Synthesis and Photophysical Properties of α-(N-Biphenyl)-Substituted 2,2′-Bipyridine-Based Push–Pull Fluorophores

A series of new α-(N-biphenyl)-substituted 2,2′-bipyridines were obtained through the combination of the ipso-nucleophilic aromatic substitution of the C5-cyano group, aza-Diels–Alder and Suzuki cross-coupling reactions, starting from 5-cyano-1,2,4-triazines. For the obtained compounds, photophysical and fluorosolvatochromic properties were studied. Fluorophores 3l and 3b demonstrated unexpected AIEE activity, while 3a and 3h showed promising nitroexplosive detection abilities.

Some limitations of the herein-reported method should be mentioned. Previously we were unable to introduce residues of [1,1 -biphenyl]-4-amines 4a,b into the 1,2,4-triazine core [24]. A possible reason for the low reactivity of 4-aminobiphenyls is the high delocalization of the electron pair of the nitrogen atom due to the resonance with the extended polyaromatic system. In this regard, we developed an alternative approach towards α-arylamino-2,2 -bipyridines 3a-l based on the use of commercially available 3-and 4-bromoanilines. As a result, the ipso-nucleophilic aromatic substitution of the C5-cyano group in 1,2,4-triazines resulted in the formation of intermediate products 5a-c, while subsequent aza-Diels-Alder reactions resulted in bromoarene-substituted 2,2 -bipyridines 6a-c. The final products 3a-l were obtained due to Suzuki cross-coupling reactions between 2,2 -bipyridines 6a-c and the corresponding arylboronic acid. In this case, the choice of the solvent system turned out to be important for the success of the cross-coupling reaction. In particular, it was not possible to satisfactorily obtain product 3 by a fairly traditional mixture of toluene, water, and ethanol, and a large number of unidentified impurities were presented in the reaction mixture. However, in a THF:water = 1:1 mixture this reaction proceeded smoothly to afford the desired products in up to 74% yields.
the solvent system turned out to be important for the success of the cross-coupling reaction. In particular, it was not possible to satisfactorily obtain product 3 by a fairly traditional mixture of toluene, water, and ethanol, and a large number of unidentified impurities were presented in the reaction mixture. However, in a THF:water = 1:1 mixture this reaction proceeded smoothly to afford the desired products in up to 74% yields. Scheme 1. Synthetic routes toward 3a-l.
The structures of the products 3a-l were confirmed by the data of 1 H and 13 C NMR spectroscopy, as well as mass spectrometry and elemental analysis. Thus, in 1 H NMR spectra of the obtained products, the signals of protons of the 2-pyridyl residue, bipyridine aromatic substituents and biphenyl fragments, as well as a broadened singlet of the N-H group proton in the region of 6.72-7.04 ppm, were observed. In addition, the structure of key 2,2′-bipyridine 3a was confirmed by means of single crystal X-ray diffraction analysis ( Figure 2). According to the X-ray data, compound 3a crystallizes in the centrosymmetric space group of the monoclinic system. The bond distances and angles in the molecule are near standard values. The molecule is nonplanar and only the bipyridine atoms are placed in a plane with trans-placed nitrogen atoms. The nitrogen atom of the diarylamino-moiety is planar and the NH-group is not involved in the formation of the H-bond. No significantly shortened intermolecular contacts in the crystal were observed.  The structures of the products 3a-l were confirmed by the data of 1 H and 13 C NMR spectroscopy, as well as mass spectrometry and elemental analysis. Thus, in 1 H NMR spectra of the obtained products, the signals of protons of the 2-pyridyl residue, bipyridine aromatic substituents and biphenyl fragments, as well as a broadened singlet of the N-H group proton in the region of 6.72-7.04 ppm, were observed. In addition, the structure of key 2,2 -bipyridine 3a was confirmed by means of single crystal X-ray diffraction analysis ( Figure 2). According to the X-ray data, compound 3a crystallizes in the centrosymmetric space group of the monoclinic system. The bond distances and angles in the molecule are near standard values. The molecule is nonplanar and only the bipyridine atoms are placed in a plane with trans-placed nitrogen atoms. The nitrogen atom of the diarylamino-moiety is planar and the NH-group is not involved in the formation of the H-bond. No significantly shortened intermolecular contacts in the crystal were observed.
the solvent system turned out to be important for the success of the cross-coupling reaction. In particular, it was not possible to satisfactorily obtain product 3 by a fairly traditional mixture of toluene, water, and ethanol, and a large number of unidentified impurities were presented in the reaction mixture. However, in a THF:water = 1:1 mixture this reaction proceeded smoothly to afford the desired products in up to 74% yields. The structures of the products 3a-l were confirmed by the data of 1 H and 13 C NMR spectroscopy, as well as mass spectrometry and elemental analysis. Thus, in 1 H NMR spectra of the obtained products, the signals of protons of the 2-pyridyl residue, bipyridine aromatic substituents and biphenyl fragments, as well as a broadened singlet of the N-H group proton in the region of 6.72-7.04 ppm, were observed. In addition, the structure of key 2,2′-bipyridine 3a was confirmed by means of single crystal X-ray diffraction analysis ( Figure 2). According to the X-ray data, compound 3a crystallizes in the centrosymmetric space group of the monoclinic system. The bond distances and angles in the molecule are near standard values. The molecule is nonplanar and only the bipyridine atoms are placed in a plane with trans-placed nitrogen atoms. The nitrogen atom of the diarylamino-moiety is planar and the NH-group is not involved in the formation of the H-bond. No significantly shortened intermolecular contacts in the crystal were observed.

Photophysical Studies
As a next step, the photophysical properties of the obtained α-biphenylamino-2,2bipyridines 3a-l were studied (Table 1 and Table S1; Figure 3 and Figure S31). These compounds exhibited an intense blue-to-green fluorescence with emission maxima in the range of 443-505 nm and fluorescence quantum yields up to 49.1% in THF solutions. Compared to previously described unsubstituted analogs (Table 1, Entries 1-4 and 12-15), as well as 3-and 4-bromophenyl-substituted precursors (Entries 11 and 22, 23), the extension of the conjugation system in the aniline moieties in 3a-l expectedly redshifted the emission maxima with the highest values in the case of 4-biphenylamino derivatives. The Stokes shift values are either the same level as described earlier, or significantly exceed them and can reach up to 9670.29 cm −1 or 169 nm (Entry 10). This difference is very significant compared to α-phenylamino 2,2 -bipyridines (Entry 1 and 12). The highest quantum yields among all the products were observed for compound 3a (49%, Entry 5), 3b (48%, Entry 16), and 3d (44%, Entry 18), functionalized at the meta-position of the aniline unit. These values are comparable with the quantum yields of α-arylamino-2,2 -bipyridines that are not functionalized with additional aromatic moieties. However, a significant decrease in quantum yields was observed in the case of some para-substituted derivatives (Entries 8-10). Table 1. Photophysical properties of α-arylamino-2,2 -bipyridines 3a-l in THF solution.

Photophysical Studies
As a next step, the photophysical properties of the obtained α-biphenylamino-2,2′bipyridines 3a-l were studied (Tables 1 and S1; Figures 3 and S31). These compounds exhibited an intense blue-to-green fluorescence with emission maxima in the range of 443-505 nm and fluorescence quantum yields up to 49.1% in THF solutions. Compared to previously described unsubstituted analogs (Table 1, Entries 1-4 and 12-15), as well as 3-and 4-bromophenyl-substituted precursors (Entries 11 and 22, 23), the extension of the conjugation system in the aniline moieties in 3a-l expectedly redshifted the emission maxima with the highest values in the case of 4-biphenylamino derivatives. The Stokes shift values are either the same level as described earlier, or significantly exceed them and can reach up to 9670,29 cm −1 or 169 nm (Entry 10). This difference is very significant compared to αphenylamino 2,2′-bipyridines (Entry 1 and 12). The highest quantum yields among all the products were observed for compound 3a (49%, Entry 5), 3b (48%, Entry 16), and 3d (44%, Entry 18), functionalized at the meta-position of the aniline unit. These values are comparable with the quantum yields of α-arylamino-2,2′-bipyridines that are not functionalized with additional aromatic moieties. However, a significant decrease in quantum yields was observed in the case of some para-substituted derivatives (Entries 8-10). It is worth noting the change in the photophysical properties of α-arylamino-2,2bipyridines bearing methoxy-(Entry 14) or 4-methoxyphenyl groups (Entry 21). In this case, the introduction of an additional 1,3-phenylene fragment into the bipyridine core results in a blueshift of the emission maximum by 19 nm and the reduction of the Stokes shift value (7543.99 cm −1 vs. 7056.13 cm −1 ). However, fluorescence quantum yield increased from 4% to 21%. Therefore, the introduction of additional aromatic substituents into the α-aniline fragment of the 2,2 -bipyridine core could be used as a tool to tune the photophysical properties and is of particular interest.  It is worth noting the change in the photophysical properties of α-arylamino-2,2′bipyridines bearing methoxy-(Entry 14) or 4-methoxyphenyl groups (Entry 21). In this case, the introduction of an additional 1,3-phenylene fragment into the bipyridine core results in a blueshift of the emission maximum by 19 nm and the reduction of the Stokes shift value (7543,99 cm −1 vs. 7056,13 cm −1 ). However, fluorescence quantum yield increased from 4% to 21%. Therefore, the introduction of additional aromatic substituents into the α-aniline fragment of the 2,2′-bipyridine core could be used as a tool to tune the photophysical properties and is of particular interest.

Studies of Fluorosolvatochromism
In our recent works, we have already demonstrated a well-pronounced fluorosolvatochromic behavior of 2,2 -bipyridines functionalized with donor substituents, including aniline residues [22,23,25,26]. The herein-reported compounds 3a-l also exhibited a pronounced fluorosolvatochromism, which was demonstrated for the most representative compounds 3b,g,i,l (Figure 4, Figure 5 and Figures S32-S35). It is worth noting the change in the photophysical properties of α-arylamino-2,2′bipyridines bearing methoxy-(Entry 14) or 4-methoxyphenyl groups (Entry 21). In this case, the introduction of an additional 1,3-phenylene fragment into the bipyridine core results in a blueshift of the emission maximum by 19 nm and the reduction of the Stokes shift value (7543,99 cm −1 vs. 7056,13 cm −1 ). However, fluorescence quantum yield increased from 4% to 21%. Therefore, the introduction of additional aromatic substituents into the α-aniline fragment of the 2,2′-bipyridine core could be used as a tool to tune the photophysical properties and is of particular interest.

Studies of Fluorosolvatochromism
In our recent works, we have already demonstrated a well-pronounced fluorosolvatochromic behavior of 2,2′-bipyridines functionalized with donor substituents, including aniline residues [22,23,25,26]. The herein-reported compounds 3a-l also exhibited a pronounced fluorosolvatochromism, which was demonstrated for the most representative compounds 3b,g,i,l (Figures 4, 5 and S32-S35).  Solvent polarity did not significantly affect the absorption spectra, while it influenced significantly the fluorescence spectra of the fluorophores 3b,g,i,l (Figures 4, 5 and S32-S35, Tables S2-S5). Thus, a gradual increase of the solvent polarity from cyclohexane to DMSO led to a gradual redshift of the fluorescence maxima with an increase of the Stokes Solvent polarity did not significantly affect the absorption spectra, while it influenced significantly the fluorescence spectra of the fluorophores 3b,g,i,l (Figures 4, 5 and S32-S35,  Tables S2-S5). Thus, a gradual increase of the solvent polarity from cyclohexane to DMSO led to a gradual redshift of the fluorescence maxima with an increase of the Stokes shift values. For example, the observed fluorescence maximum for 3i in cyclohexane was 438 nm, and the Stokes shift was 99 nm, while in DMSO these values were 515 nm and 176 nm, respectively. In the case of compound 3l, the use of more polar solvents (DMF, acetonitrile and methanol) resulted in a blueshift of the emission maxima relative to the emission in DMSO, while in a solvent row from cyclohexane to dichloromethane, an increase of the solvent polarity exhibited a redshift of the emission maxima. It is worth mentioning that the difference between the largest and smallest values of the emission maximum, in the case of 3b,g,i,l (69 nm, 67 nm, 107 nm and 112 nm, respectively, Figures S32-S35), is greater than the same difference (38-70 nm) for the previously reported aniline containing 2,2 -bipyridines [22,23].
To estimate the push-pull character of the obtained fluorophores, a mathematical analysis of the obtained experimental data was carried out using the Lippert-Mataga equation (Equation (1)) [27][28][29]. We found that the introduction of additional aromatic fragments into the aniline residue in compounds 3b,g,i,l led to an increase in the difference between the dipole moments of the ground (µ G ) and excited (µ E ) states. As a result, we calculated ∆µ for 3b,g,i,l ( Table 2). These values are relatively high for the 2,2 -bipyridine type fluorophores, second only to some examples ( Figure S36) [22,25,26,30].
Equation (1). In the Lippert-Mataga equation (ν A and ν F are the wavenumbers (cm −1 ) of the absorption and emission, respectively, h is Planck's constant, c is the speed of light in vacuum, a is the radius of the cavity in which the fluorophore resides (4Å, [27]), µ E and µ G are the excited and ground state dipole moment, respectively. For a more detailed study of the effect of solvent polarity on the photophysical properties, a Lippert-Mataga plot was constructed, that is, the dependence of the Stokes shift (cm −1 ) of the fluorophore on the orientational polarizability of the solvent (∆f). This plot indicated that 3b,g,i,l demonstrated a linear dependence (R 2 > 0.90, Figure 6a and Table S6) only in the range of cyclohexane-DCM solvents-while in more polar solvents, the linearity was broken and there was a sharp drop in the Stokes shift values (Figure 6a, Table S7). Deviations from linearity in the Lippert-Mataga plots indicate the occurrence of some intermolecular interactions in these solvents, such as the hydrogen bonds formation, which is confirmed by a certain linearity in this case (R 2 = 0.69 − 0.99, Table S7), and can not be explained by traces of water in selected solvents due to the absence of these deviations in related α-arylamino-2,2 -bipyridines [22] (that is, the ones without the 1,3-or 1,4-phenylene unit). The protic nature of methanol could influence corresponding emission spectra as well. Thus, this unusual behavior is discussible.
Equation (2). The orientational polarizability of the solvent, where ε and n are the dielectric constant and the refraction index for the solvents, respectively. of some intermolecular interactions in these solvents, such as the hydrogen bonds formation, which is confirmed by a certain linearity in this case (R 2 = 0.69 − 0.99, Table S7), and can not be explained by traces of water in selected solvents due to the absence of these deviations in related α-arylamino-2,2′-bipyridines [22] (that is, the ones without the 1,3or 1,4-phenylene unit). The protic nature of methanol could influence corresponding emission spectra as well. Thus, this unusual behavior is discussible.
Equation (2). The orientational polarizability of the solvent, where ε and n are the dielectric constant and the refraction index for the solvents, respectively.
The fluorosolvatochromism of 3b,g,i,l correlates well with the solvent polarity scales according to Kosower [31,32] and Dimroth/Reichardt [33,34] (Table 3, parameters Z and ET (30), respectively), while some deviations were observed only in the case of the most polar solvents (DMF-methanol). Nevertheless, Figure 6b indicates that the dependence of the fluorescence maxima on the values of the empirical polarity factor ET(30) proceeds linearly (R 2 > 0.82, Tables S8), except for 3b,g,i in methanol, as well as for 3l in DMSO, DMF, acetonitrile, and methanol. This linear change in emission also confirms the phenomenon of fluorosolvatochromism (Table 3) [35].  The fluorosolvatochromism of 3b,g,i,l correlates well with the solvent polarity scales according to Kosower [31,32] and Dimroth/Reichardt [33,34] (Table 3, parameters Z and E T (30), respectively), while some deviations were observed only in the case of the most polar solvents (DMF-methanol). Nevertheless, Figure 6b indicates that the dependence of the fluorescence maxima on the values of the empirical polarity factor E T (30) proceeds linearly (R 2 > 0.82, Tables S8), except for 3b,g,i in methanol, as well as for 3l in DMSO, DMF, acetonitrile, and methanol. This linear change in emission also confirms the phenomenon of fluorosolvatochromism (Table 3) [35]. The electron-donating or accepting ability of organic substituents is an important parameter affecting not only their reactivity but also the pKa of ionizable groups and chromophore properties. These substituent properties are usually described by Hammett sigma constants, constants obtained by the ionization of substituted benzoic acids.
Although the values of these constants have been measured for the most common functional groups, data are not available for many important substituents. However, Peter Ertl published the results of a quantum chemical calculation of substituent descriptors compatible with Hammett sigma constants by using a more sophisticated methodology and a larger set of training data and presented a free web-based tool to calculate substituent descriptors compatible with Hammett sigma constants. This is available at: https: //peter-ertl.com/molecular/substituents/sigmas.html (accessed on 16 May 2022) [36].
The dependence of emission maxima on Hammett sigma constants for two groups of αbiphenylamino-2,2 -bipyridine fluorophores, paraand meta-substituted with respect to the aniline residue, were plotted ( Figure S37a,b). Except for 3g, meta-substituted fluorophores 3a-f showed an acceptor character ( Figure S37a). At the same time, a good linear correlation with σ m (R 2 = 0.92) was observed provided that such strongest electron-withdrawing substituents as Cl (#3) and Br (5c) are included in the analyzed sequence. For donorsubstituted compounds 3j, 3k, #4, #14 including the hydrogen-substituted compound 3h, as well as acceptor-substituted compounds 5a, 5b, #15, #13, a well-linear correlation with σ p (R 2 = 0.89) was observed ( Figure S37b). Thus, the correlation analysis of longwavelength emission maxima plotted as a function of the Hammett constants made it possible to obtain the relationship between the structure and photophysical properties of the resulting fluorophores.

DFT Studies
To understand the structure-photophysical properties relationship, we performed density functional theory (DFT) calculations with the help of the Gaussian-09 [37] program package at the B3LYP/6-31G*//PM6 level in acetonitrile (see Computational Details and Table S8 in Supplementary Materials) to obtain optimized molecular structures, energy levels of boundary molecular orbitals, dipole moments and molecular electrostatic potentials for the molecules 3b,g,i,l. The HOMO-orbitals were distributed on the substituted biphenyl residues acting as electron donors, while LUMO-orbitals were distributed on the 2,2 -bipyridine cores acting as electron acceptors (Figure 7). This facilitates the intermolecular charge transfer (ICT) process ("push-pull" effect) in a molecule and correlates well with the photophysical experimental data. According to the calculation, the maximum difference between the dipole moments in the ground and excited states ∆µ is more than 10D for the molecule 3l (Table S9), which is typical for the ICT state [38]. However, there are significant differences in the ∆µ values between those calculated and obtained via Lippert-Mataga equations for the rest of molecules 3b,g,i (Table S9). The calculated values of the energy gaps (∆E) correlate well with the UV spectroscopic data (Table S10 and Figure S38). Thus, a significant bathochromic shift of absorption maxima (289 nm and 342 nm) is observed in 4-diphenylaminophenyl-substituted compound 3l, which is in a more favorable energy state (∆E = 3.94 eV (Figure 7)).

AIEE Properties
It was found that compound 3l exhibits a pronounced aggregation-induced enhanced emission (AIEE) behavior (Figure 8a). With an increase of the water fraction (fw) in a solution of 3l in acetonitrile, a new emission band appeared with a maximum of 468 In order to elucidate the electron transfer process for α-biphenylamino-2,2 -bipyridines, the molecular electrostatic potential (MEP) distribution (Table S9) was calculated. The results obtained also confirm that the electron transfer occurs from an electron-rich biphenylene unit to the electron-deficient 2,2 -bipyridine core leading to the "push-pull" process.

AIEE Properties
It was found that compound 3l exhibits a pronounced aggregation-induced enhanced emission (AIEE) behavior (Figure 8a). With an increase of the water fraction (f w ) in a solution of 3l in acetonitrile, a new emission band appeared with a maximum of 468 nm. The highest intensity was achieved at f w = 60%, while the further increase in f w slightly decreased the emission intensity. This AIEE behavior is due to the presence of a triphenylamine moiety that realizes the restricted intramolecular rotation (RIR) mechanism, whereas fluorophores with any other groups at both paraand meta-positions did not demonstrate any AIEE activity, except 3b. The 3b molecule exhibited unusual behavior in the wateracetonitrile mixture. In this case, the emission maximum shifted from 482 nm to 492 nm at f w = 10%, accompanied by the quenching of fluorescence. However, a bathochromic shift from 460 nm to 492 nm was detected starting from f w = 70%, accompanied by an enhancement of the fluorescent emission, which reached a limit at f w = 80% (Figure 8b). This peculiar behavior at f w = 0-70% could be explained by the high polarity of water and at f w = 70-90%, by the formation of aggregates.

AIEE Properties
It was found that compound 3l exhibits a pronounced aggregation-induced enhanced emission (AIEE) behavior (Figure 8a). With an increase of the water fraction (fw) in a solution of 3l in acetonitrile, a new emission band appeared with a maximum of 468 nm. The highest intensity was achieved at fw = 60%, while the further increase in fw slightly decreased the emission intensity. This AIEE behavior is due to the presence of a triphenylamine moiety that realizes the restricted intramolecular rotation (RIR) mechanism, whereas fluorophores with any other groups at both para-and meta-positions did not demonstrate any AIEE activity, except 3b. The 3b molecule exhibited unusual behavior in the water-acetonitrile mixture. In this case, the emission maximum shifted from 482 nm to 492 nm at fw = 10%, accompanied by the quenching of fluorescence. However, a bathochromic shift from 460 nm to 492 nm was detected starting from fw = 70%, accompanied by an enhancement of the fluorescent emission, which reached a limit at fw = 80% (Figure 8b). This peculiar behavior at fw = 0-70% could be explained by the high polarity of water and at fw = 70-90%, by the formation of aggregates.

Studies of Sensing Properties
Electron-rich π-conjugated azine fluorophores can act as sensors or probes for high electron-deficient nitroaromatic explosives via exhibiting photoinduced electron transfer (PET) from one molecule to another [39]. This process is accompanied by the quenching of the fluorescence of a sensor.
In this regard, fluorophores 3a,h were chosen among the whole series of α-(N-biphenyl)substituted 2,2 -bipyridine as model objects in the study of the sensory properties of these fluorophores in the detection of nitroaromatic explosives. The position of the phenyl ring in the aniline residue is the only difference between 3a (meta) and 3h (para) that will allow their comparative analysis. Picric acid (PA) and 2,4,6-trinitrotoluene (TNT) were chosen as the most typical analytes. To determine the efficiency of fluorescence quenching, the Stern-Volmer model was chosen as a well-known method for evaluating sensory properties. Fluorometric titration was performed by the single point methodology using a Horiba FluoroMax 4.
Based on the results of the fluorometric titration, Stern-Volmer plots (Figure 9) with corresponding quenching constants K SV (Table 4, Equation (3)), as well as limits of detection (LOD) of nitroanalytes (Table 4, Equation (4)) were determined. Samples 3a,h showed high K SV (from 10.6 to 68.3 M −1 ) and LOD (64.9 to 5535.5 ppb) values, which are in the same order as the described pyridine-based probes [40]. Probe 3a demonstrated higher K SV values and better sensitivity toward both PA and TNT resulting in a meta-position that is more promising for creating sensors and probes for nitroexplosive detection. Thus, α-(Nbiphenyl)-substituted 2,2 -bipyridines may find a potential application as sensors/probes for the determination of nitroaromatic explosives.
where I 0 is the fluorescence intensity in the absence of a nitroexplosive, I is the fluorescence intensity in the presence of a nitroexplosive, K sv is the Stern-Volmer constant, [Q] is the concentration of a nitroexplosive. Equation (3). Stern-Volmer equation.
where LOD is the limit of detection, σ is the standard deviation of the fluorophore intensity in the absence of a nitroexplosive, k is the slope of the linear calibration curve. Equation (4). LOD calculation.

Materials and Equipment
Unless otherwise indicated, all common reagents and solvents were used from
Melting points were determined on Boetius combined heating stages. TLC and column chromatography were carried out on SiO 2 . 1 H NMR and 13 C NMR spectra were recorded at room temperature at 400 and 100 MHz, respectively, on a Bruker DRX-400 spectrometer using CDCl 3 or DMSO-d 6 as the solvent. Hydrogen chemical shifts were referenced to the hydrogen resonance of the corresponding solvent (DMSO-d 6 , δ = 2.50 ppm or CDCl 3 , δ = 7.26 ppm). Carbon chemical shifts were referenced to the carbon resonances of the solvent (CDCl3, δ = 77.16 ppm). Peaks were labeled as singlet (s), doublet (d), triplet (t), doublet of doublets (dd), doublet of doublets of doublets (ddd), and multiplet (m). Mass spectra were recorded on a MicrOTOF-Q II (Bruker Daltonics), electrospray as a method of ionization UV-vis absorption spectra were recorded on a Shimadzu UV-1800 spectrophotometer, and emission spectra were measured on a Horiba FluoroMax-4 by using quartz cells with a 1 cm path length at room temperature. Absolute quantum yields of the luminescence of target compounds in solution were measured by using the integrating sphere Quanta-ϕ of the Horiba FluoroMax 4 at room temperature. The mixture of corresponding 5-arylamino-1,2,4-triazine 1a-c (0.3 mmol) or 5a-c and 1-morpholinocyclopentene (1.5 mmol) was stirred at 200 • C for 2 h under an argon atmosphere. Then, the additional portion of 1-morpholinocyclopentene (0.75 mmol) was added and the resulting mixture was stirred for an additional 1 h at the same conditions. The products were separated by flash chromatography (DCM as eluent) and were then purified by recrystallization (ethanol). The corresponding compound 6a-c (0.3 mmol) was dissolved in THF (15 mL), followed by the addition of the corresponding boronic acid (0.33 mmol), Pd(tpp) 2 Cl 2 (6.3 mg, 0.009 mmol), triphenylphosphine (3.9 mg, 0.015 mmol), and solution of K 2 CO 3 (415 mg, 3 mmol) in water (15 mL). The resulting mixture was stirred at 90 • C in an argon atmosphere for 24 h. After completion, the reaction mixture was extracted with ethyl acetate (10 mL). The organic phase was washed with an aqueous solution of KOH, ammonium chloride and water, and dried with anhydrous sodium sulfate. The solvent was removed under reduced pressure. Ethanol was added to the residue and the obtained precipitate was filtered off, washed with ethanol, and dried.

Crystallography
The XRD analysis was carried out using equipment at the Center for Joint Use "Spectroscopy and Analysis of Organic Compounds" at the Postovsky Institute of Organic Synthesis of the Russian Academy of Sciences (Ural Branch). The experiments were accomplished on an automated X-ray diffractometer Xcalibur 3 with CCD detector using a standard procedure (MoKα-irradiation, graphite monochromator, ω-scans with 1o step at T = 295(2) K). Empirical absorption correction was applied. The solution and refinement of the structures were accomplished using the Olex program package [42]. The structures were solved by the method of the intrinsic phases in ShelXT program and refined by ShelXL by the full-matrix least-squared method for non-hydrogen atoms [43]. The H-atoms at C-H bonds were placed in the calculated positions, and the H-atoms at N-H bonds were refined independently in isotropic approximation.
The result of the X-ray diffraction analysis for compound 3a was deposited with the Cambridge Crystallographic Data Centre (CCDC 2167697) and can be found in supporting documents.

Conclusions
In conclusion, a rational synthetic approach toward α-biphenylamino-2,2 -bipyridines push-pull fluorophores starting from 5-cyano-1,2,4-triazines precursors using the sequence of the ipso-nucleophilic aromatic substitution of the cyano group, aza-Diels-Alder reaction and Suzuki cross-coupling was reported. In the THF solutions, the herein-reported fluorophores exhibited an intensive emission with a maxima of up to 511 nm along with up to 49.1% quantum yields. The most representative fluorophores 3b,g,i,l exhibited a well-pronounced positive fluorosolvatochromic behavior, which was well correlated with the solvent polarity scales according to Kosower and Dimroth/Reichardt as well as Lippert-Mataga mathematical models. DFT calculations confirmed the presence of the ICT state of the fluorophores. Fluorophores 3l and 3b demonstrated an unexpected AIEE activity, while fluorophores 3a and 3h exhibited sensing properties toward nitroaromatics (explosives) with high Ksv and LOD values.