14 research outputs found
Reparameterization of PM6 Applied to Organic Diradical Molecules
We
have performed a reparameterization of PM6 (called rPM6) to
compute open-shell species, specifically organic diradical molecules,
within a framework of the spin-unrestricted semiempirical molecular
orbital (SE-UMO) method. The parameters for the basic elements (hydrogen,
carbon, nitrogen, and oxygen) have been optimized simultaneously using
the training set consisting of 740 reference data. On the basis of
the GMTKN30 database, the mean absolute error of rPM6 is decreased
from 16.1 to 14.1 kcal/mol, which reassures its accuracy for ground-state
properties. Applications of the spin-unrestricted rPM6 (UrPM6) method
to small diradicals and relatively large polycyclic aromatic hydrocarbons
have provided substantial improvement over the standard SE-UMO methods
like UAM1, UPM3, and the original UPM6. The UrPM6 calculation is much
less susceptible to spin contamination and, therefore, reproduces
geometric parameters and adiabatic singletātriplet energy gaps
obtained by UDFT (UB3LYP and/or UBHandHLYP) at much lower computational
cost
A Density Functional Theory Based Protocol to Compute the Redox Potential of Transition Metal Complex with the Correction of Pseudo-Counterion: General Theory and Applications
We propose an accurate
scheme to evaluate the redox potential of
a wide variety of transition metal complexes by adding a charge-dependent
correction term for a counterion around the charged complexes, which
is based on Generalized Born theory, to the solvation energy. The
mean absolute error (MAE) toward experimental redox potentials of
charged complexes is considerably reduced from 0.81 V (maximum error
1.22 V) to 0.22 V (maximum error 0.50 V). We found a remarkable exchange-correlation
functional dependence on the results rather than the basis set ones.
The combination of Wachters+f (for metal) and 6-31++GĀ(d,p) (for other
atoms) with the B3LYP functional gives the least MAE 0.15 V for the
test complexes. This scheme is applicable to other solvents, and heavier
transition metal complexes such as M<sub>1</sub>(CO)<sub>5</sub>(pycn)
(M<sub>1</sub> = Cr, Mo, W), M<sub>2</sub>(mnt)<sub>2</sub> (M<sub>2</sub> = Ni, Pd, Pt), and M<sub>3</sub>(bpy)<sub>3</sub> (M<sub>3</sub> = Fe, Ru, Os) with the same quality
Quantum Master Equation Approach to Singlet Fission Dynamics of Realistic/Artificial Pentacene Dimer Models: Relative Relaxation Factor Analysis
The
singlet fission (SF) dynamics of realistic/artificial pentacene
dimer models are investigated using the quantum master equation method
in order to obtain new insight into the SF dynamics and its rational
design guidelines. We comprehensively clarify the effects of the energy
offsets of diabatic Frenkel exciton (FE) and charge transfer (CT)
exciton states to the double-triplet (TT) exciton state, excitonic
couplings, and state-dependent vibronic couplings on the exciton population
dynamics using relative relaxation factors (RRFs) between the adiabatic
exciton states. As shown in previous studies, efficient sequential/superexchange
CT-mediated SF is observed in the energy level matching region (<i>E</i>(TT) ā <i>E</i>(FE) < 0). On the other
hand, it is predicted that almost the perfect energy level matching
(<i>E</i>(TT) ā <i>E</i>(FE) ā¼ 0)
causes the significant reduction of TT yields though exhibits remarkably
fast SF rates, when the corresponding adiabatic double-triplet (TTā²)
and Frenkel exciton (FEā²) states are near-degenerate to each
other with common diabatic configurations. The excitonic coupling
is also found to have a possibility of causing significant change
of SF dynamics when it has a large amplitude comparable to those of
the other electronic coupling elements. Furthermore, the large vibronic
coupling of CT state shows striking enhancement of SF rates with keeping
high TT yields in the CT-mediated superexchange region, while the
large vibronic couplings of FE and TT states do not show such striking
enhancement. These features are understood by analyzing their RRFs,
which are proportional to the product of the square of common diabatic
exciton configuration coefficients in the concerned two adiabatic
exciton states, multiplied by the spectral density (vibronic coupling)
Origin of the Enhancement of the Second Hyperpolarizabilities of MetalāCarbon Bonds
The spin-unrestricted
coupled-cluster method was employed to investigate
the origin of the second hyperpolarizabilities (Ī³) in model
systems involving metalācarbon bonds with various bond lengths
as a function of their diradical character (<i>y</i>) and
charge transfer (CT). These systems exhibit unique features: (i) Ļ
electrons give the dominant contribution to Ī³, (ii) the Ļ
electrons contribution to Ī³ is negative, (iii) when the bond
length increases, Ī³ exhibits two positive extrema, which are
associated with the CT nature and the intermediate diradical character,
respectively, (iv) and one negative extremum corresponding to intermediate
CT and diradical character, and (v) in the bond stretching process,
the maximum Ī³ amplitude per Ļ bond is about 7 times larger
than that per Ļ bond. These features are significantly different
from those observed in pure organic systems
Dissymmetric Bis(dipyrrinato)zinc(II) Complexes: Rich Variety and Bright Red to Near-Infrared Luminescence with a Large Pseudo-Stokes Shift
BisĀ(dipyrrinato)ĀmetalĀ(II)
and trisĀ(dipyrrinato)ĀmetalĀ(III) complexes
have been regarded as much less useful luminophores than their boron
difluoride counterparts (4,4-difluoro-4-bora-3a,4a-diaza-<i>s</i>-indacenes, BODIPYs), especially in polar solvent. We proposed previously
that dissymmetry in such metal complexes (i.e., two different dipyrrinato
ligands in one molecule) improves their fluorescence quantum efficiencies.
In this work, we demonstrate the universality and utility of our methodology
by synthesizing eight new dissymmetric bisĀ(dipyrrinato)ĀzincĀ(II) complexes
and comparing them with corresponding symmetric complexes. Single-crystal
X-ray diffraction analysis, <sup>1</sup>H and <sup>13</sup>C NMR spectroscopy,
and high-resolution mass spectrometry confirm the retention of dissymmetry
in both solution and solid states. The dissymmetric complexes all
show greater photoluminescence (PL) quantum yields (Ļ<sub>PL</sub>) than the corresponding symmetric complexes, allowing red to near-infrared
emissions with large pseudo-Stokes shifts. The best performance achieves
a maximum PL wavelength of 671 nm, a pseudo-Stokes shift of 5400 cm<sup>ā1</sup>, and Ļ<sub>PL</sub> of 0.62ā0.72 in
toluene (dielectric constant Īµ<sub>s</sub> = 2.4), dichloromethane
(Īµ<sub>s</sub> = 9.1), acetone (Īµ<sub>s</sub> = 21.4),
and ethanol (Īµ<sub>s</sub> = 24.3). The large pseudo-Stokes
shift is distinctive considering BODIPYs with small Stokes shifts
(ā¼500 cm<sup>ā1</sup>), and the Ļ<sub>PL</sub> values are higher than or comparable to those of BODIPYs fluorescing
at similar wavelengths. Electrochemistry and density functional theory
calculations illustrate that frontier orbital ordering in the dissymmetric
complexes meets the condition for efficient PL proposed in our theory
Diradical and Ionic Characters of Open-Shell Singlet Molecular Systems
The
diradical and ionic natures of open-shell singlet systems have
been investigated using new definitions of the diradical and ionic
characters as well as of their densities within the valence configuration
interaction (VCI) model with two electrons in two active orbitals.
The two-site symmetric and asymmetric diradical models are examined
by using these diradical/ionic characters. For realistic compounds,
we investigate a diradicaloid diphenalenyl and a rectangular graphene
nanoflake in the presence of an external static electric field, as
well as Ļ-stacked phenalenyl-derivative dimers with varying
the intermonomer distance, where the central carbon atoms in the phenalenyl
rings are substituted by boron (B) and nitrogen (N) atoms, respectively.
It is found that the increase of charge asymmetricity induced by the
static electric field decreases the diradical character and finally
induces an ionic character in the ground state, while the first excited
state is changed from pure ionic to diradical-dominant as the field
amplitude increases. On the other hand, when increasing the intermonomer
distance, the B/N substitution in the phenalenyl dimer changes the
electronic state from open-shell singlet with small diradical character
to closed-shell with large ionic character. These results indicate
that the application of a static electric field to diradicaloids and
the asymmetric substitution of a pancake bonded Ļ-dimer combined
with the variation of intermonomer distance could tune the diradical/ionic
characters and therefore control the nonlinear optical responses
ĻāConjugated Trinuclear Groupā9 Metalladithiolenes with a Triphenylene Backbone
Previously,
we synthesized Ļ-conjugated trinuclear metalladithiolene complexes
based on benzenehexathiol (<i>J. Chem. Soc., Dalton Trans.</i> <b>1998</b>, 2651; <i>Dalton Trans.</i> <b>2009</b>, 1939; <i>Inorg. Chem.</i> <b>2011</b>, <i>50</i>, 6856). Here we report trinuclear complexes with a triphenylene
backbone. A reaction with triphenylenehexathiol and group 9 metal
precursors in the presence of triethylamine gives rise to trinuclear
complexes <b>9</b>ā<b>11</b>. The planar structure
of <b>11</b> is determined using single crystal X-ray diffraction
analysis. The ligand-to-metal charge transfer bands of <b>9</b>ā<b>11</b> move to longer wavelengths compared with
those of mononuclear <b>12</b>ā<b>14</b>. Electrochemical
measurements disclose that the one-electron and two-electron reduced
mixed-valent states are stabilized thermodynamically. UVāvisāNIR
spectroscopy for the reduced species of <b>9</b> identifies
intervalence charge transfer bands for <b>9</b><sup>ā</sup> and <b>9</b><sup>2ā</sup>, substantiating the existence
of electronic communication among the three metal nuclei. These observations
prove that the triphenylene backbone transmits Ļ-conjugation
among the three metalladithiolene units
Bis(dipyrrinato)zinc(II) Complex Chiroptical Wires: Exfoliation into Single Strands and Intensification of Circularly Polarized Luminescence
One-dimensional
(1D) coordination polymers (CPs) experiences limitations
in exfoliation into individual strands, which hamper their utility
as functional 1D nanomaterials. Here we synthesize chiral 1D-CPs that
feature the bisĀ(dipyrrinato)ĀzincĀ(II) complex motif. They can be exfoliated
into single strands upon sonication in organic media, retaining lengths
of up to 3.19 Ī¼m (ca. 2600 monomer units). Their chiroptical
structure allows the exfoliated wires to show circularly polarized
luminescence at an intensity 5.9 times that of reference monomer complexes
Comparison of the Magnetic Anisotropy and Spin Relaxation Phenomenon of Dinuclear Terbium(III) Phthalocyaninato Single-Molecule Magnets Using the Geometric Spin Arrangement
Herein
we report the synthesis and characterization of a dinuclear
Tb<sup>III</sup> single-molecule magnet (SMM) with two [TbPc<sub>2</sub>]<sup>0</sup> units connected via a fused-phthalocyaninato ligand.
The stable and robust complex [(obPc)ĀTbĀ(Fused-Pc)ĀTbĀ(obPc)] (<b>1</b>) was characterized by using synchrotron radiation measurements
and other spectroscopic techniques (ESI-MS, FT-IR, UV). The magnetic
couplings between the Tb<sup>III</sup> ions and the two Ļ radicals
present in <b>1</b> were explored by means of density functional
theory (DFT). Direct and alternating current magnetic susceptibility
measurements were conducted on magnetically diluted and nondiluted
samples of <b>1</b>, indicating this compound to be an SMM with
improved properties compared to those of the well-known [TbPc<sub>2</sub>]<sup>ā/0/+</sup> and the axially symmetric dinuclear
Tb<sup>III</sup> phthalocyaninato triple-decker complex (Tb<sub>2</sub>(obPc)<sub>3</sub>). Assuming that the probability of quantum tunneling
of the magnetization (QTM) occurring in one TbPc<sub>2</sub> unit
is <i>P</i><sub>QTM</sub>, the probability of QTM simultaneously
occurring in <b>1</b> is <i>P</i><sub>QTM</sub><sup>2</sup>, meaning that QTM is effectively suppressed. Furthermore,
nondiluted samples of <b>1</b> underwent slow magnetic relaxation
times (Ļ ā 1000 s at 0.1 K), and the blocking temperature
(<i>T</i><sub>B</sub>) was determined to be ca. 16 K with
an energy barrier for spin reversal (<i>U</i><sub>eff</sub>) of 588 cm<sup>ā1</sup> (847 K) due to <i>D</i><sub>4<i>d</i></sub> geometry and weak inter- and intramolecular
magnetic interactions as an exchange bias (<i>H</i><sub>bias</sub>), reducing QTM. Four hyperfine steps were observed by
micro-SQUID measurement. Furthermore, solution NMR measurements (one-dimensional,
two-dimensional, and dynamic) were done on <b>1</b>, which led
to the determination of the high rotation barrier (83 Ā± 10 kJ/mol)
of the obPc ligand. A comparison with previously reported Tb<sup>III</sup> triple-decker compounds shows that ambient temperature NMR measurements
can indicate improvements in the design of coordination environments
for SMMs. A large <i>U</i><sub>eff</sub> causes strong uniaxial
magnetic anisotropy in <b>1</b>, leading to a Ļ<sub>ax</sub> value (1.39 Ć 10<sup>ā30</sup> m<sup>3</sup>) that is
larger than that for Tb<sub>2</sub>(obPc)<sub>3</sub> (0.86 Ć
10<sup>ā30</sup> m<sup>3</sup>). Controlling the coordination
environment and spin arrangement is an effective technique for suppressing
QTM in TbPc<sub>2</sub>-based SMMs