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Capacitance voltage curves

Fig. 13. (a) High frequency (1MHz) capacitance-voltage curves for Al/octadecyl/... [Pg.316]

Si(lll) structures formed on n- and p-doped substrates showing the typical accumulation (acc), depletion (dep) and inversion (inv) regimes, (b) Capacitance-voltage curves (1MHz) in the dark (circles) and under white illumination (squares) for a structure formed on a p-doped substrate. The increase in capacitance under illumination in positive bias is characteristic of the formation of an inversion layer. Reprinted from [25]. [Pg.316]

Figure 16.4 Dynamic capacitance-voltage curves of an organic MIS capacitor measured at 1 Hz for different gate-bulk voltage (V(3b) sweep directions at different temperatures. The organic semiconductor is a 48 nm thick poly(3-octylthiophene)... Figure 16.4 Dynamic capacitance-voltage curves of an organic MIS capacitor measured at 1 Hz for different gate-bulk voltage (V(3b) sweep directions at different temperatures. The organic semiconductor is a 48 nm thick poly(3-octylthiophene)...
Su et al. have recently employed QELS to study the potential-induced assembly of Au nanoparticles at the water/DCE interface [31]. The water-soluble Au nanoparticles featured an average diameter of 1.5 0.4 nm and were capped by mercaptosuccinic acid (MSA). The capacitance-voltage curves in Fig. 4.12a show an increase in the differential capacitance (Qi) at negative with increasing concentration of the nanoparticles in the aqueous phase. As illustrated in... [Pg.140]

Figure 27.17. Capacitance-voltage curves of CC SiC-600C at the potential sweep rate of lOmV/s (1) IL (2) 50% H2SO4 (3) 30% KOH. Figure 27.17. Capacitance-voltage curves of CC SiC-600C at the potential sweep rate of lOmV/s (1) IL (2) 50% H2SO4 (3) 30% KOH.
Figure 27.18. Capacitance-voltage curves for CCs in 50% H2SO4 at 20 mV/s (1) TiC-600C (2) SiC-600C (3) TiC-lOOOC (4) SiC-1500C. Figure 27.18. Capacitance-voltage curves for CCs in 50% H2SO4 at 20 mV/s (1) TiC-600C (2) SiC-600C (3) TiC-lOOOC (4) SiC-1500C.
A similar situation exists in an insulated gate structure the difference between the WF of the semiconductor and the gate metal adjacent to the insulator causes a deficiency or an excess of electrons in the semiconductor at its interface with the insulator. In the semiconductor/insulator/metal diodes the amount of the excess charge at the semiconductor plate is determined from the capacitance-voltage curves while in a field-effect transistor the excess charge at the semiconductor/insulator interface is related to the magnitude of the drain-to-source current [13]. In either case the observed WF difference contains the contribution from both the bulk and from the surface (or interface). [Pg.323]

If there is a pretilt, i.e., the director tilt angle at the walls is nonzero, the changes near Vq are gradual. We then define as the intersection of the extrapolated linear portion of the capacitance/voltage curve with the horizontal C=C(V 0) curve (see Fig. 1). We assume the surface coupling to be strong, so that the tilt angle at the surface is constant. [Pg.97]

A small pretilt at the walls is usually introduced in order to suppress areas of reverse tilt and twist. The value of used in the calculation was obtained from the capacitance/voltage curves. The pretilt appears to lower Nj ax (see Fig. 4) and should therefore be kept to a minimum d=10 ym, X= 0.6353 ym, no=1.549, ne 1.764. [Pg.101]

In addition, results by Armstrong and Mason (23) show similar shapes of capacitance-voltage curves for RbAg I Pt at 22° and 95°C and for Agl Pt at 200°. It seemed worthwhile, then, to attempt to develop a simple theoretical "adsorption capacitance" model and compare it with available data. [Pg.129]

To compare the theory with experimental results, we see if the capacitance expression of Eq. 14 can be fitted to the central region of Fig. 4 with a reasonable value of AzJ. In Fig. 10, the 417 experimental AgBr Pt capacitance-voltage curve of Fig. 4 is replotted on a linear scale. On the same graph, the theoretical C(e) curve is plotted, with Az chosen such that the capacitance at e = 0 equals the experimental capacitance at the midpoint... [Pg.135]

Fig. 10 Comparison of experimental (Fig. 4) and theoretical (Eq. 14) capacitance-voltage curves for AgBrjPt interface at 417 C. Solid curve is experimental solid with dots is theoretical. Dashed curves are theory-experiment difference curves. Az in Eq. 14 was chosen to match experimental capacitance at maximum ... Fig. 10 Comparison of experimental (Fig. 4) and theoretical (Eq. 14) capacitance-voltage curves for AgBrjPt interface at 417 C. Solid curve is experimental solid with dots is theoretical. Dashed curves are theory-experiment difference curves. Az in Eq. 14 was chosen to match experimental capacitance at maximum ...
Fig. 12 Capacitance - voltage curves for p-Si in acetonitrile as a function of frequency and light intensity showing behavior expected for MOS devices in inversion. Fig. 12 Capacitance - voltage curves for p-Si in acetonitrile as a function of frequency and light intensity showing behavior expected for MOS devices in inversion.

See other pages where Capacitance voltage curves is mentioned: [Pg.229]    [Pg.257]    [Pg.344]    [Pg.325]    [Pg.206]    [Pg.191]    [Pg.105]    [Pg.206]    [Pg.176]    [Pg.288]    [Pg.292]    [Pg.295]    [Pg.103]    [Pg.782]   
See also in sourсe #XX -- [ Pg.209 ]

See also in sourсe #XX -- [ Pg.33 , Pg.73 ]




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Voltage curves

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