Heterocyclic compounds with effective solid-state luminescence offer a wide range of uses. It has been observed that combining pyrimidine and indole moieties in a single molecule can enhance material behavior dramatically. Here, different heterocyclic compounds with indole and pyrimidine moieties have been synthesized effectively, and their structures have been validated using NMR, IR, and mass spectroscopy. The photoluminescence behavior of two substances was investigated in powder form and solutions of varying concentrations. After aggregation, one molecule displayed a redshifted luminescence spectrum, whereas another homolog showed a blueshift. Thus, density functional theory calculations were carried out to establish that introducing a terminal group allows modifying of the luminescence behavior by altering the molecular packing. Because of the non-planarity, intermolecular interactions, and tiny intermolecular distances within the dimers, the materials demonstrated a good emission quantum yield (Φem) in the solid state (ex. 25.6%). At high temperatures, the compounds also demonstrated a stable emission characteristic.
Heterocyclic compounds with effective solid-state luminescence offer a wide range of uses. It has been observed that combining pyrimidine and indole moieties in a single molecule can enhance material behavior dramatically. Here, different heterocyclic compounds with indole and pyrimidine moieties have been synthesized effectively, and their structures have been validated using NMR, IR, and mass spectroscopy. The photoluminescence behavior of two substances was investigated in powder form and solutions of varying concentrations. After aggregation, one molecule displayed a redshifted luminescence spectrum, whereas another homolog showed a blueshift. Thus, density functional theory calculations were carried out to establish that introducing a terminal group allows modifying of the luminescence behavior by altering the molecular packing. Because of the non-planarity, intermolecular interactions, and tiny intermolecular distances within the dimers, the materials demonstrated a good emission quantum yield (Φem) in the solid state (ex. 25.6%). At high temperatures, the compounds also demonstrated a stable emission characteristic.
Since Tang and Vanslyke
published their outstanding work in 1987,
organic light-emitting devices (OLEDs) have received the researchers’
attention.[1] OLEDs offer a variety of applications[2−5] in storage media,[6] sensors,[7] optics,[8] electronics,[9] and biological science.[10] Emitting materials in most of the lighting systems on the market
are inorganic.[11] While organic emitting
materials were anticipated to be widely used in the future, they seem
not to have been significantly utilized in the industry.[12,13] Compared to inorganic compounds, organic luminescent chromophores
offer superior luminescence characteristics and lower industrial costs.[14]Applications in biology, such as sensors,
biomedical imaging, and
bacterial imaging, benefit from materials with both luminous and antimicrobial
features.[15,16] Recently, solid-state luminous compounds
with antimicrobial effects containing indole[17,18] or pyrimidine[19,20] moieties have been produced.
Furthermore, earlier research has shown that combining two or more
active structural moieties might improve the activity.[21,22] As a result, combining pyrimidine and indole moieties in a single
molecule can dramatically boost biological activity.[23] Several heterocyclic and non-heterocyclic luminogens have
recently been described, and their luminescence was regulated by molecular
aggregation.[24−27]As a response to the challenges outlined above in addition
to what
we have already accomplished,[28−35] we present here a synthetic strategy for several novel indole–pyrimidine
hybrids. Some substances’ photophysical characteristics in
solid and solution forms were investigated. Density functional theory
(DFT) simulations were used to understand the relationship between
the luminescence behavior and molecular structure.
Results and Discussion
Molecular
Design and Characterization
The synthetic
pathway for synthesizing the materials containing both indole and
pyrimidine moieties is depicted in Schemes and 2. As shown in Scheme , The amino carboxamide
derivative (10) was effectively synthesized similar to
our previously published technique with some changes,[17] where compound 10 was prepared by treating
the uncyclized compound 9 with sodium ethoxide as an
organic base rather than its direct formation from the mercaptocarbnitrile
derivative 8.[36,37] Compound 8 was obtained through a series of reactions starting from the formation
of pyrimidine block 4, which was obtained through a multi-component
reaction of 3-chloro-1H-indole-2-carbaldehyde (1), thiourea (2), and ethyl cyanoacetate (3). The obtained compound 10 was then reacted
with different reagents to synthesize the target compounds. Condensation
of 10 with cyclohexanone or triethyl orthoformate in
glacial acetic acid followed by a cycloaddition reaction afforded
the corresponding compounds 11 and 12, respectively.
The synthesized compounds 9–12 were
successfully characterized by IR and NMR spectra. The IR spectrum
of the S-alkylated compound 9 featured
stretching vibration bands at 3455, 3389, and 3317 cm–1 for NH2, 2209 cm–1 for the CN group,
and 1651 cm–1 for the C=O group, whereas
the 1H NMR spectrum exhibited singlet signals at 7.90 and
3.94 ppm belonging to two NH2 groups. Also, the IR spectrum
of compound 11 showed bands at 3162 and 3420 cm–1 for the stretching vibration of the NH and OH tautomer. Meanwhile,
its 1H NMR spectrum showed multiplet signals in the range
of 0.89–1.97 ppm for the 10 aliphatic protons of the cyclohexanone
moiety. In a similar manner, the structure of compound 12 was confirmed by spectral data, where the IR spectrum revealed the
appearance of bands at 3288 cm–1 for NH and 1663
cm–1 for amidic C=O. The 1H NMR
spectrum of substance 12 displayed a singlet signal at
8.12 ppm, which proved the other fused pyrimidine ring formation.
Furthermore, the reaction of compound 10 with chloroacetyl
chloride under a neat condition followed by treatment with sodium
carbonate solution gave the chloromethyl compound 13.
The formation of compound 13 can be explained as follows:
The amino group in C5 of compound 10 was acylated by
chloroacetyl chloride. The amidic NH2 group was then nucleophilically
added to the carbonyl group in the newly acylated NHCOCH2Cl followed by the elimination of a water molecule. The spectral
analyses elucidated that the structure of 13, bands at
3357 and 3472 cm–1 for NH2 groups in
the starting compound 10 disappeared from the IR spectrum.
Also, new bands at 3256 and 3372 cm–1 appeared for
the formed two NH groups. Also, the 1H NMR spectrum exhibited
the disappearance of signals of NH2 groups in compound 10 and the appearance of a new singlet signal at δ =
4.43 ppm for the CH2 group. IR, 1H NMR, and 13C NMR spectra of compounds 9–12 are presented
in the electronic Supporting Information (ESI) as Figures S1–S9.
Scheme 1
Synthetic
Route for Obtaining the Amino Carboxamide (10) and Pyrimidothienopyrimidine
Compounds (11–13)
Scheme 2
Reactions of Indolylpyrmidothienopyrimidine Derivatives 12 and 13
Compound 13 underwent nucleophilic substitution reactions
with primary and secondary amines in dioxane and afforded compounds 14 and 15 (Scheme ). The structures of the obtained compounds were affirmed
based on IR and 1H NMR spectra. The IR spectrum of compound 14 demonstrated stretching vibration bands at 3245 and 3185
cm–1 for NH and 1643 cm–1 for
the C=O group. Similarly, compound 15 demonstrated
bands at 3473 and 3327 cm–1 for the two NH groups
and 1674 cm–1 for the C=O group. Moreover,
the 1H NMR spectrum of 15 exhibited signals
at 2.72, 2.73, 3.78, 3.79, and 3.80 ppm, characteristic of the morpholine
moiety, in addition to the singlet signal at 3.33 ppm for the CH2 group. Furthermore, when compound 12 was treated
with a mixture of phosphorus oxychloride and phosphorus pentachloride,
it delivered the chloropyrimidine derivative compound 16. The latter compound was reacted in dioxane with thiourea to give
the analogous thioxopyrimidine compound 17. The structure
of the obtained compound 16 was confirmed by the IR spectrum
that showed the disappearance of C=O bands in 12. Also, the IR spectrum of compound 17 showed the appearance
of new bands at 3434 and 1268 cm–1, characteristic
of NH and C=S, respectively. Moreover, the compound 171H NMR spectrum displayed a new singlet signal at 14.28
ppm, which belonged to the NH group.The nucleophilic substitution
of the chlorine atom in compound 16 with different nucleophiles
like hydrazine hydrate and
aniline produced hydrazinopyrimidothienopyrimidine (18) and anilinopyrimidiothienopyrimidine (19), respectively.
The IR spectrum of compound 18 showed new absorption
bands at 3287 and 3395 cm–1 for the amino group,
while its 1H NMR spectrum showed a singlet signal at δ
= 4.89 ppm for the NH2 group. When compound 18 was allowed to react with triethyl orthoformate in the presence
of a catalytic amount of acetic acid, it gave compound 9-(p-tolylamino)-7-(3-chloro-1H-indol-2-yl)[1,3,4]triazolo[1″,5″:1′,6′]
pyrimido[4′,5′:4,5]thieno[2,3-d]pyrimidine
(20). Bands at 3202, 3287, and 3395 cm–1 of NH and NH2 groups in the compound 18 IR
spectrum disappeared with 20. The 1H NMR spectrum
of 20 showed the appearance of a singlet signal at δ
= 6.04 ppm for CH pyrazole and the disappearance of the singlet signal
of the NH2 group in 18. On the other hand,
compound 18 reacted with acetylacetone in dioxane to
produce compound 4-(3,5-Dimethylpyrazol-1-yl)-7-morpholino-9-phenylpyrimido
[4′,5′:4,5]thieno[2,3-d]pyrimidine
(21). The IR spectrum of compound 21 exhibited
the disappearance of NH and NH2 bands in 18. There were two singlet signals at δ = 2.38 and 2.75 ppm in
the 1H NMR spectrum for 2CH3 groups, as well
as a singlet signal at 6.28 ppm, which indicated the synthesis of
the pyrazolyl ring in compound 21. IR, 1H
NMR, 13C NMR, and mass spectra of compounds 13–21 are presented in the ESI as Figures S10–S37.
Quantum-Chemical Computations
DFT calculations were
presented to reveal the structures of molecules 11 and 12 and their dimers. Calculations were carried out on compounds 11 and 12 exclusively since the former emits
in both the solid and solution phases, while the latter exhibits blueshifted
emission after aggregation. A 46.6° dihedral angle between the
indole and pyrimidine rings of molecule 11 is seen in Figure a, while molecule 12 (Figure b) has a dihedral angle of 16.2°. Figure c,d shows the dimers of molecules 11 and 12, respectively. The most stable dimer structures
were chosen from a variety of binding modes. The structures in Figure c,d are dominated
by π–π stacking. Dimerization of molecule 11 results in a binding energy of −35.4 kcal/mol, whereas
that of molecule 12 is 43.4 kcal/mol. These high binding
energies indicate that the dimers of 11 and 12 are stable. Within these dimers, the average intermolecular distance
was found less than 3.3 Å. This proximity prohibits the rings
from rotating around single bonds. To elucidate the electron distribution
in molecules 11 and 12, their highest occupied
molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO)
along with their energies computed with the B3LYP-D3BJ/6-31+G(d,p)
level of theory (Figure e,f). From these calculations, we may gain intensive information
regarding the orbital distribution. Both HOMO and LUMO spread on the
complete molecule (for both 11 and 12).
The computed band gaps in 11 and 12 were
3.32 and 3.20 eV, respectively. The critical changes in structural
parameters of the monomers and dimers are shown in Figure a,b. The structural shifts
between the excited and ground states of the dyes were estimated to
illustrate their aggregation-induced emission feature. At the same
level of theory, the structure of the initial excited state was optimized.
The key structural differences between the excited and ground states
of molecules 11 and 12 are depicted in Figure c,d. In general,
we noticed a greater deviation from planarity in the excited state,
and the rings are more twisted. The maximum absorption wavelengths
(λabs) of the studied compounds 11 and 12 computed with B3LYP/6-31+G(d,p) for the monomers and dimers
are presented in Figure S38 (ESI).[38−46] The energy gaps of 3.32 and 3.20 eV between the HOMO and LUMO of
compounds 11 and 12 gave λabs = 381 and 479 nm for monomers as compared to 376 and 515 nm for
dimers, respectively. The monomers and dimers exhibited several absorption
bands, the short-wavelength bands can be attributed to the delocalized
π–π* transitions, while absorptions at the long
wavelengths may result from the prolonged conjugation along the molecule.
Figure 1
(a) 11 and (b) 12 geometry of the ground
state. (c) 11 and (d) 12 geometry of the
most stable dimers optimized using B3LYP-D3BJ/6-31+G(d,p). For both
dimers, specific intermolecular distances between some atoms and the
center of the nearest ring (in Å) are presented. Color: blue
= N; gray = C; yellow = S; red = O; green = Cl. (e) 11 and (f) 12 HOMO and LUMO and the energies calculated
at the B3LYP-D3BJ/6-31+G(d,p) level of theory.
Figure 2
Key changes
in the structural parameters calculated at the B3LYP-D3BJ/6-31+G(d,p)
level of theory between the (a) monomer and dimer of molecule 11, (b) monomer and dimer of molecule 12, (c)
excited and ground states of molecule 11, and (d) ground
and excited states of molecule 12.
(a) 11 and (b) 12 geometry of the ground
state. (c) 11 and (d) 12 geometry of the
most stable dimers optimized using B3LYP-D3BJ/6-31+G(d,p). For both
dimers, specific intermolecular distances between some atoms and the
center of the nearest ring (in Å) are presented. Color: blue
= N; gray = C; yellow = S; red = O; green = Cl. (e) 11 and (f) 12 HOMO and LUMO and the energies calculated
at the B3LYP-D3BJ/6-31+G(d,p) level of theory.Key changes
in the structural parameters calculated at the B3LYP-D3BJ/6-31+G(d,p)
level of theory between the (a) monomer and dimer of molecule 11, (b) monomer and dimer of molecule 12, (c)
excited and ground states of molecule 11, and (d) ground
and excited states of molecule 12.
Photophysical Properties
As illustrated in Figure and Table , the optical behavior of compounds 11 and 12, as representative samples, was investigated
for powders and DMSO solutions. Only compounds 11 and 12 exhibited solid-state emission under UV irradiation and
hence were chosen for photophysical analysis. The two dyes showed
absorption until 420 nm but seemed transparent at longer wavelengths,
a desirable feature for emissive molecules. The absorption spectra
of these compounds are similar, implying that their solution ground
states are comparable as a result of their similar electronic structures.
On the other hand, solutions emit from a variety of excited states
as specified by their diverse excitation spectra. Additionally, because
solids and solutions have distinct ground and excited states, their
excitation spectra differ from their corresponding absorption spectra,
as seen in Figure a,b. These findings demonstrate that aggregation and substitution
influence excited and ground states.
Figure 3
Photophysical behavior of the powders
(dashed lines) and DMSO solutions
(solid lines). Absorption (blue, 3 × 10–6 mol
L–1) and excitation spectra (red, λem = 520 nm for 11 and 464 nm for 12) of
(a) 11 and (b) 12. Emission spectra at λex = 300 nm of (c) 11 and (d) 12 (violet:
powder, blue: 1 × 10–3 mol L–1, black: 3 × 10–6 mol L–1, and red: 1 × 10–7 mol L–1). CIE diagrams of the emission colors of (e) 11 and
(f) 12. Photos under UV irradiation at λex = 360 nm of (g) 11 and (h) 12.
Table 1
Photophysical Data of the Examined
Compounds in the Powder and Different Solution Concentrations
11
12
λmaxb (nm)
powder
520
466
1 × 10–3 M
492
477
3 × 10–6 M
332 (w), 373 (s), 466 (m)
373 (w), 472 (s)
1 × 10–7 M
332 (s), 373 (m)
332 (w), 373 (s), 477 (m)
CIE
(x, y)a
powder
0.22, 0.59
0.17, 0.23
1 × 10–3 M
0.20, 0.42
0.16, 0.28
3 × 10–6 M
0.17, 0.23
0.15, 0.25
1 × 10–7 M
0.17, 0.18
0.15, 0.21
Φem (%)b
powder
25.6
9.7
τ (ns)c
powder
3.7 (36%) + 5.8 (64%)
2.3 (30%) + 5.3 (70%)
Kr (× 107 s–1)d
powder
4.4
1.8
Knr (× 107 s–1)e
powder
12.8
17.1
CIE coordinates for the emission
at λex = 300 nm.
Φem: emission quantum
yield.
τ: emission
lifetime.
Kr:
radiative decay rate constant for the major component (Kr = Φem/τ).
Knr:
non-radiative decay rate constant for the major component (Knr = (1/τ) – Kr).
Photophysical behavior of the powders
(dashed lines) and DMSO solutions
(solid lines). Absorption (blue, 3 × 10–6 mol
L–1) and excitation spectra (red, λem = 520 nm for 11 and 464 nm for 12) of
(a) 11 and (b) 12. Emission spectra at λex = 300 nm of (c) 11 and (d) 12 (violet:
powder, blue: 1 × 10–3 mol L–1, black: 3 × 10–6 mol L–1, and red: 1 × 10–7 mol L–1). CIE diagrams of the emission colors of (e) 11 and
(f) 12. Photos under UV irradiation at λex = 360 nm of (g) 11 and (h) 12.CIE coordinates for the emission
at λex = 300 nm.Φem: emission quantum
yield.τ: emission
lifetime.Kr:
radiative decay rate constant for the major component (Kr = Φem/τ).Knr:
non-radiative decay rate constant for the major component (Knr = (1/τ) – Kr).Emission
spectra of compounds 11 and 12 were recorded
for powders and solutions with varying DMSO concentrations
(from 1 × 10–3 to 1 × 10–7 mol L–1), as shown in Figure c,d. The color of the emission was further
validated by the Commission Internationale de l’Eclairage (CIE)
chromaticity diagrams and digital photos under UV light (Figure e–h). Compound 11 gave emission with maximum wavelengths (λmax) at 332 nm (strong) and 373 nm (medium), resulting in CIE coordinates
of (0.17, 0.18). Under UV light, these CIE coordinates created blue
emission that can be seen with the naked eye. Using a more concentrated
solution (3 × 10–6 mol L–1) diminished the high energy emission at 332 nm compared to that
at 373 nm, and a new wide emission band with λmax = 466 nm developed. Increasing the solution concentration to 1 ×
10–3 mol L–1 led to a significant
quenching of the emissions at <425 nm, resulting in a significant
emission band mainly at long wavelengths (λmax =
492 nm). The luminescence spectrum of dye 11 powder with
λmax = 520 nm was redshifted compared to that of
the 1 × 10–3 mol L–1 solution.
This redshift in emission is normal for organic components as molecules
gather in powders and concentrated solutions, where π–π
interactions between neighboring molecules strengthen, enabling the
redshift in emission.[47−49] The emission color on the CIE diagram changed from
blue to light blue, then cyan, and eventually greenish-yellow as the
molecular aggregation increased from 1 × 10–7 to 3 × 10–6 then 1 × 10–3 mol L–1 followed by the powder state. Because
the emissions at 332 and 373 nm were only significantly observed in
diluted solutions, these bands can be attributed to monomer emission
(emission from non-interacted molecules due to the solvation effect).
However, bands at >420 nm were released by molecular aggregation,
and these bands were observed using concentrated solutions and powder.The increased solution concentration of dye 12 suppressed
emission at shorter wavelengths (332 and 373 nm) while improving luminescence
intensity at longer wavelengths (477 nm). However, the powder emission
of compound 12 (λmax = 466 nm) displayed
a blueshift compared with its solutions (λmax = 477
nm). This strange behavior has been documented previously.[20,50] The blueshift denotes a reduction in π–π interactions
in dye 12 powder aggregates compared with its solutions.
Intermolecular interactions between dye 12 aggregates
may also shorten the conjugation and induce the blueshift. Therefore,
we may conclude that adding cyclohexyl as a terminal group to compound 11 changed the molecular packing and, thus, the optical characteristics
of the solid-state luminescent material. The decay profiles and lifetimes
(τ) were also evaluated, and the results are displayed in Figure and Table . τ of dyes 11 and 12 are expressed on a nanosecond scale, and then
the resulting emissions are fluorescence. The decay characteristics
of both materials were monoexponential. The emission quantum yields
(Φem) of dyes 12 and 13 in the solid state were determined to be 25.6 and 9.7%, respectively.
These reasonable values of Φem, as verified by DFT
calculations, can be attributed to the small intermolecular distances
within the dimers (less than 3.3 Å), which prohibits the rings
from rotating around single bonds. Non-planarity, in conjunction with
intermolecular interactions, can also open up new routes for radiative
decay in the solid state. Additionally, Table summarizes the observed Φem and the radiative decay rate constant (Kr) and non-radiative decay rate constant (Knr). Compound 11 has a greater Kr value and a lower Knr value than
compound 12. The increased non-planarity may result in
the blockage of non-radiative channels by further inhibiting molecule
stacking, hence increasing emission efficiency. Thus, we hypothesize
that the increased Φem of 11 (25.6%)
over 12 (9.7%) is due to the presence of a non-planar
cyclohexyl group in the molecular structure of 11, which
increases Kr and decreases Knr. The photoluminescence behavior of dye 12 powder was examined by heating and cooling the sample at various
temperatures (Figure ). Because of thermally stimulated molecular motions, the emission
intensity decreases with heating. So, cooling the sample increased
the intensity once again. Since λmax was not shifted
upon heating, it can be suggested that the emission from this compound
is due to the aggregation-induced emission enhancement. Even at 150
°C, the material emits effectively, and its spectral structure
is substantially identical as before heating. As a result, this dye
may be used in applications that need extreme conditions, such as
elevated temperatures. In comparison to our previously published compounds,[17] the present research demonstrated the influence
of non-planar groups on the emission behavior, lifetime, and decay
rate constants, where the presence of the cyclohexyl group enhanced
emission efficiency and altered the characteristics of the excited
state relative to the ground state, as shown above by comparing molecular
orbitals and absorption, excitation, or emission spectra.
Figure 4
(a) 11 and (b) 12 emission decay profiles
in the air at room temperature excited at 340 nm; green: decay, blue:
IRF, and red: fitting.
Figure 5
Photoluminescence spectra
of 12 at λex = 300 nm under various
temperatures: (a) first heating and (b) first
cooling.
(a) 11 and (b) 12 emission decay profiles
in the air at room temperature excited at 340 nm; green: decay, blue:
IRF, and red: fitting.Photoluminescence spectra
of 12 at λex = 300 nm under various
temperatures: (a) first heating and (b) first
cooling.
Experimental Section
Synthesis
The solvents and reagents utilized in this
study were of analytical grade and were utilized as provided. A Fisher-Johns
instrument was used to determine the melting points. On a Pye-Unicam
Sp-100 spectrophotometer, IR spectra were recorded using the KBr disk
method. Bruker BioSpin GmbH spectrometers (1H: 400 MHz; 13C: 101 MHz) were used to produce 1H and 13C NMR spectra with DMSO-d6 as a solvent
and tetramethylsilane (TMS) as a reference. A JEOL JMS-600 spectrometer
was used to obtain electron impact mass spectra. Using UV light, preparative
and analytical TLC were done on silica gel plates (Fluka 70643-50EA.
SIGMA-ALDRICH, Germany). All of the chemical reactions occurred in
the atmosphere. Compounds 4–8 were previously
synthesized according to reported procedures.[17,28]
A mixture of compound 8 (3.9 g, 10 mmol),
fused sodium acetate (1.64 gm, 20 mmol), and chloroacetamide (0.94
gm, 12 mmol) in 50 mL of ethanol was refluxed for 3 h. The solid precipitate
formed during reflux was filtrated off, washed with water and ethanol,
and dried in air to afford the opened structure compound 9 as off-white crystals in 95% yield. This compound was employed in
the next step without additional purification. m.p.: 150–152
°C. IR: ν (cm–1) 3455, 3389, 3317, 2209,
1651. 1H NMR (400 MHz, DMSO) δ = 11.96 (s, 1H, NH
indole), 10.28 (s, 1H, NH p-tolyl), 8.13–6.87
(10H, Ar–H and CONH2), 3.94 (s, 2H, NH2), 2.33 (s, 3H, CH3). 13C NMR (101 MHz, DMSO)
δ = 171.30, 169.57, 147.14, 136.87, 133.28, 127.48, 124.17,
122.69, 119.11, 118.59, 113.51, 110.52, 92.81, 44.96, 20.62.
To an ethanolic solution of compound 9 (4.48 gm, 10 mmol), sodium ethoxide (0.5 M) was added in
a dropwise manner, and the mixture was stirred for 30 min at ambient
temperature. The produced yellow crystals were collected, filtrated
off, and dried in air to afford the desired product in 80% yield.
m.p.: 223–225 °C, which is in agreement with the data
reported for this compound.[17]
For 5 min, a mixture
of chloromethyl derivative 13 (4.13 gm, 10 mmol) and
aniline (20 mmol) was fused followed by the addition of ethanol (20
mL). After 2 h of refluxing, the solid product produced on heat was
filtered off, dried, and recrystallized as yellow crystals from dioxane
in an 80% yield, m.p.: 301–302 °C. IR: ν (cm–1) 3245, 3185, 3026, 2969, 1643. 1H NMR
(400 MHz, DMSO) δ = 12.68 (s, 1H, NH), 11.98 (s, 1H, NH indole),
9.92 (s, 1H, NH p-tolyl), 7.39–6.57 (m, 13H,
Ar–H), 6.16(s, 1H, NH anilino), 4.21 (s, 2H, CH2), 2.32 (s, 3H, CH3).
A mixture of compound 12 (2.0
gm, 4 mmol) in phosphorylchloride (10 mL) and phosphorus pentachloride
(2.0 gm) was refluxed for 3 h on a water bath, after which it was
allowed cooling to room temperature before being poured into a 100
mL mixture of ice-cold water and neutralized with sodium carbonate
solution. The solid product was filtered out, dried, and purified
by recrystallization from dioxane to obtain white crystals with a
yield of 62.5%, m.p.: 228–230 °C. IR: ν (cm–1) 3396, 3069, 2967. 1H NMR (400 MHz, DMSO)
δ = 11.92 (s, 1H, NH indole), 10.52 (s, 1H, NH p-tolyl), 8.87 (s, 1H, CH pyrimidine), 7.92 (d, J = 7.3 Hz, 2H, Ar–H), 7.60 (m, 4H, Ar–H), 7.18 (d, J = 8.1 Hz, 2H, Ar–H), 2.29 (s, 3H, CH3). 13C NMR (101 MHz, DMSO) δ = 166.80, 155.08, 145.89,
143.32, 142.75, 130.48, 129.60, 128.11, 127.88, 120.72, 120.23, 20.94.
For 6 h, a mixed
solution of compound 16 (2.0 gm, 4 mmol) and thiourea
(0.4 gm, 6 mmol) was refluxed in 30 mL of ethanol. The yellow thiouronium
salt generated during the heating process was filtered out and washed
with dioxane, then treated with 10% NaOH, and acidified with dilute
HCl. The yellow crude product was filtered, washed repeatedly with
water, dried in the air, and recrystallized as yellow crystals from
dioxane in an 89% yield, m.p.: 297–299 °C. IR: ν
(cm–1) 3434, 3025, 2964, 1268. 1H NMR
(400 MHz, DMSO) δ = 14.28 (s, 1H, NH), 11.98 (s, 1H, NH indole),
10.34 (s, 1H, NH p-tolyl), 8.30 (s, 1H, CH pyrimidine),
7.86 (d, J = 7.0 Hz, 2H), 7.78–7.45 (m, 4H),
7.16 (d, J = 7.8 Hz, 2H), 2.28 (s, 3H). 13C NMR (101 MHz, DMSO) δ = 175.07, 174.08, 167.02, 158.44, 147.48,
146.93, 137.26, 136.88, 132.26, 131.96, 130.66, 129.54, 127.97, 120.43,
115.45, 20.93. Mass spectrum m/z = 474.3.
A mixture of chloropyrimidine
derivative 16 (3.0 gm, 6 mmol) and aniline (0.6 mL, 6
mmol) was fused for 5 min, and then ethanol (20 mL) was added. The
mixture was refluxed for 2 h. The solid product formed on heat was
filtrated off, dried, and recrystallized from dioxane as yellow crystals
in 80% yield, m.p.: 260–262 °C. IR: ν (cm–1) 3207, 3154, 3098, 3053, 2923. 1H NMR (400 MHz, DMSO)
δ = 11.93 (s, 1H, NH indole), 9.61 (s, 1H, NH p-tolyl), 9.05 (s, 1H, NH anilino), 8.63 (s, 1H, CH pyrimidine), 7.58–6.84
(m, 13H, Ar–H), 2.33 (s, 3H, CH3).
A mixture of hydrazinyl
compound 20 (2.0 gm,
4 mmol) and acetyl acetone (0.5 mL, 5 mmol) was refluxed in dioxane
(20 mL) for 3 h. After cooling the reaction mixture, the solid precipitate
produced was collected, filtered out, dried, and recrystallized in
75% yield from dioxane as white crystals, m.p.: 220–222 °C.
IR: ν (cm–1) 3465, 3061, 2926. 1H NMR (400 MHz, DMSO) δ = 11.87 (s, 1H, NH indole), 10.28 (s,
1H, NH p-tolyl), 8.64 (s, 1H, CH pyrimidine), 7.87–7.03
(m, 8H, Ar–H), 6.28 (s, 1H, CH pyrazole), 2.75 (s, 3H, CH3), 2.38 (s, 3H, CH3), 2.24 (s, 3H, CH3). 13C NMR (101 MHz, DMSO) δ = 169.21, 165.91, 162.33,
158.71, 156.81, 152.06, 147.60, 143.01, 140.44, 137.58, 135.18, 131.09,
129.14, 127.56, 122.73, 120.05, 116.21, 116.03, 111.81, 105.31, 21.69,
13.36, 12.12.
Quantum-Chemical Calculations
To
acquire information
about the structure of molecules 11 and 12, quantum-chemical computations were done. The ground states were
optimized via DFT with B3LYP functional, D3BJ correction, and the
basis set 6-31+G(d,p).[51,52] This dispersion correction is
needed to explain non-covalent and long-range interactions such as
π–π stacking and hydrogen bonding, which are critical
in this work and are required to achieve realistic intermolecular
interactions.[53] For the ground state geometry,
many conformers were investigated, and the one with the minimum energy
was chosen. Harmonic vibrational frequency validated this global minimum.
The binding energies (ΔEb) of dimers
were estimated using the relationship: ΔEb = Edimer – 2Emonomer.UV–vis
absorption spectra
were detected using a JASCO V-550 absorption spectrometer. A Hitachi
F-7000 fluorescence spectrometer equipped with a Hamamatsu R928 photomultiplier
detector was used to record the steady-state photoluminescence spectra.
Φem were measured in powder form using a calibrated
integrating sphere (Hitachi). The powder luminescence behavior at
various temperatures was investigated by placing it in a thin quartz
cell (1 × 10 × 20 mm) set on a homemade heating stage. The
decay patterns and emission lifetimes of 11 and 12 were measured at λ = 545 and 477 nm, respectively,
using a Quantaurus-Tau photoluminescence lifetime measurement device
(C1136-21, Hamamatsu) with λex = 340.
Conclusions
Different heterocyclic compounds containing both indole and thienopyrimidine
moieties have been successfully synthesized from 5-amino-4-(3-chloro-1H-indol-2-yl)-2-(p-tolylamino)thieno[2,3-d]pyrimidine-6-carboxamide (10). Spectral analysis
was used to confirm the structures of all novel compounds. Due to
the dependence of the luminescence spectrum on the aggregate structure,
the photoluminescence behavior of two homologous dyes displayed opposing
emission behavior upon aggregation of molecules. DFT simulations indicated
that introducing a terminal group may substantially modify molecular
packing and hence the emission spectrum by encouraging or suppressing
the development of specific intermolecular interactions such as π–π
interactions, and as a result of which, the emission spectrum exhibits
a redshift or blueshift. Because of the short intermolecular distance
among the dimers of the two materials (less than 3.3 Å), which
makes it difficult for aromatic rings to rotate around single bonds,
the materials demonstrated excellent Φem in the solid
state (25.6 and 9.7%). Non-planarity and intermolecular interactions
can also open up new routes for radiative decay in the solid state.
At high temperatures, the compounds also demonstrated a stable emission
characteristic.
Authors: Marc Warner; Salahud Din; Igor S Tupitsyn; Gavin W Morley; A Marshall Stoneham; Jules A Gardener; Zhenlin Wu; Andrew J Fisher; Sandrine Heutz; Christopher W M Kay; Gabriel Aeppli Journal: Nature Date: 2013-10-27 Impact factor: 49.962
Authors: Sheng Xie; Sesha Manuguri; Giampiero Proietti; Joakim Romson; Ying Fu; A Ken Inge; Bin Wu; Yang Zhang; Daniel Häll; Olof Ramström; Mingdi Yan Journal: Proc Natl Acad Sci U S A Date: 2017-07-25 Impact factor: 11.205