USH548H - Group orthogonal arrays for elimination of multiple-time-around echos in radars - Google Patents
Group orthogonal arrays for elimination of multiple-time-around echos in radars Download PDFInfo
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- USH548H USH548H US02/633,091 US63309187A USH548H US H548 H USH548 H US H548H US 63309187 A US63309187 A US 63309187A US H548 H USH548 H US H548H
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- 238000003491 array Methods 0.000 title claims abstract description 35
- 238000002592 echocardiography Methods 0.000 title 1
- 230000008030 elimination Effects 0.000 title 1
- 238000003379 elimination reaction Methods 0.000 title 1
- 230000002123 temporal effect Effects 0.000 claims abstract description 14
- 239000013598 vector Substances 0.000 claims abstract description 11
- 239000011159 matrix material Substances 0.000 claims abstract description 4
- 238000000034 method Methods 0.000 claims description 8
- 238000001208 nuclear magnetic resonance pulse sequence Methods 0.000 abstract description 13
- 239000002131 composite material Substances 0.000 abstract description 9
- 238000005314 correlation function Methods 0.000 abstract description 7
- 230000015572 biosynthetic process Effects 0.000 description 5
- 238000003786 synthesis reaction Methods 0.000 description 5
- 230000000875 corresponding effect Effects 0.000 description 4
- 238000010586 diagram Methods 0.000 description 4
- 230000000295 complement effect Effects 0.000 description 3
- 230000000737 periodic effect Effects 0.000 description 3
- 238000009825 accumulation Methods 0.000 description 1
- 230000009286 beneficial effect Effects 0.000 description 1
- 230000001276 controlling effect Effects 0.000 description 1
- 230000002596 correlated effect Effects 0.000 description 1
- 230000003111 delayed effect Effects 0.000 description 1
- 238000001514 detection method Methods 0.000 description 1
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Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S7/00—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00
- G01S7/02—Details of systems according to groups G01S13/00, G01S15/00, G01S17/00 of systems according to group G01S13/00
- G01S7/28—Details of pulse systems
- G01S7/2813—Means providing a modification of the radiation pattern for cancelling noise, clutter or interfering signals, e.g. side lobe suppression, side lobe blanking, null-steering arrays
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01S—RADIO DIRECTION-FINDING; RADIO NAVIGATION; DETERMINING DISTANCE OR VELOCITY BY USE OF RADIO WAVES; LOCATING OR PRESENCE-DETECTING BY USE OF THE REFLECTION OR RERADIATION OF RADIO WAVES; ANALOGOUS ARRANGEMENTS USING OTHER WAVES
- G01S13/00—Systems using the reflection or reradiation of radio waves, e.g. radar systems; Analogous systems using reflection or reradiation of waves whose nature or wavelength is irrelevant or unspecified
- G01S13/02—Systems using reflection of radio waves, e.g. primary radar systems; Analogous systems
- G01S13/06—Systems determining position data of a target
- G01S13/08—Systems for measuring distance only
- G01S13/10—Systems for measuring distance only using transmission of interrupted, pulse modulated waves
- G01S13/26—Systems for measuring distance only using transmission of interrupted, pulse modulated waves wherein the transmitted pulses use a frequency- or phase-modulated carrier wave
- G01S13/28—Systems for measuring distance only using transmission of interrupted, pulse modulated waves wherein the transmitted pulses use a frequency- or phase-modulated carrier wave with time compression of received pulses
- G01S13/284—Systems for measuring distance only using transmission of interrupted, pulse modulated waves wherein the transmitted pulses use a frequency- or phase-modulated carrier wave with time compression of received pulses using coded pulses
- G01S13/288—Systems for measuring distance only using transmission of interrupted, pulse modulated waves wherein the transmitted pulses use a frequency- or phase-modulated carrier wave with time compression of received pulses using coded pulses phase modulated
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q21/00—Antenna arrays or systems
- H01Q21/06—Arrays of individually energised antenna units similarly polarised and spaced apart
- H01Q21/22—Antenna units of the array energised non-uniformly in amplitude or phase, e.g. tapered array or binomial array
Definitions
- group-complementary and group-orthogonal arrays to radar waveform design allows sidelobe control not only in the principal unambiguous range interval, but also in multiple time around range intervals.
- Previous waveform designs concentrated on controlling responses in the principal unambiguous range interval, and usually responses for multiple time around range intervals were identical to those of the first time around range interval.
- Interleaved group-orthogonal/group complementary arrays provides sidelobe cancellation in the principal unambiguous range interval as well as for complete sidelobe cancellation in one or more multiple time around range intervals.
- the uniqueness of this waveform design, compared to previous designs is that it simultaneously controls near-in sidelobes as well as far-out sidelobes in multiple time around intervals.
- a unique aspect of this design is that it allows for placing the maximum response in a multiple time around interval while providing cancellation of responses from nearer-in range intervals including the principal unambiguous range interval.
- interleaved group-orthogonal/group complementary arrays lies in their property of sidelobe cancellation over multiple range intervals. This results in reduced clutter interference when tracking low speed targets in clutter.
- a high PRF can be used to increase energy on target or increase Doppler coverage, and allows detection and tracking of targets in multiple time around range intervals with cancellation of clutter responses form the principal unambiguous range interval and from other multiple time around range intervals.
- Group-complementary code arrays which have the property of being mutually orthogonal over a subinterval of their total cross-correlation function have been identified. These group-orthogonal arrays are generated by a multiplication operation upon a given group-complementary array using a matrix which has diagonal elements from vectors which are orthogonal. Walsh vectors are examples of such orthogonal vectors.
- Composite code arrays are synthesized by interleaving rows from the group-orthogonal set of arrays, and the resulting rows of codes are applied to bi-phase modulate pulses in bursts.
- the resulting composite waveform has the desirable property of temporal (zero-Doppler) sidelobe cancellation in the maximum unambiguous range interval and response cancellation over one or more multiple-time-around range intervals of an equivalent uncoded pulse sequence.
- the waveforms also have the property of maximizing the receiver response in one of the multiple-time-around range intervals, while achieving response cancellation in the maximum unambiguous range interval of an equivalent uncoded pulse sequence.
- FIG. 1 is a schematic of radar processing with group-complementary codes.
- FIG. 2 is a pulse sequence timing diagram.
- FIG. 3 shows transmit/reference waveforms--aperiodic cross-correlation.
- FIG. 4 shows transmit/reference waveforms--aperiodic cross-correlation.
- FIG. 5 shows cross-correlation between A0 and A3.
- FIG. 6 is a timing diagram for transmitted (C T ) and reference (C R ) coded pulse sequences.
- FIG. 7 shows cross-correlation between C T and C R .
- Group-Complementary arrays can be produced which provide for the temporal distribution of carrier phase in each transmitted pulse through binary coding. These are applied to synthesize a radar waveform with the desirable property of temporal sidelobe cancellation (G. Weathers, and E. M. Holliday, "Group-Complementary Array Coding for Radar Clutter Rejection," IEEE Transactions and Aerospace and Electronic Systems, AES-19, No. 3, pp. 369-379, May 1983).
- FIG. 1 illustrates the cross-correlation process in the receiver.
- the group-complementary array is a code set of K pulses. Each row codes (bi-phase) a single pulse.
- a single burst composed of rows of shifted maximum-length sequences, with a final "all 1" row and column.
- Each row bi-phase codes a single pulse, and the receiver summation is over K pulses corresponding to the K rows of the code array.
- the code 10 is transmitted by antenna 11 to target 12.
- the reflection is received by antenna 13, correlated by correlation 14 in accordance with range delayed 15 code and accumulation in 16.
- FIG. 2 is a timing diagram of the coded pulse sequence for the periodic and aperiodic cases, where each pulse is numbered corresponding to the row from the code array which bi-phase modulates that pulse.
- FIG. 3 gives the transmit/reference waveforms aperiodic correlation function for the group complementary array from FIG. 1.
- Temporal sidelobes are seen to cancel over the temporal range interval of ⁇ (T-T 1 ), but sidelobes do exist at multiple-time-around range intervals centered around ⁇ T, ⁇ 2T, . . . , ⁇ (K-1)T.
- the rows of a group-complementary array can be interchanged without affecting the temporal sidelobe cancellation property in the interval ⁇ (T-T 1 ).
- FIG. 4 gives the aperiodic correlation function for this array.
- the peak sidelobes are seen to be smaller than for the previous example, however still relatively large.
- the group-complementary array's property of temporal sidelobe cancellation in the ⁇ (T-T 1 ) interval can be extended to multiple-time-around intervals through an array synthesis procedure which utilizes a "group-orthogonality" property of certain sets of group-complementary arrays. This extension applies to both the periodic and aperiodic cross-correlation functions.
- a single group-complementary array can be operated upon to generate a set of group-complementary arrays which have a group-orthogonality property. That is, each array in the set is orthogonal to all other arrays in the set over a ⁇ (T-T 1 ) interval of the cross-correlation two pulse-sequences which are coded by any two arrays from the set.
- the method of generating a group-orthogonal array, A z , from a group-complementary array, A 0 is to perform a matrix multiplication
- a 0 is a K row by N column array
- V z is an N by N diagonal array of the form ##EQU1##
- a set of group-complementary arrays which are also group-orthogonal can be generated from the Walsh vectors, W z ##EQU3## then ##EQU4## The resulting group orthogonal arrays are ##EQU5##
- FIG. 5 is the cross-correlation function for A 0 and A 3 , and illustrates the orthogonality of the two arrays over the interval ⁇ (T-T 1 ).
- the group-orthogonal array set synthesis procedure given utilizes group-complementary arrays in the form of Hadamard matrices with the sign pattern of a Walsh vector operating on columns of the original array.
- a group-orthogonal set of group-complementary arrays can be used to synthesize composite transmitted and reference code arrays.
- the cross-correlation of these two resulting arrays will have the property of temporal sidelobe cancellation over the maximum unambiguous range interval, and over one or more multiple-time-around range intervals.
- the synthesis procedure for the composite code arrays is to interleave rows from the arrays of the group-orthogonal sets to bi-phase modulate K bursts of pulses, with up to S pulses in each burst.
- the K bursts will be separated by a time interval equal to one or more pulse-repetition intervals, depending on the number of multiple-time-around intervals which are to have temporal responses cancelled.
- the resulting K*S pulse sequence can be utilized as the radar waveform on a periodic or aperiodic basis.
- the composite receiver response is formed from the sum of the K*S pulses or upon integer multiples of K*S pulses.
- FIG. 6 The timing diagram corresponding to transmitter code, C T , and reference code, C R , is shown in FIG. 6, and FIG. 7 gives the cross-correlation between C T and C R .
- This cross-correlation function corresponds to the zero-Doppler cut of the waveform's cross-ambiguity function.
- temporal sidelobes have been cancelled over the maximum unambiguous range interval and over the second-time-around range interval of an equivalent, but uncoded, pulse sequence.
- the waveform shown as C T and C R could, by timing of C R , be used to place the maximum cross-correlation response in the second-time-around range interval (for an uncoded pulse sequence with the same pulse repetition interval), with zero response (for zero-Doppler offset) in the maximum unambiguous range interval, and in the third-time-around range interval.
- This radar waveform and processing could be useful for detecting targets in the second-time-around range interval, while reducing clutter interference from clutter sources in the maximum unambiguous range interval.
- the time between each burst of four pulses is 2T. If this period is increased to 3T, then sidelobe cancellation is extended to the third-time-around range interval for the equivalent uncoded pulse sequence, and so on.
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- Engineering & Computer Science (AREA)
- Radar, Positioning & Navigation (AREA)
- Remote Sensing (AREA)
- Computer Networks & Wireless Communication (AREA)
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Radar Systems Or Details Thereof (AREA)
Abstract
Sets of group-complementary code arrays which have the property of being ually orthogonal over a subinterval of their total cross-correlation function have been identified. These group-orthogonal arrays are generated by a multiplication operation upon a given group-complementary array using a matrix which has diagonal elements from vectors which are orthogonal. Composite code arrays are synthesized by interleaving rows from the group-orthogonal set of arrays, and applying the resulting rows of codes to bi-phase modulate pulses in bursts. The resulting composite waveform has the desirable property of temporal (zero-Doppler) sidelobe cancellation in the maximum unambiguous range interval and response cancellation over one or more multiple-time-around range intervals of an equivalent uncoded pulse sequence. The waveforms also have the property of maximizing the receiver response in one of the multiple-time-around range intervals, while achieving response cancellation in the maximum unambiguous range interval of an equivalent uncoded pulse sequence.
Description
The invention described herein may be manufactured, used, and licensed by or for the Government for governmental purposes without the payment to us of any royalties thereon.
The unique application of group-complementary and group-orthogonal arrays to radar waveform design allows sidelobe control not only in the principal unambiguous range interval, but also in multiple time around range intervals. Previous waveform designs concentrated on controlling responses in the principal unambiguous range interval, and usually responses for multiple time around range intervals were identical to those of the first time around range interval. Interleaved group-orthogonal/group complementary arrays provides sidelobe cancellation in the principal unambiguous range interval as well as for complete sidelobe cancellation in one or more multiple time around range intervals. The uniqueness of this waveform design, compared to previous designs is that it simultaneously controls near-in sidelobes as well as far-out sidelobes in multiple time around intervals. Also, a unique aspect of this design is that it allows for placing the maximum response in a multiple time around interval while providing cancellation of responses from nearer-in range intervals including the principal unambiguous range interval.
The advantage of interleaved group-orthogonal/group complementary arrays lies in their property of sidelobe cancellation over multiple range intervals. This results in reduced clutter interference when tracking low speed targets in clutter. With this waveform, a high PRF can be used to increase energy on target or increase Doppler coverage, and allows detection and tracking of targets in multiple time around range intervals with cancellation of clutter responses form the principal unambiguous range interval and from other multiple time around range intervals.
Sets of group-complementary code arrays which have the property of being mutually orthogonal over a subinterval of their total cross-correlation function have been identified. These group-orthogonal arrays are generated by a multiplication operation upon a given group-complementary array using a matrix which has diagonal elements from vectors which are orthogonal. Walsh vectors are examples of such orthogonal vectors. Composite code arrays are synthesized by interleaving rows from the group-orthogonal set of arrays, and the resulting rows of codes are applied to bi-phase modulate pulses in bursts. The resulting composite waveform has the desirable property of temporal (zero-Doppler) sidelobe cancellation in the maximum unambiguous range interval and response cancellation over one or more multiple-time-around range intervals of an equivalent uncoded pulse sequence. The waveforms also have the property of maximizing the receiver response in one of the multiple-time-around range intervals, while achieving response cancellation in the maximum unambiguous range interval of an equivalent uncoded pulse sequence.
FIG. 1 is a schematic of radar processing with group-complementary codes.
FIG. 2 is a pulse sequence timing diagram.
FIG. 3 shows transmit/reference waveforms--aperiodic cross-correlation.
FIG. 4 shows transmit/reference waveforms--aperiodic cross-correlation.
FIG. 5 shows cross-correlation between A0 and A3.
FIG. 6 is a timing diagram for transmitted (CT) and reference (CR) coded pulse sequences.
FIG. 7 shows cross-correlation between CT and CR.
Group-Complementary arrays can be produced which provide for the temporal distribution of carrier phase in each transmitted pulse through binary coding. These are applied to synthesize a radar waveform with the desirable property of temporal sidelobe cancellation (G. Weathers, and E. M. Holliday, "Group-Complementary Array Coding for Radar Clutter Rejection," IEEE Transactions and Aerospace and Electronic Systems, AES-19, No. 3, pp. 369-379, May 1983). FIG. 1 illustrates the cross-correlation process in the receiver. The group-complementary array is a code set of K pulses. Each row codes (bi-phase) a single pulse. Included in the figure is a single burst composed of rows of shifted maximum-length sequences, with a final "all 1" row and column. Each row bi-phase codes a single pulse, and the receiver summation is over K pulses corresponding to the K rows of the code array. The code 10 is transmitted by antenna 11 to target 12. The reflection is received by antenna 13, correlated by correlation 14 in accordance with range delayed 15 code and accumulation in 16.
The algebraic property which results in zero-valued temporal sidelobes holds in the maximum unambiguous range interval of the equivalent uncoded pulse sequence, ±(T-T1), where T is the pulse repetition interval and T1 is the pulse width. FIG. 2 is a timing diagram of the coded pulse sequence for the periodic and aperiodic cases, where each pulse is numbered corresponding to the row from the code array which bi-phase modulates that pulse.
FIG. 3 gives the transmit/reference waveforms aperiodic correlation function for the group complementary array from FIG. 1. Temporal sidelobes are seen to cancel over the temporal range interval of ±(T-T1), but sidelobes do exist at multiple-time-around range intervals centered around ±T, ±2T, . . . , ±(K-1)T.
The rows of a group-complementary array can be interchanged without affecting the temporal sidelobe cancellation property in the interval ±(T-T1).
______________________________________ -1 -1 -1 1 1 -1 1 1 1 1 1 1 1 1 1 1 -1 -1 1 1 -1 1 -1 1 1 -1 -1 -1 1 1 -1 1 1 1 -1 1 -1 -1 -1 1 -1 1 -1 -1 -1 1 1 1 -1 1 1 -1 1 -1 -1 1 1 -1 1 -1 -1 -1 1 1 ______________________________________
The array from interchanging several rows of the array in FIG. 1. FIG. 4 gives the aperiodic correlation function for this array. The peak sidelobes are seen to be smaller than for the previous example, however still relatively large.
In many cases, it is beneficial to eliminate the temporal sidelobes from multiple-time-around range intervals. It will be shown that the group-complementary array's property of temporal sidelobe cancellation in the ±(T-T1) interval can be extended to multiple-time-around intervals through an array synthesis procedure which utilizes a "group-orthogonality" property of certain sets of group-complementary arrays. This extension applies to both the periodic and aperiodic cross-correlation functions.
A single group-complementary array can be operated upon to generate a set of group-complementary arrays which have a group-orthogonality property. That is, each array in the set is orthogonal to all other arrays in the set over a ±(T-T1) interval of the cross-correlation two pulse-sequences which are coded by any two arrays from the set.
The method of generating a group-orthogonal array, Az, from a group-complementary array, A0, is to perform a matrix multiplication
A.sub.z =A.sub.0 V.sub.z (1)
where A0 is a K row by N column array, and Vz is an N by N diagonal array of the form ##EQU1##
Even though we consider only the case where N=K, (with K being a power of 2), group-orthogonal arrays exist for any even N. For N=K=2n, the diagonal elements of Vz will be elements of Walsh vectors. Each Walsh vector (index z) used in Vz to form Az results in a new array which is set group-orthogonal to A0. Also the arrays generated from a set of Walsh vectors will be group-orthogonal to each other.
As an example, consider the group-complementary array ##EQU2##
A set of group-complementary arrays which are also group-orthogonal can be generated from the Walsh vectors, Wz ##EQU3## then ##EQU4## The resulting group orthogonal arrays are ##EQU5##
The four arrays, A0, A1, A2, and A3, for a group-orthogonal set of arrays. FIG. 5 is the cross-correlation function for A0 and A3, and illustrates the orthogonality of the two arrays over the interval ±(T-T1).
For N=2n, the number of arrays in a group-orthogonal set, S, is
S=N, (13)
corresponding to the N Walsh vectors which can be applied in (2).
The group-orthogonal array set synthesis procedure given utilizes group-complementary arrays in the form of Hadamard matrices with the sign pattern of a Walsh vector operating on columns of the original array.
A group-orthogonal set of group-complementary arrays can be used to synthesize composite transmitted and reference code arrays. The cross-correlation of these two resulting arrays will have the property of temporal sidelobe cancellation over the maximum unambiguous range interval, and over one or more multiple-time-around range intervals.
The synthesis procedure for the composite code arrays is to interleave rows from the arrays of the group-orthogonal sets to bi-phase modulate K bursts of pulses, with up to S pulses in each burst. The K bursts will be separated by a time interval equal to one or more pulse-repetition intervals, depending on the number of multiple-time-around intervals which are to have temporal responses cancelled. The resulting K*S pulse sequence can be utilized as the radar waveform on a periodic or aperiodic basis. The composite receiver response is formed from the sum of the K*S pulses or upon integer multiples of K*S pulses.
As an example of this synthesis procedure, the group orthogonal arrays A0, A1, A2, and A3 given by equations (3), (10), (11), and (12) respectively will be the basis for the synthesis of a composite waveform. The composite code formed from interleaving rows from A0, A1, A2, and A3 is ##EQU6##
The timing diagram corresponding to transmitter code, CT, and reference code, CR, is shown in FIG. 6, and FIG. 7 gives the cross-correlation between CT and CR. This cross-correlation function corresponds to the zero-Doppler cut of the waveform's cross-ambiguity function. As can be seen from the figure, temporal sidelobes have been cancelled over the maximum unambiguous range interval and over the second-time-around range interval of an equivalent, but uncoded, pulse sequence.
Observe that the waveform shown as CT and CR could, by timing of CR, be used to place the maximum cross-correlation response in the second-time-around range interval (for an uncoded pulse sequence with the same pulse repetition interval), with zero response (for zero-Doppler offset) in the maximum unambiguous range interval, and in the third-time-around range interval. This radar waveform and processing could be useful for detecting targets in the second-time-around range interval, while reducing clutter interference from clutter sources in the maximum unambiguous range interval.
For the example given, the time between each burst of four pulses is 2T. If this period is increased to 3T, then sidelobe cancellation is extended to the third-time-around range interval for the equivalent uncoded pulse sequence, and so on.
Claims (2)
1. In a radar system for detecting a target in which a plurality of pulses with a carrier are transmitted and reflection of those pulses from the target are received, the improvement comprising the method of arranging the temporal distribution of carrier phase in each transmitted pulse by biphased binary coding; utilizing a set of at least two different group-orthogonal arrays for a series of at least eight transmitted pulses; and providing a corresponding reference set of arrays and combining them in a range gate manner with the reflection of the transmitted pulses whereby crosscorrelation sidelobes of multiple time around reflections from the target are cancelled.
2. A method as set forth in claim 1 wherein said set of group-orthogonal arrays are generated by a multiplication operation upon a given group-complementary array using a matrix which has diagonal elements from vectors which are orthogonal.
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US02/633,091 USH548H (en) | 1987-12-07 | 1987-12-07 | Group orthogonal arrays for elimination of multiple-time-around echos in radars |
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US02/633,091 USH548H (en) | 1987-12-07 | 1987-12-07 | Group orthogonal arrays for elimination of multiple-time-around echos in radars |
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Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP0520489A2 (en) * | 1991-06-27 | 1992-12-30 | Hughes Aircraft Company | Glittering array for radar pulse shaping |
US7259713B1 (en) * | 1990-08-16 | 2007-08-21 | Selex Sensors And Airborne Systems Limited | Ranging systems |
US9791552B1 (en) * | 2014-11-19 | 2017-10-17 | Src, Inc. | On-site calibration of array antenna systems |
US10459071B2 (en) * | 2014-08-28 | 2019-10-29 | Japan Radio Co., Ltd. | Orthogonal separation device and orthogonal separation method |
-
1987
- 1987-12-07 US US02/633,091 patent/USH548H/en not_active Abandoned
Cited By (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US7259713B1 (en) * | 1990-08-16 | 2007-08-21 | Selex Sensors And Airborne Systems Limited | Ranging systems |
EP0520489A2 (en) * | 1991-06-27 | 1992-12-30 | Hughes Aircraft Company | Glittering array for radar pulse shaping |
EP0520489A3 (en) * | 1991-06-27 | 1993-06-30 | Hughes Aircraft Company | Glittering array for radar pulse shaping |
US10459071B2 (en) * | 2014-08-28 | 2019-10-29 | Japan Radio Co., Ltd. | Orthogonal separation device and orthogonal separation method |
US9791552B1 (en) * | 2014-11-19 | 2017-10-17 | Src, Inc. | On-site calibration of array antenna systems |
US20170301988A1 (en) * | 2014-11-19 | 2017-10-19 | Src, Inc. | On-site calibration of array antenna systems |
US20180164407A1 (en) * | 2014-11-19 | 2018-06-14 | Src, Inc. | On-site calibration of array antenna systems |
US10663563B2 (en) * | 2014-11-19 | 2020-05-26 | Src, Inc. | On-site calibration of array antenna systems |
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