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Both the saturation current density (J0) and the ideality factor (n) were extracted by fitting the dark J-V curves at intermediate voltages (approximately 0.4 to 0.5 V) using a diode equation J = J0exp qV / nkT), where q is the electron charge, T is the temperature, and k is the Boltzmann constant [21].
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The prepared emitter generates very high current density of ∼11.2 A/cm2 when measured using a diode configuration.
Infrared reflectance images were generated using a diode laser at 830 nm.
Phalloidin was imaged by using a diode laser at 405 nm also mounted on the microscope.
The absorbance was measured using a diode array detector at 286 nm.
DyLight 488 was excited using an argon laser (488 nm), and DAPI was excited using a diode laser (405 nm).
The devices were characterized under AM 1.5 conditions and the I V curves were fitted using a two diode equation.
Sugars were detected by indirect UV detection using a diode-array detector.
Spectra were obtained using a diode-array spectrophotometer for both standard and kinetics measurements.
UV visible spectra were measured using a diode-array Agilent 89090A spectrophotometer.
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