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Related Concept Videos

MOSFET Amplifiers01:17

MOSFET Amplifiers

The MOSFET, when operating in its active region, functions as a voltage-controlled current source. In this region, the gate-to-source voltage controls the drain current. This principle underlies the operation of the transconductance MOSFET amplifier. The output current is directed through a load resistor to convert this amplifier into a voltage amplifier. The output voltage is then obtained by subtracting the voltage drop across the load resistance from the supply voltage. This process results...
MOSFET: Enhancement Mode01:22

MOSFET: Enhancement Mode

Enhancement-mode MOSFETs are pivotal components in electronics, distinguished by their capacity to act as highly efficient switches. They are part of the larger family of metal-oxide Semiconductor Field-Effect Transistors (MOSFETs). They are available in two types: p-channel and n-channel, each tailored to specific polarity operations.
In their basic form, enhancement-mode MOSFETs are typically non-conductive when the gate-source voltage (Vgs) is zero. This default 'off' state means no current...
MOSFET01:16

MOSFET

The Metal-Oxide-Semiconductor Field-Effect Transistor (MOSFET) plays a pivotal role in modern electronics thanks to its versatility and efficiency in controlling electrical currents. This device, also known as IGFET, MISFET, and MOSFET, has three main terminals: the Source, Drain, and Gate. MOSFETs are classified into n-channel or p-channel types based on the doping characteristics of their substrate and the source or drain regions.
In an n-MOSFET, the structure includes n-type source and drain...
Bipolar Junction Transistor01:22

Bipolar Junction Transistor

Bipolar Junction Transistors (BJTs) are essential elements in electronic circuits, playing a crucial role in the functionality of amplifiers, memories, and microprocessors. These transistors can be designed as NPN or PNP based on their doping patterns. They consist of three layers: the emitter, base, and collector. The configuration of these layers and their respective doping levels—with N-type or P-type impurities—define the transistor's type and its operational characteristics.
The structure...
Small-Signal Analysis of MOSFET Amplifiers01:23

Small-Signal Analysis of MOSFET Amplifiers

In small-signal analysis, a MOSFET transistor amplifier acts as a linear amplifier when operating in its saturation region. The gate-to-source voltage (VGS) of the MOSFET is the sum of the DC biasing voltage and the small time-varying input signal. This combination sets up the operating point and modulates the drain current (ID) that flows from the drain to the source. When a small AC signal is superimposed on the DC bias voltage at the gate, the instantaneous drain current comprises three...
Photoelectric Effect02:26

Photoelectric Effect

When light of a particular wavelength strikes a metal surface, electrons are emitted. This is called the photoelectric effect. The minimum frequency of light that can cause such emission of electrons is called the threshold frequency, which is specific to the metal. Light with a frequency lower than the threshold frequency, even if it is of high intensity, cannot initiate the emission of electrons. However, when the frequency is higher than the threshold value, the number of electrons ejected...

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Related Experiment Video

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Fabrication of Flexible Image Sensor Based on Lateral NIPIN Phototransistors
09:59

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Published on: June 23, 2018

CMOS Optoelectronic Lock-In Amplifier With Integrated Phototransistor Array.

An Hu, Vamsy P Chodavarapu

    IEEE Transactions on Biomedical Circuits and Systems
    |July 16, 2013
    PubMed
    Summary

    We developed an optoelectronic lock-in amplifier (LIA) for optical sensing. This LIA demonstrates high sensitivity and linearity, making it suitable for precise optical measurements.

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    Area of Science:

    • Optoelectronics
    • Instrumentation
    • Semiconductor device physics

    Background:

    • Optical sensing and spectroscopy require sensitive and accurate signal processing.
    • Traditional lock-in amplifiers can be bulky and expensive.
    • Integration of lock-in amplification functionality into optoelectronic systems offers miniaturization and improved performance.

    Purpose of the Study:

    • To design and develop a novel optoelectronic lock-in amplifier (LIA) for enhanced optical sensing and spectroscopy.
    • To demonstrate the feasibility of fabricating an integrated LIA using standard semiconductor technology.
    • To characterize the performance of the developed LIA in terms of sensitivity, linearity, and dynamic range.

    Main Methods:

    • Fabrication of a prototype LIA using Taiwan Semiconductor Manufacturing Co. 0.35-μm complementary metal-oxide semiconductor technology.
    • Utilization of a phototransistor array for optical-to-electrical conversion.
    • Implementation of a transimpedance amplifier, filters, and a phase-locked loop (PLL) for signal processing.
    • Testing the system with a light-emitting diode (LED) source and measuring output voltage versus optical power.

    Main Results:

    • The LIA operates effectively in the 13 kHz to 25 kHz range, optimized for 20 kHz modulation.
    • Achieved minimum dynamic reserve of 1.31 dB and sensitivity of 34 mV/μW.
    • Demonstrated good linearity in the output voltage versus incident optical power relationship.
    • The developed LIA exhibits low power consumption (12.79 mW) with a 3.3-V supply.

    Conclusions:

    • The developed optoelectronic lock-in amplifier is a viable solution for advanced optical sensing and spectroscopy.
    • The integrated design offers high sensitivity, linearity, and noise suppression.
    • The LIA's performance metrics indicate its suitability for various optical measurement applications requiring precise signal detection.