X. Shao et al.
Dyes and Pigments 188 (2021) 109198
aniline (0.28 g, 3.03 mmol), 8-(benzyloxy)quinoline-2-carbaldehyde
(0.53 g, 2.02 mmol), ammonium acetate (NH4OAc, 1.09 g, 14.12 mmol),
and acetic acid (HOAc, 10 mL) were added into flask, followed with
refluxed for 12 h under argon (Ar) environment. The reaction solution
was cooled down to room temperature, then deionized water was
poured into flask, then filtered. The residue was purified by column
chromatography on silica gel using ethyl PE/EtOAc at 10:1 by volume as
the eluent to give a white powder with yield of 75.0% (0.80 g): 1H NMR
(400 MHz, CDCl3) δ 8.94 (dd, J = 8.4, 3.6 Hz, 1H), 8.72 (dd, J = 20.4,
8.3 Hz, 2H), 8.54 (d, J = 8.6 Hz, 1H), 8.16 (d, J = 8.6 Hz, 1H), 7.82–7.72
(m, 1H), 7.70–7.58 (m, 3H), 7.53–7.44 (m, 1H), 7.45–7.15 (m, 11H),
7.07 (dd, J = 8.3, 1.3 Hz, 1H), 6.85 (dd, J = 7.3, 1.6 Hz, 1H), 5.21 (s,
2H). 13C NMR (101 MHz, CDCl3) δ 154.63, 149.48, 148.37, 139.75,
139.56, 137.56, 137.28, 136.20, 129.76, 129.54, 129.33, 129.23,
128.82, 128.74, 128.58, 128.52, 127.88, 127.36, 127.26, 127.05,
126.35, 125.78, 125.23, 124.05, 123.26, 123.20, 122.83, 122.52,
121.54, 119.57, 110.34, 70.28. Found C, 84.09; H, 4.56; N, 8.63%;
molecular formula C37H25N3O; requires C, 84.23; H, 4.78; N, 7.96%.
intramolecular charge transfer (ICT) band from the phenanthro[9,10-d]
imidazole moiety to the 8-(benzyloxy)quinolin group [24]. The ab-
sorption bands are observed in the range of 300–325 nm approximately
match to the quinoline group π-π* transition [25]. Compare the UV–Vis
absorption spectra of THF solution with that of thin films, the shape and
peak position of QL-PPI are similar. No obvious red-shift of absorption
peaks manifests that no crystallization occurs in the films [26,27].
Notably, as shown in Fig. 2, three peaks located at around 330–406 nm
in absorption spectra are not obvious than that in thin films. The peak at
about 380 nm was redshift to 390 nm and enhanced greatly. This is
owing to the dispersed state of the QL-PPI in solution and the aggrega-
tion state of the QL-PPI in solid film [28]. In the aggregated state, there is
a large molecular interaction between skeleton of the 8-(benzyloxy)
quinolin group or the phenanthro[9,10-d]imidazole moiety, which
changes the absorption peak intensity.
In the THF solution, the QL-PPI exhibits maximum PL (PLmax) value
at deep-blue wavelengths of 421 nm. As shown in Fig. S3, its emission
wavelength red-shifted (429 nm in MeCN solution) with increasing
solvent polarity, implying the emission originating from the ICT state
[29]. The photoluminescence quantum yields (PLQYs) of compound
QL-PPI was tested by using trans-1-(9-anthryl)-2-phenylethene (t-APE,
PLQYs 0.46 in MeCN) as the reference substance, the PLQYs of com-
pound QL-PPI reached 0.77. The full width at half maximum (FWHM) of
the deep-blue spectrum is 58 nm. Nevertheless, the maximum emission
peak in PL spectrum of the QL-PPI in thin film state showed large
red-shift about 34 nm with FWHM of 82 nm, comparing with its PL
spectrum in THF solution. The red-shift of the emission observed in the
film state is probably due to the presence of strong intermolecular in-
teractions or aggregation in film states.
3. Result and discussion
3.1. Synthesis and thermal properties of QL-PPI
The synthesis of QL-PPI is outlined in Scheme 1, involving a series of
hydroxyl protection reaction (benzylation), oxidation reaction and
Debus-Radziszewski reaction (see Experiment section). As described in
Fig. 1, the decomposition temperature (Td, 5% weight loss) value of the
compound QL-PPI was evaluated to be 407 ◦C. The DSC (Fig. 1 insert)
analysis uncovered that the glass transition temperature (Tg) of QL-PPI
was 92 ◦C. Moreover, no distinct crystalline peak was observed at a
temperature beyond Tg. The small molecular compound QL-PPI has
terrific thermodynamic stability due to molecular rigidity. The related
data are listed in Table 1.
To obtain a good understanding on the optical properties in the
molecular level, density functional theory (DFT) calculations (B3LYP/6-
31G(d)) were carried out by using Gaussian 03 software [30]. The
optimized geometry and the electron distribution of the compound
QL-PPI are shown in Fig. 3. The calculation results indicate that the
QL-PPI is not a planar molecule structure. There exists a dihedral angle
of the QL-PPI between benzene ring and imidazole ring and dihedral
angle between benzyloxy and quinoline ring. However, quinoline ring is
coplanar with phenomidazole ring. The HOMO and LUMO orbitals of
the QL-PPI are located on quinoline ring and phenomidazole ring. Thus,
it is suggesting that the QL-PPI shows enhanced absorption peaks
locating at 330–406 nm and more red-shifted emission in the film
comparison to solution, which is consistent with our experimental
results.
3.2. Optical properties and energy levels
The normalized UV–Vis absorption and photoluminescence (PL)
spectra of QL-PPI in THF solution (1 × 10ꢀ 5 M) and thin films (quartz
plate) are shown in Fig. 2, relevant data are summarized in Table 1. In
the THF solution, there are three peaks located at around 330–406 nm in
the UV–Vis absorption spectra of QL-PPI. The absorption peak in the
range of 345 nm can be assigned to the
of 2-imidazole to the imidazole unit. A lower-energy band with peaks at
around 365 and 380 nm can be assigned as the * transition and an
π-π* transition of the substituent
In order to measure the HOMO values of the compound QL-PPI,
cyclic voltammetry (CV) measurements using a three-electrode cell
were conducted (See ESI Fig. S4). The edge of the UV–Vis spectra was
used to calculate the band gap (Eg) of the QL-PPI. The band gaps and the
HOMO and LUMO levels are summarized in Table 1. The HOMO and
LUMO level of the QL-PPI is ꢀ 5.9 eV and ꢀ 2.9 eV, respectively. This
result implies that the QL-PPI is easy to inject an electron in the OLED.
π-π
3.3. Non-doped blue OLED
To investigate the potential application of the compound QL-PPI,
non-doped OLED with the configuration of ITO/NPB (25 nm)/QL-PPI
(40 nm)/TPBi (15 nm)/LiF (1 nm)/Al (100 nm) was fabricated. In this
device, N,N′-Di-1-naphthyl-N,N′-diphenylbenzidine (NPB), QL-PPI, and
1,3,5-tris(1-phenyl-1H-benzimidazol-2-yl)benzene (TPBi) were acted as
the hole-transport layer (HTL), emitting layer (EML) electron-transport
layer (ETL), respectively [31]. LiF was employed as the
electron-injecting layer (EIL) and Al metal served as the cathode [32].
The device configuration and the energy level diagrams of used mate-
rials are shown in Fig. 4.
The electroluminescence (EL) spectrum, current density-voltage-
brightness (J-V-B) characteristics, CE, and PE of the non-doped OLED
device using compound QL-PPI as the emitting materials are shown in
Fig. 1. TGA and DSC thermogram (insert) of QL-PPI.
3