First, you can use the following general property of linear equations or systems. For Wronskian of any system of solutions only one statement is true:
- Wronskian is always zero, for all $x$ where solutions are defined. Thus, solutions of this system are linearly dependent.
- Wronskian is always non-zero and solutions are linearly independent.
This general property can be proven without Abel's formula, but we can use it here (formulas are taken from here):
Theorem
Let $y_1$ and $y_2$ be any two solutions of $y'' + p ( x ) y'+ q ( x ) y =0$ , then $$W \lbrack y_1 ,y_2 \rbrack(x) = C \cdot \exp{\left (− \int\limits_{x_0}^{x} p ( u )\, du \right )},$$ where $C$ is a constant.
Exponential function never turns zero at any finite value, so this justifies our dichotomy: if $W[y_1, y_2](x) =0$ at some point then $C = 0$ and $W[y_1, y_2](x) \equiv 0$. I implicitly assume here that $p(x)$ is something like continuous function or at least integrable — this excludes the case when integral inside of exponential function is infinite.
Returning back to your question, we can state the following: were the function $\sin t^2$ a solution of second order ODE, then it must exist second function which is also a solution, it is linearly independent from $\sin t^2$ and thus their Wronskian must be everywhere non-zero. But we see that Wronskian of any function and $\sin t^2$ is always zero at $x = 0$. This is a contradiction which ends proof of your statement.