The de Broglie wavelength \( \lambda \) of a particle is related to its momentum \( p \) by:
\[
\lambda = \frac{h}{p}
\]
where \( h \) is Planck's constant. For a particle with kinetic energy \( E \), its momentum is:
\[
p = \sqrt{2mE}
\]
Thus, the de Broglie wavelength \( \lambda \) is:
\[
\lambda = \frac{h}{\sqrt{2mE}}
\]
Now, consider two particles, one with energy \( E \) and the other with energy \( 3E \). The ratio of the wavelengths is:
\[
\frac{\lambda_1}{\lambda_2} = \frac{\frac{h}{\sqrt{2mE}}}{\frac{h}{\sqrt{2m(3E)}}} = \frac{\sqrt{3}}{1}
\]
Thus, the ratio of wavelengths is \( 1: \sqrt{3} \).