Search
You can find the results of your search below.
Fulltext results:
- 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 sample will only be illuminated indirectly (b
- 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