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| I'm posting this because a few people have emailed pointing me to a discussion in sci.physics about making nano-antennas for lightwave detection. I don't see it but I got a fragment in the email, so here goes. First, photodiodes are considered to be distinct from Hertz antennas. On prior art: Marks proposed using tuned elements in various configurations but didn't talk about how to make them. So-called uncooled IR detectors have been proposed and some have been made of pillars of materials that are scaled to light wavelngths. Lots of people suggested and wrote about using carbon 60 or nanotubes as electrical or optical devices. A quick search in uspto.gov will locate a few of these. I proposed a way to make them to specific sizes needed for operation at short wavelengths, such as light wavelengths. My personally funded research work in the mid 90's was based directly upon conventional antenna design, and specifically on the monopole or dipole version as "the basic building block" for practical nano-antennas. I found we could place and tune wavelength-specific elements on substrates such as silicon and get them to be "real" antennas. I proposed experiments to uncover the "velocity factor" - a term borrowed from transmission line engineering after realizing that the nano-antennas were going to be physically shorter than the free space wavelength, just as we find with our 80M dipole antennas strung between the trees. But, the shortening effect is more severe at light wavelengths - stated simplistically, the inertia of electrons affects these structures to a greater degree than, say, on a 2M Yagi. (that's about 146 Mhz for the non-hams) Using groups of nano-antennas, directivity, gain, steering, phased array, narrow and broadband operation could be achieved. Additionally, we can attach the nano-antennas to junctions. The junctions and antennas can be accessed to switch, modulate, further tune, detect, demodulate, upconvert, downconvert - all useful. The nano-antennas are a bit small and hard to wire up, so one handy way to use them is to look at reradiation - that's what the BC group appears to be doing. Carbon nanotube antennas can be metallic (linear) or semiconducting (nonlinear). The addition of a rectifyng junction at an end can render the structure nonlinear, which makes it a nice reradiating frequency doubler, tripler, mixer etc. To do this you beam light in and look at what gets reradiated. The reradiation is polarized, has frequency components that are related to the tuned operation of the little antennas, and can also have other information superimposed upon it by modulating the substrate. The antennas are close together so some band gap effects (cavity tuning effects to the hams) are also present. The size of these structures is very small, about 100nm or so, depending upon wavelength. The junctions are also very small and are fast. That allows us to switch lightwaves, make logical devices, or mass array memory. There is also an attraction of oppositely charged nanotubes and a repulsion of those nanotubes when like-charged. They move and can be used as a sort of electrostatic switch. Other interesting stuff can be done at the nano-scale using tuned structures or arrays of lightwave antennas. It all started with Maxwell, Fourier, Hertz and Armstrong, and ham radio, of course. If you want, check out [Only registered users see links. ] That will bring you to some other work and patents on this technology and related fun and probably useful electromagnetic devices. Cheers, Bob Crowley w1xyz |
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| antennas , carbon , nanotube |
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