13 research outputs found
Tetraaza[1.1.1.1]<i>m</i>,<i>p</i>,<i>m</i>,<i>p</i>‑cyclophane Diradical Dications Revisited: Tuning Spin States by Confronted Arenes
Diradical dications
of two kinds of alternate-<i>meta</i>-<i>para</i>-linked tetraazacyclophanes in which <i>p</i>-phenylene
(<b>1</b>) and 9,10-anthracenylene (<b>2a</b>) moieties
are embedded in their macrocyclic backbones were
successfully isolated as air-stable salts. The structures of <b>1</b><sup>2+</sup> and <b>2a</b><sup>2+</sup> were elucidated
by X-ray analysis, and significantly different types of structural
deformation led to different spin density distributions due to the
steric demand of the confronted arene moieties. The singlet–triplet
energy gaps were determined to be +0.3 kcal mol<sup>–1</sup> (+151 K) and −1.0 kcal mol<sup>–1</sup> (−503
K) by SQUID measurements, indicating the triplet ground state for <b>1</b><sup>2+</sup> and the singlet ground state for <b>2a</b><sup>2+</sup>
Tetraaza[1<sub>4</sub>]- and Octaaza[1<sub>8</sub>]paracyclophane: Synthesis and Characterization of Their Neutral and Cationic States
Two
kinds of azaÂ[1<sub><i>n</i></sub>]Âparacyclophanes,
tetraazaÂ[1<sub>4</sub>]Âparacyclophane (<b>P4</b>) and octaazaÂ[1<sub>8</sub>]Âparacyclophane (<b>P8</b>), were synthesized as the
smallest and the largest monodisperse macrocyclic oligomers of polyaniline
ever made. Herein we report the electronic nature of the cationic
species of these two macrocycles with different ring size. By combining
ESR spectroscopy and DFT calculations it was suggested that <b>P4</b><sup>·+</sup> was classified as delocalized class III
or poised on the class II/III borderline while <b>P8</b><sup>·+</sup> was regarded as a localized class II mixed-valence
system. We successfully isolated the dication of <b>P4</b> as
a stable dicationic salt <b>P4</b><sup>2+</sup>·2Â[SbF<sub>6</sub>]<sup>−</sup>, and the structure of <b>P4</b><sup>2+</sup> was determined by X-ray crystal analysis. Variable-temperature
NMR measurements for <b>P4</b><sup>2+</sup>·2Â[SbF<sub>6</sub>]<sup>−</sup> unequivocally showed that <b>P4</b><sup>2+</sup> was a 22Ï€ electron system with a singlet ground state.
The supercharged hexacation of <b>P8</b> was also isolated as <b>P8</b><sup>6+</sup>·6Â[SbCl<sub>6</sub>]<sup>−</sup>, and X-ray crystal analysis revealed that <b>P8</b><sup>6+</sup> includes one SbCl<sub>6</sub><sup>–</sup> anion in its macrocyclic
cavity
<i>Meta</i>–<i>Para</i>-Linked Octaaza[1<sub>8</sub>]cyclophanes and Their Polycationic States
Octaazacyclophanes,
octaazaÂ[1<sub>8</sub>]<i>m</i>,<i>p</i>,<i>m</i>,<i>p</i>,<i>m</i>,<i>p</i>,<i>m</i>,<i>p</i>-cyclophane
(<b>2</b>) and octaazaÂ[1<sub>8</sub>]<i>m</i>,<i>p</i>,<i>p</i>,<i>p</i>,<i>m</i>,<i>p</i>,<i>p</i>,<i>p</i>-cyclophane
(<b>3</b>), as ring-size extended congeners of tetraazaÂ[1<sub>4</sub>]<i>m</i>,<i>p</i>,<i>m</i>,<i>p</i>-cyclophane were synthesized, and the electronic states
of their polycationic species were investigated by quantum chemical
calculations, electrochemical measurements (cyclic voltammetry (CV)
and differential pulse voltammetry (DPV)), UV–vis–NIR
spectroelectrochemical measurements, and pulsed electron spin resonance
(ESR) spectroscopy. These octaazacyclophanes exhibited multiredox
activities depending on different linkage patterns along the macrocyclic
molecular skeletons, and both molecules were oxidizable up to their
respective octacations. Spectroelectrochemical measurements demonstrated
that <i>p</i>-phenylenediamine (PD) moieties in <b>2</b> could be converted from the semiquinoidal structure to the quinoidal
sturcture with increasing oxidation number, whereas higher oxidation
states of <b>3</b> did not show definite quinoidal deformation
of PD moieties. A pulsed ESR spectrum gave evidence about formation
of the almost pure spin-triplet state for <b>3</b><sup>2+</sup>, whereas the high-spin states of <b>2</b><sup>2+</sup> and <b>2</b><sup>4+</sup> are virtually degenerate with the competing
low-spin states even at low temperatures, probably due to the fragility
of spin-coupling pathway caused by facile conformational changes
Landscape of Charge Carrier Transport in Doped Poly(3-hexylthiophene): Noncontact Approach Using Ternary Combined Dielectric, Paramagnetic, and Optical Spectroscopies
We report on a comprehensive measurement
system for mobility and
energy states of charge carriers in matter under dynamic chemical
doping. The temporal evolution of the iodine doping process of polyÂ(3-hexylthiophene)
(P3HT) was monitored directly through electron paramagnetic resonance
(EPR) and optical absorption spectroscopy, as well as differential
electrical conductivity by the microwave conductivity measurement.
The increase in conductivity was observed after the EPR intensity
reached a maximum and declined thereafter, and the conductivity finally
reached ∼80 S cm<sup>–1</sup>. The carrier species changed
from a paramagnetic polaron with an estimated mobility of μ<sub>P+</sub> ≈ 2 × 10<sup>–3</sup> cm<sup>2</sup> V<sup>–1</sup> s<sup>–1</sup> to an antiferromagnetic polaron
pair with μ<sub>PP+</sub> ≈ 0.6 cm<sup>2</sup> V<sup>–1</sup> s<sup>–1</sup>. The technique presented here
can be a ubiquitous method for rapid and direct observation of charge
carrier mobility and energy states in p-type semiconducting materials
as a completely noncontact, experimental, and quantitative technique
Hash-Mark-Shaped Azaacene Tetramers with Axial Chirality
The tetramers of azapentacene derivatives
with unique hash mark
(#)-shaped structures were prepared in a quite facile manner. The
#-shaped tetramers are optically active due to possessing extended
biaryl skeletons, and the structure of the tetramer composed of four
dihydrodiazaÂpentacene (DHDAP) units (<b>1</b>) was investigated
as the first example of this kind of molecule. The tetramer <b>1</b> showed characteristic chiroptical properties reflecting
its orthogonally arranged quadruple DHDAP moieties, as well as redox
activity. The solution of enantiopure <b>1</b> exhibited intense
circularly polarized luminescence (CPL) with a dissymmetry factor
of 2.5 × 10<sup>–3</sup>. The absolute configuration of
the enantiomers of <b>1</b> was experimentally determined by
X-ray crystal analysis for the dication salt of the enantiomer of <b>1</b> with SbCl<sub>6</sub><sup>–</sup> counterions. The
solutions of enantiopure <b>1</b><sup>2+</sup>·2Â[SbCl<sub>6</sub><sup>–</sup>] also showed NIR circular dichroism (CD)
spectra over the entire range from visible to 1100 nm, enabling the
modulation of the chiroptical properties by redox stimuli
Hash-Mark-Shaped Azaacene Tetramers with Axial Chirality
The tetramers of azapentacene derivatives
with unique hash mark
(#)-shaped structures were prepared in a quite facile manner. The
#-shaped tetramers are optically active due to possessing extended
biaryl skeletons, and the structure of the tetramer composed of four
dihydrodiazaÂpentacene (DHDAP) units (<b>1</b>) was investigated
as the first example of this kind of molecule. The tetramer <b>1</b> showed characteristic chiroptical properties reflecting
its orthogonally arranged quadruple DHDAP moieties, as well as redox
activity. The solution of enantiopure <b>1</b> exhibited intense
circularly polarized luminescence (CPL) with a dissymmetry factor
of 2.5 × 10<sup>–3</sup>. The absolute configuration of
the enantiomers of <b>1</b> was experimentally determined by
X-ray crystal analysis for the dication salt of the enantiomer of <b>1</b> with SbCl<sub>6</sub><sup>–</sup> counterions. The
solutions of enantiopure <b>1</b><sup>2+</sup>·2Â[SbCl<sub>6</sub><sup>–</sup>] also showed NIR circular dichroism (CD)
spectra over the entire range from visible to 1100 nm, enabling the
modulation of the chiroptical properties by redox stimuli
Hash-Mark-Shaped Azaacene Tetramers with Axial Chirality
The tetramers of azapentacene derivatives
with unique hash mark
(#)-shaped structures were prepared in a quite facile manner. The
#-shaped tetramers are optically active due to possessing extended
biaryl skeletons, and the structure of the tetramer composed of four
dihydrodiazaÂpentacene (DHDAP) units (<b>1</b>) was investigated
as the first example of this kind of molecule. The tetramer <b>1</b> showed characteristic chiroptical properties reflecting
its orthogonally arranged quadruple DHDAP moieties, as well as redox
activity. The solution of enantiopure <b>1</b> exhibited intense
circularly polarized luminescence (CPL) with a dissymmetry factor
of 2.5 × 10<sup>–3</sup>. The absolute configuration of
the enantiomers of <b>1</b> was experimentally determined by
X-ray crystal analysis for the dication salt of the enantiomer of <b>1</b> with SbCl<sub>6</sub><sup>–</sup> counterions. The
solutions of enantiopure <b>1</b><sup>2+</sup>·2Â[SbCl<sub>6</sub><sup>–</sup>] also showed NIR circular dichroism (CD)
spectra over the entire range from visible to 1100 nm, enabling the
modulation of the chiroptical properties by redox stimuli
Hash-Mark-Shaped Azaacene Tetramers with Axial Chirality
The tetramers of azapentacene derivatives
with unique hash mark
(#)-shaped structures were prepared in a quite facile manner. The
#-shaped tetramers are optically active due to possessing extended
biaryl skeletons, and the structure of the tetramer composed of four
dihydrodiazaÂpentacene (DHDAP) units (<b>1</b>) was investigated
as the first example of this kind of molecule. The tetramer <b>1</b> showed characteristic chiroptical properties reflecting
its orthogonally arranged quadruple DHDAP moieties, as well as redox
activity. The solution of enantiopure <b>1</b> exhibited intense
circularly polarized luminescence (CPL) with a dissymmetry factor
of 2.5 × 10<sup>–3</sup>. The absolute configuration of
the enantiomers of <b>1</b> was experimentally determined by
X-ray crystal analysis for the dication salt of the enantiomer of <b>1</b> with SbCl<sub>6</sub><sup>–</sup> counterions. The
solutions of enantiopure <b>1</b><sup>2+</sup>·2Â[SbCl<sub>6</sub><sup>–</sup>] also showed NIR circular dichroism (CD)
spectra over the entire range from visible to 1100 nm, enabling the
modulation of the chiroptical properties by redox stimuli
Hash-Mark-Shaped Azaacene Tetramers with Axial Chirality
The tetramers of azapentacene derivatives
with unique hash mark
(#)-shaped structures were prepared in a quite facile manner. The
#-shaped tetramers are optically active due to possessing extended
biaryl skeletons, and the structure of the tetramer composed of four
dihydrodiazaÂpentacene (DHDAP) units (<b>1</b>) was investigated
as the first example of this kind of molecule. The tetramer <b>1</b> showed characteristic chiroptical properties reflecting
its orthogonally arranged quadruple DHDAP moieties, as well as redox
activity. The solution of enantiopure <b>1</b> exhibited intense
circularly polarized luminescence (CPL) with a dissymmetry factor
of 2.5 × 10<sup>–3</sup>. The absolute configuration of
the enantiomers of <b>1</b> was experimentally determined by
X-ray crystal analysis for the dication salt of the enantiomer of <b>1</b> with SbCl<sub>6</sub><sup>–</sup> counterions. The
solutions of enantiopure <b>1</b><sup>2+</sup>·2Â[SbCl<sub>6</sub><sup>–</sup>] also showed NIR circular dichroism (CD)
spectra over the entire range from visible to 1100 nm, enabling the
modulation of the chiroptical properties by redox stimuli
Isolable Triradical Trication of Hexaaza[1<sub>6</sub>]paracyclophane with Embedded 9,10-Anthrylenes: A Frustrated Three-Spin System
A new derivative
of hexaazaÂ[1<sub>6</sub>]Âparacyclophane in which <i>p</i>-phenylenes are alternately replaced by 9,10-anthrylenes was prepared
to investigate the impact on overall π-conjugation as well as
conformational change of the macrocycle. The charge and spin distribution
for one-electron and three-electron oxidation of the macrocycle was
elucidated by means of electrochemical, spectroelectrochemical, EPR
spectroscopic, and SQUID magnetometric methods. In particular, the
triradical trication was successfully isolated as an air-stable salt,
and moreover, its structure was disclosed by X-ray analysis. The triradical
trication was characterized as a spin-frustrated three-spin system
with the antiferromagnetic exchange interaction (<i>J</i>/<i>k</i><sub>B</sub> ≃ – 74 K)