Fig. S2.

Shape fluctuations of CGS and NE are cell cycle-dependent. (A) Wavenumber-dependent fluctuations $⟨u_q^2⟩$ with error bars (SE) calculated for CGS (H2B-GFP, green solid line, n = 47) and NE (LMNA-GFP, red solid line, n = 47). (B) The $⟨u_q^2⟩$ of CGS calculated with error bars (SE) for four groups determined based on their measured nuclear area $A$. (C) The $⟨u_q^2⟩$ of NE calculated with error bars (SE) for four groups determined based on their measured nuclear area $A$. (D) Wavenumber-dependent fluctuations $⟨u_q^2⟩$ with error bars (SE) of CGS (green) and NE (red) measured at different times during the cell cycle; $⟨u_q^2⟩$ for both CGS and NE exhibits a monotonous decrease with increasing time during the cell cycle. (E) Wavenumber-dependent fluctuations $⟨u_q^2⟩$ as a function of wavelength $\lambda$ with error bars (SE) of CGS (green) and NE (red) measured at different times during the cell cycle.