JOURNAL ARTICLE

New Lithium\nCopper Borates with BO<sub>3</sub> Triangles:\nLi<sub>6</sub>CuB<sub>4</sub>O<sub>10</sub>, Li<sub>3</sub>CuB<sub>3</sub>O<sub>7</sub>, Li<sub>8</sub>Cu<sub>7</sub>B<sub>14</sub>O<sub>32</sub>, and Li<sub>2</sub>Cu<sub>9</sub>B<sub>12</sub>O<sub>28</sub>

Abstract

Crystal structures of three new lithium\ncopper borates, Li<sub>3</sub>CuB<sub>3</sub>O<sub>7</sub>, Li<sub>8</sub>Cu<sub>7</sub>B<sub>14</sub>O<sub>32</sub>, and Li<sub>2</sub>Cu<sub>9</sub>B<sub>12</sub>O<sub>28</sub>, and a new Li<sub>6</sub>CuB<sub>4</sub>O<sub>10</sub> polymorph were solved by single-crystal\nX-ray diffraction.\nIn all of the structures, the boron cations form BO<sub>3</sub> triangles,\nwhich are connected with each other and with copper polyhedra only\nvia corners in Li<sub>6</sub>CuB<sub>4</sub>O<sub>10</sub> and Li<sub>3</sub>CuB<sub>3</sub>O<sub>7</sub> and via both corners and edges\nin Li<sub>8</sub>Cu<sub>7</sub>B<sub>14</sub>O<sub>32</sub> and Li<sub>2</sub>Cu<sub>9</sub>B<sub>12</sub>O<sub>28</sub>. The Li<sub>3</sub>CuB<sub>3</sub>O<sub>7</sub> and Li<sub>8</sub>Cu<sub>7</sub>B<sub>14</sub>O<sub>32</sub> compounds were synthesized as pure samples\nwith only trace amounts of impurities; hence, their magnetic properties\ncould be investigated and analyzed in terms of underlying magnetic\ncouplings. Other compositions always represented multiphase mixtures.\nLi<sub>3</sub>CuB<sub>3</sub>O<sub>7</sub> features infinite Cu,O\nchains formed by Cu<sub>2</sub>O<sub>6</sub> units consisting of edge-shared\nCuO<sub>4</sub> squares. Together with two apical oxygen atoms with\nlong interatomic Cu–O distances of 2.7–2.8 Å, the\nCu<sub>2</sub>O<sub>6</sub> units form chains extended along the <i>a</i> axis. These pseudochains are responsible for strong anisotropic\nthermal expansion behavior. The temperature dependence of the magnetization\nbetween 4 and 380 K for Li<sub>3</sub>CuB<sub>3</sub>O<sub>7</sub> could be fit well by a spin-dimer model. The magnetic susceptibility\nof Li<sub>8</sub>Cu<sub>7</sub>B<sub>14</sub>O<sub>32</sub> showed\na more complex temperature dependence, with two different Curie–Weiss\nregimes in the temperature range of 2–380 K.

Keywords:
Boron Polyhedron Copper Crystal structure Atmospheric temperature range Crystal (programming language) Single crystal

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Topics

Crystal Structures and Properties
Physical Sciences →  Materials Science →  Electronic, Optical and Magnetic Materials
Zeolite Catalysis and Synthesis
Physical Sciences →  Chemistry →  Inorganic Chemistry
Boron and Carbon Nanomaterials Research
Physical Sciences →  Materials Science →  Materials Chemistry

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