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As expected, it reveals progressively decreasing rotational arm stiffness for higher deflection angles.
With increased dc bias, larger deflection angles were obtained.
Far-field deflection angles are extended to more than 10°.
Current cholangioscopes are restricted to 2 deflection angles and require more than 1 operator.
The calculated deflection angles using this equation are in good agreement with the trajectory simulations.
The distribution of the deflection angles to the different magnet types has been optimized.
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For a demonstration of the dependence of the electron deflection angle on the optical phase of the deflecting fields, we again use two spatially separated laser pulses with an adjustable time delay.
Our perturbation framework is also used to derive as a consistency check, the recently found weak deflection bending angle series.
In Fig. 4c, we show the measured electron current as a function of the minimum deflection angle and of the phase difference between the two laser pulses (the deflection angle of the beam centre is shown in Supplementary Fig. 3).
The transverse angular streaking velocity is defined as, where ϕ t0) is the deflection angle and t0 the electron arrival time.
The deflection angle, in the order of 50 mrad, is sufficiently small to avoid deflection aberrations.
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