operatorname{Sym}^{n}(\mathbb{C}^{3}) is an irreducible representation with highest weight nโขL1nL_{1}. See problem 4.20.3.

Problemย 60. (monster!) Let V=โ„‚3V=\mathbb{C}^{3}, let W=Vโˆ—W=V^{*}, and let a,b>0a,b>0. For ๐ฏโˆˆV,๐ฐโˆˆW{\bf v}\in V,{\bf w}\in W, define (๐ฏ,๐ฐ)=wโข(๐ฏ)({\bf v},{\bf w})=w({\bf v}).

Let

ฯ•:Symaโก(V)โŠ—Symbโก(W)โŸถSymaโˆ’1โก(V)โŠ—Symbโˆ’1โก(W)\phi:\operatorname{Sym}^{a}(V)\otimes\operatorname{Sym}^{b}(W)\longrightarrow% \operatorname{Sym}^{a-1}(V)\otimes\operatorname{Sym}^{b-1}(W)

be defined by

ฯ•โข((๐ฏ1โขโ€ฆโข๐ฏa)โŠ—(๐ฐ1โขโ€ฆโข๐ฐa))=โˆ‘i=1aโˆ‘j=1b(๐ฏi,๐ฐj)โข(๐ฏ1โขโ€ฆโข๐ฏ^iโขโ€ฆโข๐ฏa)โŠ—๐ฐ1โขโ€ฆโข๐ฐ^jโขโ€ฆโข๐ฐb\phi(({\bf v}_{1}\ldots{\bf v}_{a})\otimes({\bf w}_{1}\ldots{\bf w}_{a}))=\sum% _{i=1}^{a}\sum_{j=1}^{b}({\bf v}_{i},{\bf w}_{j})({\bf v}_{1}\ldots\hat{{\bf v% }}_{i}\ldots{\bf v}_{a})\otimes{\bf w}_{1}\ldots\hat{{\bf w}}_{j}\ldots{\bf w}% _{b}

where ๐ฏ^i\hat{{\bf v}}_{i} means ๐ฏi{\bf v}_{i} is omitted (and similarly for ๐ฐ^j\hat{{\bf w}}_{j}).

  1. (a)
    โ€‹

    Show that ฯ•\phi is an ๐”ฐโข๐”ฉ3,โ„‚\mathfrak{sl}_{3,\mathbb{C}}-homomorphism.

  2. (b)
    โ€‹

    Show that Symaโก(V)โŠ—Symbโก(W)\operatorname{Sym}^{a}(V)\otimes\operatorname{Sym}^{b}(W) has a unique highest weight vector of weight (aโˆ’i)โขL1โˆ’(bโˆ’i)โขL3(a-i)L_{1}-(b-i)L_{3} for each 0โ‰คiโ‰คminโก(a,b)0\leq i\leq\min(a,b), and no other highest weight vectors.

  3. (c)
    โ€‹

    Show that the highest weight vector from the previous part is in kerโก(ฯ•)\ker(\phi) if and only if i=0i=0.

  4. (d)
    โ€‹

    Deduce that kerโก(ฯ•)โ‰…V(a,b)\ker(\phi)\cong V^{(a,b)} is the irreducible representation of highest weight aโขL1โˆ’bโขL3aL_{1}-bL_{3}.

  5. (e)
    โ€‹

    Show that ฯ•\phi is surjective, and hence decompose Symaโก(V)โŠ—Symbโก(Vโˆ—)\operatorname{Sym}^{a}(V)\otimes\operatorname{Sym}^{b}(V^{*}) into irreducibles.

  6. (f)
    โ€‹

    Find the dimension of V(a,b)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 โ€™clearlyโ€™ just before Claim 13.4.