“…Remark For the case where a (near‐) integrated component is present at all of the zero and seasonal frequencies, such that h k = 1, for k = 0,…,⌊ S /2⌋, it follows from Lemma A.1 of del Barrio Castro et al (), noting that the circulant matrices , k = 1,…, S ∗ , which appear in Lemma A.1 of del Barrio Castro et al () can be written as , that The result in is a special case of Lemma 1. Notice that in this example each of the ψ 0 , ψ S /2 , and , k = 1,…, S ∗ , weights is equal to 1/ S .…”