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The 1040 nm beam was modulated at 20 MHz using an electro-optic modulator (ThorLabs EO-AM-R-20-C2, NJwton, NJ, USA), and the modulation transfer from the 1040 nm beam to the pump beam was detected using a photodiode coupled to a lock-in amplifier (APE Lock-In Amplifier, Berlin, Germany).
The transmitted beam was detected by a photodiode detector (PD).
The PSi samples were illuminated with the tungsten source, and the reflected beam was detected with the silicon diode detector.
PSi samples were illuminated with the xenon source, and the reflected beam was detected with the silicon diode detector.
Once the beam was detected, its direction was confirmed by means of the beam spot luminance on the image monitor (not shown) that was measured with a luminance meter.
The interruption of a photocell beam was detected by a counter that recorded the total number of photocell beam interruptions.
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This second beam reflects off the object and the return, reflected beam is detected.
The probe beam is detected after being collected by an objective lens (20x, NA = 0.42) and focused to a photodiode.
Besides, the change in electrical resistance of the beam is detected under monotonic loading.
Electrons and recoil protons from neutron decay in a cold beam are detected in coincidence.
When a laser beam is detected on any one of the vest's phototransistors, the hardware circuitry generates an interrupt on the INT0 pin.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com