Variable-temperature X-ray structural investigation of {Fe[HC(3,5-Me(2)pz)(3)](2)}(BF4)(2) (pz = pyrazolyl ring): Observation of a thermally induced spin state change from all high spin to an equal high spin-low spin mixture, concomitant with the onset of nonmerohedral twinning
Dl. Reger et al., Variable-temperature X-ray structural investigation of {Fe[HC(3,5-Me(2)pz)(3)](2)}(BF4)(2) (pz = pyrazolyl ring): Observation of a thermally induced spin state change from all high spin to an equal high spin-low spin mixture, concomitant with the onset of nonmerohedral twinning, INORG CHEM, 40(12), 2001, pp. 2870-2874
The complex {Fe[HC(3,5-Me(2)pz)(3)](2)}(BF4)(2) (pz = pyrazolyl ring) under
goes a phase transition that occurs concomitantly with a thermally induced
spin conversion between the high-spin (HS. S = 2) and low-spin (LS, S = 0)
states. Above 204 K the compound is completely HS with the structure in the
C2/c space group with Z = 4. A crystal structure determination of this pha
se was performed at 220 K yielding the cell constants a = 20.338(2) Angstro
m, b = 10.332(1) Angstrom, c = 19.644(2) Angstrom, beta = 111.097(2)degrees
, and V = 3851.5(6) Angstrom (3). There is one unique iron(II) site at this
temperature. Below 206 K the compound converts to a 50:50 mixture of HS an
d LS, The radical change in the coordination sphere for half of the iron(II
) sites, most notably a shortening of the Fe-N bond distances by ca. 0.2 An
gstrom, that accompanies this magnetic transition causes a phase transition
. The crystal system changes from C-centered monoclinic to primitive tricli
nic with Z = 2 with two half-molecules on independent inversion centers. A
crystal structure determination was performed at 173 K in space group P (1)
over bar with a 10.287(2) Angstrom, b = 11.355(3) Angstrom, c 18.949(4) An
gstrom, alpha = 90.852(4)degrees, beta = 105.245(4)degrees, gamma = 116.304
(4)degrees, and V = 1892.3(8) Angstrom (3). All specimens investigated belo
w the phase transition temperature were determined to be nonmerohedral twin
s. Temperature cycling between these two forms does not appear to degrade c
rystal quality. previous magnetic susceptibility measurements indicate a se
cond, irreversible increase in the magnetic moment the first time the cryst
als are cooled below 85 K. A crystal structure determination at 220 K of a
specimen precooled to 78 K was not significantly different from those not c
ooled below 220 K.