Open Access Article
M. Carmen Borrallo-Anicetoa,
Beatriz Fuerte-Díeza,
Laura González-Aguileraa,
M. Luisa Ferrer
a,
M. Pilar Lillob,
Andreas Mavrandonakisa,
Urbano Díaz
c,
Eva M. Maya
*a and
Marta Iglesias
*a
aInstituto de Ciencia de Materiales de Madrid. CSIC, C/Sor Juana Inés de la Cruz, 3, 28049, Madrid, Spain. E-mail: eva.maya@csic.es; marta.iglesias@icmm.csic.es
bInstituto de Química Física Blas Cabrera. CSIC, C/Serrano, 119, 28006, Madrid, Spain
cInstituto de Tecnología Química, Universitat Politècnica de València, Consejo Superior de Investigaciones Científicas, Avenida de los Naranjos s/n, E-46022 Valencia, Spain
First published on 25th February 2026
In this work, we describe the synthesis of a series covalent triazine frameworks (CTFs) based on 1,6-substituted-pyrene-derivatives, in which triazine units (electron acceptor groups) are either directly bonded to the pyrene core (1,6-Pyr-CTF) or connected via aryl or fluoroaryl-π-linkers (1,6-DPhPyr-CTF and 1,6-2FDPhPyr-CTF). These CTFs were readily synthesized through cyclotrimerization of the corresponding dinitriles, yielding thermally stable products with favorable photophysical properties and fluorescence emission maxima at 401 nm (1,6-Pyr-CTF), 428 nm (1,6-DPhPyr-CTF) and 433 nm (1,6-2FDPhPyr-CTF). These characteristics make them promising candidates for fluorescent sensing of nitroaromatic compounds. Among the synthesized frameworks, the fluorinated diphenylpyrene-triazine (1,6-2FDPhPyr-CTF) exhibits the highest selectivity and sensitivity toward nitro compounds, in EtOH/H2O dispersions, with KSV = 4.35 × 104 M−1 (LOD = 0.15 ppm) for picric acid (TNP) or 3.39 × 104 M−1 (LOD = 0.11 ppm) for (p-nitroaniline, 4-NA). These results demonstrate the beneficial effect of extended π-conjugation and fluorine incorporation on the sensing performance of CTFs.
Covalent triazine frameworks (CTFs) are a well-known type of organic frameworks consisting of triazine units covalently bonded to different aromatic nodes, which have become increasingly attractive since they were first reported16–20 CTFs have highly robust structures with attractive properties such as high thermal and chemical stability, high nitrogen content and porosity. These properties make CTFs attractive for promising applications including molecular recognition,21 catalysis,22–26 energy storage,27,28 environmental remediation,29–31 gas separation and storage,32,33 and have provided a suitable platform for the chemical detection of hazardous compounds and ions.13,15,34–36 Pyrene molecule is a polycyclic aromatic hydrocarbon (PAH) characterized by a long excited-state lifetime, and excellent emission properties, high photochemical and thermal stability.37–40 Due to its special properties, it has been used as structural building block for the synthesis of pyrene-based derivatives for applications in optoelectronics (organic photovoltaic cells (OPV), dye-sensitized solar cells (DSSCs), organic light-emitting diodes (OLEDs), nonlinear optical (NLO)).41–44 Pyrene compounds have also applied as sensors for temperature,45 pH,46,47 or metal ions48,49 The functionalization of the pyrene nucleus with electron donor or acceptor groups combined with the extension of π-conjugation allows the control of the electronic properties of pyrene-based compounds, resulting in their wide range of applications.50–52 The most reactive positions for functionalizing the pyrene core are 1, 3, 6, and 8. Different acceptor groups such as nitro, cyano, cyanoacrylonitrile, and cyanoacrylic acid have been attached to the pyrene moiety at these positions through different π-conjugated linkers, and their resulting properties and applications have been reported.42,53 It has also been reported that the incorporation of fluorine atoms on the acceptor group can modulate the energy levels of organic dyes,54 and this effect has been demonstrated by Gao et al., who reported that perfluorobenzonitrile-substituted pyrenes exhibited enhanced properties such as stronger electron-withdrawing ability, greater thermal stability and improved fluorescence compared to perfluorotoluyl-pyrene derivatives.55
Recently, we reported the synthesis of a family of 2,7-substituted pyrene-based covalent triazine frameworks (CTFs) and demonstrated their dual detection capabilities. By extending conjugation through the 2,7-positions of the pyrene ring, these materials exhibited excellent fluorescence responses toward dichloran (DCNA), picric acid (PA), and metal ions such as Au3+ and Fe3+.56 In the present work, we focus on a new design strategy by synthetizing 1,6 pyrene-substituted-CTFs, in which the electron-acceptor triazine units are either directly attached to the pyrene core (1,6-Pyr-CTF) or connected via π-conjugated phenyl or fluoroaryl groups (1,6-DPhPyr-CTF, 1,6-2FDPhPyr-CTF) (Scheme 1). In the latter, two fluorine atoms are positioned ortho to the phenyl ring, acting as additional electron-withdrawing groups. This modification enhances the electron-acceptor character of the framework, promotes charge transfer, and reduces the HOMO–LUMO energy gap.
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| Scheme 1 Synthesis of 1-6-pyrene-based triazines (1,6-Pyr-CTF, 1,6-DPPhPyr-CFT and 1,6-2FDPPhPyr-CTF). | ||
By shifting the substitution pattern from 2,7- to 1,6-positions and incorporating tunable electron-withdrawing groups, the current design explores a distinct electronic configuration and charge-transfer pathway, highlighting a new structure–property relationship that is different from our previous 2,7-pyrene CTFs.
(C
N) stretching vibrations bands at 2223 cm−1 for dinitriles 1 and 2, and 2237 cm−1 for compound 3. In addition, the spectrum of compound 3 shows a distinct C–F stretching band at 1030 cm−1, confirming the presence of fluorine substituents. The 1H-NMR spectra (Fig. S1–S3) exhibit the characteristic chemical shifts of the pyrene rings protons at 8.68 and 8.41 ppm for dinitrile 1, 8.27 and 8.11 ppm for 2, and 8.48 and 8.34 ppm for 3. 13C NMR spectra (Fig. S1–S3) show the nitrile carbon signals (
N) at 116.8, 110.4 and 112 ppm for monomers 1–3 respectively. Compound 3 exhibits a signal at 162.2 ppm corresponding to the C–F bond along with the corresponding signal at −105.57 ppm in its 19F-NMR spectrum (Fig. S3), confirming the presence of fluorinated aryl groups. Thermogravimetric analyses (TGA) indicate that 1,6-pyrene-dinitriles possess good thermal stability with the decomposition temperatures of 300 °C, 380 °C, and 375 °C for compounds 1 to 3, respectively.
Dinitriles were successfully used to obtain the corresponding 1,6-pyrene-based triazines in high yields. The elemental analysis is in close agreement with the theoretical values (Table S1).
The FT-IR spectra (Fig. 1a) show the characteristic bands corresponding to the pyrene core, the aromatic rings, and the triazine units. Fluorinated-CTF exhibits the C–F band at 1022 cm−1. In addition, the disappearance of the CN stretching band at 2220 cm−1 confirms the formation of the covalent triazine framework (Fig. S4). The fluorinated-1,6-2FDPhPyr-CTF exhibits two Raman bands at ∼1590 cm−1 (G-band of sp2-hybridized carbon) and D-band at ∼1350 cm−1 assigned to sp2-hybridized carbon atoms containing structural defects (Fig. S5). The solid-state 13C-NMR (CP-MAS) spectra showed the characteristic resonance of the triazine carbon at approximately 170 ppm. In the fluorinated CTF spectrum, an additional signal is observed at around 165 ppm.
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| Fig. 1 Characterization data of 1,6-pyrene-based CTFs. (a) FT-IR spectra; (b) 13C-NMR spectra; (c) TGA; (d) CO2 sorption; (e) PXRD and (f) XPS survey. | ||
The signals corresponding to aromatic carbons from the pyrene and aryl groups are observed in the region between 100 ppm and 140 ppm (Fig. 1b). Importantly, the absence of the CN signal confirms complete conversion of the dinitrile precursors into the framework. TGA performed under an air atmosphere also indicates that 1,6-pyrene-based CTFs exhibit excellent thermal stability with a major decomposition step occurring around 500 °C (Fig. 1c).
All materials show a Lorentzian signal in their EPR spectra, indicative of the presence of unpaired electrons (Fig. S6). The most intense signal is observed for 1,6-2FDPhPyr-CTF, suggesting a higher concentration of centers with unpaired spins (radicals/defects) in this material.
The porosity of the materials was studied using nitrogen adsorption/desorption isotherms at 77K. Brunauer–Emmett–Teller (BET) surface area analysis revealed values below 20 m2 g−1 for all materials, except for 1,6-DPhPyr-CTF, which exhibited a higher surface area of 75 m2 g−1 (Fig. S7). Additionally, CO2 adsorption capability was evaluated from the sorption isotherms measured at 273 K and pressures up to 1 atm. The surface areas calculated from the CO2 adsorption isotherms using the Dubinin–Astakhov (DA) method were 192.5, 81.4, and 121.8 m2 g−1 for 1,6-Pyr-CTF, 1,6-DPhPyr-CTF and 1,6-2FDPhPyr-CTF, respectively. The CO2 uptake ranged from 0.276 mmol g−1 for 1,6-Pyr-CTF to 1.149 mmol g−1 for 1,6-2FDPhPyr-CTF (Table 1, Fig. 1d). These results indicate the good affinity of acidic CO2 molecules for the basic triazine units present in the framework. The polymer 1,6-2FDPhPyr-CTF has a water contact angle of 65.4° (Fig. S8), indicating a moderately hydrophilic surface.
The XPS survey spectra of 1,6 pyrene-based CTFs are shown in Fig. 1f and the corresponding high-resolution C 1s, N 1s, O 1s, and F 1s traces are shown in Fig. S9. In the C 1s spectrum, two main components at binding energies (BE) of ∼285–286 eV and ∼289–290 eV corresponding to C
C and C
N bonds, respectively, can be observed. The N 1s spectrum showed one type of nitrogen with BE ranging from 399.3 eV to 399.7 eV Additionally, 1,6-2FDPhPyr-CTF shows a peak at 691.4 eV in the F 1s spectrum, confirming the presence of fluorinated groups.
SEM and TEM analyses (Fig. 2 and 3) reveal irregular agglomerates composed of dense, nanosized particles, consistent with the low N2-BET surface areas measured. The TEM images reveal predominantly amorphous domains with locally ordered lamellar regions, indicating partial π–π stacking between aromatic layers.
This short-range order correlates with the broad diffraction band observed by PXRD (Fig. 1e) and, for 1,6-DPhPyr-CTF, with a reflection centred at 2θ ≈ 18°, probably corresponding to an interlayer spacing of ∼4.9 Å. Such spacing suggests loose aromatic stacking modulated by the phenyl connectors. In contrast, 1,6-Pyr-CTF and 1,6-2FDPhPyr-CTF exhibit fully amorphous patterns, in agreement with their more disordered morphology seen by TEM. Overall, the combined microscopy and XRD data indicate poorly crystalline networks with limited local stacking, which could still promote efficient charge-transfer pathways relevant to their sensing performance.
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| Fig. 4 Fluorescence colour changes of dinitriles and their corresponding 1,6-Pyrene-based CTFs dispersed in different solvents (0.1 mg mL−1), under UV light (λ = 365 nm). | ||
The solid-state UV/visible spectra of the 1,6-pyrene-based CTFs showed strong and broad absorption bands extending across the visible region (Fig. 5a), with a pronounced red shift in the absorption maxima compared to the parent dinitriles. This shift is attributed to the formation of extended π-conjugated network within the CTFs (Fig. S10).
The emission spectrum of 1,6-pyrene-based CTFs in different solvents (Fig. 5b) showed the highest fluorescence intensity in ethanol (EtOH) and the lowest in water. To identify a solvent compatible with real sample applications, various EtOH–H2O mixtures were evaluated. A 1
:
1 EtOH–H2O mixture was found to provide an optimal balance between fluorescence intensity and dispersion stability (Fig. S11). Fig. 5c shows the fluorescence emission spectra recorded in EtOH–H2O (1
:
1) mixture with maxima at 401 nm for 1,6-Pyr-CTF, and 433 nm for 1,6-2FDPhPyr-CTF. For 1,6-DPhPyr-CTF, which showed no measurable signal in EtOH–H2O mixture, the emission spectrum was recorded in pure EtOH, displaying a maximum at 428 nm.
To assess the influence of pyrene substitution at positions 1,6 versus 2,7 on the sensing behavior of the resulting materials, it is important to consider the dispersibility of the materials in solvents of different polarities and the intensity of their corresponding emission spectra.
The emission spectra of the 2,7-series indicated that the highest intensity is observed in solvents such as toluene, dioxolane, and a 1
:
1 dioxolane–water mixture.56 However, as mentioned above, the emission spectra of 1,6-Pyr-CTF in solvents of varying polarity revealed that the highest intensity corresponds to ethanol or an ethanol–water mixture (1
:
1), while the intensity in dioxolane is only half as strong (Fig. 5b). Therefore, a comparative study between the two series cannot be directly conducted, as each exhibits optimal behavior in solvents with different characteristics, with polar solvents being more favorable in the case of the 1,6-series.
Fluorescence quenching experiments were carried out by adding solutions of the analyte (NAC) to dispersions of the corresponding sensor (0.3 mg/3 mL) in the appropriate solvent (HPLC grade). The quenching behavior was analyzed using the Stern–Volmer (SV) equation (I0/I = 1 + KSV[C]), where I0 and I are the fluorescence intensities of sensor before and after analyte addition, respectively, and [C] is the analyte molar concentration. From the linear fitting of SV plot at low analyte concentrations, the quenching constant (KSV, M−1) was determined. The detection capability of the 1,6-Pyr-CTF series was studied in the ethanol–water mixture, a solvent with greater potential for detecting contaminants in real-world samples. We first evaluated the sensing performance of 1,6-Pyr-CTF toward a range of NACs (Fig. 6a and Table S2). The highest KSV values were observed for NACs containing amine groups in the para position relative to the nitro group specifically 4-nitroaniline (4-NA), dicyanoaniline (DCNA), and 2-amino-5-nitrophenol (2A-5NP), with values of 3.08 × 104 M−1, 2.29 × 104 M−1, and 1.84 × 104 M−1, respectively. The particularly strong response toward 4-NA is attributed to its high dipole moment and hyperpolarizability, which facilitate strong interactions with the CTF framework, including N–H and hydrogen bonding interactions. Furthermore, the distinct quenching behaviour of 4-NA compared with other nitroaniline isomers, such as 2-NA, highlights the potential of the CTFs for selective discrimination among structurally similar NACs.
A second group of NACs includes those bearing hydroxyl groups in the para position relative to the nitro group—namely TNP, 2A-4NP, and 4-NP—with KSV values of 1.75 × 104 M−1, 1.09 × 104 M−1, and 0.50 × 104 M−1, respectively. In contrast, 1,6-Pyr-CTF exhibited negligible fluorescence quenching in the presence of nitro derivatives such as nitrobenzene (NB) and 1,4-dinitrobenzene (1,4-DNB), as well as other aromatic compounds like toluene, indicating high selectivity. As shown in Fig. 6a, the presence of an amine group has a more pronounced effect on quenching than nitro or hydroxyl groups alone. Furthermore, 1,6-Pyr-CTF demonstrated the highest quenching efficiency when the NAC contained both nitro and amine groups, highlighting its sensitivity to strong electron-donating/electron-withdrawing combinations. Based on these findings, we further examined the sensing behavior of the D-π-A type CTF, 1,6-2FDPhPyr-CTF, toward selected NACs, including TNP, 4-NA, DCNA, and 2A-5NP. Reproducible data could not be obtained with 1,6-DPhPyr-CTF because it does not disperse well in an ethanol-water mixture. For this reason, we only studied the sensing performance of 1,6-2FDPhPyr-CTF. In this case, significantly higher KSV values were obtained compared to 1,6-Pyr-CTF (Fig. 6b), with the best response observed for TNP (KSV = 4.35 × 104 M−1). For comparison, the sensing performance of corresponding parent dinitriles was also evaluated, revealing substantially lower quenching responses than those observed for the CTFs. This highlights the enhanced sensing capability provided by the framework structure.
The quenching efficiency (QE) for TNP was found to be 82.8% with 1,6-Pyr-CTF and 86.5% with 1,6-2FDPhPyr-CTF. For DCNA, the QE values were 84.2% and 68.0%, respectively, while for 4-NA the QE reached 82.8% and 91.4% (Fig. S12). To further investigate the sensing behaviour, fluorescence intensity was measured as a function of analyte concentration (Fig. S13). Upon the addition of 149 μmol L−1 or 165 μmol L−1 of TNP or 165 μmol L−1 of 4-NA, the fluorescence of both 1,6-Pyr-CTF and 1,6-2FDPhPyr-CTF was almost completely quenched (QE > 93%), indicating highly efficient detection. Fig. 6c visually confirms that under UV illumination (365 nm), the fluorescence of both materials is fully suppressed upon exposure to TNP, demonstrating their practical potential applicability for NAC detection. Selectivity studies (Fig. S14) further show that in the presence of 4-NA or TNP, the quenching response toward other anilines or phenols is significantly lower, underscoring the high selectivity of both CTFs for target NACs.
The limit of detection (LOD) was calculated using the equation LOD = 3σ/ρ. where σ is the standard deviation of the fluorescence intensity of blank samples (based on 10 replicates) and ρ is slope of the calibration curve (relative fluorescent intensity vs. analyte concentration).62 The LOD values for 1,6-Pyr-CTF and 1,6-2FDPhPyr-CTF were 0.25 and 0.15 ppm for TNP and 0.31 and 0.11 ppm for 4-NA (Table S2). These results confirm the potential of these CTFs for the sensitive detection of 4-NA or TNP in environmental samples. A comparative summary of reported data for triazine-based small molecules and various polymeric organic frameworks is provided in Table S4. The detection capabilities of 1,6-pyrene-based CTFs are comparable to those of other reported materials, with KSV values on the order of 104 M−1 and limits of detection at the ppm level. Particularly, this work demonstrates how the combination of donor and acceptor units, along with the introduction of functional groups such as fluorine (F), can effectively modulate the properties of a material, in this case, a sensor, to achieve optimal performance.
Finally, the recyclability of both CTFs was studied. As it can be observed in Fig. S15a and S15b, the recovered CTF retained nearly their original fluorescence intensity and maintained consistent sensing performance over at least five cycles for 1,6-Pyr-CTF and three cycles for 1,6-2FDPhPyr-CTF, which indicates the good stability and reusability of both CTFs for the detection of 4-NA or TNP. Additionally, Fig. S15c displays the IR spectra of the recovered samples after the sensing experiments, confirming the preservation of the framework structure.
The band-gap values obtained were 1.68 eV, 1.75 eV, and 1.72 eV for 1,6-Pyr-CTF, 1,6-DPhPyr-CTF and 1,6-2FDPhPyr-CTF, respectively. Fig. 7a, shows the HOMO–LUMO energy levels estimated from cyclic voltammetry (CV) measurements (Fig. S18 and Table S3). As shown, the LUMO energy levels of all Pyr-CTFs are higher than those of TNP (−3.89 eV) and 4-NA (−3.71 eV), enabling efficient electron transfer from the photoexcited CTF to these analytes. In contrast, the LUMO level of DCNA (−3.01 eV) lies above those of the CTFs, making PET less favourable in this case.
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| Fig. 7 (a) Energy level diagrams (LUMO from onset reduction potentials Eredonset) and (b) Nyquist plot from electrochemical impedance spectroscopy (EIS measurements) of 1,6-Pyr-based CTFs. | ||
To gain deeper insight into the fluorescence quenching mechanism, Fig. S19 shows the spectral overlap between the emission spectra of 1,6-Pyr-based CTFs and the absorption spectra of various nitro compounds. A significant overlap is observed for TNP, 4-NA, 2A-5NP, and DCNA, while negligible overlap is found for the other analytes tested. This suggests that resonance energy transfer (RET)63 may also contribute to the quenching process.
To further investigate charge separation and transfer properties, electrochemical impedance spectroscopy (EIS) was performed (Fig. 7b). The Nyquist plots reveal that 1,6-2FDPhPyr-CTF exhibits a smaller semi-circular radius compared to its non-fluorinated counterpart, indicating lower charge transfer resistance. Taken together, these data suggest a discrepancy between the LUMO energy levels of 1,6-pyrene-based CTFs and certain NACs during the quenching process, particularly in their limited response toward DCNA. This implies that fluorescence quenching is not governed exclusively by PET.
Additional mechanisms may contribute to the observed quenching behaviour, including ground-electrostatic interaction between the triazines and analytes,64 resonance energy transfer processes (RET),65 or inner filter effect (IFE)66 due to spectral overlap. These findings underscore the complex interplay of structural, electronic, and intermolecular factors that influence the sensing performance of 1,6-pyrene-based CTFs.
To explain the mechanism more, time-resolved fluorescence experiments were conducted (Fig. 8a). The average fluorescence lifetimes obtained were 4.0 ns, 2.5 ns and 1.4 ns for 1,6-Pyr-CTF, 1,6-DPhPyr-CTF and 1,6-2FDPhPyr-CTF respectively. Upon addition of TNP, the lifetimes remained nearly unchanged (〈τ〉 = 2.3 ± 0.3 ns and 〈τ〉 = 1.4 ± 0.3 ns) before and after analyte addition (Fig. 8b and c) confirming a static quenching mechanism. Considering these data and previous findings,67 these results suggest that the selectivity and sensitivity of 1,6-pyrene-based CTFs toward TNP likely arise from the combined contribution of multiple mechanisms64 including PET, RET and IFE.66 This highlights the complex interplay of structural, electronic, and intermolecular factors governing the sensing performance of these materials.
These calculations offer theoretical explanations for the interfacial interactions involved in the adsorption of nitroaromatic compounds in 1,6-Pyr-based CTFs. For this study, we selected 1,6-Pyr-CTF and 1,6-2FDPhPyr-CTF as sensors and 4-NA and 4-NP as representative analytes due to their structural similarity and the presence of distinct functional groups, an amino group in 4-NA and a hydroxyl group in 4-NP, which allowed us to investigate the influence of different substituents on the sensing behavior. As a 1,6-Pyr-CTF model, we chose a molecular model that consists of a triazine core, which is further extended by three (dimethyl-triazinyl)-pyrene groups, as shown in the top part of Fig. 9. The molecular model for the 1,6-2FDPhPyr-CTF has been constructed in a similar manner.
The conformational sampling identified two main interaction motifs between the 4-NA and 4-NP molecules with the 1,6-Pyr-CTF and 1,6-2FDPhPyr-CTF. The molecules can interact via π–π stacking and hydrogen-bonding. In most cases, only π–π stacking binding pattern is observed, and in fewer cases a combination of π–π stacking and hydrogen-bonding. For 4-NA interacting with the 1,6-Pyr-CTF, all configurations are similar in energy and differ by only 0.3 kJ mol−1, while for 4-NP they differ up to ∼10 kJ mol−1. The most stable adsorption configurations are presented in Fig. 9. The computed interaction energies of both 4-NA and 4-NP with the 1,6-Pyr-CTF have similar values of ∼−58.5 kJ mol−1. The interactions of 4-NA and 4-NP with the 1,6-2FDPhPyr-CTF are slightly weaker compared to the 1,6-Pyr-CTF. For the most stable adsorption configurations of 4-NA with the 1,6-2FDPhPyr-CTF, the interaction energies are calculated to be ∼−48 and ∼−54 kJ mol−1, while for 4-NP are ∼−51 kJ mol−1. In both molecules, the stable interaction configurations are a combination of π–π stacking and hydrogen-bonding. The DFT calculated interaction values are shown in Table S5. To further analyze the H-bonds, the Interaction Region Indicator (IRI) plots are presented in Fig. 10, where the color of the plots can qualitatively measure the strength of the H-bonds. According to the coloring scheme in the bottom part of Fig. 10, stronger interactions are depicted with isosurfaces of blue color, while green color areas represent weaker interactions. This analysis is presented for the 1,6-PYR-CTF only. H-bonds between the 4-NP with the triazine ring are always depicted in green color, while in the most stable configuration I of the 4-NA, the H-bond is depicted in blue color. This indicates qualitatively, that 4-NA interacts via stronger H-bonding with the 1,6-Pyr-CTF than the 4-NP. The IRI plots can also qualitatively explain the trend in the interaction energies between the configurations I and V of 4-NP (−58.8 vs. −43.9 kJ mol−1, respectively). In Configuration I, the isosurface of the IRI plot is blue, whereas it is green for V, indicating that the H-bond is weaker in V. A general trend in the 4-NP, is that H-bonding is stronger than π–π stacking by comparing the value of I with the values of II, III, IV, and VI. However, there is no trend observed for 4-NA, where the interaction energies are computed to be almost isoenergetic.
:
1) (HPLC grade). Titration experiments were performed after adding different concentrations of each analyte to 0.1 mg of a well-dispersed CTF powder in 3 mL of EtOH : H2O (quartz cuvette, 1 cm × 1 cm). The fluorescence emission spectrum of each resultant mixture was recorded after thorough mixing by using ultrasonic treatment (5 min) to obtain a homogeneous mixture. The spectrum of each titration was repeated at least three times.
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