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

Les condensateurs MOS ont trois couches : la couche inférieure est un substrat semi-conducteur, la couche intermédiaire est une couche isolante et la couche métallique supérieure est l'électrode de grille, qui contrôle la tension du condensateur.
À une tension de grille nulle, aucun courant ne circule et le condensateur n’est pas chargé.
L'application d'une tension négative au niveau de la grille attire des trous à la surface du semi-conducteur, formant une zone d'accumulation. L’appareil se comporte comme un condensateur conventionnel.
En appliquant une tension positive, les trous sont repoussés dans le substrat, établissant une région de charge spatiale appelée région d’appauvrissement, qui agit comme une autre capacité en série.
Avec une tension suffisamment élevée, la concentration d’électrons à la surface augmente, formant une couche d’inversion et diminuant encore la capacité. Il en résulte une forte augmentation du courant.
La suppression de la tension dissipe la charge accumulée, fait disparaître le canal et éteint l’appareil.
Les condensateurs MOS sont utilisés dans les dispositifs de mémoire comme la DRAM, où l’écriture des données implique l’application d’une tension de grille pour créer une couche d’inversion, qui stocke temporairement la charge. La présence ou l’absence de cette charge représente des données binaires, qui nécessitent une actualisation périodique en raison de leur nature transitoire.

condensateur mos

Un condensateur métal-oxyde-semiconducteur (MOS) est une structure fondamentale largement utilisée dans la technologie des dispositifs à semi-conducteurs, en particulier dans la fabrication de circuits intégrés et de MOSFET (transistors à effet de champ métal-oxyde-semiconducteur). Le condensateur MOS se compose de trois couches : une grille métallique, un oxyde diélectrique et un substrat semi-conducteur.

La grille métallique est généralement fabriquée à partir de matériaux hautement conducteurs tels que l'aluminium ou le polysilicium. Sous la grille métallique se trouve une fine couche d'oxyde isolant, généralement du dioxyde de silicium (SiO₂), qui constitue le diélectrique. Le substrat semi-conducteur est généralement du silicium, qui peut être de type p ou de type n.

Lorsqu’une tension est appliquée à la grille métallique, elle influence la répartition des porteurs électriques dans le semi-conducteur. Les bandes d'énergie du semi-conducteur sont plates à tension appliquée nulle, ce qui indique l'absence de charge excessive à l'intérieur de l'oxyde ou à la surface du semi-conducteur. Lorsque la tension de grille augmente positivement, elle attire les électrons vers l’interface de l’oxyde et du semi-conducteur. Cela crée une accumulation d’électrons dans le silicium de type n et une diminution des trous dans le silicium de type p, formant ainsi la couche d’appauvrissement.

Une nouvelle augmentation de la tension conduit à une forte inversion, où la surface semi-conductrice située sous l'oxyde change de type ; par exemple, un type p devient un type n, à mesure que les électrons deviennent les porteurs majoritaires. Cette couche d'inversion est essentielle au fonctionnement des MOSFET. La capacité de la structure MOS varie en fonction de la tension appliquée à la grille.

La couche d'inversion est cruciale pour le fonctionnement des condensateurs MOS dans la DRAM. L'écriture de données consiste à appliquer une tension qui crée cette couche et à stocker la charge dans le semi-conducteur. Cette charge stockée représente des données binaires, permettant le stockage et la récupération d'informations. La suppression de la tension entraîne la dissipation de la charge, désactivant le canal et préservant les données stockées. Ce cycle de charge est essentiel à la fonctionnalité et à la fiabilité de la DRAM dans les applications informatiques.

Condensateur MOS

Les condensateurs MOS ont trois couches : la couche inférieure est un substrat semi-conducteur, la couche intermédiaire est une couche isolante et la couche métallique supérieure est la grille ...

Education

Enseignement

JoVE Core

Electrical Engineering

Génie électrique

Unit 1

Unité 1

Transistors

KEY TERMS AND CONCEPTS

TERMES ET CONCEPTS CLÉS

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

Description

Transcript

Tags