We report here the synthesis and photophysical study of a series of electron donor-acceptor molecules, in which electron-donating 4-methoxyphenoxy groups are attached to the 1,7-bay positions of four different perylene tetracarboxylic acid derivatives, namely, perylene tetraesters 1, perylene monoimide diesters 2, perylene bisimides 3, and perylene monobenzimidazole monoimides 4. These perylene derivatives are used because of their increasing order of electron-accepting capability upon moving from 1 to 4. Two additional donor-acceptor molecules are synthesized by linking electron-donating 4-methoxyphenyl groups to the imide position of perylene monoimide diester 2 and perylene bisimide 3. The motivation for this study is to achieve a good control over the photoinduced charge-transfer (CT) process in perylene-based systems by altering the position of electron donors and tuning the electron deficiency of perylene core. A comprehensive study of the photophysical properties of these molecules has shown a highly systematic trend in the magnitude of CT as a function of increased electron deficiency of the perylene core and solvent polarity. Importantly, just by changing the attachment of electron-donating group from "bay" to "imide" position, we are able to block the CT process. This implies that the positioning of the electron donor at the perylene core strongly influences the kinetics of the photoinduced CT process. In these compounds, the CT process is characterized by the quenching of fluorescence and singlet excited-state lifetimes as compared to model compounds bearing non-electron-donating 4-tert-butylphenoxy groups. Transient absorption spectroscopy did not reveal spectra of CT states. This most likely implies that the CT state is not accumulated, because of the faster charge recombination.
We report here the synthesis and photophysical study of a series of electron donor-acceptor molecules, in which electron-donating 4-methoxyphenoxy groups are attached to the 1,7-bay positions of four different perylene tetracarboxylic acid derivatives, namely, perylene tetraesters 1, perylene monoimide diesters 2, perylene bisimides 3, and perylene monobenzimidazole monoimides 4. These perylene derivatives are used because of their increasing order of electron-accepting capability upon moving from 1 to 4. Two additional donor-acceptor molecules are synthesized by linking electron-donating 4-methoxyphenyl groups to the imide position of perylene monoimide diester 2 and perylene bisimide 3. The motivation for this study is to achieve a good control over the photoinduced charge-transfer (CT) process in perylene-based systems by altering the position of electron donors and tuning the electron deficiency of perylene core. A comprehensive study of the photophysical properties of these molecules has shown a highly systematic trend in the magnitude of CT as a function of increased electron deficiency of the perylene core and solvent polarity. Importantly, just by changing the attachment of electron-donating group from "bay" to "imide" position, we are able to block the CT process. This implies that the positioning of the electron donor at the perylene core strongly influences the kinetics of the photoinduced CT process. In these compounds, the CT process is characterized by the quenching of fluorescence and singlet excited-state lifetimes as compared to model compounds bearing non-electron-donating 4-tert-butylphenoxy groups. Transient absorption spectroscopy did not reveal spectra of CT states. This most likely implies that the CT state is not accumulated, because of the faster charge recombination.
A good control over
photoinduced charge and energy transfer between
donor and acceptor moieties is essential for the development of artificial
photosynthesis.[1−4] Important variables, which dictate the yields and kinetics of these
interactions, are excited-state and redox properties of the donor
and acceptor components, their relative distance, mutual orientation,
and electronic coupling.[5−10] During the past three decades, molecular assemblies consisting of
light-harvesting chromophores, charge separators, and catalysts have
been designed and studied to gain a better understanding of the photochemistry
and photophysics involved in these systems.[11−13] Such assemblies
are of prime importance because of their ability to mimic the natural
photosynthetic process and to convert sunlight into fuel.Several
chromophores have been tested as integrative building blocks
for light-harvesting and charge separation. Perylene tetracarboxylic
acid derivatives, of which perylene bisimides (PBIs) are the best-known
representatives, are particularly attractive chromophores due to their
exceptional photochemical stability, high electron deficiency, strong
absorption in the visible region of the solar spectrum, and possibility
to further tune their photophysical properties by structural modifications.[14,15] Taking advantage of high photochemical robustness and strong absorption,
various light-harvesting antenna systems have been prepared using
perylene tetracarboxylic acid derivatives as the active chromophore.[16−18,10] However, because of the high
electron deficiency of the perylene core, charge separation has been
commonly observed when these compounds are covalently coupled even
with moderately electron-rich donors.[18,19]Perylene
tetracarboxylic acid derivatives (mostly PBIs) are also
attractive components of charge separators, and for this application,
their high electron deficiency is highly beneficial. In the past,
many separate studies on perylene-based donor–acceptor systems
have been performed.[19−23] These studies have revealed that the efficiency and kinetics of
charge transfer (CT) are highly sensitive to even small structural
variations. In a recent study on PBI-based isoelectronic donor-bridge-acceptor
compounds, we showed that small changes in the molecular bridge have
a large impact on the dynamics of charge separation.[24] In another recent study, Shoer et al. observed that the
charge separation can be an order of magnitude faster for systems
in which donors are connected to the ortho (or headland) positions
of the perylene core as compared to the imide position.[25]Another recent study by Pagoaga et al.
reported strong fluorescence
quenching ascribed to charge separation, for PBIs bearing 4-methoxybenzene
substituents as electron donors at various bay positions.[26] Preceding work by Flamigni et al. on non-bay-substituted
PBIs, bearing mono-, di-, and trimethoxy-benzene at the imide position,
has revealed that CT rates strongly correlate with the redox properties
of the methoxybenzene and the positioning of the methoxy group.[27] A comparison between efficiency of CT and the
positioning of the electron donors cannot be made from these studies,
because 1,7-bay substitution decreases the reduction potential of
the perylene acceptor, that is, makes the perylene core less electron-deficient.[14] Therefore, there is still a need for a comprehensive
study to understand the kinetics of CT toward perylenes as a function
of the position at which the electron-donating substituents are attached,
so that perylene-containing devices can be designed in which the perylene
derivatives serve a well-defined role of energy acceptor or donor
in a light harvesting antenna and that of electron acceptor in a charge-separating
unit.In this work, we report on the design, the synthesis,
and the photophysical
properties of a series of perylene-3,4,9,10-tetracarboxylic acid derivatives
bearing either 4-methoxyphenoxy or 4-methoxyphenyl groups as electron
donors. The choice of these groups as electron donors is based on
reports in which facile CT was observed upon photoexcitation of perylene
bisimides bearing methoxyphenyl groups as electron donors.[26,27] In this study, the electrochemical and optical properties of the
perylene core were also systematically tuned by the modifications
at the peri-positions. For the photophysical characterization of our
compounds, steady-state and time-resolved spectroscopic studies were
performed in solvents of different polarity. In these compounds, the
strong fluorescence of the perylene moiety was quenched to different
extent by electron-donating groups attached to the perylene core at
different positions. The aim of this work is to establish a relation
between molecular structure and the extent of fluorescence quenching
observed for these molecules in solvents of different polarity. We
ascribe this fluorescence quenching to photoinduced CT and assume
that the positions from which quenching is efficient are the appropriate
positions to attach electron donors and achieve efficient charge separation.
Finally, the obtained experimental results are rationalized by computational
calculations based on time-dependent density functional theory (TD-DFT).
Results
and Discussion
Synthesis and Characterization
As
described in Scheme , the reported 1,7-diphenoxy-substituted
compounds (1a–b, 2a–c, 3a–c, and 4a–b) were synthesized from their corresponding
1,7-dibromoperylene-3,4,9,10-tetracarboxylic acid derivatives, 1,7-dibromoperylene
tetrabutylester 1, N-(2,6-diisopropylphenyl)-1,7-dibromoperylenemonoimide dibutylester 2, N,N′-bis(2,6-diisopropylphenyl)-1,7-dibromoperylenebisimide 3, and the N-(2,6-diisopropylphenyl)-1,7-dibromoperylenemonoimide monobenzimidazoles (4 and 4′).
Scheme 1
Synthesis of 1,7-Di(4-tert-butylphenoxy) and
1,7-Di(4-methoxyphenoxy)perylene-3,4,9,10-tetracarboxylic
Acid Derivatives
The syntheses of these regioisomerically pure 1,7-dibromo-precursors
(1–4) was performed from commercially
available perylene-3,4,9,10-tetracarboxylic bisanhydride (PBA) using
a previously reported procedure.[28] The
subsequent substitution of bromine atoms with 4-tert-butylphenoxy and 4-methoxyphenoxy groups was achieved in high yields
(80–90%) as shown in Scheme . The phenoxy substitution on 1,7-dibromoperylene tetrabutylester 1 was performed in anhydrous dimethylformamide (DMF) at elevated
temperature (115 °C) owing to the low reactivity of the 1,7-dibromoperylene
tetrabutylester toward nucleophilic substitution reactions.[28] For all other derivatives (2, 3, and 4), the reaction was performed under milder
reaction conditions in toluene at temperatures ∼90 °C.[10,29]An isomeric mixture of 1,7-dibromoperylene monoimide monobenzimidazole
compounds (4 + 4′) was obtained by
the reaction between 1,7-dibromoperylene monoimide monoanhydride 7 and 1,2-diaminobenzene in refluxing propionic acid (Scheme ).[30] The thin-layer chromatography (TLC) analysis of this mixture
revealed two slightly separated spots corresponding to 4 and 4′. Efforts to separate the two regioisomers
by column chromatography, however, were not successful. The presence
of two isomers was also evident from the 1H NMR spectrum,
in which two sets of signals in the aromatic region are clearly visible
(Figure ). These signals,
corresponding to the perylene core protons H8, H8′ and H11, H11′, were very well-resolved.
On the basis of the relative intensities of these signals, surprisingly,
the two regioisomers (4 and 4′) were
found in a ratio of ca. 2:1. The obtained ratio is rather surprising,
because we cannot deduct differences in electron density of both anhydride
carbonyl in compound 7, based on resonance structures.
Thus, the reactivity of both anhydride carbonyl moieties is expected
to be identical. For the synthesis of tetrachlorobisimidazoles, both
1:1[31] and 2:1[32] isomeric mixtures have been reported. The assignment of the signals
(H8, H8′ and H11, H11′) to the individual regioisomers was done based on 1H–1H COSY, and by the direct comparison of 1H NMR spectrum of (4 + 4′) with the spectrum of 1,7-dibromoperylene bisimide 3 (Figure ). The ring
current effect of the additional aromatic benzimidazole moiety was
a decisive argument for explaining changes in the chemical shifts.
Scheme 2
Synthesis of 4-Methoxyphenyl Functionalized Derivatives 2c and 3c
Figure 1
Comparison between 1H NMR spectra of compound 4 + 4′ and 1,7-dibromoperylene bisimide 3.
Comparison between 1H NMR spectra of compound 4 + 4′ and 1,7-dibromoperylene bisimide 3.When comparing the 1H NMR spectra of compounds 3 and 4 + 4′, the chemical
shifts for the perylene core protons H2 and H5, in the “left” imide part of these compounds, are
expected to be very similar. Indeed, protons H2 and H5 have identical chemical shifts in compounds 3 and 4 + 4′. Placement of the imidazole
moiety on the “right” part of the molecule should effect
the chemical shifts of protons H8 and H11, upon
going from 3 to 4 or 4′, but to a different extent. A larger shift is expected for the proton
H11 in compound 4, whereas the imidazole placement
in compound 4′ should have a larger effect on
the chemical shift of proton H8′. The predicted
shifts are clearly visible in the 1H NMR spectrum depicted
in Figure , in which
the proton assignment is shown.The two compounds 2c and 3c, containing
4-methoxyphenyl moiety at the imide position, were synthesized to
investigate photoinduced CT from substituents attached to the imide
position of perylene tetracarboxylic acid derivatives 2 and 3. The synthesis was performed in two steps from
their corresponding mono-anhydride precursors 5 and 7, respectively. In the first step, imidization was performed
with 4-methoxyaniline in refluxing propionic acid to afford corresponding
imides 6 and 8.[29] Thereafter, nucleophilic substitution of bromine atoms with 4-tert-butylphenol yielded the desired products 2c and 3c in good yields.
Electrochemical Studies
The redox properties of compounds 1–4 were investigated by cyclic voltammetry
in dichloromethane. The obtained redox potentials (V vs Fc/Fc+) for these molecules are summarized in Table .
Table 1
First Redox Potentials
of Perylene
Derivatives (V vs Fc/Fc+) Obtained by Cyclic Voltammetry
in CH2Cl2
compound
E1/2 ox
E1/2 red
1
–1.55
1a
+0.84
a
1b
+0.82
a
2a
+0.95
–1.38b
2b
+0.94
–1.38
2c
+0.97
–1.33
3a
+1.05
–1.11
3b
+1.04
–1.10
3c
+1.06
–1.09
4a
+1.01
–1.06
4b
+1.02
c
No reduction potential was observed.
Irreversible.
Not detectable.
No reduction potential was observed.Irreversible.Not detectable.As shown
in Table , the redox
properties of the molecules change significantly if the
substitution at the peri-positions is altered. When the groups attached
to peri positions become more electron-withdrawing (e.g., from tetraester
to monoimide), the redox potentials of the compounds become more positive.[32,33] This clearly shows that molecules have higher electron affinities
going from compound 1 to 2 to 3, which makes them better electron acceptors. From the data in Table , it is clearly seen
that the perylene tetracarboxylic derivatives 3 and 4 are rather similar as far as their electronic properties
are concerned. This implies that the imide and benzimidazole groups
are electrochemically equivalent.[32] Finally,
it is apparent that attaching different phenoxy groups at the bay
positions does not result in notably different redox potentials. This
indicates the absence of significant interaction between these groups
in the ground state.
Steady-State Absorption Studies
The absorption spectra
of compounds 1–4, in chloroform,
are shown in Figure , and the relevant data, in toluene, chloroform, and acetonitrile
(or benzonitrile), are given in Table . All compounds are readily soluble in toluene and
chloroform. However, the solubility in polar and weakly polarizable
acetonitrile was much lower. Especially, the compounds 4a and 4b were insoluble in this solvent. At low solubility,
perylene derivatives tend to aggregate.[34] This aggregation alters the optical properties and optoelectronic
performances. In general, spectral broadening and shifts in absorption
and emission spectra, along with fluorescence quenching, are the common
signatures of this aggregation.[35,36] Therefore, to preclude
spectral changes caused by aggregation, benzonitrile was used as a
polar solvent for compounds 3 and 4.
Figure 2
Normalized
UV/vis absorption (left) and emission spectra (right)
of the compounds 1–4b in chloroform.
Table 2
Optical Properties
of Compounds in
Toluene, Chloroform, Acetonitrile/Benzonitrile
compound
solvent
λabs (nm)
λem (nm)
ϵ (M–1 cm–1)
ΦFa
τF (ns)b
1a
toluene
475
515
31 500
0.91
4.26
chloroform
475
515
25 600
0.84
4.40
acetonitrile
471
512
24 800
0.90
4.73
1b
toluene
479
515
24 000
0.88
4.25
chloroform
478
517
29 300
0.81
4.38
acetonitrile
479
517
33 200
0.02
∼0.21c
2a
toluene
515
552
38 900
0.85
4.52
chloroform
517
557
36 700
0.87
4.82
acetonitrile
512
563
31 700
0.90
5.23
2b
toluene
520
555
34 300
0.85
4.34
chloroform
522
561
36 000
0.32
3.21
acetonitrile
517
566
34 100
0.03
∼0.08c
2c
toluene
513
549
35 900
0.93
4.36
chloroform
519
563
36 900
0.87
4.73
acetonitrile
511
558
34 700
0.92
4.69
3a
toluene
543
572
57 800
0.94
4.44
chloroform
547
578
54 200
0.91
4.64
benzonitrile
552
586
54 600
0.86
4.47
3b
toluene
549
575
53 300
0.19
∼0.71c
chloroform
551
580
53 100
0.04
∼0.43c
benzonitrile
561
583
51 400
0.01
∼0.12c
3c
toluene
542
572
52 500
1.00
3.80
chloroform
548
577
51 000
0.87
3.89
benzonitrile
555
582
50 900
0.63
3.30
4a
toluene
578
607
63 600
0.71
4.42
chloroform
581
614
63 700
0.66
4.31
benzonitrile
584
619
61 350
0.70
4.22
4b
toluene
582
609
63 300
0.75
4.22
chloroform
584
616
67 600
0.23
2.45
benzonitrile
591
621
69 500
0.04
∼0.43c
Fluorescence
quantum yield.
Fluorescence
lifetime.
Non-monoexponential
decay.
Normalized
UV/vis absorption (left) and emission spectra (right)
of the compounds 1–4b in chloroform.Fluorescence
quantum yield.Fluorescence
lifetime.Non-monoexponential
decay.The absorption spectra
of all donor-substituted compounds (1b–4b) are characterized by a strong absorption
band at longer wavelengths (425–625 nm) and a weaker absorption
band at shorter wavelengths (Figure ). As shown previously in literature, bay substitution
leads to a disappearance of the pronounced vibronic structure observed
for perylenes without bay substitution. This is accompanied by a bathochromic
shift of the absorption bands.[29,37] When the size of the
π-system increased, that is, going from compounds 1 to 2 to 3 and 4, the molar
extinction coefficient increases gradually, and the absorption maxima
shift to longer wavelengths. When the bay substituent attached to
the perylene core is changed from tert-butylphenoxy
to 4-methyoxyphenoxy is changed, small 5 nm red shifts are observed.
The influence of solvent polarity on the absorption maxima is rather
modest. Positive solvatochromism, a red shift in absorption upon increasing
the solvent polarity, was observed, in particular, for compounds with
more electron-deficient perylene cores, but these spectral shifts
do not exceed 15 nm.
Steady-State and Time-Resolved Emission Studies
The
emission spectra of compounds 1–4 roughly resemble the mirror images of the corresponding absorption
spectra (Figure ).
The positions of the emission wavelengths exhibit the same trend as
those of the absorption maxima (Table ). While the effects of changing the bay substituents
and solvent polarity on the emission wavelengths of these perylene
compounds are modest, the emission intensities, quantified by their
fluorescence quantum yields (ΦF), are extremely sensitive
to these parameters. Fluorescence quantum yields close to unity with
fluorescence lifetimes (τF) in the 4–5 ns
range are observed for compounds bearing the non-electron-donating tert-butylphenoxy substituents at the bay positions (compounds 1a–4a, Table ).[29] These fluorescent
properties are similar to those of non-bay-substituted perylenes;
that is, no significant fluorescence quenching occurs from the 4-tert-butylphenoxy substituents. Note that the high fluorescence
of compound 4a in toluene is remarkable, because fluorescence
quantum yields of perylene benzimidazoles are, in general, substantially
lower as compared to perylene bisimides.[32]For the compounds bearing the electron-donating 4-methoxyphenoxy
substituents at the bay positions (compounds 1b–4b), fluorescence quantum yields gradually decreased with
the increase in solvent polarity and electron deficiency of the perylene
core. The effect of solvent polarity is clearly illustrated by compound 2b that has strong fluorescence in toluene (ΦF = 0.75) but shows negligible fluorescence in acetonitrile (ΦF = 0.03). The effect of the increased electron deficiency
of the perylene core is clearly illustrated by the weak fluorescence
found for compound 3b in all solvents. These observations
suggest that quenching of perylene fluorescence in these compounds
is induced by photoinduced CT, although other quenching mechanisms
cannot be excluded.[38]To establish
whether the quenching depends on the position at which
the electron-donating substituent is attached to the perylene core,
the optical properties of the bay-substituted compounds 2b and 3b are compared to the corresponding imide-substituted
compounds 2c and 3c. The fluorescence of
the bay-substituted compounds 2b and 3b is
much weaker compared to the compounds 2c and 3c. This is clearly seen by comparing the fluorescence of compound 2b with that of compound 2c. While the fluorescence
of 2b strongly decreases upon increasing the solvent
polarity, compound 2c remains strongly fluorescent in
all solvents. A similar observation is made by comparing the fluorescence
of compounds 3b and 3c. Note that ascribing
the differences in photophysical properties between 2b and 2c, and 3b and 3c solely
to the positioning of the electron donor is not entirely valid. This
is mainly because the number of electron-donating substituents is
different in both cases, and the oxidation potential of the 4-methoxyphenoxy
bay substituent is ca. 0.30 V lower than that of the methoxyphenylimide substituent.[39] However, since it
has been previously shown that 4-methoxyphenyl substituents at all
bay positions strongly quench the fluorescence of PBIs,[26] it can still be concluded that fluorescence
quenching from bay position is substantially faster than from imide
position. This conclusion is further supported by a previous report,[40] in which we observed that the fluorescence quenching
of perylene tetraester by an aniline electron donor is substantially
faster from the bay position as compared to the peri-position.Time-resolved fluorescence spectroscopy reveals that the fluorescence
of the strongly emitting compounds (ΦF > 0.2)
decays
monoexponentially. Additionally, the emission of these compounds is
not significantly influenced by the presence of oxygen. Using the
fluorescence quantum yields and the fluorescence lifetimes, the rates
of fluorescence and of nonradiative decay (quenching by CT) were calculated
and summarized in Table S1 (Supporting Information). From this table it is evident that upon increasing the solvent
polarity, lifetimes and rates of fluorescence decrease for all compounds.
Rates of fluorescence between 2.5 and 1 × 108 s–1 were determined for all compounds, and these rates
do not appear to be influenced by the bay substituents. Quenching
rates are in the order of 1 × 107 s–1 for the nonquenched compounds. For the strongly quenched compounds,
rates of quenching (and fluorescence) cannot be determined accurately,
because fluorescence decay is no longer monoexponential. Nevertheless,
CT rates are estimated to be in the order from 1 × 109 to 1 × 1010 s–1.
Transient Absorption
Spectroscopy
To investigate the
time-resolved photophysics in more detail, we selected two series
of compounds (2a–c and 3a–c) for which femtosecond pump–probe transient
absorption spectroscopy measurements were performed. In these series,
the molecules have different substitution patterns, nearly identical
absorption spectra, and markedly different rates of fluorescence quenching
in polar solvents. The transient absorption spectra were measured
in either acetonitrile (2a–2c) or
benzonitrile (3a–3c) using pump wavelengths
between 510 and 550 nm. The transient absorption spectra for compounds 2a and 2b, and 3a and 3b, immediately after excitation are shown in the inset in Figures and 4, respectively. These transient spectra are very similar to
previously reported spectra with pronounced excited-state absorption
features.[10,19,24,41] For the monoimide compounds (2a,b,c) ground-state bleaching below 520 nm, stimulated
emission between 520 and 620 nm, and a broad excited-state absorption
with two maxima near 685 and 800 nm are observed. For the bisimide
compounds (3a,b,c) similar
induced emission and absorption features are observed, but now the
excited-state absorptions are shifted to longer wavelengths (710 and
>900 nm). The spectra of 2c and 3c are
depicted
in Figure S5 in the Supporting Information. It is interesting that the spectra for compounds 2a and 2b and those of 3a and 3b are indistinguishable, even though very large differences in the
radiative lifetime and fluorescence quantum yields were observed.
Figure 3
Kinetic
traces at photoinduced absorption (685 nm) of molecules 2a [a] and 2b [b] in acetonitrile. The transient
absorption spectrum immediately after excitation (inset).
Figure 4
Kinetic traces at photoinduced absorption (775 nm) of
molecules 3a [a] and 3b [b] in benzonitrile.
The transient
absorption spectrum immediately after excitation (inset).
Kinetic
traces at photoinduced absorption (685 nm) of molecules 2a [a] and 2b [b] in acetonitrile. The transient
absorption spectrum immediately after excitation (inset).Kinetic traces at photoinduced absorption (775 nm) of
molecules 3a [a] and 3b [b] in benzonitrile.
The transient
absorption spectrum immediately after excitation (inset).The identical photoinduced absorption spectra immediately
after
excitation (at 1 ps) indicate that the nature of the excited states
is the same in both cases. However, the lifetimes of the excited states
are much shorter for 2b and 3b than they
are for 2a and 3a, respectively. To determine
the lifetime of the singlet excited state of 2a–2c and 3a–3c we performed
a global analysis. When we compared the lifetime of the singlet excited
state with the fluorescence lifetime for all compounds in polar solvent,
we see that these lifetimes are very close to the fluorescence lifetimes
for all the compounds (Table ).
Table 3
Comparison of the Lifetimes of S1
State Obtained from the Global Analysis of Transient Spectrum (τTA) and Fluorescence Lifetimes (τF) Obtained
from Time-Resolved Emission Measurements in Acetonitrile or Benzonitrile
compound
τTA (ns)
τF (ns)
2a
5.23
5.23
2b
0.04
0.08
2c
4.53
4.69
3a
4.51
4.47
3b
0.04
0.12
3c
4.81
3.30
The data presented
so far are in accordance to the expected photophysical
behavior of 2a–2c and 3a–3c. For 2a and 2c,
a very slow decay of the singlet excited state is observed on a nanosecond
time scale. Similar lifetimes were observed by transient absorption
and emission spectroscopy. However, for compound 2b,
a 100-fold increased decay rate of the S1 state is observed.
Similarly, for 3b, a significantly increased decay rate
of the S1 state is observed, which is indicative of the
occurrence of a substantially faster decay process. An explanation
that is often invoked for such observations is the formation of a
charge-separated state that is stabilized in polar solvents. The proposed
scheme for such a photophysical behavior is depicted in Figure .
Figure 5
Schematic representation
of photoinduced processes after photoillumination.
Schematic representation
of photoinduced processes after photoillumination.Although the initial excited state disappears,
it is remarkable
that we do not observe the characteristic absorption spectrum of the
perylene radical anion of the CS state D+.–A–.–D. For related compounds, CS states have been
observed upon excitation,[27] but on some
occasions spectroscopic evidence of charge separation is illusive.[18,40] The absence of a CS absorption can be explained in a straightforward
manner by assuming that charge recombination is faster than charge
separation, which prevents accumulation of the CS state. For compounds 2b and 3b this implies that charge recombination
rates are at least from 1 × 109 to 1 × 1010 s–1, respectively (Table S1)
Molecular Simulations
To gain more
insight of the nature
of the initial excited state in the studied compounds, we performed
DFT calculations. The excitations of compounds 2a and 2b were calculated by TD-DFT using a DZP basis set consisting
of Slater-type function and a M06-2X exchange-correlation function.
All calculations were performed using the Amsterdam Density Functional
theory package. The calculated absorption spectra of compounds 2a and 2b show a strong absorption feature with
an oscillator strength close to 0.8 at 480 nm (Figure ). In both cases, these absorptions mainly
consist of the transition from highest occupied molecular orbital
of perylene (HOMOperylene) to lowest unoccupied molecular
orbital of perylene (LUMOperylene). The computational transition
energies are somewhat higher than those observed experimentally. This
is attributed to the absence of solvent effects in the calculations
that generally shift the absorption bands to lower energy.
Figure 6
Optical excitation
of 2a (top) and 2b (bottom) calculated using
TD-DFT with DZP/M06-2X.
Optical excitation
of 2a (top) and 2b (bottom) calculated using
TD-DFT with DZP/M06-2X.In the calculated spectrum of 2a, there is an
additional
absorption near 345 nm, which has transition from the HOMO of bay
substituents to the LUMO of perylene core. For 2b, multiple
higher-lying bands are observed between 300 and 420 nm. All of these
bands contain substantial contributions from the CT transitions from
occupied orbitals of the substituents to the LUMO of the perylene
core. These calculations show that for both compounds there is no
clear low-energy CT state present in vacuum. However, note that the
nature of the excited states is not necessarily the same in solution.
First of all, the excited states with (partial) CT character will
be stabilized considerably in highly polar solvents such as acetonitrile
and benzonitrile and, therefore, arise much closer to the local excited
state localized on the perylene core. From the calculations presented
here, it can be seen that for 2b the excited charge-separated
states are lower in energy than for 2a, which can be
understood in terms of the stronger electron-donating character of
the substituents in 2b. Second, the presence of a polar
solvent can also change the nature of the excited state considerably
after excitation. This can result in the formation of a CT state that
is not present in vacuum.The results from the molecular simulations
are in line with the
experimental data obtained by TA and fluorescence spectroscopy. These
experimental data reveal the formation of identical “locally
excited states” for all compounds of the same class, irrespective
of the electron-donating substituent attached. Subsequently, fluorescence
takes place for compounds bearing weak donors in all solvents, while
strong fluorescence quenching takes place for compounds bearing strong
donors in polar solvents. The fluorescence quenching takes place by
electron transfer from the electron donor to the perylene core. This
process is thermodynamically favored and, from bay-attached electron
donors, kinetically allowed. This charge-separation process occurs after the primary excitation process and is therefore not
described by the molecular simulations based on DFT calculations.
Conclusions
We have synthesized a series of perylene tetracarboxylic
acid derivatives,
bearing electron-donating 4-methoxyphenoxy groups at 1,7-bay positions
and, in two cases, also a 4-methoxypenyl group at the imide position.
Subsequent photophysical characterization of these compounds revealed
the various variables that dictate the CT process in perylene-based
systems; electronic nature of the perylene core, the position of electron
donor, and the solvent polarity. For the perylene tetraester-based
compound, which has the least electron-deficient perylene core, CT
was observed only in polar acetonitrile. Upon moving to perylenemonoimide
diester, which has an increased electron deficiency due to presence
of a more electron-withdrawing imide group, significant CT is observed
already in chloroform. An efficient CT occurred in both polar and
nonpolar solvents for the most electron-deficient perylene bisimide
based compounds. From transient absorption spectroscopy and DFT calculations,
it has been concluded that charge separation takes place after local
excitation of the perylene core. The kinetics of CT is strongly influenced
by the positioning of the electron-donor on the perylene scaffold.
Changing position from “bay” to “imide”
exerted a significantly negative impact on the CT rates. In this way,
this study has revealed that the photoinduced CT process can be precisely
tuned in perylene-based systems by altering the electronic nature
of the perylene core, the positioning of the electron donor, and the
solvent polarity.
Experimental Section
Materials
All
the reagents utilized in the synthesis
were purchased from commercial suppliers, unless otherwise stated.
The DMF used in the synthesis was of anhydrous grade. Toluene was
dried over sodium under an argon atmosphere prior to use. All other
solvents used in the syntheses were of reagent grade and were used
as received from suppliers. The purifications of the products were
performed by column chromatography (silica gel 60, mesh size 0.063–0.200
mm). For all the spectroscopic measurements, spectroscopy-grade solvents
were purchased from commercial suppliers and were used as received.
Instrumentation and Characterization
The NMR spectra
were recorded with 400 MHz pulsed Fourier transform NMR spectrometer
in CDCl3 at room temperature. The chemical shifts are quoted
relative to tetramethylsilane (TMS). δ values are given in parts
per million, and J values are in hertz. Electrochemical
behavior of the compounds was studied by cyclic voltammetry in a three-electrode
single-compartment cell consisting of a platinum sheet as the working
electrode, Ag wire as the reference electrode, and a Pt wire as the
counter electrode (scan rate = 0.5 V/s). Predried CH2Cl2 containing 0.1 M tetrabutylammonium hexafluorophosphate was
used as solvent. The measurements were done under continuous flow
of nitrogen. The concentration of the prepared samples was ca. 0.5
mM. Under these conditions, the ferrocene oxidation was observed at
0.52 V.Absorption measurements were performed in PerkinElmer
Lambda 40 UV–vis spectro-photometer. Photoluminescence studies
were done in SPEX Fluorimeter. Fluorescence lifetimes were performed
with LifeSpec-ps Fluorescence spectrometer with fixed excitation wavelength
of 400 nm. For quantum yield measurements, the formula for optically
dilute solutions was used.[42] Fluorescence
quantum yields of compounds 1–2 were
determined by using perylene-3,4,9,10-tetracarboxylic tetrabutylester
(ϕF = 0.98 in CH2Cl2) as a
reference, whereas, for compounds 3–4, N,N′-bis(1-hexylheptyl)-perylenebisimide (ϕF = 0.99 in CH2Cl2) was used.[43]Pump–probe
transient-absorption measurements were performed
by using tunable Yb:KGW laser system consisting of a YB:KGW laser
(1028 nm), which operates at 5 kHz with a pulse duration of less than
180 fs (PHAROS-SP-06–200 Light Conversion) and an optical parametric
amplifier (ORPHEUS-PO15F5HNP1, Light Conversion). A white light continuum
probe pulse was generated by focusing part of the fundamental 1028
nm from Pharos into a sapphire crystal. Transient absorption data
were collected using a commercial pump–probe spectrometer,
HELIOS (Ultrafast Systems) in the wavelength range of 490–910
nm. The maximum time-delay between the pump and the probe pulse was
3.3 ns. The compounds were dissolved in spectroscopic grade toluene,
chloroform, and acetonitrile/benzonitrile and placed in quartz cuvettes
with a 2 mm path length. To prevent aggregation and photobleaching,
the samples were stirred with a magnetic stirrer.The geometrical
and optical properties of the chromophores were
investigated by DFT calculations using the Amsterdam Density Functional
(ADF) software package. The geometry of the molecules was optimized
using the PBE functional together with a double-ζ plus polarization
(DZP) type basis set consisting of Slater functions. The optical absorption
spectra were calculated by TD-DFT theory calculations using the M06-2X
meta-GGA functional with a DZP basis set.
Synthesis of 1,7-Di(4-tert-butylphenoxy)perylene-3,4,9,10-tetracarboxy
Tetrabutylester (1a)
In a 25 mL round-bottomed
flask, weighed amounts of 1,7-dibromoperylene tetrabutylester 1 (200 mg, 0.25 mmol), 4-tert-butylphenol
(148 mg, 0.99 mmol), and Cs2CO3 (485 mg, 1.49
mmol) were taken. Subsequently, anhydrous DMF (8 mL) was added. The
reaction mixture was stirred at 115 °C for 3 h under argon atmosphere.
After the mixture cooled to room temperature, CH2Cl2 (50 mL) was added to the reaction mixture, and the resultant
solution was washed with water several times. The organic layer was
collected and evaporated. The crude product was chromatographed with
dichloromethane (DCM) to afford
the desired product 1a (199 mg, 85%). Later, it was recrystallized
from refulxing EtOH. 1H NMR (400 MHz, CDCl3):
δ = 9.08 (d, J = 8.0 Hz, 2H), 7.98 (d, J = 8.0 Hz, 2H), 7.73 (s, 2H), 7.39 (d, J = 8.0 Hz, 4H), 7.01 (d, J = 8.0 Hz, 4H), 4.29 (t, J = 6.8 Hz, 4H), 4.23 (t, J = 6.8 Hz, 4H),
1.78–1.70 (m, 4H), 1.69–1.62 (m, 4H), 1.50–1.33
(m, 4H), 1.41–1.30 (m, 4H), 1.33 (s, 18H), 0.96 (t, J = 6.8 Hz, 6H), 0.89 ppm (t, J = 6.8 Hz,
6H). 13C NMR (100 MHz, CDCl3): δ = 168.5,
167.8, 153.3, 152.2, 147.0, 132.0, 131.2, 129.4, 129.1, 127.1, 127.0,
124.7, 124.3, 122.5, 118.3, 65.3, 65.2, 34.4, 31.4, 30.6, 30.4, 19.2,
19.1, 13.8, 13.7 ppm.
Synthesis of 1,7-Di(4-methoxyphenoxy)perylene-3,4,9,10-tetracarboxy
Tetrabutylester (1b)
Synthesis of N-(2,6-Diisopropylphenyl)-1,7-dibromoperylene-3,4,9,10-tetracarboxy
Monoimide Monobenzimidazole (4 + 4′)
1,7-dibromo perylene monoimide monoanhydride 7 (50 mg, 0.07 mmol) and 1,2-diaminobenzene (10 mg, 0.09 mmol) were
taken in propionic acid (10 mL). The mixture was refluxed for 3 h.
After the mixture cooled to room temperature, it was poured into water
to precipitate the crude product. The precipitate was filtered off
and washed with several portions of water to remove all the propionic
acid. The precipitate was dried and chromatographed on silica-60 eluting
with DCM to afford the pure product (48 mg, 87%) as the mixture of
two regioisomers 4 and 4′ in a ratio
ca. 2:1. 1H NMR (400 MHz, CDCl3): δ =
9.60–9.50 (m, 2H), 9.22 (s, 0.35H), 9.11 (s, 0.65H), 8.99 (s,
1H), 8.94 (d, J = 8.0 Hz, 0.65H), 8.90 (d, J = 8.0 Hz, 0.35H), 8.78 (d, J = 8.0 Hz,
1H), 8.56–8.51 (m, 1H), 7.95–7.90 (m, 1H), 7.56–7.47
(m, 3H), 7.35 (d, J = 8.0 Hz, 2H), 2.79–2.70
(m, J = 6.8 Hz, 2H), 1.22–1.16 ppm (m, 12H). 13C NMR spectra could not be measured because of its low solubility.
Synthesis of N-(2,6-Diisopropylphenyl)-1,7-di(4-tert-butylphenoxy)perylene-3,4,9,10-tetracarboxy Monoimide
Monobenzimidazole (4a)
Synthesized from 4-tert-butylphenol (59 mg, 0.39 mmol), K2CO3 (108 mg, 0.78 mmol), 18-Crown-6 (206 mg, 0.78 mmol), and
1,7-dibromoperylene monoimide monobenzimidazole 4 (100
mg, 0.13 mmol) in dry toluene (25 mL) according to the procedure described
for compound 2a. The crude product was chromatographed
using silica-60/CHCl3 to afford compound 4a (95 mg; 80%) as the mixture of two regioisomers. 1H NMR
(400 MHz, CDCl3): δ = 9.68–9.52 (m, 2), 8.80–8.74
(m, 1H), 8.64–8.58 (m, 1.45 H), 8.52 (s, 0.55H), 8.49–8.45
(m, 0.60H), 8.42–8.36 (m, 1.50H), 7.83–7.75 (m, 1H),
7.51–7.38 (m, 7H), 7.30 (d, J = 7.6 Hz, 2H),
7.17–7.09 (m, 4H), 2.77–2.73 (m, 2H), 1.39–1.34
(m, 18H), 1.17–1.14 ppm (m, 12H). 13C NMR spectrum
could not be measured because of its low solubility.
Synthesis
of N-(2,6-Diisopropylphenyl)-1,7-di(4-methoxyphenoxy)perylene-3,4,9,10-tetracarboxy
Monoimide Monobenzimidazole (4b)
Synthesized
from 4-methoxyphenol (48 mg, 0.39 mmol), K2CO3 (108 mg, 0.78 mmol), 18-Crown-6 (206 mg, 0.78 mmol), and 1,7-dibromoperylenemonoimide monobenzimidazole 4 (100 mg, 0.13 mmol) in
dry toluene (30 mL) according to the procedure described for compound 2a. The crude product was chromatographed using silica-60/CHCl3 to afford compound 4b (96 mg, 86%) as the mixture
of two regioisomers. 1H NMR (400 MHz, CDCl3):
δ = 9.68–9.52 (m, 2H), 8.72 (d, J =
8.4 Hz, 1H), 8.65–8.55 (m, 1H), 8.50 (s, 0.55H), 8.41 (s, 0.45H),
8.40–8.29 (m, 2H), 7.77–7.71 (m, 1H), 7.46 (t, J = 8.0 Hz, 1H), 7.41–7.35 (m, 2H), 7.31 (d, J = 8.0 Hz, 2H), 7.22–7.13 (m, 4H), 7.08–6.94
(m, 4H), 3.89–3.83 (m, 6H), 2.77–2.73 (m, 2H), 1.19–1.13
ppm (m, 12H). 13C NMR spectrum could not be measured because
of its low solubility.
Synthesis of N-(4-Methoxyphenyl)-1,7-dibromoperylene-3,4,9,10-tetracarboxy
Monoimide Dibutylester (6)
A 25 mL round-bottomed
flask was charged with 1,7-dibromoperylene monoanhydridedibutylester 5 (150 mg, 0.22 mmol), 4-methoxyaniline (35 mg, 0.29 mmol),
and propionic acid (6 mL). The reaction mixture was refluxed for 24
h. After it cooled to room temperature, the reaction mixture was poured
into the water to precipitate the crude product. The precipitate was
filtered off and washed with several portions of water to remove all
the propionic acid. The precipitate was dried and chromatographed
on silica, eluting with CH2Cl2, to afford the
desired product 6 (140 mg, 81%). 1H NMR (400
MHz, CDCl3): δ = 9.24 (d, J = 8.0
Hz, 1H), 9.21 (d, J = 8.0 Hz, 1H), 8.89 (s, 1H),
8.68 (d, J = 8.0 Hz, 1H), 8.34 (s, 1H), 8.13 (d, J = 8.0 Hz, 1H), 7.24 (d, J = 8.0 Hz, 2H),
7.08 (d, J = 8.0 Hz, 2H), 4.35 (t, J = 6.8 Hz, 4H), 3.88 (s, 3H), 1.84–1.75 (m, 4H), 1.53–1.46
(m, 4H), 1.00 ppm (t, J = 7.2 Hz, 6H). 13C NMR (100 MHz, CDCl3): δ = 167.7, 166.9, 166.8,
163.5, 162.95, 162.91, 159.7, 138.0, 136.8, 134.2, 133.7, 132.0, 131.9,
131.6, 130.8, 130.5, 130.4, 130.3, 129.6, 129.5, 129.1, 129.0, 128.2,
128.13, 128.11, 127.3, 127.0, 126.9, 122.2, 122.1, 120.3, 119.4, 114.8,
66.0, 65.8, 55.5, 30.6, 30.5, 19.3, 19.2, 19.1, 13.8, 13.7 ppm.
Synthesis of N-(4-Methoxyphenyl)-1,7-di(4-tert-butylphenoxy)perylene-3,4,9,10-tetracarboxy Monoimide
Dibutylester (2c)
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