Existence of Uncountable Zeros in Continuous Functions

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Discussion Overview

The discussion centers on the existence of a continuous function f:ℝ→ℝ that is nowhere constant and has an uncountable set of zeros. Participants explore various examples, counterexamples, and theoretical implications related to this concept.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants propose that a continuous function can exist with uncountably many zeros, while being nowhere constant.
  • One participant suggests that a function defined as zero on the irrationals cannot be nowhere constant due to continuity constraints.
  • A later reply introduces the idea of a continuous but nowhere differentiable function that intersects a horizontal line uncountably many times, expressing uncertainty about its existence.
  • Another participant describes a construction involving triangle waves and the Cantor set to create a continuous function that is nowhere constant and has uncountably many zeros.
  • There is a request for a formal definition of the proposed function, highlighting concerns about continuity in the construction process.
  • One participant suggests a simpler function based on the distance from a point to the Cantor set, while also noting a preference for terminology regarding "nowhere constant."
  • Another participant discusses the uniform continuity of the sequence of functions and the potential for a formal proof of convergence.
  • A different approach is presented, defining a function that is zero on the Cantor set and linear on its complement, illustrating another method to achieve the desired properties.

Areas of Agreement / Disagreement

Participants express differing views on the existence of such a function, with no consensus reached on the validity of the proposed examples or constructions. The discussion remains unresolved regarding the existence of a continuous, nowhere constant function with uncountably many zeros.

Contextual Notes

Some arguments depend on the definitions of continuity and the properties of specific sets, such as the Cantor set. There are unresolved questions about the formal construction of the proposed functions and their continuity.

Dragonfall
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Does there exist a continuous function [tex]f:\mathbb{R}\rightarrow\mathbb{R}[/tex] such that f is nowhere constant and [tex]\{x:f(x)=0\}[/tex] is uncountable?
 
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Sure there is.
 
Can you give an example?
 
Well...the irrationals aren't countable...
 
That is a misleading answer - any continuous function that is zero on the irrationals is 0 everywhere. [0,1] is uncountable, and surely anyone can think of a function that is

1) continuous
2) non-constant
3) 0 on [0,1]
 
He said that f is nowhere constant.
 
Yes, I did say f is nowhere constant. If f=0 on the subset of irrationals of some interval, then continuity implies that f=0 on that interval.

Intuitively, what I want is a everywhere continuous nowhere differentiable function that is "straight" enough so that a horizontal line intersects the values uncountably many times. I don't think such a function exists, but I can't prove it either way.

The "continuous but nowhere differentiable" requirement might not be necessary, or even relevant, but it's a good place to start looking.
 
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Take the function f(x) = 0 on [0,1]. Now replace f on the interval [1/3,2/3] with a triangle wave. Now replace f on the intervals [1/9,2/9] and [7/9,8/9] with a similar triangle wave. Repeat this process for every interval on which f is zero, and we have a continuous function that vanishes on the Cantor set (which is uncountable), and is nowhere constant. Replacing the triangle wave with a suitable [itex]C^{\infty}[/itex] function yields an infinitely differentiable function that vanishes uncountably many times but is not constant. If you want it to be continuous but nowhere differentiable, replace each triangle wave with such a function instead.
 
Whoops. Missed the continuity assumption.
 
  • #10
Moo Of Doom said:
Take the function f(x) = 0 on [0,1]. Now replace f on the interval [1/3,2/3] with a triangle wave. Now replace f on the intervals [1/9,2/9] and [7/9,8/9] with a similar triangle wave. Repeat this process for every interval on which f is zero, and we have a continuous function that vanishes on the Cantor set (which is uncountable), and is nowhere constant. Replacing the triangle wave with a suitable [itex]C^{\infty}[/itex] function yields an infinitely differentiable function that vanishes uncountably many times but is not constant. If you want it to be continuous but nowhere differentiable, replace each triangle wave with such a function instead.

Can you please "formally" define your function? "if we infinitely repeat..." is not a formal term and I am not sure the ultimate function remains a continuous one.
 
  • #11
"if we infinitely repeat..." simply refers to the limit function of the sequence of functions I described.

Define
[tex] f_1[a,b](x) = \left\{<br /> \begin{array}{cc}<br /> 0 & x \in \left[a,\frac{2a+b}{3}\right]\cup\left[\frac{a+2b}{3},b\right]\\<br /> x-\frac{2a+b}{3} & x \in \left[\frac{2a+b}{3},\frac{a+b}{2}\right]\\<br /> \frac{a+2b}{3}-x & x \in \left[\frac{a+b}{2},\frac{a+2b}{3}\right]<br /> \end{array}[/tex]

and
[tex] f_{n+1}[a,b](x) = \left\{<br /> \begin{array}{cc}<br /> f_n\left[a,\frac{2a+b}{3}\right](x) & x \in \left[a,\frac{2a+b}{3}\right]\\<br /> x-\frac{2a+b}{3} & x \in \left[\frac{2a+b}{3},\frac{a+b}{2}\right]\\<br /> \frac{a+2b}{3}-x & x \in \left[\frac{a+b}{2},\frac{a+2b}{3}\right]\\<br /> f_n\left[\frac{a+2b}{3},b\right](x) & x \in \left[\frac{a+2b}{3},b\right]<br /> \end{array}[/tex]

Then [tex]f(x) = \lim_{n\to\infty}f_n[0,1](x)[/tex] is the function I just described.
 
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  • #12
There's a simpler description of (something like) Moo's function:

f(x) = [distance from x to the Cantor set]


Incidentally, I don't think I've heard "nowhere constant" before -- I would have used the phrase "locally nonconstant".
 
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  • #13
Moo Of Doom said:
"if we infinitely repeat..." simply refers to the limit function of the sequence of functions I described.

Define
[tex] f_1[a,b](x) = \left\{<br /> \begin{array}{cc}<br /> 0 & x \in \left[a,\frac{2a+b}{3}\right]\cup\left[\frac{a+2b}{3},b\right]\\<br /> x-\frac{2a+b}{3} & x \in \left[\frac{2a+b}{3},\frac{a+b}{2}\right]\\<br /> \frac{a+2b}{3}-x & x \in \left[\frac{a+b}{2},\frac{a+2b}{3}\right]<br /> \end{array}[/tex]

and
[tex] f_{n+1}[a,b](x) = \left\{<br /> \begin{array}{cc}<br /> f_n\left[a,\frac{2a+b}{3}\right](x) & x \in \left[a,\frac{2a+b}{3}\right]\\<br /> x-\frac{2a+b}{3} & x \in \left[\frac{2a+b}{3},\frac{a+b}{2}\right]\\<br /> \frac{a+2b}{3}-x & x \in \left[\frac{a+b}{2},\frac{a+2b}{3}\right]\\<br /> f_n\left[\frac{a+2b}{3},b\right](x) & x \in \left[\frac{a+2b}{3},b\right]<br /> \end{array}[/tex]

Then [tex]f(x) = \lim_{n\to\infty}f_n[0,1](x)[/tex] is the function I just described.

Hmm.. each f_n is uniformly continuous, then if the seq {f_n} converges uniformly, the trick is done.
For the triangular waves become more little as n surges up, I think the convergence is uniform. But, can you dfevise a formal, maybe inductive, proof?
 
  • #14
If C is a closed uncountable set in R containing no intervals (like the Cantor set), then it's complement is a countable union of disjoint open intervals. Define f to be 0 on C, and f is a triangle of slope with absolute value 1 on each open interval. So let C be the Cantor set. [itex]\mathbb{R} = (-\infty ,0) \sqcup \bigsqcup (a_n,b_n) \sqcup C \sqcup (1,\infty )[/itex]. Define [itex]f : \mathbb{R} \to \mathbb{R}[/itex] by:

[tex]f(x)=\left\{\begin{array}{cc}x,&\mbox{ if }<br /> x < 0\\ \frac{b_n-a_n}{2} - |x - \frac{b_n+a_n}{2}|, & \mbox{ if } a_n < x < b_n\\ 0, & \mbox{ if } x \in C\\ 1-x, & \mbox{ if } x > 1\right.[/tex]
 
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