The dynamic evolution of rays in 3D geodesic lens.

The dynamic evolution of waves in 2D MFE lens.

Animation of FIg. 3

Additional file 6. KEGG and GO enrichment analysis of 452 differential proteins in our dataset.

Additional file 3. The Gaussian fitting curve of log2 ratio of the intensities of two replicates of 20/0 (A), 80/0 (B) and 160/0 (C). The red and blue curves represent the experimental and Gaussian fitting curve, respectively.

Supplemental material, sj-pptx-1-cpa-10.1177_07067437231154993 for A Meta-Research of Randomized Controlled Trials in the Field of Mental Health: Comparing Pharmacological to Non-Pharmacological Interventions from 1955 to 2020 by Sheng Chen, PhD, Alina Lee, MSc, and Wei Wang, PhD in The Canadian Journal of Psychiatry

Additional file 1. Preparation for iTRAQ quantitative proteomics study.

Additional file 4. High correlation between the two technical replicates. The scatterplot of two technical replicates treated with 20/80/160 Gy heavy ion irradiation.

Additional file 5. String analysis of 113 overlapped differential proteins in our dataset.

Trapping of a 3μm SiO2 sphere and a yeast by a double-tapered optical fiber probe. Turn on the laser source and move the probe close to a 3μm SiO2 sphere, the sphere will be attracted to the fiber tip. Then move the probe with a 3μm SiO2 sphere close to a yeast, and it will be attracted to the SiO2 sphere. When the fiber probe is moving, two microparticles will move along with it. Finally,...

When a 980 nm laser with the out power of 12.743 mW is coupled to the structure via MMF, the bubble moves down vertically and then suspends in the thick HCF. When the laser is turned off, the micro-bubble returns to the top of the thick HCF.

Animation of FIg. 3

Additional file 1. Preparation for iTRAQ quantitative proteomics study.

Additional file 3. The Gaussian fitting curve of log2 ratio of the intensities of two replicates of 20/0 (A), 80/0 (B) and 160/0 (C). The red and blue curves represent the experimental and Gaussian fitting curve, respectively.

Supplemental material, sj-pptx-1-cpa-10.1177_07067437231154993 for A Meta-Research of Randomized Controlled Trials in the Field of Mental Health: Comparing Pharmacological to Non-Pharmacological Interventions from 1955 to 2020 by Sheng Chen, PhD, Alina Lee, MSc, and Wei Wang, PhD in The Canadian Journal of Psychiatry

Trapping of a 3μm SiO2 sphere and a yeast by a double-tapered optical fiber probe. Turn on the laser source and move the probe close to a 3μm SiO2 sphere, the sphere will be attracted to the fiber tip. Then move the probe with a 3μm SiO2 sphere close to a yeast, and it will be attracted to the SiO2 sphere. When the fiber probe is moving, two microparticles will move along with it. Finally,...

After the driven power is increased to 17.570 mW, the bubble takes 1.1 s to move to the bottom of the thick HCF and subsequently stays still. When the laser is turned off, the micro-bubble returns to the top of the thick HCF after 1.0 s.

Additional file 5. String analysis of 113 overlapped differential proteins in our dataset.

Additional file 6. KEGG and GO enrichment analysis of 452 differential proteins in our dataset.

The dynamic evolution of waves in 2D MFE lens.

The dynamic evolution of rays in 3D geodesic lens.

Additional file 4. High correlation between the two technical replicates. The scatterplot of two technical replicates treated with 20/80/160 Gy heavy ion irradiation.

When a 980 nm laser with the out power of 12.743 mW is coupled to the structure via MMF, the bubble moves down vertically and then suspends in the thick HCF. When the laser is turned off, the micro-bubble returns to the top of the thick HCF.

After the driven power is increased to 17.570 mW, the bubble takes 1.1 s to move to the bottom of the thick HCF and subsequently stays still. When the laser is turned off, the micro-bubble returns to the top of the thick HCF after 1.0 s.