The biggest problem with your work is that you use the unfortunate convention to use $y$ both as a variable, and also for the function relating $y$ to $t$.
I will introduce the letter $f$ for that function; that is, $y$ is related to $t$ by the equation $y = f(t)$.
You can't cancel the differentials in the sense of combining everything into a single fraction cancelling like terms out of the numerator and denominator. However, it is true (in single-variable calculus) that
$$ \frac{dy}{dx} \, dx = dy \qquad \qquad \frac{dy}{dx} \frac{dz}{dw} = \frac{dy}{dw} \frac{dz}{dx} $$
so you can do things that look very much like what you can do with fractions, even if you can't treat them as actually being fractions.
In multivariable calculus, for most pairs of differentials, you can't write one as a multiple of the other, so ratios like $\frac{dy}{dx}$ are nonsensical unless you happen to know $y$ and $x$ are related by a differentiable function. Partial derivatives, e.g. $\frac{\partial y}{\partial x}$, have a lot of subtle issues and shouldn't really be treated like ratios at all.
When you're using notation involving variables like $y$, rather than one using functions like $f$, integrals are often better thought as integrating over a path rather than between two numbers. It's not usually introduced that way, however, since it would make definitions somewhat more complicated.
At one endpoint of the path, you have $t=0$ and $y = f(0)$, and at the other endpoint, you have $t=+\infty$ and $y = f(+\infty)$. It doesn't really matter which letter you use in an expression as the 'variable' for the path integral, since the path 'remembers' what all the variables should be. But, of course, if you don't use notation reminding yourself that you're thinking of a path, you can get into trouble. (e.g. you could easily forget half-way through and think you've written numbers that are the values of the variable you're currently using)
Finally, you should take care to remember that this is an improper integral: it really should be computed as a limit of proper integrals. I'm not sure if any of the ideas I've described here run into problems when you try to use them in an improper integral.