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The '''thinned array curse''' (sometimes, ''sparse array curse'') is a theorem in [[electromagnetic radiation | electromagnetic]] theory of transmitters[[transmitter]]s. It states that a transmitting aperture which is synthesized by a coherent [[phased array]] of smaller apertures that are spaced apart will have a smaller minimum beam spot size (typically, athe [[main lobe]] of a [[solid angle]] that is smaller by an amount proportional to the ratio of the area of the synthesized array divided by the total area of the individual apertures), but the amount of power that is beamed into this main lobe is reduced by an exactly proportional amount, so that the total power density in the beam is constant.
The origin of the term "thinned arrrayarray curse" is not clear. [[Robert L. Forward]] cites use of the term in unpublished [[Hughes Research Laboratories]] reports dating from 1976 <ref>T. R. O'Meara, ''The Thinned Array Curse Theorems,'' Hughes Research Laboratories, unpublished internal report, Malibu CA Dec. 1976</ref>,<ref>W. B. Bridges, ''Looking at the Thinned Array Curse from a Slightly Different View,'' Hughes Research Laboratories, unpublished internal report, Malibu CA April 1976</ref>
==Example==
Consider as an example the case of a number of small apertures that are mutually adjacent to one another, so that they form a filled aperture array. Now, supose you separate these (but keep them mutually phased) so as to synthesize a larger aperture (that is, like a [[radiotelescope]] array). The spot size on the ground is reduced in size proportionally the diameter of the synthesized array (and hence the area reduced proportionate to the diameter of the synthesized array squared), *but the power density at the ground is unchanged.*
Thus:
3. The receiving spot on the ground is smaller.
From these three facts, it is trivial to now derive the factclear that if the synthesized aperture has an area A, and the total area of thisit that is filled by active transmitters is a, then onlyat most a fraction a/A of the radiated power reaches the target, and the fraction (1-a/A) is lost. This loss shows up in the form of power in [[side lobe]]s.
This theorem can also be derived in more detail by considering a partially-filled transmitter array as being the superposition of a fully-filled array plus an array consisting of only the gaps, broadcasting exactly out of phase with the filled array. The interference pattern between the two reduces the main beam lobe by exactly the ratio (1-a/A).
It is worth noting that the thinned array curse applies only to [[mutual coherence | mutually coherent]] sources. If the transmitting sources are not mutually coherent, the size of the ground spot is not dependent on the relationship of the individual sources to one another, but is simply the sum of the individual spots from each source. ▼
▲It is worth noting that the thinned array curse applies only to [[mutual coherence | mutually coherent]] sources. If the transmitting sources are not mutually coherent, the size of the ground spot isdoes not dependentdepended on the relationship of the individual sources to one another, but is simply the sum of the individual spots from each source.
==Consequences==
The thinned array curse means that while synthesized apertures are useful for narrow-beam receivers with high angular resolution, butthey are not useful for power transmitters. It also means that if an filled array transmitter has gaps between individual elements, the main lobe of the beam will lose an amount of power proprotionalproportional to the area of the gaps. Likewise, if a transmitter comprising multiple individual individual transmitters has subapertures which have fail, the power lost will not merely equal the power of the lost transmitter, but will also have an equal amount of power lost from the beam.
The thinned array curse has important consequences to concepts for [[Microwave power transmission]] and [[Wireless energy transfer]] such as design of a [[Solar power satellite]], in that it suggests that it is not possible to make a smaller beam and hence reduce the size of a receiver (or ''[[Rectenna]]'', for the case of microwave power beaming] by phasing together beams from many small satellites.
A short derivation of the thinned array curse, focussingfocusing on the implications for use of [[lasers]] to provide impulse for an interstellar probe (that is, an application of [[Beam-powered propulsion]], can be found in Robert Forward's paper "Roundtrip Interstellar Travel Using Laser Pushed LIghtsailsLightsails<ref>Robert L. Forward, "Roundtrip Interstellar Travel Using Laser Pushed LIghtsailsLightsails," ''J. Spacecraft and Rockets, Vol. 21,'' No. 2, Mar-Apr 1984, pp. 190.</ref>."
==References==
<references />
*The general theory of phased array antennas, from which the thinned- array curse can be derived, can be found in [http://www.ece.rutgers.edu/~orfanidi/ewa/ch18.pdf Chapter 18] of Sophocles J. Orfanidis, ''Electromagnetic Waves and Antennas'' (electronic version accessed May 22, 2007).
*See also Constantine A. Balanis: “Antenna Theory, Analysis and Design”, John Wiley & Sons, Inc., 2nd ed. 1982 ISBN 0-471-59268-4
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