On-Surface Crystallization Behaviors of H-Bond Donor-Acceptor Complexes at Liquid/Solid Interfaces

被引:6
|
作者
Cheng, Linxiu [1 ,6 ]
Tu, Bin [2 ]
Xiao, Xunwen [3 ]
Feringan, Beatriz [4 ]
Gimenez, Raquel [4 ]
Li, Xiaokang [5 ]
Fang, Qaojun [2 ]
Sierra, Teresa [4 ]
Li, Yibao [5 ]
Zeng, Qingdao [1 ,6 ]
Wang, Chen [2 ]
机构
[1] Natl Ctr Nanosci & Technol NCNST, CAS Ctr Excellence Nanosci, CAS Key Lab Standardizat & Measurement Nanotechno, Beijing 100190, Peoples R China
[2] Natl Ctr Nanosci & Technol NCNST, CAS Ctr Excellence Nanosci, CAS Key Lab Biomed Effects Nanomat & Nanosafety, Beijing 100190, Peoples R China
[3] Ningbo Univ Technol, Coll Chem Engn, Ningbo 315016, Zhejiang, Peoples R China
[4] Univ Zaragoza, CSIC, ICMA, Dept Quim Organ, E-50009 Zaragoza, Spain
[5] Gannan Normal Univ, Key Lab Organopharmaceut Chem, Ganzhou 341000, Peoples R China
[6] Univ Chinese Acad Sci, Ctr Mat Sci & Optoelect Engn, Beijing 100049, Peoples R China
基金
中国国家自然科学基金;
关键词
MULTICOMPONENT SUPRAMOLECULAR NETWORKS; STRUCTURAL TRANSFORMATION; CORONENE CLUSTERS; SOLID INTERFACE; ASSEMBLIES; MOLECULES; GRAPHITE; CRYSTALS; MONOLAYERS; SUBSTRATE;
D O I
10.1021/acs.langmuir.9b01350
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
Two-dimensional (2D) crystallization behaviors of A-TPCn (n = 4, 6, 10), T3C(4), and hydrogen-bonded complexes T3C(4)@TPCn (n = 4, 6, 10) are investigated by means of scanning tunneling microscope (STM) observations and density functional theory (DFT) calculations. The STM observations reveal that A-TPC4, A-TPC10, and T3C(4) self-organize into dumbbell-shaped structures, well-ordered bright arrays, and zigzag structures, respectively. Interestingly, T3C(4)@TPC10 fails to form the cage-ball structure, whereas T3C(4)@TPC4 and T3C(4)@TPC6 co-assemble into cage-ball structures with the same lattice parameters. The filling rates of the balls of these two kinds of cage-ball structures depend heavily on the deposition sequence. As a result, the filling rates of the cages in T3C(4)/A-TPCn (n = 4, 6) with deposition of T3C(4) anterior to A-TPC are higher than those in A-TPCn/T3C(4) (n = 4, 6) with the opposite deposition sequence. Furthermore, lattice defects formed by T3C(4) coexist with the cage-ball structures. Moreover, the similar energy per unit area of lattice defects (-0.101 kcal mol(-1) angstrom(-2)) and the two cage-ball networks (-0.194 and -0.208 kcal mol(-1) angstrom(-2), respectively), illustrating the similar stabilities of lattice defects and cage-ball networks, demonstrates the rationality of lattice defects. Combining STM investigations and DFT calculations, this work could provide a useful approach to investigate the 2D crystallization mechanisms of supramolecular liquid crystals on surfaces.
引用
收藏
页码:8935 / 8942
页数:8
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