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Molecular self-assembly |
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Self-assembled monolayers (SAM) are assemblies of organic molecules that form spontaneously on surfaces by adsorption and organize themselves into more or less distinct domains (head group, chain/backbone, and tail/end group).[1][2] In some cases, molecules that form the monolayer do not interact strongly with the substrate. This is the case for porphyrins on HOPG[3] and two-dimensional supramolecular networks[4] of PTCDA on gold[5]. In other cases, the head group has a strong affinity for the substrate and anchors the molecule.[6] Such an SAM consisting of a head group, chain (labeled "tail"), and functional end group is depicted in Figure 1. Common head groups include thiols, silanes, and phosphonates.
SAMs are created by the chemisorption of head groups onto a substrate from either the vapor or liquid phase[7][8] followed by a slower organization of "tail groups".[9] Initially, at small molecular density on the surface, adsorbate molecules form either a disordered mass of molecules or an ordered two-dimensional "lying down phase".[7] At higher molecular coverage, adsorbates can begin to form three-dimensional crystalline or semicrystalline structures on the substrate surface over a period of minutes to hours.[10] The head groups assemble on the substrate, while the tail groups assemble far from the substrate. Areas of close-packed molecules nucleate and grow until the surface of the substrate is covered in a single monolayer.
Adsorbate molecules adsorb readily because they lower the surface free-energy of the substrate[1] and are stable due to the strong chemisorption of the head groups. These bonds create monolayers that are more stable than the physisorbed bonds of Langmuir–Blodgett films.[11][12] For example, the trichlorosilane head group of an FDTS molecule reacts with a hydroxyl group on a substrate to form a very stable covalent bond [R-Si-O-substrate] with an energy of 452 kJ/mol.[citation needed] Thiol-metal bonds are on the order of 100 kJ/mol, making them fairly stable in a variety of temperatures, solvents, and potentials.[10] Monolayers pack tightly due to van der Waals interactions,[1][12] thereby reducing their own free energy.[1] The adsorption can be described by the Langmuir adsorption isotherm if lateral interactions are neglected. If they cannot be neglected, the adsorption is better described by the Frumkin isotherm.[10]
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