9 research outputs found
Novel Iron(II) Microporous Spin-Crossover Coordination Polymers with Enhanced Pore Size
In this Communication, we report the synthesis and characterization
of novel Hofmann-like spin-crossover porous coordination polymers
of composition {FeĀ(L)Ā[MĀ(CN)<sub>4</sub>]}Ā·G [L = 1,4-bisĀ(4-pyridylethynyl)Ābenzene
and M<sup>II</sup> = Ni, Pd, and Pt]. The spin-crossover properties
of the framework are closely related to the number and nature of the
guest molecules included in the pores
Novel Iron(II) Microporous Spin-Crossover Coordination Polymers with Enhanced Pore Size
In this Communication, we report the synthesis and characterization
of novel Hofmann-like spin-crossover porous coordination polymers
of composition {FeĀ(L)Ā[MĀ(CN)<sub>4</sub>]}Ā·G [L = 1,4-bisĀ(4-pyridylethynyl)Ābenzene
and M<sup>II</sup> = Ni, Pd, and Pt]. The spin-crossover properties
of the framework are closely related to the number and nature of the
guest molecules included in the pores
Synthesis of Nanocrystals and Particle Size Effects Studies on the Thermally Induced Spin Transition of the Model Spin Crossover Compound [Fe(phen)<sub>2</sub>(NCS)<sub>2</sub>]
Surfactant-free
nanocrystals of the model spin-crossover compound [FeĀ(phen)<sub>2</sub>(NCS)<sub>2</sub>] (phen: 1,10-phenanthroline) have been synthesized
applying the reverse micelle technique. The morphology of the nanocrystals,
characterized by scanning electronic microscopy, corresponds to rhombohedric
platelets with dimensions ranging from 203 Ć 203 Ć 106 nm
to 142 Ć 142 Ć 74 nm. Variation of the concentration of the FeĀ(BF<sub>4</sub>)<sub>2</sub>Ā·6H<sub>2</sub>O salt in the synthesis has been found
to have little influence on the crystallite size. In contrast, the
solventāsurfactant ratio (Ļ) is critical for a good particle
growth. The spin transition of the nanocrystals has been characterized
by magnetic susceptibility measurements and MoĢssbauer spectroscopy.
The nanocrystals undergo an abrupt and more cooperative spin transition
in comparison with the bulk compound. The spin transition is centered
in the interval of temperature of 175ā185 K and is accompanied
by 8 K of thermal hysteresis width. The crystallite quality more than
the crystallite size is responsible for the higher cooperativity.
The magnetic properties of the nanocrystals embedded in organic polymers
such as polyethylene glycol, nujol, glycerol, and triton have been
studied as well. The spin transition in the nanocrystals is affected
by the polymer coating. The abrupt and first-order spin transition
transforms into a more continuous spin transition as a result of the
chemical pressure asserted by the organic polymers on the FeĀ(II) centers
Fast Detection of Water and Organic Molecules by a Change of Color in an Iron(II) Microporous Spin-Crossover Coordination Polymer
Here we present a novel three-dimensional ironĀ(II) spin-crossover
porous coordination polymer based on the bisĀ(1,2,4-triazol-4-yl)Āadamantane
(tr<sub>2</sub>ad) ligand and the [AuĀ(CN)<sub>2</sub>]<sup>ā</sup> metalloligand anions with the formula {Fe<sub>3</sub>(tr<sub>2</sub>ad)<sub>4</sub>[AuĀ(CN)<sub>2</sub>)]<sub>2</sub>}Ā[AuĀ(CN)<sub>2</sub>]<sub>4</sub>Ā·G. The sorption/desorption of guest molecules,
water, and five/six-membered-ring organic molecules is easily detectable
because the guest-free and -loaded frameworks present drastically
distinct coloration and spin-state configurations
Fast Detection of Water and Organic Molecules by a Change of Color in an Iron(II) Microporous Spin-Crossover Coordination Polymer
Here we present a novel three-dimensional ironĀ(II) spin-crossover
porous coordination polymer based on the bisĀ(1,2,4-triazol-4-yl)Āadamantane
(tr<sub>2</sub>ad) ligand and the [AuĀ(CN)<sub>2</sub>]<sup>ā</sup> metalloligand anions with the formula {Fe<sub>3</sub>(tr<sub>2</sub>ad)<sub>4</sub>[AuĀ(CN)<sub>2</sub>)]<sub>2</sub>}Ā[AuĀ(CN)<sub>2</sub>]<sub>4</sub>Ā·G. The sorption/desorption of guest molecules,
water, and five/six-membered-ring organic molecules is easily detectable
because the guest-free and -loaded frameworks present drastically
distinct coloration and spin-state configurations
Heterobimetallic MOFs Containing Tetrathiocyanometallate Building Blocks: Pressure-Induced Spin Crossover in the Porous {Fe<sup>II</sup>(pz)[Pd<sup>II</sup>(SCN)<sub>4</sub>]} 3D Coordination Polymer
Here we describe the synthesis, structure, and magnetic
properties
of two related coordination polymers made up of self-assembling FeĀ(II)
ions, pyrazine (pz), and the tetrathiocyanopalladate anion. Compound
{FeĀ(MeOH)<sub>2</sub>[PdĀ(SCN)<sub>4</sub>]}Ā·pz (<b>1a</b>) is a two-dimensional coordination polymer where the FeĀ(II) ions
are equatorially coordinated by the nitrogen atoms of four [PdĀ(SCN)<sub>4</sub>]<sup>2ā</sup> anions, each of which connects four
FeĀ(II) ions, forming corrugated layers {FeĀ[PdĀ(SCN)<sub>4</sub>]}<sub>ā</sub>. The coordination sphere of FeĀ(II) is completed by
the oxygen atoms of two CH<sub>3</sub>OH molecules. The layers stack
one on top of each other in such a way that the included pz molecule
establishes strong hydrogen bonds with the coordinated methanol molecules
of adjacent layers. Compound {FeĀ(pz)Ā[PdĀ(SCN)<sub>4</sub>]} (<b>2</b>) is a three-dimensional porous coordination polymer formed
by flat {FeĀ[PdĀ(SCN)<sub>4</sub>]}<sub>ā</sub> layers pillared
by the pz ligand. Thermal analysis of <b>1a</b> shows a clear
desorption of the two coordinated CH<sub>3</sub>OH molecules giving
a rather stable phase (<b>1b</b>), which presumably is a polymorphic
form of <b>2</b>. The magnetic properties of the three derivatives
are typical of the high-spin FeĀ(II) compounds. However, compounds <b>1b</b> and <b>2</b>, with coordination sphere [FeN<sub>6</sub>], show thermal spin crossover behavior at pressures higher than
ambient pressure (10<sup>5</sup> MPa)
Heterobimetallic MOFs Containing Tetrathiocyanometallate Building Blocks: Pressure-Induced Spin Crossover in the Porous {Fe<sup>II</sup>(pz)[Pd<sup>II</sup>(SCN)<sub>4</sub>]} 3D Coordination Polymer
Here we describe the synthesis, structure, and magnetic
properties
of two related coordination polymers made up of self-assembling FeĀ(II)
ions, pyrazine (pz), and the tetrathiocyanopalladate anion. Compound
{FeĀ(MeOH)<sub>2</sub>[PdĀ(SCN)<sub>4</sub>]}Ā·pz (<b>1a</b>) is a two-dimensional coordination polymer where the FeĀ(II) ions
are equatorially coordinated by the nitrogen atoms of four [PdĀ(SCN)<sub>4</sub>]<sup>2ā</sup> anions, each of which connects four
FeĀ(II) ions, forming corrugated layers {FeĀ[PdĀ(SCN)<sub>4</sub>]}<sub>ā</sub>. The coordination sphere of FeĀ(II) is completed by
the oxygen atoms of two CH<sub>3</sub>OH molecules. The layers stack
one on top of each other in such a way that the included pz molecule
establishes strong hydrogen bonds with the coordinated methanol molecules
of adjacent layers. Compound {FeĀ(pz)Ā[PdĀ(SCN)<sub>4</sub>]} (<b>2</b>) is a three-dimensional porous coordination polymer formed
by flat {FeĀ[PdĀ(SCN)<sub>4</sub>]}<sub>ā</sub> layers pillared
by the pz ligand. Thermal analysis of <b>1a</b> shows a clear
desorption of the two coordinated CH<sub>3</sub>OH molecules giving
a rather stable phase (<b>1b</b>), which presumably is a polymorphic
form of <b>2</b>. The magnetic properties of the three derivatives
are typical of the high-spin FeĀ(II) compounds. However, compounds <b>1b</b> and <b>2</b>, with coordination sphere [FeN<sub>6</sub>], show thermal spin crossover behavior at pressures higher than
ambient pressure (10<sup>5</sup> MPa)
Heterobimetallic MOFs Containing Tetrathiocyanometallate Building Blocks: Pressure-Induced Spin Crossover in the Porous {Fe<sup>II</sup>(pz)[Pd<sup>II</sup>(SCN)<sub>4</sub>]} 3D Coordination Polymer
Here we describe the synthesis, structure, and magnetic
properties
of two related coordination polymers made up of self-assembling FeĀ(II)
ions, pyrazine (pz), and the tetrathiocyanopalladate anion. Compound
{FeĀ(MeOH)<sub>2</sub>[PdĀ(SCN)<sub>4</sub>]}Ā·pz (<b>1a</b>) is a two-dimensional coordination polymer where the FeĀ(II) ions
are equatorially coordinated by the nitrogen atoms of four [PdĀ(SCN)<sub>4</sub>]<sup>2ā</sup> anions, each of which connects four
FeĀ(II) ions, forming corrugated layers {FeĀ[PdĀ(SCN)<sub>4</sub>]}<sub>ā</sub>. The coordination sphere of FeĀ(II) is completed by
the oxygen atoms of two CH<sub>3</sub>OH molecules. The layers stack
one on top of each other in such a way that the included pz molecule
establishes strong hydrogen bonds with the coordinated methanol molecules
of adjacent layers. Compound {FeĀ(pz)Ā[PdĀ(SCN)<sub>4</sub>]} (<b>2</b>) is a three-dimensional porous coordination polymer formed
by flat {FeĀ[PdĀ(SCN)<sub>4</sub>]}<sub>ā</sub> layers pillared
by the pz ligand. Thermal analysis of <b>1a</b> shows a clear
desorption of the two coordinated CH<sub>3</sub>OH molecules giving
a rather stable phase (<b>1b</b>), which presumably is a polymorphic
form of <b>2</b>. The magnetic properties of the three derivatives
are typical of the high-spin FeĀ(II) compounds. However, compounds <b>1b</b> and <b>2</b>, with coordination sphere [FeN<sub>6</sub>], show thermal spin crossover behavior at pressures higher than
ambient pressure (10<sup>5</sup> MPa)
Reversible Chemisorption of Sulfur Dioxide in a Spin Crossover Porous Coordination Polymer
The chemisorption
of sulfur dioxide (SO<sub>2</sub>) on the Hofmann-like spin crossover
porous coordination polymer (SCO-PCP) {FeĀ(pz)Ā[PtĀ(CN)<sub>4</sub>]}
has been investigated at room temperature. Thermal analysis and adsorptionādesorption
isotherms showed that ca. 1 mol of SO<sub>2</sub> per mol of {FeĀ(pz)Ā[PtĀ(CN)<sub>4</sub>]} was retained in the pores. Nevertheless, the SO<sub>2</sub> was loosely attached to the walls of the host network and completely
released in 24 h at 298 K. Single crystals of {FeĀ(pz)Ā[PtĀ(CN)<sub>4</sub>]}Ā·<i>n</i>SO<sub>2</sub> (<i>n</i> ā
0.25) were grown in water solutions saturated with SO<sub>2</sub>,
and its crystal structure was analyzed at 120 K. The SO<sub>2</sub> molecule is coordinated to the Pt<sup>II</sup> ion through the sulfur
atom ion, PtāS = 2.585(4) Ć
. This coordination slightly
stabilizes the low-spin state of the Fe<sup>II</sup> ions shifting
the critical temperatures of the spin transition by 8ā12 K.
DFT calculations have been performed to rationalize these observations