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To prevent the beam divergence, a suspended multi-layer graphene (MLG) was fabricated on a very large gate aperture to be used as an electron-transparent gate in a field emission triode.
The solid angles of the beams obtained using conventional gate aperture and suspended MLG gate were 0.225 and 0.074 sr, respectively, indicating that the suspended MLG resulted in a focused electron beam.
The triode structure fabricated with a miniature CNT paste emitter and a gate aperture (20 μm in diameter) generated a collimated electron beam by which very high resolution (>16 lp/mm) X-ray imaging was achieved.
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The effects of different transmit pulses, receive gates, apertures, SV depths and lateral foci were studied using a one-dimensional (1-D) beam-forming array, with a fixed lens in the elevation direction.
He suggested replacing the camera's aperture gate with laser-cut metal stencils, thus eliminating the gap between the film and the masks.
In a standard movie camera, advancing film presses tightly against the back of the aperture gate, a rectangular metal frame that determines the size of the exposure.
In the past, masking had been achieved by placing a metal stencil in front of the aperture gate, an arrangement that left a gap between the film and the mask.
In contrast to the previously described gates, the residues that form aperture type gates do not need to rotate and can maintain a rigid conformation.
Although a focused electron beam is required in field emission-based various applications, the electron beam is generally diverged in a conventional triode because the gate has a circular aperture through which the electrons are accelerated to reach the anode.
The floating gate level utilized an alternating aperture phase shift mask, a binary mask was used to expose the control gate level.
This electrode had many apertures for each gate perforation, and was mounted approximately 0.2 mm above the gate electrode.
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