Related Experiment Video
Updated: Nov 26, 2025

12:18
Microwave Photonics Systems Based on Whispering-gallery-mode Resonators
Published on: August 5, 2013
17.3K
Dominant Loss Mechanisms of Whispering Gallery Mode RF-MEMS Resonators with Wide Frequency Coverage
Zeji Chen1,2,3, Qianqian Jia1,2,3, Wenli Liu1,2,3
1Institute of Semiconductors, Chinese Academy of Sciences, Beijing 100083, China.
Sensors (Basel, Switzerland)
|December 11, 2020
Summary
This study reveals dominant energy loss mechanisms in whispering gallery mode (WGM) resonators. Squeezed film damping is key in air, while Akhiezer damping and anchor loss dominate in vacuum, enhancing resonator performance.
Area of Science:
- Physics
- Materials Science
- Acoustics
Background:
- Whispering gallery mode (WGM) resonators are crucial for sensitive measurements.
- Understanding energy dissipation is vital for optimizing WGM resonator performance.
Purpose of the Study:
- To investigate dominant energy dissipation mechanisms in multi-frequency WGM resonators.
- To provide insights into the loss mechanisms affecting device performance.
Main Methods:
- Developed theoretical models for various loss sources.
- Experimentally validated theoretical predictions.
- Analyzed loss mechanisms under atmospheric and vacuum conditions.
Main Results:
- Squeezed film damping (SFD) identified as a major loss in air for all WGMs.
- In vacuum, frequency-dependent Akhiezer damping (AKE) significantly impacts different modes.
- For low-order WGMs, anchor loss dominates; for high-order modes, AKE is the primary factor limiting Q values.
Conclusions:
- Achieved substantial Q enhancements (over four times).
- Demonstrated an excellent figure of merit (f × Q product) up to 6.36 × 10^13 at 7 K.
- Established a framework for understanding and mitigating losses in WGM resonators.
Related Concept Videos
Characteristics of Series Resonant Circuit
401
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:
401
Standing Waves in a Cavity
1.3K
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:
1.3K
Parallel Resonance
380
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:
380
Design Example: Underdamped Parallel RLC Circuit
503
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...
Starting with a fixed...
503
Sound Waves: Resonance
2.9K
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...
2.9K
Resonance in an AC Circuit
2.3K
The property of an inductor makes it resist any change in the current passing through it, while the property of a capacitor is to build up the charge across its terminals. Hence, if an inductor and capacitor are connected in series, they have opposite effects on the relative phase between current and voltage. The current through the circuit undergoes forced oscillation at the frequency of the source. The resistance term in an R-L-C circuit acts as a damping term because power is dissipated...
2.3K

