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Related Concept Videos

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:
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...
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:
Sound Waves: Resonance01:14

Sound Waves: Resonance

Resonance is produced depending on the boundary conditions imposed on a wave. Resonance can be produced in a string under tension with symmetrical boundary conditions (i.e., has a node at each end). A node is defined as a fixed point where the string does not move. The symmetrical boundary conditions result in some frequencies resonating and producing standing waves, while other frequencies interfere destructively. Sound waves can resonate in a hollow tube, and the frequencies of the sound...
Standing Electromagnetic Waves01:15

Standing Electromagnetic Waves

Electromagnetic waves can be reflected; the surface of a conductor or a dielectric can act as a reflector. As electric and magnetic fields obey the superposition principle, so do electromagnetic waves. The superposition of an incident wave and a reflected electromagnetic wave produces a standing wave analogous to the standing waves created on a stretched string.
Suppose a sheet of a perfect conductor is placed in the yz-plane, and a linearly polarized electromagnetic wave traveling in the...
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

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Fabrication and Characterization of Superconducting Resonators
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Published on: May 21, 2016

Planar resonator and integrated oscillator using magnetostatic waves.

Y Kinoshita1, S Kubota, S Takeda

  • 1Hitachi Ltd., Tokyo.

IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control
|January 1, 1990
PubMed
Summary

Researchers developed a tunable magnetostatic wave (MSW) resonator on YIG/GGG substrates. This device enables a compact, high-performance microwave oscillator with spectral purity comparable to YIG sphere technology.

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Area of Science:

  • * Condensed matter physics
  • * Microwave engineering
  • * Materials science

Background:

  • * Magnetostatic waves (MSWs) offer unique properties for microwave devices.
  • * Yttrium-iron-garnet (YIG) films on Gadolinium-Gallium-Garnet (GGG) substrates are suitable for MSW applications.
  • * Development of compact and tunable microwave oscillators remains a key challenge.

Purpose of the Study:

  • * To design and fabricate a planar magnetostatic wave resonator.
  • * To characterize the resonator's performance, including filter response and Q-factor.
  • * To demonstrate a tunable microwave oscillator utilizing the developed resonator.

Main Methods:

  • * Fabrication of a planar MSW resonator on a YIG/GGG substrate using aluminum finger electrodes.
  • * Integration of the resonator with a silicon bipolar transistor on a ceramic substrate.
  • * Characterization of the resonator's notch filter response and the oscillator's frequency tunability and spectral purity.

Main Results:

  • * A tunable MSW resonator chip (2 mmx5 mm) was successfully realized.
  • * The resonator exhibited a deep notch filter response (20-35 dB) and a high loaded Q (up to 2000).
  • * A tunable microwave oscillator (8 cm³) operating at 3 GHz with high spectral purity was demonstrated.

Conclusions:

  • * The planar MSW resonator shows promise for compact microwave oscillator applications.
  • * Achieved performance metrics are comparable to established YIG sphere technology.
  • * Further improvements are needed for practical oscillator implementation.