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Related Concept Videos

Oscillations In An LC Circuit01:30

Oscillations In An LC Circuit

An idealized LC circuit of zero resistance can oscillate without any source of emf by shifting the energy stored in the circuit between the electric and magnetic fields. In such an LC circuit, if the capacitor contains a charge q before the switch is closed, then all the energy of the circuit is initially stored in the electric field of the capacitor. This energy is given by
Cascaded Op Amps01:16

Cascaded Op Amps

Operational amplifiers (op-amps) are versatile electronic components that can be interconnected in a cascade - one after another in a linear sequence. This cascading is possible due to their infinite input resistance and zero output resistance, allowing them to maintain their input-output relationships even when connected in series.
In a cascaded system, each op-amp is referred to as a stage. The output of one stage drives the input of the subsequent stage. As the input signal passes through...
RLC Circuit as a Damped Oscillator01:30

RLC Circuit as a Damped Oscillator

An RLC circuit combines a resistor, inductor, and capacitor, connected in a series or parallel combination.
Consider a series RLC circuit. Here, the presence of resistance in the circuit leads to energy loss due to joule heating in the resistance. Therefore, the total electromagnetic energy in the circuit is no longer constant and decreases with time. Since the magnitude of charge, current, and potential difference continuously decreases, their oscillations are said to be damped. This is...
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...
Biasing of Metal-Semiconductor Junctions01:27

Biasing of Metal-Semiconductor Junctions

Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
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...

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Related Experiment Video

Updated: Jun 19, 2026

Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators
09:23

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Published on: May 30, 2014

Copper-laser oscillator with adjoint-coupled self-filtering injection.

J J Chang

    Optics Letters
    |October 28, 2009
    PubMed
    Summary

    A novel laser resonator design achieves near-diffraction-limited beam quality for high-gain, short-pulse lasers. This injection-controlled system improves beam quality using self-filtering and a unique resonator configuration.

    Area of Science:

    • Optics and Photonics
    • Laser Physics
    • High-Gain Laser Systems

    Background:

    • Achieving diffraction-limited beam quality is crucial for high-gain, short-pulse lasers.
    • Traditional resonators often suffer from beam deterioration, limiting performance.
    • Advanced resonator designs are needed to overcome these limitations.

    Purpose of the Study:

    • To develop and demonstrate a new injection-controlled laser resonator.
    • To improve beam quality for high-gain, short-pulse laser applications.
    • To achieve near-diffraction-limited performance throughout the laser pulse.

    Main Methods:

    • Utilizing adjoint-coupled injection of a short-pulse laser signal.
    • Implementing self-filtering of the injected beam through prepulse cavity propagation.

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  • Employing a self-imaging unstable resonator to minimize edge-diffraction effects.
  • Main Results:

    • The developed resonator achieved a beam quality of 1.1-1.3 times diffraction limited.
    • This high beam quality was maintained throughout the entire 70-ns laser pulse.
    • The system was demonstrated on a 30-W copper-vapor laser.

    Conclusions:

    • The novel injection-controlled resonator effectively enhances beam quality.
    • This technology is suitable for high-gain, short-pulse laser systems requiring excellent beam quality.
    • The self-filtering and self-imaging unstable resonator design are key to the improved performance.