“…In particular, it is well‐known that isotropic random fields on the sphere can be decomposed by means of the spectral representation theorem into the sum of orthogonal components, each of them corresponding to a different multipole . The behavior of geometric functionals in the high‐frequency/high‐energy limit for these components has been studied by several authors in recent years, starting from Nazarov and Sodin (, ) for the number of connected components; Wigman () for the nodal length; and then including, among others, Marinucci and Rossi () and Marinucci and Wigman () for the excursion area; Marinucci and Wigman (), Marinucci and Wigman () and Rossi () for the defect; Cammarota and Marinucci () for the Euler‐Poincaré characteristic; Marinucci, Peccati, Rossi, and Wigman (), Marinucci, Rossi, and Wigman (), Rossi () and Wigman () for the distribution of the nodal length; Cammarota, Marinucci, and Wigman () for the critical values; and Cammarota and Wigman () for the total number of critical points (see also Dalmao, Nourdin, Peccati, and Rossi (), Krishnapur, Kurlberg, and Wigman (), Maffucci (), Peccati and Rossi (), Rossi and Wigman (), Rudnick and Wigman () for related works covering also the 2‐dimensional torus; Maffucci () for the 3‐dimensional torus; and Nourdin, Peccati, and Rossi () for planar random waves).…”