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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
Design Example: Underdamped Parallel RLC Circuit01:17

Design Example: Underdamped Parallel RLC Circuit

Consider designing an oscillator circuit, a crucial component in various electronic devices and systems. The objective is to create an oscillator circuit with specific characteristics: a damped natural frequency of 4 kHz and a damping factor of 4 radians per second. To accomplish this, a parallel RLC circuit is employed, known for its ability to sustain oscillations at a resonant frequency. In this case, the damping factor is pivotal in achieving the desired performance.
Starting with a fixed...
Standing Waves in a Cavity01:28

Standing Waves in a Cavity

A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
Parallel Resonance01:23

Parallel Resonance

The parallel RLC circuit is an arrangement where the resistor (R), inductor (L), and capacitor (C) are all connected to the same nodes and, as a result, share the same voltage across them. The parallel RLC circuit is analyzed in terms of admittance (Y), which reflects the ease with which current can flow. The admittance is given by:
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...
Characteristics of Series Resonant Circuit01:24

Characteristics of Series Resonant Circuit

Series resonance occurs in a circuit containing inductive (L), capacitive (C), and resistive (R) elements connected sequentially. At the resonance frequency, the inductive and capacitive reactances are equal in magnitude but opposite in sign, effectively canceling each other. This causes the circuit's impedance is minimal, primarily determined by the resistance R. The resonant frequency of an RLC circuit is defined as:

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Related Experiment Video

Updated: Jul 8, 2026

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

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

Published on: May 30, 2014

Continuous-wave, singly resonant, intracavity parametric oscillator.

F G Colville, M H Dunn, M Ebrahimzadeh

    Optics Letters
    |January 15, 1997
    PubMed
    Summary
    This summary is machine-generated.

    This study details a continuous-wave intracavity optical parametric oscillator using KTP within a Ti:sapphire laser. It achieved stable 0.4W idler output power tunable from 2.53 to 2.87 micrometers.

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    Fabrication and Characterization of High-Q Silicon Nitride Membrane Resonators

    Published on: August 8, 2025

    Area of Science:

    • Laser physics
    • Nonlinear optics
    • Quantum optics

    Background:

    • Intracavity optical parametric oscillators (OPOs) offer enhanced nonlinear conversion efficiency.
    • Ti:sapphire lasers are widely used for tunable, high-power laser generation.
    • Integrating OPOs within laser cavities presents opportunities for novel light sources.

    Purpose of the Study:

    • To characterize the performance of a continuous-wave (CW) intracavity KTP singly resonant OPO.
    • To analyze the power, tuning, spectral, and stability characteristics of the OPO system.
    • To evaluate the efficiency of frequency conversion within the Ti:sapphire laser cavity.

    Main Methods:

    • Experimental setup utilizing a KTP singly resonant OPO inside a Ti:sapphire laser cavity.
    • Steady-state model analysis for performance evaluation.
    • Measurement of internal/external powers, circulating fields, tuning ranges, spectral bandwidth, and amplitude stability.

    Main Results:

    • The nonresonant idler output tuned from 2.53 to 2.87 micrometers.
    • Maximum idler output power reached approximately 0.4W.
    • Long-term amplitude-stable operation was achieved with the OPO.

    Conclusions:

    • The intracavity OPO demonstrated efficient frequency conversion.
    • The downconverted power approached the optimum power extractable from the Ti:sapphire laser.
    • The system provides a stable, tunable source in the mid-infrared spectrum.