Abstract

Self-assembly—the autonomous organization of components into patterns and structures1—is a promising technology for the mass production of organic electronics. Making integrated circuits using a bottom-up approach involving self-assembling molecules was proposed2 in the 1970s. The basic building block of such an integrated circuit is the self-assembled-monolayer field-effect transistor (SAMFET), where the semiconductor is a monolayer spontaneously formed on the gate dielectric. In the SAMFETs fabricated so far, current modulation has only been observed in submicrometre channels3,4,5, the lack of efficient charge transport in longer channels being due to defects and the limited intermolecular π–π coupling between the molecules in the self-assembled monolayers. Low field-effect carrier mobility, low yield and poor reproducibility have prohibited the realization of bottom-up integrated circuits. Here we demonstrate SAMFETs with long-range intermolecular π–π coupling in the monolayer. We achieve dense packing by using liquid-crystalline molecules consisting of a π-conjugated mesogenic core separated by a long aliphatic chain from a monofunctionalized anchor group. The resulting SAMFETs exhibit a bulk-like carrier mobility, large current modulation and high reproducibility. As a first step towards functional circuits, we combine the SAMFETs into logic gates as inverters; the small parameter spread then allows us to combine the inverters into ring oscillators. We demonstrate real logic functionality by constructing a 15-bit code generator in which hundreds of SAMFETs are addressed simultaneously. Bridging the gap between discrete monolayer transistors and functional self-assembled integrated circuits puts bottom-up electronics in a new perspective.

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Acknowledgements

We acknowledge H. Nulens and C. van der Marel for the AFM and X-ray photoemission spectroscopy measurements, M. Kaiser for the FIB-TEM analysis, A. P. Pleshkova for the mass spectrometry analysis, F. Zontone for technical assistance and N. Willard for discussions. We acknowledge financial support from the Dutch Polymer Institute, project 516, the EU project NAIMO (NMP4-CT-2004-500355), the Dutch Technology Foundation STW, the Austrian Science Foundation and H. C. Starck GmbH. We thank the European Synchrotron Research Facility for the use of the beamline ID10B.

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Affiliations

  1. Molecular Electronics, Zernike Institute for Advanced Materials, University of Groningen, Nijenborgh 4, 9747 AG Groningen, The Netherlands

    • Edsger C. P. Smits
    • , Bert de Boer
    • , Paul W. M. Blom
    •  & Dago M. de Leeuw
  2. Philips Research Laboratories, High Tech Campus 4, 5656 AE Eindhoven, The Netherlands

    • Edsger C. P. Smits
    • , Simon G. J. Mathijssen
    • , Paul A. van Hal
    • , Sepas Setayesh
    • , Thomas C. T. Geuns
    • , Kees A. H. A. Mutsaers
    • , Harry J. Wondergem
    •  & Dago M. de Leeuw
  3. Dutch Polymer Institute, PO Box 902, 5600 AX Eindhoven, The Netherlands

    • Edsger C. P. Smits
  4. Department of Applied Physics,

    • Simon G. J. Mathijssen
    •  & Martijn Kemerink
  5. Mixed-Signal Microelectronics Group, Department of Electrical Engineering, Eindhoven University of Technology, PO Box 513, 5600 MB Eindhoven, The Netherlands

    • Eugenio Cantatore
  6. Institute of Solid State Physics, Graz University of Technology, Petersgasse 16A, 8010 Graz, Austria

    • Oliver Werzer
    •  & Roland Resel
  7. H. C. Starck GmbH, Chemiepark Leverkusen, Building B202, 51368 Leverkusen, Germany

    • Stephan Kirchmeyer
  8. Enikolopov Institute of Synthetic Polymer Materials, Russian Academy of Sciences, Profsoyuznaya 70, 117393 Moscow, Russia

    • Aziz M. Muzafarov
    •  & Sergei A. Ponomarenko

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https://doi.org/10.1038/nature07320

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