The de Broglie wavelength \( \lambda \) of a particle is calculated using \( \lambda = \frac{h}{p} \). Here, \( h \) is Planck's constant, given as \( 6.626 \times 10^{-34} \, \text{J} \cdot \text{s} \), and \( p \) is the particle's momentum.
For an electron with kinetic energy \( E \), its momentum \( p \) is derived from \( E = \frac{p^2}{2m} \), resulting in \( p = \sqrt{2mE} \). In this formula, \( m \) is the electron's mass, \( 9.11 \times 10^{-31} \, \text{kg} \), and \( E \) is its kinetic energy.
The electron's kinetic energy is provided as 5 eV. This energy is converted to joules using the conversion factor \( 1 \, \text{eV} = 1.602 \times 10^{-19} \, \text{J} \). Therefore, \( E = 5 \, \text{eV} = 5 \times 1.602 \times 10^{-19} \, \text{J} = 8.01 \times 10^{-19} \, \text{J} \).
The momentum \( p \) is then calculated as \( p = \sqrt{2 \times (9.11 \times 10^{-31}) \times (8.01 \times 10^{-19})} = 1.347 \times 10^{-24} \, \text{kg} \cdot \text{m/s} \).
Finally, the de Broglie wavelength is computed: \( \lambda = \frac{6.626 \times 10^{-34}}{1.347 \times 10^{-24}} = 4.92 \times 10^{-10} \, \text{m} \), which is equivalent to \( 0.49 \, \text{nm} \).
The closest answer is \( \boxed{0.55 \, \text{nm}} \).