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Rational self-assembly of polygonal organic microcrystals for shape-dependent multi-directional 2D optical waveguides
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Chao-Fei Xua, Yue Yua, Qiang Lva, Chang-Cun Yana, Xue-Dong Wanga, *, Liang-Sheng Liaoa, b, *
Chinese Chemical Letters | 2022, 33(6) : 3255 - 3258
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Chinese Chemical Letters | 2022, 33(6): 3255-3258
• Communication •
Rational self-assembly of polygonal organic microcrystals for shape-dependent multi-directional 2D optical waveguides
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Chao-Fei Xua, Yue Yua, Qiang Lva, Chang-Cun Yana, Xue-Dong Wanga, *, Liang-Sheng Liaoa, b, *
Affiliations
  • a Jiangsu Key Laboratory for Carbon-Based Functional Materials and Devices, Institute of Functional Nano and Soft Materials (FUNSOM), Soochow University, Suzhou 215123, China
  • b Macao Institute of Materials Science and Engineering, Macau University of Science and Technology, Macau 999078, China
Published: 2022-06-15 doi: 10.1016/j.cclet.2021.10.076
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Micro-nano-level photonic waveguide regulation is essential for future on-chip photonic integrated systems and is still of great challenges. We report a molecular design strategy, changing the position of the methyl substituent makes the arrangement of the three isomer molecules different in their respective crystals. Based on this strategy, three sheet-like crystals with different polygonal morphologies were prepared via solution self-assembly approach. The in-depth optical measurements demonstrated that these three microsheet crystals have different 2D optical waveguide performances related to the shapes. Our work provides a feasible design strategy and material preparation method for realizing precise 2D optical waveguide modulation, which lays the foundation for complex photonic integrated systems in the future.

2D optical waveguide  /  Polygonal organic microcrystals  /  Optical waveguide modulation  /  Precise self-assembly  /  Molecular design
Chao-Fei Xu, Yue Yu, Qiang Lv, Chang-Cun Yan, Xue-Dong Wang, Liang-Sheng Liao. Rational self-assembly of polygonal organic microcrystals for shape-dependent multi-directional 2D optical waveguides[J]. Chinese Chemical Letters, 2022 , 33 (6) : 3255 -3258 . DOI: 10.1016/j.cclet.2021.10.076
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Due to the excellent optical properties and the inherent characteristics of organic semiconductor materials, organic semiconductor crystals, as a promising optoelectronic material [1], have received extensive attention in optoelectronic fields [2-4], including organic light-emitting diodes (OLEDs) [5, 6], organic field effect transistors (OFETs) [7, 8], organic solid-state lasers (OSSLs) [9, 10] and organic light-emitting transistors (OLETs) [11]. In particular, organic semiconductor crystals have the advantages such as ordered structures, uniform and regular cavities, as well as fewer defects [12], which are of great significance for the development of optical waveguide materials as the basic structure of photonics devices [13]. Therefore, a wide variety of organic semiconductor crystal materials with excellent optical waveguide properties have been prepared [14, 15]. For example, in the research of 1D optical waveguide materials, Bao et al. prepared high-quality perylene diimide (PDI) microwires with a uniform cylindrical shape and a length of several hundred microns to millimeters, which are ideal materials for low-loss and ultra-long optical waveguides and optoelectronic interconnectors [16]. Furthermore, through the efforts of scientists, the 1D optical waveguide material has developed from a straight single crystal to a flexible material with multiple excitations [17-19]. Zhao and co-workers controllably prepared two kinds of cocrystal polymorphs with different two-dimensional (2D) molecular orientations and nanophotonic transport behaviorfrom the same donor and acceptor. Based on the anisotropic waveguiding mechanism of the cocrystal, they constructed the directional signal outcoupler (DSO), which can be used for the high-fidelity and directional transmission of the real signal [20]. The research of these organic semiconductor crystal materials has paved the way for the exploration of multifunctional optical waveguide materials for future optoelectronic integrated circuits.
It has been demonstrated that the morphology of the crystal can be changed by adjusting the arrangement of molecules, thereby realizing the adjustment of the optical waveguide performance [21]. Yao et al. and his colleagues obtained different self-assembly organic crystals (nanowires and nanosheets) with different optical waveguide performances by adjusting the different dominant intermolecular interactions (H bonding and π-π stacking) through rational molecular design [22]. Notably, sheet-like micro-crystals used for photon conduction medium exhibit unique advantages compared with traditional one-dimensional (1D) crystal materials. These sheet-like crystals usually have polygonal morphology for the reason of π-π stacking in two directions between molecules [23], contributes to shape-dependent multi-directional 2D photon conduction within the crystal, which will be more suitable for future chip-level planar photonic integrated systems [24]. Furthermore, the control of photon conduction on the micro/nano scale via changing the shape of the polygonal microsheets through adjusting the molecular arrangement is crucial for the development of the integrated photonic system. In the previous study, Li et al. prepared two phases of perylene microcrystals by simply controlling the concentration of the solution. Perylene microcrystals with different polygonal shape were obtained because of the different molecular arrangement in these two phases, showing diverse emission colors and 2D optical waveguide performances [25]. However, this polymorph strategy is not suitable for all crystals, and there are few reports on universal molecular structure design strategies based on the same molecular skeleton to change the molecule arrangement of sheet-like crystals [26]. Therefore, it is still a challenge nowadays to adjust the shape-dependent multi-directional 2D optical waveguide performances of the sheet crystal.
Herein, a molecular design strategy was proposed based on the same isomer molecular skeleton to prepare three different microsheet crystals (Fig. 1a). The solid-state packing of the crystals is governed by π-π stacking in two directions, leading to a 2D molecular arrangement. This 2D molecular arrangement in the three microsheet crystals can be adjusted by only changing the position of the methyl substituents in the isomers, which contributes to different polygonal morphologies of the three microsheet crystals after subtle choice of the crystal growth conditions. Optical tests have demonstrated that the microsheets exhibit three different shape-dependent multi-directional 2D optical waveguide performances, suggesting potential applications in optical devices.
The microsheet crystals of 1, 4-bis(2-methylstyryl)benzene (o-MSB), 1, 4-bis(3-methylstyryl)benzene (m-MSB) (see synthesis method in Supporting information) and 1, 4-bis(4-methylstyryl)benzene (p-MSB) are prepared through the mixed solution self-assembly method. Typically, the dichloromethane (DCM) solution (5 mmol/L) of o-MSB or m-MSB and ethanol were mixed and dropped on the quartz substrate, then covered with a watch glass. After the solvent evaporated, large-scale microsheets can be observed. Due to the poor solubility of p-MSB in DCM, we chose carbon disulfide (CS2) as the solvent to prepare p-MSB microsheet crystals. The CS2 solution of p-MSB is directly dropped onto the quartz substrate, through the remaining same steps, large-scale p-MSB microsheets can be obtained.
The fluorescence microscopy (FM) images of obtained microsheets reveal that these microsheets have different morphologies due to the different positions of methyl substituent. As shown in Figs. 1b–d, the shapes of o-MSB, m-MSB and p-MSB microsheets are rectangle, parallelogram and hexagon, and the Inner angles of them are 90°, 80° and 103°, respectively. Meanwhile, the absorption and emission properties of the three crystals are also different, to reveal this difference, the absorption and emission spectra of these three microsheets were tested. Under the excitation of 375 nm ultraviolet light, the o-MSB and m-MSB microsheets show similar blue emission (455 nm), while the p-MSB microsheets show lighter sky-blue emission (500 nm). Besides, as shown in Fig. 1e, the maximum absorption wavelengths of o-MSB and m-MSB microsheets are 400 and 410 nm, respectively.
Through analyzing the single crystal data with Mercury package, the molecular packing of these three crystals were obtained (Figs. 2a–c). The existence of π-π stacking in two directions between molecules leads to the formation of 2D crystals. Furthermore, we simulated the growth morphology of these three crystals based on the attachment energies via using the Materials Studio package (Figs. 2d-f). According to the calculated results (Table S2 in Supporting information), the {001}s crystal planes of o-MSB and the {002}s crystal planes of m-MSB and p-MSB have the smallest attachment energy (Eatt) among various crystal faces as well as the corresponding highest exposed facet area percentage. In addition, the X-ray diffraction (XRD) measurements of the microcrystals demonstrated these crystal planes are dominant in the crystal (Fig. 2g), which makes the microcrystals easy to form sheet-like polygonal structures. The (XRD) measurement of o-MSB microsheets exhibits a series of intensive characteristic peaks that are from the same sequence of {001}s crystal planes. Likewise, the values of m-MSB and p-MSB microsheets exhibit a series of intensive characteristic peaks that are from the sequence of {002}s. The actual test results are consistent with the theoretical settlement data.
Importantly, based on the same molecular skeleton of the isomer, the changes in the positions of the methyl substituent leads to the different molecular arrangements in the crystals, which means that the shapes of the three microsheets are different, ultimately reflected in the three different 2D optical waveguide performances. In order to study the different 2D optical waveguide performances of these three crystals, the spatially resolved PL spectra of the microsheets excited by a 375 nm laser were performed (Fig. 3, Fig. 4). When the microsheet was excited, the photons propagated in the two-dimensional direction on the microsheet, resulting brighter blue emission at the edges than the middle part of the microsheet surface, which reveals that efficient light guiding can occur within the microsheets. These results demonstrate that the microsheets are excellent optical waveguide materials. Furthermore, it can be found that the optical waveguide performances of the three microsheet crystals are diverse and are related to the shape. Intuitively, o-MSB and m-MSB microsheets are both quadrilaterals with two sets of parallel sides, as a result, the photons propagate mainly in two directions parallel to the sides, and the angles between the two directions are equal to the inner angles of the quadrilaterals. In detail, the photons propagate on the o-MSB microsheets in two mutually perpendicular directions because of the rectangle, shape of o-MSB microsheets, while the m-MSB is a parallelogram with an acute angle of 80°, accordingly, the photons propagate along two directions with an angle of 80° In addition, it can be clearly noticed that the emission intensity at the midpoint of the edge decreases as the propagation length increases. The optical loss coefficients (α) were calculated by a nonlinear fitting equation (y = A1exp(-x/t1)). From the calculation results, the optical loss coefficients in the two directions of a typical o-MSB microsheet are, respectively, 0.142 and 0.080 dB/µm, which are very close, indicating that the crystal structure is uniform. The same test performed on m-MSB revealed that the m-MSB microsheet also have similar properties. The optical loss coefficient in direction Ⅰ (0.234 dB/µm) is almost equal to the value in direction Ⅱ (0.276 dB/µm) due to the uniformity of the crystal structure.
Different from the bidirectional 2D optical waveguides of the o-MSB and m-MSB microsheets, three-directional 2D optical waveguides is realized based on the p-MSB microsheets because of the hexagonal morphology of p-MSB microsheets. As shown by the dotted line in Fig. 4a, when a typical p-MSB microsheet was excited by a 375 nm laser, the photons propagated to the edges in three directions. The angles between these three directions have a certain relationship with the internal angle of the hexagon. Through measurement and calculation, the angle between directions, Ⅰ and Ⅱ is 18°, and the angles between directions Ⅰ, Ⅲ and directions Ⅱ, Ⅲ are 81° By changing the position of the excitation point and detecting the edges of the microsheet marked by the dashed frames, the spatially resolved PL spectrum in three directions varied with the propagation length were obtained. Similarly, through calculation, the optical loss coefficients (α) in the three directions are 0.264, 0.259 and 0.350 dB/µm, respectively. The small difference in the optical loss coefficients of the three directions indicates that p-MSB microsheets also have good uniformity of crystal.
In summary, three polygonal microsheet crystals of the three isomer materials were prepared via rational molecular structure design based on the same molecular skeleton. Structural analysis and morphological characterization revealed that the formation of the polygonal shapes of the microsheets is caused by the π-π stacking in two directions between molecules. The change of the position of the substituents changed the angle of π-π stacking and the molecular arrangement on a microscopic level, which further changed the shapes and internal angles of the microsheets on a macroscopic level. In the end, these all manifested in the different photon conduction directions and angles of on the microsheets, which means that the three microsheets achieved different shape-dependent multi-directional 2D optical waveguide performances. This molecular design strategy provides a feasible method for preparing sheet-like crystal materials with adjustable optical waveguide performances as photon transmission medium.
Declaration of competing interest
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There are no conflicts to declare.
Acknowledgments
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The authors acknowledge financial support from the National Natural Science Foundation of China (Nos. 21971185, 52173177), and this project is also funded by the Collaborative Innovation center of Suzhou Nano Science and Technology (CIC-Nano), and by the "111″ Project of the State Administration of Foreign Experts Affairs of China.
Supplementary materials
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Supplementary material associated with this article can be found, in the online version, at doi:10.1016/j.cclet.2021.10.076
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Year 2022 volume 33 Issue 6
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Article Info
doi: 10.1016/j.cclet.2021.10.076
  • Receive Date：2021-09-30
  • Online Date：2025-12-19
  • Published：2022-06-15
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  • Received：2021-09-30
  • Revised：2021-10-18
  • Accepted：2021-10-26
Affiliations
    a Jiangsu Key Laboratory for Carbon-Based Functional Materials and Devices, Institute of Functional Nano and Soft Materials (FUNSOM), Soochow University, Suzhou 215123, China
    b Macao Institute of Materials Science and Engineering, Macau University of Science and Technology, Macau 999078, China
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表12种不同金属材料的力学参数
科
Family		 属数
Number of
genus		 种数
Number of
species		 占总种数比例
Percentage of
total species (%)		 属
Genus		 种数
Number of
species		 占总种数比例
Percentage of total
species (%)
鹅膏菌科Amanitaceae 2 11 5.26 鹅膏菌属 Amanita 10 4.78
小菇科 Mycenaceae 2 12 5.74 丝盖伞属 Inocybe 5 2.39
多孔菌科 Polyporaceae 8 14 6.70 蜡蘑属 Laccaria 5 2.39
红菇科 Russulaceae 3 23 11.00 小皮伞属 Marasmius 6 2.87
小菇属 Mycena 11 5.26
光柄菇属 Pluteus 5 2.39
红菇属 Russula 17 8.13
栓菌属 Trametes 5 2.39
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