Does a Holomorphic Function Extend Continuously to the Unit Circle?

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Show that there is no holomorphic function f in the unit disc D that extends continuously to |z|=1 such that f(z) =1/z for |z|=1

Some thoughts that might not be relevant:
If such f existed then, I can see that f maps the unit circle to the unit circle and the unit disc onto the unit disc.
On |z|=1 f would be equal to the conjugate function which is not differentiable anywhere.

I'm kind of stuck. I appreciate any suggestions.
 
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Do you mean that if I integrate f on circles with radii approaching 1, I get
0 = int f approaches int 1/z =2ipi ?

but does the continuity of f imply the continuity of the integral like that?
 
Office_Shredder said:
Think integration

Does integration work with this problem? I assume you had an argument like the following in mind:
If [itex]f[/itex] had an analytic extension to [itex]\partial D[/itex], then take the curve [itex]\gamma:[0,1] \rightarrow \mathbb{C}[/itex] given by [itex]\gamma(t)=\exp(2 \pi i t)[/itex]. Notice that [itex]\int_{\gamma} f = 2\pi i[/itex] by calculation but that [itex]\int_{\gamma} f = 0[/itex] since [itex]f[/itex] is analytic. This is a contradiction so [itex]f[/itex] cannot have such an analytic extension.
But since the extension of [itex]f[/itex] to [itex]\partial D[/itex] is only continuous, none of the integration theorems for analytic functions will work here. The notion of what it means for [itex]f[/itex] to be analytic on [itex]D \cup \partial D[/itex] is ill-defined as well, since [itex]D \cup \partial D[/itex] is not open. Maybe I am just missing something here and you found a way to do this with integration (which would be pretty neat).

I am pretty sure that you can do this without integration though. Notice that the maximum/minimum modulus principle apply since [itex]f[/itex] is holomorphic on [itex]D[/itex] and continuous on [itex]\partial D[/itex]. This means [itex]|f|[/itex] assumes its maximum and minimum values on [itex]\partial D[/itex]; in particular, it follows that [itex]|f|=1[/itex] on [itex]D[/itex]. From here you should be able to derive a contradiction.
 
Thank you jgens.
About your approach, you say f doesn't have a min in D.
How do we know 0 is not a min ?
 
symbol0 said:
About your approach, you say f doesn't have a min in D.

I said [itex]|f|=1[/itex] on [itex]D[/itex] which means that every point of [itex]D[/itex] is a minimum for [itex]|f|[/itex].
 
I want to understand how do you conclude |f| = 1 on D.
I know f cannot have a maximum in D. So |f|<1 on D.
...what else?
 
symbol0 said:
I want to understand how do you conclude |f| = 1 on D.
I know f cannot have a maximum in D. So |f|<1 on D.
...what else?

The maximum modulus principle says that [itex]|f| \leq 1[/itex] on [itex]D[/itex]. The minimum modulus principle says that [itex]1 \leq |f|[/itex]. This means that [itex]|f|=1[/itex]. There is not much to it.
 
To jgens: you say 1 leq |f|. How do we know f is not a function like f(z)=z which has a minimum in D ?

To office shredder: to get that contradiction don't we need to know that integrals are continuous ? is that a fact?
 
I don't follow you mathwonk.
If the curve is going counterclockwise, the winding number is greater or equal to 0.
And how is that related to the question?