Deqing
Zhang
*a,
Liang
Ding
a,
Wei
Xu
a,
Huaiming
Hu
a,
Daoben
Zhu
*a,
Yuanhe
Huang
b and
Decai
Fang
b
aOrganic Solids Laboratory, Center for Molecular Sciences, Institute of Chemistry, Chinese Academy of Sciences, Beijing, 100080, China. E-mail: dqzhang@infoc3.icas.ac.cn
bDepartment of Chemistry, Beijing Normal University, Beijing, 100875, China
First published on 4th December 2001
A 1D silver(I) complex of nitronyl nitroxide was prepared and its structure was determined by X-ray diffraction analysis; magnetic studies indicate that the spin–spin interaction of nitronyl nitroxides through silver(I) ions along the chain are fairly strong (J/kb = −84 K).
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Scheme 1 Chemical structure of m-N-methylpyridinium nitronyl nitroxide iodide. |
Complex 1 was prepared starting from m-N-methylpyridinium nitronyl nitroxide iodide6 and silver nitrate. After removal of the yellow precipitate, the solution was slowly evaporated to yield black crystals of complex 1.† Its structure was established by X-ray diffraction analysis.‡
Fig. 1 shows the asymmetric unit of complex 1 together with selected bond lengths and angles. There are two nitrate ions, one silver(I) ion and one m-N-methylpyridinium nitronyl nitroxide group (MPYNN), and thus the asymmetric unit is neutral as a whole. For the MPYNN unit, the bond lengths of N(1)–O(1) and C(7)–N(1) are almost identical to those of N(2)–O(2) and C(7)–N(2), respectively (see the caption of Fig. 1); the pyridinium and imidazoline rings are not coplanar, and they form a dihedral angle of 43.3°. Five oxygen atoms O(11), O(21), O(22), O(1) and O(2)i (not shown in Fig. 1) are coordinated to silver(I). The bond lengths of Ag(1)–O(1) and Ag(1)–O(2)i, which are formed between the silver(I) ion and nitronyl nitroxide units, are comparable to those of bonds linking silver(I) and nitrate ions [Ag(1)–O(11), Ag(1)–O(21) and Ag(1)–O(22)].
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Fig. 1 The asymmetric unit of complex 1 together with selected bond lengths (Å) and angles (°): N(1)–O(1) 1.281(3), N(1)–C(7) 1.342(3), N(2)–O(2) 1.284(3), N(2)–C(7) 1.339(3), Ag(1)–O(1) 2.4452(19), Ag(1)–O(2)i 2.3706(19), Ag(1)–O(11) 2.459(2), Ag(1)–O(21) 2.480(2), Ag(1)–O(22) 2.540(2); N(2)–C(7)–N(1) 109.6(2), N(1)–O(1)–Ag(1) 120.74(14), N(2)–O(2)–Ag(1)i 123.51(15), O(1)–Ag(1)–O(11) 89.58(7), O(1)–Ag(1)–O(21) 125.91(7), O(11)–Ag(1)–O(21) 81.82(8), O(11)–Ag(1)–O(22) 108.19(7), O(21)–Ag(1)–O(22) 51.23(7) [symmetrical operation:ix, y − 1, z]. |
Atoms O2 and Ag1 shown in Fig. 1 are further linked to another silver(I) ion and MPYNN unit, respectively, and the structure is extended in this manner to generate a one dimensional chain as clearly indicated in Fig. 2. Interestingly, despite the steric hindrance the m-N-methylpyridinium ring and the nitrate ions are arranged on one side of the chain, which is very likely due to electrostatic attraction interactions among the m-N-methylpyridinium and the nitrate ions. The inter-chain arrangement of complex 1 is also shown in Fig. 2. Besides the short contacts among the hydrogen atoms of m-N-methylpyridinium ring and oxygen atoms of nitrate ions, no short interatomic distances are found among the neighboring chains. According to previous studies,7 for nitronyl nitroxide derivatives most of the spin density is distributed onto the atoms of the imidazoline ring, and the spin densities carried by other atoms, in particular hydrogen atom attached to m-N-methylpyridinium ring, are negligible. Thus, each of the one-dimensional chains in the crystal lattice of complex 1 can be treated independently from the magnetic point of view. Preliminary theoretical investigations were performed for a “dimer” of the asymmetrical unit.8 The calculation results show that the electron densities ρb for the bonds of silver(I) ions and oxygen atoms of nitronyl nitroxide units are only about 0.004, indicating that these bonds are not typical covalent ones but electrovalent bonds. The electron density distribution around the silver(I) ions are spherical, from which it can be inferred that only the s orbitals of silver(I) ions are involved in the formation of the bonds of silver(I) ions with oxygen atoms of MPYNN units and nitrate ions.
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Fig. 2 The 1D structure and inter-chain arrangement of complex 1. |
Fig. 3 shows a plot of the χTvs. T for complex 1, where χ is the molar magnetic susceptibility in terms of the asymmetric unit formula C13H19AgN5O8. The room temperature value of χT is 0.330 emu K mol−1, smaller than 0.375 emu K mol−1, the theoretically expected value for a one spin (S = 1/2) system. By lowering temperature, χT is reduced gradually from 300 to 100 K, and then it decreases more sharply reaching 0.014 emu K mol−1 at 5 K. Such temperature dependent behavior of χT indicates the presence of antiferromagnetic spin–spin interaction in complex 1.
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Fig. 3 Plot of χT product vs. T for complex 1; the solid line represents the best theoretical fit (see text). |
As discussed above, the spin–spin interaction among the one-dimensional chains (inter-chain interaction) in the crystal lattice of complex 1 should be rather weak. Therefore, the experimental magnetic data was fitted to a one dimensional antiferromagnetic model with eqn. (1):9
χ = (Ng2β2/kbT)(0.25 + 0.074975x + 0.075235x2)/(1.0 + 0.9931x + 0.172135x2 + 0.757825x3), x = |J|/kbT | (1) |
In summary, a novel silver(I) complex of nitronyl nitroxide with an extended 1D structure has been prepared and characterized. The spin–spin interaction of nitronyl nitroxides through the silver(I) ions along the chain is fairly strong with an exchange constant J/kb = −84 K.
The present research work was supported by Chinese Academy of Sciences, NSFC (29972044, 90101025) and the Major State Basic Research Development Program (G2000077500). The authors also thank Prof. Xianglin Jin of Peking University for his kind help on crystal structural analysis.
Footnotes |
† Yield, 40.9%; mp, 175–176 °C (decomp.); IR (KBr), 1384 (s), 1290 (w), 1215 (w), 1170 (w), 1137 (w) cm−1; Anal. Calc. for C13H19AgN5O8: C, 32.50; H, 3.99; N, 14.59. Found: C, 32.25; H, 3.95; N, 14.60%. |
‡ Crystal data: C13H19AgN5O8, M = 481.20, monoclinic, C2/c, a = 28.278(6), b = 7.0410(14), c = 18.894(4) Å, β =112.55(3)°, V = 3474.3(12) Å3, Z = 8, Dc = 1.840 g cm−3; F(000) = 1944, μ(Mo-Kα) = 1.216 mm−1. 16047 reflections of which 3956 are unique (Rint = 0.0204) were collected to a θ limit of 27.48° on a Rigaku RAXIS RAPID IP instrument at 293(2) K. The structure was solved by direct methods and refined by a least-squares matrix method. The final cycle of full-matrix least-square refinement was based on 3400 observed reflections [I > 2σ(I)] and 244 variable parameters and converged to R1 = 0.0292, wR2 = 0.0775. CCDC reference number 172993. See http://www.rsc.org/suppdata/cc/b1/b109354a/ for crystallographic data in CIF or other electronic format. |
This journal is © The Royal Society of Chemistry 2002 |