Terahertz photoelectric conductive antenna array and use thereof
A photoconductive antenna and terahertz technology, which is applied in the field of terahertz radiation, can solve problems such as the input impedance of antenna arrays without consideration, and achieve the effects of overcoming light saturation, increasing input resistance, and increasing input resistance
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Embodiment 1
[0032] Growth of 3 micron thick low-temperature gallium arsenide on a 50 micron thick gallium arsenide substrate, and then vapor-deposited with gold Figure 4 shaped antenna array, gold-plated with a thickness of 0.5 µm. The model is arranged in 1 row and 3 columns, with a total of three antenna elements. Each antenna unit is a dipole antenna, and the illuminated area of the antenna is indicated by a small arrow in the CST software, named port3, port1, and port2 from left to right. After software calculation, the input resistance and average resistance of the three ports in the working frequency band are obtained, and Figure 6 express. Remove the triangular choke coil in the model to get the input resistance and average resistance of the three ports in the working frequency band, such as Figure 7 . Since the total energy of the antenna array is formed by superimposing the energy of each unit, the average resistance is used here as an indicator for evaluating performanc...
Embodiment 2
[0034] On the basis of Embodiment 1, the triangular choke coil is changed to a trapezoidal choke coil, and other parameters remain unchanged. Calculated by CST software Figure 8 The input resistance (inset) and average resistance of the three ports in . Compared Figure 7 and Figure 8 It can be seen that after adding the ladder choke coil, the peak value of the average resistance increases from 457Ω to 3308Ω, an increase of 7.2 times.
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