Let $u$ and $\tilde u$ be two solutions, and let $v = u - \tilde u$. Then
$$ v_{tt} + v_{xxxx} = 0,\\ v(0,t) = v(1,t) = v_x(0,t) = v_x(1,t) = 0, \\v(\cdot,0) = v_t(\cdot,0) = 0 .$$
Multiply the first equation by $v_t$, and integrate w.r.t. $x$ from $x=0$ to $1$, and integrate by parts twice on one of the integrals (noting $v_t(0,t) = \cdots = v_{tx}(1,t) = 0$), and use the product rule for differentiation to see $(v_t^2)_t = 2v_{tt}v_t$ and $(v_{xx}^2)_t = 2v_{xxt}v_{xx}$, to conclude
$$ \frac12 \frac{\partial}{\partial t}\left(\|v_t\|_2^2 + \|v_{xx}\|_2^2\right) = 0$$
where we define $\|f\|_2^2 = \int_0^1 |f(x)|^2 \, dx $. Hence
$$ \|v_t\|_2^2 + \|v_{xx}\|_2^2 = \text{constant} .$$
Setting $t=0$, we see that this constant is zero. Hence for all $t>0$
$$ v_t = 0, v_{xx} = 0 .$$
Since $v_{xx} = 0$, from the boundary conditions we obtain $v = 0$.