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Two-dimensional polymer : ウィキペディア英語版
Two-dimensional polymer

A two-dimensional polymer (2DP) is a sheet-like monomolecular macromolecule consisting of laterally connected repeat units with end groups along all edges.〔J. Sakamoto, J. van Heijst, O. Lukin, A. D. Schlüter, ''Angew. Chem., Int. Ed.'' 2009, ''48'', 1030.〕〔''Rationally synthesized two-dimensional polymers'' John W. Colson, William R. Dichtel Nature Chemistry 5, 453–465 (2013) 〕 This recent definition of 2DP is based on Hermann Staudinger’s polymer concept from the 1920s.〔H. Staudinger, Ber. Dtsch. Chem. Ges. 1920, 53, 1073; H. Staudinger, J. Fritschi, ''Helv. Chim. Acta'' 1922, ''5'', 785.〕〔H. F. Mark, ''Naturwiss.'' 1980, ''67'', 477.; H. Ringsdorf, ''Angew. Chem., Int. Ed.'' 2004, ''43'', 1064.〕 According to this, covalent long chain molecules (“Makromoleküle”) do exist and are composed of a sequence of linearly connected repeat units and end groups at both termini.
Moving from one dimension to two offers access to surface
morphologies such as increased surface area, porous membranes, and possibly in-plane
pi orbital-conjugation for enhanced electronic properties. They are distinct
from other families of polymers because 2D polymers can be isolated as
multilayer crystals or as individual sheets.
The term
2D polymer has also been used more broadly to include linear polymerizations
performed at interfaces, layered non-covalent assemblies, or to irregularly
cross-linked polymers confined to surfaces or layered films. 2D
polymers can be organized based on these methods of linking (monomer
interaction): covalently linked monomers, coordination polymers and
supramolecular polymers.
Topologically, 2DPs may thus be understood as structures made up from regularly tessellated regular polygons (the repeat units). Figure 1 displays the key features of a linear and a 2DP according to this definition. For usage of the term “2D polymer” in a wider sense, see “History”.
== Covalently-Linked Polymers ==
There are several examples of covalently linked 2DPs which include the individual layers or sheets of graphite (called graphenes), MoS2, (BN)x and layered covalent organic frameworks. As required by the above definition, these sheets have a periodic internal structure.
i. Graphene: A
well-known example of a 2D polymer is graphene; whose optical, electronic and mechanical properties
have been studied in depth. Graphene has a honeycomb lattice of carbon
atoms that exhibit semiconducting properties. A potential repeat unit of graphene is a sp2-hybridized carbon atom. Individual sheets can in principle be obtained by exfoliation procedures, though in reality this is a non-trivial enterprise.
ii. MoS2: Molybdenumdisulfide can exist in two-dimensional,
single or layered polymers where each Mo(IV) center occupies a trigonal
prismatic coordination sphere.
iii. BN: Boron nitride polymers are
stable in its crystalline hexagonal form where it has a two-dimensional layered
structure similar to graphene. There are covalent bonds formed between boron
and nitrogen atoms, yet the layers are held together by weak van der Waals
interactions, in which the boron atoms are eclipsed over the nitrogen.
iv. Covalent Organic Frameworks
Two dimensional covalent organic frameworks
(COFs) are one type of microporous coordination polymer that can be fabricated
in the 2D plane. The
dimensionality and topology of the 2D COFs result from both the shape of the monomers
and the relative and dimensional orientations of their reactive groups. These materials contain
desirable properties in fields of materials chemistry including thermal
stability, tunable porosity, high specific surface area, and the low density of
organic material. By
careful selection of organic building units, long range π-orbital overlap parallel to the stacking direction of
certain organic frameworks can be achieved.〔
Many covalent
organic frameworks derive their topology from the directionality of the
covalent linkages, thus small changes in organic linkers can dramatically
affect their mechanical and electronic properties.〔 Even small changes in their
structure can induce dramatic changes in stacking behavior of molecular
semiconductors.
Porphyrins are an additional class of
conjugated, heterocyclic macrocycles. Control of monomer assembly through covalent assembly has also been
demonstrated using covalent interactions with porphyrins. Upon
thermal activation of porphyrin building blocks, covalent bonds form to create
a conductive polymer, a versatile route for bottom-up construction of
electronic circuits been demonstrated. (Figure 2)

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