In Situ CCVD Grown Graphene Transistors with Ultra-High On/Off-Current Ratio in Silicon CMOS Compatible Processing

We invented a novel method to fabricate graphene transistors on oxidized silicon wafers without the need to transfer graphene layers. By means of catalytic chemical vapor deposition (CCVD) the in-situ grown monolayer graphene field-effect transistors (MoLGFETs) and bilayer graphene transistors (BiLGFETs) are realized directly on oxidized silicon substrate, whereby the number of stacked graphene layers is determined by the selected CCVD process parameters. In-situ grown MoLGFETs exhibit the expected Dirac point together with the typical low on/off-current ratios between 16 (hole conduction) and 8 (electron conduction), respectively. In contrast, our BiLGFETs possess unipolar p-type device characteristics with an extremely high on/off-current ratio up to 1E7 exceeding previously reported values by several orders of magnitude. We explain the improved device characteristics by a combination of effects, in particular graphene-substrate interactions, hydrogen doping and Schottky-barrier effects at the source/drain contacts as well. Besides the excellent device characteristics, the complete CCVD fabrication process is silicon CMOS compatible. This will allow the usage of BiLGFETs for digital applications in a hybrid silicon CMOS environment.

[1]  M. Lemme Current Status of Graphene Transistors , 2009, 0911.4685.

[2]  Peng Chen,et al.  Effective doping of single-layer graphene from underlying SiO2 substrates , 2009 .

[3]  Rafael Reif,et al.  Electrochemical and Solid-Sates Letters , 1999 .

[4]  Yihong Wu,et al.  Raman Studies of Monolayer Graphene: The Substrate Effect , 2008 .

[5]  G. Duesberg,et al.  Reliable processing of graphene using metal etchmasks , 2011, Nanoscale research letters.

[6]  Takahashi,et al.  Angle-resolved ultraviolet photoelectron spectroscopy of the unoccupied band structure of graphite. , 1985, Physical review. B, Condensed matter.

[7]  Kwang S. Kim,et al.  Tuning the graphene work function by electric field effect. , 2009, Nano letters.

[8]  Martín Heidegger Physica A-E , 2013, Phänomenologische Interpretationen zu Aristoteles.

[9]  G. G. Stokes "J." , 1890, The New Yale Book of Quotations.

[10]  Max C. Lemme,et al.  Direct graphene growth on insulator , 2011, 1106.2070.

[11]  Yihong Wu,et al.  Hysteresis of electronic transport in graphene transistors. , 2010, ACS nano.

[12]  Yi Zhang,et al.  Synthesis, Transfer, and Devices of Single- and Few-Layer Graphene by Chemical Vapor Deposition , 2009, IEEE Transactions on Nanotechnology.

[13]  Andre K. Geim,et al.  Raman spectrum of graphene and graphene layers. , 2006, Physical review letters.

[14]  C. Berger,et al.  Epitaxial graphene , 2007, 0704.0285.

[15]  Andre K. Geim,et al.  The rise of graphene. , 2007, Nature materials.

[16]  U. Schwalke,et al.  Hysteresis of In Situ CCVD Grown Graphene Transistors , 2012 .

[17]  Roland Bennewitz,et al.  Local work function measurements of epitaxial graphene , 2008 .

[18]  D. R. Strachan,et al.  Surface potentials and layer charge distributions in few-layer graphene films. , 2008, Nano letters.

[19]  J. Brink,et al.  Doping graphene with metal contacts. , 2008, Physical review letters.

[20]  Yoshio Watanabe,et al.  Dependence of electronic properties of epitaxial few-layer graphene on the number of layers investigated by photoelectron emission microscopy , 2009 .

[21]  Fu-Rong Chen,et al.  Direct formation of wafer scale graphene thin layers on insulating substrates by chemical vapor deposition. , 2011, Nano letters.

[22]  Graphene-on-Sapphire and Graphene-on-Glass: Raman Spectroscopy Study , 2007, 0710.2369.