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- measuring_quantum_yield
- ition **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 sample will only be illuminated indirectly (b... oving the sample holder make sure it is in the IN-Position. * Insert the blank sample into the sample hold... egrating sphere put the sample holder into the IN-position. * Select either IN or OUT position. **Note:**
- intensity_time_trace_analysis
- return from the end of the line to the line start position is done with highest possible speed. In contrast,
- diamond_nv_centers
- w NV-centers (see figure 5), *select one, and position the focus on the NV-center. *use the oscillos
- 2ffcs
- the time trace oscilloscope optimize the pinhole position **with** Nomarski Prism and **both** lasers.
- burst_duration_and_fcs_diffusion_time @howto:burst_duration_and_fcs_diffusion_time
- n depends on the diffusion coefficient, the entry position of the molecule, and the spatial weighting impose
- using_the_antibunching_script
- lly moves the red and yellow curve to the correct position. Press "Calculate" again to recalculate the corre
- align_beam_backreflection
- ch quadrant. To reach this, you have to precisely position the beam to enter at the center of the objective
- 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.
- 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
- 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