Architectural Isomerism in the Three-Dimensional Polymeric Spin Crossover System {Fe(pmd)2[Ag(CN)2]2}: Synthesis, Structure, Magnetic Properties, and Calorimetric Stud
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- 作者：Ana Galet ; M. Carmen Muñ ; oz ; Ana B. Gaspar ; and José ; A. Real
- 刊名：Inorganic Chemistry
- 出版年：2005
- 出版时间：November 28, 2005
- 年：2005
- 卷：44
- 期：24
- 页码：8749 - 8755
- 全文大小：407K
- 年卷期：v.44,no.24(November 28, 2005)
- ISSN：1520-510X
文摘
Two coordination polymers formulated {Fe(pmd)2[Ag(CN)2]2} (pmd = pyrimidine) have been synthesized andcharacterized. Both polymers, considered to be architectural isomers, display different crystal structures and magneticproperties. Isomer 1 crystallizes in the monoclinic C2/c space group with a = 6.9750(8) Å, b = 16.1700(9) Å, c= 14.2020(8) Å, 
= 97.954(2)
, V = 1586.37(14) Å3, and Z = 4. The crystal structure of isomer 2 has beenstudied at 250 and 150 K. At both temperatures, 2 displays the orthorhombic Pccn space group with a = 15.7700(2) [14.8950(2)] Å, b = 8.2980(4) [8.1580(4)] Å, c = 13.4180(6) [13.3480(5)] Å, V = 1755.87(14) [1621.96(10)] Å3,and Z = 4 for 250 [150] K. The iron(II) ions define distorted octahedral [FeN6] chromophores in both isomers. Theequatorial positions are occupied by four [Ag(CN)2]- bridging ligands, which connect the defining layers of twoiron(II) ions. Isomer 1 has two crystallographically distinct [Ag(CN)2]- groups; one is essentially linear, while theother is severely distorted [C(5)-Ag(2)-C(5i)] = 138.8(5). This fact facilitates the parallel interpenetration of twolayers, which in addition show short Ag(1)····Ag(2) interactions (distance Ag(1)····Ag(2) = 2.9972(10) Å). Isomer2 shows only one type of Ag atom, which is slightly bent [C-Ag-C = 161.54(12)], and as a consequence, thelayers defined are not interpenetrated. In both cases, the axial positions are occupied by the pmd ligands whichinteract with the Ag atoms of adjacent layers defining a 3D coordination polymer. Compound 1 is high spin in thewhole range of temperatures, while 2 undergoes a cooperative high-spin 
low-spin effect centered at ca. 184 Kwith a hysteresis loop ca. 5 K wide. The experimental enthalpy and entropy variations were 11.5 ± 0.4 kJ mol-1and 64 ± 3 J K-1 mol-1. Consistency between the experimental thermodynamic data and the magnetic data waschecked in the frame of regular solution theory.
= 97.954(2), V = 1586.37(14) Å3, and Z = 4. The crystal structure of isomer 2 has beenstudied at 250 and 150 K. At both temperatures, 2 displays the orthorhombic Pccn space group with a = 15.7700(2) [14.8950(2)] Å, b = 8.2980(4) [8.1580(4)] Å, c = 13.4180(6) [13.3480(5)] Å, V = 1755.87(14) [1621.96(10)] Å3,and Z = 4 for 250 [150] K. The iron(II) ions define distorted octahedral [FeN6] chromophores in both isomers. Theequatorial positions are occupied by four [Ag(CN)2]- bridging ligands, which connect the defining layers of twoiron(II) ions. Isomer 1 has two crystallographically distinct [Ag(CN)2]- groups; one is essentially linear, while theother is severely distorted [C(5)-Ag(2)-C(5i)] = 138.8(5). This fact facilitates the parallel interpenetration of twolayers, which in addition show short Ag(1)····Ag(2) interactions (distance Ag(1)····Ag(2) = 2.9972(10) Å). Isomer2 shows only one type of Ag atom, which is slightly bent [C-Ag-C = 161.54(12)], and as a consequence, thelayers defined are not interpenetrated. In both cases, the axial positions are occupied by the pmd ligands whichinteract with the Ag atoms of adjacent layers defining a 3D coordination polymer. Compound 1 is high spin in thewhole range of temperatures, while 2 undergoes a cooperative high-spin low-spin effect centered at ca. 184 Kwith a hysteresis loop ca. 5 K wide. The experimental enthalpy and entropy variations were 11.5 ± 0.4 kJ mol-1and 64 ± 3 J K-1 mol-1. Consistency between the experimental thermodynamic data and the magnetic data waschecked in the frame of regular solution theory.