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I'm trying to understand how to write the Killing form $B: \mathfrak{g} \times \mathfrak{g} \to \mathbb{R}$ defined by $$ B(X,Y) = \mathrm{Tr}(\mathrm{ad}_{X} \circ \mathrm{ad}_{Y}) $$

I'm trying to do this specifically for the Lie algebra $\mathfrak{g} = \mathfrak{so}(n)$, but I'm getting stuck right at the end. I know I $should$ be getting $B(X,Y) = (n-2)\mathrm{Tr}(XY)$ at the end of the day.

In my solution I try to keep things in terms of a general Lie algebra, and then specify to $\mathfrak{so}(n)$ at the end.

Assume $\mathfrak{g}$ is a matrix of size $n \times n$. Since $\mathrm{ad}_{X}(A) = [X,A]$, I'm thinking of the linear transformation $ad_{X}:\mathfrak{g} \to \mathfrak{g}$ as a matrix of size $n^{2} \times n^{2}$. Since $$ \left( \mathrm{ad}_{X} \circ \mathrm{ad}_{Y}\right)(A) = [X,[Y,A]] = XYA - YAX - XAY + AYX $$

If $M$ is my matrix (with components $M_{(j,k)(p,q)}$) corresponding to $\mathrm{ad}_{X} \circ \mathrm{ad}_{Y}$ in the sense that: $$ \left( \mathrm{ad}_{X} \circ \mathrm{ad}_{Y}\right)(A)_{jk} = \sum_{p,q=1}^{n} M_{(j,k)(p,q)} A_{pq} $$

I'm assuming then that $B(X,Y) = \mathrm{Tr}\left( \mathrm{ad}_{X} \circ \mathrm{ad}_{Y} \right) = \sum_{j,k=1}^{n} M_{(j,k),(j,k)}$. So after a little grinding, I find that: $$ \left( \mathrm{ad}_{X} \circ \mathrm{ad}_{Y}\right)(A)_{jk} = \sum_{p,q=1}^{n} \left[ X_{jp}Y_{pq}A_{qk} - Y_{jp}A_{pq}X_{qk} - X_{jp}A_{pq}Y_{qk} + A_{jp}Y_{pq}X_{qk} \right] \\ = \sum_{p,q=1}^{n} \left[ \sum_{\ell=1}^{n} \left( X_{j\ell}Y_{\ell p} \delta_{kq} + Y_{q\ell} X_{\ell k} \delta_{j p} \right) - X_{jp} Y_{qk} - Y_{jp} X_{qk} \right] A_{pq} \\ $$

Where $\delta$ is the kronecker delta. So my matrix components are: $$ M_{(j,k)(p,q)} = \sum_{\ell=1}^{n} \left( X_{j\ell}Y_{\ell p} \delta_{kq} + Y_{q\ell} X_{\ell k} \delta_{j p} \right) - X_{jp} Y_{qk} - Y_{jp} X_{qk} $$

Finally, this tells me that the Killing-form ends up looking like: $$ B(X,Y) = \sum_{j,k=1}^{n} M_{(j,k)(j,k)} \\ = \sum_{j,k=1}^{n} \left[ \sum_{\ell=1}^{n} \left( X_{j\ell}Y_{\ell j} \delta_{kk} + Y_{k\ell} X_{\ell k} \delta_{j j} \right) - X_{jj} Y_{kk} - Y_{jj} X_{kk} \right] \\ = 2n \mathrm{Tr}(XY) - 2 \mathrm{Tr}(X)\mathrm{Tr}(Y) $$

So $B(X,Y) = 2n \mathrm{Tr}(XY) - 2 \mathrm{Tr}(X)\mathrm{Tr}(Y)$, and so far I'm still working with a general Lie algebra $\mathfrak{g}$.

Looking at $\mathfrak{so}(n)$, I know this this is the set of skew-symmetric real matrices of size $n \times n$, which means they are all traceless. This simplifies my answer to $B(X,Y) = 2n \mathrm{Tr}(XY)$.

However, $2n \neq n-2$! Where am I going wrong in my proof? Am I taking too large of a leap in assuming that I can write the matrix M corresponding to $\mathrm{ad}_{X} \circ \mathrm{ad}_{Y}$ so easily?

2 Answers2

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Short answer : Not all matrices are skew-symmetric, and $\mathfrak{so}(n)$ has dimension $\frac{n^2-n}{2}$ not $n^2$, so you cannot apply directly your computation on the $n^2$-dimensional space of $n\times n$ matrices, you have to adapt them a little bit.

Longer answer : let $E_{ab}$ be the matrix all of those coefficients are zero except the one at the intersection of the $a$-th row and the $b$-th column, which is equal to one (so $E_{ab}=(\delta_{ai}\delta_{bj})_{1\leq i,j \leq n}$). Let $\phi=\mathrm{ad}_{X} \circ \mathrm{ad}_{Y},Z=XY,T=YX$.

The main formula for $\phi$ in your OP can be rewritten as follows :

$$ \phi(E_{jk})=\sum_{p,q} M_{(j,k),(p,q)} E_{pq} \tag{1} $$

Now, a basis for $\mathfrak{so}(n)$ is $\lbrace D_{jk} \rbrace_{j<k}$ where $D_{jk}=E_{jk}-E_{kj}$. We already have $\phi(E_{jk})$ above, so we need to compute $\phi(D_{jk})$.

In the sequel, by "negligible terms" I mean terms who will not contribute in the final computation of the trace of $\phi$.

$$ \begin{array}{lcl} \phi(E_{jk}) &=& M_{(j,k),(j,k)} E_{jk} + M_{(j,k),(k,j)} E_{kj}+ \text{negligible terms} \\ \phi(E_{kj}) &=& M_{(k,j),(j,k)} E_{jk} + M_{(k,j),(k,j)} E_{kj}+ \text{negligible terms} \\ \phi(D_{jk}) &=& (M_{(j,k),(j,k)}-M_{(k,j),(j,k)})D_{jk} + \text{negligible terms} \\ \end{array}\tag{2} $$

Note that by the formula for $M_{(j,k),(p,q)}$ in the OP, we have for any $j,k$, distinct or not :

$$ \begin{array}{lcl} M_{(j,k),(j,k)} &=& Z_{jj}+T_{kk} - X_{jj} Y_{kk} - X_{kk} Y_{jj} \\ M_{(j,k),(k,j)} &=& \delta_{jk}(Z_{jj}+T_{kk})- X_{jk} Y_{kj} - Y_{jk} X_{kj} \\ \end{array}\tag{3} $$

So the Killing form is

$$ \begin{array}{lcl} B(X,Y) &=& \sum_{j< k} \bigg(Z_{jj} + T_{kk} - X_{jj} Y_{kk} - X_{kk} Y_{jj} + X_{jk} Y_{kj} + Y_{jk} X_{kj} \bigg) \\ &=& \frac{1}{2}\sum_{j\neq k} \bigg(Z_{jj} + T_{kk} - X_{jj} Y_{kk} - X_{kk} Y_{jj} + X_{jk} Y_{kj} + Y_{jk} X_{kj} \bigg) \\ &=& \frac{n-1}{2}(\mathrm{Tr}(Z)+\mathrm{Tr}(T))-\frac{1}{2}\sum_{j\neq k} \bigg( X_{kk} Y_{jj}+X_{jj} Y_{kk} - X_{jk} Y_{kj} - Y_{jk} X_{kj} \bigg) \\ &=& (n-1)\mathrm{Tr}(XY)-\frac{1}{2}\sum_{j\neq k} \bigg( X_{kk} Y_{jj}+X_{jj} Y_{kk} - X_{jk} Y_{kj} - Y_{jk} X_{kj} \bigg) \\ &=& (n-1)\mathrm{Tr}(XY)-\frac{1}{2}\sum_{j,k} \bigg( X_{kk} Y_{jj}+X_{jj} Y_{kk} - X_{jk} Y_{kj} - Y_{jk} X_{kj} \bigg) \\ &=& (n-1)\mathrm{Tr}(XY)-\mathrm{Tr}(X)\mathrm{Tr}(Y)-\frac{1}{2}(\mathrm{Tr}(Z)+\mathrm{Tr}(T)) \\ &=& (n-2)\mathrm{Tr}(XY). \end{array} $$

Ewan Delanoy
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    Great process thank you. My only issue is concerning the "negligible terms". To me is seems like they should be exactly 0 - what are these negligible terms precisely? – QuantumEyedea Mar 27 '17 at 04:33
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    @Greg.Paul as my text says, they are "terms who will not contribute who will not contribute in the final computation of the trace of $\phi$". To be precise, there are two bases here : base $B_1=(E_{ab})$ for all matrices and base $B_2=(D_{jk})$ for $\mathfrak{so}(n)$. The final computation of $\mathrm{Tr}(\phi)$ is made relatively to $B_2$, so in the expansion of $\phi(b)$ for $b\in B_2$ the only component that matters is the one that's a multiple of $b$, the others are "negligible". And to compute this component in $B_2$, we deduce it from a computation in $B_1$, via $D_{jk}=E_{jk}-E_{kj}$. – Ewan Delanoy Mar 27 '17 at 06:19
  • Okay that makes sense. One more question; how is it that you pull out the factor of $n-1$ in the third line of the final calculation? – QuantumEyedea Mar 27 '17 at 08:36
  • Never mind, I think understand! You sum over all $j = 1 \ldots n$, which leaves you with $\sum_{k=2}^{n} \mathrm{Tr}(Z) = (n-1)\mathrm{Tr}(Z)$. Is there a way to write the summation $\sum_{j\neq k}$ more explictly? I was thinking something along the lines $\sum_{j=1}^{n} \sum_{k \neq j =1}^{n}$.... – QuantumEyedea Mar 27 '17 at 08:41
  • @Greg.Paul the notation $\sum_{j\neq k}$ means : sum over all pairs $(j,k)$ satisfying $j\neq k$. You can rewrite it, starting either with $j$ (it then becomes $\sum_{j=1}^n \sum_{1\leq k\leq n,k\neq j}$) or with $k$ (it then becomes $\sum_{k=1}^n \sum_{1\leq j\leq n,j\neq k}$). – Ewan Delanoy Mar 27 '17 at 11:22
  • @Greg.Paul Answer to the "how do you pull the $n-1$ factor " question : consider for example $\sum_{j\neq k} Z_{jj}$. I can rewrite as $\sum_{j=1}^n \sum_{1\leq k\leq n,k\neq j} Z_{jj}$. But $\sum_{1\leq k\leq n,k\neq j} Z_{jj}=(n-1)Z_{jj}$ since $Z_{jj}$ is independent of $k$, so $\sum_{j\neq k} Z_{jj}=\sum_{j=1}^n (n-1)Z_{jj}=(n-1)\mathrm{Tr}(Z)$. – Ewan Delanoy Mar 27 '17 at 11:22
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(1) Since $so(n)$ is set of skew symmetric matrices so we have a basis $\{ a_{ij} \}_{1\leq i<j\leq n}$ : If $\{e_i\}$ is orthonormal basis on $\mathbb{R}^n$, then $$ a_{ij} e_j=e_i,\ a_{ij} e_i=-e_j $$ and $a_{ij}e_k=0$ for all $k\neq i,\ j$.

Hence we have the following cases :

i) $i<j<k$ : $$[a_{ij},a_{jk}]=a_{ik}$$

$$[a_{ik},a_{ij}]=a_{jk} $$

$$ [a_{ik},a_{jk}]=-a_{ij} $$

ii) $[a_{ij},a_{ij}]=0$

iii) $\{i,j\}\cap \{k,l\}=\emptyset$ : $[a_{ij},a_{kl}]=0$

And $$ {\rm Tr}\ (a_{ij}a_{ij})=-2 $$ and if $\{ i,j\}\neq \{ k,l\}$, then $$ {\rm Tr}\ (a_{ij}a_{kl})=0$$

(2) $g,\ h\in SO(n),\ X,\ Y\in so(n)$ so that $$ {\rm Tr}\ (ghXh^{-1}g^{-1} Y) ={\rm Tr}\ (hXh^{-1}g^{-1} Yg)\ \ast$$

(3) If $B(X,Y)={\rm Tr}\ (ad_X \circ ad_Y)$, so we suffice to consider $\{a_{ij}\}$.

Assume that $i\leq k$

\begin{align*} B(a_{ij},a_{kl}) &=\sum_{x<y}\ {\rm Tr}\ \bigg( [a_{ij},[a_{kl},a_{xy}]]\ a_{xy} \bigg) \\&=-\sum_{x<y}\ {\rm Tr}\ \bigg( [a_{kl},a_{xy}] \ [a_{ij}, a_{xy} ]\bigg)\ ({\rm cf}.\ \ast) \end{align*}

i) $i=k<j<l$ : $x=j,\ y=l$ so that $$ {\rm Tr}\ ([a_{kl},a_{xy}] \ [a_{ij}, a_{xy} ])={\rm Tr}\ ( -a_{ij} a_{il} )=0 $$

ii) $i=k<j=l$ : By symmetry we can assume that $i=1,\ j=2$ So $x=1,\ y>2$ or $x=2,\ y>2$ so that $$ {\rm Tr}\ ([a_{12},a_{1y}] \ [a_{12}, a_{1y} ])= {\rm Tr}\ ( a_{2y}a_{2y} )=-2(n-2) $$

$$ {\rm Tr}\ ([a_{12},a_{2y}] \ [a_{12}, a_{2y} ])= {\rm Tr}\ ( a_{1y}a_{1y} )=-2(n-2) $$

iii) $i<j<k<l$ : If $x=j,\ y=k$, then $${\rm Tr}\ ([a_{kl},a_{xy}] \ [a_{ij}, a_{xy} ])= {\rm Tr}\ (-a_{jl} a_{ik})=0$$ So we do not consider this case including the following cases : $$ i<k<j<l,\ i<k<l<j$$

Hence $B(X,Y)=2(n-2){\rm Tr}\ (XY)$

HK Lee
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