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The contrary photocurrent responses of the TiO2 nanostructures under ultraviolet and visible light were measured.
The guiding modes and the near-field intensity distribution of the light were measured by the prism-coupling method and the end-facing coupling arrangement separately.
The spectra of specular reflection of p- and s-polarized light were measured at near-normal incidence of light (approximately 10°) on GaAs surface over the range of GaAs fundamental photosensitivity (0.4 to 0.9 μm).
The irradiances of UVA light were measured with a calibrated UVA-meter (type No. 37, Dr. Hönle) prior to each experiment.
Dark adapted pupil area prior to light pulse and pupil area after 30 sec of light were measured and pupil constriction was defined as 1- dark adapted pupil width)̂2/(pupil width after 30 sec of light)̂2.
In the same experiments, action spectra during chromatic adaptation to 551 nm or 656 nm background light were measured for test flashes of 365 nm, 452 nm, 500 nm, 520 nm, 550 nm, 604 nm, and 649 nm.
Similar(51)
Rate measurements under light are measured after the measurements in the dark.
Raman measurements had a maximum acquisition time of 50 seconds, while excitation light was measured for 5 seconds.
Light is measured in lumens, but this is too complicated to work out every time you buy a bulb.
The scattered light was measured at an angle of 173°.
The light was measured to approximately 17 lux in front of the monitor.
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