Considering the Sturm-Liouville problem $$-y'' = \lambda y, $$ with $y(0)=0$ and $y'(1)-y(1)=0$, and where we let $\lambda_0 < \lambda_1 < \lambda_2 <...$ be the eigenvalues in increasing order, I want to show that $\lambda_0 = 0$ and that $(\pi n)^2 < \lambda_n < ((n+\frac{1}{2})\pi)^2$ for $n \geq 1$.
I've found that the general solution is $y(x) = A\cos(\sqrt{\lambda} x) + B\sin(\sqrt{\lambda} x)$. So $y(0) = 0$ gives $A=0$ and we're left with $y(x) = B\sin(\sqrt{\lambda}x)$. Then $y'(1)-y(1)=0$ gives $\tan (\sqrt{\lambda}) = \sqrt{\lambda}$.
Is this enough to say that $\lambda$ must be nonnegative, because otherwise $\sqrt{\lambda}$ would be undefined (or at least not real, and the eigenvalues of a Sturm-Liouville problem must be real)?
Clearly $\tan (\sqrt{\lambda}) = \sqrt{\lambda}$ is satisfied by $\lambda = 0$, so if the above was enough to show that $\lambda$ is nonnegative, then we have found that $\lambda_0 = 0$.
But then I am pretty lost on how to show that $(\pi n)^2 < \lambda_n < ((n+\frac{1}{2})\pi)^2$ for $n \geq 1$.
I know that $\tan (k)$is strictly increasing on each interval $\left((n-\frac{1}{2}\pi), (n+\frac{1}{2})\pi \right)$, and positive when $k \in \left(n\pi, (n+\frac{1}{2})\pi \right)$. But I can't seem to figure out why this implies that $\lambda_n \in \left((n\pi)^2, ((n+\frac{1}{2})\pi)^2\right)$. Why couldn't we have for example $\lambda_1 \in \left((2\pi)^2,(\frac{5\pi}{2})^2\right)$?