6 research outputs found
Practical Porous Matrix for Molecular Structure Determination of General Liquid Chemicals
A practical
porous crystalline matrix for molecular structure determination
of a wide range of liquid chemicals has been set up. We herein report
proof-of-concept research on the temperature-dependent single-crystal-to-single-crystal
(SCSC) guest exchange of the <i>P</i>- and <i>M</i>-helix-enantiomeric multilayered ensemble with flexible open-channels
of the shortest diameter, 4.4 × 4.4 Å<sup>2</sup>. This
landmark ensemble is, to the best of our knowledge, the most efficient,
practical, tolerant, and reproducible porous matrix for single crystal
structure determination of general liquid compounds via easy SCSC
guest exchange without any desolvation process. The innovative channel
behaves in a guest-dependent flexible response manner and enables
scientists to solve structures of a wide range of liquid chemicals.
This paper reports the molecular structures of 41 liquid chemicals
including chiral and natural compounds via guest exchange at >75%
success rate
Suprachannels via a Molecular Array of 2D Networks: Solvent Effects, Anion Exchange, and Physicochemical Properties of Silver(I) Complexes Bearing <i>N</i>,<i>N</i>′,<i>N</i>″‑Tris(2-pyridinylethyl)-1,3,5-benzenetricarboxamide
The
solvent effects on suprachannel formation via a molecular array
of 2D networks were studied. The basic structure of the [Ag<sub>3</sub>L<sub>2</sub>](X)<sub>3</sub> (X<sup>–</sup> = NO<sub>2</sub><sup>–</sup>, NO<sub>3</sub><sup>–</sup>) 2D network
consists of hexagonal (Ag<sub>6</sub>L<sub>6</sub>) motifs formed
via self-assembly of Ag(I) with <i>C</i><sub>3</sub>-tridentate <i>N</i>-donors. The 2D networks are arranged in an eclipsed mode
in aqueous solution, thus forming suprachannels (5.2 × 7.3 Å<sup>2</sup>, 6.2 × 7.7 Å<sup>2</sup>) of [Ag<sub>3</sub>L<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>](X)<sub>3</sub>, whereas they
are arranged in a staggered <i>abab</i>... mode in nonaqueous
solution, thus forming semisuprachannels (3.1 × 5.1 Å<sup>2</sup>) of [Ag<sub>3</sub>(NO<sub>3</sub>)<sub>2</sub>L<sub>2</sub>](NO<sub>3</sub>). The suprachannel structure of [Ag<sub>3</sub>L<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>](NO<sub>3</sub>)<sub>3</sub> is
soluble in methanol; contrastingly, the semisuprachannel structure
of [Ag<sub>3</sub>(NO<sub>3</sub>)<sub>2</sub>L<sub>2</sub>](NO<sub>3</sub>) is insoluble in that solvent. In the present study, significant
differences in molecular recognition and anion exchangeability between
[Ag<sub>3</sub>L<sub>2</sub>(H<sub>2</sub>O)<sub>2</sub>](NO<sub>3</sub>)<sub>3</sub> and [Ag<sub>3</sub>(NO<sub>3</sub>)<sub>2</sub>L<sub>2</sub>](NO<sub>3</sub>) were found
Crystals of Ni<sub>6</sub>L<sub>12</sub> Ellipsoidal Tubes as Single-Crystal-to-Single-Crystal Adsorption Matrix: Penetrative Study of Self-Assembled Crystals vs Guest-Exchanged Crystals
Informative similarities/differences between self-assembled
and
single-crystal-to-single-crystal (SCSC) guest-exchanged crystals based
on both the molecular structure and adsorption nature are observed.
The self-assembly of Ni(ClO4)2 with a dicyclopentyldi(pyridine-3-yl)silane
bidentate ligand (L) in a mixture of toluene and acetonitrile gives
rise to purple crystals consisting of double-stranded ellipsoidal
tubes, [Ni6(ClO4)4(CH3CN)8L12]·8ClO4·4CH3CN·5C7H8. The coordinated acetonitriles
as well as the solvates are removed at 170 °C to transform the
purple crystals into blue crystals of [Ni(ClO4)2L2]n that return to the original
crystals in the mixture of toluene and acetonitrile. Further, the
toluene and acetonitrile solvates of the original crystals are replaced
by o-, m-, and p-xylene isomers within 5 min in a SCSC manner. In the present study,
SCSC xylene-exchanged crystals were compared with crystals obtained
from direct self-assembly in a mixture of each xylene isomer and acetonitrile
Host–Guest Chemistry of 1D Suprachannels and Dihalomethane Molecules: Metallacyclodimeric Ensembles Consisting of Zinc(II)-2,7-bis(nicotinoyloxy)naphthalene Complexes
Self-assembly
of ZnX<sub>2</sub> (X = Cl, Br, and I) with 2,7-bis(nicotinoyloxy)naphthalene
(L) as a hemicircular bidentate ligand containing a chromophore moiety
yields a systematic metallacyclodimeric unit, [ZnX<sub>2</sub>(L)]<sub>2</sub>. These basic skeletons constitute, via interdigitated π···π
interactions, a unique columnar ensemble forming a suprachannel. This
can then be employed as an unusual “diiodomethane within the
suprachannel” host–guest system, CH<sub>2</sub>I<sub>2</sub>@[ZnX<sub>2</sub>(L)]<sub>2</sub>. Specifically, the
suprachannel significantly stabilizes the CH<sub>2</sub>I<sub>2</sub> molecules in the order [ZnI<sub>2</sub>(L)]<sub>2</sub> > [ZnBr<sub>2</sub>(L)]<sub>2</sub> > [ZnCl<sub>2</sub>(L)]<sub>2</sub>. This
suprachannel has significant halogen effects on the photoluminescence
(PL), thermal properties, and host–guest inclusion
Suprachannel as a Radical Trap: Crystal Structure of Single Carbon Radicals
We report proof-of-concept
experiments on the unprecedented crystal
structure of an iodomethyl radical (·CH<sub>2</sub>I) nestled
within an ensemble’s suprachannel via single crystal-to-single
crystal photoreaction without destruction of the suprachannel. The
trapped nonconjugated carbon radical was additionally confirmed by
EPR, <sup>13</sup>C MAS, UPS, and Raman spectra
Host–Guest Conversion: Transformation of Diiodomethane within 1D-Ensemble Suprachannels into Triiodide–Iodine Channel via Photoreaction
Self-assembly
of ZnBr<sub>2</sub> with 2,7-bis(isonicotinoyloxy)naphthalene
(L) yields one-dimensional (1D) zigzag chains of [ZnBr<sub>2</sub>L] composition. This 1D chain ensemble forms unique suprachannels
of 4.0 × 4.2 Å<sup>2</sup> size via weak C–H···π
and π···π interactions. A 350 nm ultraviolet
irradiation affects host–guest conversion. Diiodomethane molecules
within the suprachannel structure of CHCl<sub>3</sub>·CH<sub>2</sub>I<sub>2</sub>@[ZnBr<sub>2</sub>L] were transformed into an
unprecedented triiodide–iodine channel skeleton, HL<sup>+</sup>@[I<sub>3</sub>·I<sub>2</sub>]<sup>−</sup>. Specifically,
two clear, quasi-reversible redox peaks were observed at +0.33 and
+0.70 V versus Ag/AgCl in the anodic scan and at +0.19 and +0.62 V
in the cathodic scan in acetonitrile for HL<sup>+</sup>@[I<sub>3</sub>·I<sub>2</sub>]<sup>−</sup>