Inorganic Chemistry Communications 9 (2006) 316–318 www.elsevier.com/locate/inoche The alexandrite-like Cr-doped aluminum oxalato complexes Laongjit Chaiyapoom a, Sumpun Wongnawa a,*, Chaveng Pakawatchai a, Jonathan Charmant b, Saowanit Saithong a a Department of Chemistry, Faculty of Science, Prince of Songkla University, 15 Kanjanavanich Road, Ko Hong, Hat Yai, Songkla 90112, Thailand b School of Chemistry, The University of Bristol, Bristol BS8 1TS, UK Received 1 November 2005; accepted 5 December 2005 Available online 18 January 2006 Abstract The Cr-doped aluminum oxalato complexes were obtained by substituting Al with trace of Cr. Three types of products were obtained in two colors: blue (one) and red (two). One of the red crystallizes in the hexagonal crystal system with space group R 3. The two red complexes possess the color-change property under different light sources (fluorescence and incandescence lights) similar to alexandrite – the rare and expensive gemstone. Ó 2005 Elsevier B.V. All rights reserved. Keywords: Aluminum complexes; Oxalate ligand; Oxalato complexes; Bimetallic oxalato complexes; Alexandrite Oxalato complexes are interesting materials, having technological applications as precursors to nanocrystalline metallic oxides, and to molecular-based magnetic materials [1]. The oxalate ion can act as bridging ligand between metals and thus constructing one-, two- or three-dimensional honeycomb anionic networks ½M2 ðC2 O4 Þ3 2n that behave n as ferro, ferri or antiferro-magnets [2]. The crystal structures of trioxalato metallate salts of general formula MI3 MIII ðC2 O4 Þ3 3H2 O, with MI = K, Rb, NH4 and MIII = Al, Cr, Ga, Fe, Mn [3] have been reported as monoclinic cells, space group P21/c, or as triclinic cells, space group P1. Mixed oxalato Al–Cr complexes, [Rh(bpy)3][NaAlx Cr1x(ox)3]ClO4 (x = 0.05–1), were prepared but the emphasis was placed on the study of energy transfer within the [Cr(ox)3]3 chromophores rather than on the structural framework [4]. K3[Cr(C2O4)3] Æ 3H2O (0.244 g, 0.5 mmol) was dissolved in 20 mL distilled water and K3[Al(C2O4)3] Æ 3H2O (4.390 g, 9.5 mmol) was added and stirred to dissolve. The two starting materials were prepared according to the method described by Booth [5]. Solution of NaCl * Corresponding author. Tel.: +66 74 288443; fax: +66 74 212918. E-mail address: sumpun.w@psu.ac.th (S. Wongnawa). 1387-7003/$ - see front matter Ó 2005 Elsevier B.V. All rights reserved. doi:10.1016/j.inoche.2005.12.004 (1.170 g in minimum volume of water) was added to the mixture solution followed by further stirring for about 10 min and was allowed to stand at room temperature for crystallization. After about one week the blue crystals were filtered out and the filtrate was allowed to crystallize further from which the red crystals were obtained and filtered out. The two types of crystals were washed with mixed water–ethanol (1:1), dried and weighed (2.47 g for the blue, 0.98 g for the red). All the products were recrystallized in water prior to further studies. The red crystals under close examination and unit cell parameters checked by X-ray diffractometer consisted of two types of crystals: hexagonal and cubic. The crystal structure to be reported here is the hexagonal one. The other two crystals, blue and red cubic, present some difficulties in terms of stability under X-ray irradiation (blue) and structural elucidation technique (red cubic). However, work on both complexes have been underway and, hopefully, we will be able to report it in due course along with their other spectroscopic properties. The unit cell parameters and intensity data of the red hexagonal crystal system were collected at 293 K on a Bruker SMART APEX CCD area-detector diffractometer with graphite monochromated Mo Ka radiation (k = 0.71073 Å) L. Chaiyapoom et al. / Inorganic Chemistry Communications 9 (2006) 316–318 (at a detector distance of 6.0 cm) using SMART program (Bruker, 2000). A fullsphere of the reciprocal space was covered by a combination of three sets of exposures; each set had a different / angle (0°, 120°, 240°) and each exposure of 10 s covered 0.3° in x. Raw data frame integration was performed with SAINT (Bruker, 2000), with applied correction for Lorentz and polarization effects. An empirical absorption correction by using the SADABS program (Bruker, 2000) was applied, which resulted in transmission coefficients ranging from 0.905 to 1.000. A total of 16191 reflections (2595 independent reflections, Rint = 0.0245) were collected in the range 2.22° < h < 24.70°. This structure was solved by Direct methods using SHLLXTL-PC V6.12 software package (Bruker, 2000) and refined by full matrix least-squares method based on jFj with anisotropic thermal parameters for all non-hydrogen atoms by using XTAL3.7 program system [6]. The hydrogen atoms were found by Fourier maps and refined isotropically. View of the molecular unit of this complex is shown in Fig. 1. 17 The structure consists of discrete K½AlðoxÞ3 6 anions, + K cations, a Cl anion, and water molecules. The asymmetric unit of the complex contains four potassium atoms, one chloride atom, one aluminum atom, three oxalate ligands, and three water molecules. Chlorine atom and one potassium atom (K1) lie on 3 axis, then the remaining parts of the structure generated by this axis forming the formula unit or the structure of K18{K[Al(C2O4)3]6} Cl Æ 18H2O. However, there is a small amount of Cr in the crystal structure which is in the same position as Al. The site occupancies of Al and Cr are 0.97 and 0.03, respectively, therefore, the molecular formula of the red hexagonal crystal may be written as K18{K[Al0.97Cr0.03(C2O4)3]6}Cl Æ 18H2O [7]. Fig. 1. The 50% thermal ellipsoid of core structure of K18{K[Al0.97Cr0.03 (C2O4)3]6}Cl Æ 18H2O complex molecule plot (all counterions, H2O, and H atoms are omitted for clarity). 317 The potassium ion in the unit core structure, 17 K½AlðC2 O4 Þ3 6 , lies on 3 axis and is surrounded, in octahedral geometry, by six terminal oxygen atoms from six oxalate ligands of six [Al(C2O4)3]3 anions as shown in Fig. 1 with the K–O equidistances of 2.400(3) Å. One of the oxalate ligands of [Al(C2O4)3] 3 unit acts as tridentate ligand bonded to K and Al atoms whereas the remaining two C2 O2 4 ligands bond to Al atom as bidentate ligands. [Al(C2O4)3]3 unit has a distorted octahedral geometry with the oxalate ligand bite O–Al–O angles of 84.4(1)°, 84.4(1)°, and 84.0(1)° for O1–Al–O2, O3–Al–O4, and O5–Al–O6, respectively. The three new complexes (two reds and one blue) readily dissolve in water yielding similar greenish violet solutions whose UV–Vis absorption spectra are almost identical to that of K3[Cr(ox)3] Æ 3H2O (Fig. 2) indicating the chromophore being responsible for the color in the three solutions are the same as that in K3[Cr(ox)3] Æ 3H2O, that is, the [Cr(ox)3]3 moiety. Based on the energy diagram of Cr3+ (d3), there are three spin-allowed transitions, namely, m1(4A2g ! 4T2g), m2(4A2g ! 4T1g(F)), and m3(4A2g ! 4T1g(P)). For the [Cr(ox)3]3 these three transitions have been reported as: 571, 417, 263 nm for m1, m2, m3, respectively [8]. Our solution samples also yielded the same results (Table 1). The kmax of m3 transition is not decisive as it overlaps with the p–p* transition of the oxalate ligand which occurs at ca. 300 nm [9]. The solid state diffused reflectance spectra (Fig. 3) show the same pattern as in the solution forms but on a closer look one can detect a slight shift of the m1(4A2g ! 4T2g transition) peak (Table 1) and a small difference in shape especially the position of kmin of the trough at ca. 480–490 nm (Fig. 3). The reason they appear in different colors in solid state is due to slight change in the kmax of m1 peak and kmin of the trough originating from slight different environment around the chromophore [Cr(ox)3]3 in solid state. In Fig. 3, the spin-forbidden transition 4A2g ! 2Eg, 2 T1g, 2T2g is also discernible at 697 nm [10]. In addition, the two red crystals also show the colorchange property under different light sources: fluorescence Fig. 2. UV–Vis absorption spectra of red cubic, red hexagonal, blue complexes, and K3[Cr(C2O4)3] Æ H2O in aqueous solution. (For interpretation of the references in color in this figure legend, the reader is referred to the web version of this article.) 318 L. Chaiyapoom et al. / Inorganic Chemistry Communications 9 (2006) 316–318 Table 1 Absorption bands of red cubic, red hexagonal, blue, and K3[Cr(C2O4)3] Æ 3H2O change property is well known in the rare and expensive gemstone alexandrite [12]. Complex Acknowledgments Phase Absorption band (nm) m3 + p–p* m2 m1 Red cubic Solution Solid 299 263 419 421 572 571 Red hexagonal Solution Solid 299 257 424 419 579 567 Blue Solution Solid 299 269 419 421 572 579 L.C. would like to express her sincere thanks to the consortium of Postgraduate Education and Research Program in Chemistry (PERCH) for financial support (scholarship and research fund) and also to the Graduate School of Prince of Songkla University for the Thesis Research Fund. K3[Cr(C2O4)3] Æ 3H2O Solution Solid 299 258 420 420 572 580 References Fig. 3. UV–Vis absorption spectra of red cubic, red hexagonal, blue complexes, and K3[Cr(C2O4)3] Æ H2O in solid state by diffused reflectance method. (For interpretation of the references in color in this figure legend, the reader is referred to the web version of this article.) Fig. 4. The color-change red cubic crystals: dark blue under fluorescent light, and reddish violet under incandescent light. (For interpretation of the references in color in this figure legend, the reader is referred to the web version of this article.) and incandescence lights. Fig. 4 shows the red cubic crystals appeared as dark blue under fluorescence light but reddish violet under incandescence light [11]. This color- [1] H. Tamaki, Z.J. Zhong, N. Matsumoto, S. Kida, M. Koikawa, N. Achiwa, Y. Hashimoto, H. Ökawa, J. Am. Chem. Soc. 114 (1992) 6974. [2] F. Bérézovsky, A.A. Hajem, S. Triki, J.S. Pala, P. Molinié, Inorg. Chim. 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In addition, SEM/EDX was also used to check the purity of this complex where only characteristic X-ray lines of C, O, Al, Cl, K, and Cr were detected. [8] F.A. Cotton, G. Wilkinson, Advanced Inorganic Chemistry, third edn., Interscience Publishers, John Wiley & Sons, New York, 1972, p. 839; J.E. Huheey, E.A. Keiter, R.L. Keiter, Inorganic Chemistry: Principles of Structure and Reactivity, fourth edn., Harper Collins College Publishers, New York, 1993, p. 447. The value of m3 usually was not available experimentally, the value shown here was obtained by calculation. [9] D.P. Graddon, J. Inorg. Nucl. Chem. 3 (1956) 308. [10] T.D. Yager, G.R. Eaton, J. Chem. Educ. 56 (1979) 635. [11] The photographs of only the red cubic crystals are shown here because the crystals of the red hexagonal ones were too small for the photograph to be taken. [12] B.M. Loeffler, R.G. 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