Molecular electronics

For quantum mechanical study of the electron distribution in a molecule, see stereoelectronics.

Molecular electronics, sometimes called moletronics, involves the study and application of molecular building blocks for the fabrication of electronic components. This includes both bulk applications of conductive polymers as well as single-molecule electronic components for nanotechnology.

An interdisciplinary pursuit, molecular electronics spans physics, chemistry, and materials science. The unifying feature is the use of molecular building blocks for the fabrication of electronic components. This includes both passive (e.g. resistive wires) and active components such as transistors and molecular-scale switches. Due to the prospect of size reduction in electronics offered by molecular-level control of properties, molecular electronics has aroused much excitement both in science fiction and among scientists. Molecular electronics provides means to extend Moore's Law beyond the foreseen limits of small-scale conventional silicon integrated circuits.

Molecular electronics is split into two related but separate subdisciplines: molecular materials for electronics utilizes the properties of the molecules to affect the bulk properties of a material, while molecular scale electronics focuses on single-molecule applications.^[1][2]

Molecular scale electronics

Main article: Molecular scale electronics

Part of a series of articles on Nanoelectronics Single-molecule electronics Molecular scale electronics Molecular logic gate Molecular wires Solid state nanoelectronics Nanocircuitry Nanowires Nanolithography NEMS Nanosensor Related approaches Nanoionics Nanophotonics Nanomechanics See also Nanotechnology v · d · e

Molecular scale electronics, also called single molecule electronics, is a branch of nanotechnology that uses single molecules, or nanoscale collections of single molecules, as electronic components. Because single molecules constitute the smallest stable structures imaginable this miniaturization is the ultimate goal for shrinking electrical circuits.

Conventional electronics have traditionally been made from bulk materials. With the bulk approach having inherent limitations in addition to becoming increasingly demanding and expensive, the idea was born that the components could instead be built up atom for atom in a chemistry lab (bottom up) as opposed to carving them out of bulk material (top down). In single molecule electronics, the bulk material is replaced by single molecules. That is, instead of creating structures by removing or applying material after a pattern scaffold, the atoms are put together in a chemistry lab. The molecules utilized have properties that resemble traditional electronic components such as a wire, transistor or rectifier.

Single molecule electronics is an emerging field, and entire electronic circuits consisting exclusively of molecular sized compounds are still very far from being realized. However, the continuous demand for more computing power together with the inherent limitations of the present day lithographic methods make the transition seem unavoidable. Currently, the focus is on discovering molecules with interesting properties and on finding ways to obtaining reliable and reproducible contacts between the molecular components and the bulk material of the electrodes.

Molecular electronics operates in the quantum realm of distances less than 100 nanometers. The miniaturization down to single molecules brings the scale down to a regime where quantum effects are important. As opposed to the case in conventional electronic components, where electrons can be filled in or drawn out more or less like a continuous flow of charge, the transfer of a single electron alters the system significantly. The significant amount of energy due to charging has to be taken into account when making calculations about the electronic properties of the setup and is highly sensitive to distances to conducting surfaces nearby.

Graphical representation of a rotaxane, useful as a molecular switch.

One of the biggest problems with measuring on single molecules is to establish reproducible electrical contact with only one molecule and doing so without shortcutting the electrodes. Because the current photolithographic technology is unable to produce electrode gaps small enough to contact both ends of the molecules tested (in the order of nanometers) alternative strategies are put into use. These include molecular-sized gaps called break junctions, in which a thin electrode is stretched until it breaks. Another method is to use the tip of a scanning tunneling microscope (STM) to contact molecules adhered at the other end to a metal substrate.^[3] Another popular way to anchor molecules to the electrodes is to make use of sulfur's high affinity to gold; though useful, the anchoring is non-specific and thus anchors the molecules randomly to all gold surfaces, and the contact resistance is highly dependent on the precise atomic geometry around the site of anchoring and thereby inherently compromises the reproducibility of the connection. To circumvent the latter issue, experiments has shown that fullerenes could be a good candidate for use instead of sulfur because of the large conjugated π-system that can electrically contact many more atoms at once than a single atom of sulfur.^[4]

One of the biggest hindrances for single molecule electronics to be commercially exploited is the lack of techniques to connect a molecular sized circuit to bulk electrodes in a way that gives reproducible results. Also problematic is the fact that some measurements on single molecules are carried out in cryogenic temperatures (close to absolute zero) which is very energy consuming.

Molecular materials for electronics

Main articles: Conductive polymer and Organic electronics

Chemical structures of some conductive polymers. From top left clockwise: polyacetylene; polyphenylene vinylene; polypyrrole (X = NH) and polythiophene (X = S); and polyaniline (X = NH/N) and polyphenylene sulfide (X = S).

Voltage-controlled switch, a molecular electronic device from 1974. From Smithsonian Chip collection.^[5]

Molecular materials for electronics is a term used to refer to bulk applications of conductive polymers.^[2] Conductive polymers or, more precisely, intrinsically conducting polymers (ICPs) are organic polymers that conduct electricity in their bulk state.^[6] Such compounds may have metallic conductivity or can be semiconductors. The biggest advantage of conductive polymers is their processability, mainly by dispersion. Conductive polymers are not plastics, i.e., they are not thermoformable, but they are organic polymers, like (insulating) polymers. They can offer high electrical conductivity but do not show mechanical properties as other commercially used polymers do. The electrical properties can be fine-tuned using the methods of organic synthesis ^[7] and by advanced dispersion techniques.^[8]

The linear-backbone "polymer blacks" (polyacetylene, polypyrrole, and polyaniline) and their copolymers are the main class of conductive polymers. Historically, these are known as melanins. PPV and its soluble derivatives have similarly emerged as the prototypical electroluminescent semiconducting polymers. Today, poly(3-alkylthiophenes) are the archetypical materials for solar cells and transistors.^[7]

Conducting polymers have backbones of contiguous sp² hybridized carbon centers. One valence electron on each center resides in a p_z orbital, which is orthogonal to the other three sigma-bonds. The electrons in these delocalized orbitals have high mobility when the material is "doped" by oxidation, which removes some of these delocalized electrons. Thus the conjugated p-orbitals form a one-dimensional electronic band, and the electrons within this band become mobile when it is partially emptied. Despite intensive research, the relationship between morphology, chain structure and conductivity is poorly understood yet.^[9]

Due to their poor processability, conductive polymers enjoy few large-scale applications . They have some promise in antistatic materials^[7] and they have been incorporated into commercial displays and batteries, but there have had limitations due to the manufacturing costs, material inconsistencies, toxicity, poor solubility in solvents, and inability to directly melt process. Nevertheless, conducting polymers are rapidly gaining attraction in new applications with increasingly processable materials with better electrical and physical properties and lower costs. With the availability of stable and reproducible dispersions, PEDOT and polyaniline have gained some large scale applications. While PEDOT (poly(3,4-ethylenedioxythiophene)) is mainly used in antistatic applications and as a transparent conductive layer in form of PEDOT:PSS dispersions (PSS=polystyrene sulfonic acid), polyaniline is widely used for printed circuit board manufacturing – in the final finish, for protecting copper from corrosion and preventing its solderability.^[8] The new nanostructured forms of conducting polymers particularly, provide fresh air to this field with their higher surface area and better dispersability.

See also

• Software for molecular modeling
• Molecular conductance
• Molecular wires
• Organic Semiconductors
• Single-molecule magnet
• Spin transition

References

1. ^ Petty, M.C.; Bryce, M.R. & Bloor, D. (1995). Introduction to Molecular Electronics. New York: Oxford University Press. pp. 1–25. ISBN 0195211561. 
2. ^ ^{a b} Tour, James M.; et al. (1998). "Recent advances in molecular scale electronics". Annals of the New York Academy of Sciences 852: 197–204. doi:10.1111/j.1749-6632.1998.tb09873.x. 
3. ^ Gimzewski, J.K.; Joachim, C. (1999). "Nanoscale science of single molecules using local probes". Science 283 (5408): 1683–1688. doi:10.1126/science.283.5408.1683. PMID 10073926. 
4. ^ Sørensen, J.K.. (2006). “Synthesis of new components, functionalized with (60)fullerene, for molecular electronics”. 4th Annual meeting - CONT 2006, University of Copenhagen.
5. ^ "Organic Semiconductor (I/O), 1973 a melanin (polyacetylenes) bistable switch". National Museum of American History. http://smithsonianchips.si.edu/proctor/. 
6. ^ György Inzelt (2008). Conducting Polymers: A New Era in Electrochemistry. Springer. pp. 265–269. doi:10.1007/978-3-540-75930-0_8. ISBN 978-3-540-75930-0. 
7. ^ ^{a b c} Herbert Naarmann “Polymers, Electrically Conducting” in Ullmann's Encyclopedia of Industrial Chemistry 2002 Wiley-VCH, Weinheim. doi:10.1002/14356007.a21_429
8. ^ ^{a b} Handbook of Nanostructured Materials and Nanotechnology; Nalwa, H.S., Ed.; Academic Press: New York, NY, USA, 2000; Volume 5, pp. 501–575.
9. ^ Skotheim, T., Elsenbaumer, R., Reynolds, J., Eds.; Handbook of Conducting Polymers, 2nd ed.; Marcel Dekker, Inc.: New York, NY, USA, 1998

External links

• Online lecture on Molecular Electronics and the Bottom-up View of Electronic Conduction by S. Datta
• Online lecture on Molecular Electronics Pathway for Molecular Memory Devices by Ranganathan Shashidhar
• organicsemiconductors.com