Synthesis, Cytotoxicity, and Photophysical Investigations of 2-Amino-4,6-diphenylnicotinonitriles: An Experimental and Theoretical Study

In this study, we present a comprehensive investigation of 2-amino-4,6-diphenylnicotinonitriles (APNs, 1–6), including their synthesis, cytotoxicity against breast cancer cell lines, and photophysical properties. Compound 3 demonstrates exceptional cytotoxicity, surpassing the potency of Doxorubicin. The fluorescence spectra of the synthesized 1–6 in different solvents reveal solvent-dependent shifts in the emission maximum values, highlighting the influence of the solvent environment on their fluorescence properties. A quantum chemical TD-DFT analysis provides insights into the electronic structure and fluorescence behavior of 1–6, elucidating HOMO-LUMO energy gaps, electronegativity values, and dipole moments, contributing to a deeper understanding of their electronic properties and potential reactivity. These findings provide valuable knowledge for the development of APNs (1–6) as fluorescent sensors and potential anticancer agents.


Introduction
2-Amino-4,6-diphenylnicotinonitriles (APNs) are compounds of considerable interest due to their intriguing structure and diverse biological activities.APNs showed antimicrobial activity against various pathogens [1], antiproliferative activity with PIM-1 kinase inhibitory potential [2,3], anti-tubercular activity against Mycobacterium tuberculosis [4], SIRT1 inhibitory activity [5], and A 2A adenosine receptor antagonism [6].In addition to their biological activities, APNs have also shown promise as fluorescent sensors for monitoring photopolymerization processes.APNs exhibited higher sensitivity compared to commercially available probes (7-diethylamino-4-methylcoumarin and trans-2-(2 ′ ,5 ′dimethoxyphenyl)ethenyl-2,3,4,5,6-pentafluorobenzene) and have demonstrated their ability to accelerate cationic photopolymerization processes, particularly in the photoinitiation of epoxide and vinyl monomers [7].This suggests the potential utility of APNs as fluorescent sensors for monitoring various polymerization processes and as long-wavelength co-initiators for diphenyliodonium salt initiators.Researchers have conducted extensive studies to synthesize these compounds using various approaches.Several research groups have successfully synthesized APNs from aldehydes and acetophenones with malonitrile, employing different reaction conditions.The synthesis of APNs has been achieved using solvent-free (neat) conditions, where the reaction takes place without the use of any additional solvents.This approach offers the advantages of simplicity and environmentally friendly characteristics [8][9][10].Water has also been utilized as a reaction medium for synthesizing these compounds, providing a greener alternative [11][12][13][14].Microwave irradiation [6, [15][16][17] and ultrasonic irradiation [18,19] have also been employed as energy also been utilized as a reaction medium for synthesizing these compounds, providing a greener alternative [11][12][13][14].Microwave irradiation [6, [15][16][17] and ultrasonic irradiation [18,19] have also been employed as energy sources to expedite the reaction and enhance the yield and efficiency of the synthesis of APNs.Various catalysts have been employed to facilitate the synthesis of APNs.Notably, HBF4 has been used as an oxidizing promoter catalyst under mild and solvent-free conditions, providing an efficient and practical method for the synthesis of APNs [20].Other catalysts include [HO3S-PhospIL@SBA-15] [21], the CoFe2O4-TRIS-sulfated boric acid nano catalyst [22], ClO4 − /Al-MCM-41 nanoparticles [23], SrFe12O19 [24], amberlyst-15 [5], Cu(OAc)2 [1], nicotinium methane sulfonate (NMS) [17], doped nano-sized copper(I) oxide (Cu2O) on melamineformaldehyde resin [25], [Bmim]BF4 ionic liquid [26], Bu4N + Br − in aqueous medium [27], SnO2/SiO2 nanocomposite [28], ytterbium perfluorooctanoate [Yb(PFO)3] [29], poly N,Ndimethylaniline-formaldehyde supported on silica-coated magnetic nanoparticles [30], eggshell-based nano-magnetic solid acid catalyst [31], sulfonic acid-functionalized graphitic carbon nitride composite [32], and trifluoroethanol (TFE) [33].Despite APNs's intriguing structure and versatile biological activities, no comprehensive structural or photophysical studies have been conducted thus far.Therefore, in this study, we aim to address this research gap by presenting a convenient synthesis of APNs (Figure 1) and investigating their photophysical properties by examining the solvent effects on their emission spectra experimentally and computationally using density functional theory (DFT) and time-dependent density functional theory (TD-DFT).The DFT and TD-DFT computational methods were employed to provide insights concerning the physicochemical properties of these compounds at the molecular level.In light of the computational study and in good agreement with the experimental results, the resonance structures and the type of spectral bands in solution for the synthesized APN compounds were highlighted and discussed.This research will contribute to a deeper understanding of APNs's characteristics and potential applications in various fields.

Results and Discussion
2.1.Synthesis of 2-Amino-4,6-diphenylnicotinonitriles (APNs, 1-6) The synthesis of the APNs (1-6) was efficiently achieved according to the depicted scheme (Scheme 1).The synthetic route involved a straightforward two-step process.In the initial step, a mixture of equimolar amounts of acetophenones (7a-7c) and aldehydes (8a-8c) was subjected to a reaction under basic conditions.This reaction yielded the corresponding chalcones [34].Moving to the second step, the obtained chalcones (9a-9f) were then reacted with malononitrile (10) and ammonium acetate under refluxing conditions.This step involved heating the reaction mixture and allowing for efficient conversion and subsequent cyclization to form the desired APNs (1-6) [35].The confirmation of the structures of the chalcone intermediates (9a-9f) and the final APNs (1-6) was accomplished through the utilization of various analytical techniques, including melting point determination, infrared (IR) spectroscopy, nuclear magnetic resonance (NMR) spectroscopy, and mass spectrometry.In addition to that, the observed melting points, IR spectra, NMR spectra, and mass spectra of known APNs (1-6) were compared with the expected values reported in the literature.These findings provide evidence for the successful synthesis of the desired APNs (1-6).
Molecules 2024, 29, x FOR PEER REVIEW 3 of 20 conditions.This step involved heating the reaction mixture and allowing for efficient conversion and subsequent cyclization to form the desired APNs (1-6) [35].The confirmation of the structures of the chalcone intermediates (9a-9f) and the final APNs (1-6) was accomplished through the utilization of various analytical techniques, including melting point determination, infrared (IR) spectroscopy, nuclear magnetic resonance (NMR) spectroscopy, and mass spectrometry.In addition to that, the observed melting points, IR spectra, NMR spectra, and mass spectra of known APNs (1-6) were compared with the expected values reported in the literature.These findings provide evidence for the successful synthesis of the desired APNs (1-6).
In brief, the infrared (IR) spectral analysis of 1-6 revealed characteristic absorption bands associated with the presence of specific functional groups, namely the amino (N-H) and cyanide (-CN) groups.The amino (N-H) group in 1-6 exhibited distinctive stretching vibrations in the IR spectra.The N-H stretching bands were observed in the range of 3412-3487 cm −1 and 3300-3368 cm −1 .These absorption bands arise from the stretching motion of the nitrogen-hydrogen bonds in the amino group.The broad nature of these bands is typical for N-H stretching vibrations.Additionally, the N-H bending vibrations of the amino group were observed in the IR spectra of 1-6.The N-H bending bands appeared in the range of 1606-1654 cm −1 .These absorption bands result from the bending motion of the nitrogen-hydrogen bonds in the amino group.The presence of these bands further confirms the presence of the amino group in the synthesized compounds (1)(2)(3)(4)(5)(6).Furthermore, the cyanide (-CN) groups in compounds 1-6 exhibited characteristic absorption bands in the IR spectra.The IR spectra showed strong peaks at around 2204-2210 cm −1 , which correspond to the stretching vibrations of the carbonnitrogen triple bond (-C≡N) in the cyanide group.These absorption bands are indicative of the presence of the cyanide group in compounds 1-6.
The proton nuclear magnetic resonance ( 1 H-NMR) spectra of compounds 1-6 exhibit characteristic signals associated with specific proton environments, including the proton at the 5-position and the -NH2 group.In the 1 H-NMR spectra, a characteristic singlet signal is observed at 7.09-7.25 ppm for the proton at the 5-position of compounds 1-6.The -NH2 peaks of compounds 1-6 appear as a broad singlet at 5.30-5.38 ppm.The mass spectra of compounds 1-6 exhibit protonated molecular ions and, in some cases, sodium adducts.Additionally, compounds 3 and 6 show chlorine isotopes ( 35 Cl and 37 Cl) in their mass spectra.In brief, the infrared (IR) spectral analysis of 1-6 revealed characteristic absorption bands associated with the presence of specific functional groups, namely the amino (N-H) and cyanide (-CN) groups.The amino (N-H) group in 1-6 exhibited distinctive stretching vibrations in the IR spectra.The N-H stretching bands were observed in the range of 3412-3487 cm −1 and 3300-3368 cm −1 .These absorption bands arise from the stretching motion of the nitrogen-hydrogen bonds in the amino group.The broad nature of these bands is typical for N-H stretching vibrations.Additionally, the N-H bending vibrations of the amino group were observed in the IR spectra of 1-6.The N-H bending bands appeared in the range of 1606-1654 cm −1 .These absorption bands result from the bending motion of the nitrogen-hydrogen bonds in the amino group.The presence of these bands further confirms the presence of the amino group in the synthesized compounds (1-6).Furthermore, the cyanide (-CN) groups in compounds 1-6 exhibited characteristic absorption bands in the IR spectra.The IR spectra showed strong peaks at around 2204-2210 cm −1 , which correspond to the stretching vibrations of the carbon-nitrogen triple bond (-C≡N) in the cyanide group.These absorption bands are indicative of the presence of the cyanide group in compounds 1-6.
The proton nuclear magnetic resonance ( 1 H-NMR) spectra of compounds 1-6 exhibit characteristic signals associated with specific proton environments, including the proton at the 5-position and the -NH 2 group.In the 1 H-NMR spectra, a characteristic singlet signal is observed at 7.09-7.25 ppm for the proton at the 5-position of compounds 1-6.The -NH 2 peaks of compounds 1-6 appear as a broad singlet at 5.30-5.38 ppm.The mass spectra of compounds 1-6 exhibit protonated molecular ions and, in some cases, sodium adducts.Additionally, compounds 3 and 6 show chlorine isotopes ( 35 Cl and 37 Cl) in their mass spectra.

Photophysical Properties of APNs (1-6)
The fluorescence spectra of the synthesized APNs (1-6) in different solvents (DCM, DMSO, MeOH, THF, and Toluene) at a concentration of 1.45 × 10 −8 M are shown in Figure 2. The fluorescence emission for each compound (1-6) is summarized in Table 2.As shown in Table 2, we observe different emission maximum values for each compound in different solvent systems.The varying λ max values suggest that different solvents can influence the energy levels and electronic transitions involved in the fluorescence process.Solvents with different polarity and dielectric constants interacted differently with compounds 1-6, leading to shifts in the emission maximum.
Several interesting observations can be made upon analyzing the emission maxima (λem) of compounds 1-6 in different solvents.As shown in Table 2, all six compounds exhibit similar trends in their fluorescence properties across the different solvents.This suggests that the core structure, compound 1, significantly determines the overall fluorescence behavior.In all five solvents, all the compounds (1-6) give more or less similar fluorescence properties.A very little red shift is observed for polar solvents as well as electron-withdrawing/containing groups.When dissolved in dimethyl sulfoxide (DMSO), all compounds undergo a significant red shift compared to the other solvents.The emission maximum range is between 420 and 433 nm in DMSO, indicating a shift towards longer wavelengths.This red shift can be attributed to the polar nature of DMSO, which stabilizes charge-separated states and polar excited states, resulting in a longer-wavelength emission.Among the six compounds, compound 3 consistently exhibits higher emission maximum values in all solvents.This implies that compound 3 has a stronger ability to absorb light energy and undergo efficient electronic transitions, leading to enhanced fluorescence.The specific substituents, such as the chloro groups, present in compound 3 likely contribute to its favorable electronic properties.Compound 6 shows similar fluorescence behavior to compound 3, as both compounds exhibit relatively higher emission maximum values compared to the other compounds.This suggests that the specific substitution of chloro groups in compound 6, similar to compound 3, contributes to its enhanced fluorescence properties.To summarize, the fluorescence properties of compounds 1-6 reveal intriguing patterns.
similar fluorescence behavior to compound 3, as both compounds exhibit relatively higher emission maximum values compared to the other compounds.This suggests that the specific substitution of chloro groups in compound 6, similar to compound 3, contributes to its enhanced fluorescence properties.To summarize, the fluorescence properties of compounds 1-6 reveal intriguing patterns.While all the APNs (1-6) exhibit similarities in their fluorescence behavior, the choice of solvent has a significant influence on the emission maximum values (Figure 3).The solvents tetrahydrofuran (THF, 407-418 nm) and methanol (MeOH, 410-419 nm) display a pronounced red shift compared to dichloromethane (DCM, 396-416 nm) and toluene (397-405 nm).Additionally, dimethyl sulfoxide (DMSO, 420-433 nm) induces an exceptional red shift for all compounds.Compounds 3 and 6 consistently exhibit higher emission maximum values across all solvents, indicating their superior fluorescence properties.These findings provide valuable insights into the structure-property relationships and solvatochromic effects in the fluorescence of these APNs (1-6).Besides the solvent effect, there is clear evidence of electron with/donating group effects on emission shifting.Figure 3 illustrates the fluorescence properties of the compounds in methanol (extension).Compound 1, without any substituents, exhibits an emission maximum at 416 nm.Substitutions of a 3-methoxy group in ring A (compound 2), a 4methoxy group in ring A (compound 5), and both a 3-methoxy group in ring A and a 4methoxy group in ring B (compound 4) result in blue shifts of approximately 1-6 nm, with emission maxima at 415, 411, and 410 nm, respectively.Conversely, compound 6, with a 3-methoxy group in ring A and a 4-chloro group in ring B, and compound 3, with a 4methoxy group in ring A and a 4-chloro group in ring B, exhibit red shifts of approximately 2-4 nm, with emission maxima at 418 and 420 nm, respectively.These observations highlight the influence of electron with/donating substitutions on the fluorescence properties of the APNs (1-6).The red and blue shifts observed in the APNs (1-6) have diverse applications.These shifts can be utilized to develop fluorescent probes for imaging and sensing applications, where the emission wavelengths can be tuned for specific targets.Compounds 1-6 can also be used in optical sensors to detect analytes or environmental parameters based on changes in emission spectra.Additionally, the red and blue shifts are valuable in energy transfer systems and can be applied in areas such as solar energy conversion and light harvesting.Overall, the red and blue shifts of the APNs (1-6) offer versatile applications in various fields, ranging from biological imaging to energy-related technologies.However, the analysis of compounds 1-6 reveals several significant findings for the optimization and development of APN therapeutics or fluorescent sensors.The choice of solvent influences the emission maximum values, suggesting the importance of solvent selection for tuning fluorescence properties.Specific substituents, such as chloro groups, contribute to enhanced fluorescence properties, as observed in compounds 3 and 6.Additionally, the position of methoxy groups (3-OCH3 vs. 4-OCH3) affects the emission maxima, indicating their role in determining donor/acceptor sites.These findings offer valuable insights for designing APN-based compounds with improved fluorescence behavior.While all the APNs (1-6) exhibit similarities in their fluorescence behavior, the choice of solvent has a significant influence on the emission maximum values (Figure 3).The solvents tetrahydrofuran (THF, 407-418 nm) and methanol (MeOH, 410-419 nm) display a pronounced red shift compared to dichloromethane (DCM, 396-416 nm) and toluene (397-405 nm).Additionally, dimethyl sulfoxide (DMSO, 420-433 nm) induces an exceptional red shift for all compounds.Compounds 3 and 6 consistently exhibit higher emission maximum values across all solvents, indicating their superior fluorescence properties.These findings provide valuable insights into the structure-property relationships and solvatochromic effects in the fluorescence of these APNs (1-6).Besides the solvent effect, there is clear evidence of electron with/donating group effects on emission shifting.Figure 3 illustrates the fluorescence properties of the compounds in methanol (extension).Compound 1, without any substituents, exhibits an emission maximum at 416 nm.Substitutions of a 3-methoxy group in ring A (compound 2), a 4-methoxy group in ring A (compound 5), and both a 3-methoxy group in ring A and a 4-methoxy group in ring B (compound 4) result in blue shifts of approximately 1-6 nm, with emission maxima at 415, 411, and 410 nm, respectively.Conversely, compound 6, with a 3-methoxy group in ring A and a 4-chloro group in ring B, and compound 3, with a 4-methoxy group in ring A and a 4-chloro group in ring B, exhibit red shifts of approximately 2-4 nm, with emission maxima at 418 and 420 nm, respectively.These observations highlight the influence of electron with/donating substitutions on the fluorescence properties of the APNs (1-6).The red and blue shifts observed in the APNs (1-6) have diverse applications.These shifts can be utilized to develop fluorescent probes for imaging and sensing applications, where the emission wavelengths can be tuned for specific targets.Compounds 1-6 can also be used in optical sensors to detect analytes or environmental parameters based on changes in emission spectra.Additionally, the red and blue shifts are valuable in energy transfer systems and can be applied in areas such as solar energy conversion and light harvesting.Overall, the red and blue shifts of the APNs (1-6) offer versatile applications in various fields, ranging from biological imaging to energy-related technologies.However, the analysis of compounds 1-6 reveals several significant findings for the optimization and development of APN therapeutics or fluorescent sensors.The choice of solvent influences the emission maximum values, suggesting the importance of solvent selection for tuning fluorescence properties.Specific substituents, such as chloro groups, contribute to enhanced fluorescence properties, as observed in compounds 3 and 6.Additionally, the position of methoxy groups (3-OCH 3 vs.4-OCH 3 ) affects the emission maxima, indicating their role in determining donor/acceptor sites.These findings offer valuable insights for designing APN-based compounds with improved fluorescence behavior.

Quantum Chemical TD-DFT Analysis of APNs (1-6)
In order to gain a deep insight into the structure of the synthesized compounds 1-6, a time-dependent density functional theory (TD-DFT) approach was conducted to model the electronic fluorescence spectra of the synthesized APNs (1-6) and compare them with the experimental ones.A chemical species with a small HOMO-LUMO energy gap is highly polarizable and requires only a small amount of energy for excitation.On the other

Quantum Chemical TD-DFT Analysis of APNs (1-6)
In order to gain a deep insight into the structure of the synthesized compounds 1-6, a time-dependent density functional theory (TD-DFT) approach was conducted to model the electronic fluorescence spectra of the synthesized APNs (1-6) and compare them with the experimental ones.A chemical species with a small HOMO-LUMO energy gap is highly polarizable and requires only a small amount of energy for excitation.On the other hand, a large HOMO-LUMO gap indicates that the species is highly stable and has low reactivity.The molecular electrostatic surface potentials, HOMO, and LUMO of the APNs (1-6) are shown in Figures 4 and 5, and the important HOMO, LUMO, and their related values are summarized in Table 3.The negative electrostatic potential (ESP) of the species is shown in red, indicating the relative polarities and reactive sites.The order of increasing electrostatic potential (i.e., the highest negative value) is red > orange > yellow > green > blue.The yellow color indicates the slightly rich electron regions, and the green color reflects more neutral zones.The HOMO-LUMO transition implies an electron density transfer from the ring to the lone pairs of atoms on the main chain.This explains the significant degree of intramolecular charge transfer by the π-π and n-π transitions.
Molecules 2024, 29, x FOR PEER REVIEW 8 of hand, a large HOMO-LUMO gap indicates that the species is highly stable and has lo reactivity.The molecular electrostatic surface potentials, HOMO, and LUMO of the AP (1-6) are shown in Figures 4 and 5, and the important HOMO, LUMO, and their relat values are summarized in Table 3.The negative electrostatic potential (ESP) of the spec is shown in red, indicating the relative polarities and reactive sites.The order of increasi electrostatic potential (i.e., the highest negative value) is red > orange > yellow > green blue.The yellow color indicates the slightly rich electron regions, and the green co reflects more neutral zones.The HOMO-LUMO transition implies an electron dens transfer from the ring to the lone pairs of atoms on the main chain.This explains t significant degree of intramolecular charge transfer by the π-π and n-π transitions.
(a) (b) (c)     The results obtained from Table 3 provide valuable insights into the electronic properties of the compounds, specifically the HOMO-LUMO energy levels and the electronegativity (χ) values.The HOMO-LUMO energy gap is a crucial parameter that reflects the electronic structure and potential reactivity of compounds.In this study, all the compounds displayed comparable HOMO-LUMO energy gaps, ranging from 3.441 eV to 3.617 eV.This indicates a consistent degree of electronic delocalization and suggests that these compounds may exhibit similar reactivity patterns.The property of attracting electrons, known as electronegativity (χ), serves as a gauge for predicting chemical reactivity.The electronegativity values, ranging from 4.235 eV to 4.435 eV, highlight the varying electronattracting capabilities among atoms in the synthesized APNs (1)(2)(3)(4)(5)(6).These values offer a deeper understanding of the compounds' electronic characteristics and their propensity for electron transfer reactions.The similarity in the HOMO-LUMO energy gaps and the range of electronegativity values observed in the compounds (1-6) suggest that they may share comparable electronic properties.This information is valuable for understanding their potential reactivity and applications.The chemical potential (µ) for an electron in a molecule represents its ability to be either added to or removed from the molecule, and it is a critical parameter in understanding the electronic behavior and reactivity of chemical systems.The chemical potential (µ) values, ranging from −4.235 eV to −4.435 eV, highlight the varying electron-attracting capabilities among atoms in compounds 1-6.The dipole moment of a molecule can significantly influence its emission spectra.When a molecule moves from a higher to a lower energy state, such as in fluorescence or phosphorescence, the dipole moment is crucial in determining the intensity and shape of the emitted spectrum.Additionally, solvent polarity can modulate a molecule's dipole moment, leading to changes in the emission spectra.It can be seen that the dipole moment values are higher for compounds 3, 5, and 6 (11.787, 6.726, and 8.098, respectively).These values influence their emission spectra to undergo a red shift at higher wavelengths in the DMSO solvent (309/414, 316/420, and 345/427 nm, respectively) compared to other less polar solvents, as shown in Table 4.
The TD-DFT analysis of compounds 1-6 provides valuable insights for the development of APN therapeutics or fluorescent sensors.The similar HOMO-LUMO energy gaps and range of electronegativity values suggest comparable electronic properties among the compounds.The chemical potential values indicate varying electron-attracting capabilities.The higher dipole moment values of compounds 3, 5, and 6 suggest the potential for red-shifted emission spectra in polar solvents.Additionally, the position of methoxy groups influences donor/acceptor sites.These findings aid in optimizing the APN compounds (1-6) for the desired properties and applications.energy gaps and range of electronegativity values suggest comparable electronic properties among the compounds.The chemical potential values indicate varying electron-attracting capabilities.The higher dipole moment values of compounds 3, 5, and 6 suggest the potential for red-shifted emission spectra in polar solvents.Additionally, the position of methoxy groups influences donor/acceptor sites.These findings aid in optimizing the APN compounds (1-6) for the desired properties and applications.The geometry-optimized structures of APNs 1-6 were further TD-DFT-calculated by computing five singlet excited states on top of the structures obtained at the TD-DFT/b3lyp/6-311++g(d,p) level of theory with the solvent polarizable continuum model (PCM) in toluene, tetrahydrofuran (THF), dichloromethane (DCM), dimethyl sulfoxide (DMSO), and methanol solvents, as shown in Figures 6 and 7.
The spectra were plotted by applying a Gaussian broadening of 0.333 eV half-width at half-height.The fluorescence emission spectra exhibit two bands of compounds 1-6 in toluene, THF, DCM, DMSO, and methanol solvents.These bands are at 299−325 nm and 394−427 nm, respectively, as summarized in Table 4.The short-wavelength region in 299−325 nm is assigned to the n-π* electron transition of the periphery of the APN moieties.The region 394−427 nm is consistent with the π−π* electron transition due to charge transfer emission (Figures 8 and 9).The geometry-optimized structures of APNs 1-6 were further TD-DFT-calculated by computing five singlet excited states on top of the structures obtained at the TD-DFT/b3lyp/6-311++g(d,p) level of theory with the solvent polarizable continuum model (PCM) in toluene, tetrahydrofuran (THF), dichloromethane (DCM), dimethyl sulfoxide (DMSO), and methanol solvents, as shown in Figures 6 and 7.

TD-DFT Emission Maxima (λ em , nm) Calculated by Using the TD-SCF-B3LYP/6311++G(d,p) Level of Theory in Different Solvent
The spectra were plotted by applying a Gaussian broadening of 0.333 eV half-width at half-height.The fluorescence emission spectra exhibit two bands of compounds 1-6 in toluene, THF, DCM, DMSO, and methanol solvents.These bands are at 299−325 nm and 394−427 nm, respectively, as summarized in Table 4.The short-wavelength region in 299−325 nm is assigned to the n-π* electron transition of the periphery of the APN moieties.The region 394−427 nm is consistent with the π−π* electron transition due to charge transfer emission (Figures 8 and 9).
As depicted, the TD-DFT-calculated electronic fluorescence emission spectra of compounds 1-6 were obtained at the TD-DFT/B3LYP/6-311++g(d,p) basis set level of theory in the MeOH (Figure 8) and DMSO (Figure 9) solvent systems at 298 K.For compound 1, Figure 8 shows two broad bands at 408.18 nm (excitation energy of 3.037 eV and oscillator strength f = 0.640 for HOMO to LUMO) and 309 nm (excitation energy of 4.009 eV and oscillator strength f = 0.412).Similarly, in Figure 9, compound 1 displays two broad bands at 408.14 nm (excitation energy of 3.037 eV and oscillator strength f = 0.640 for HOMO to LUMO) and 309 nm (excitation energy of 4.009 eV and oscillator strength f = 0.412 for HOMO-2 to LUMO).For compound 2, Figure 8 shows two broad bands at 410.30 nm (excitation energy of 3.022 eV and oscillator strength f = 0.606 for HOMO to LUMO) and 306 nm (excitation energy of 4.050 eV and oscillator strength f = 0.415 for HOMO-4 to LUMO).Similarly, in Figure 9, compound 2 exhibits two broad bands at 410.72 nm (excitation energy of 3.018 eV and oscillator strength f = 0.610 for HOMO to LUMO) and 306.23 nm (excitation energy of 4.048 eV and oscillator strength f = 0.416 for HOMO-4 to LUMO).For compound 3, Figure 8 shows two broad bands at 414.07 nm (excitation energy of 2.994 eV and oscillator strength f = 0.596 for HOMO to LUMO) and 309.38 nm (excitation energy of 4.007 eV and oscillator strength f = 0.439 for HOMO-3 to LUMO).Similarly, in Figure 9, compound 3 exhibits two broad bands at 410.47 nm (excitation energy of 2.991 eV and oscillator strength f = 0.601 for HOMO to LUMO) and 309.54 nm (excitation energy of 4.005 eV and oscillator strength f = 0.440 for HOMO-3 to LUMO).For compound 4, Figure 8 shows two broad bands at 411.20 nm (excitation energy of 3.015 eV and oscillator strength f = 0.694 for HOMO to LUMO) and 305.81 nm (excitation energy of 4.007 eV and oscillator strength f = 0.486 for HOMO-3 to LUMO).Similarly, in Figure 9, compound 4 exhibits two broad bands at 411.68 nm (excitation energy of 3.011 eV and oscillator strength f = 0.698 for HOMO to LUMO) and 306.02 nm (excitation energy of 4.051 eV and oscillator strength f = 0.487 for HOMO-3 to LUMO).For compound 5, Figure 8 displays two broad bands at 420.37 nm (excitation energy of 2.949 eV and oscillator strength f = 0.905 for HOMO to LUMO) and 316.38 nm (excitation energy of 3.918 eV and oscillator strength f = 0.362 for HOMO-2 to LUMO).Similarly, in Figure 9, compound 5 exhibits two broad bands at 420.88 nm (excitation energy of 2.945 eV and oscillator strength f = 0.912 for HOMO to LUMO) and 316.52 nm (excitation energy of 3.917 eV and oscillator strength f = 0.363 for HOMO-2 to LUMO).For compound 6, Figure 8 shows two broad bands at 426.66 nm (excitation energy of 2.905 eV and oscillator strength f = 0.866 for HOMO to LUMO) and 324.79 nm (excitation energy of 3.817 eV and oscillator strength f = 0.509 for HOMO-2 to LUMO).Similarly, in Figure 9, compound 6 exhibits two broad bands at 427.16 nm (excitation energy of 2.902 eV and oscillator strength f = 0.873 for HOMO to LUMO) and 324.90 nm (excitation energy of 3.816 eV and oscillator strength f = 0.510 for HOMO-2 to LUMO).The emission bands experienced a red shift when the solvent was changed from non-polar toluene to polar DMSO or a methanol solvent system.The highest red shift was observed for compounds 3, 5, and 6 from 304/401 to 309/414, 311/404 to 316/420, and 320/412 to 325/427, respectively.As depicted, the TD-DFT-calculated electronic fluorescence emission spectra of compounds 1-6 were obtained at the TD-DFT/B3LYP/6-311++g(d,p) basis set level of theory in the MeOH (Figure 8) and DMSO (Figure 9) solvent systems at 298 K.For compound 1, Figure 8 shows two broad bands at 408.18 nm (excitation energy of 3.037 eV and oscillator strength f = 0.640 for HOMO to LUMO) and 309 nm (excitation energy of 4.009 eV and oscillator strength f = 0.412).Similarly, in Figure 9, compound 1 displays two broad bands at 408.14 nm (excitation energy of 3.037 eV and oscillator strength f = 0.640

General
The experiments were conducted using commercially available reagents and solvents without any additional purification.Melting points were measured using a Barnstead electrothermal digital melting point apparatus (model IA9100, BIBBY Scientific Limited, Staffordshire, UK).IR spectra were recorded using a Jasco FT/IR-6600 spectrometer (Tokyo, Japan).NMR spectra were obtained using a Bruker 700 MHz NMR spectrometry instrument (Zurich, Switzerland); 1 H NMR, 13 C NMR, and 2D spectra were determined on a Bruker (700 MHz).Chemical shifts are expressed as δ values (ppm) using tetramethyl silane (TMS) as an internal reference.Signals are indicated by the following abbreviations: s = singlet, d = doublet, t = triplet, q = quartet, m = multiple, br = broad, dd = doublet of doublet, ddd = doublet of doublet of doublet, td = triplet of doublet, dt = doublet of triplet, and qd = quartet of doublet.Electrospray ionization (ESI) mass spectrometry (MS) experiments were carried out using an Agilent 6320 ion trap mass spectrometer equipped with an ESI ion source (Agilent Technologies, Palo Alto, CA, USA).High-resolution mass spectrometry was performed using an HRMS JMS 700 JEOL mass spectrometry instrument (Tokyo, Japan).The reagents were RPMI-1640 medium, MTT, and DMSO (Sigma Co., St. Louis, MO, USA), as well as fetal bovine serum (GIBCO, Cambridge, UK).The cell lines (MDA-MB-231, association number HTB-26 ™ ; and MCF-7, association number HTB-22) were obtained from the ATCC database via the Holding company for biological products and vaccines (VACSERA), Cairo, Egypt.

General Synthetic Method for the Synthesis of 1-6
Compounds 1-6 were synthesized according to the previously reported method [35].In the first step, chalcones (9) were synthesized using various aldehydes (7, 10 mmol) and acetophenones (8, 10 mmol) under a basic (10% alcoholic NaOH) condition in ethanol [34] at room temperature and were used for the second step without further purification.In the second step, each chalcone (1 mmol) was reacted with 1 equivalent of malononitrile and ammonium acetate (3 equiv.)under reflux overnight in absolute ethanol to obtain 2-amino-4,6-diphenylnicotinonitrile derivatives 1-6.

Cytotoxicity Assay of APNs 1-6
The cytotoxic activity of compounds 1-6 was evaluated against mammary gland breast cancer (MCF-7) and breast cancer (MDA-MB-231) using the MTT assay as previously described [39,40].The cell lines were cultured in RPMI-1640 medium with 10% fetal bovine serum.Antibiotics (100 units/mL of penicillin and 100 µg/mL of streptomycin) were added at 37 • C in a 5% CO 2 incubator.The cell lines were seeded in a 96-well plate at a density of 1.0 × 10 4 cells/well at 37 • C for 48 h under 5% CO 2 .After incubation, the cells were treated with different concentrations of the compounds and incubated for 24 h.After 24 h of drug treatment, 20 µL of MTT solution at 5mg/mL was added and incubated for 4 h.Dimethyl sulfoxide (DMSO) in a volume of 100 µL was added to each well to dissolve the purple formazan formed.The colorimetric assay was measured and recorded at an absorbance of 570 nm using a plate reader (EXL 800, Winooski, VT, USA).The relative cell viability in percentage was calculated as (A570 of treated samples/A570 of untreated sample) × 100.

Computational Studies of APNs 1-6
The initial molecular structures of all of the examined structures were drawn using the GaussView 6.0.16 program [41] and optimized at the DFT/b3lyp/6-311++g(d,p) level using Gaussian 16, Revision C.01 [42].Geometry-optimized structures were subjected to further TD-DFT calculation using Gaussian 16, Revision C.01 by computing 5 singlet excited states on top of the structures obtained at the TD-DFT/b3lyp/6-311++g(d,p) level of theory with the solvent polarizable continuum model (PCM) in toluene, tetrahydrofuran (THF), dichloromethane (DCM), dimethyl sulfoxide (DMSO), and methanol solvents.A vibrational analysis was carried out for each optimized molecule to ensure that they were at a vibrational energy minimum and had no imaginary frequencies.The Frontier Molecular Orbital (FMO) in terms of the energy distribution from HOMO (highest occupied molecular orbital) to LUMO (lowest unoccupied molecular orbital) and a molecular electrostatic potential (MEP) map were calculated using the GaussView 6.0.16 program.The disparity in energy levels between the highest occupied molecular orbital (HOMO) and the lowest unoccupied molecular orbital (LUMO), commonly referred to as the H-L energy gap, correlates with the polarizability of a species and was calculated according to Koopmans' theorem [43].Several chemical descriptors, such as energy gap (E Gap ), ionization potential (IP), electron affinity (EA), chemical potential (µ), electronegativity (χ), hardness (η), softness (σ), and electrophilicity (ω), were calculated using the following equations: E Gap (eV) = (E LUMO − E HOMO ); IP (eV) = −E HOMO ; EA (eV) = −E LUMO ; µ (eV) = (IP + EA)/2; χ = − µ; η = (IP − EA)/2; σ = 1/η; ω = µ 2 /2η where µ and η were used to derive the electrophilicity indexes.

Figure 7 .
Figure 7.Comparison of the TD-DFT-calculated electronic fluorescence emission spectra of compounds 1-6 at the TD-DFT/B3LYP/6-311++g(d,p) basis set level of theory in DMSO and methanol solvent systems.