Step 1: Find tension at the highest point.
At the highest point of vertical circular motion, both tension and weight act towards the center.
Therefore,
\[
T_H+mg=\frac{mv_H^2}{r}
\]
Given,
\[
v_H=\sqrt{7gr}
\]
So,
\[
v_H^2=7gr
\]
Substitute:
\[
T_H+mg=\frac{m(7gr)}{r}
\]
\[
T_H+mg=7mg
\]
\[
T_H=6mg
\]
Step 2: Find speed at the lowest point using energy conservation.
The particle descends through a height
\[
2r
\]
from the highest point to the lowest point.
Using conservation of mechanical energy:
\[
\frac{1}{2}mv_L^2
=
\frac{1}{2}mv_H^2+mg(2r)
\]
Substitute
\[
v_H^2=7gr
\]
\[
\frac{1}{2}mv_L^2
=
\frac{1}{2}m(7gr)+2mgr
\]
\[
\frac{1}{2}mv_L^2
=
\frac{7}{2}mgr+2mgr
\]
\[
\frac{1}{2}mv_L^2
=
\frac{11}{2}mgr
\]
Thus,
\[
v_L^2=11gr
\]
Step 3: Find tension at the lowest point.
At the lowest point,
\[
T_L-mg=\frac{mv_L^2}{r}
\]
Substitute
\[
v_L^2=11gr
\]
\[
T_L-mg=\frac{m(11gr)}{r}
\]
\[
T_L-mg=11mg
\]
\[
T_L=12mg
\]
Step 4: Find the ratio of tensions.
\[
T_H:T_L
=
6mg:12mg
\]
\[
=1:2
\]
Step 5: Final conclusion.
Hence, the required ratio is
\[
\boxed{1:2}
\]