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Azimuthal resistivity measurement mode is achieved by the electric potential difference between 12 azimuthal electrodes disposed in the electrical potential guiding ring (M0).
In the height image (Fig. 1a), the measurement mode is strictly related to height proportions and reveals the actual 3D topography, but small height differences are difficult to discern in this imaging mode.
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For measuring the continuous measurement mode was selected.
Instrumented nanoindentation tests (in a continuous stiffness measurement mode) were also conducted employing a Berkovich indenter with a maximum load of 9.8 N.
Two measurement modes were related including attenuated total reflection (ATR) mapping and micro transmission with diamond compression cell.
In the following measurements, the pulse mode is analysed, hence the available power has to be corrected with the duty cycle of the pulse signal.
In Raman backscattering measurements, TO phonon mode is forbidden in the (100) direction, a small TO phonon mode peak for the bulk GaSb (100) substrate might be attributed to a slight substrate mis-orientation or imperfection [44].
Since the blood perfusion of the extremities can be strongly decreased in this conditions, SpO2 measurements in transmission mode is no longer possible in the body extremities e.g. in the fingers [ 23– 25].
Since in this measurement mode it is not possible to distinguish dark noise photons from photons produced by the source, DCMs were acquired in absence of a source and at different temperatures to calculate the expected dark counts as a function of the cell temperature.
Alternatively, a single homodyne measurement is nearly optimal in this lossy case, still only requires measurement on a single mode, is simpler to implement than parity, and is not nearly as sensitive to loss.
This means that the optimal estimation measurement over the auxiliary mode is comprised by projectors onto coherent states, antisqueezed along the line between (alpha_{0}) and the origin (which represents the vacuum) in phase space.
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