Cuthbert Heather L, Greedan John E, Vargas-Baca Ignacio, Derakhshan Shahab, Swainson Ian P
Department of Chemistry, McMaster University, Hamilton, Ontario, Canada, L8S 4M1.
Inorg Chem. 2007 Oct 15;46(21):8739-45. doi: 10.1021/ic701011r. Epub 2007 Sep 14.
The compound La(3)Re(2)O(10) has been synthesized by solid-state reaction and characterized by powder neutron diffraction, SQUID magnetometry, and heat capacity measurements. Its structure consists of isolated Re(2)O(10) dimer units of two edge-shared ReO(6) octahedra, separated by La(3+) within the lattice. The Re-Re distance within the dimer units is 2.488 A, which is indicative of metal-metal bonding with a bond order of 1.5. The average oxidation state of the Re atom is +5.5, leaving one unpaired electron per dimer unit (S = 1/2). Although the closest interdimer distance is 5.561 A, the magnetic susceptibility data and heat capacity measurements indicate this compound exhibits both short- and long-range magnetic order at surprisingly high temperatures. The zero field cooled (ZFC) magnetic susceptibility data show two broad features at 55 and 105 K, indicating short-range order, and a sharper cusp at 18 K, which signifies long-range antiferromagnetic order. The heat capacity of La(3)Re(2)O(10) shows a lambda-type anomaly at 18 K, which is characteristic of long-range magnetic order. DFT calculations determined that the unpaired electron resides in a pi-bonding orbital and that the unpaired electron density is widely delocalized over the atoms within the dimer, with high values at the bridging oxygens. Extended Hückel spin dimer calculations suggest possible interaction pathways between these dimer units within the crystal lattice. Results from the calculations and fits to the susceptibility data indicate that the short-range magnetic ordering may consist of 1-D antiferromagnetic linear chains of coupled S = 1/2 dimers. The magnetic structure of the antiferromagnetic ground state could not be determined by unpolarized neutron powder diffraction.
化合物La(3)Re(2)O(10)通过固态反应合成,并通过粉末中子衍射、超导量子干涉仪磁力测量和热容量测量进行了表征。其结构由两个边缘共享的ReO(6)八面体的孤立Re(2)O(10)二聚体单元组成,在晶格中被La(3+)隔开。二聚体单元内的Re-Re距离为2.488 Å,这表明金属-金属键的键级为1.5。Re原子的平均氧化态为+5.5,每个二聚体单元留下一个未配对电子(S = 1/2)。尽管最近的二聚体间距离为5.561 Å,但磁化率数据和热容量测量表明该化合物在令人惊讶的高温下同时表现出短程和长程磁有序。零场冷却(ZFC)磁化率数据在55和105 K处显示出两个宽峰,表明短程有序,在18 K处有一个更尖锐的尖峰,这表示长程反铁磁有序。La(3)Re(2)O(10)的热容量在18 K处显示出λ型异常,这是长程磁有序的特征。密度泛函理论(DFT)计算确定未配对电子位于一个π键轨道中,并且未配对电子密度在二聚体内的原子上广泛离域,在桥连氧原子处具有高值。扩展休克尔自旋二聚体计算表明晶格中二聚体单元之间可能存在相互作用途径。计算结果和对磁化率数据的拟合表明,短程磁有序可能由耦合的S = 1/2二聚体的1-D反铁磁线性链组成。反铁磁基态的磁结构无法通过非极化中子粉末衍射确定。