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

לקבלי MOS שלוש שכבות: השכבה התחתונה היא מצע מוליך למחצה, האמצעית היא שכבת בידוד, ושכבת המתכת העליונה היא אלקטרודת השער, השולטת במתח הקבל.
במתח שער אפס, לא זורם זרם והקבל אינו טעון.
הפעלת מתח שלילי בשער מושכת חורים לפני השטח של המוליך למחצה, ויוצרת אזור הצטברות. המכשיר מתנהג כמו קבל קונבנציונאלי.
בהפעלת מתח חיובי, חורים נדחים חזרה לתוך המצע, ויוצרים אזור מטען חלל הנקרא אזור הדלדול, הפועל כקיבול נוסף בסדרה.
עם מתח גבוה מספיק, ריכוז האלקטרונים על פני השטח עולה, ויוצר שכבת היפוך ומקטין עוד יותר את הקיבול. התוצאה היא עלייה חדה בזרם.
הסרת המתח מפזרת את המטען המצטבר, גורמת לערוץ להיעלם ומכבה את המכשיר.
קבלי MOS משמשים בהתקני זיכרון כמו DRAM, שבהם כתיבת נתונים כרוכה בהפעלת מתח שער כדי ליצור שכבת היפוך, המאחסנת טעינה באופן זמני. נוכחותו או היעדרו של מטען זה מייצג נתונים בינאריים, הזקוקים לרענון תקופתי בשל אופיו הארעי.

קבל mos

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קבל מתכת-תחמוצת-חצי מוליך (MOS) הוא מבנה בסיסי בשימוש נרחב בטכנולוגיית התקן מוליכים למחצה, במיוחד בייצור של מעגלים משולבים ו-MOSFET (טרנזיסטורי אפקט שדה של מתכת-תחמוצת-מוליכים למחצה). קבל MOS מורכב משלוש שכבות: שער מתכת, תחמוצת די-אלקטרית ומצע מוליכים למחצה.


שער המתכת עשוי בדרך כלל מחומרים מוליכים מאוד כגון אלומיניום או פוליסיליקון. מתחת לשער המתכת מונחת שכבה דקה של תחמוצת בידוד, בדרך כלל צורן דו-חמצני (SiO₂), שהיא הדי-אלקטרית. מצע המוליך למחצה הוא בדרך כלל סיליקון, שיכול להיות מסוג p או מסוג n.


כאשר מתח מופעל על שער המתכת, הוא משפיע על חלוקת הספקים החשמליים במוליך למחצה. פסי האנרגיה של המוליך למחצה שטוחים במתח מופעל אפס, מה שמצביע על מטען עודף בתוך התחמוצת או במשטח המוליך למחצה. כאשר מתח השער גדל באופן חיובי, הוא מושך אלקטרונים לעבר הממשק של התחמוצת והמוליך למחצה. זה יוצר הצטברות אלקטרונים בסיליקון מסוג n ודלדול של חורים בסיליקון מסוג p, היוצרים את שכבת הדלדול.


עלייה נוספת במתח מובילה להיפוך חזק, כאשר משטח מוליך למחצה מתחת לתחמוצת משנה את סוגו; לדוגמה, סוג p הופך לסוג n, מכיוון שהאלקטרונים הופכים לנשאי הרוב. שכבת היפוך זו היא קריטית בפעולת MOSFETs. הקיבול של מבנה MOS משתנה עם המתח המופעל על השער.


שכבת ההיפוך חיונית לתפקוד של קבלי MOS ב-DRAM. כתיבת נתונים כרוכה בהפעלת מתח שיוצר שכבה זו ואחסון המטען במוליך למחצה. מטען מאוחסן זה מייצג נתונים בינאריים, המאפשרים אחסון ושליפה של מידע. הסרת המתח גורמת להתפזרות המטען, לנטרול הערוץ ולשמירה על הנתונים המאוחסנים. מחזור טעינה זה הוא מרכזי בפונקציונליות ובאמינות של DRAM ביישומי מחשוב.


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קבל MOS

לקבלי MOS שלוש שכבות: השכבה התחתונה היא מצע מוליך למחצה, האמצעית היא שכבת בידוד, ושכבת המתכת העליונה היא השער ...

Education

JoVE Core

Electrical Engineering

הנדסה חשמלית

Unit 1

יחידה 1

Transistors

טרנזיסטורים

KEY TERMS AND CONCEPTS

מונחים ומושגים מרכזיים

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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