Related Experiment Video
Updated: Jan 8, 2026

12:18
Microwave Photonics Systems Based on Whispering-gallery-mode Resonators
Published on: August 5, 2013
17.4K
Ultracompact high-Q whispering gallery mode microresonator in a non-closed waveguide path
Optics Express
|December 19, 2025
Summary
Researchers developed an ultracompact silicon photonic resonator using an open-path design. This innovation achieves a high Q-factor in a significantly smaller footprint, enabling dense integration of photonic circuits.
Area of Science:
- Photonics and Optical Engineering
- Integrated Photonics
- Microresonator Technology
Background:
- High-performance traveling-wave optical resonators are essential for integrated photonic circuits.
- Conventional whispering-gallery mode microresonators (WGMRs) have large footprints due to their closed-loop waveguide paths.
Purpose of the Study:
- To report an ultracompact, high-loaded Q silicon photonic WGMR utilizing an open curved path.
- To demonstrate a novel approach for achieving high Q-factors in a minimized device size.
Main Methods:
- Leveraging spatial mode multiplexing and low-loss mode converter-based photonic routers.
- Implementing reentrant photon recycling within a single non-closed waveguide.
- Fabricating a silicon photonic device with an open-path design.
Main Results:
- Achieved a measured loaded Q-factor of 1.78 × 10^5 at 1554.3 nm.
- Device footprint is 0.00137 mm², significantly smaller than standard WGMRs.
- Demonstrated a 100× higher Q-factor compared to photonic crystal counterparts.
Conclusions:
- Pioneered dense integration of high-performance WGMR arrays through open-path mode recirculation.
- The ultracompact WGMR offers a pathway to miniaturized and high-performance photonic integrated circuits.
- This open-path approach overcomes the size limitations of conventional WGMRs.
Related Concept Videos
Standing Waves in a Cavity
1.4K
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:
1.4K
Sound Waves: Resonance
3.2K
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...
3.2K

