Evidences are given that two classes of the transient JR-absorption bands: (a) with max. at 0.27-0.36 eV in NaC1, KC1, KBr, KI and RbC1 (due to 'shallow electron traps' according G. Jacobs or due to "bound poiarons" according B. V. Korovkin and T. A. Lebedkina) and (b) with max. at 0.15-0.36 eV in Nal, NaBr, NaC1:I, KC1:I, RbC1:I and RbBr:I (due to "on-centre STE localised at iodine dimer" according M. Hirai and collaborators) are caused by the same defect -"atomic alkali impurity" centre [M]00e (electron e trapped by a substitutional smaller size alkali cation impurity [M]0). The Moliwo-Ivey plots (for the transient JR-absorption bands) ofthe zero-phonon line energy E0 (for NaC1, KC1, KBr, RbCl and NaBr, KC1:I) and/or the low-energy edge values E0 (for NaT, RbC1:I, RbBr:Ij) versus anion-cation distance (d) evidence that two types of the [M]°e centres are predominant: (a) [Nai°e in the KX and RbX host crystals with the relation E06. 15/d274; (b) [Li]°e in the NaX host crystals -E029.4/d472. The Moliwo-Ivey relation E018.36/d27° is fulfilled as well for the F' band in NaCl, KC1, KBr, KI, RbC1, RbI if we use the F' centre optical binding energy values B0.