Self-assembled monolayers (SAMs) of organic molecules generally modify the surface properties when covalently linked to substrates. In organic electronics, SAMs are used to fine-tune the work functions of inorganic electrodes, thereby minimizing the energy barriers for injection or extraction of charge carriers into or out of an active organic layer; a detailed understanding of the interface energetics on an atomistic scale is required to design improved interfaces. In the field of molecular electronics, the SAM itself (or, in some cases, one or a few molecules) carries the entire device functionality; the interface then essentially becomes the device and the alignment of the molecular energy levels with those of the electrodes defines the overall charge-transport characteristics. This Account provides a review of recent theoretical studies of the interface energetics for SAMs of π-conjugated molecules covalently linked to noble metal surfaces. After a brief description of the electrostatics of dipole layers at metal/molecule interfaces, the results of density functional theory calculations are discussed for SAMs of representative conjugated thiols on Au(111). Particular emphasis is placed on the modification of the work function of the clean metal surface upon SAM formation, the alignment of the energy levels within the SAM with the metal Fermi level, and the connection between these two quantities. To simplify the discussion, we partition the description of the metal/SAM system into two parts by considering first an isolated free-standing layer of molecules and then the system obtained after molecule-metal bond formation. From an electrostatic standpoint, both the isolated monolayer and the metal-molecule bonds can be cast in the form of dipole layers, which lead to steps in the electrostatic potential energy at the interface. While the step due to the isolated molecular layer impacts only the work function of the SAM-covered surface, the step arising from the bond formation influences both the work function and the alignment of the electronic levels in the SAM with respect to the metal Fermi energy. Interestingly, headgroup substitutions at the far ends of the molecules forming the SAM are electrostatically decoupled from the metal-thiol interface in densely packed SAMs; as a result, the nature of these substituents and the binding chemistry between the metal and the molecules are two largely unrelated handles with which to independently tune the work function and the level alignment. The establishment of a comprehensive atomistic picture regarding the impact of the individual components of a SAM on the interface energetics at metal/organic junctions paves the way for clear guidelines to design improved functional interfaces in organic and molecular electronics.

The energetics at the interfaces between metal and monolayers of covalently bound organic molecules is studied theoretically. Despite the molecules under consideration displaying very different frontier orbital energies, the highest occupied molecular levels are found to be pinned at a constant energy offset with respect to the metal Fermi level. In contrast, the molecular properties strongly impact the metal work function. These interfacial phenomena are rationalized in terms of charge fluctuations and electrostatics at the atomic length scale as determined by first-principles calculations.

Self-assembled monolayers (SAMs) of organic molecules provide an important tool to tune the work function of electrodes in plastic electronics and significantly improve device performance. Also, the energetic alignment of the frontier molecular orbitals in the SAM with the Fermi energy of a metal electrode dominates charge transport in single-molecule devices. On the basis of first-principles calculations on SAMs of pi-conjugated molecules on noble metals, we provide a detailed description of the mechanisms that give rise to and intrinsically link these interfacial phenomena at the atomic level. The docking chemistry on the metal side of the SAM determines the level alignment, while chemical modifications on the far side provide an additional, independent handle to modify the substrate work function; both aspects can be tuned over several eV. The comprehensive picture established in this work provides valuable guidelines for controlling charge-carrier injection in organic electronics and current-voltage characteristics in single-molecule devices.

Interface energetics are of fundamental importance in organic and molecular electronics. By combining complementary experimental techniques and first-principles calculations, we resolve the complex interplay among several interfacial phenomena that collectively determine the electronic structure of the strong electron acceptor tetrafluoro-tetracyanoquinodimethane chemisorbed on copper. The combination of adsorption-induced geometric distortion of the molecules, metal-to-molecule charge transfer, and molecule-to-metal back transfer leads to a net increase of the metal work function.

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Van der Waals (vdW) interactions play a prominent role in the structure and function of organic/organic and organic/inorganic interfaces. Their accurate determination from first principles, however, is a notoriously difficult task. Recently, a surge of interest in modeling vdW interactions has led to promising theoretical developments. This article reviews the state-of-the-art of describing vdW interactions by density-functional theory with respect to accuracy and practicability. The performance of the different methods is demonstrated for simple systems, such as rare-gas dimers and small organic molecules. The nature of binding at organic/inorganic interfaces is then exemplified for the perylene-3,4,9,10-tetracarboxylic-3,4,9,10-dianhydride (PTCDA) molecule at surfaces of coinage metals. This fundamental system is the best-characterized organic molecule/metal interface in experiment and theory. We emphasize the crucial importance of a balanced description of both geometry and electronic structure in order to understand and model the properties of such systems. Finally, the relevance of vdW interactions to the function of actual devices based on interfaces is discussed.

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