The donor concentration in a non-degenerate semiconductor is related to the shift in the Fermi level by:
\[
\Delta E_F = k_B T \ln \left( \frac{N_d}{N_{d0}} \right),
\]
where:
- \( N_d \) is the final donor concentration,
- \( N_{d0} \) is the initial donor concentration.
Given that the donor concentration is increased by a factor of 100, we have:
\[
\frac{N_d}{N_{d0}} = 100.
\]
Substitute \( k_B T = 25 \, \text{meV} \):
\[
\Delta E_F = 25 \, \text{meV} \times \ln(100) \approx 25 \, \text{meV} \times 4.605 = 115 \, \text{meV}.
\]
Thus, the shift in the Fermi level is approximately 115 meV.