Why Is the Inverse Function Theorem by Spivak Difficult to Follow?

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tjkubo
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I'm having trouble following the proof of the IFT by Spivak. The statement of the theorem was posted in a similar thread:
https://www.physicsforums.com/showthread.php?t=319924

He says, "If the theorem is true for [tex]\lambda^{-1} \circ f[/tex], it is clearly true for [tex]f[/tex]. Therefore we may assume at the outset that [tex]\lambda[/tex] is the identity."

These statements are not clear to me, so if anyone can provide a little more explanation, that would be helpful.
 
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I'm not sure I follow the chain of reasoning from the thread. But the basic proof is straightforward.

Apply the chain rule to the derivative (w.r.t. y) of [tex][f\circ f^{-1}](\mathbf{y})=\mathbf{y}[/tex]
you get:
[tex][Df]\circ f(\mathbf{y})\cdot Df^{-1}(\mathbf{y}) = \mathbf{1}[/tex]
thence
[tex]Df^{-1}(\mathbf{y}) = [Df(f^{-1}(\mathbf{y}))]^{-1}[/tex]

This works for single valued functions and for functions of many variables (treated as a vector valued function of a vector.)