1. Optics-Integrated Microfluidic Platforms for Biomolecular Analyses
Kathleen E. Bates, Hang Lu 
Biophysical Journal 
Volume 110, Issue 8, Pages (April 2016)
DOI: /j.bpj
Copyright © 2016 Biophysical Society Terms and Conditions

2. Figure 1
Physical configuration of variable focus lenses. (A) Pneumatically tuned lens. (B) Lens controlled by electrowetting. (C) Hydrodynamic lens. (D) Environmentally responsive lens. Dashed lines indicate approximate limits of physical tunability. ITO, indium tin oxide. To see this figure in color, go online.
Biophysical Journal  , DOI: ( /j.bpj )
Copyright © 2016 Biophysical Society Terms and Conditions

3. Figure 2
Single influenza virus particle detection. (A) The incorporation of both solid-core (orange) and liquid-core (blue) ARROW waveguides allow small volume optical excitation of fluorescent virus particles, whereas virus particle transversal of a nanopore results in transient drops in current. (B) Particles pass first through the nanopore, over which current changes are measured (top, black) and then through optical detection volume, where fluorescence signals from viruses (red) and nanoparticles (blue) are measured, resulting in a known dwell time. Blockade depths from both types of particles are very similar, but variable dwell times allow them to be distinguished. The incorporation of both optical and electrical detectors enables the separation of single viruses from a mixture of nanobeads and viruses (81). This is an unofficial adaptation of an article that appeared in an ACS publication. ACS has not endorsed the content of this adaptation or the context of its use. To see this figure in color, go online.
Biophysical Journal  , DOI: ( /j.bpj )
Copyright © 2016 Biophysical Society Terms and Conditions

4. Figure 3
Principle of WGM sensors. Light from a laser (red) is evanescently coupled into the dielectric toroid, sphere, cylinder, ring, or disk via a light guide, such as a tapered optical fiber. The wavelength of the laser is tuned so that the light traveling around the surface of the WGM remains in phase when it returns back to the point of coupling. As the resonant wavelength is approached, power is extracted from the fiber, decreasing the amount of light transmitted to the detector. When analytes (orange) are bound to the sensing surface through antibodies (green), the resonant wavelength of the system shifts due to local changes in the index of refraction. Resonance shifts down to 6 fm can be detected with appropriate detectors (90). To see this figure in color, go online.
Biophysical Journal  , DOI: ( /j.bpj )
Copyright © 2016 Biophysical Society Terms and Conditions

5. Figure 4
Optofluidic human blood immunoanalysis. (A) Schematic of optofluidic device. (B) System functional states during optofluidic ELISA. (C) Scanning electron microscopy image of cells conjugated to microbeads trapped by micropillar array in the microfluidic chamber. (D) Representative readout from LSPR experiment (141). This is an unofficial adaptation of an article that appeared in an ACS publication. ACS has not endorsed the content of this adaptation or the context of its use. To see this figure in color, go online.
Biophysical Journal  , DOI: ( /j.bpj )
Copyright © 2016 Biophysical Society Terms and Conditions