The de Broglie wavelength of a particle is given by:
\[
\lambda = \frac{h}{p} = \frac{h}{\sqrt{2m k_B T}}
\]
where:
- \( h \) is Planck’s constant,
- \( p \) is the momentum,
- \( m \) is the mass,
- \( k_B \) is Boltzmann’s constant,
- \( T \) is the absolute temperature in Kelvin.
1. Convert temperatures to Kelvin:
\[
T_1 = 77 + 273 = 350 \text{ K}
\]
\[
T_2 = 1127 + 273 = 1400 \text{ K}
\]
2. Ratio of wavelengths:
Since \( \lambda \propto \frac{1}{\sqrt{T}} \),
\[
\frac{\lambda_2}{\lambda_1} = \sqrt{\frac{T_1}{T_2}}
\]
\[
= \sqrt{\frac{350}{1400}} = \sqrt{\frac{1}{4}} = \frac{1}{2}
\]
\[
\lambda_2 = \frac{\lambda_1}{2}
\]
Thus, the correct answer is \(\boxed{\frac{\lambda}{2}}\).