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Light output values take the emission lines of the mercury arc lamp, filter sets, and dye absorbance and emission spectra into account to determine the light output of particular fluorophores given a particular optical configuration.
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The experimental device consisted of an illumination source or xenon lamp filtered with an ultraviolet and an infrared filter.
Infrared fluorescence (IRF) requires illumination in the visible range only, which can be implemented with a white light LED lamp filtered with the X-Nite CC1 filter to cut off emission in the near-IR.
Current-voltage characteristics of solar cells were measured under illumination of white light (100 mW cm−2) from a Hg-Xe lamp filtered by a Newport 81094 Air Mass Filter, using a Gwinstek SFG-1023 source meter.
A μSL system for tissue engineering was developed using a Digital Micromirror Device (DMD™) for dynamic pattern generation and an ultraviolet (UV) lamp filtered at 365 nm for crosslinking the photoreactive polymer solution.
Photoconversion of mKO was performed by illuminating the sample for 10s with light from a 100 W Hg lamp filtered by a 436/20 nm filter.
We tested the constructs for UV-induced photochromism by subjecting cells to brief flashes of UV from a Mercury arc lamp, filtered through a Dapi filter cube (Figure 6).
This can be thought of as the emission of an idealised xenon arc lamp, filtered to produce a square cut-off, as is commonly used in traditional colorimetric studies.
The reaction mixture was exposed to light (50 W mercury arc lamp filtered via 5 cm H2O and a 400 nm UV blocking filter) for 1 sec, and quenched in the dark with 89 mM DTT before ultrafiltration (10 kDa filter) and dilution with H2O.
Excitation was generated with an X-Ford metal halide lamp filtered with a fluo-4 filter cube.
Light stimuli were delivered using a Leica EL6000 mercury lamp filtered for ChR2 or NpHR excitation using a Leica GFP2 or ET DSR filter, respectively.
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