6 research outputs found
Guest Programmable Multistep Spin Crossover in a Porous 2‑D Hofmann-Type Material
The
spin crossover (SCO) phenomenon defines an elegant class of
switchable materials that can show cooperative transitions when long-range
elastic interactions are present. Such materials can show multistepped
transitions, targeted both fundamentally and for expanded data storage
applications, when antagonistic interactions (i.e., competing ferro-
and antiferro-elastic interactions) drive concerted lattice distortions.
To this end, a new SCO framework scaffold, [Fe<sup>II</sup>(bztrz)<sub>2</sub>(Pd<sup>II</sup>(CN)<sub>4</sub>)]·<i>n</i>(guest) (bztrz = (<i>E</i>)-1-phenyl-<i>N</i>-(1,2,4-triazol-4-yl)methanimine, <b>1·</b><i><b>n</b></i><b>(guest)</b>), has been prepared that supports
a variety of antagonistic solid state interactions alongside a distinct
dual guest pore system. In this 2-D Hofmann-type material we find
that inbuilt competition between ferro- and antiferro-elastic interactions
provides a SCO behavior that is intrinsically frustrated. This frustration
is harnessed by guest exchange to yield a very broad array of spin
transition characters in the one framework lattice (one- (<b>1·(H</b><sub><b>2</b></sub><b>O,EtOH)</b>), two- (<b>1·3H</b><sub><b>2</b></sub><b>O</b>) and three-stepped (<b>1·∼2H</b><sub><b>2</b></sub><b>O</b>)
transitions and SCO-deactivation (<b>1</b>)). This variety of
behaviors illustrates that the degree of elastic frustration can be
manipulated by molecular guests, which suggests that the structural
features that contribute to multistep switching may be more subtle
than previously anticipated
Guest Programmable Multistep Spin Crossover in a Porous 2‑D Hofmann-Type Material
The
spin crossover (SCO) phenomenon defines an elegant class of
switchable materials that can show cooperative transitions when long-range
elastic interactions are present. Such materials can show multistepped
transitions, targeted both fundamentally and for expanded data storage
applications, when antagonistic interactions (i.e., competing ferro-
and antiferro-elastic interactions) drive concerted lattice distortions.
To this end, a new SCO framework scaffold, [Fe<sup>II</sup>(bztrz)<sub>2</sub>(Pd<sup>II</sup>(CN)<sub>4</sub>)]·<i>n</i>(guest) (bztrz = (<i>E</i>)-1-phenyl-<i>N</i>-(1,2,4-triazol-4-yl)methanimine, <b>1·</b><i><b>n</b></i><b>(guest)</b>), has been prepared that supports
a variety of antagonistic solid state interactions alongside a distinct
dual guest pore system. In this 2-D Hofmann-type material we find
that inbuilt competition between ferro- and antiferro-elastic interactions
provides a SCO behavior that is intrinsically frustrated. This frustration
is harnessed by guest exchange to yield a very broad array of spin
transition characters in the one framework lattice (one- (<b>1·(H</b><sub><b>2</b></sub><b>O,EtOH)</b>), two- (<b>1·3H</b><sub><b>2</b></sub><b>O</b>) and three-stepped (<b>1·∼2H</b><sub><b>2</b></sub><b>O</b>)
transitions and SCO-deactivation (<b>1</b>)). This variety of
behaviors illustrates that the degree of elastic frustration can be
manipulated by molecular guests, which suggests that the structural
features that contribute to multistep switching may be more subtle
than previously anticipated
Guest Adsorption in the Nanoporous Metal–Organic Framework Cu<sub>3</sub>(1,3,5-Benzenetricarboxylate)<sub>2</sub>: Combined <i>In Situ</i> X‑ray Diffraction and Vapor Sorption
The
structure of the nanoporous metal–organic framework
Cu<sub>3</sub>(BTC)<sub>2</sub> (BTC = 1,3,5-benzenetricarboxylate)
with a variety of molecular guests was studied <i>in situ</i> using single crystal X-ray diffraction. By collecting crystal structure
data for a series of guests within the same host crystal, insights
into the molecular interactions underpinning guest adsorption processes
have been gained. Adsorption behaviors are influenced strongly by
both enthalpic and entropic thermodynamic, as well as interpore steric
(size-exclusion) effects, and we note correlations between guest attributes
and these effects. Vapor adsorption measurements revealed a guest
uptake capacity inversely proportional to guest size. Correspondingly,
structural results show that guests reside in the smallest pores accessible
to them. Interpore steric effects for larger guests cause these to
be excluded from the smallest pores, and this corresponds to lower
total uptake. Both hydrophilic and lipophilic small guests adsorb
favorably into the 5 Å diameter smallest pore of the material,
with the number of guests in these pores dependent on guest size and
their location, in turn dependent upon both guest–guest interactions
and competition between hydrogen-bonding interactions at the apertures
of the smallest pore and lipophilic interactions at the center of
the smallest pore. Hydrophilic guests with lone electron pairs interact
preferentially with the coordinatively unsaturated Cu sites of the
desolvated framework, with the number of these depending on steric
interactions between neighboring bound guests and guest flexibility.
Guest coordination at the Cu sites has a significant effect on the
framework structure, increasing the Cu···Cu distance
in the dinuclear unit, with the Cu<sub>3</sub>(BTC)<sub>2</sub> unit
cell being smaller when guests that do not coordinate with the Cu
are present, and in the case of cyclohexane, smaller than for the
desolvated framework. Overall, our comprehensive structural study
reconciles Cu<sub>3</sub>(BTC)<sub>2</sub> adsorption properties with
the underlying guest–host and guest–guest interactions
that gives rise to these
Mixed-Component Sulfone–Sulfoxide Tagged Zinc IRMOFs: <i>In Situ</i> Ligand Oxidation, Carbon Dioxide, and Water Sorption Studies
Reported
here are the syntheses and adsorption properties of a
series of single- and mixed-component zinc IRMOFs derived from controlled
ratios of sulfide and sulfone functionalized linear biphenyldicarboxylate
(bpdc) ligands. During MOF synthesis the sulfide moieties undergo <i>in situ</i> oxidation, giving rise to sulfoxide functionalized
ligands, which are incorporated to give mixed-component sulfoxide–sulfone
functionalized MOFs. The single- and mixed-component systems all share
the IRMOF-9 structure type as determined by a combination of single
crystal and powder X-ray diffraction analyses. The functionalized
IRMOF-9 series was investigated by N<sub>2</sub>, CO<sub>2</sub>,
and water adsorption measurements. MOFs containing higher proportions
of sulfoxide have slightly larger accessible surface areas and pore
volumes, whereas MOFs containing a greater proportion of the sulfone
functionality demonstrated higher CO<sub>2</sub> adsorption capacities,
enthalpies of CO<sub>2</sub> adsorption, and CO<sub>2</sub>/N<sub>2</sub> selectivities. Water adsorption studies at 298 K showed the
MOFs to have pore-filling steps starting around 0.4 <i>P/P</i><sub>0</sub>. In general, only small changes in water adsorption
were observed with regards to ligand ratios in the mixed-component
MOFs, suggesting that the location of the step is primarily determined
by the pore size. A ligand-directed fine-tuning approach of changing
alkyl chain length was demonstrated to give smaller more hydrophobic
pores with better adsorption characteristics
Selective Gas Adsorption in a Pair of Robust Isostructural MOFs Differing in Framework Charge and Anion Loading
Activation
of the secondary assembly instructions in the mononuclear pyrazine
imide complexes [Co<sup>III</sup>(dpzca)<sub>2</sub>](BF<sub>4</sub>) or [Co<sup>II</sup>(dpzca)<sub>2</sub>] and [Ni<sup>II</sup>(dpzca)<sub>2</sub>] has facilitated the construction of two robust nanoporous
three-dimensional coordination polymers, [Co<sup>III</sup>(dpzca)<sub>2</sub>Ag](BF<sub>4</sub>)<sub>2</sub>·2(H<sub>2</sub>O) [<b>1</b>·2(H<sub>2</sub>O)] and [Ni<sup>II</sup>(dpzca)<sub>2</sub>Ag]BF<sub>4</sub>·0.5(acetone) [<b>2</b>·0.5(acetone)].
Despite the difference in charge distribution and anion loading, the
framework structures of <b>1</b>·2(H<sub>2</sub>O) and <b>2</b>·0.5(acetone) are isostructural. One dimensional channels
along the <i>b</i>-axis permeate the structures and contain
the tetrafluoroborate counterions (the Co<sup>III</sup>-based MOF
has twice as many BF<sub>4</sub><sup>–</sup> anions as the
Ni<sup>II</sup>-based MOF) and guest solvent molecules. These anions
are not readily exchanged whereas the solvent molecules can be reversibly
removed and replaced. The H<sub>2</sub>, N<sub>2</sub>, CO<sub>2</sub>, CH<sub>4</sub>, H<sub>2</sub>O, CH<sub>3</sub>OH, and CH<sub>3</sub>CN sorption behaviors of the evacuated frameworks <b>1</b> and <b>2</b> at 298 K have been studied, and modeled, and both show very
high selectivity for CO<sub>2</sub> over N<sub>2</sub>. The increased
anion loading in the channels of Co<sup>III</sup>-based MOF <b>1</b> relative to Ni<sup>II</sup>-based MOF <b>2</b> results
in increased selectivity for CO<sub>2</sub> over N<sub>2</sub> but
a decrease in the sorption kinetics and storage capacity of the framework
Exploiting Pressure To Induce a “Guest-Blocked” Spin Transition in a Framework Material
A new functionalized
1,2,4-triazole ligand, 4-[(<i>E</i>)-2-(5-methyl-2-thienyl)vinyl]-1,2,4-triazole
(thiome), was prepared to assess the broad applicability of strategically
producing multistep spin transitions in two-dimensional Hofmann-type
materials of the type [Fe<sup>II</sup>Pd(CN)<sub>4</sub>(R-1,2,4-trz)<sub>2</sub>]·<i>n</i>H<sub>2</sub>O (R-1,2,4-trz = a 4-functionalized
1,2,4-triazole ligand). A variety of structural and magnetic investigations
on the resultant framework material [Fe<sup>II</sup>Pd(CN)<sub>4</sub>(thiome)<sub>2</sub>]·2H<sub>2</sub>O (<b>A·2H</b><sub><b>2</b></sub><b>O</b>) reveal that a high-spin
(HS) to low-spin (LS) transition is inhibited in <b>A·2H</b><sub><b>2</b></sub><b>O</b> due to a combination of guest
and ligand steric bulk effects. The water molecules can be reversibly
removed with retention of the porous host framework and result in
the emergence of an abrupt and hysteretic one-step spin transition
due to the removal of guest internal pressure. A spin transition can,
furthermore, be induced in <b>A·2H</b><sub><b>2</b></sub><b>O</b> (0–0.68 GPa) under hydrostatic pressure,
as evidenced by variable-pressure structure and magnetic studies,
resulting in a two-step spin transition at ambient temperatures at
0.68 GPa. The presence of a two-step spin crossover (SCO) in <b>A·2H</b><sub><b>2</b></sub><b>O</b> under hydrostatic
pressure compared to a one-step SCO in <b>A</b> at ambient pressure
is discussed in terms of the relative ability of each phase to accommodate
mixed HS/LS states according to differing lattice flexibilities