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Using a 105- μm fiber, a 150- μm wide optrode with a 45° tip taper emits a λ = 1550 nm beam with 122 μm diameter and 16° far-field full angle divergence.
An advantage of having the ϕ = 56° full angle divergence instead of 16° is that light can be delivered to a continuous plane at about 150 μm depth from the tip when a block of optrodes in the array is excited.
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Normalized output power ranged from 0.23 to 0.35 with longer optrodes performing at higher efficiencies; output beams had a nominal beam width and far-field full-angle divergence of 55 μm and 17°, respectively [ 41].
The divergent trajectory for the electrospun nanofibers results in the increasing in-plane angle of divergence for the nozzles further from the midpoint of the tube.
Such a small angle of divergence will produce a one-metre spot at a distance of one kilometre.
In the stationary chiral medium the angle of divergence between the circular birefringent beams is calculated to be 1.3 radian.
The angle of divergence between the circular birefringent beams and the polarization states of the two light beams is manipulated with Kerr nonlinearity.
The change in the angle of divergence between circular birefringent beams by rotary photon drag is calculated to be 0.4 microradian.
Microchannel with 8° angle of divergence and 156 μm of hydraulic diameter is employed for experiments in both diverging and converging modes.
Angle of divergence slit for the incident X-ray beam was set to 1º and the antiscatter slit was set at 0.5º.
Beam steering due to refractive index gradients within the combusting gases was observed, and a full-angle beam divergence of over 100 mrad was measured.
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