Silicon Micromachined Microlens Array for THz Antennas
- Created: Monday, 01 July 2013
There is strong demand for a multi-pixel heterodyne detector array for Earth observation, astrophysics, future planetary, and ground applications.
A 5×5 silicon microlens array was developed using a silicon micromachining technique for a silicon-based THz antenna array. The feature of the silicon micromachining technique enables one to microfabricate an unlimited number of microlens arrays at one time with good uniformity on a silicon wafer. This technique will resolve one of the key issues in building a THz camera, which is to integrate antennas in a detector array. The conventional ap proach of building single-pixel receivers and stacking them to form a multi-pixel receiver is not suited at THz because a single-pixel receiver already has difficulty fitting into mass, volume, and power budgets, especially in space applications.
Photograph of Silicon Microlens Array Antenna. The reason why there are different sizes of silicon microlenses is that each column has a different diameter of microlens on the mask plate. The microlens diameter of each column is very uniform.">In this proposed technique, one has controllability on both diameter and curvature of a silicon microlens. First of all, the diameter of microlens depends on how thick photoresist one could coat and pattern. So far, the diameter of a 6- mm photoresist microlens with 400 μm in height has been successfully microfabricated. Based on current researchers’ experiences, a diameter larger than 1-cm photoresist microlens array would be feasible.
In order to control the curvature of the microlens, the following process variables could be used:
1. Amount of photoresist: It determines
the curvature of the photoresist
microlens. Since the photoresist lens
is transferred onto the silicon substrate,
it will directly control the curvature
of the silicon microlens.
2. Etching selectivity between photoresist and silicon: The photoresist microlens is formed by thermal reflow. In order to transfer the exact photoresist curvature onto silicon, there needs to be etching selectivity of 1:1 between silicon and photoresist. However, by varying the etching selectivity, one could control the curvature of the silicon microlens.
The figure shows the microfabricated silicon microlens 5×5 array. The diameter of the microlens located in the center is about 2.5 mm. The measured 3-D profile of the microlens surface has a smooth curvature. The measured height of the silicon microlens is about 280 μm. In this case, the original height of the photoresist was 210 μm. The change was due to the etching selectivity of 1.33 between photoresist and silicon. The measured surface roughness of the silicon microlens shows the peak-to-peak surface roughness of less than 0.5 μm, which is adequate in THz frequency. For example, the surface roughness should be less than 7 μm at 600 GHz range. The SEM (scanning electron microscope) image of the microlens confirms the smooth surface. The beam pattern at 550 GHz shows good directivity.
This work was done by Choonsup Lee, Goutam Chattopadhyay, Imran Mehdi, John J. Gill, and Cecile D. Jung-Kubiak of Caltech; and Nuria Llombart of the Universidad Complutense de Madrid, Spain, for NASA’s Jet Propulsion Laboratory.
In accordance with Public Law 96-517, the contractor has elected to retain title to this invention. Inquiries concerning rights for its commercial use should be addressed to:
Innovative Technology Assets Management
Mail Stop 321-123
4800 Oak Grove Drive
Pasadena, CA 91109-8099
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