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{{short description|Form of digital logic family in integrated circuits}}
[[File:Nmos depletion and.svg|right|thumb|A depletion-load
In [[integrated circuit]]s, '''depletion-load NMOS''' is a form of digital [[logic family]] that uses only a single power supply voltage, unlike earlier [[NMOS logic|NMOS]] (n-type [[metal-oxide semiconductor]]) logic families that needed more than one different power supply voltage. Although manufacturing these integrated circuits required additional processing steps, improved switching speed and the elimination of the extra power supply made this logic family the preferred choice for many [[microprocessor]]s and other logic elements.
[[Depletion and enhancement modes|Depletion-mode]] n-type [[MOSFET]]s as load transistors allow single voltage operation and achieve greater speed than possible with pure enhancement-load devices. This is partly because the depletion-mode MOSFETs can be a better [[current source]] approximation than the simpler enhancement-mode transistor can, especially when no extra voltage is available (one of the reasons early
The inclusion of depletion-mode
Although the [[CMOS]] process replaced most NMOS designs during the 1980s, some depletion-load
==History and background==
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In the late 1960s, [[bipolar junction transistor]]s were faster than (p-channel) MOS transistors then used and were more reliable, but they also consumed much more power, required more area, and demanded a more complicated manufacturing process. MOS ICs were considered interesting but inadequate for supplanting the fast bipolar circuits in anything but niche markets, such as low power applications. One of the reasons for the low speed was that MOS transistors had [[Gate (transistor)|gates]] made of [[aluminum]] which led to considerable [[parasitic capacitance]]s using the manufacturing processes of the time. The introduction of transistors with gates of [[polycrystalline silicon]] (that became the ''de facto'' standard from the mid-1970s to early 2000s) was an important first step in order to reduce this handicap. This new [[self-aligned gate|''self-aligned silicon-gate'']] transistor was introduced by [[Federico Faggin]] at [[Fairchild Semiconductor]] in early 1968; it was a refinement (and the first working implementation) of ideas and work by John C. Sarace, Tom Klein and [[Robert W. Bower]] (around 1966–67) for a transistor with lower parasitic capacitances that could be manufactured as part of an IC (and not only as a [[discrete component]]). This new type of pMOS transistor was 3–5 times as fast (per watt) as the aluminum-gate pMOS transistor, and it needed less area, had much lower leakage and higher reliability. The same year, Faggin also built the first IC using the new transistor type, the ''Fairchild 3708'' (8-bit [[analogue electronics|analog]] [[multiplexer]] with [[Binary decoder|decoder]]), which demonstrated a substantially improved performance over its metal-gate counterpart. In less than 10 years, the silicon gate MOS transistor replaced bipolar circuits as the main vehicle for complex digital ICs.
===
There are a couple of drawbacks associated with
Early work on
The production-ready
===Depletion-mode transistors===
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Early MOS logic had one transistor type, which is [[enhancement mode]] so that it can act as a logic switch. Since suitable resistors were hard to make, the logic gates used saturated loads; that is, to make the one type of transistor act as a load resistor, the transistor had to be turned always on by tying its gate to the power supply (the more negative rail for [[PMOS logic]], or the more positive rail for [[NMOS logic]]). Since the current in a device connected that way goes as the square of the voltage across the load, it provides poor pullup speed relative to its power consumption when pulled down. A resistor (with the current simply proportional to the voltage) would be better, and a current source (with the current fixed, independent of voltage) better yet. A [[depletion-mode]] device with gate tied to the opposite supply rail is a much better load than an enhancement-mode device, acting somewhere between a resistor and a current source.
The first depletion-load
Depletion-load
A large number of support and peripheral ICs were also implemented using (often static) depletion-load based circuitry. However,
there were never any standardized [[logic family|logic families]] in
===Intel HMOS===
Intel's own depletion-load NMOS process was known as '''HMOS''', for ''High density, short channel MOS''. The first version was introduced in late 1976 and first used for their [[static RAM]] products,<ref>{{cite journal |first1=A.M. |last1=Volk |first2=P.A. |last2=Stoll |first3=P. |last3=Metrovich |title=Recollections of Early Chip Development at Intel |journal=Intel Technology Journal |volume=5 |issue=Q1 |pages= |date=2001 |url=https://www.intel.com/content/dam/www/public/us/en/documents/research/2001-vol05-iss-1-intel-technology-journal.pdf}}</ref> it was soon being used for faster and/or less power hungry versions of the 8085, 8086, and other chips.
HMOS continued to be improved and went through four distinct generations. According to Intel, HMOS II (1979) provided twice the density and four times the speed/power product over other typical contemporary depletion-load
The original HMOS process, later referred to as HMOS I, had a channel length of 3 microns, which was reduced to 2 for the HMOS II, and 1.5 for HMOS III. By the time HMOS III was introduced in 1982, Intel had begun a switch to their [[CHMOS]] process, a [[CMOS]] process using design elements of the HMOS lines. One final version of the system was released, HMOS-IV. A significant advantage to the HMOS line was that each generation was deliberately designed to allow existing layouts to die-shrink with no major changes. Various techniques were introduced to ensure the systems worked as the layout changed.<ref>{{cite conference |conference=ISSCC 82 |date=1982 |title=HMOS III Technology}}</ref><ref>{{cite journal |first1=G.E. |last1=Atwood |first2=H. |last2=Dun |first3=J. |last3=Langston |first4=E. |last4=Hazani |first5=E.Y. |last5=So |first6=S. |last6=Sachdev |first7=K. |last7=Fuchs |title=HMOS III technology |journal=IEEE Journal of Solid-State Circuits |volume=17 |issue=5 |pages=810–5 |date=October 1982 |doi=10.1109/JSSC.1982.1051823 |url=}}</ref>
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===Further development===
In the mid-1980s, faster CMOS variants, using similar HMOS process technology, such as Intel's CHMOS I, II, III, IV, etc. started to supplant n-channel HMOS for applications such as the [[Intel 80386]] and certain [[microcontroller]]s. A few years later, in the late 1980s, [[BiCMOS]] was introduced for high-performance microprocessors as well as for high speed [[analog circuit]]s. Today, most digital circuits, including the ubiquitous [[7400 series]], are manufactured using various CMOS processes with a range of different topologies employed. This means that, in order to enhance speed and save die area (transistors and wiring), high speed CMOS designs often employ other elements than just the [[:wikt:complementary|complementary]] ''[[CMOS|static]]'' [[logic gate|gate]]s and the [[transmission gate]]s of typical slow low-power CMOS circuits (the ''only'' CMOS type during the 1960s and 1970s). These methods use significant amounts of [[dynamic logic (digital logic)|dynamic]] circuitry in order to construct the larger building blocks on the chip, such as latches, decoders, multiplexers, and so on, and evolved from the various dynamic methodologies developed for
==Compared to CMOS==
Compared to static CMOS, all variants of
== Evolution from preceding NMOS types ==
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== Static power consumption ==
[[File:Nmos enhancement saturated nand.svg|right|thumb|An
Depletion-load circuits consume less power than enhancement-load circuits at the same speed. In both cases the connection to ''1'' is always active, even when the connection to ''0'' is also active. This results in high static power consumption. The amount of waste depends on the strength, or physical size, of the pull-up. Both (enhancement-mode) saturated-load and depletion-mode pull-up transistors use greatest power when the output is stable at ''0'', so this loss is considerable. Because the strength of a depletion-mode transistor falls off less on the approach to ''1'', they may reach ''1'' faster despite starting slower, i.e. conducting less current at the beginning of the transition and at steady state.
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