In
search of functional molecular materials and the study of their
formation mechanism, we report the elucidation of a hierarchical step-by-step
formation from monomer (Mn) to heptamer (Mn<sub>7</sub>) to nonadecamer
(Mn<sub>19</sub>) satisfying the relation 1 + Σ<sub><i>n</i></sub>6<i>n</i>, where <i>n</i> is
the ring number of the Brucite structure using high-resolution electrospray
ionization mass spectrometry (HRESI-MS). Three intermediate clusters,
Mn<sub>10</sub>, Mn<sub>12</sub>, and Mn<sub>14</sub>, were identified.
Furthermore, the Mn<sub>19</sub> disc remains intact when dissolved
in acetonitrile with a well-resolved general formula of [Mn<sub>19</sub>(<i>L</i>)<sub><i>x</i></sub>(OH)<sub><i>y</i></sub>(N<sub>3</sub>)<sub>36–<i>x</i>−<i>y</i></sub>]<sup>2+</sup> (<i>x</i> = 18, 17, 16; <i>y</i> = 8, 7, 6; H<i>L</i> = 1-(hydroxymethyl)-3,5-dimethylpyrazole) indicating progressive
exchange of N<sub>3</sub><sup>–</sup> for OH<sup>–</sup>. The high symmetry (<i>R</i>-3) Mn<sub>19</sub> crystal
structure consists of a well-ordered discotic motif where the peripheral
organic ligands form a double calix housing the anions and solvent
molecules. From the formula and valence bond sums, the charge state
is mixed-valent, [Mn<sup>II</sup><sub>15</sub>Mn<sup>III</sup><sub>4</sub>]. Its magnetic properties and electrochemistry have been
studied. It behaves as a ferrimagnet below 40 K and has a coercive
field of 2.7 kOe at 1.8 K, which can be possible by either weak exchange
between clusters through the anions and solvents or through dipolar
interaction through space as confirmed by the lack of ordering in
frozen CH<sub>3</sub>CN. The moment of nearly 50 Nμ<sub>B</sub> suggests Mn<sup>II</sup>–Mn<sup>II</sup> and Mn<sup>III</sup>–Mn<sup>III</sup> are ferromagnetically coupled while Mn<sup>II</sup>–Mn<sup>III</sup> is antiferromagnetic which is likely
if the Mn<sup>III</sup> are centrally placed in the cluster. This
compound displays the rare occurrence of magnetic ordering from nonconnected
high-spin molecules