Related Experiment Video
Updated: Feb 22, 2026

12:18
Microwave Photonics Systems Based on Whispering-gallery-mode Resonators
Published on: August 5, 2013
17.6K
Self-frequency doubling in a laser-active whispering-gallery resonator
Optics Letters
|September 29, 2017
Summary
This study demonstrates combined lasing and frequency doubling in a single neodymium-doped lithium niobate whispering-gallery resonator, producing green light from a low-cost laser diode. This integrated approach offers a novel pathway for compact nonlinear optical devices.
Area of Science:
- Photonics and Optical Engineering
- Materials Science
Background:
- Whispering-gallery resonators offer high optical confinement for nonlinear processes.
- Neodymium-doped lithium niobate is a promising material for integrated optics.
Purpose of the Study:
- To demonstrate simultaneous lasing and self-frequency doubling in a single whispering-gallery resonator.
- To achieve efficient green light generation from a compact device.
Main Methods:
- Fabrication of a millimeter-sized neodymium-doped lithium niobate whispering-gallery resonator.
- Pumping the resonator with a low-cost 808-nm laser diode.
- Characterization of lasing at 1.08 μm and subsequent second-harmonic generation.
Main Results:
- Achieved stable lasing and self-frequency doubling within the same resonator.
- Generated green light via the nonlinear χ(2) process.
- Observed an electrical-optical efficiency of up to 2×10⁻⁴.
Conclusions:
- This work presents the first integration of lasing and second-harmonic generation in a single high-Q whispering-gallery resonator.
- The demonstrated approach is versatile and applicable to other materials and nonlinear optical processes.
- This offers a pathway towards compact and efficient integrated photonic devices.
Related Concept Videos
Sound Waves: Resonance
3.5K
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...
3.5K
Standing Waves in a Cavity
1.5K
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:
1.5K
Parallel Resonance
644
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:
644
Double Resonance Techniques: Overview
797
Double resonance techniques in Nuclear Magnetic Resonance (NMR) spectroscopy involve the simultaneous application of two different frequencies or radiofrequency pulses to manipulate and observe two distinct nuclear spins. One important application of double resonance is spin decoupling, which selectively suppresses coupling with one type of nucleus while observing the NMR signal from another nucleus, simplifying the spectrum and enhancing resolution.
Spin decoupling is usually achieved by...
Spin decoupling is usually achieved by...
797
Design Example: Underdamped Parallel RLC Circuit
689
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...
689
Oscillations In An LC Circuit
3.2K
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
3.2K

