“…In [7], Fridli introduced an atomic Hardy type space H 1 F (0, ∞) as follows. A measurable function a defined on (0, ∞) is said to be an F -atom if (a) a = 1 δ χ (0,δ) , for some δ > 0, where χ (0,δ) denotes the characteristic function on the interval (0, δ), or (b) there exists a bounded interval I ⊂ (0, ∞) such that supp a ⊂ I, I a(x)dx = 0, and a L ∞ ((0,∞), dx) ≤ |I| −1 , where |I| denotes the length of I.…”