Caveat: this is a longer answer, but I find it easier to understand just what's going on here.
Using the method of characteristics, you examine the function $u$ along a trajectory $(x(t),y(t))$ through some point $(x_0,y_0)$ (usually in a boundary value problem you choose a convenient pair for the initial conditions, i.e. where you have boundary data) converting the partial differential equation into an ordinary differential equation. Namely, you want
$$
x'(t)=1\\
y'(t)=2x(t)
$$
since then $\frac{d}{dt}u(x(t),y(t))=u_x+2x(t)u_y=0$ for $u$ which solve the pde. So along trajectories of the above sort, as $u(x(t),y(t))=u(x_0,y_0)$.
Solving the coupled system, we find
$$
x(t)=t+x_0\\
y(t)=t^2+2x_0t+y_0
$$
and eliminating the parameter $t$, we have that $u$ is constant as long as
$$
y=(x-x_0)^2+2x_0(x-x_0)+y_0=x^2-x_0^2+y_0
$$
We know that
$$
u(x,y)=u(x,x^2+y_0-x_0^2)=u(x_0,y_0)
$$
From here, it is obvious that the first condition is easy to satisfy. We know that the desired function is constant along the parabola $y=x^2$, this condition just fixes such a constant to be $2$.
For the second, it is clearly impossible, since we know that $u$ is constant on the parabola $y=x^2$, but $e^{-x}$ is not constant.
For the third, we have data on the line $x=0$, so it is convenient to set $x_0=0$. Then your condition yields
$$
u(x,y)=u(0,y_0)=e^{-y_0}
$$
but our choice of characteristic is valid for any $y_0$, so what is $y_0$ when $x_0$ is zero in terms of $x$ and $y$? It is $y-x^2$. Giving us the answer
$$
u(x,y)=e^{-(y-x^2)}
$$