Compensation of direction finding estimates for polarimetric errors
AssigneeRaytheon Company
InventorMark A. Owens
Life of this patent
Estimating the term…
Abstract
An algorithmic technique which allows antenna arrays that are used for interferometric direction finding to have elements with arbitrary orientation. This technique allows the phase errors associated with non-identical element orientation to be estimated, without explicit knowledge of either the polarimetrics of the array elements or the polarimetrics of the source. It relies upon the fact that there exists a single number which describes the polarimetric interaction, and that this number can be estimated and then utilized to remove the phase component due to polarimetric interaction. This technique makes it feasible to incorporate direction finding arrays into articles that could benefit from such arrays, but because of size or shape constraints, were previously not able to do so.
Claims11
An interferometric method for estimating the angle of arrival of a signal from a source, using an antenna array having antenna elements with arbitrary orientation, where each element has an orientation αn relative to some reference element, and each element has a measured complex voltage of vn=MnejΨn, the method comprising:
- computing the measured powers {pn} and the measured phases {Ψn} from the measured complex voltages of {vn};
- using the measured powers {pn} and {αn}, solving for a polarimetric ratio ζ;
- using ζ, computing a set of estimated polarimetric phase components {};
- and
- using the corrected phase measurements {Ψn−}, solving for the angle of arrival Ω;
- wherein the polarimetric ratio is defined by ζ=bd/ac, the polarimetric vectors en of the antenna elements represented with eigenvectors eR and eL, the right-hand circular and left-hand circular basis set, the polarimetric vector e1 for the first element is expressed in terms of this basis set as:
- e1=aeR+beL, where a and b represent unknown complex scalars, and the polarimetric vector of the source is expressed as:
- eT=ceR+deL, where c and d are unknown complex scalars;
- and
- wherein the set of estimated polarimetric phase components {} is defined as:
- =arg((exp(jαn)+ζexp(−jαn)) (1+ζ)−1).
An interferometric method for estimating the angle of arrival of a signal from a source, using an antenna array having antenna elements with arbitrary orientation, and each element has a measured complex voltage of vn=MnejΨn, the method comprising the following steps:
- computing the measured powers {pn} and the measured phases {Ψn} from the measured complex voltages of {vn};
- selecting one element of the array as a reference element;
- computing the set of rotations {αn} relative to the reference element;
- from {pn} and {αn}, providing an estimate for {M,β} in the set of equations
- pn=p1(1+2*M*cos(2α−β)+M2) (1+2*M*cos(β)+(M2)−1;
- using ζ=Mejβ, computing the estimated polarimetric phase components {} using the equation
- =arg((exp(jαn)+ζexp(−jαn)) (1+ζ)−1);
- and
- using the corrected phase measurements {Ψn−}, determining the angle of arrival Ω.
An apparatus for estimating the direction of arrival of a signal from a source, comprising:
- an antenna array comprising at least two antenna elements with arbitrary orientation, wherein each element has an orientation αn relative to a reference element;
- measurement apparatus for measuring a complex voltage vn=MnejΨn for each element of the array resulting from the signal;
- a signal processor responsive to the measured complex voltages for estimating the angle of arrival of the signal at the antenna array, the signal processor including means for computing the measured powers {pn} and the measured phases {Ψn} from the measured complex voltages of {vn}, means for calculating ζ using the measured powers {pn} and {αn}, means for computing estimated polarimetric phase components {} using ζ, and means for determining the angle of arrival Ω using the corrected phase measurements {Ψn−};
- and
- wherein ζ is defined as bd/ac, the polarimetric vectors en of the antenna elements represented with eigenvectors eR and eL, the right-hand circular and left-hand circular basis set, the polarimetric vector e1 for the first element is expressed in terms of this basis set as:
- e1=aeR+beL, where a and b represent unknown complex scalars, and the polarimetric vector of the source is expressed as:
- eT=ceR+deL, where c and d are unknown complex scalars, and the polarimetric component of the voltage at the first element is:
- v1+ac+bd=ac(1+bd/ac)=ac (1+ζ);
- and
- wherein the set of estimated polarimetric phase components {} is defined as:
- =arg((exp(jαn)+ζexp(−jαn)) (1+ζ)−1).
Dependencies are inferred from the claim text.