This question builds on top of my former question in which I asked whether constant symbols are necessary in first-order theories. In that question I gave a rough idea on how to get rid of these symbols, which was not completely thought through. I will try to fix this now and would be glad if someone can verify this approach.
Lets say we have a first-order theory $T$
- over a language $L$ with (possibly countably infinite many) constant symbols $c_i$.
- we choose (possibly countably infinite many) predicates $\varphi_i(x_1,...,x_{n_i})$ so that $\varphi_i(c_{\sigma_i(1)},...,c_{\sigma_i(n_i)})$ makes up an axiom system of $T$. The $\sigma(i)$ will choose the constant symbols that are present in the $i$-th axiom and $n_i$ (possibly zero) will denote how many are in there.
I want to construct a theory $T'$ over a language $L'$ which got all the constant symbols removed. Still, $T$ and $T'$ should have the exact same models (in some sense). I will do this by replacing the axioms $\varphi_i$
I will need some shorthand notations:
- I write $\vec x$ for a sequence of some of the variables $x_1,x_2,...$ where the exact names are derived from the place of use of this sequence. E.g. in $(\forall \vec x)\varphi_i(\vec x)$ the sequence will consist of the variables $x_{\sigma_i(1)},...,x_{\sigma_i(n_i)}$.
- I write $\vec x=\vec y$ for the statement that the two sequences agree element-wise on the variables that are contained in both of them. If a variable $x_j$ is not in both sequences then $\vec x=\vec y$ does not contain $x_j$.
- I write $\Delta(\vec x)$ for the statement, that all the variables of $\vec x$ are different. So $\Delta(\vec x)$ contains the statement $x_i\not= x_j$ for any pair of distinct variables $x_i,x_j\in\vec x$ conjugated together.
Now I am going to replace the axiom $\varphi_i$ by
$$(A_i)\qquad (\exists \vec x)[\Delta(\vec x)\wedge \varphi_i(\vec x)\quad\wedge\quad(\forall \vec y)\left[\Delta(\vec y)\wedge \varphi_i(\vec y)\rightarrow \vec x=\vec y]\right],$$
and for any pair $\varphi_i, \varphi_j$ of former axioms I will introduce the axiom
$$(A_{ij})\qquad (\forall \vec x \forall \vec y)[\varphi_i(\vec x)\wedge\varphi_j(\vec y)\rightarrow \vec x= \vec y] $$
In the special case that we have constant symbols in $T$, but no axiom contains any of them, I will introduce the axiom $(\exists x)[x=x]$ to ensure that there is at least one element in the model.
In my opinion, this reflects all the properties that the constants inherently brought into the theory. Is this correct? Does this give me an equivalent theory (in some sense, see note 2)?
NOTE:
I do not think we should get rid of contant symbols. My motivation is purely academic in the sense, that I want to know whether there is always an equivalent theory without constant symbols, like there is always an equivalent theory replacing function symbols and constant symbols by relation symbols.
As Giorgio and Rene pointed out in there answers to my former question, there are legitimate and useful applications for constant symbols. I do not doubt this.
NOTE 2:
I am not sure how to directly compare the (whole "space" of) models of these theories as they are defined over different languages. So the first on is an $L$-structure, the second one an $L'$-structure. Is this done by comparing the categories of structures created by these two theories?