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Furthermore, the powers of the exciting lasers should be adjusted such that the red brightness is larger than the green brightness.
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The cross-talk correction scheme was validated herein by experiment only on a system with single, well-defined red and green brightnesses.
If dyes, filters, and laser intensities allow working with a favorable red-to-green brightness ratio of, then a maximum green-to-red particle number ratio of =10 will be permissible in the titration experiment.
Equation (34) shows that increasing the red-to-green brightness ratio by increasing the laser power for the red dye and decreasing the laser power for the green dye offers a way of increasing the maximum permissible green-to red particle number ratio in an experiment.
Obviously, the high brightness green light further confirmed the high quality of InGaN/GaN MQW green LEDs optimized by 405-nm light beam in situ monitoring system.
Since rods are generally more sensitive to blue light, and LWS cones are more sensitive to green light, the brightness contrasts between blue and green in the present experiment differed for scotopic and photopic vision.
The red and green luminance was adjusted psychophysically by brightness matching in a pilot study, to appear isoluminant with respect to each other.
Nevertheless, to confirm that their choice was based on assessments of brightness, we replaced the green light with a (4×) dimmer red light.
This contribution is mostly about phenomenology of what we see in space time evolution of coronal green line brightness (CGLB), including its cyclic variations.
Spectral variation analysis (SVAN) was applied to our own database of the coronal green line brightness (CGLB) covering almost six solar cycles (1939 2001).
The pattern of emission coronal green line brightness (Fe XIV 530.3 nm) has been used as a tracer to determine differential rotation of the solar corona.
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