Let $\Omega\subset\mathbb R^n$ be a bounded domain with a sufficiently smooth boundary $\partial\Omega$. We assume $\lambda_1\in\mathbb R$ is the principle eigenvalue of the operator $$ -\Delta:\ H^2(\Omega)\to L^2(\Omega), $$ taken with zero Dirichlet boundary condition. Now for any $\lambda\in[0,\lambda_1)$ so that $\lambda$ is not an eigenvalue of $L$, the following boundary value problem \begin{equation} \left\{ \begin{alignedat}{2} &-\Delta u = \lambda u + f &\quad& \mbox{in $\Omega$,} \\ &u=0 &\quad& \mbox{on $\partial\Omega$,} \end{alignedat} \right. \end{equation} where $f$ is assumed to be a $L^2(\Omega)$-function, admits a unique weak solution $u_\lambda\in H_0^1(\Omega)$ via Fredholm alternative principle. Moreover, we have the following estimate $$ \|u_\lambda\|_{L^2(\Omega)} \le C(\lambda) \|f\|_{L^2(\Omega)}. $$
This constant will blow up when $\lambda$ approaches the principle eigenvalue $\lambda_1$.
I am interested to see that what kind of contradiction will occur if we assume $C$ is independent of $\lambda\in[0,\lambda_1]$ for a fixed $f\in L^2(\Omega)$.