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We have experimentally demonstrated surface tracking control with 100 Hz unity-crossover frequency, 70 degrees phase margin, and 0.12 nm RMS noise in a 100 Hz measurement bandwidth.
Phantom measurements demonstrated a linear regression coefficient of 4.70 degrees phase difference per degree Celsius, with an R2 = 0.998.
After human images with artifact were excluded, the linear regression demonstrated a correlation coefficient of 5.5 degrees phase difference per degree Celsius, with an R2 = 0.84.
The sequence used to derive T1 and density values was a multiple-saturation recovery which consists of four pairs of 90 degrees pulses, followed by a 180 degrees phase reversal pulse, generating four T1-weighted images.
Shortly after, there is a 180 degrees phase change in the grid current with respect to the grid voltage signifying that the direction of the power flow is reversed.
Due to MTP, the output of the MZM1 consists only the even order sidebands as shown in Fig. 2. Output of the first MZM is then passed on to the MZM2 to MZM4 which are driven by RF LO with 45 degrees phase shift.
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Thus, a binary 1 might be sent as a zero-degree phase shift, while a binary 0 might be sent as a 180-degree phase shift.
Note that they only differ by a relative degree phase shift.
The image was obtained at a 50 degree phase angle between the spacecraft, asteroid, and the sun.
And there's one procedure that is discussed in more detail in the text, which uses what's referred to as a 90 degree phase splitter.
Our approach uses microfabricated electrodes that are placed on-axis within the objective aperture, in order to apply a 90-degree phase shift to the unscattered component of the electron wave.
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