“…These materials, subject to applications at different frequency bands, can be grouped into three categories: (1) high‐ k materials ( k ∼80–100) but low Q × f s, such as BaO–Ln 2 O 3 –TiO 2 (Ln=La, Nd, Sm, etc. ) 1–4 ; (2) med‐ k materials ( k ∼40–50) with Q × f ∼30 000–80 000 GHz, such as Ba 2 Ti 9 O 20 , (Sn,Zr)TiO 4 , and Nd(Zn 1/2 Ti 1/2 )O 3 ‐SrTiO 3 5–7 ; and (3) extremely high‐ Q × f materials (>150 000 GHz) with k ∼15–30, such as Ba(Mg 1/3 Ta 2/3 )O 3 , Ba(Zn 1/3 Ta 2/3 )O 3 , Nd(Zn 1/2 Ti 1/2 )O 3 , and Nd(Co 1/2 Ti 1/2 )O 3 8–11 . However, due to the extension of the carrier frequency of interest in communication systems to a higher frequency range (such as millimeter wave), materials with high‐ k or med‐ k have become of less interest.…”