“…This relation is independent on EOS and it is a good approximation for the slowly rotating NSs. However, according to numerical results, inclusion of relativistic corrections may increase f GW by a few tens of percent (Lockitch et al, 2003;Pons et al, 2005;Idrisy et al, 2015;Jasiulek & Chirenti, 2017). Exact value depends mostly on the object compactness C (dimensionless massradius ratio: C ≈ 0.207 M 1.4 M 10 km R , for NSs typically 0.11 C 0.31), but also on rotational frequency of the object (Lindblom et al, 1999;Idrisy et al, 2015;Jasiulek & Chirenti, 2017), including rigid versus differential rotation (Stavridis et al, 2007;Idrisy 12 Unlike in the case of the elastic deformations, what was shown in Section 2, r-modes affect equation of motion δv = α(r/R) l RωY B lm exp(iω r t), where α is dimensionless amplitude and ω r = − 2m l(l+1) ω is the angular frequency in co-rotating frame.…”