Slot Array Base Station Antenna with Electrical Control of Down-Tilt Beam Presenter: George J. Chen Author: Ming Hui Chen Victory Microwave Corporation Xizhi, Taiwan Contents § Motivation for Beam Tilting § Theory § Propagation in Slab Loaded Waveguide § Downtilt § Measured Results C!"#$%&#'(%$)%*)!+',-',#%.'/)0*)+&' ' ' Coverage Variation by Beam Tilting ' ' ' ' ' 1+*#++%' ' ' ' ' ' ' ' ' ' Beam A Beam B Beam C ' ' ' ' ' ' 2!"#$%&#'1' 2!"#$%&#',' 2!"#$%&#'2' ' ' ' Beam down tilt changes the coverage area ! Beam Tilting Options ! ! ෘ ෘ ෘ ! ! ! ! 3##4!5#+67.8! ! ෘ ! ! "#$%&'($&)!*()+(',! /0(',!1%&0#!0%(2+#.! /0(',!4(#)#$+.($!0)&9! Expensive mechanical design Electrical tilting using phase shifter -)#$+.($!*()+(',! Mechanical tilting -)#$+.($!*()+(',! Expensive electronic design (phase shifters) shifters Electrical tilting using dielectric slab Low cost motor attached to dielectric slab in waveguide Propagation in Slab-Loaded Waveguide b Ey equivalent to b Ey a' a dielectric vertical b Ey a dielectric horizontal Kx decreases => β larger" equivalent to b'' Ey a Kx same => β smaller" Propagation constant β can be controlled through the orientation of the dielectric. Example Circular Polarizer Ey ¡í Ex ¡í+90¢X Ey 0 Ex 0 Y X Application: Down Tilt Slot array antenna has alternating slanted slots cut at intervals of d = π/βH Slot Array Antenna Antenna without down tilt with down tilt wavefront wavefront kd sinθ Results in wavefront without downtilt d When slot array propagation is lowered, wavefront is downtilted at an angle θ βH !Hd = ! d θ βL " Ld=!-kd sinθ θ= down tilt angle !H = propagation constant for waveguide withα=90° !L = propagation constant for waveguide withα=0° θ Testing Setup Electronic down tilt Manual down tilt Transmit + receive antennas, attached together to a single structure. Testing Setup Offset 5° In order to measure the downtilt, we raised the antenna. Testing Setup TX θ TX Radiation pattern measurement with downtilt angle Results (1.95GHz, 0° DownTilt) Elevation of peak a function of slab orientation 90° slab orientation corresponds to a 10° downtilt Azimuth pattern at 0° for different downtilts (slab orientation) retains relatively same shape slab rotation Results (1.95GHz, 5° DownTilt) Elevation of peak a function of slab orientation 90° slab orientation corresponds to a 10° downtilt Azimuth pattern at 5° offset remains relatively the same across different offsets. slab rotation Results (2.14GHz, 0° DownTilt) Elevation of peak a function of slab orientation 90° slab orientation corresponds to a 10° downtilt Azimuth pattern at 0° for different downtilts (slab orientation) retains relatively same shape slab rotation Results (2.14GHz, 5° DownTilt) Elevation of peak a function of slab orientation 90° slab orientation corresponds to a 10° downtilt Azimuth pattern at 5° offset relatively constant for a given slab orientation slab rotation Return Loss Return loss varied with the slab orientation Over all conditions, the return loss was under 10 db which is acceptable for antenna designs. Isolation Isolation is better than -25dB, indicating little interference between the two antennas If additional isolation is needed between Tx and Rx bands, a band-pass filter can be used Summary Downtilt capability of antenna structures traditionally relies on expensive mechanical design or expensive phase shifters. We noted dielectric slabs in waveguides change propagation constant. We’ve demonstrated a method to use this property to design an electronically controlled downshift on a slot array antenna. Contact Information Ming Hui Chen Victory Microwave Corporation 396 Fude 1st Rd. Xizhi City, Taipei County 22150 Taiwan (R.O.C.) Tel. 886-2-8693-3799 Fax 886-2-8693-3798 Email: mchen@vicmic.com.tw Web site: www.vicmic.com.tw