The
complex salts [Fe(
L
1
)
2
]X
2
(
1X
2
;
L
1
= 4-(isopropyldisulfanyl)-2,6-bis(pyrazolyl)pyridine;
X
–
= BF
4
–
, ClO
4
–
) form solvated crystals from common organic
solvents. Crystals of
1X
2
·Me
2
CO show abrupt spin transitions near 160 K, with up to 22
K thermal hysteresis.
1X
2
·Me
2
CO cocrystallizes with other, less cooperative acetone solvates,
which all transform into the same solvent-free materials
1X
2
·sf upon exposure to air, or mild heating.
Conversion of
1X
2
·Me
2
CO to
1X
2
·sf proceeds
in a single-crystal to single-crystal fashion.
1X
2
·sf are not isomorphous with the acetone
solvates, and exhibit abrupt spin transitions at low temperature with
hysteresis loops of 30–38 K (X
–
= BF
4
–
) and 10–20 K (X
–
= ClO
4
–
), depending on the measurement
method. Interestingly, the desolvation has an opposite effect on the
SCO temperature and hysteresis in the two salts. The hysteretic spin
transitions in
1X
2
·Me
2
CO and
1X
2
·sf do
not involve a crystallographic phase change but are accompanied by
a significant rearrangement of the metal coordination sphere. Other
solvates
1X
2
·MeNO
2
,
1X
2
·MeCN, and
1X
2
·H
2
O are mostly isomorphous
with each other and show more gradual spin-crossover equilibria near
room temperature. All three of these lattice types have similar unit
cell dimensions and contain cations associated into chains through
pairwise, intermolecular S···π interactions.
Polycrystalline [Fe(
L
2
)
2
][BF
4
]
2
·MeNO
2
(
2[BF
4
]
2
·MeNO
2
;
L
2
= 4-(methyldisulfanyl)-2,6-bis(pyrazolyl)pyridine)
shows an abrupt spin transition just above room temperature, with
an unsymmetrical and structured hysteresis loop, whose main features
are reversible upon repeated thermal scanning.