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- measuring_quantum_yield
- ple holder. * Put the sample holder into the IN-position. * Put the sample holder into the integrating s... 14-35-37.jpg?600 |}} * Select either IN or OUT position **Note:** The sample holder has two indexed positions. When in the IN position, the excitation beam will directly hit the sample, when in the OUT position the s
- pattern_matching
- composing the overall decay, it performs the decomposition on each pixel. The linear decompositions of the particular pixels give different αi's for every pixel.\\ Af
- 2ffcs
- the time trace oscilloscope optimize the pinhole position **with** Nomarski Prism and **both** lasers.
- align_beam_backreflection
- ch quadrant. To reach this, you have to precisely position the beam to enter at the center of the objective
- diamond_nv_centers
- w NV-centers (see figure 5), *select one, and position the focus on the NV-center. *use the oscillos
- how_to_measure_the_instrument_response_function_irf
- or upon changes of the excitation wavelength, the position of the IRF can shift slightly, but this is accoun
- how_to_work_with_the_instrument_response_function_irf
- power of the laser changes the shape and temporal position of the laser pulse. ((You can use the driver sett
- intensity_time_trace_analysis
- return from the end of the line to the line start position is done with highest possible speed. In contrast,
- select_the_correct_pinhole_size
- ger than the image of the [[wp>Airy Disc]] at the position of the pinhole: $$d_{Airy} = (1.22 * lambda / N.
- using_the_antibunching_script
- lly moves the red and yellow curve to the correct position. Press "Calculate" again to recalculate the corre