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These characteristics are exploited in making semiconductor lasers that produce light of any given wavelength within a considerable range.
Compared to laser scanners, cameras normally capture wavelength within the visible light, i.e. mostly what a human eye can see.
There exhibits a one-to-one correspondence between absorbance and wavelength within the range 550 to approximately 250 nm.
A low-pass filter with cut-off at 50 km wavelength within the frequency domain is used to deal with the FGAs to remove the short-wavelength fluctuation.
We observed that the peak wavelength within PL spectrum shifts from 720 to 700 nm indicating the energy bandgap of PS changes from 1.72 to 1.77 eV.
It is suggested by theoretical optical absorbance calculations that alloy ZnS0.375Se0.625 monolayer has a higher absorption performance than pristine ZnSe and ZnS monolayers under certain wavelength within the visible light region.
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Except in semiconductor lasers, cavities are thousands of wavelengths long, so the wavelengths of adjacent modes are closely spaced and usually the laser simultaneously emits light on two or more wavelengths within 0.1 percent of each other.
However, for such NP structures, light-stimulated resonance can only occur at specific wavelengths within a narrow wavelength range[1].
Thus, there is a vector of values for each pixel corresponding to different wavelengths within the sensor spectral range.
Applications include cascaded Raman lasers as well as lasers running on several wavelengths within one Stokes band.
Instead, the researchers shot in a beam of electrons to generate light of all wavelengths within the waveguide and measured the light leaking out of it.
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