In almost any calculus book I can think of (for example, "The Calculus with analytic geometry" by Louis Leithold), and even the books of analysis (for example, the Rudin's "Principles of analysis" and "Real and complex analysis"), one can find that an integral is represented with the $dx$ (the differential; actually $x$ here is a dummy variable), written after the integrand. For example: $$ \int f(x)dx$$ However, on reading papers which I would call about "theoretical physics", I have found very often the other way around: the $dx$ or whatever variable being integrated, is written before the integrand. Take for example "Special Relativity induced by Granular Space", by Petr Jizba and Fabio Scardigli, 2013, equation (4): $$w(\zeta ,t_1+t_2)=\int_0^\zeta {\rm d}\zeta' w(\zeta',t_1)w(\zeta - \zeta',t_2)$$ notice the romanization of ${\rm d}$ as opposite of $d$, from the previous example.
I have the feeling that it is not just a matter of style, but there is a meaning involved in the usage of either way.
Question: what is involved in choosing to write either $\int f(x) dx$ as opposite to $\int {\rm d}x f(x)$ ? is this (these) reason(s) of mathematical nature or are they related with the problem that is being dealt with in theoretical physics?
Also, I would appreciate if someone points to a bibliographical reference were such justification for writting it so, is being explained.