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See supporting text on Science Online.
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5
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4344702867
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note
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Others have also used vacuum filtration as the initial step to fabricate free-standing SWNT films (6). However, their transfer process involved cutting a rectangular hole in adhesive tape, laying this tape onto the nanotube layer on the membrane, and peeling up the tape to obtain the free-standing film within the hole in the tape. This gives comparatively little control over the film thickness and is not amenable to film deposition over large areas compatible with microelectronic processing.
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8
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4344644678
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Work over recent years has shown that this simple picture for NFET operation is by no means complete and ignores Schottky barriers that develop at the nanotube-metal contact junctions, which are also modulated by the gate fields (13). Nonetheless, carrier concentration modulation contributes to the effect and under some conditions dominates (14).
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14
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0042991275
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A. Javey, J. Guo, Q. Wang, M. Lundstrom, H. Dai, Nature 424, 654 (2003).
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Forro, L.5
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x dielectric layer.
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0042991275
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4344694218
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Modulation of the three principal SWNT absorption bands in a three-terminal electrochemical cell has been reported (20, 21). There, the effect was ascribed to nanotube Fermi level shifts associated with intercalated species generated by electrochemical redox reactions in the electrolyte. The SWNT film (produced by airbrushing) used in those experiments evidently did not have sufficient intrinsic conductivity to be used without a thin, transparent platinum electrode (20) or ITO electrode (21) onto which the nanotubes were sprayed. The ionic liquid in our experiments acts merely as a near-lying gate electrode undergoing no complicating redox reactions. It also yields substantially cleaner SWNT spectra over broader voltage and spectral ranges. The spectra we show are raw data.
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20
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0035926920
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S. Kazaoui, N. Minami, N. Matsuda, H. Kataura, Y. Achiba, Appl. Phys. Lett. 78, 3433 (2001).
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Kataura, H.4
Achiba, Y.5
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22
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4344629473
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Although the S1 band overlaps the 1.55-μm wavelength important in optical communications, the ionic liquid-gated device (or any electrolyte-gated device) is far too slow to be useful for modulation at the rates needed in communication devices. Because of the high viscosity of the ionic liquid, the time scale for electrostatic gate equilibration is on the order of minutes.
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4344564615
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Our all-solid-state device has similar spectral behavior with "gate" voltage; however, the magnitude of the modulation is much smaller (0.2% over ±6 V at the peak of S1) because electrostatic screening allows only the layer of nanotubes nearest the ITO counterelectrode to participate. Because gating is all electronic (as opposed to ionic), however, the response time is much faster than the ionic liquid device.
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4344581440
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With the spectrophotometer in a mode that records the transmittance at fixed wavelength as a function of time, we sat on the peak of the S1 absorption band while driving the O-NFET with a square wave potential. No systematic changes in the amplitude of the modulation were observed over multiple measurements totaling several hundred cycles. Only small changes (a few percent) in the average transmittance, both up and down, were seen-entirely consistent with spectrometer drift over the long time scale of these measurements.
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Four-probe measurements were performed with a Linear Research 700 resistance bridge using 2-mV excitation at 16 Hz.
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27
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4344559494
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Supported by the U.S. Army through Center for Materials in Sensors and Actuators grant DAAD19-001-0002 (J.R.R., D.B.T., A.F.H., A.G.R.), NSF grants DMR 0101856 (A.F.H.) and ECS-0210S74 (A.G.R.), and NSF-MTA-OTKA international grants 021, N31622 (D.B.T., K.K.), NSF-INT-9902050 (D.B.T., K.K.), and OTKA 034198 (K.K.).
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