[[Noteworthy Uses]]:: *[[Noteworthy Uses]]*
[[Proved By]]:: *[[Proved By|Crucial Dependencies]]*
Intuition:: [[dual transform of forms#^d39630|Inspiration is here]]
Specializations:: *[[Specializations]]*
Generalizations:: *[[Generalizations]]*
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- Let $\v x := (x_{1},\dots,x_{k})$ denote a generic point in $\rr ^{k}$ and let $A \subset \rrk$ be [[open set|open in]] $\rrk$;
- Let $\v y = (y_{1},\dots,y_{k})$ denote a generic point in $\rrn$ and let $B \subset \rrn$ be [[open set|open in]] $\rrn$; then $dx_{i}$ and $dy_{i}$ denote the elementary $1$-forms on $\rrk$ and $\rrn$, respectively;
- Let $\alpha: A \subset \rrk \to B \subset \rrn$ be a [[smooth]] map.
> [!theorem] Theorem. ([[computation of dual transform of forms]])
> Then,
>1. ($1-\text{form}$) $\alpha ^{*}(dy_{i})=d\alpha_{i} = \sum_{j=1}^{k}D_{j} \alpha_{i} \ dx_{j}$ ;
>2. ($k-\text{form}$) For $I = (i_{1},\dots,i_{k}) \in$ [[set of all ascending k-tuples from 1 to n]], $\alpha ^{*} (dy_{I}) = \left( \det \frac{ \partial \alpha_{I} }{ \partial \v x } \right)\ dx_{I}$, where $dy_{I}=dy_{i_{1}}\wedge \dots \wedge dy_{i_{k}} \and \frac{ \partial \alpha_{I} }{ \partial \v x } = \frac{ \partial (\alpha_{i_{1}} , \dots, \alpha_{i_{k}})}{ \partial (x_{1},\dots,x_{k} )} .$
>3. ($\ell-\text{form}$) For $I=(i_{1},\dots,i_{\ell}) \in \asc_{\ell ,n}$, $\alpha ^{*}(dy_{I})=\sum_{J \in \asc_{\ell, k}}^{}\left( \det \frac{ \partial \alpha_{I} }{ \partial x_{J} } \right) \ dx_{J},$
>where $J=(j_{1},\dots,j_{\ell})$ and $\frac{ \partial \alpha_{I} }{ \partial x_{J} }=\frac{ \partial (\alpha_{i_{1}},\dots, \alpha_{i_{\ell}}) }{ \partial (x_{j_{1}},\dots, x_{j_{\ell}}) }$ .
> [!proof]- Proof. ([[computation of dual transform of forms]])
> 1. Set $\v y = \alpha(\v x)$. Let $\v v \in \rrk$ be arbitrary. Then compute $\begin{align}
> \alpha ^{*}(dy_{i})(\v x)(\v v)= & \big(dy_{i} (\alpha(\v x))\big) \ (D\alpha(\v x )\v v) \\
> = & (i^{th} \text{ component of the vector } D\alpha(\v x) \v v )\\
> = & \sum_{j=1}^{k} D_{j}\alpha_{i}(\v x) v_{j} \\
> \end{align}$
> and since $v_{j}=dx_{j}(\v v)$, this implies $\alpha ^{*}(dy_{i})=\sum_{j=1}^{k}(D_{j}\alpha _{i})dx_{j}$
> which by definition equals $d\alpha_{i}$ as desired.
>
> 2. Since the [[dual transform of forms#^f2843f|dual transform of forms respects the]] [[algebra of alternating multilinear forms|wedge product]] we have $\begin{align}
> \alpha ^{*}(dy_{i_{1}} \wedge \dots \wedge dy_{i_{k}}) = & \alpha ^{*}(dy_{i_{1}}) \wedge \dots \wedge \alpha ^{*}(dy_{i_{k}}) \\
> = & d\alpha_{i_{1}} \wedge \dots \wedge d\alpha_{i_{k}} \text{ (part 1)} \\
> = & \det \begin{bmatrix}
> — & D\alpha_{i_{1}} & — \\ & \vdots & \\ — & D\alpha_{i_{k}} & —
> \end{bmatrix} \ dx_{1} \wedge \dots \wedge dx_{k},
> \end{align}$
> where in the last step we used the **[[396 HW4 Q1 Lemma]]**. Since $\begin{bmatrix}
> — & D\alpha_{i_{1}} & — \\ & \vdots & \\ — & D\alpha_{i_{k}} & —
> \end{bmatrix} = \begin{bmatrix}
> \frac{ \partial \alpha_{i_{1}} }{ \partial x_{1} } & \dots & \frac{ \partial \alpha _{i_{1}} }{ \partial x_{k} } \\ \vdots& \ddots & \vdots \\
> \frac{ \partial \alpha_{i_{k}} }{ \partial x_{1}} & \dots & \frac{ \partial \alpha_{i_{k}} }{ \partial x_{k} }\end{bmatrix} := \frac{ \partial \alpha_{I} }{ \partial \v x }, $
> this is the result.
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####
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#### References
> [!backlink]
> ```dataview
TABLE rows.file.link as "Further Reading"
FROM [[]]
FLATTEN file.tags
GROUP BY file.tags as Tag
> [!frontlink]
> ```dataview
> TABLE rows.file.link as "Further Reading"
> FROM outgoing([[]])
> FLATTEN file.tags as Tag
> WHERE Tag = "#definition" OR Tag = "#theorem" OR Tag = "#MOC" OR Tag = "#proposition" OR Tag = "#axiom"
> GROUP BY Tag
> ```