How can we represent the $3$ space coordinates uniquely by one point that can be put on a single axis?

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In the Space-Time diagram (in the rest frame) we often take the Space axis as the horizontal axis and the time axis as the axis perpendicular to it as in the given figure. plotting of space-time

While there are other models to graphically represent space-time, my question is:

What function $f(x,y,z)$ on a $3$ dimensional surface can we define such that no two distinct points $(x_1,y_1,z_1)$ and $(x_2,y_2,z_2)$ shall have the same value?

i.e $f(x_1,y_1,z_1)=f(x_2,y_2,z_2)$ if and only if $x_1=x_2$, $y_1=y_2$ and $z_1=z_2$.

That way every point in the $X$ axis of the figure will represent a unique point in $3$-$D$ space.

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Well, you can interleave the digits. That is, if the first value are $x$, represented in base 10 by digits $x_n x_{n-1} \dotsm x_2 x_1 x_0 . x_{-1} x_{-2} \dotsm$, and the other values $y$ and $z$ are similarly represented in base 10 by digits $y_i$ and $z_i$, then your output is $$ x_N y_N z_N x_{N-1} y_{N-1} z_{N-1} \dotsm x_0 y_0 z_0 . x_{-1} y_{-1} z_{-1} \dotsm $$ where $N$ is the maximum index required by $x$, $y$, or $z$ (pad out the other numbers by zeros.)

(You may use any base you please, of course, not just base 10.)

This is a 1-to-1 function, as you require, but it's probably not all that useful: you can't keep the features you expect from 3-dimensionality in a single real value.

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Basically the answer is no such function exists. This is not actually true, but it may as well be as far as a physicist is concerned. The more specific formulation is no function that you would regard as sufficiently nice (for use in physics) exists.

To actually put this down in concrete terms, there are such functions, but they have various pathological properties.${}^1$ What you are basically looking for is the inverse of a space-filling curve. A space-filling curve is a surjection $\mathbb{R} \to \mathbb{R}^2$ (and you can extend to $\mathbb{R}^n$ without much trouble), so its inverse is an injection $\mathbb{R}^2 \to \mathbb{R}$.

Searching on this site or MathOverflow will turn up a large variety of posts showing why you don't get any nice properties for more than a small set of points: most of this is based on them not being Lipschitz functions.

${}^1$ And indeed, I know at least one senior mathematician in my department who will assert that the existence of these things is much weirder than anything you can do with the axiom of choice, Banach-Tarski included.