Step 1: Centre and axial fields.
A circular coil gives $B_c = \dfrac{\mu_0 I}{2r}$ at its centre and $B_a = \dfrac{\mu_0 I r^2}{2(r^2+x^2)^{3/2}}$ at axial distance $x$.
Step 2: Take the ratio.
Dividing the axial field by the centre field cancels $\mu_0 I$: \[ \frac{B_a}{B_c} = \frac{r^3}{(r^2+x^2)^{3/2}}. \]
Step 3: Substitute $x = \sqrt{3}\,r$.
Then $r^2 + x^2 = r^2 + 3r^2 = 4r^2$.
Step 4: Plug into the ratio.
\[ \frac{B_a}{B_c} = \frac{r^3}{(4r^2)^{3/2}}. \]
Step 5: Simplify the denominator.
$(4r^2)^{3/2} = 4^{3/2}\,r^{3} = 8r^3$, so $\dfrac{B_a}{B_c} = \dfrac{r^3}{8r^3} = \dfrac{1}{8}$.
Step 6: Use $B_c = 1\,\text{T}$.
$B_a = \dfrac{1}{8}\times 1 = \dfrac{1}{8}\,\text{T}$.
\[ \boxed{\dfrac{1}{8}\ \text{T}} \]