More New Modules from Old:
There are a few constructions we can make, starting with
the ones from last time and applying them in certain special cases.
First off, if

and

are two finite-dimensional

-modules, then I say we can put an

-module structure on the space

of linear maps from

to

. Indeed, we can identify

with

: if

is a basis for

and

is a basis for

, then we can set up the dual basis

of

, such that

. Then the elements

form a basis for

, and each one can be identified with the linear map sending

to

and all the other basis elements of

to

. Thus we have an inclusion

, and a simple dimension-counting argument suffices to show that this is an isomorphism.
Now, since we have an action of

on

we get a dual action on

. And because we have actions on

and

we get one on

. What does this look like, explicitly? Well, we can write any such tensor as the sum of tensors of the form

for some

and

. We calculate the action of

on a vector

:
&=\left[(x\cdot\lambda)\otimes w\right](v)+\left[\lambda\otimes(x\cdot w)\right](v)\\&=\left[x\cdot\lambda\right](v)w+\lambda(v)(x\cdot w)\\&=-\lambda(x\cdot v)w+x\cdot(\lambda(v)w)\\&=-\left[\lambda\otimes w\right](x\cdot v)+x\cdot\left[\lambda\otimes x\right](w)\end{aligned} \displaystyle\begin{aligned}\left[x\cdot(\lambda\otimes w)\right](v)&=\left[(x\cdot\lambda)\otimes w\right](v)+\left[\lambda\otimes(x\cdot w)\right](v)\\&=\left[x\cdot\lambda\right](v)w+\lambda(v)(x\cdot w)\\&=-\lambda(x\cdot v)w+x\cdot(\lambda(v)w)\\&=-\left[\lambda\otimes w\right](x\cdot v)+x\cdot\left[\lambda\otimes x\right](w)\end{aligned}](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_vEkqjUf5jpgcF9KfWduFR1x1sjEOEsW0LbkOSWCBxnrl-sQu1CPxXNmeztWl_usOs21x7KC04mlTgPYEbRu8MXHuK3vr36P6ofyMrbGU2tMsdzOOsU3c6F8w_Qrg2eTqT_GThFYVO94q9vvH5bmS0TH4t5hT2dtmO9gPApOYIyjqLmIz2ulME6Tgp5Y-4UvUvew7ydftXwyhbkexQJd2E-JyBN_8333EBM_JJznBFrMo-b6p5-9wFFfsXOg6yijHEJYHob-9QpocZcnwViawBqSOjildUEa0OSNMFFf0iJ79Xa3j8uF23Ci_9GFwjkJFGsse56QmiUK26PmXTDLfoDdSazlQXQ-Q-NFL1dMxGp2UBijQfkCkfyBtewAQTxR5Vb-XjidmdN3A8S1XB4nl1c-BRxLKsPnjmzgMouCoKgBiYS1zle1HfPEglp7jmEqqILAO3ighbkP0zhUqBI5pS4kcHYccJ_5JfrHuFgtbt1enVSurFbVVYlcYYStUD4w5M3Le9D5fZsVhDqDLKh5yiDYkKMVBek-8dnyMWYE-gkJHGU3g0XBR3YchZYnKR7kcZ4BFLFbtYNgfzAD8kDYLTXmfUDyMB7tWpBE14woo3VsopgMoc_qf5IMN7v4xOzQFiuDAg1BVDwCgeOU9JwH6gXOP8-CAnrsG8nxOyZeT24aoXfkK-pPI1kfu4xmoSuTuzYJ21TnCfzpQCff4YI5uhb2wsBsDbyJW42wGZyJoSkHcbs889_dDn_Vd3ffcB_tDM3L7iO91A=s0-d)
In general we see that
=x\cdot f(v)-f(x\cdot v) \left[x\cdot f\right](v)=x\cdot f(v)-f(x\cdot v)](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_sS_OOtIMgHxRmnT29EqW0wo3KQ-k8s1Ty6ZSwlf3T8nLOLfR092IwHqugii1S4FEWK-f7WtepR-u1ALs0Hd1iimrUaSJ1dIso4oY7AVP11_8dvOPLA1qzA0MbimgQSMf60SWxC7AgTf5UbANenqIYqJNcHEuXD1Yti3PwSaYnKJekOtc6QsNtVUodKwvxNzA5woGpaOzjJS1Pz4Yk=s0-d)
. In particular, the space of linear endomorphisms on

is

, and so it get an

-module structure like this.
The other case of interest is the space of bilinear forms on a module

. A bilinear form on

is, of course, a linear functional on

. And thus this space can be identified with

. How does

act on a bilinear form

? Well, we can calculate:
&=\left[x\cdot B\right](v_1\otimes v_2)\\&=-B\left(x\cdot(v_1\otimes v_2)\right)\\&=-B\left((x\cdot v_1)\otimes v_2\right)-B\left(v_1\otimes(x\cdot v_2)\right)\\&=-B(x\cdot v_1,v_2)-B(v_1,x\cdot v_2)\end{aligned} \displaystyle\begin{aligned}\left[x\cdot B\right](v_1,v_2)&=\left[x\cdot B\right](v_1\otimes v_2)\\&=-B\left(x\cdot(v_1\otimes v_2)\right)\\&=-B\left((x\cdot v_1)\otimes v_2\right)-B\left(v_1\otimes(x\cdot v_2)\right)\\&=-B(x\cdot v_1,v_2)-B(v_1,x\cdot v_2)\end{aligned}](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_torJbkTNHC-qoPkXebYjDpYOisUpkvRQrDCLf5zwgVpx8FDEtecVySgMKeyejEWZeBuOTlgu2i6SdCIUcExqQvG1NY4ytdUoaB43FBUy6wwok8QdMVoG73Ry14q6Ojgd8bR255PLi0mYZv_OmXmbRqW39TQUblJUzqanfhFM5nRHcc2rTFvBy9gWaxslzzcEwzyGARsGgASA-zwG00xTEft3bZoY9DkVX79zK-YFww-AIDAJvEwQ6XRkeSoiwO-X9J1cfbNZG1gRBbha-rI-gS_cVBy3NZm3XqfjNN18pIgP5aXTZNmiOb-MpTYqbYeyjp9edDG2BRl901Er8ijQhknqV6Uv3HYC1m28SVOFK91gRYEc5ZTDPAa39UzqF7pWhnfWlBZHcdAlOxRdYprYomcCTeZ4azTtbSzAQn1yV1bEKCHWqBNh30V07MaxeU5mk6_w7KuRKovAyhZCO1OmEP3LwAPijm4nUrz2EL89qlKCX3HqGjMum66ZtcS2eRT-Nssb1sT4SccYfUmcwN4VcbDOeHxaLLKIgJjr7-_VLo0g27A0J-tYd7lji7zEVrvzhCTWtfIopFlPpbzsLq461E5jkc2qHK=s0-d)
In particular, we can consider the case of bilinear forms on

itself, where

acts on itself by

. Here we read
=-B([x,v_1],v_2)-B(v_1,[x,v_2]) \displaystyle\left[x\cdot B\right](v_1,v_2)=-B([x,v_1],v_2)-B(v_1,[x,v_2])](https://lh3.googleusercontent.com/blogger_img_proxy/AEn0k_tWqVQuHQMb8UDTA2uUaS9S1iuiNxDFwKBu_Zj6YHdF8Zl2pSbUAAQmYiN3FVA8NEOYr3CYJlOCPcorLln853xl78ciZ9ItRXXG4_H0ZfVqE93Q1F4pVP3tH8sJDPrrdZdN_nHMrFUqW6SBzsZvHRhbRTvCI-8WKlGq2DViJtpvupmpBhuB9Go-PKWaKwERO0QMWmZ0OvnUy6Q91gMp1G71uS5WH7ja3_hZBGY73s6JWsUHQpXUG2qz1tCLTgg=s0-d)

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