Step 1: Using the components of the magnetic field.
The resultant magnetic field \( B \) is calculated using the vector sum of the vertical and horizontal components:
\[
B = \sqrt{B_v^2 + B_h^2}
\]
where \( B_v = 2 \times 10^{-5} \, \text{T} \) and \( B_h = 2\sqrt{3} \times 10^{-5} \, \text{T} \). Substituting these values:
\[
B = \sqrt{(2 \times 10^{-5})^2 + (2\sqrt{3} \times 10^{-5})^2} = 4 \times 10^{-5} \, \text{T}
\]
Step 2: Finding the angle of dip.
The angle of dip \( \delta \) is given by:
\[
\tan \delta = \frac{B_v}{B_h}
\]
Substituting the values:
\[
\tan \delta = \frac{2 \times 10^{-5}}{2\sqrt{3} \times 10^{-5}} = \frac{1}{\sqrt{3}}
\]
Thus,
\[
\delta = \tan^{-1} \left( \frac{1}{\sqrt{3}} \right)
\]
Step 3: Conclusion.
Thus, the angle of dip is \( \tan^{-1} \left( \frac{1}{\sqrt{3}} \right) \) and the resultant magnetic field is \( 4 \times 10^{-5} \, \text{T} \), corresponding to option (D).