51
|
Iritani K, Ikeda M, Yang A, Tahara K, Hirose K, Moore JS, Tobe Y. Hexagonal Molecular Tiling by Hexagonal Macrocycles at the Liquid/Solid Interface: Structural Effects on Packing Geometry. LANGMUIR : THE ACS JOURNAL OF SURFACES AND COLLOIDS 2017; 33:12453-12462. [PMID: 28968503 DOI: 10.1021/acs.langmuir.7b03007] [Citation(s) in RCA: 13] [Impact Index Per Article: 1.6] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/07/2023]
Abstract
We present here hexagonal tiling using hexagonal phenylene-ethynylene and phenylene-butadiynylene macrocycles attached by alkyl ester groups, PEM-C6 and PBM-C8, respectively, or triethylene glycol ester groups, PEM-TEG and PBM-TEG, respectively, at each vertex of the macrocyclic periphery at the liquid/solid interface. In this study, we focused on the effects of macrocyclic core size and the chemical properties of side chains attached to macrocyclic cores as well as solute concentrations on the hexagonal geometry of self-assembled monolayers. STM observations at the 1,2,4-trichrolobenzene/graphite interface revealed that PEM-C6 formed a honeycomb structure by van der Waals interactions between the interdigitated alkyl chains. However, upon increasing solute concentration, it changed to more dense hexagonal structure (tentatively called loose hexagonal structure I). In contrast, PBM-C8 formed loose hexagonal structure II of a slightly different packing mode at low concentration, while at high concentration it formed a high-density hexagonal structure in which alkyl chains are not adsorbed on the surface (dense hexagonal structure). In the dense hexagonal structure, macrocyclic cores are linked by hydrogen bonds between the ester carbonyl oxygen and the aromatic hydrogen atoms of the neighboring macrocycles. The packing geometries of loose hexagonal structures of PEM-C6 and PBM-C8 are different due to the different distance between the attachment of the alkyl ester groups which are located in confined space. On the other hand, PEM-TEG and PBM-TEG formed dense hexagonal structures, similar to PBM-C8 at high concentration, with their TEG units not adsorbed on the surface.
Collapse
Affiliation(s)
- Kohei Iritani
- Division of Frontier Materials Science, Graduate School of Engineering Science, Osaka University , Toyonaka, Osaka 560-8531, Japan
| | - Motoki Ikeda
- Division of Frontier Materials Science, Graduate School of Engineering Science, Osaka University , Toyonaka, Osaka 560-8531, Japan
| | - Anna Yang
- Department of Chemistry and Beckman Institute for Advanced Science and Technology, University of Illinois at Urbana-Champaign , Urbana, Illinois 61801, United States
| | - Kazukuni Tahara
- Division of Frontier Materials Science, Graduate School of Engineering Science, Osaka University , Toyonaka, Osaka 560-8531, Japan
- Department of Applied Chemistry, School of Science and Technology, Meiji University , Kawasaki, Kanagawa 214-8571, Japan
| | - Keiji Hirose
- Division of Frontier Materials Science, Graduate School of Engineering Science, Osaka University , Toyonaka, Osaka 560-8531, Japan
| | - Jeffrey S Moore
- Department of Chemistry and Beckman Institute for Advanced Science and Technology, University of Illinois at Urbana-Champaign , Urbana, Illinois 61801, United States
| | - Yoshito Tobe
- Division of Frontier Materials Science, Graduate School of Engineering Science, Osaka University , Toyonaka, Osaka 560-8531, Japan
- The Institute of Scientific and Industrial Research, Osaka University , 8-1, Mihogaoka, Ibaraki Osaka 567-0047, Japan
| |
Collapse
|
52
|
MacLeod JM, Lipton-Duffin J, Fu C, Taerum T, Perepichka DF, Rosei F. A 2D Substitutional Solid Solution through Hydrogen Bonding of Molecular Building Blocks. ACS NANO 2017; 11:8901-8909. [PMID: 28806527 DOI: 10.1021/acsnano.7b03172] [Citation(s) in RCA: 19] [Impact Index Per Article: 2.4] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/07/2023]
Abstract
Two-dimensional (2D) molecular self-assembly allows for the formation of well-defined supramolecular layers with tailored geometrical, compositional, and chemical properties. To date, random intermixing and entropic effects in these systems have largely been associated with crystalline disorder and glassy phases. Here we describe a 2D crystalline self-assembled molecular system that exhibits random incorporation of substitutional molecules. The lattice is formed from a mixture of trimesic acid (TMA) and terthienobenzenetricarboxylic acid (TTBTA), C3-symmetric hydrogen-bonding units of very different sizes (0.79 and 1.16 nm, respectively), at the solution-highly oriented pyrolitic graphite (HOPG) interface. Remarkably, the TTBTA substitutes into the TMA lattice at a fixed stoichiometry near 12%. The resulting lattice constant is consistent with Vegard's law prediction for an alloy with a composition TMA0.88TTBTA0.12, and the substrate orientation of the lattice is defined by an epitaxial relation with the HOPG substrate. The Gibbs free energy for the TMA/TTBTA lattice was elucidated by considering the entropy of intermixing, via Monte Carlo simulations of multiplicity of the substitutional lattices, and the enthalpy of intermixing, via density functional theory calculations. The latter show that both the bond enthalpy of the H-bonded lattice and the adsorption enthalpy of the molecule/substrate interactions play important roles. This work provides insight into the manifestation of entropy in a molecular crystal constrained by both epitaxy and intermolecular interactions and demonstrates that a randomly intermixed yet crystalline 2D solid can be formed through hydrogen bonding of molecular building blocks of very different size.
Collapse
Affiliation(s)
- Jennifer M MacLeod
- Institut National de la Recherche Scientifique, Centre Énergie, Matériaux, Télécommunications , 1650 Lionel Boulet Boulevard, Varennes, QC, Canada J3X 1S2
| | - Josh Lipton-Duffin
- Institut National de la Recherche Scientifique, Centre Énergie, Matériaux, Télécommunications , 1650 Lionel Boulet Boulevard, Varennes, QC, Canada J3X 1S2
| | - Chaoying Fu
- Department of Chemistry, McGill University , 801 Sherbrooke Street W., Montreal, QC, Canada H3A 0B8
| | - Tyler Taerum
- Department of Chemistry, McGill University , 801 Sherbrooke Street W., Montreal, QC, Canada H3A 0B8
| | - Dmitrii F Perepichka
- Department of Chemistry, McGill University , 801 Sherbrooke Street W., Montreal, QC, Canada H3A 0B8
| | - Federico Rosei
- Institut National de la Recherche Scientifique, Centre Énergie, Matériaux, Télécommunications , 1650 Lionel Boulet Boulevard, Varennes, QC, Canada J3X 1S2
- Institute of Fundamental and Frontier Science, University of Electronic Science and Technology of China , Chengdu 610054, People's Republic of China
| |
Collapse
|
53
|
Cometto F, Frank K, Stel B, Arisnabarreta N, Kern K, Lingenfelder M. The STM bias voltage-dependent polymorphism of a binary supramolecular network. Chem Commun (Camb) 2017; 53:11430-11432. [DOI: 10.1039/c7cc06597c] [Citation(s) in RCA: 16] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/16/2023]
Abstract
We control complex multicomponent switches by tuning the local electric field at the liquid/solid interface.
Collapse
Affiliation(s)
- F. Cometto
- Max Planck-EPFL Laboratory for Molecular Nanoscience, and Institut de Physique
- École Polytechnique Fédérale de Lausanne
- CH 1015 Lausanne
- Switzerland
- Departamento de Fisicoquímica
| | - K. Frank
- Max Planck-EPFL Laboratory for Molecular Nanoscience, and Institut de Physique
- École Polytechnique Fédérale de Lausanne
- CH 1015 Lausanne
- Switzerland
| | - B. Stel
- Max Planck-EPFL Laboratory for Molecular Nanoscience, and Institut de Physique
- École Polytechnique Fédérale de Lausanne
- CH 1015 Lausanne
- Switzerland
| | - N. Arisnabarreta
- Departamento de Fisicoquímica
- Instituto de Investigaciones en Fisicoquímica de Córdoba (INFIQC)
- Facultad de Ciencias Químicas
- Universidad Nacional de Córdoba
- Córdoba
| | - K. Kern
- Max Planck-EPFL Laboratory for Molecular Nanoscience, and Institut de Physique
- École Polytechnique Fédérale de Lausanne
- CH 1015 Lausanne
- Switzerland
- Max-Planck-Institut für Festkörperforschung
| | - M. Lingenfelder
- Max Planck-EPFL Laboratory for Molecular Nanoscience, and Institut de Physique
- École Polytechnique Fédérale de Lausanne
- CH 1015 Lausanne
- Switzerland
| |
Collapse
|