Table 3.

Various Shape Properties Based on the Eigenvalues of Gyration Tensor G Are Defined Here for N_f = 0, N_f = 1, and ICE-Normalized Contact Matrix for K562 and GM12878 Cell Lines

Shape properties	K562 (ON state)			GM12878 (OFF state)
	Nf = 0	Nf = 1	ICE	Nf = 0	Nf = 1	ICE
$\langle {\lambda }_1^2\rangle /R_g^2$	0.058	0.057	0.078	0.081	0.066	0.083
$\langle {\lambda }_2^2\rangle /R_g^2$	0.164	0.175	0.189	0.201	0.177	0.195
$\langle {\lambda }_3^2\rangle /R_g^2$	0.778	0.768	0.732	0.718	0.757	0.722
$\langle {\lambda }_2^2\rangle /\langle {\lambda }_1^2\rangle$	2.828	3.054	2.417	2.479	2.703	2.357
$\langle {\lambda }_3^2\rangle /\langle {\lambda }_1^2\rangle$	13.412	13.422	9.356	8.874	11.563	8.727
B/$R_g^2$	0.667	0.652	0.599	0.578	0.636	0.583
C/$R_g^2$	0.106	0.118	0.111	0.120	0.112	0.112
S	0.913	0.816	0.988	0.772	0.926	0.867
κ2	0.545	0.513	0.537	0.452	0.525	0.497