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Synthesis, Crystal Structure, and Characterization of Two Novel One‐ and Two‐Dimensionally Polymeric Copper(II) Phosphonoacetates
Author(s) -
Köferstein Roberto,
Arnold Michael,
Robl Christian
Publication year - 2017
Publication title -
zeitschrift für anorganische und allgemeine chemie
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.354
H-Index - 66
eISSN - 1521-3749
pISSN - 0044-2313
DOI - 10.1002/zaac.201600457
Subject(s) - crystallography , superexchange , octahedron , chemistry , antiferromagnetism , paramagnetism , crystal structure , hydrogen bond , molecule , copper , counterion , square pyramidal molecular geometry , aqueous solution , ion , physics , organic chemistry , quantum mechanics , condensed matter physics
Blue single crystals of Cu[μ 2 ‐OOC(CH 2 )PO 3 H] · 2H 2 O ( 1 ) and Cu 1.5 [μ 3 ‐OOC(CH 2 )PO 3 ] · 5H 2 O ( 2 ) were prepared in aqueous solution. In compound 1 [space group C 2/ c (no. 15) with a = 1623.3(2), b = 624.0(1), c = 1495.5(2) pm, β = 122.45(1)°], Cu is coordinated by three oxygen atoms stemming from the hydrogenphosphonoacetate dianion and three water molecules to form a distorted octahedron. The Cu–O bonds range from 190.4(3) to 278.5(3) pm. The connection between the Cu 2+ cations and the hydrogenphosphonoacetate dianions leads to a two‐dimensional structure with layers parallel to ( 1 01). The layers are linked by hydrogen bonds. In compound 2 [space group P 1 (no. 2) with a = 608.2(1), b = 800.1(1), c = 1083.6(1) pm, α = 94.98(1)°, β = 105.71(1)°, γ = 109.84(1)°], two crystallographically independent Cu 2+ cations are coordinated in a square pyramidal and an octahedral fashion, respectively. The Cu–O bonds range from 192.9(2) to 237.2(2) pm. The coordination of the phosphonoacetate trianion to Cu(1) results in infinite polyanionic chains parallel to [100] with a composition of {Cu(H 2 O)[OOC(CH 2 )PO 3 ]} n n – . Hydrated Cu(2) cations are accommodated between the chains as counterions. 1 and 2 show structural features of cation exchangers. Magnetic measurements reveal a paramagnetic Curie‐Weiss behavior. Compound 2 shows antiferromagnetic coupling between Cu 2+ ions due to a super‐superexchange coupling. The UV/Vis spectra of 1 suggest three d–d transition bands at 763 nm ( 2 B 1 → 2 E), 878 nm ( 2 B 1 → 2 B 2 ), and 1061 nm ( 2 B 1 → 2 A 1 ). Thermoanalytical investigations in air show that compound 1 is stable up to 165 °C, whereas decomposition of 2 begins at 63 °C.