Yong Yang
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Yong Yang has a total of 98 co-authors. Here are the top co-authors by number of shared publications:
- Síle Nic Chormaic
Okinawa Institute of Science and Technology Graduate University
27 shared publications Jonathan M. Ward
Okinawa Institute of Science and Technology Graduate University
16 shared publicationsGuang-Can Guo
Key Lab of Quantum Information , University of Science and Technology of China, Hefei, China
11 shared publicationsJonathan Ward
Light-Matter Interactions Unit Okinawa Institute of Science and Technology Graduate University 904-0495 Onna Okinawa Japan
11 shared publications- Yun-Feng Xiao
Peking University
9 shared publications - Ramgopal Madugani
Okinawa Institute of Science and Technology Graduate University
8 shared publications
Latest Publications
- 9 July 2026
- Published by Elsevier in Measurement
- Vol. 287
Experimental study on the coupling performance between long-gauge ultra-weak FBG array strain sensing cable and soil
- 9 July 2026
- Published by Elsevier in Measurement
- Vol. 287
Experimental study on the coupling performance between long-gauge ultra-weak FBG array strain sensing cable and soil
- Open Access
- 1 July 2026
- Published by AIP Publishing in APL Photonics
- Vol. 11 (7)
Optomechanical interactions in a coupled whispering gallery Microbubble–Micropendulum system
In this work, we theoretically and experimentally investigate the optomechanical transduction mechanism in a system of two coupled microresonators under different coupling scenarios, categorized into electromagnetically induced transparency, intermediate, and Autler–Townes splitting regimes. We show that interference between the dispersion and dissipation channels gives rise to an asymmetric line shape in the optomechanical spectrum. These effects are experimentally demonstrated using a fiber taper-coupled whispering gallery resonator system consisting of a microbubble resonator and a micropendulum. Finally, we conduct a comprehensive analysis of the optical forces between the microbubble and the micropendulum and propose that an experimentally feasible trapping scheme is achievable, even in the presence of strong optomechanical interference.
- 1 July 2026
- Published by AIP Publishing in APL Photonics
- Vol. 11 (7)
Open AccessOptomechanical interactions in a coupled whispering gallery Microbubble–Micropendulum system
In this work, we theoretically and experimentally investigate the optomechanical transduction mechanism in a system of two coupled microresonators under different coupling scenarios, categorized into electromagnetically induced transparency, intermediate, and Autler–Townes splitting regimes. We show that interference between the dispersion and dissipation channels gives rise to an asymmetric line shape in the optomechanical spectrum. These effects are experimentally demonstrated using a fiber taper-coupled whispering gallery resonator system consisting of a microbubble resonator and a micropendulum. Finally, we conduct a comprehensive analysis of the optical forces between the microbubble and the micropendulum and propose that an experimentally feasible trapping scheme is achievable, even in the presence of strong optomechanical interference.
- 10 November 2020
- Published by Institute of Electrical and Electronics Engineers (IEEE) in Journal of Lightwave Technology
- Vol. 39 (5) , 1509-1514
A Fabry–Perot Interferometer With Asymmetrical Tapered-Fiber for Improving Strain Sensitivity
An effective method, reducing the material volume of the air cavity by asymmetrical tapering fiber, is demonstrated to enhance the sensitivity of the strain sensor dramatically. High-sensitive strain sensors are fabricated through this method that splicing and tapering fiber with arc discharge at the misaligned center of the air cavity. The strain sensitivity of the sensor is measured to be ~ 41.81 pm/μ at a resonant wavelength ~ 1560 nm ranging from 0 to 500. In addition, the experimental results show that the asymmetrical tapered-fiber enables both the material volume to smaller and the wall thickness to thinner, resulting in strain sensitivity higher. The proposed sensors have the advantages of fabricated repeatability, high sensitivity, and compact size, benefiting its practical sensing applications.
- 10 November 2020
- Published by Institute of Electrical and Electronics Engineers (IEEE) in Journal of Lightwave Technology
- Vol. 39 (5) , 1509-1514
A Fabry–Perot Interferometer With Asymmetrical Tapered-Fiber for Improving Strain Sensitivity
An effective method, reducing the material volume of the air cavity by asymmetrical tapering fiber, is demonstrated to enhance the sensitivity of the strain sensor dramatically. High-sensitive strain sensors are fabricated through this method that splicing and tapering fiber with arc discharge at the misaligned center of the air cavity. The strain sensitivity of the sensor is measured to be ~ 41.81 pm/μ at a resonant wavelength ~ 1560 nm ranging from 0 to 500. In addition, the experimental results show that the asymmetrical tapered-fiber enables both the material volume to smaller and the wall thickness to thinner, resulting in strain sensitivity higher. The proposed sensors have the advantages of fabricated repeatability, high sensitivity, and compact size, benefiting its practical sensing applications.
- Open Access
- 3 January 2018
- Published by Springer Nature
- p. 629-646
Cavity Ring-Up Spectroscopy for Dissipative and Dispersive Sensing in a Whispering Gallery Mode Resonator
In whispering gallery mode resonator sensing applications, the conventional way to detect a change in the parameter to be measured is by observing the steady-state transmission spectrum through the coupling waveguide. Alternatively, sensing based on cavity ring-up spectroscopy, i.e. CRUS, can be achieved transiently. In this work, we investigate CRUS using coupled mode equations and find analytical solutions with a large spectral broadening approximation of the input pulse. The relationships between the frequency detuning, coupling gap and ring-up peak height are determined and experimentally verified using an ultrahigh Q-factor silica microsphere. This work shows that distinctive dispersive and dissipative transient sensing can be realised by simply measuring the peak height of the CRUS signal, which may improve the data collection rate.
- 3 January 2018
- Published by Springer Nature
- p. 629-646
Open AccessCavity Ring-Up Spectroscopy for Dissipative and Dispersive Sensing in a Whispering Gallery Mode Resonator
In whispering gallery mode resonator sensing applications, the conventional way to detect a change in the parameter to be measured is by observing the steady-state transmission spectrum through the coupling waveguide. Alternatively, sensing based on cavity ring-up spectroscopy, i.e. CRUS, can be achieved transiently. In this work, we investigate CRUS using coupled mode equations and find analytical solutions with a large spectral broadening approximation of the input pulse. The relationships between the frequency detuning, coupling gap and ring-up peak height are determined and experimentally verified using an ultrahigh Q-factor silica microsphere. This work shows that distinctive dispersive and dissipative transient sensing can be realised by simply measuring the peak height of the CRUS signal, which may improve the data collection rate.
- Open Access
- 18 January 2017
- Published by Optica Publishing Group in Optics Express
- Vol. 25 (2) , 1308-1313
Tunable erbium-doped microbubble laser fabricated by sol-gel coating
In this work, we show that the application of a sol-gel coating renders a microbubble whispering gallery resonator into an active device. During the fabrication of the resonator, a thin layer of erbium-doped sol-gel is applied to a tapered microcapillary, then a microbubble with a wall thickness of 1.3 μm is formed with the rare earth ions diffused into its wall. The doped microbubble is pumped at 980 nm and lases in the emission band of the Er3+ ions at 1535 nm. The laser wavelength can be shifted by aerostatic pressure tuning of the whispering gallery modes of the microbubble. Up to 240 pm tuning is observed with 2 bar of applied pressure. We also show that the doped microbubble could be used as a compact, tunable laser source.
- 18 January 2017
- Published by Optica Publishing Group in Optics Express
- Vol. 25 (2) , 1308-1313
Open AccessTunable erbium-doped microbubble laser fabricated by sol-gel coating
In this work, we show that the application of a sol-gel coating renders a microbubble whispering gallery resonator into an active device. During the fabrication of the resonator, a thin layer of erbium-doped sol-gel is applied to a tapered microcapillary, then a microbubble with a wall thickness of 1.3 μm is formed with the rare earth ions diffused into its wall. The doped microbubble is pumped at 980 nm and lases in the emission band of the Er3+ ions at 1535 nm. The laser wavelength can be shifted by aerostatic pressure tuning of the whispering gallery modes of the microbubble. Up to 240 pm tuning is observed with 2 bar of applied pressure. We also show that the doped microbubble could be used as a compact, tunable laser source.
- Open Access
- 26 November 2016
- Published by Springer Nature in Applied Physics B
- Vol. 122 (12) , 1-10
Cavity ring-up spectroscopy for dissipative and dispersive sensing in a whispering gallery mode resonator
- 26 November 2016
- Published by Springer Nature in Applied Physics B
- Vol. 122 (12) , 1-10
Open AccessCavity ring-up spectroscopy for dissipative and dispersive sensing in a whispering gallery mode resonator
- 9 November 2016
- Published by Optica Publishing Group in Optics Letters
- Vol. 41 (22) , 5266-5269
Four-wave mixing parametric oscillation and frequency comb generation at visible wavelengths in a silica microbubble resonator
Frequency comb generation in microresonators at visible wavelengths has found applications in a variety of areas such as metrology, sensing, and imaging. To achieve Kerr combs based on four-wave mixing in a microresonator, dispersion must be in the anomalous regime. In this Letter, we demonstrate dispersion engineering in a microbubble resonator (MBR) fabricated by a two- laser beam technique. By decreasing the wall thickness of the MBR to 1.4 μm, the zero dispersion wavelength shifts to values shorter than 764 nm, making phase matching possible around 765 nm. With the optical -factor of the MBR modes being greater than , four-wave mixing is observed at 765 nm for a pump power of 3 mW. By increasing the pump power, parametric oscillation is achieved, and a frequency comb with 14 comb lines is generated at visible wavelengths.- 9 November 2016
- Published by Optica Publishing Group in Optics Letters
- Vol. 41 (22) , 5266-5269
Four-wave mixing parametric oscillation and frequency comb generation at visible wavelengths in a silica microbubble resonator
Frequency comb generation in microresonators at visible wavelengths has found applications in a variety of areas such as metrology, sensing, and imaging. To achieve Kerr combs based on four-wave mixing in a microresonator, dispersion must be in the anomalous regime. In this Letter, we demonstrate dispersion engineering in a microbubble resonator (MBR) fabricated by a two- laser beam technique. By decreasing the wall thickness of the MBR to 1.4 μm, the zero dispersion wavelength shifts to values shorter than 764 nm, making phase matching possible around 765 nm. With the optical -factor of the MBR modes being greater than , four-wave mixing is observed at 765 nm for a pump power of 3 mW. By increasing the pump power, parametric oscillation is achieved, and a frequency comb with 14 comb lines is generated at visible wavelengths.- Open Access
Tunable erbium-doped microbubble laser fabricated by sol-gel coating
In this work, we show that the application of a sol-gel coating renders a microbubble whispering gallery resonator into an active device. During the fabrication of the resonator, a thin layer of erbium-doped sol-gel is applied to a tapered microcapillary, then a microbubble with a wall thickness of 1.3 $\mu$m is formed with the rare earth diffused into its walls. The doped microbubble is pumped at 980 nm and lasing in the emission band of the Er$^{3+}$ ions with a wavelength of 1535 nm is observed. The laser wavelength can be tuned by aerostatic pressure tuning of the whispering gallery modes of the microbubble. Up to 240 pm tuning is observed with 2 bar of applied pressure. It is shown that the doped microbubble could be used as a compact, tunable laser source. The lasing microbubble can also be used to improve sensing capabilities in optofluidic sensing applications.Open AccessTunable erbium-doped microbubble laser fabricated by sol-gel coating
In this work, we show that the application of a sol-gel coating renders a microbubble whispering gallery resonator into an active device. During the fabrication of the resonator, a thin layer of erbium-doped sol-gel is applied to a tapered microcapillary, then a microbubble with a wall thickness of 1.3 $\mu$m is formed with the rare earth diffused into its walls. The doped microbubble is pumped at 980 nm and lasing in the emission band of the Er$^{3+}$ ions with a wavelength of 1535 nm is observed. The laser wavelength can be tuned by aerostatic pressure tuning of the whispering gallery modes of the microbubble. Up to 240 pm tuning is observed with 2 bar of applied pressure. It is shown that the doped microbubble could be used as a compact, tunable laser source. The lasing microbubble can also be used to improve sensing capabilities in optofluidic sensing applications. - 18 July 2016
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Photonics Technology Letters
- Vol. 28 (20) , 2277-2280
Packaged Optical Add-Drop Filter Based on an Optical Microfiber Coupler and a Microsphere
In this letter, a packaged add-drop filter composed of a silica microsphere resonator with a diameter of $80~\mu \text{m}$ and an optical microfiber coupler with a waist diameter of 1 $\mu \text{m}$ is investigated. A one-step fabrication process using UV curable epoxy is shown to stabilize the coupling between the microsphere and the microfiber coupler, which is used for the add and drop ports. The packaged microsphere-microfiber coupler device has a high $Q$ -factor of $1\times 10^{7}$ in the add–drop filter configuration. This device has excellent features, such as improved ease of fabrication, multiple resonant peaks, and high mechanical stability.
- 18 July 2016
- Published by Institute of Electrical and Electronics Engineers (IEEE) in IEEE Photonics Technology Letters
- Vol. 28 (20) , 2277-2280
Packaged Optical Add-Drop Filter Based on an Optical Microfiber Coupler and a Microsphere
In this letter, a packaged add-drop filter composed of a silica microsphere resonator with a diameter of $80~\mu \text{m}$ and an optical microfiber coupler with a waist diameter of 1 $\mu \text{m}$ is investigated. A one-step fabrication process using UV curable epoxy is shown to stabilize the coupling between the microsphere and the microfiber coupler, which is used for the add and drop ports. The packaged microsphere-microfiber coupler device has a high $Q$ -factor of $1\times 10^{7}$ in the add–drop filter configuration. This device has excellent features, such as improved ease of fabrication, multiple resonant peaks, and high mechanical stability.
- Open Access
Cavity ring-up spectroscopy for dissipative and dispersive sensing in a whispering gallery mode resonator
In whispering gallery mode resonator sensing applications, the conventional way to detect a change in the parameter to be measured is by observing the steady state transmission spectrum through the coupling waveguide. Alternatively, cavity ring-up spectroscopy (CRUS) sensing can be achieved transiently. In this work, we investigate CRUS using coupled mode equations and find analytical solutions with a large spectral broadening approximation of the input pulse. The relationships between the frequency detuning, coupling gap and ring-up peak height are determined and experimentally verified using an ultrahigh \textit{Q}-factor silica microsphere. This work shows that distinctive dispersive and dissipative transient sensing can be realised by simply measuring the peak height of the CRUS signal, which might improve the data collection rate.
Open AccessCavity ring-up spectroscopy for dissipative and dispersive sensing in a whispering gallery mode resonator
In whispering gallery mode resonator sensing applications, the conventional way to detect a change in the parameter to be measured is by observing the steady state transmission spectrum through the coupling waveguide. Alternatively, cavity ring-up spectroscopy (CRUS) sensing can be achieved transiently. In this work, we investigate CRUS using coupled mode equations and find analytical solutions with a large spectral broadening approximation of the input pulse. The relationships between the frequency detuning, coupling gap and ring-up peak height are determined and experimentally verified using an ultrahigh \textit{Q}-factor silica microsphere. This work shows that distinctive dispersive and dissipative transient sensing can be realised by simply measuring the peak height of the CRUS signal, which might improve the data collection rate.