Electron de- Broglie wavelength
\(\lambda=\frac{h}{m v}=\frac{h}{\sqrt{2 m K}}\)
\(\Rightarrow K=\frac{h^2}{2 m \lambda^2}\)
Now, cut- off wavelenth for continuous \(X\) - rays,
\(\lambda_c=\frac{h c}{K}=\frac{h c}{\left(h^2 / 2 m \lambda^2\right)}\)
\(\therefore \lambda_c=\frac{2 m c \lambda^2}{h}\)
Hence, option \((C)\) is correct.