Abstract

The crystal and molecular structures of 2′-amino-6′-dibutylamino-3′-methylspiro[isobenzofuran-1(3 H), 9′[9 H]xanthen]-3-one ( 1), 2′-amino-6′-( N-cyclohexyl- N-methylamino)-3′-methylspiro[isobenzofuran-1(3 H), 9′[9 H]xanthen]-3-one ( 2) and 2′-(2-chlorophenyl)amino-6′-dibutylaminospiro[isobenzofuran-1(3 H), 9′[9 H]xanthen-3-one ( 3) have been determined by single-crystal X-ray diffraction analysis. Atom-atom non-bonded potential energy and semiempirical quantum chemical calculations have been performed. The xanthene rings of 1 to 3 are slightly bent and the phthalide rings are planar. The phthalide ring moieties are almost perpendicular (88.9(1)–93.5(5)°) to the xanthene rings. The bond lengths C(6)O(2) are apparently extended from the normal C(sp 3O (lactone) length. The temperature factors for one butyl group C(32)C(35)) of 1 increase gradually toward the terminal carbon. The temperature factors for C(30)C(33) of 2 indicate large vibrations and these are reflected in short bond lengths. Two butyl groups of 3 are disordered and these CC bond lengths are short and long alternately. Atomic net charges around spirocarbon C(6) and toward N(1) to C(6) indicate the weak alternative system in the colorless form. As the xanthene ring has a planar geometry, the π electron density migration will easily occur from the auxochromes attached to the phthalide ring to the xanthene ring.

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