By Wai-Kai Chen
That includes countless numbers of illustrations and references, this quantity within the 3rd version of the Circuits and Filters instruction manual, presents the most recent details on analog and VLSI circuits, omitting wide idea and proofs in desire of diverse examples all through every one chapter.
The first a part of the textual content specializes in analog built-in circuits, featuring up to date wisdom on monolithic equipment versions, analog circuit cells, excessive functionality analog circuits, RF conversation circuits, and PLL circuits.
In the second one half the ebook, famous individuals provide the most recent findings on VLSI circuits, together with electronic structures, info converters, and systolic arrays.
Read or Download Analog and VLSI Circuits, 3rd Edition (The Circuits and Filters Handbook) PDF
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Additional resources for Analog and VLSI Circuits, 3rd Edition (The Circuits and Filters Handbook)
Example text
96 that the effect of an increasing bulk-to-source reverse bias (Vbs < 0) is to increase the threshold voltage above its zero bias value, Vho, as a square root function of Vbs. 90 projects as directly dependent on the gate oxide thickness, Tox. One reason for the current penchant toward progressively decreased oxide thickness is the minimization of threshold voltage modulation, which is generally an undesirable effect in MOSFETs deployed in analog network applications. 17 stipulate the dependence of the static drain current, Id, on the static values of the gate–source voltage, Vgs, the drain–source voltage, Vds, and the bulk–source voltage, Vbs, which is invariably a nonpositive voltage.
21a. (b) The electric field intensity as a function of bulk substrate depth measured with respect to the interfacial surface, corresponding to the charge profile in (a). (c) The potential implied by the electric field plot in (b). In view of the fact that E(Wd) is zero in the undepleted, charge neutral substrate region corresponding to W ! 56 for the Debye length is invoked. 24b. 24c. 84 suggests that the surface potential, w(0), which is effectively the net voltage dropped across the depleted region of the bulk substrate, is 2 qNA Wd2 1 Wd Eo Wd , ¼ VT 2es Db 2 2 w(0) D¼ wo ¼ (1:85) Since the interface potential, wo, and hence the depletion depth, Wd, is controlled externally by the applied gate-to-bulk voltage, Vgb, it is of interest to determine wo as an explicit function of Vgb.
45)(1010) atoms=cm3 is the intrinsic carrier concentration of silicon at T ¼ 278C. 19 is established in response to an applied gate–bulk voltage, Vgb, or an applied gate– source voltage, Vgs. 52 of Qo(0) ¼ 0. 52 is premised on Poisson’s equation and the Boltzmann carrier relationship, p(0) ¼ NA eÀwo =VT , (1:58) where p(0) signifies the hole concentration at the surface if complete ionization of substrate dopant atoms is tacitly presumed. 55 has been exploited. 52 is a positive real number. 53 forces Qo(wo) > 0 for wo < 0 and Qo(wo) < 0 for wo > 0.