(GMT−24π2)1/3−R\left(\dfrac{G M T^{-2}}{4 \pi^{2}}\right)^{1 / 3}-R(4π2GMT−2)1/3−R
(GMT24π2)1/3−R\left(\dfrac{G M T^{2}}{4 \pi^{2}}\right)^{1 / 3}-R(4π2GMT2)1/3−R
(GMT24π2)1/3−R\left(\dfrac{G M T^{2}}{4 \pi^{2}}\right)^{1 /\sqrt{3}}-R(4π2GMT2)1/3−R
(GMT−24π2)1/3−R2\left(\dfrac{G M T^{-2}}{4 \pi^{2}}\right)^{1 / 3}-R^2(4π2GMT−2)1/3−R2