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(Researchers made a major breakthrough in smart printed electronics. ) 2D transistors make displays so cheap that they would be literally disposable. Then wine labels could show when the contents is at the optimal drinking temperature. Researchers from AMBER and TU Delft, Netherlands have fabricated printed transistors consisting entirely of 2-dimensional nanomaterials for the first time. These 2D materials combine exciting electronic properties with the potential for low-cost production. This breakthrough could unlock the potential for applications such as food packaging that displays a digital countdown to warn you of spoiling, wine labels that alert you when your white wine is at its optimum temperature, or even a window pane that shows the day’s forecast. This discovery opens the path for industry, such as ICT and pharmaceutical, to cheaply print a host of electronic devices from solar cells to LEDs with applications from interactive smart food and drug labels to next-generation banknote security and e-passports. Printed electronic circuitry will allow consumer products to gather, process, display and transmit information: for example, milk cartons could send messages to your phone warning that the milk is about to go out-of-date. 2D nanomaterials can compete with the materials currently used for printed electronics. Compared to other materials employed in this field, they have the capability to yield more cost effective and higher performance printed devices. However, while the last decade has underlined the potential of 2D materials for a range of electronic applications, only the first steps have been taken to demonstrate their worth in printed electronics. Nanosheets for two-dimensional transistorsResearchers now show that conducting, semiconducting and insulating 2D nanomaterials can be combined together in complex devices. It was critically important to focus on printing transistors as they are the electric switches at the heart of modern computing. This work opens the way to print a whole host of devices solely from 2D nanosheets. Standard printing techniques were used to combine graphene nanosheets as the electrodes with two other nanomaterials, tungsten diselenide and boron nitride as the channel and separator (two important parts of two-dimensional transistors) to form an all-printed, all-nanosheet, working transistor. Carbon-based molecules with limitationsPrintable electronics have developed over the last thirty years based mainly on printable carbon-based molecules. While these molecules can easily be turned into printable inks, such materials are somewhat unstable and have well-known performance limitations. There have been many attempts to surpass these obstacles using alternative materials, such as carbon nanotubes or inorganic nanoparticles, but these materials have also shown limitations in either performance or in manufacturability. While the performance of printed 2D devices cannot yet compare with advanced transistors, the team believe there is a wide scope to improve performance beyond the current state-of-the-art for printed transistors. The ability to print 2D nanomaterials is based on Prof. Coleman’s (AMBER) scalable method of producing 2D nanomaterials, including graphene, boron nitride, and tungsten diselenide nanosheets, in liquids, a method he has licensed to Samsung and Thomas Swan. These nanosheets are flat nanoparticles that are a few nanometres thick but hundreds of nanometres wide. Critically, nanosheets made from different materials have electronic properties that can be conducting, insulating or semiconducting and so include all the building blocks of electronics. Liquid processing is especially advantageous in that it yields large quantities of high quality 2D materials in a form that is easy to process into inks. Prof. Coleman’s publication provides the potential to print circuitry at extremely low cost which will facilitate a range of applications from animated posters to smart labels. Ref.KY56-C4706KY56-2SA1860 

LMX3268VBHXThe International Labor Organization (ILO) points out that some 40 million tons of electronic waste (including computers, mobile phones, printers, etc.) are produced every year. The prospect is that this amount will increase even more over time, as electronic devices with new functions and more attractive designs are constantly appearing, stimulating new purchases from the consumer without the old product being out of date. Being present is most electronic devices, Printed Circuit Boards, also known as PCBs, are among the most discarded parts. They are made up of a plastic board and fibrous materials (such as plastic polymers) and a thin film of metallic substance (copper, silver, gold or nickel). These films form “tracks” or “paths” that will be responsible for the electrical conduction done by the electronic components. They can also have other materials in their composition, such as alloys, which have distinct melting points, thus allowing for manipulation and arrangement. There are several alloys available to be used, such as cerrobend, low melting point alloy or fusible alloys. Recycling electronic waste is much needed, because of the chemical components in its composition, with some of them being toxic – they can cause problems if they are disposed of incorrectly. For PCBs specifically, their recycling process involves quite some steps. Mechanical processesIt starts with a pre-treatment system that aims to separate metals, polymer materials and ceramics. After this step, the metals are sent to the metallurgical refining process. The techniques that make up this process are: comminution, classification and separation. Comminution is the technique used to reduce particle size and release metals for future concentrations. In the classification step, the material particles obtained by the previous process must be separated or classified according to their size. After the steps of comminution and classification, the enrichment of the material takes place by means of separation techniques: the parts that are interesting for the refining process of the metal are separated, discarding any impurities. In the case of circuit boards, the difference in electrical conductivity between metals and non-metals is a fundamental condition for the good result of the technique. Non-conductive materials (polymers and ceramics) can be separated from conductors (metals). Some techniques employed for this purpose are explained below. Pyrometallurgy processIt is a metallurgical process that uses high temperatures to produce pure metals, alloys or intermediate compounds. Pyrometallurgy requires high energy consumption to reach the appropriate temperatures for each stage of the process. There are several steps in the process, from the drying of the raw material to the refining of the final product. The chemical transformation step to be used will depend on the material in question. The best known are calcination (decomposition by heat in the presence of oxygen), roasting (calcination applied to sulphides) and pyrolysis (decomposition by the action of heat in an environment with little or no oxygen). Some of the major problems in the use of pyrometallurgical processes are the possibility of emission of toxic compounds such as dioxins and the high energy consumption. Hydrometallurgy processIt consists of the separation of metals. Some of the advantages of this method are the energy savings and the lower pollution of the environment. Electrometallurgy processIt is a process of refining metals through electrolysis. During electrolysis, metals without the impurities undergo electrodeposition, in which metals such as copper, zinc, cadmium, aluminum, precious metals, among others, can be recovered with a high degree of purity; Biometallurgy processThis process uses the action of microorganisms and minerals to recover valuable metals. This process requires a lot of time and metal needs to be exposed to microbial action. Where to recycle?If your computer and its PCBs are not broken but only technologically lagged, look for specialized places that accept donations of these items. You can also resell those components on the Internet, for example. However, and regardless of the final decision, always be sure that the final destination to be given to these materials is a proper one, always avoiding to harm the environment. Ref.IC ChipsPCB2B12ALMZ12001EXT

(Random telegraph noise from single molecule was adsorbed on SWNT.) Noise is low-frequency random fluctuation that occurs in many systems, including electronics, environments, and organisms. Noise can obscure signals, so it is often removed from electronics and radio transmissions. The origin of noise in nanoscale electronics is currently of much interest, and devices that operate using noise have been proposed. Materials with a high surface-to-volume ratio are attractive for studying the noise produced by nanoscale electronics because they are very sensitive to changes of their surfaces. A representative material of this type is carbon nanotubes, which are rolled sheets of the graphene hexagonal network, which is only one carbon atom thick. A Japanese collaboration led by Osaka University has explored the ability of single molecules to affect the noise generated by carbon nanotube-based nanoscale electronic devices. The team fabricated simple devices consisting of a carbon nanotube bridging two electrodes. The devices were exposed to different large molecules, causing some to bind to the carbon nanotube surface. It was found that different molecules gave unique noise signals related to the properties of the molecules. The strength of the interaction between the carbon nanotubes and molecules was able to be predicted from the obtained noise signals. "The signal generated by the carbon nanotube device changed following the adsorption of specific single molecules," says first author Agung Setiadi. "This is because the adsorbed molecule generated a trap state in the carbon nanotube, which changed its conductance." What this means is that the carbon nanotube-based devices were so sensitive that the researchers were able to detect unique signature from single molecules. The ability to characterize single molecules using highly sensitive nanoelectronics is an exciting prospect in the field of sensors, particularly for neuro- and biosensor applications. "Use of noise signals to identify molecular activity ((interaction) or (active orbital)) is attractive for developing advanced sensing devices," explains corresponding author Megumi Akai-Kasaya. "We demonstrated that noise can be exploited to improve the signal detection ability of a device." The results of this successful demonstration will be published in the near future in a follow-up article. Signal detection sensitivity may be increased through controllable noise generation. These carbon nanotube-based devices illustrate that it is possible to detect single molecules through their unique noise signatures in the device current signals. Improved knowledge of the molecular-level origin of noise should lead to the development of electronics that use noise to improve their performance rather than degrade it.. Ref.A1321ELHLT-TAS5030-ATST 

  A MOSFET is a four-terminal device having source(S), gate (G), drain (D), and body (B) terminals. In general, the body of the MOSFET is in connection with the source terminal thus forming a three-terminal device such as a field-effect transistor. MOSFET is generally considered as a transistor and employed in both analog and digital circuits. This is the basic introduction to MOSFET. Let’s step into the world of MOSFET and find out its secret.     Catalog   I. What is MOSFET? 1.1 Brief Introduction 1.2 MOSFET Structure 1.3 Electrical Symbol and Types 1.4 MOSFET Operating Principle II. MOSFET Selection III. MOSFET Gate Material IV. MOSFET Advantage V. MOSFET Technology VI. Common MOSFET Failures VII. MOSFET Well-known Brands FAQ   I. What is MOSFET?   1.1 Brief Introduction     MOSFET(metal-oxide-semiconductor field-effect transistor) is a type of field-effect transistor (FET), most commonly fabricated by the controlled oxidation of silicon. It has an insulated gate, whose voltage determines the conductivity of the device. This video will cover the basics of what you need to use it in your circuit, including calculating if you need a heat sink or not.   MOSFET (metal-oxide semiconductor field-effect transistor) is a kind of field effect transistors (FET), that is, the gate of metal layer (M) is separated by oxide layer (O) to control the semiconductors (S) by the field effect transistor.   1.2 MOSFET Structure   Fig. 1 mosfet body structure Fig. 1 is a cross-sectional view of a typical N-channel enhanced NMOSFET diagram. a P-type silicon semiconductor material is used as a substrate, two N-type regions are diffused on the surface of the substrate, a layer of silicon dioxide (SiO2) insulating layer is covered on the substrate, and finally, two holes are formed by using an etching method over the N region. The metallization method is used to make three electrodes: G (gate), S (source), and D (drain) in the insulating layer and the two holes, respectively.   From Fig. 1, we can see that the gate G is insulated from drain D and source S, and there are two PN junctions between D and S. In general, the substrate and the source S are connected internally, in other words, there is a PN junction between D and S.   Fig. 1 is a basic block diagram of a common n-channel enhancement MOSFET. To improve the performance of some parameters, such as improving the working current, increasing the working voltage, reducing the on-resistance, improving the switching characteristic, and so on. With different structures and processes, there are VMOS, DMOS, TMOS, etc. Although their structures are different, the working principle is the same.   1.3 Electrical Symbol and Types Fig. 2 mosfet symbols There are many variations in circuit symbols commonly used in MOSFET. The most common design is to represent the channel in a straight line, two lines perpendicular to the channel to represent the source and drain, and the left and the channel parallel and shorter lines to represent the grid. Sometimes a straight line representing the channel is replaced by a broken line to distinguish between an enhancement mode MOSFET or a depletion mode MOSFET and each mode divided into two types respectively, NMOSFET and PMOSFET. Fig. 3 NMOSFET and PMOSFET     Depletion Mode: the Gate-Source voltage of a transistor switches the device “OFF”. The depletion-mode MOSFET is equivalent to a “Normally Closed” switch.   Fig. 4 structure and electrical symbol  (depletion mode mosfet)   Enhancement Mode: the Gate-Source voltage of a transistor switches the device “ON”. The enhancement-mode MOSFET is equivalent to a “Normally Open” switch.   Fig. 5 enhancement type MOSFET(channel structure) Since the MOSFET on the integrated circuit chip is a four-terminal component, there is a bulk or body except for the gate, source and drain. The arrow extending from the channel to the right can indicate that the component is an NMOSFET or PMOSFET. In addition, the arrow direction is always pointed from the P end to the N end, so the arrow points from the channel to the base is the P-type MOSFET, abbreviated PMOS.   On the contrary, if the arrow points from the base to the channel, the base is P-type, and the channel is N-type, which is the N-type MOSFET. In a typical discrete device, that base and source are typically connected together so that the distributed MOSFET is typically a three-terminal element. Whereas a MOSFET in an integrated circuit, the polarity of the base is not indicated because of the use of the same base, and a circle is added to the gate terminal of the PMOS to distinguish.     P-Channel MOSFET: It has a P-Channel region between source and drain. It is a four-terminal device such as gate, drain, source, body. The drain and source are heavily doped p+ region and the body or substrate is n-type. The flow of current is positively charged holes. When we apply the negative gate voltage, the electrons present under the oxide layer are pushed downward into the substrate with a repulsive force. The depletion region populated by the bound positive charges which are associated with the donor atoms. The negative gate voltage also attracts holes from the p+ source and drain region into the channel region.       N- Channel MOSFET: It has an N-channel region between source and drain. It is a four-terminal device such as gate, drain, source, body. In this type of MOSFET, the drain and source are heavily doped n+ region and the substrate or body is P-type. The current flows due to the negatively charged electrons. When we apply the positive gate voltage the holes present under the oxide layer pushed downward into the substrate with a repulsive force. The depletion region is populated by the bound negative charges which are associated with the acceptor atoms. The electron's reach channel is formed. The positive voltage also attracts electrons from the n+ source and drains regions into the channel. Now, if a voltage is applied between the drain and source the current flows freely between the source and drain and the gate voltage controls the electrons in the channel. Instead of positive voltage if we apply negative voltage a hole channel will be formed under the oxide layer.       Therefore, the MOSFET has 4 modes: P-channel enhancement mode, P-channel depletion mode, N-channel enhancement mode, N-channel depletion mode. Their circuit symbols and application characteristic curves are shown in the following figure.  Fig. 6 circuit symbols and application characteristic curves of MOSFET 1.4 MOSFET Operating Principle The internal structure and electrical symbols of power MOSFET can be divided into NPN type and PNP type. That is, the source and drain poles of the N-channel FET are connected to the N-type semiconductor, and the source and drain of the P-channel FET are connected to the P-type semiconductor. We know that the output current of the general transistor is controlled by the input current. But for field-effect transistors, the output current is controlled by the input voltage (or field voltage), which can be considered to be minimal or no input current, causing the device to have a high input impedance, and it is the reason why we call it a FET.   The working principle of power MOSFET is as follows: adding positive power supply between drain and source, and no voltage between gate and sources. The PN junction J1 formed between drain and source is anti-biased, and there is no current flow between drain-source.    Conductive: adding the positive voltage UGS, the gate is insulated between the gate and source, so there will be no gate current flowing through. However, the positive voltage of the gate pushes the hole in the P region below it and attracts the minority electron in the P region to the surface of the P region below the gate when the UGS is greater than the UT (on voltage or threshold voltage). The electron concentration on the surface of the P region under the gate will exceed the hole concentration, making the P-type semiconductor invert into the N-type. For the inversion layer, the N-channel is formed and the PN junction J1 is disappeared, and meanwhile, the drain electrode and the source electrode are conductive.    Basic static characteristics of power MOSFET: Its transfer and output characteristics are shown in Fig. 7.   Fig. 7 transfer and output characteristics of mosfet The relationship between drain current ID and voltage UGS between gate and source is called the transfer characteristic of MOSFET. When ID is large, the relationship between ID and UGS is approximately linear, and the slope of the curve is defined as grid-anode transconductance Gfs.   The voltage-current characteristic (output characteristics) of drain include the cut-off region (corresponding to the cut-off region of GTR), the saturated region (corresponding to the magnification region of GTR), and the unsaturated region (corresponding to the saturation region of GTR). The MOSFET operates in the on-off state, that is, switching back and forth between the cut-off zone and the unsaturated zone. There are parasitic diodes between the drain and source, and the devices are on when a reverse voltage is added between the drain and source. The on-state resistance of the power MOSFET has a positive temperature coefficient, which is beneficial to the current sharing of the devices in parallel.   1. Cut-off Region: with the transistor acting as an open switch, the gate-source voltage is much lower than the transistor's threshold voltage so the MOSFET transistor is switched off fully.   2. Linear (Ohmic) Region: the transistor is in its constant resistance region behaving as a voltage-controlled resistance whose resistive value is determined by the gate voltage.   3. Saturation Region: the transistor is in its constant current region and is therefore switched on fully. The Drain current is equal to the maximum with the transistor acting as a closed switch.   Dynamic Properties   On-delay time (Td): it is the time experienced when the gate-source voltage rises to 10% of the gate drive voltage to the specified current rises to 10%.   Rise time (Tr): it is the time taken to increase the drain current from 10% to 90%. The ID steady-state value is determined by the drain-source voltage UE and the drain load resistance. The UGSP is related to the steady-state value of the ID, and when the UGS reaches the UGSP, it continued to increase until it reached the steady-state, but the ID did not change.   Turn-on time: the sum of turn-on delay time and rise time.   Turn-off delay time (Td): it refers to the time from when the voltage between gate and source drops to 90% of the gate drive voltage to the leakage current of 90% of the specified current. This shows the delay before the current is transferred to the load.    Drop time: it is the time experienced by the drain current drops from 90% to 10%.    Turn-off time: the sum of the turn-off delay time and drop time.   Understand several commonly used parameters of MOSFET. VDS is the drain-source voltage, which is an absolute parameter rating of MOSFET, which indicates the maximum voltage value that MOSFET can bear between drain and source. It is important to note that this parameter is related to junction temperature, and the higher the junction temperature is, the greater the value is. RDS (on), refers to the leakage source on-resistance, which represents the on-resistance between drain and source when MOSFET is on under certain conditions.    This parameter is related to MOSFET junction temperature and driving voltage Vgs. In a certain range, the higher the junction temperature, the greater the Rds, the higher the driving voltage, the smaller the Rds. Qg is the gate charge, gate charge is the charge required to increase the gate voltage from 0V to the termination voltage (such as 15V) under the action of the driving signal.   That is the charge required by the driving circuit from the cut-off state to the full-on state, which is the main parameter used to evaluate the driving ability of the driving circuit of the MOSFET. Id (drain current), is usually described in several different ways. According to the form of the working current, it divided into the continuous drain current and the pulse drain current.    In addition, it is also an absolute parameter rating of MOSFET, but this maximum current value does not mean that the drain current can reach this value during operation. It means that when the shell temperature is at a certain point if the operating current of MOSFET is the maximum drain current mentioned above, the junction temperature will reach the maximum value. Thus this parameter is also related to device packaging and ambient temperature.   Eoss (output volume energy), representing the output capacitance Coss stored in the MOSFET. Because the output capacitance Coss of MOSFET has very obvious nonlinear characteristics, it varies with the change of Vds voltage. If the datasheet identifies this parameter, it will be helpful to evaluate the switching loss of the MOSFET. The current rate of the body diode di/dt reflects the MOSFET reverse recovery characteristics. Because the diode is a bipolar device, it is affected by the charge storage, when the diode reverses bias, the charge stored in the PN junction must be removed, which is precisely the reaction of the above-mentioned parameters characteristic.   The maximum gate-source driving voltage Vgs, which is also an absolute parameter rating of the MOSFET, represents the maximum driving voltage that the MOSFET can withstand. Once the driving voltage exceeds this limit, permanent damage to the gate oxide can occur even in a very short period of time. Generally speaking, as long as the driving voltage does not exceed the limit, there will be no problem. However, due to the existence of parasitic parameters in some special cases, the Vgs will be affected unpredictably, which needs to be paid more attention to. SOA (safe work area), each MOSFET will give its safe working area. For example, different bipolar transistors, power MOSFET does not show a second breakdown, so the safe operation area is simply defined from the dissipative power that causes the junction temperature to reach the maximum allowable value.      II. MOSFET Selection   After understanding the principle of MOSFET selection, You can select the correct MOSFET with the following four steps.   1) channel selection The first step in choosing the right device for design is to decide whether to use N-channel or P-channel MOSFET. In typical power applications, when a MOSFET is grounded and the load is connected to the trunk voltage, the MOSFET forms a low-voltage side switch. N-channel MOSFET should be used in the low-voltage side switch, which is due to the voltage required by switching on or switching off the device. When the MOSFET is connected to the bus and the load is grounded, the high-voltage side switch is used. P-channel MOSFET is usually used in this case, which is also due to the consideration of driving voltage.   2) selection of voltage and current The higher the rated voltage, the higher the cost of the device. According to practical experience, the rated voltage should be greater than trunk voltage or bus voltage. This will provide sufficient protection so that the MOSFET can work well. As far as MOSFET is concerned, it is necessary to determine the maximum possible voltage between the drain and the source. Other safety factors that design engineers need to consider include voltage transients induced by switchgear, such as motors or transformers. And rated voltages vary from application to application, typically, portable devices are 20V, FPGA power supplies are 20V~30V, and so on.　   In the continuous conduction state, the MOSFET is stable and the current passes through the device continuously. A pulse spike refers to a large number of surge current (or peak current) flowing through the device. Once the maximum current is determined under these conditions, simply select the device that can withstand the maximum current.   3) calculating on-loss The power loss of MOSFET devices can be calculated by Iload2×RDS (on). Because the on-resistance varies with temperature, the power loss also varies proportionally. For portable designs, lower voltages are more common, and for industrial designs, higher voltages can be used. Note that the RDS (on) resistance increases slightly with the current. Variations in the electrical parameters of the RDS (on) resistance can be found in the technical datasheet provided by the manufacturer.   4) heat dissipation requirements for a computing system　 The designer must consider two different situations, the worst case, and the real situation. It is recommended that the worst-case results be used because the results provide a greater security margin to ensure that the system does not fail. There are also some measurements on the MOSFET table that need to be noticed, such as the thermal resistance between the semiconductor junction and the environment of the packaged device, and the maximum junction temperature.   Switching loss is also a very important indicator. The voltage-current product of the on-off moment is quite large, which determines the switching performance of the device to a certain extent. However, if the system requires high switching performance, you can choose a power MOSFET with a lower gate charge.     III. MOSFET Gate Material   Theoretically, the gate of MOSFET should be chosen as well as possible, and the conductivity of polysilicon doped by heavy can be used on the gate of MOSFET.    The reasons for using polysilicon in MOSFETs are as follows:    1) The threshold voltage of the MOSFET is mainly determined by the difference between the work function of the gate and the channel material, and because the polysilicon is essentially a semiconductor, it is possible to change its work function by doping impurities of different polarities. More importantly, since the gap between the polysilicon and the silicon as the channel is the same, it is possible to achieve the demand by directly adjusting the work function of the polysilicon when the threshold voltage of the PMOS or NMOS is reduced. Conversely, the work function of the metallic material is not like the semiconductor is then easily changed so that it becomes difficult to reduce the critical voltage of the MOSFET. And if the threshold voltage of the PMOS and the NMOS is to be reduced at the same time, two different metals are required to do their gate material, respectively, and a large variable for the producing process.   2) After years of research on the silicon-silica interface, it has been proved that the defect between the two materials is relatively small. On the contrary, there are many defects in the metal-insulator interface, so it is easy to form a lot of surface energy levels between the two, which greatly affects the characteristics of the elements.   3) The melting point of the polycrystalline silicon is higher than most of the metal, while in the modern semiconductor process, the gate material is used to deposit the gate material at high temperatures to improve the efficiency of the element. The low melting point of the metal will affect the upper-temperature limit that can be used by the process.   However, although polysilicon has been the standard material for the manufacture of MOSFET gates, there are also a number of shortcomings of it, which makes it possible for some MOSFET to use metal gates in the future.    These shortcomings are as follows:   (1) Polysilicon is less conductive than metal, limiting the speed of signal transmission. Although doping can be used to improve its conductivity, the effectiveness is still limited. Some metal materials with a high melting point, such as tungsten, titanium, cobalt, or nickel, are used to make alloys with polysilicon. This type of mixture is commonly referred to as metal silicide. The polysilicon gate with metal silicide has good electrical conductivity and can withstand a high-temperature process. In addition, because the position of the metal silicide is on the surface of the grid, therefore, the critical voltage of MOSFET will not be affected much.   The process of plating a metal silicide on the gate, source, and drain is referred to as self-aligned metal, commonly referred to as salicide process.   (2) When the size of the MOSFET is small and the gate oxide layer also becomes very thin, for example, the new process can reduce the oxide layer to a thickness of about one nanometer, and a phenomenon is also generated unprecedentedly, and that is "polysilicon depletion". When the inversion layer of the MOSFET is formed, the MOSFET gate polysilicon depletion phenomenon is occurring close to the oxide layer, and a depletion layer is present to influence the conduction characteristics of the MOSFET. To address this problem, one way is the metal gate. Reasonable materials include tantalum, tungsten, tantalum nitride, or titanlium nitride. The gates made by these metals usually form MOS capacitors along with oxide formed by high permittivity substances. Another solution is the polysilicon alloying, also called FUSI (FUlly-SIlicide polysilicon gate).   IV. MOSFET Advantage   MOSFET was first made successfully in 1960 by D. Kahng and Martin Atalla in Bell Labs, and the operating principle of this element was very different from that of the bipolar junction transistor (BJT) invented by William Shockley in 1947. And because of the low cost and small size, it plays a very important role in large-scale integrated circuits (LSI) and very large-scale integrated circuits (VLSI) than BJT.   1) Field-effect transistor (FET) is a voltage control element, and bipolar junction transistor (BJT) is a current control element. The FET should be selected when only less current is allowed, and the BJT should be chosen when the signal voltage is low and more current is allowed to flow through from the source of the signal.   2) The source and drain poles of some FET can be used interchangeably, the gate voltage can also be positive and negative, and the flexibility is better than the bipolar transistor.   3) FET is called a monopole device because it makes use of majority carriers to conduct electricity, while BJT is conducting by majority carrier or minority carrier, therefore, it is called bipolar device.   4) FET can work under the conditions of very low current and low voltage, and its manufacturing process can easily integrate many FETs on a silicon wafer. Therefore, FET has been widely used in large-scale integrated circuits (LSI).   With the improvement of the performance of MOSFET components, except the traditional applications in digital signal processing such as microprocessors and microcontrollers, more and more integrated circuits for analog signal processing can be implemented by MOSFET.   V. MOSFET Technology   1) Dual-gate MOSFET Dual-gate MOSFET is usually used in radio frequency (RF) integrated circuits. The two gates of the MOSFET can control the current. In RF circuits, the second gate of the dual-gate MOSFET is mostly used for gain, mixer, or frequency conversion control.   2) Depletion Type MOSFET In general, a depletion-mode MOSFET is less common than the enhancement mode MOSFET. The depletion-mode MOSFET changes the impurity concentration of the channel in the doping process so that the channel still exists even if the gate of the MOSFET is not applied voltage. If you want to close the channel, you must apply a negative voltage to the gate. Thus the most application of the depleted MOSFETs is in the "normally-off" switch, while the enhancement-mode MOSFET is usually used in the " normally-on" switch.   3) NMOS Logic The NMOS of the same driving capability is generally smaller than the area occupied by the PMOS, and therefore, if an NMOS is used only on the design of the logic gate, the chip area itself can be reduced. However, although the area of the NMOS logic is small, the static power will be consumed unlike the CMOS logic, so it has gradually exited the market after the mid-1980s.   4) Power MOSFET There is a significant structural difference between the power MOSFET and the above-mentioned MOSFET elements. In general, MOSFET in integrated circuits are planar structures, and the endpoints of transistors are only a few microns away from the surface of the chip. But all the power components are vertical structures, which allows the components to withstand both high voltage and high current working environments. A power MOSFET withstand voltage is a function of the doping concentration and the thickness of the N-type epitaxial layer, and the width of the channel is related to how much the current can pass through, that is, the wider channel can accommodate more current. For a planar MOSFET, the current and the breakdown voltage are dependent on the length and width of the channel. For a vertical MOSFET, the area of the element is approximately proportional to the current it can hold, and the thickness of the epitaxial layer is proportional to its breakdown voltage.   Working principle Due to the positive power supply between the source and the drain, the voltage between them is zero. The PN junction J1 formed between the P base region and the N drift region is anti-biased, and no current flows between the source and the drain.   Conduction: the positive voltage UGS, the gate is insulated between the gate and the source, so there will be no gate current flowing through. However, when the positive voltage of the gate pushes the hole in the P region below it and attracts the minority electron in the P region to the surface of the P region below the gate and the UGS is greater than the UT (on voltage or threshold voltage), the electron concentration on the surface of the P region under the gate will exceed the hole concentration, which causes the P-type semiconductor inversion to become N-type and becomes the inversion layer. The inversion layer forms N-channel and makes the PN junction J1 disappear, and the drain and the source turn to conductive.   It is worth mentioning that power MOSFET with planar structure is not non-existent, and this kind of element is mainly used in advanced sound amplifiers. The characteristics of planar power MOSFET in the saturation region are better than that of vertical structure MOSFET. Vertical power MOSFET takes the advantage of very small turn-on resistance and is mostly used for switches.   5) DMOS DMOS is an abbreviation for a double-diffused MOSFET, which is mainly used for high voltage and belongs to the category of high-voltage MOSFET.   The MOSFET is used to realize the analog switch. The channel resistance of the MOSFET is low when the MOSFET is turned on, and the resistance is almost infinite when the MOSFET is turned off so that the switch which is suitable as a switch of the analog signal (the energy of the signal is not lost due to the resistance of the switch). When the MOSFET is a switch, its source and drain are different from each other, respectively, because the signal can be accessed from any end of the MOSFET. For an NMOS switch, the negative voltage is in the source, it opposite to the PMOS, the positive voltage is in the source. The signal that the MOSFET switch can transmit is subject to its voltage between gate and source, gate and drain, drain and source. If the upper limit of the voltage is exceeded, the MOSFET may burn out.   MOSFET switches have a wide range of applications, such as the need for sampling holding circuit (sample-and-hold circuits) or truncated circuit (chopper circuits) design, For example, MOSFET switch can be seen on the analog-digital converter (A / D converter) or switched capacitor filter (switch-capacitor filter).   6) Single MOSFET Switch When the NMOS is used as a switch, the base is grounded and the gate is the controlling end of the switch. The state of the switch is on when the gate voltage subtracts the source voltage exceeding the critical voltage. If the gate voltage continues to rise, the current through which the NMOS can pass more. NMOs operate in the linear region when the switch is turned on because the voltage of the source and drain tends to be consistent when the switch is on.   When the PMOS is used as a switch, its base is connected to the highest potential in the circuit, usually a power supply. The voltage of the gate is very low than the source. And when the gate exceeds the critical voltage, the PMOS switch will be turned on.   And a single MOSFET switch may reduce the amplitude of the signal and distort the signal.   7) Double MOSFET (CMOS) Switch In order to improve the signal distortion caused by the single MOSFET switch mentioned above, the use of a PMOS plus and an NMOS of CMOS switch has become the most common practice at present. The PMOS switch connects the source and drain of the NMOS separately. The basic joining rule is the same as the traditional connecting method of NMOS and PMOS. When the input voltage is at (VDD-Vthn) and (VSS+Vthp), the PMOS and NMOS are on, but when the input is less than (VSS+Vthp), only NMOS is on and the input is greater than (VDD-Vthn), and only the PMOS turns on. The advantage of this is that under most of the input voltage, both the PMOS and the NMOS are turned on at the same time, and if the on-resistance of either side is increased, the on-resistance on the other side is reduced, so that the resistance of the switch can be kept almost constant, thus the signal distortion is reduced.   Fig. 8 switching process of power MOSFET   VI. Common MOSFET Failures     Overvoltage damage, including gate overvoltage and drain overvoltage, often accompanied by overcurrent. If protection happened in a very short period of time, it may be overvoltage damage. If there is no overvoltage protection and the state turns into overcurrent damage, the chip in the source non-line region will burn out.   A large current, such as severe over-current short-circuit damage, will cause a large amount of heat to burn out the chip.   Overheat damage, if the MOS tube isn’t appearing overcurrent and overvoltage, just because the junction temperature is too high, if the chip is protected, the surface will not see obvious burns, if not, there will be a large amount of burning area.   In general, the mechanism of MOS tube damage is usually thermal damage, local overheating, or overall heating, such as overvoltage, is a crystal package that can’t stand high voltage breakdown causing heating damage.   The fault analysis of the MOS tube should be based on the combination of specific circuit and burning phenomenon to be more accurate. Fig. 9 basic structure of an n-channel mosfet     VII. MOSFET's Well-Known Brands   MOSFETs are mainly divided into several series: American, Japanese, Korean, Taiwan, and so on. The brand's representatives of each system are as follows:   American: IR ST TI PI Fairchild Infineon ON Semiconductor Japanese: TOSHIBA RENESAS SHINDENGEN Taiwan: APEC CET Korean: KEC AUK MagnaChip KIA Truesemi Wisdom   FAQ 1. What is Mosfet and how it works? In general, the MOSFET works as a switch, the MOSFET controls the voltage and current flow between the source and drain. The working of the MOSFET depends on the MOS capacitor, which is the semiconductor surface below the oxide layers between the source and drain terminal.   2. What is Mosfet and its characteristics? MOSFETs are tri-terminal, unipolar, voltage-controlled, high input impedance devices which form an integral part of vast variety of electronic circuits. ... In this region, MOSFET behaves like an open switch and is thus used when they are required to function as electronic switches.   3. How many types of Mosfet are there? Four types. There are two classes of MOSFETs. There is depletion mode and there is enhancement mode. Each class is available as n- or a p-channel, giving a total of four types of MOSFETs.   4. What is an ideal Mosfet? In an ideal MOSFET, setting the gate-source voltage to a value VGS < VTn places the transistor into cutoff with ID = O. Increasing the gate-source voltage to a value VGS > VTn allows the transistor to conduct current ID; this defines the active mode of operation. 5. How do I know if my MosFet is bad? A good MOSFET should have a reading of 0.4V to 0.9V (depends on the MOSFET type). If the reading is zero, the MOSFET is defective and when the reading is “open” or no reading, the MOSFET is also defective. When you reverse the DMM probe connections, the reading should be “open” or no reading for a good MOSFET.   6. What is a Mosfet used for? What is a MOSFET and How does it work? MOSFET, in short, is a metal oxide semiconductor field-effect transistor used to switch or amplify voltages in circuits. Being part of the field-effect transistor family, it is a current-controlled device that is constructed with 3 terminals.   7. Is Mosfet still used? The MOSFET is by far the most widely used transistor in both digital circuits and analog circuits, and it is the backbone of modern electronics. It is the basis for numerous modern technologies, and is commonly used for a wide range of applications.   8. Why is it called Mosfet? The source is so named because it is the source of the charge carriers (electrons for n-channel, holes for p-channel) that flow through the channel; similarly, the drain is where the charge carriers leave the channel.   9. What causes a Mosfet to fail? If the maximum operating voltage of a MOSFET is exceeded, it goes into Avalanche breakdown. ... If the energy contained in the transient over-voltage is above the rated Avalanche energy level, then the MOSFET will fail. The device fails short circuit, initially, with no externally visible signs.   10. Why N channel is better than P channel Mosfet? N-Channel MOSFETs are more efficient than P-Channel MOSFETs.It comes down to physics. N-Channel MOSFETs use electron flow as the charge carrier. P-Channel MOSFETs use hole flow as the charge carrier, which has less mobility than electron flow. And therefore, they have higher resistance and are less efficient.   You May Also Like Selection of Drive Resistor: MOSFET | Gate Drive Reference Component KY56-SQ7415AEN-T1_GE3 KY56-STP160N3LL

Industrial design researchers at Brunel University London have solved two of the major challenges which prevent everyday items of clothing being turned into power sources for smartphones, tablets and other personal tech.Technology to produce super capacitor thread capable of being made into cloth has been around for some time. But until now scientists have been unable to make it provide sufficient voltage for most devices or devise a method to produce it economically outside the lab.Now patented breakthroughs made by colleagues Professors David Harrison and John Fyson, Dr Yanmeng Xu, Dr Fulian Qiu and Ruirong Zhang of Brunel's Department of Design mean thread capable of storing and supplying enough power for common devices and of being manufactured at industrial scale are a reality.Explained Prof Harrison: "Supercapacitors are already ubiquitous as back-up power in phones, PCs and tablets."They store energy without a chemical reaction so can be charged and discharged almost indefinitely. But in thread form they have never before been able to break the 1V barrier."What we have done is show we can produce a multi-layered structure with two sequential capacitive layers capable of producing up to 2V. Breaking the 1V threshold is important as in the real world we work on the voltage of common batteries – 1.5V."We also wanted to address mass production issues so developed a process to semi-automatically coat stainless steel wire the thickness of a human hair with eight separate layers."The work at Brunel is part of the EU-sponsored Powerweave programme which brings together researchers from seven countries to produce textiles which can both generate and store power.Reference:KY36-F17724102900KY36-MKP1841410254KY36-BFC246816474

Samsung Electronics unveiled the industry’s first removable memory cards based on the JEDEC UFS 1.0 Card Extension Standard, for use in high-resolution mobile shooting devices such as DSLRs, 3D VR cameras, action cams and drones. Coming in a wide range of storage capacities including 256, 128, 64 and 32 GB, Samsung’s UFS cards are expected to bring a significant performance boost to the external memory storage market, allowing much more satisfying multimedia experiences.“Our new 256GB UFS card will provide an ideal user experience for digitally-minded consumers and lead the industry in establishing the most competitive memory card solution,” said Jung-bae Lee, senior vice president, Memory Product Planning & Application Engineering, Samsung Electronics.“By launching our new high-capacity, high-performance UFS card line-up, we are changing the growth paradigm of the memory card market to prioritise performance and user convenience above all.”Samsung’s new 256GB UFS removable memory card ─ simply referred to as the UFS card will provide greatly improved user experiences, especially in high-resolution 3D gaming and high-resolution movie playback.It provides more than five times faster sequential read performance compared to that of a typical microSD card, reading sequentially at 530 MB/s which is similar to the sequential read speed of the most widely used SATA SSDs.With this UFS card, consumers have the ability to read a 5GB, Full-HD movie in approximately 10 seconds, compared to a typical UHS-1 microSD card, which would take over 50 seconds with 95MB/s of sequential reading speed.Also, at a random read rate of 40,000 IOPS, the 256GB card delivers more than 20 times higher random read performance compared to a typical microSD, which offers approximately 1,800 IOPS.When it comes to writing, the new 256GB UFS card processes 35,000 random IOPS, which is 350 times higher than the 100 IOPs of a typical microSD card, and attains a 170MB/s sequential write speed, almost doubling the top-end microSD card speed.With these substantial performance improvements, the new 256GB UFS card significantly reduces multimedia data downloading time, photo thumbnail loading time and buffer clearing time in burst shooting mode, which, collectively, can be particularly beneficial to DSLR camera users.To shoot 24 large/extra fine JPEG photographs (1,120 MB-equivalent) continuously with a high-end DSLR camera, the 256GB UFS card takes less than seven seconds, compared to a UHS-1 microSD card which typically takes about 32 seconds, at 35MB/s.To achieve the highest performance and most power-efficient data transport, the UFS card supports multiple commands with command queuing features and enables simultaneous reading and writing through the use of separately dedicated paths, doubling throughput.As the leading memory storage provider, Samsung has been aggressive in preparing UFS solutions for the marketplace, while contributing to JEDEC standardisation of the Universal Flash Storage 2.0 specification in September 2013 and the UFS 1.0 Card Extension standard in March 2016.Following its introduction of the industry-first 128GB embedded UFS chip in January 2015, the company successfully launched a 256GB embedded UFS memory for high-end mobile devices in February of this year.As of earlier this month, Samsung also completed the Universal Flash Storage Association (UFSA)’s certification program that evaluates electrical and functional specifications for compatibility of a UFS card, and Samsung’s new UFS card products were approved as UFSA-certified UFS cards with the right to use the official UFS logo for the first time in the industry.Reference:S29GL032N11FFIS42S29GL064N90FFIS30S29AS016J70BFA040