Tunable Unexplored Luminescence in Waveguides Based on D-A-D Benzoselenadiazoles Nanofibers

A set of novel Donor-Acceptor-Donor (D-A-D) benzoselenadiazole derivatives has been synthesized and crystallized in nanocrystals in order to explore the correlation between their chemical structure and the waveguided luminescent properties. The findings reveal that all crystals exhibit luminescence and active optical waveguiding, demonstrating the ability to adjust their luminescence within a broad spectral range of 550–700 nm depending on the donor group attached to the benzoselenadiazole core. Notably, a clear relationship exists between the HOMO-LUMO energy gaps of each compound and the color emission of the corresponding optical waveguides. These outcomes affirm the feasibility of modifying the color emission of organic waveguides through suitable chemical functionalization. Importantly, this study marks the first utilization of benzoseleniadiazole derivatives for such purposes, underscoring the originality of this research. In addition, the obtention of nanocrystals is a key tool for the implementation of miniaturized photonic devices.


Introduction
In the past decade, rapid advancements in the field of photonic devices have brought about an unprecedented transformation in optics, catalyzing breakthroughs spanning from communications to medicine [1][2][3][4].In this dynamic landscape, optical waveguides have emerged as foundational building blocks, playing an irreplaceable role in manipulating and transmitting light at nanoscale dimensions.Their ability to guide light through microscopic structures has spearheaded a revolution in the miniaturization and efficiency of photonic systems [5][6][7][8].
Against the backdrop of this revolution, a pressing demand arises: the need for even smaller and more efficient photonic devices.Miniaturization has become a crucial pillar for developing more advanced technologies; in this context, nanoscale optical waveguides emerge as prominent players [9].The capability of these structures to direct and modulate light at sub-microscopic levels proves crucial for adapting photonic devices to the emerging demands of the modern era.In addition, one of the main problems with organic crystals for implementation in photonic devices such as optical waveguides is their stiffness.In this sense, the search for flexible organic crystals has been a tremendously expanding line of research in recent years [10][11][12].Obtaining nanostructures also contributes to the possibility of increasing their flexibility to be implemented in photonic devices, since longer structures are more difficult to deform and recover their original shape without breaking.
Nanomaterials 2024, 14, 822 2 of 12 However, miniaturization alone is not sufficient.The precise modulation of emission color in these optical waveguides stands out as an imperative, radically transforming the functionality of these devices.From quantum communication to exploration in biophotonics, the significance of accurately tuning emission color lies not only in miniaturization, but also in the ability to customize and optimize these structures at nanoscale levels [13].
In the last decade, the benzoselenodiazole core has emerged as a chemically intriguing entity, particularly in photophysical and electronic applications.It has exhibited notable electrochemical properties, propelling its application in electronic or photovoltaic devices [14][15][16].This heterocyclic system, which amalgamates a benzene ring with a selenodiazole ring, has proven exceptionally promising in the design and development of compounds with unique optical and electronic properties.Additionally, this core possesses an acceptor character, easily modulating with the introduction of donor groups at positions 4 and 7, thereby forming donor-acceptor-donor (D-A-D) systems capable of modulating HOMO (Highest Occupied Molecular Orbital) and LUMO (Lowest Unoccupied Molecular Orbital) facilitating the generation of intramolecular charge transfer (ICT) states, resulting in significant bathochromic emission shifts and achieving red-shifting properties [17][18][19][20][21].
The strategic presence of selenium in the structure of benzoselenodiazole imparts distinctive photophysical characteristics to these compounds, making them ideal candidates for applications in optoelectronic devices.Their ability to absorb and emit light within specific ranges of the electromagnetic spectrum has spurred intensive research in the design of photosensitive materials and efficient light-emitting compounds [22,23].However, its application in emissive optical waveguides is still unexplored, and to the best of our knowledge, there are no examples in the literature about this application, and this fact directed us to explore the employment of this moiety in this application.
Drawing from these characteristics and our prior exploration of benzoazole-based optical waveguides [24], different benzoselenadiazole derivatives were synthesized (1) with the introduction of four diverse donor groups in the peripheral positions 4 and 7, connected by a π-bridge through an alkynyl group, aiming to fine-tune the emission properties and build D-π-A-π-D architectures (Figure 1).Nanocrystalline forms of these compounds were cultivated via straightforward solution-based techniques for the investigation of their luminescent and light-conducting attributes in optical waveguides.
Nanomaterials 2024, 14, x FOR PEER REVIEW 2 of 12 longer structures are more difficult to deform and recover their original shape without breaking.However, miniaturization alone is not sufficient.The precise modulation of emission color in these optical waveguides stands out as an imperative, radically transforming the functionality of these devices.From quantum communication to exploration in bio-photonics, the significance of accurately tuning emission color lies not only in miniaturization, but also in the ability to customize and optimize these structures at nanoscale levels [13].
In the last decade, the benzoselenodiazole core has emerged as a chemically intriguing entity, particularly in photophysical and electronic applications.It has exhibited notable electrochemical properties, propelling its application in electronic or photovoltaic devices [14][15][16].This heterocyclic system, which amalgamates a benzene ring with a selenodiazole ring, has proven exceptionally promising in the design and development of compounds with unique optical and electronic properties.Additionally, this core possesses an acceptor character, easily modulating with the introduction of donor groups at positions 4 and 7, thereby forming donor-acceptor-donor (D-A-D) systems capable of modulating HOMO (Highest Occupied Molecular Orbital) and LUMO (Lowest Unoccupied Molecular Orbital) facilitating the generation of intramolecular charge transfer (ICT) states, resulting in significant bathochromic emission shifts and achieving red-shifting properties [17][18][19][20][21].
The strategic presence of selenium in the structure of benzoselenodiazole imparts distinctive photophysical characteristics to these compounds, making them ideal candidates for applications in optoelectronic devices.Their ability to absorb and emit light within specific ranges of the electromagnetic spectrum has spurred intensive research in the design of photosensitive materials and efficient light-emitting compounds [22,23].However, its application in emissive optical waveguides is still unexplored, and to the best of our knowledge, there are no examples in the literature about this application, and this fact directed us to explore the employment of this moiety in this application.
Drawing from these characteristics and our prior exploration of benzoazole-based optical waveguides [24], different benzoselenadiazole derivatives were synthesized (1) with the introduction of four diverse donor groups in the peripheral positions 4 and 7, connected by a π-bridge through an alkynyl group, aiming to fine-tune the emission properties and build D-π-A-π-D architectures (Figure 1).Nanocrystalline forms of these compounds were cultivated via straightforward solution-based techniques for the investigation of their luminescent and light-conducting attributes in optical waveguides.

General Techniques
All the chemicals utilized in the experiments for the synthesis of derivatives 1 were procured commercially, except styrene, which underwent prior distillation.Reactions involving air-sensitive materials were conducted under an atmosphere of argon.Microwave irradiations were executed using a Discover ® (CEM, Matthews, NC, USA).focused microwave reactor.Silica gel, (Merck, Kieselgel 60, 230-240 mesh, Merck, Darmstadt, Germany), was employed for flash chromatography.Analytical thin layer chromatography (TLC) was carried out on aluminum-coated Merck Kieselgel 60 F254 plates (Merck, Darmstadt, Germany).
1 H-NMR and 13 C-NMR spectra collection were recorded using a Bruker Advance Neo NMR spectrometer that operates at 500.16 MHz for 1 H and 125.75 MHz for 13 C.All spectra were acquired at 298 K, employing partially deuterated solvents as internal references.Coupling constants (J) are expressed in hertz (Hz), and chemical shifts (δ) are reported in parts per million (ppm).Multiplicities are described in the following way: s = singlet, d = doublet, t = triplet, m = multiplet.
For elemental analysis experiments (EA) C, H, N and S micro-sample elemental analyzer LECO (model CNHS-932, St. Joseph, MI, USA) was used, employing 2 mg of sample for each experiment.
Mass spectra were obtained on a Bruker Autoflex II TOF/TOF (Bruker, Billerica, MA, USA) spectrometer using dithranol as the matrix for all the experiments.
UV-visible and fluorescence spectra studies in solution were carried out using a Jasco V-750 spectrophotometer (JASCO-Spain, Madrid, Spain) and Jasco FP-8300 spectrofluorimeter (JASCO-Spain, Madrid, Spain), respectively.The absorption and emission spectra were taken using dichloromethane as a solvent and at a concentration of 10 −5 M at room temperature using standard quartz cells of 1 cm width and high spectroscopic grade solvents with very high purity.

Experimental Section
General procedure: A mixture of 4,7-dibromobenzo[c][1,2,5]selenadiazole (2) (0.100 g, 0.29 mmol), the corresponding acetylene derivative (3) (0.6 mmol), DBU (0.088 g, 0.58 mmol), CuI (0.003 g, 0.015 mmol) and Pd-EncatTM TPP30 (0.026 g, 0.01 mmol) was charged to a dried microwave vessel under an argon atmosphere.After that, 1 mL of CH 3 CN was added to the vessel, which was then closed and irradiated at 150 • C for 20 min in all the cases.The crudes' reactions were purified by column chromatography using hexane/ethyl acetate as eluent to achieve analytically pure products 1.It can be pointed out that for all the reactions, microwave irradiation was used as an energy source and Pd-EncatTM TPP30 was recovered after its use by filtration, and was used again for following reactions to reduce the environmental impact of the process.

Synthesis
The synthesis of D-A-D benzoselenadiazole derivatives 1 was performed through a Sonogashira C-C cross-coupling reaction between derivatives 2 and 3 (Scheme 1), optimized previously by our research group for other azoles and benzoazoles [25,26].All the reactions were carried out using microwave irradiation, with the reusable catalyst Pd-Encat TPP30 to increase the sustainability of the synthetic procedure, achieving the desired compounds 1 in 30 min in very good yields (65-91%), that gave adequate analytical NMR spectroscopic data (NMR spectra collection is recorded in Supporting Information section).We would like to point out that derivative 1a had been previously synthesized by Li and co-workers under conventional conditions [27], improving the yield with this procedure using microwave irradiation as an energy source and considerably reducing the reaction time.

Theoretical Calculations
Before later optical characterization, the minimum-energy optimized structures were calculated at the B3LYP/6-31G (d,p) theoretical level [28,29] and are detailed in Table 1.
Across all compounds, the HOMO molecular orbital is situated along the horizontal axis of the molecule, mainly affected by the donor group, while the LUMO orbital predominantly occupies the vertical axis, which mainly corresponds to the benzoselenadiazole core, existing as a shared overlap region, thus facilitating intramolecular charge transfer (ICT) [30].

Theoretical Calculations
Before later optical characterization, the minimum-energy optimized structures were calculated at the B3LYP/6-31G (d,p) theoretical level [28,29] and are detailed in Table 1.Across all compounds, the HOMO molecular orbital is situated along the horizontal axis of the molecule, mainly affected by the donor group, while the LUMO orbital predominantly occupies the vertical axis, which mainly corresponds to the benzoselenadiazole core, existing as a shared overlap region, thus facilitating intramolecular charge transfer (ICT) [30].

2.05
The variation in donor peripheral groups (1a-d) correlates with the electron-donating tendency of the substituent, as indicated by the HOMO-LUMO gap.The most dramatical changes can be detected in HOMO values due to the changes in the donor group that implies changes in the HOMO-LUMO gaps, while LUMO values are not significantly affected because the major contribution is because the benzoselenadiazole moiety that keeps constant in all the derivatives.Specifically, compound 1a, featuring peripheral phenyl groups (weaker donor groups), exhibits a higher HOMO-LUMO gap value compared to compounds 1b-d.The introduction of methoxy groups in the periphery in 1b with +I and +K characters increases the donor character and decreases the HOMO-LUMO gap with respect to 1a (2.44 vs. 2.60 eV).Consequently, 1c, with enhanced donor character due to its triphenylamine group, demonstrates a lower HOMO-LUMO gap value relative to 1a and 1b (2.20 vs. 2.60 and 2.44 eV).Finally, 1d, with the strongest donor group, phenylphenoxazine, showed the lowest HOMO-LUMO gap (2.05 eV), and this fact will directly impact their photophysical properties.−3.06

Theoretical Calculations
Before later optical characterization, the minimum-energy optimized structures were calculated at the B3LYP/6-31G (d,p) theoretical level [28,29] and are detailed in Table 1.Across all compounds, the HOMO molecular orbital is situated along the horizontal axis of the molecule, mainly affected by the donor group, while the LUMO orbital predominantly occupies the vertical axis, which mainly corresponds to the benzoselenadiazole core, existing as a shared overlap region, thus facilitating intramolecular charge transfer (ICT) [30].

2.05
The variation in donor peripheral groups (1a-d) correlates with the electron-donating tendency of the substituent, as indicated by the HOMO-LUMO gap.The most dramatical changes can be detected in HOMO values due to the changes in the donor group that implies changes in the HOMO-LUMO gaps, while LUMO values are not significantly affected because the major contribution is because the benzoselenadiazole moiety that keeps constant in all the derivatives.Specifically, compound 1a, featuring peripheral phenyl groups (weaker donor groups), exhibits a higher HOMO-LUMO gap value compared to compounds 1b-d.The introduction of methoxy groups in the periphery in 1b with +I and +K characters increases the donor character and decreases the HOMO-LUMO gap with respect to 1a (2.44 vs. 2.60 eV).Consequently, 1c, with enhanced donor character due to its triphenylamine group, demonstrates a lower HOMO-LUMO gap value relative to 1a and 1b (2.20 vs. 2.60 and 2.44 eV).Finally, 1d, with the strongest donor group, phenylphenoxazine, showed the lowest HOMO-LUMO gap (2.05 eV), and this fact will directly impact their photophysical properties.

Theoretical Calculations
Before later optical characterization, the minimum-energy optimized structures were calculated at the B3LYP/6-31G (d,p) theoretical level [28,29] and are detailed in Table 1.Across all compounds, the HOMO molecular orbital is situated along the horizontal axis of the molecule, mainly affected by the donor group, while the LUMO orbital predominantly occupies the vertical axis, which mainly corresponds to the benzoselenadiazole core, existing as a shared overlap region, thus facilitating intramolecular charge transfer (ICT) [30].

2.05
The variation in donor peripheral groups (1a-d) correlates with the electron-donating tendency of the substituent, as indicated by the HOMO-LUMO gap.The most dramatical changes can be detected in HOMO values due to the changes in the donor group that implies changes in the HOMO-LUMO gaps, while LUMO values are not significantly affected because the major contribution is because the benzoselenadiazole moiety that keeps constant in all the derivatives.Specifically, compound 1a, featuring peripheral phenyl groups (weaker donor groups), exhibits a higher HOMO-LUMO gap value compared to compounds 1b-d.The introduction of methoxy groups in the periphery in 1b with +I and +K characters increases the donor character and decreases the HOMO-LUMO gap with respect to 1a (2.44 vs. 2.60 eV).Consequently, 1c, with enhanced donor character due to its triphenylamine group, demonstrates a lower HOMO-LUMO gap value relative to 1a and 1b (2.20 vs. 2.60 and 2.44 eV).Finally, 1d, with the strongest donor group, phenylphenoxazine, showed the lowest HOMO-LUMO gap (2.05 eV), and this fact will directly impact their photophysical properties.−3.14

Theoretical Calculations
Before later optical characterization, the minimum-energy optimized structures were calculated at the B3LYP/6-31G (d,p) theoretical level [28,29] and are detailed in Table 1.Across all compounds, the HOMO molecular orbital is situated along the horizontal axis of the molecule, mainly affected by the donor group, while the LUMO orbital predominantly occupies the vertical axis, which mainly corresponds to the benzoselenadiazole core, existing as a shared overlap region, thus facilitating intramolecular charge transfer (ICT) [30].

2.05
The variation in donor peripheral groups (1a-d) correlates with the electron-donating tendency of the substituent, as indicated by the HOMO-LUMO gap.The most dramatical changes can be detected in HOMO values due to the changes in the donor group that implies changes in the HOMO-LUMO gaps, while LUMO values are not significantly affected because the major contribution is because the benzoselenadiazole moiety that keeps constant in all the derivatives.Specifically, compound 1a, featuring peripheral phenyl groups (weaker donor groups), exhibits a higher HOMO-LUMO gap value compared to compounds 1b-d.The introduction of methoxy groups in the periphery in 1b with +I and +K characters increases the donor character and decreases the HOMO-LUMO gap with respect to 1a (2.44 vs. 2.60 eV).Consequently, 1c, with enhanced donor character due to its triphenylamine group, demonstrates a lower HOMO-LUMO gap value relative to 1a and 1b (2.20 vs. 2.60 and 2.44 eV).Finally, 1d, with the strongest donor group, phenylphenoxazine, showed the lowest HOMO-LUMO gap (2.05 eV), and this fact will directly impact their photophysical properties.

Theoretical Calculations
Before later optical characterization, the minimum-energy optimized structures were calculated at the B3LYP/6-31G (d,p) theoretical level [28,29] and are detailed in Table 1.Across all compounds, the HOMO molecular orbital is situated along the horizontal axis of the molecule, mainly affected by the donor group, while the LUMO orbital predominantly occupies the vertical axis, which mainly corresponds to the benzoselenadiazole core, existing as a shared overlap region, thus facilitating intramolecular charge transfer (ICT) [30].

2.05
The variation in donor peripheral groups (1a-d) correlates with the electron-donating tendency of the substituent, as indicated by the HOMO-LUMO gap.The most dramatical changes can be detected in HOMO values due to the changes in the donor group that implies changes in the HOMO-LUMO gaps, while LUMO values are not significantly affected because the major contribution is because the benzoselenadiazole moiety that keeps constant in all the derivatives.Specifically, compound 1a, featuring peripheral phenyl groups (weaker donor groups), exhibits a higher HOMO-LUMO gap value compared to compounds 1b-d.The introduction of methoxy groups in the periphery in 1b with +I and +K characters increases the donor character and decreases the HOMO-LUMO gap with respect to 1a (2.44 vs. 2.60 eV).Consequently, 1c, with enhanced donor character due to its triphenylamine group, demonstrates a lower HOMO-LUMO gap value relative to 1a and 1b (2.20 vs. 2.60 and 2.44 eV).Finally, 1d, with the strongest donor group, phenylphenoxazine, showed the lowest HOMO-LUMO gap (2.05 eV), and this fact will directly impact their photophysical properties.−3.08

Theoretical Calculations
Before later optical characterization, the minimum-energy optimized structures were calculated at the B3LYP/6-31G (d,p) theoretical level [28,29] and are detailed in Table 1.Across all compounds, the HOMO molecular orbital is situated along the horizontal axis of the molecule, mainly affected by the donor group, while the LUMO orbital predominantly occupies the vertical axis, which mainly corresponds to the benzoselenadiazole core, existing as a shared overlap region, thus facilitating intramolecular charge transfer (ICT) [30].

2.05
The variation in donor peripheral groups (1a-d) correlates with the electron-donating tendency of the substituent, as indicated by the HOMO-LUMO gap.The most dramatical changes can be detected in HOMO values due to the changes in the donor group that implies changes in the HOMO-LUMO gaps, while LUMO values are not significantly affected because the major contribution is because the benzoselenadiazole moiety that keeps constant in all the derivatives.Specifically, compound 1a, featuring peripheral phenyl groups (weaker donor groups), exhibits a higher HOMO-LUMO gap value compared to compounds 1b-d.The introduction of methoxy groups in the periphery in 1b with +I and +K characters increases the donor character and decreases the HOMO-LUMO gap with respect to 1a (2.44 vs. 2.60 eV).Consequently, 1c, with enhanced donor character due to its triphenylamine group, demonstrates a lower HOMO-LUMO gap value relative to 1a and 1b (2.20 vs. 2.60 and 2.44 eV).Finally, 1d, with the strongest donor group, phenylphenoxazine, showed the lowest HOMO-LUMO gap (2.05 eV), and this fact will directly impact their photophysical properties.

Theoretical Calculations
Before later optical characterization, the minimum-energy optimized structures were calculated at the B3LYP/6-31G (d,p) theoretical level [28,29] and are detailed in Table 1.Across all compounds, the HOMO molecular orbital is situated along the horizontal axis of the molecule, mainly affected by the donor group, while the LUMO orbital predominantly occupies the vertical axis, which mainly corresponds to the benzoselenadiazole core, existing as a shared overlap region, thus facilitating intramolecular charge transfer (ICT) [30].

2.05
The variation in donor peripheral groups (1a-d) correlates with the electron-donating tendency of the substituent, as indicated by the HOMO-LUMO gap.The most dramatical changes can be detected in HOMO values due to the changes in the donor group that implies changes in the HOMO-LUMO gaps, while LUMO values are not significantly affected because the major contribution is because the benzoselenadiazole moiety that keeps constant in all the derivatives.Specifically, compound 1a, featuring peripheral phenyl groups (weaker donor groups), exhibits a higher HOMO-LUMO gap value compared to compounds 1b-d.The introduction of methoxy groups in the periphery in 1b with +I and +K characters increases the donor character and decreases the HOMO-LUMO gap with respect to 1a (2.44 vs. 2.60 eV).Consequently, 1c, with enhanced donor character due to its triphenylamine group, demonstrates a lower HOMO-LUMO gap value relative to 1a and 1b (2.20 vs. 2.60 and 2.44 eV).Finally, 1d, with the strongest donor group, phenylphenoxazine, showed the lowest HOMO-LUMO gap (2.05 eV), and this fact will directly impact their photophysical properties.

Theoretical Calculations
Before later optical characterization, the minimum-energy optimized structures were calculated at the B3LYP/6-31G (d,p) theoretical level [28,29] and are detailed in Table 1.Across all compounds, the HOMO molecular orbital is situated along the horizontal axis of the molecule, mainly affected by the donor group, while the LUMO orbital predominantly occupies the vertical axis, which mainly corresponds to the benzoselenadiazole core, existing as a shared overlap region, thus facilitating intramolecular charge transfer (ICT) [30].

2.05
The variation in donor peripheral groups (1a-d) correlates with the electron-donating tendency of the substituent, as indicated by the HOMO-LUMO gap.The most dramatical changes can be detected in HOMO values due to the changes in the donor group that implies changes in the HOMO-LUMO gaps, while LUMO values are not significantly affected because the major contribution is because the benzoselenadiazole moiety that keeps constant in all the derivatives.Specifically, compound 1a, featuring peripheral phenyl groups (weaker donor groups), exhibits a higher HOMO-LUMO gap value compared to compounds 1b-d.The introduction of methoxy groups in the periphery in 1b with +I and +K characters increases the donor character and decreases the HOMO-LUMO gap with respect to 1a (2.44 vs. 2.60 eV).Consequently, 1c, with enhanced donor character due to its triphenylamine group, demonstrates a lower HOMO-LUMO gap value relative to 1a and 1b (2.20 vs. 2.60 and 2.44 eV).Finally, 1d, with the strongest donor group, phenylphenoxazine, showed the lowest HOMO-LUMO gap (2.05 eV), and this fact will directly impact their photophysical properties.

2.05
The variation in donor peripheral groups (1a-d) correlates with the electron-donating tendency of the substituent, as indicated by the HOMO-LUMO gap.The most dramatical changes can be detected in HOMO values due to the changes in the donor group that implies changes in the HOMO-LUMO gaps, while LUMO values are not significantly affected because the major contribution is because the benzoselenadiazole moiety that keeps constant in all the derivatives.Specifically, compound 1a, featuring peripheral phenyl groups (weaker donor groups), exhibits a higher HOMO-LUMO gap value compared to compounds 1b-d.The introduction of methoxy groups in the periphery in 1b with +I and +K characters increases the donor character and decreases the HOMO-LUMO gap with respect to 1a (2.44 vs. 2.60 eV).Consequently, 1c, with enhanced donor character due to its triphenylamine group, demonstrates a lower HOMO-LUMO gap value relative to 1a and 1b (2.20 vs. 2.60 and 2.44 eV).Finally, 1d, with the strongest donor group, phenylphenoxazine, showed the lowest HOMO-LUMO gap (2.05 eV), and this fact will directly impact their photophysical properties.

Photophysical Studies
The UV-vis and fluorescence spectra of the different derivatives 1 were carried out in 10 −5 M CH 2 Cl 2 solutions.They are recorded in Figure 2 and photophysical data are summarized in Table 2.

Photophysical Studies
The UV-vis and fluorescence spectra of the different derivatives 1 were carried out in 10 −5 M CH2Cl2 solutions.They are recorded in Figure 2 and photophysical data are summarized in Table 2.It can be pointed out that the data recorded in Table 2 for 1a agree with the data previously described by Li and co-workers for this compound [27].The compounds 1a-d exhibit absorption spectra characterized by a broad band with peaks ranging from around 300 to 330 nm, attributed to a π-π* transition, and a second band centered at longer wavelengths (around 430-490 nm), attributed to an ICT state.When the photoluminescence (PL) spectra are calculated following photoexcitation at the peaks of the longest-wavelength absorption band, the maxima shifts from 546 nm to 664 nm.This gradual red-shift of the PL spectra corresponds to the push-pull nature of the dyes, moving towards longer wavelengths as the donor-acceptor character strengthens.Consequently, 1d displays the longest emission wavelength among all D-A-D derivatives due to the pronounced electron-donating properties of the phenylphenoxazine moiety.Similarly, 1c also exhibits bathochromic shifts compared to 1a and 1b, attributed to the enhanced donor character of the triphenylamine derivative in comparison to phenyl or trimethoxyphenyl groups.
Consequently, the photoluminescence (PL) spectra of the derivatives 1 undergo spectral changes in alignment with the calculated HOMO-LUMO gap energies.The experimental optical HOMO-LUMO gaps were determined based on the onset of the lowest energy band absorption and demonstrated satisfactory agreement with theoretical   It can be pointed out that the data recorded in Table 2 for 1a agree with the data previously described by Li and co-workers for this compound [27].The compounds 1a-d exhibit absorption spectra characterized by a broad band with peaks ranging from around 300 to 330 nm, attributed to a π-π* transition, and a second band centered at longer wavelengths (around 430-490 nm), attributed to an ICT state.When the photoluminescence (PL) spectra are calculated following photoexcitation at the peaks of the longest-wavelength absorption band, the maxima shifts from 546 nm to 664 nm.This gradual red-shift of the PL spectra corresponds to the push-pull nature of the dyes, moving towards longer wavelengths as the donor-acceptor character strengthens.Consequently, 1d displays the longest emission wavelength among all D-A-D derivatives due to the pronounced electron-donating properties of the phenylphenoxazine moiety.Similarly, 1c also exhibits bathochromic shifts compared to 1a and 1b, attributed to the enhanced donor character of the triphenylamine derivative in comparison to phenyl or trimethoxyphenyl groups.
Consequently, the photoluminescence (PL) spectra of the derivatives 1 undergo spectral changes in alignment with the calculated HOMO-LUMO gap energies.The experimental optical HOMO-LUMO gaps were determined based on the onset of the lowest energy band absorption and demonstrated satisfactory agreement with theoretical predictions (Table 2).Additionally, it is noteworthy that a similar observation can be made regarding the spectral evolution of the lowest π-π* absorption transition.. Finally, the fluorescence quantum yields of these derivatives in solution were determined in CHCl 3 using quinine sulfate in 0.1 M H 2 SO 4 (Φ = 0.54) and fluorescein in 0.1 M NaOH (Φ = 0.79) for 1a-c, and cresyl violet in ethanol (Φ = 0.56) for 1d as standards, revealing moderate values (Table 2).The values of the quantum yield in the solid state (Table 2) are moderate and slightly decreased for all the derivatives in comparison with values in the solution state to values between 0.13 and 0.43.

Self-Assembling Studies
The creation of supramolecular assemblies using derivatives 1 was achieved through the slow diffusion method.In this procedure, a container holding a diluted solution (1 mg) of derivatives 1 in 1 mL of either chloroform or tetrahydrofuran, recognized as effective solvents, was carefully placed into another container containing a non-soluble poor solvent such as hexane, acetonitrile, ethanol or methanol.The second container was securely sealed and left undisturbed at room temperature.After a few days, the emergence of supramolecular aggregates becomes observable.
SEM images of the resultant nanofibers were acquired, with a focus on selecting the most promising ones in the form of fibers.Examples showcasing the optimal morphologies are presented in Figure 3, while additional SEM images can be found in the Supporting Information (Figure S1).
predictions (Table 2).Additionally, it is noteworthy that a similar observation can be made regarding the spectral evolution of the lowest π-π* absorption transition.. Finally, the fluorescence quantum yields of these derivatives in solution were determined in CHCl3 using quinine sulfate in 0.1 M H2SO4 (Φ = 0.54) and fluorescein in 0.1 M NaOH (Φ = 0.79) for 1a-c, and cresyl violet in ethanol (Φ = 0.56) for 1d as standards, revealing moderate values (Table 2).The values of the quantum yield in the solid state (Table 2) are moderate and slightly decreased for all the derivatives in comparison with values in the solution state to values between 0.13 and 0.43.

Self-Assembling Studies
The creation of supramolecular assemblies using derivatives 1 was achieved through the slow diffusion method.In this procedure, a container holding a diluted solution (1 mg) of derivatives 1 in 1 mL of either chloroform or tetrahydrofuran, recognized as effective solvents, was carefully placed into another container containing a non-soluble poor solvent such as hexane, acetonitrile, ethanol or methanol.The second container was securely sealed and left undisturbed at room temperature.After a few days, the emergence of supramolecular aggregates becomes observable.
SEM images of the resultant nanofibers were acquired, with a focus on selecting the most promising ones in the form of fibers.Examples showcasing the optimal morphologies are presented in Figure 3, while additional SEM images can be found in the Supporting Information (Figure S1).As we can observe in Figure 3, all nanocrystals exhibit a well-defined fibrillar shape, making them ideal candidates for investigating their optical waveguide properties.It can be pointed out that the best fibrillar morphologies were obtained using MeOH or EtOH as poor solvents.As we can observe in Figure 3, all nanocrystals exhibit a well-defined fibrillar shape, making them ideal candidates for investigating their optical waveguide properties.It can be pointed out that the best fibrillar morphologies were obtained using MeOH or EtOH as poor solvents.

Optical Waveguiding Behaviour
After identifying the most promising crystalline microfibers with suitable morphologies, confocal fluorescence microscopy images (Figure 4) of these nanocrystals were taken and recorded to assess their optical waveguiding characteristics.

Optical Waveguiding Behaviour
After identifying the most promising crystalline microfibers with suitable morphologies, confocal fluorescence microscopy images (Figure 4) of these nanocrystals were taken and recorded to assess their optical waveguiding characteristics.The outcomes revealed that all nanocrystals of compounds 1a-d exhibited luminescence.Upon irradiation with a 365 nm laser at the fiber body, it was notable that the emitted light propagated to the crystal's tip, while the body itself brightened with emission.This phenomenon indicated strong luminescence with a distinct contrast between the  The outcomes revealed that all nanocrystals of compounds 1a-d exhibited luminescence.Upon irradiation with a 365 nm laser at the fiber body, it was notable that the emitted light propagated to the crystal's tip, while the body itself brightened with emission.This phenomenon indicated strong luminescence with a distinct contrast between the bright tip/edges and the darker bulk, confirming efficient photon transport along the nanocrystals.Additionally, each nanocrystal was emitted at varying wavelengths, all distinct from the excitation wavelength, thus affirming their active optical waveguiding behavior (Figure 4).In addition, we can observe that in function on the molecular structure and the substitution in the benzoselenadiazole moiety, nanocrystals emitted a broad range of wavelengths, spanning from 550-700 nm.Notably, in the solid state, a significant redshift in PL is observed compared to the solution phase (Table 2 and Figure 2b vs. Figure 4).It is important to highlight that structural modifications of these derivatives exert an identical influence in both solution and solid states, resulting in consistent bathochromic shifts as the donor-acceptor (D-A) character of the derivative intensifies.Comparison of the emission wavelengths with theoretically calculated HOMO-LUMO gap values at the B3LYP/6-31G (d,p) theory level revealed a clear correlation, demonstrating the influence of different functional groups on the optical waveguide emission color.Fluorescence microscopy images revealed a progressive red-shift in the emission from green to red as theoretically calculated HOMO-LUMO gap energies decreased, indicating that TD-DFT could be utilized for on-demand emission tuning of the optical waveguides, and confirmed by the experimental HOMO-LUMO gaps obtained through the onset in absorption spectra.Like this, beginning with the highest HOMO-LUMO gap (2.60 eV), compound 1a exhibited green emission (550 nm), compound 1b, with the introduction of the trimethoxy groups, induces a lower HOMO-LUMO gap (2.44 eV), emitting in yellow (595 nm).The introduction of a stronger donor group like triphenylamine decreases the HOMO-LUMO gap (2.20 eV), achieving an orange color emission in the nanocrystals (640 nm).Finally, 1d, with the strongest donor group (phenylphenoxazine), shows the lowest HOMO-LUMO gap (2.05 eV), with strong emission in red in the nanocrystals (698 nm).(Figure 5).
Nanomaterials 2024, 14, x FOR PEER REVIEW 9 of 12 bright tip/edges and the darker bulk, confirming efficient photon transport along the nanocrystals.Additionally, each nanocrystal was emitted at varying wavelengths, all distinct from the excitation wavelength, thus affirming their active optical waveguiding behavior (Figure 4).In addition, we can observe that in function on the molecular structure and the substitution in the benzoselenadiazole moiety, nanocrystals emitted a broad range of wavelengths, spanning from 550-700 nm.Notably, in the solid state, a significant redshift in PL is observed compared to the solution phase (Table 2 and Figure 2b vs. Figure 4).It is important to highlight that structural modifications of these derivatives exert an identical influence in both solution and solid states, resulting in consistent bathochromic shifts as the donor-acceptor (D-A) character of the derivative intensifies.Comparison of the emission wavelengths with theoretically calculated HOMO-LUMO gap values at the B3LYP/6-31G (d,p) theory level revealed a clear correlation, demonstrating the influence of different functional groups on the optical waveguide emission color.Fluorescence microscopy images revealed a progressive red-shift in the emission from green to red as theoretically calculated HOMO-LUMO gap energies decreased, indicating that TD-DFT could be utilized for on-demand emission tuning of the optical waveguides, and confirmed by the experimental HOMO-LUMO gaps obtained through the onset in absorption spectra.Like this, beginning with the highest HOMO-LUMO gap (2.60 eV), compound 1a exhibited green emission (550 nm), compound 1b, with the introduction of the trimethoxy groups, induces a lower HOMO-LUMO gap (2.44 eV), emitting in yellow (595 nm).The introduction of a stronger donor group like triphenylamine decreases the HOMO-LUMO gap (2.20 eV), achieving an orange color emission in the nanocrystals (640 nm).Finally, 1d, with the strongest donor group (phenylphenoxazine), shows the lowest HOMO-LUMO gap (2.05 eV), with strong emission in red in the nanocrystals (698 nm).(Figure 5).While numerous studies have explored this subject, as far as we know, there is currently no literature correlating the variation of emission color of a waveguide for benzoseleniadiazole derivatives, highlighting the novelty of this work.
Moreover, it is noteworthy that derivatives 1a-d exhibit a tendency to form crosslinked and bunch-shaped nanocrystals as SEM images reveal.Irradiation of a single point on one fiber facilitated the light propagation in different directions; for example, in 1a (Figure 6).This curious behavior, as described in recent literature [31][32][33], enhances the practical utility of these materials in real-world devices.It enables light to travel through different channels, facilitating parallel connectivity and interconnection between nanowires and various devices and facilitating the implementation in real miniaturized devices, which are very in demand these days in current society.For all these reasons, these results may be very useful in the coming years for the development of miniaturized photonic chips.While numerous studies have explored this subject, as far as we know, there is currently no literature correlating the variation of emission color of a waveguide for benzoseleniadiazole derivatives, highlighting the novelty of this work.
Moreover, it is noteworthy that derivatives 1a-d exhibit a tendency to form crosslinked and bunch-shaped nanocrystals as SEM images reveal.Irradiation of a single point on one fiber facilitated the light propagation in different directions; for example, in 1a (Figure 6).This curious behavior, as described in recent literature [31][32][33], enhances the practical utility of these materials in real-world devices.It enables light to travel through different channels, facilitating parallel connectivity and interconnection between nanowires and various devices and facilitating the implementation in real miniaturized devices, which are very in demand these days in current society.For all these reasons, these results may be very useful in the coming years for the development of miniaturized photonic chips.

Scheme 1 .
Scheme 1. Synthesis of D-A-D benzoselenadiazoles derivatives 1, as described in this work.Scheme 1. Synthesis of D-A-D benzoselenadiazoles derivatives 1, as described in this work.

Table 1 .
Energies and topologies of the HOMO and LUMO frontier molecular orbitals, and HOMO-LUMO gaps of benzoselenadiazoles 1 obtained using DFT calculations at the B3LYP/6-31G (d,p) theory level.

Table 1 .
Energies and topologies of the HOMO and LUMO frontier molecular orbitals, and HOMO-LUMO gaps of benzoselenadiazoles 1 obtained using DFT calculations at the B3LYP/6-31G (d,p) theory level.

Table 1 .
Energies and topologies of the HOMO and LUMO frontier molecular orbitals, and HOMO-LUMO gaps of benzoselenadiazoles 1 obtained using DFT calculations at the B3LYP/6-31G (d,p) theory level.

Table 1 .
Energies and topologies of the HOMO and LUMO frontier molecular orbitals, and HOMO-LUMO gaps of benzoselenadiazoles 1 obtained using DFT calculations at the B3LYP/6-31G (d,p) theory level.

Table 1 .
Energies and topologies of the HOMO and LUMO frontier molecular orbitals, and HOMO-LUMO gaps of benzoselenadiazoles 1 obtained using DFT calculations at the B3LYP/6-31G (d,p) theory level.

Table 1 .
Energies and topologies of the HOMO and LUMO frontier molecular orbitals, and HOMO-LUMO gaps of benzoselenadiazoles 1 obtained using DFT calculations at the B3LYP/6-31G (d,p) theory level.

Table 1 .
Energies and topologies of the HOMO and LUMO frontier molecular orbitals, and HOMO-LUMO gaps of benzoselenadiazoles 1 obtained using DFT calculations at the B3LYP/6-31G (d,p) theory level.

Table 1 .
Energies and topologies of the HOMO and LUMO frontier molecular orbitals, and HOMO-LUMO gaps of benzoselenadiazoles 1 obtained using DFT calculations at the B3LYP/6-31G (d,p) theory level.

Table 1 .
Energies and topologies of the HOMO and LUMO frontier molecular orbitals, and HOMO-LUMO gaps of benzoselenadiazoles 1 obtained using DFT calculations at the B3LYP/6-31G (d,p) theory level.

[a] Absorption maxima of derivatives 1
in solution; [b] Emission maxima of derivatives 1 in solution; [c] Emission maxima of nanocrystals of derivatives 1; [d] Onset wavelength calculated from the absorption spectra of the lowest energy band; [e] PL quantum yield in solution of derivatives 1. [f] PL quantum yield measured in the solid state; [g] Theoretical HOMO-LUMO gap of compounds 1 computed at B3LYP/6-31G(d,p) level.[h] Experimental HOMO-LUMO gap of compound 1 calculated from the onset of the lowest energy absorption band using the 1240/λonset formula.

[a] Absorption maxima of derivatives 1
in solution; [b] Emission maxima of derivatives 1 in solution; [c] Emission maxima of nanocrystals of derivatives 1; [d] Onset wavelength calculated from the absorption spectra of the lowest energy band; [e] PL quantum yield in solution of derivatives 1. [f] PL quantum yield measured in the solid state; [g] Theoretical HOMO-LUMO gap of compounds 1 computed at B3LYP/6-31G(d,p) level.[h] Experimental HOMO-LUMO gap of compound 1 calculated from the onset of the lowest energy absorption band using the 1240/λ onset formula.

Figure 5 .
Figure 5. Theoretical HOMO-LUMO gap of derivatives 1a-d/emission color relationship of the optical waveguides obtained from the nanocrystals of benzoselenadiazoles 1.

Figure 5 .
Figure 5. Theoretical HOMO-LUMO gap of derivatives 1a-d/emission color relationship of the optical waveguides obtained from the nanocrystals of benzoselenadiazoles 1.