Table 1: Initial models and their parametrisation: A and $\beta _{{\rm rot}}$ are the rotation law parameter (Eq. (12)) and the ratio of rotational to gravitational energy, respectively. Larger values of A correspond to more rigidly rotating cores. $\Gamma _1$ is the sub-nuclear adiabatic index of our hybrid equation of state (see Sect. 2.2).
Model $A [{\rm cm}]$ Model $\beta_{{\rm rot}} [\%]$ Model $\Gamma _1$

A1 $5\times 10^{9}$ B1 $\approx$ 0.25 G1 1.325

A2 $1\times 10^{8}$ B2 $\approx$ 0.45 G2 1.32

A3 $5\times 10^{7}$ B3 $\approx$ 0.9 G3 1.31

A4 $1\times 10^{7}$ B4 $\approx$ 1.8 G4 1.30

B5 $\approx$ 4.0 G5 1.28

**Table 1:** Initial models and their parametrisation: A and $\beta _{{\rm rot}}$ are the rotation law parameter (Eq. (12)) and the ratio of rotational to gravitational energy, respectively. Larger values of A correspond to more rigidly rotating cores. $\Gamma _1$ is the sub-nuclear adiabatic index of our hybrid equation of state (see Sect. 2.2).
Model	$A [{\rm cm}]$	Model	$\beta_{{\rm rot}} [\%]$	Model	$\Gamma _1$
A1	$5\times 10^{9}$	B1	$\approx$ 0.25	G1	1.325
A2	$1\times 10^{8}$	B2	$\approx$ 0.45	G2	1.32
A3	$5\times 10^{7}$	B3	$\approx$ 0.9	G3	1.31
A4	$1\times 10^{7}$	B4	$\approx$ 1.8	G4	1.30
		B5	$\approx$ 4.0	G5	1.28

Source LaTeX | All tables | In the text