MHB Relationship between two entire functions

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If f and g are entire functions satisfying |f(z)| ≤ |g(z)| for all z in the complex plane, then f can be expressed as f(z) = αg(z) for some complex constant α, according to Liouville's theorem. The discussion highlights the use of the Maximum Modulus Principle to analyze the relationship between f and g, suggesting that if g is non-constant, the same relationship holds. The function h(z) = f(z)/g(z) is introduced to demonstrate that h is bounded, leading to the conclusion that all zeros of g must also be zeros of f. This implies that h is entire and constant, reinforcing that g is a multiple of f. The conversation emphasizes the importance of understanding these properties in complex analysis.
Bingk1
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Hello, this was another question on the exam which I wasn't sure about:

Let f and g be entire such that |f(z)| \leq |g(z)| \ \forall z \in \mathbb{C}. Find a relationship between f and g.

I'm kinda lost on this one...

Thanks!
 
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Bingk said:
Hello, this was another question on the exam which I wasn't sure about:

Let f and g be entire such that |f(z)| \leq |g(z)| \ \forall z \in \mathbb{C}. Find a relationship between f and g.

I'm kinda lost on this one...

Thanks!

A consequence of the Liouville's theorem is that if $\displaystyle |f(z)|\le |g(z)| \forall z \in \mathbb{C}$, then it must be $f(z)=\alpha\ g(z)$ for some complex $\alpha$...

Kind regards

$\chi$ $\sigma$
 
Hi, that's actually what I got, but I'm pretty sure I got it the wrong way. I don't remember exactly what I did (the exam wasn't returned to us), but my method involved the Maximum Modulus Principle (sort of like applying Liouville's on open balls).

How exactly is that a consequence of Liouville's theorem?
I can see that for the case of g being constant, then f should be constant, so g will be a multiple of f. What about for when g is non-constant?

From what I can recall, what I think I did was I said that in an open ball, f and g attain their maximum modulus on the boundary and the modulus of g will be greater than that of f at that point in the boundary. This will happen for any open balls. So, if we consider two balls with the same center, and let the radius of one approach the other, and see what happens to the modulus of f and g at that boundary, it should turn out that g is a multiple of f. Is this sort of right?
 
Bingk said:
Hi, that's actually what I got, but I'm pretty sure I got it the wrong way. I don't remember exactly what I did (the exam wasn't returned to us), but my method involved the Maximum Modulus Principle (sort of like applying Liouville's on open balls).

How exactly is that a consequence of Liouville's theorem?
I can see that for the case of g being constant, then f should be constant, so g will be a multiple of f. What about for when g is non-constant?

From what I can recall, what I think I did was I said that in an open ball, f and g attain their maximum modulus on the boundary and the modulus of g will be greater than that of f at that point in the boundary. This will happen for any open balls. So, if we consider two balls with the same center, and let the radius of one approach the other, and see what happens to the modulus of f and g at that boundary, it should turn out that g is a multiple of f. Is this sort of right?

If You consider the function...

$\displaystyle h(z)=\frac{f(z)}{g(z)}$ (1)

... then, because is $\displaystyle |f(z)| \le |g(z)|$ h(*) is bounded. That means that all the zeroes of g(*) must be also zeroes of f(*) and h(*) is entire, so that h(*) for the Liouville's theorem must be a constant that we call $\alpha$...

Kind regards

$\chi$ $\sigma$
 
Thank you! I didn't think to consider the function h ... but it should've occurred to me.
 

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