Doing the Bump: Generating Precise Wavelengths of Visible Laser Light

“In our previous experiments, we reached the general range of a wavelength of interest, but for many applications that isn’t good enough. You really have to nail the wavelength to a high degree of accuracy,” says Stone. “We now achieve this accuracy by incorporating a periodic arrangement of corrugations on a microring resonator.”

The technique has potential applications in precision timekeeping and quantum information science, which require highly specific wavelengths of visible laser light that cannot always be achieved with diode lasers (devices akin to LED lights) to drive atomic or solid-state systems.

As a result, researchers have had to fabricate as many as 100 of the silicon nitride microrings to be confident that at least some would have the right dimensions to generate the target wavelength. But even that laborious measure does not guarantee success.

The researchers described their work online in the Nov. 16, 2023, issue of Nature Photonics.

In their new study, the researchers designed a microring whose dimensions, without corrugations, would not have allowed the photons to resonate in the ring and produce new wavelengths because the process would not have conserved energy.

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The energy carried by two near-infrared photons must equal the sum of the energy carried by a single photon from each of the two output wavelengths. Credit: S. Kelley/NIST

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In addition, each of the input and output wavelengths must correspond to one of the resonant wavelengths permitted by the dimensions of the microring, just as the length of a tuning fork determines the one specific note at which it resonates.

Published Nov. 28, 2023, on the NIST blog.

Paper: Jordan R. Stone; Xiyuan Lu; Gregory Moille; Daron Westly; Tahmid Rahman; and Kartik Srinivasan. “Wavelength-accurate nonlinear conversion through wavenumber selectivity in photonic crystal resonators.” Nature Photonics, published online Nov. 16, 2023. DOI:

In previous experiments, NIST researcher Kartik Srinivasan and his colleagues used perfectly smooth microresonators—ring-shaped devices with a diameter about one-quarter the thickness of a human hair—to transform a single wavelength of NIR light into two other wavelengths. The resonator, small enough to fit on a microchip, can be designed so that one of the two output wavelengths falls within the spectrum of visible light. The transformation occurs when the NIR laser light, confined to circle the ring-shaped resonator thousands of times, reaches intensities high enough to strongly interact with the resonator material.

The corrugations act like tiny mirrors, collectively reflecting back and forth visible light racing around the ring—but only for one particular wavelength. The reflections result in two identical waves traveling around the ring in opposite directions. Inside the ring, the counterpropagating waves interfere with each other to create a pattern known as a standing wave—a waveform whose peaks remain fixed at a particular point in space as the wave vibrates, like a plucked guitar string.

In research, sometimes the bumpy path proves to be the best one. By creating tiny, periodic bumps in a miniature racetrack for light, researchers at the National Institute of Standards and Technology (NIST) and their colleagues at the Joint Quantum Institute (JQI), a research partnership between the University of Maryland and NIST, have converted near-infrared (NIR) laser light into specific desired wavelengths of visible light with high accuracy and efficiency.

In theory, by choosing a particular radius, width, and height of the resonator—which determine the properties of the light that can resonate in the ring—researchers can select any among a rainbow of colors possible with the technique. In practice, however, the method, known as optical parametric oscillation (OPO), is not always precise. Even deviations as small as a few nanometers (billionths of a meter) from the specified dimensions of the microring produce visible-light colors that differ significantly from the desired output wavelength.