Name: mos capacitor voltage and charge
Uploaded: 2024-07-08T13:20:41.000Z
Duration: 1 min 25 s
Channel: JoVE

Kondensatory MOS mają trzy warstwy: dolna warstwa to podłoże półprzewodnikowe, środkowa to warstwa izolacyjna, a górna warstwa metalowa to elektroda bramkowa, która kontroluje napięcie kondensatora.
Przy zerowym napięciu bramki nie płynie prąd, a kondensator jest nienaładowany.
Przyłożenie ujemnego napięcia do bramki przyciąga do powierzchni półprzewodnika, tworząc obszar akumulacji. Urządzenie zachowuje się jak konwencjonalny kondensator.
Stosując dodatnie napięcie, są odpychane z powrotem do podłoża, tworząc obszar ładunku kosmicznego zwany obszarem zubożenia, który działa jako kolejna pojemność szeregowo.
Przy wystarczająco wysokim napięciu koncentracja elektronów na powierzchni wzrasta, tworząc warstwę inwersyjną i jeszcze bardziej zmniejszając pojemność. Powoduje to gwałtowny wzrost prądu.
Odłączenie napięcia powoduje rozproszenie nagromadzonego ładunku, powodując zanik kanału i wyłączenie urządzenia.
Kondensatory MOS są stosowane w urządzeniach pamięci, takich jak DRAM, gdzie zapis danych polega na przyłożeniu napięcia bramki w celu utworzenia warstwy inwersyjnej, która tymczasowo przechowuje ładunek. Obecność lub brak tego ładunku reprezentuje dane binarne, które wymagają okresowego odświeżania ze względu na ich przejściowy charakter.

kondensator mos

Kondensator metalowo-tlenkowo-półprzewodnikowy (MOS) to podstawowa konstrukcja szeroko stosowana w technologii urządzeń półprzewodnikowych, szczególnie przy produkcji układów scalonych i tranzystorów MOSFET (tranzystory polowe z efektem metalo-tlenku-półprzewodnika). Kondensator MOS składa się z trzech warstw: metalowej bramki, tlenku dielektrycznego i podłoża półprzewodnikowego.


Bramka metalowa jest zwykle wykonana z materiałów o wysokiej przewodności, takich jak aluminium lub polikrzem. Pod metalową bramką znajduje się cienka warstwa izolującego tlenku, zwykle dwutlenku krzemu (SiO_2), który jest dielektrykiem. Podłoże półprzewodnika jest zwykle krzemem, który może być typu p lub n.


Kiedy do metalowej bramki przyłożone jest napięcie, wpływa to na rozkład nośników elektrycznych w półprzewodniku. Pasma energii półprzewodnika są płaskie przy zerowym przyłożonym napięciu, co wskazuje na brak nadmiernego ładunku w tlenku lub na powierzchni półprzewodnika. Gdy napięcie bramki wzrasta dodatnio, przyciąga elektrony w kierunku granicy tlenku i półprzewodnika. Powoduje to akumulację elektronów w krzemie typu n i zubożenie dziur w krzemie typu p, tworząc warstwę zubożoną.


Dalszy wzrost napięcia prowadzi do silnej inwersji, podczas której powierzchnia półprzewodnika pod tlenkiem zmienia swój rodzaj; na przykład typ p staje się typem n, ponieważ elektrony stają się nośnikami większościowymi. Ta warstwa inwersyjna ma kluczowe znaczenie w działaniu tranzystorów MOSFET. Pojemność struktury MOS zmienia się w zależności od napięcia przyłożonego do bramki.


Warstwa inwersyjna ma kluczowe znaczenie dla działania kondensatorów MOS w pamięci DRAM. Zapisywanie danych polega na przyłożeniu napięcia tworzącego tę warstwę i magazynowaniu ładunku w półprzewodniku. Ten przechowywany ładunek reprezentuje dane binarne, umożliwiające przechowywanie i odzyskiwanie informacji. Usunięcie napięcia powoduje rozproszenie ładunku, dezaktywację kanału i zachowanie przechowywanych danych. Ten cykl ładowania ma kluczowe znaczenie dla funkcjonalności i niezawodności pamięci DRAM w zastosowaniach komputerowych.

Kondensator MOS

Kondensatory MOS mają trzy warstwy: dolna warstwa to podłoże półprzewodnikowe, środkowa to warstwa izolacyjna, a górna warstwa metalowa to bramka ...

Education

JoVE Core

Electrical Engineering

Elektrotechnika

Unit 1

Jednostka 1

Transistors

Tranzystory

KEY TERMS AND CONCEPTS

KLUCZOWE TERMINY I POJĘCIA

MOS Capacitor

mos capacitor voltage and charge

A MOS capacitor uses voltage to control charge in a semiconductor. It is a key structure in semiconductor device technology and in the fabrication of integrated circuits and MOSFETs, or metal-oxide-semiconductor field-effect transistors.

The structure has three layers. A metal gate sits on top and is usually made from a highly conductive material such as aluminum or polysilicon. Below it is a thin insulating oxide layer, usually silicon dioxide (SiO2), and below that is a semiconductor substrate, often silicon that can be p-type or n-type.

At zero applied voltage, the semiconductor energy bands are flat. This means there is no excess charge in the oxide or at the semiconductor surface. When a positive voltage is applied to the gate, it changes how charge carriers are distributed in the semiconductor.

A positive gate voltage attracts electrons toward the oxide-semiconductor interface. In n-type silicon, this creates electron accumulation. In p-type silicon, it causes holes to leave the surface region, which forms a depletion layer.

If the voltage increases further, strong inversion occurs. In this state, the semiconductor surface beneath the oxide changes type. For example, a p-type surface can behave like n-type material because electrons become the majority carriers. This inversion layer is important for MOSFET operation.

The capacitance of a MOS structure changes with the gate voltage. In DRAM, this inversion layer is used to write data by applying a voltage and storing charge in the semiconductor. The stored charge represents binary data. When the voltage is removed, the charge dissipates, the channel turns off, and the stored data is preserved.

MOS Capacitor Voltage and Charge

bipolar junction transistor

BJT Structure and Carrier Flow

Bipolar junction transistors are important parts of electronic circuits. They help make amplifiers, memories, and microprocessors work. A BJT can be built as either NPN or PNP, depending on its doping pattern, which means the type of impurities added to the material. A BJT has three layers: the emitter, base, and collector. It also has two p-n junctions, so the device has a sandwich-like structure. The emitter is heavily doped so it can inject charge carriers into the base. The base is very...

configurations of bjt

BJT Amplifier Modes and Uses

Bipolar Junction Transistor (BJT) configurations are defined by which terminal is shared by the input and output circuits. The shared terminal can be the base, emitter, or collector. Each setup has different electrical behavior and fits different circuit needs. In the common base configuration, the base is the common terminal. This setup has high voltage gain, so it can work well in single-stage amplifier circuits such as microphone pre-amplifiers. It also reduces the input current signal...

working principle of bjt

PNP BJT Current Flow in Active Mode

PNP bipolar junction transistors control current flow by moving charge carriers between the emitter, base, and collector. In a common-base setup, the transistor can amplify or switch electronic signals when it operates in active mode. In a PNP transistor, the emitter is heavily doped with holes, which are positive charge carriers. The base is lightly doped with electrons, which are negative carriers. A forward bias across the emitter-base junction lowers the potential barrier and lets holes...

characteristics of bjt

BJT Current-Voltage Curves in Common Emitter

The Bipolar Junction Transistor (BJT) in a common-emitter setup is studied by measuring its current-voltage curves. These measurements show how the transistor responds when voltage and current are changed in a controlled way. They are key to understanding how a BJT works in electronic circuits. The input characteristics are found by varying the base-emitter voltage while keeping the collector-emitter voltage constant. This test shows a Shockley-type relationship between the collector current...

modes of operations of bjt

BJT Biasing: Active to Inverted Mode

A bipolar junction transistor (BJT) works in four modes that depend on how its two junctions are biased. Those modes are active, saturation, cut-off, and inverted. The biasing pattern controls whether the transistor amplifies current or acts like a switch. Active mode is the most common mode for amplification. In this mode, the emitter-base junction is forward-biased and the base-collector junction is reverse-biased. Electrons move from the emitter into the base, while the collector blocks...

frequency response of bjt

BJT Amplifier Response at Low and High Freq

A BJT amplifier’s response changes with frequency in a common-emitter circuit. Its behavior at low frequencies and high frequencies depends on the circuit’s equivalent model. These models help explain how the transistor handles AC signals. At low frequencies, the DC bias point sets the transistor’s operation. The emitter-base voltage, base current, and collector current define this bias point. The load line also shapes how the amplifier works, using the applied voltage and load resistance. <br...

cut-off frequency of bjt

BJT Frequency Limits and Gain Drop

BJT frequency limits show when a bipolar junction transistor stops keeping a steady gain. These limits matter because they mark the shift from the pass band to the stop band in an electronic signal. They help explain why a transistor may amplify one range of frequencies well and weaken signals at higher frequencies. The alpha cut-off frequency applies to the common-base configuration. At low frequencies, the current gain alpha stays stable. Beyond this upper-frequency limit, alpha drops and...

switching of bjt

BJT as a Digital On-Off Switch

Bipolar junction transistors (BJTs) can work as digital on-off switches in electronic circuits. In this mode, the transistor moves between cut-off and saturation. These two states match the off and on positions of an ideal switch. In cut-off mode, both the emitter-base junction and the collector-base junction are reverse-biased. This blocks current flow through the transistor and keeps it off. Circuits use this state when no signal transmission is needed, which helps maintain a low-power...

bjt amplifiers

Common-Emitter BJT Voltage Gain

Bipolar junction transistors, or BJTs, can act as amplifier parts when they work in the active region. In this mode, a small change in base-emitter voltage controls a larger collector current. That makes the transistor act like a voltage-controlled current source and lets it boost a weak signal into a stronger one. A common-emitter BJT amplifier uses that current change to create voltage gain. The output current flows through a load resistor, and the voltage drop across that resistor sets the...

small-signal analysis of bjt amplifiers

BJT Amplifier Gain and Input Resistance

BJT amplifier gain and input resistance can be analyzed with a small-signal model. In the active region, a bipolar junction transistor is used for linear amplification. Its base-emitter voltage includes a DC bias and a small AC signal. That input produces a collector current with both DC and AC parts. When the AC input signal is much smaller than the thermal voltage VT, the small-signal approximation applies. This makes it possible to find the AC collector current from the DC collector current...

field effect transistor

Field Effect Transistor Types and Uses

Field-effect transistors, or FETs, are important parts of electronic circuits. They have three terminals: gate, drain, and source. FETs are unipolar devices, which means they use either electrons or holes as charge carriers. That is different from bipolar transistors, which use both types of carriers. A FET controls the flow of charge from the source to the drain through a channel. The voltage difference between the gate and source controls how well that channel conducts. This makes the device...

characteristics of jfet

JFET Output Regions and Current Control

JFET output characteristics show how drain current changes with drain-source voltage and gate-source voltage. In a junction field effect transistor, the gate-source voltage controls the drain current. When the drain and gate voltages are set to zero, the device is in equilibrium and no net current flows. With the gate voltage held at zero, the drain current rises linearly as the source-drain voltage increases. This linear part is called the Ohmic region. In this region, the JFET acts like a...

biasing of fet

JFET Gate-Source Bias and Current Control

JFET gate-source bias controls current flow in a junction field effect transistor. A JFET uses one carrier type and comes in N-channel or P-channel forms. In both cases, the channel is surrounded by PN junctions, and those junctions help control how current moves through the device. In an N-channel JFET, N-type material forms the channel on a P-type substrate. The gate is made of P-type material. Biasing this device means applying a negative voltage to the gate relative to the source. That...

mos capacitor

A MOS capacitor uses voltage to control charge in a semiconductor. It is a key structure in semiconductor device technology and in the fabrication of integrated circuits and MOSFETs, or metal-oxide-semiconductor field-effect transistors. The structure has three layers. A metal gate sits on top and is usually made from a highly conductive material such as aluminum or polysilicon. Below it is a thin insulating oxide layer, usually silicon dioxide (SiO2), and below that is a semiconductor...

mosfet

MOSFET Current Control in Electronics

The MOSFET is a semiconductor device that controls electrical current in modern electronics. It is also called an IGFET or MISFET. The three main terminals are the source, drain, and gate. MOSFETs are classified as n-channel or p-channel devices. The type depends on the doping of the substrate and the source or drain regions. In an n-MOSFET, the source and drain are n-type regions separated from a p-type substrate by reverse-biased p-n diodes. The gate is built from a metal plate over an...

characteristics of mosfet

MOSFET Structure and Operating Regions

MOSFETs, or metal-oxide-semiconductor field-effect transistors, are important parts of electronic circuits. They are used to amplify and switch signals. Their behavior depends on several design features, including channel size, oxide thickness, junction depth, and substrate doping. Channel length and channel width shape how much current a MOSFET can carry and how fast it can switch. Shorter channels usually allow faster operation. The oxide thickness also matters. This silicon dioxide layer...

mosfet: enhancement mode

MOSFET Switching in Enhancement Mode

Enhancement-mode MOSFETs are MOSFETs that work as controlled electronic switches. They belong to the metal-oxide semiconductor field-effect transistor family. These devices come in two forms: n-channel and p-channel, and each one is used for a different polarity of operation. At zero gate-source voltage, or Vgs, an enhancement-mode MOSFET is usually non-conductive. In that default off state, no current flows between the drain and source terminals. When a positive Vgs is applied, it creates an...

mosfet: depletion mode

Depletion MOSFET Channel Control

Depletion-mode MOSFETs are normally on transistors with a built-in channel that conducts current without gate bias. They work differently from enhancement-mode MOSFETs, which need a positive gate-source voltage, or V gs, to turn on. In a depletion device, the channel is already open because the channel doping creates a low-resistance path between the drain and source. These devices behave much like junction field-effect transistors, or JFETs. The channel conductivity is set by the material...

mosfet amplifiers

MOSFET Gain and Biasing

MOSFET gain and biasing shape how a MOSFET amplifier works. When a MOSFET operates in its active region, it acts like a voltage-controlled current source. The gate-to-source voltage sets the drain current, and that behavior supports transconductance amplification. The output current then flows through a load resistor. That load resistor turns the circuit into a voltage amplifier. The output voltage is found by subtracting the voltage drop across the load resistor from the supply voltage, so...

small-signal analysis of mosfet amplifiers

small-signal-analysis-of-mosfet-amplifiers

MOSFET Amplifier Gain and Signal Distortion

MOSFET amplifiers can be treated as linear circuits when they operate in the saturation region. The gate-to-source voltage, or VGS, is the sum of a DC bias voltage and a small time-varying input signal. That bias sets the operating point and controls the drain current that flows from drain to source. When a small AC signal is added at the gate, the drain current has three parts. One part is the DC bias current, ID0, which is the quiescent current with no signal applied. A second part changes...

key terms and concepts

Learn how a MOS capacitor uses gate voltage to move charge, form depletion and inversion layers, and store data in DRAM.

MOS Capacitor Voltage and Charge | JoVE K12

JoVE Core Electrical Engineering offers easy-to-understand animated videos that cover fundamental concepts of electric circuits along with circuit analysis techniques. It incorporates first-order and second-order circuits using operational amplifiers and circuit transformation concepts. The inclusion of practical design examples and real-world applications through scientist-in-action videos adds significant educational value, making complex concepts accessible.

electrical engineering

MOS Capacitor Voltage and Charge

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