Insight into Unusual Supramolecular Self-Assemblies of Terthiophenes Directed by Weak Hydrogen Bonding

A supramolecular self-assembly of semiconducting polymers and small molecules plays an important role in charge transportation, performance, and lifetime of an optoelectronic device. Tremendous efforts have been put into the strategies to self-organize these materials. In this regard, here, we present the self-organization of terthiophene and its methyl alcohol derivative with 4,4′-bipyridine (44BiPy). An unexpected 2D layered organization of 5,5″-dimethyl-2,2′:5′,2″-terthiophene (DM3T) and 44BiPy was obtained and analyzed. Single-crystal X-ray diffraction analysis revealed that DM3T and 44BiPy consist of stacked, almost independent, infinite 2D layers while held together by weak hydrogen bonds. In addition to this peculiar supramolecular arrangement of these compounds, the investigation of their photophysical properties showed strong fluorescence quenching of DM3T by 44BiPy in the solid state, suggesting an efficient charge transfer. On the other hand, the methyl alcohol derivative of terthiophene, DM3TMeOH, organized in a closed cyclic motif with 44BiPy via hydrogen bonds.


Introduction
Over the last several decades, organic π-conjugated compounds have emerged as a new class of semiconducting materials because of their fascinating optical and electronic properties offering a wide range of applications in organic light-emitting diodes (OLEDs), organic solar cells (OSCs), organic field-effect transistors (OFETs), organic lasers, optical or electrochemical sensors, and many more [1][2][3][4][5][6][7]. Thiophene and its derivatives, alone or along with many other aromatic and heteroaromatic constituents, are well-known building blocks in the construction and development of today's high-performance organic semiconducting materials [8]. Thousands of papers on thiophene-based compounds have been published over the last several decades describing the rational design, synthetic methodology, and investigation of their semiconducting and photophysical properties. Thiophene oligomers (e.g., bithiophene, terthiophene, and quaterthiophene) and polymers (e.g., poly(3-hexylthiophene) (P3HT) and poly (3,4-ethylenedioxythiophene):polystyrene sulfonate (PEDOT:PSS)) are widely studied and used materials in the fabrication of organic optoelectronic devices [9].
As we know, without any substituent, polythiophene is a poorly soluble polymer in most common organic solvents, which makes it difficult to process for fundamental study of charge transportation and redundant to use for any practical application. Therefore, for practical purposes, solution-processed poly(3,(4)-(di)alkyl)thiophenes have been obtained by introducing alkyl chains at the backbone polythiophenes and utilized various optoelectronic application. Nevertheless, many well-defined oligothiophenes have been synthesized and studied to serve as the basis for a thorough understanding of the electrical properties of synthesized and studied to serve as the basis for a thorough understanding of the electrical properties of polythiophenes. Among these oligothiophenes, terthiophene and its derivatives, because of their facile synthesis, are widely studied to understand the electronic structure and charge transport mechanism in this class of materials. For example, Birnbaum and Kohler recorded the fluorescence excitation and emission spectra of 2,2′:5′,2″terthiophene and performed a detailed analysis of the lowest-energy excited singlet state [10], which was followed by the publication of hundreds of papers, investigating theoretical and experimental photophysical and electrochemical properties to establish a structure-property relationship in terthiophenes and oligothiophenes [11][12][13][14][15][16][17]. Pappenfus and coworkers synthesized a terthiophene-based quinodimethane derivative and fabricated a thin-film field-effect transistor to measure the charge mobility [14,15]. These studies have also immensely helped to understand and extrapolate the photophysical, thermal, electrochemical, and charge transport properties of polythiophenes, albeit theoretically. Furthermore, the self-assembly of organic semiconductors plays an important role in electronic transportation, thus acting as a deciding factor in the performance of an organic optoelectronic device [18,19].
The synthesis, purification, and characterization of alkyl-substituted and/or alkylcapped oligothiophene have been reported in literature [20,21]. However, the crystal structure of methyl-capped terthiophene has been missing. Herein we describe the synthesis, single-crystal X-ray structure, and crystal packing of 5,5"-dimethyl-2,2′:5′,2″-terthiophene (DM3T) (Figure 1). Weak hydrogen bonding-driven supramolecular self-assembly of DM3T was studied, and Hirshfeld surface analysis was carried out to support the interactions. Furthermore, in our recently published study, the supramolecular self-assemblies of thiophene derivatives via halogen bonding [22] led to the observation of a N···S interaction between the S-atom of a thiophene derivative and N-atom of 4,4′-bipyridine (44BiPy) [23,24]. To verify the universal viability of the N···S interaction, we co-crystallized DM3T with 4,4′-bipyridine (44BiPy) via slow evaporation of the solvent, hoping that these two molecules would organize into a supramolecular self-assembly via chalcogen bonding (ChB). However, this experiment led to a totally unexpected result. The crystal structure and Hirshfeld surface analysis of DM3T-44BiPy is presented. We also present the synthesis of (5,5′′-dimethyl-[2,2′:5′,2″-terthiophen]-3′-yl)methanol (DM3TMeOH) and its hydrogen-bonded cocrystal structure analysis with 44BiPy. A detailed comparison of structural analysis of DM3T, DM3T-44BiPY, and DM3TMeOH-44BiPy is presented. We then discuss the photophysical properties and fluorescence quenching of DM3T and DM3TMeOH in the presence of 44BiPy. The chemical structures of the DM3T, DM3TMeOH, and 44BiPy are shown in Figure 1. The crystal structure and Hirshfeld surface analysis of DM3T-44BiPy is presented. We also present the synthesis of (5,5 -dimethyl-[2,2 :5 ,2 -terthiophen]-3 -yl)methanol (DM3TMeOH) and its hydrogen-bonded cocrystal structure analysis with 44BiPy. A detailed comparison of structural analysis of DM3T, DM3T-44BiPY, and DM3TMeOH-44BiPy is presented. We then discuss the photophysical properties and fluorescence quenching of DM3T and DM3TMeOH in the presence of 44BiPy. The chemical structures of the DM3T, DM3TMeOH, and 44BiPy are shown in Figure 1.

Synthesis
DM3T was prepared by a palladium-catalyzed Suzuki cross-coupling reaction [25] between 2,5-dibromothiophene and 5-methylthiophene-2-boronic acid pinacol ester in the presence of tetrakis(triphenylphosphine)palladium (Pd(PPh 3 ) 4 ) as a catalyst derivative ( Figures S5 and S6, see Supplementary Materials). On the other hand, DM3TMeOH was prepared starting from 3-thiophenemethanol (TMeOH) via a multistep organic synthesis procedure as depicted in Scheme 1. Briefly, the bromination of TMeOH with NBS in dichloromethane at room temperature gave a dibromo derivative (DBTMeOH) which was subsequently subjected to protection of -OH group by tert-butyldimethylsilyl chloride (TBDMSCl). Following the same Suzuki cross-coupling reaction conditions and reagents as used to synthesize DM3T except using newly synthesized DBTMeOTBDMS instead of 2,5-dibromothiophene gave the -OH-protected desired terthiophene derivative, DM3TMeOTBDMS, which was easily deprotected by treatment with TBAF in THF at room temperature to yield DBTMeOH ( Figures S7 and S8

Synthesis
DM3T was prepared by a palladium-catalyzed Suzuki cross-coupling reaction [25] between 2,5-dibromothiophene and 5-methylthiophene-2-boronic acid pinacol ester in the presence of tetrakis(triphenylphosphine)palladium (Pd(PPh3)4) as a catalyst derivative ( Figures S5 and S6, see Supplementary Materials). On the other hand, DM3TMeOH was prepared starting from 3-thiophenemethanol (TMeOH) via a multistep organic synthesis procedure as depicted in Scheme 1. Briefly, the bromination of TMeOH with NBS in dichloromethane at room temperature gave a dibromo derivative (DBTMeOH) which was subsequently subjected to protection of -OH group by tert-butyldimethylsilyl chloride (TBDMSCl). Following the same Suzuki cross-coupling reaction conditions and reagents as used to synthesize DM3T except using newly synthesized DBTMeOTBDMS instead of 2,5-dibromothiophene gave the -OH-protected desired terthiophene derivative, DM3TMeOTBDMS, which was easily deprotected by treatment with TBAF in THF at room temperature to yield DBTMeOH ( Figures S7 and S8

Crystal Growth
Crystal growth was conducted via slow evaporation of a mixture of solvents. Brightgreen-yellow single crystals of DM3T were obtained from slow evaporation of a dichloromethane and hexane solution. Similarly, pale-yellow needle-shaped cocrystals were obtained from a solution consisting of DM3T (2 equiv.) and 44BiPy (3 equiv.), while palegreen cocrystals were obtained for DM3TMeOH-44BiPy from a solution of DM3TMeOH (2 equiv.) and 44BiPy (1 equiv.). All single crystals were subsequently analyzed.

DM3T
Single-crystal X-ray diffraction analysis revealed the characteristic conformational parameters of DM3T. DM3T crystallized in the monoclinic non-centrosymmetric space group P21 with four molecules per unit cell. All the thiophene units adopted an S-trans conformation with slightly curved molecular plane geometry ( Figure 2). The asymmetric unit was composed of two DM3T molecules, held together by strong C-H···π interactions. These molecules aligned themselves at an angle of 57.95° with respect to their molecular planes. To form the single crystal, the neighboring molecules organized themselves longitudinally and transversally via several noncovalent interactions. The metrics of all the noncovalent interactions present in the DM3T single crystal are summarized in Table 1.

Crystal Growth
Crystal growth was conducted via slow evaporation of a mixture of solvents. Bright-greenyellow single crystals of DM3T were obtained from slow evaporation of a dichloromethane and hexane solution. Similarly, pale-yellow needle-shaped cocrystals were obtained from a solution consisting of DM3T (2 equiv.) and 44BiPy (3 equiv.), while pale-green cocrystals were obtained for DM3TMeOH-44BiPy from a solution of DM3TMeOH (2 equiv.) and 44BiPy (1 equiv.). All single crystals were subsequently analyzed.

Single-Crystal X-ray Diffraction Analysis
Single-crystal X-ray diffraction analysis revealed the characteristic conformational parameters of DM3T. DM3T crystallized in the monoclinic non-centrosymmetric space group P2 1 with four molecules per unit cell. All the thiophene units adopted an S-trans conformation with slightly curved molecular plane geometry ( Figure 2). The asymmetric unit was composed of two DM3T molecules, held together by strong C-H···π interactions. These molecules aligned themselves at an angle of 57.95 • with respect to their molecular planes. To form the single crystal, the neighboring molecules organized themselves longitudinally and transversally via several noncovalent interactions. The metrics of all the noncovalent interactions present in the DM3T single crystal are summarized in Table 1 In the transverse arrangement of DM3T molecules, several noncovalent interactions were observed. In addition to the intermolecular C21-H21···S1 and intramolecular C11-H11···S2 hydrogen bonds, there were strong C-H···π interactions involving C3-H3·· π, C8-H8···π, C24-H24···π, and C28-H28···π. Furthermore, weak chalcogen bonds (ChBs) were evidenced by the S23···π interaction (d = 3.868 Å), as well as chalcogen-chalcogen contacts between S1 and S21 (d = 3.690(3) Å). Although the distances between these noncovalent interactions were slightly higher than the sum of their van der Waals radii [26], their presence was supported by Hirshfeld surface analysis. The supramolecular packing exhibited a herringbone pattern. In the transverse arrangement of DM3T molecules, several noncovalent interactions were observed. In addition to the intermolecular C21-H21···S1 and intramolecular C11-H11···S2 hydrogen bonds, there were strong C-H···π interactions involving C3-H3·· π, C8-H8···π, C24-H24···π, and C28-H28···π. Furthermore, weak chalcogen bonds (ChBs) were evidenced by the S23···π interaction (d = 3.868 Å), as well as chalcogen-chalcogen contacts between S1 and S21 (d = 3.690(3) Å). Although the distances between these noncovalent interactions were slightly higher than the sum of their van der Waals radii [26], their presence was supported by Hirshfeld surface analysis. The supramolecular packing exhibited a herringbone pattern. The relative strengths and contributions of intermolecular interactions of a crystalline compound can be visualized by Hirshfeld surface analysis. For this purpose, a software program, CrystalExplorer (Version 21.5, Revision: 608bb32), was used to generate and analyze the Hirshfeld surface ( Figure 3), shape index, and curvedness surfaces ( Figure S3, see Supplementary Materials). In our study, we conducted an in-depth analysis of the crystal packing of DM3T using Hirshfeld surface analysis and fingerprint plots. Figure 4 presents the overall and resolved 2D fingerprint plots of DM3T, which provide valuable insights into the atom pair interactions and their relative contributions to the Hirshfeld surface.   The fingerprint plots revealed that the major contributions to the Hirshfeld surface of DM3T arose from three types of interactions: H···H (40.2%), C···H/H···C (29.7%), and S···H/H···S (18.7%). These interactions involved hydrogen bonding, as well as C-H···π interactions between carbon and hydrogen atoms. The significant contribution from H···H interactions suggests that the vast majority of London dispersion forces were acting within the crystal structure. Additionally, the fingerprint plots showed lower proportions of S···C/C···S (7.8%) and S···S (3.6%) interactions. The presence of S···C/C···S interactions indicates the presence of chalcogen bonds, while S···S interactions represent the chalcogen-chalcogen contacts, and both contribute to the overall crystal packing of DM3T. The Hirshfeld surface analysis, combined with the fingerprint plots, provides a comprehensive understanding of the atom pair interactions such as HB, CH···π, ChB, and S···S contacts and highlights their significance in the arrangement of DM3T molecules within the crystal lattice.

DM3T-44BiPy
Single-crystal X-ray diffraction analysis of the cocrystal agreed well with the expected structure of the constituents, DM3T and 44BiPy, as shown in Figure 5. The cocrystal belonged to the triclinic space group P1 with five molecules in the asymmetric unit, two DM3T and three 44BiPy molecules. In DM3T, all the thiophene units were in S-trans conformation. These molecules were held together by strong HB, C-H···π, and S···S interactions.

DM3T-44BiPy
Single-crystal X-ray diffraction analysis of the cocrystal agreed well with the expected structure of the constituents, DM3T and 44BiPy, as shown in Figure 5. The cocrystal belonged to the triclinic space group P1 with five molecules in the asymmetric unit, two DM3T and three 44BiPy molecules. In DM3T, all the thiophene units were in S-trans conformation. These molecules were held together by strong HB, C-H···π, and S···S interactions.
The typical distances of C-H···π interactions were within the range of 2.714-3.094 Å, while the S6···S6 separation was measured at 3.554 Å, which is approximately 1.3% shorter than the sum of van der Waals radii of sulfur atoms ( Figure 5). Even stronger S···S short contacts, with separation measured at 3.491 Å, were observed and reported for 2,2 :5 ,2 -terthiophene-5-carbaldehyde [27]. Figure S1 shows the complex network of HBs involving C-H···N interactions in cohesion of 44BiPy molecules. The details of all noncovalent interactions are summarized in Table 2. Crystal data, data collection, and structure refinement details are summarized in Table S1. The typical distances of C-H···π interactions were within the range of 2.714-3.094 Å, while the S6···S6 separation was measured at 3.554 Å, which is approximately 1.3% shorter than the sum of van der Waals radii of sulfur atoms ( Figure 5). Even stronger S···S short contacts, with separation measured at 3.491 Å, were observed and reported for 2,2′:5′,2′′terthiophene-5-carbaldehyde [27]. Figure S1 shows the complex network of HBs involving C-H···N interactions in cohesion of 44BiPy molecules. The details of all noncovalent interactions are summarized in Table 2. Crystal data, data collection, and structure refinement details are summarized in Table S1.   The supramolecular cocrystal packing of DM3T-44BiPy revealed a remarkable and distinctive layered structure, as depicted in Figure 6. Both DM3T and 44BiPy compounds self-organized into independent infinite layers, which were stacked on top of one another and connected by weak hydrogen-bonding interactions. The DM3T layer was primarily stabilized by a combination of hydrogen bonding and short contacts between sulfur atoms (S···S). In contrast, the 44BiPy molecules formed an infinite layer characterized by a complex arrangement, primarily stabilized by strong HBs. distinctive layered structure, as depicted in Figure 6. Both DM3T and 44BiPy compounds self-organized into independent infinite layers, which were stacked on top of one another and connected by weak hydrogen-bonding interactions. The DM3T layer was primarily stabilized by a combination of hydrogen bonding and short contacts between sulfur atoms (S···S). In contrast, the 44BiPy molecules formed an infinite layer characterized by a complex arrangement, primarily stabilized by strong HBs. Figure 6 illustrates that the average distance between any two layers of DM3T and 44BiPy was measured to be 15.291 Å and 14.076 Å, respectively. These data highlight the separation between adjacent layers in the crystal structure.
The observed layered arrangement and intermolecular interactions in the supramolecular cocrystal packing of DM3T-44BiPy are noteworthy. The distinct characteristics of the individual layers and their stacking provide valuable insights into the crystal packing structure. Understanding these arrangements is crucial for comprehending the properties and potential applications of this cocrystal system (see Section 2.4).  Figure 7 presents the Hirshfeld surface of DM3T-44BiPy, visualized by mapping over dnorm within the range of −0.05 to 1.30 Å. The surface was prominently filled with red spots, indicating regions where the intermolecular contacts were shorter than the van der Waals separation. These spots were attributed to a complex network of hydrogen bonds,  Figure 6 illustrates that the average distance between any two layers of DM3T and 44BiPy was measured to be 15.291 Å and 14.076 Å, respectively. These data highlight the separation between adjacent layers in the crystal structure.
The observed layered arrangement and intermolecular interactions in the supramolecular cocrystal packing of DM3T-44BiPy are noteworthy. The distinct characteristics of the individual layers and their stacking provide valuable insights into the crystal packing structure. Understanding these arrangements is crucial for comprehending the properties and potential applications of this cocrystal system (see Section 2.4). Figure 7 presents the Hirshfeld surface of DM3T-44BiPy, visualized by mapping over d norm within the range of −0.05 to 1.30 Å. The surface was prominently filled with red spots, indicating regions where the intermolecular contacts were shorter than the van der Waals separation. These spots were attributed to a complex network of hydrogen bonds, as observed in the X-ray structure of DM3T-44BiPy ( Figure S1, see Supplementary Materials). The formation of these hydrogen bonds contributed to the overall stability and organization of the crystal structure. Additionally, the shape index and curvedness surfaces, which provide further insights into the molecular arrangement, were generated ( Figure S3, see Supplementary Materials). Figure 8 depicts the overall and resolved 2D fingerprint plots, which illustrate the atom pair interactions and their respective contributions to the Hirshfeld surface of DM3T-44BiPy. As anticipated, the major contributions stemmed from various types of hydrogenbonding interactions, occurring simultaneously within the crystal structure. The relative contributions of these interactions were as follows: H···H (41.5%), C···H/H···C (28.9%), N···H/H···N (12.9%), and S···H/H···S (9.9%). While the proportions of S···C/C···S (4.0%) and S···S (2.0%) interactions were relatively low, they were still significant enough to confirm their presence in the crystal packing. In contrast, the contributions from C···N/N···C (0.5%) and C···C/C···C (0.3%) interactions were negligible, aligning with the findings of the X-ray structure. as observed in the X-ray structure of DM3T-44BiPy ( Figure S1, see Supplementary Materials). The formation of these hydrogen bonds contributed to the overall stability and organization of the crystal structure. Additionally, the shape index and curvedness surfaces, which provide further insights into the molecular arrangement, were generated ( Figure  S3, see Supplementary Materials).  Figure 8 depicts the overall and resolved 2D fingerprint plots, which illustrate the atom pair interactions and their respective contributions to the Hirshfeld surface of DM3T-44BiPy. As anticipated, the major contributions stemmed from various types of hydrogen-bonding interactions, occurring simultaneously within the crystal structure. The relative contributions of these interactions were as follows: H···H (41.5%), C···H/H···C (28.9%), N···H/H···N (12.9%), and S···H/H···S (9.9%). While the proportions of S···C/C···S (4.0%) and S···S (2.0%) interactions were relatively low, they were still significant enough to confirm their presence in the crystal packing. In contrast, the contributions from C···N/N···C (0.5%) and C···C/C···C (0.3%) interactions were negligible, aligning with the findings of the X-ray structure.
Notably, the Hirshfeld surface analysis combined with the fingerprint plots revealed a complete absence of N···S/S···N interactions (0%). This finding elucidates the layered crystal packing observed in DM3T-44BiPy.
The comprehensive understanding of the atom pair interactions and their contributions provided by these analyses enhances our knowledge of the crystal packing of DM3T-44BiPy. The dominance of hydrogen-bonding interactions, along with the confirmation of other intermolecular contacts, explains the layered organization observed in the crystal structure. Further investigations can delve into the implications of these interactions on the physical and chemical properties of DM3T-44BiPy, facilitating the development of advanced materials and functional devices. Single X-ray diffraction analysis confirmed the presence of both constituents, DM3TMeOH and 44BiPy, in the cocrystal (Figure 9). The supramolecular complex belonged to the triclinic space group P 1 , with the asymmetric unit consisting of one DM3TMeOH and one 44BiPy molecule. In the structure, a cyclic motif was formed by four units, comprising two bipyridine and two terthiophene molecules (Figure 9). The or- Notably, the Hirshfeld surface analysis combined with the fingerprint plots revealed a complete absence of N···S/S···N interactions (0%). This finding elucidates the layered crystal packing observed in DM3T-44BiPy.
The comprehensive understanding of the atom pair interactions and their contributions provided by these analyses enhances our knowledge of the crystal packing of DM3T-44BiPy. The dominance of hydrogen-bonding interactions, along with the confirmation of other intermolecular contacts, explains the layered organization observed in the crystal structure. Further investigations can delve into the implications of these interactions on the physical and chemical properties of DM3T-44BiPy, facilitating the development of advanced materials and functional devices.

DM3TMeOH-44BiPy
Single X-ray diffraction analysis confirmed the presence of both constituents, DM3TMeOH and 44BiPy, in the cocrystal (Figure 9). The supramolecular complex belonged to the triclinic space group P1, with the asymmetric unit consisting of one DM3TMeOH and one 44BiPy molecule. In the structure, a cyclic motif was formed by four units, comprising two bipyridine and two terthiophene molecules ( Figure 9). The organization of these units was governed by HBs involving C-H···O, O-H···N, and C-H···S interactions ( Figure S2). Specifically, the hydrogen bonds O1-H1···N2 and C15-H15B···N1, with lengths of 2.053 Å and 2.557 Å, respectively, played a crucial role in forming the cyclic arrangement observed in the crystal structure. More details about the metrics of noncovalent interactions can be found in Table 3. interactions ( Figure S2). Specifically, the hydrogen bonds O1-H1···N2 and C15-H15B···N1, with lengths of 2.053 Å and 2.557 Å, respectively, played a crucial role in forming the cyclic arrangement observed in the crystal structure. More details about the metrics of noncovalent interactions can be found in Table 3.
Remarkably The findings from the X-ray diffraction analysis provide valuable insights into the structural characteristics and bonding arrangements within the DM3TMeOH-44BiPy cocrystal. Understanding the intermolecular and intramolecular hydrogen-bonding interactions contributes to our knowledge of the stability and conformational preferences of the cocrystal. These insights can guide further investigations into the properties and potential  Remarkably, the presence of intramolecular hydrogen bonding influenced by C7-H7···O1 (with a length of 2.389 Å) led to the adoption of the S-cis conformation by the 5-methyl-2-thienyl unit attached to the 2-position of the central 3-thiophenemethanol unit in DM3TMeOH.
The findings from the X-ray diffraction analysis provide valuable insights into the structural characteristics and bonding arrangements within the DM3TMeOH-44BiPy cocrystal. Understanding the intermolecular and intramolecular hydrogen-bonding interactions contributes to our knowledge of the stability and conformational preferences of the cocrystal. These insights can guide further investigations into the properties and potential applications of this cocrystal system (see Section 2.4).
In the crystal structure, the arrangement of molecules in the DM3TMeOH-44BiPy cocrystal exhibited the formation of molecular sheets that are parallel to the bc plane (as depicted in Figure 10). These molecular sheets were constructed through weak hydrogen bonds between neighboring cyclic motifs, specifically, the hydrogen bond C8-H8···O1, with a bond length of 2.616 Å. a Distance between H-atom and centroid of the thiophene ring. b Distance between C-atom and centroid of the thiophene ring. c Angle of C, H, and centroid of the thiophene ring.
In the crystal structure, the arrangement of molecules in the DM3TMeOH-44BiPy cocrystal exhibited the formation of molecular sheets that are parallel to the bc plane (as depicted in Figure 10). These molecular sheets were constructed through weak hydrogen bonds between neighboring cyclic motifs, specifically, the hydrogen bond C8-H8···O1, with a bond length of 2.616 Å. Furthermore, the molecules were held together by additional hydrogen bonds along the a-axis. These hydrogen bonds included C15-H15A···S1, with a bond length of 2.950 Å, and C15-H15A···π, with a separation measured at 2.638 Å. The C-H···π interactions coupled with the intermolecular HBs played a significant role in stabilizing the crystal structure of the DM3TMeOH-44BiPy cocrystal (Figure 11). Like DM3T-44BiPy cocrystal, the Hirshfeld surface analysis of DM3TMeOH-44BiPy revealed the presence of red spots corresponding to various hydrogen bonds observed in the X-ray structure ( Figure 12). Notably, due to the hydroxymethyl (-CH2OH) group present in DM3TMeOH, the red spot corresponding to the O···H interaction is particularly prominent on the surface, indicating its strength and size.  Like DM3T-44BiPy cocrystal, the Hirshfeld surface analysis of DM3TMeOH-44BiPy revealed the presence of red spots corresponding to various hydrogen bonds observed in the X-ray structure ( Figure 12). Notably, due to the hydroxymethyl (-CH 2 OH) group present in DM3TMeOH, the red spot corresponding to the O···H interaction is particularly prominent on the surface, indicating its strength and size. Like DM3T-44BiPy cocrystal, the Hirshfeld surface analysis of DM3TMeOH-44BiPy revealed the presence of red spots corresponding to various hydrogen bonds observed in the X-ray structure ( Figure 12). Notably, due to the hydroxymethyl (-CH2OH) group present in DM3TMeOH, the red spot corresponding to the O···H interaction is particularly prominent on the surface, indicating its strength and size.  (Figure 13). Once again, the major contributions arose from the simultaneous occurrence of various  (Figure 13). Once again, the major contributions arose from the simultaneous occurrence of various hydrogenbonding interactions. However, an important observation is that the relative proportions of N···H/H···N (7.2%) and S···H/H···S (14.1%) interactions in DM3TMeOH-44BiPy were reversed compared to those in DM3T-44BiPy, where N···H/H···N accounted for 12.9% and S···H/H···S accounted for 9.9%. This reversal was attributed to the extensive complex network of hydrogen bonds observed within the 44BiPy layer of the DM3T-44BiPy crystal, which changed to linear hydrogen-bonding interactions between DM3TMeOH and 44BiPy in the DM3TMeOH-44BiPy cocrystal. hydrogen-bonding interactions. However, an important observation is that the relative proportions of N···H/H···N (7.2%) and S···H/H···S (14.1%) interactions in DM3TMeOH-44BiPy were reversed compared to those in DM3T-44BiPy, where N···H/H···N accounted for 12.9% and S···H/H···S accounted for 9.9%. This reversal was attributed to the extensive complex network of hydrogen bonds observed within the 44BiPy layer of the DM3T-44BiPy crystal, which changed to linear hydrogen-bonding interactions between DM3TMeOH and 44BiPy in the DM3TMeOH-44BiPy cocrystal.  Furthermore, the proportion of S···S (1.4%) interactions confirms their presence in the crystal packing, while the insignificant proportion of C···C/C···C (0.8%) interactions ruled out the occurrence of π-π stacking, which aligns with the observations from the X-ray structure of DM3TMeOH-44BiPy.

Photophysical Properties
In the literature, the photophysical properties of α-oligothiophenes (n = 1-7, where n is the number of thiophene rings) have been extensively studied both theoretically and experimentally [28,29]. We also investigated the photophysical properties of our newly synthesized terthiophene derivatives, DM3T and DM3TMeOH, and their binding with 44BiPy in solution and solid-state using UV/visible spectroscopy and fluorescence spectroscopy. The UV/visible spectra of all materials were recorded in chloroform solution at room temperature and are presented in Figure S4 (see Supplementary Materials).
As anticipated, the UV/visible absorption spectrum of DM3T in chloroform solution was devoid of structural features and exhibited a single broad absorption band at 365 nm (reported literature value of λ abs,max at 354 nm in dioxane [28]). This characteristic electronic spectrum is typical of oligothiophenes lacking distinct structural features and is attributed to the π(1 1 A g )-π*(1 1 B u ) transition (S 0 →S 1 ) of the oligothiophene backbone [28,30]. Importantly, this electronic spectrum is known to be unaffected by the presence of foreign species; in line with expectations, the presence of 44BiPy did not show any noticeable effect on the absorption spectra of DM3T [30]. In the solid state, the overall absorption spectrum region remains unaffected but the absorbance of both DM3T and DM3T-44BiPy decreased significantly as the bulk of the material remained unexcited.
Similarly, DM3TMeOH was also devoid of structural features and displayed only a single broad absorption band with slight blue-shift by 8 nm compared to that of DM3T. This blue-shift was attributed to the S-cis configuration of the terthiophene units in the ground state. Like DM3T in the solution state, the absorption spectrum of DM3TMeOH remained unaffected by the presence of 44BiPy. In the solid state, DM3TMeOH-44BiPy exhibited similar absorption to that of DM3TMeOH in the solution state.
Moving on to the emission properties, Figure 14 depicts the fluorescence spectra of all materials, recorded both in solution and in the solid state at room temperature along with emission colors under a UV lamp (λ = 365 nm). The fluorescence spectrum exhibits the distinctive vibronic features typically observed in terthiophenes. The origin of these vibronic features in the fluorescence spectrum of oligothiophenes has been the subject of detailed theoretical and experimental investigations, which have been reported in previous studies [28][29][30][31]. It is well established that the α-oligothiophenes adopt a quinoid planar geometry in the excited state. As a result of rigid and planar structure, the fluorescence spectra appeared with well-resolved vibronic features as the molecules of α-oligothiophenes relaxed back to the aromatic ground state radiatively.
In chloroform solution, DM3T exhibited characteristic well-resolved vibronic features at 421 nm, 442 nm, and 473 nm. This is consistent with the previous literature that reported maximum fluorescence at 407 nm and 426 nm in dioxane [28]. Compared to the solution state, the entire fluorescence spectrum of DM3T experienced a red-shift of 40 nm in the solid state due to the aggregation-caused quenching (ACQ) effect [32], while maintaining its structural features (Figure 14a,b).
Upon the addition of 44BiPy, fluorescence quenching was observed in the solution state, and this quenching became more pronounced in the solid state. This suggests an electron transfer process from DM3T to 44BiPy in the excited state. Interestingly, in the solid state of DM3T-44BiPy, the vibronic band at 465 nm completely disappeared, and the broad shoulder of DM3T's emission spectrum became a distinct emission band. On the basis of the energetics of DM3T's electronic states, this indicates that electron transfer occurred from DM3T's 1B u electronic state to the lowest unoccupied molecular orbital (LUMO) of 44BiPy. In chloroform solution, DM3T exhibited characteristic well-resolved vibronic features at 421 nm, 442 nm, and 473 nm. This is consistent with the previous literature that reported maximum fluorescence at 407 nm and 426 nm in dioxane [28]. Compared to the solution state, the entire fluorescence spectrum of DM3T experienced a red-shift of 40 nm in the solid state due to the aggregation-caused quenching (ACQ) effect [32], while maintaining its structural features (Figure 14a,b).
Upon the addition of 44BiPy, fluorescence quenching was observed in the solution state, and this quenching became more pronounced in the solid state. This suggests an electron transfer process from DM3T to 44BiPy in the excited state. Interestingly, in the solid state of DM3T-44BiPy, the vibronic band at 465 nm completely disappeared, and the broad shoulder of DM3T's emission spectrum became a distinct emission band. On the basis of the energetics of DM3T's electronic states, this indicates that electron transfer occurred from DM3T's 1Bu electronic state to the lowest unoccupied molecular orbital (LUMO) of 44BiPy.
Similarly, DM3TMeOH exhibited vibronic bands at 428 nm and 448 nm in its fluorescence spectrum in the solution state. In the presence of 44BiPy, pronounced fluorescence quenching was observed due to the formation of strong hydrogen bonds ( Figure  14c). In the solid state, both DM3TMeOH and DM3TMeOH-44BiPy became non-luminescent due to aggregation driven by strong hydrogen bonding (Figure 14d). Similarly, DM3TMeOH exhibited vibronic bands at 428 nm and 448 nm in its fluorescence spectrum in the solution state. In the presence of 44BiPy, pronounced fluorescence quenching was observed due to the formation of strong hydrogen bonds (Figure 14c). In the solid state, both DM3TMeOH and DM3TMeOH-44BiPy became non-luminescent due to aggregation driven by strong hydrogen bonding (Figure 14d).

Discussion
In this section, we provide a comparative discussion of the X-ray structure and the Hirshfeld surface analysis of DM3T, DM3T-44BiPy, and DM3TMeOH-44BiPy. The crystallographic data and refinement parameters for these compounds are summarized in Table  S1. DM3T crystallized in the monoclinic crystal system with space group P2 1 , while both DM3T-44BiPy and DM3TMeOH-44BiPy crystallized in the triclinic space group P1.
In the X-ray structure of DM3T, all thiophene units adopted an S-trans conformation with a slightly curved molecular plane geometry. This conformation was maintained within the DM3T layer of its cocrystal with 44BiPy, although the planar geometry was further distorted. In contrast, the thiophene units in DM3TMeOH adopted a combination of S-trans and S-cis conformations. The S-trans portion of the molecule remained planar, while the S-cis part adopted an out-of-plane geometry.
The DM3T molecules in the DM3T-44BiPy cocrystal continued to exhibit a herringbone pattern. However, due to the absence of desired N···S interactions, the strong hydrogen bonds within DM3T and 44BiPy molecules resulted in an almost independent layered structure of DM3T-44BiPy. On the other hand, the presence of a hydroxymethyl group on DM3TMeOH ensures that the self-assembly of DM3TMeOH with 44BiPy was exclusively directed by hydrogen bonding involving O-H···N interactions, forming a cyclic motif.
The resolved 2D fingerprint plots in all cases revealed that hydrogen bonds were the major contributors to the overall Hirshfeld surface. Interestingly, the relative proportions of N···H/H···N (12.9%) and S···H/H···S (9.9%) interactions in DM3T-44BiPy were reversed compared to N···H/H···N (7.2%) and S···H/H···S (14.1%) interactions in DM3TMeOH-44BiPy. This change in proportions reflected the difference in crystal packing, transitioning from an almost independent layered cocrystal to a molecular packing arrangement involving a cyclic motif, although both self-assemblies were directed by hydrogen bonds.
In summary, the X-ray structures and Hirshfeld surface analyses provided valuable insights into the molecular arrangements and intermolecular interactions in DM3T, DM3T-44BiPy, and DM3TMeOH-44BiPy. The differences observed in their crystal packings and hydrogen-bonding patterns highlighted the influence of molecular composition and functional groups on the supramolecular organization of these cocrystals. The findings of photophysical properties investigations demonstrated the influence of 44BiPy on the fluorescence properties of both DM3T and DM3TMeOH, suggesting electron transfer and fluorescence-quenching effects in the presence of 44BiPy. The solid-state behavior of these systems highlighted the impact of aggregation and hydrogen bonding on their luminescent properties.

Materials and Methods
General experimental information. Solution NMR spectroscopy analyses were performed at the Centre d'Instrumentation en Resonance Magnétique (CIREM) of the Université Libre de Bruxelles in Belgium. 1 H-and 13 C-NMR spectra were recorded on JEOL 400 Hz spectrometers at 298 K. CDCl 3 was used as received (purchased from Eurisotop, France). The residual nondeuterated solvent was used as an internal standard for calibration of 1 H-and 13 C-NMR spectra. Chemical shifts (δ) are expressed in ppm, and coupling constants values ( n J) are expressed in Hz. Abbreviations used for NMR spectra are as follows: s, singlet; d, doublet; m, multiplet.
Data collection and refinement. Single-crystal data collection (at 100 K) and evaluation of the cocrystal, DM3T-44BiPy, was performed on a Rigaku Oxford Diffraction Supernova Dual Source (Cu at zero) diffractometer equipped with an Atlas CCD detector using ω scans and Mo Kα (λ = 0.71073 Å) radiation. The images were interpreted and integrated with the program CrysAlisPro [35]. Using Olex2 [36], the structure was solved by direct methods using the ShelXT structure solution program and refined by full-matrix least squares on F2 using the ShelXL program package [37,38]. Non-hydrogen atoms were anisotropically refined, and the hydrogen atoms were in riding mode with isotropic temperature factors fixed at 1.2 times U(eq) of the parent atoms.
UV/visible and fluorescence spectroscopy. The HPLC-grade chloroform solvent was used for solution preparations. All solutions were in ranges of 10 −5 to 10 −6 M. Solidstate samples were prepared using the solution drop-cast method on a glass slide by dissolving 1 mg of sample in 100 µL of chloroform. Absorption spectra were recorded on a Shimazu spectrophotometer UV-1800, and fluorescence spectra were recorded on a HORIBA Fluoromax-4_1507D-3516-FM fluorescence spectrometer at room temperature. For DM3T and DM3T-44BiPy, the excitation wavelength was 365 nm for both the solution and the solid state, while the excitation wavelength of 357 nm was used for DM3TMeOH and DM3TMeOH-44BiPy samples.

Conclusions
In our study, we presented the synthesis and self-organization of methyl-capped terthiophene (DM3T) and its methyl alcohol derivative in combination with 4,4 -bipyridine (44BiPy). Through single-crystal X-ray diffraction analysis, we made the unexpected discovery of a three-dimensional stacked, layered organization of DM3T and 44BiPy. These layers were found to be nearly independent of each other and held together by weak hydrogen bonds. The investigation of the photophysical properties of this system revealed a strong fluorescence quenching of DM3T by 44BiPy in the solid state. This suggests an efficient charge transfer between the two components. Such phenomena are of significant interest in the development of energy-generation devices, particularly in the field of organic solar cells. Furthermore, we observed that DM3TMeOH, the methyl alcohol derivative of DM3T, organized itself in a closed cyclic motif with 44BiPy through strong hydrogen bonds. Overall, our findings shed light on the unique self-organization and supramolecular arrangements of DM3T and its derivatives with 44BiPy. The unexpected 3D stacked, layered organization, along with the efficient charge transfer offers new avenues for future research in self-organized layered materials. Further exploration of the photophysical properties and applications of this system could lead to advancements in the development of energy generation devices.