Correct answer: option 1
The potential at the centre of a spherical shell can be written as the sum of potential due to two identical hemispheres
Vtotal=Vhemisphere1+Vhemisphere2
⟹Vtotal=2 Vhemisphere
⟹ $\frac{\sigma R }{\epsilon_0}$ =2Vhemisphere
⟹Vhemisphere= $\frac{\sigma R }{2\epsilon_0}$