I guess the problem is behind interpreting of what we know about $\alpha(t)$.
In particular, great point by lulu about second condition.
First "condition":
$$P(t_1 \le t \le t_2)=\int_{t_1}^{t_2}\alpha(t)dt \quad \forall t,t_1,t_2\in\Re_0^+\tag{1}\label{1}$$
Since in this context it's just another way to say that $\alpha(t)$ represents a probability density for probability distribution $P$ you shouldn't be able to get something specific about $\alpha(t)$ from the first "condition".
So let's consider second condition:
$$P(0\le t \le t_1)=P(t_0+t_1\le t \le t_0|t\ge t_0) \quad \forall t,t_0,t_1\in\Re_0^+\tag{2}\label{2}$$
Let's rewrite to perform "more functional" approach:
$$P(t \le t_1)=\frac{P(t_0\le t \le t_0+t_1)}{P(t\ge t_0)}$$
Notice that $P(t\ge t_0)=0$ is pointless, so let's multiply both parts by it:
$$P(t \le t_1)P(t\ge t_0)=P(t_0\le t \le t_0+t_1)=\\P(t \le t_1)(1-P(t\le t_0))=P(t \le t_0+t_1)-P(t \le t_0)=\\P(t \le t_1)-P(t \le t_1)P(t\le t_0)=P(t \le t_0+t_1)-P(t \le t_0)$$
Denoting $f(z)=P(t \le z)$, $x=t_1$, $y=t_0$ and getting:
$$f(x)-f(x)f(y)=f(y+x)-f(y)\\f(x+y)=f(x)+f(y)-f(x)f(y)\tag{3}\label{3}$$
Considering $0\le f(x)\le1$ and solving (in a similar way) we get $f(x)=1-e^{Cx},\,C<0$ and consequently $\alpha (t)=f'(t)=-Ce^{Cx}$ (we can get the same even with constraints $x>0,\,y>0$ in \eqref{3}).
However, if you refer to $t_0=0$ as to the case it seems like $t_0$ is meant to be some fixed value (and if so $t_0=0$ is pointless in \eqref{2}).
With the last interpretation $t_0=0$ is pointless (as it transforms \eqref{2} into identity) and similarly to the previous approach we can get:
$$f(x+t_0)=f(x)+f(t_0)-f(x)f(t_0),\,f(t_0)>0\tag{4}\label{4}\\f(x)=1-g(x)\\1-g(x+t_0)=(1-g(x))+(1-g(t_0))-(1-g(x))(1-g(t_0))\\1-g(x+t_0)=1-g(x)+1-g(t_0)-1+g(x)+g(t_0)-g(x)g(t_0)\\g(x+t_0)=g(x)g(t_0)$$
If $g(t_0)=0$ then $f(t_0)=1-g(t_0)=1$ and \eqref{4} transforms into $f(x+t_0)=1\,\, \forall x\ge 0$ what is already satisfied inasmuch as $f$ stands for probability distribution and reaches value $1$ at $t=t_0$. So any probability distribution function $f$ that satisfies $f(t_0)=1$ and \eqref{1} will also satisfy both conditions (for instance $f(t)=\sin (\frac{\pi t}{2t_0})$ if $t\le t_0$ otherwise $f(t)=1$ and corresponding $\alpha (t)=f'(t)$).
If $g(t_0)>0$ we can use the following substitution:
$$g(x)=h(x)g(t_0)^{x/t_0}\\h(x+t_0)g(t_0)^{(x+t_0)/t_0}=h(x)g(t_0)^{x/t_0}g(t_0)^{t_0/t_0}=h(x)g(t_0)^{(x+t_0)/t_0}\\h(x+t_0)=h(x)$$
Returning back to $f$ we get $f(x)=1-h(x)(1-f(t_0))^{x/t_0}$ where $h$ is periodic with period $t_0$ and such that $f$ satisfies \eqref{1} ($h(0)=1$ will also come in hand).
To provide another non-exponential example for this "broader" case let's take for convenience $t_0=1$, $f(t_0)=0.5$ and $h(x)=1+\frac{\sin^2 (\pi x)}{8}$, so $f(t)=1-(1+\frac{\sin^2 (\pi t)}{8})0.5^t$ and correspondent $\alpha (t)=f'(t)=\ln (2)(1+\frac{\sin^2 (\pi t)}{8})0.5^t-\pi \sin (2\pi t)0.5^{t+3}$ (you can check that $\alpha (t)\ge0$, $f(t)\rightarrow 1$ as $t\rightarrow \infty$, so that condition \eqref{1} is also satisfied).
In short, your claim is provable ($\alpha(t)$ is and only exponential) if we assume condition \eqref{2} $\forall t_0,t_1\in \Re$.
From the other hand, if $t_0$ is fixed value (and by the way the same concerning $t_1$ thanks to \eqref{3} being symmetrical) non-exponential examples of $\alpha(t)$ can be provided as well.