WO2017199125A1 - Range-independent resolution radar - Google Patents
Range-independent resolution radar Download PDFInfo
- Publication number
- WO2017199125A1 WO2017199125A1 PCT/IB2017/052670 IB2017052670W WO2017199125A1 WO 2017199125 A1 WO2017199125 A1 WO 2017199125A1 IB 2017052670 W IB2017052670 W IB 2017052670W WO 2017199125 A1 WO2017199125 A1 WO 2017199125A1
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- WO
- WIPO (PCT)
- Prior art keywords
- radar
- cell
- antenna
- signal
- delay
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Ceased
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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
- 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
-
- 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
- G01S13/88—Radar or analogous systems specially adapted for specific applications
- G01S13/89—Radar or analogous systems specially adapted for specific applications for mapping or imaging
-
- 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
- G01S13/003—Bistatic radar systems; Multistatic radar systems
-
- 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
- G01S13/32—Systems for measuring distance only using transmission of continuous waves, whether amplitude-, frequency-, or phase-modulated, or unmodulated
-
- 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
- G01S13/87—Combinations of radar systems, e.g. primary radar and secondary radar
- G01S13/878—Combination of several spaced transmitters or receivers of known location for determining the position of a transponder or a reflector
-
- 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
-
- 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
- G01S7/03—Details of HF subsystems specially adapted therefor, e.g. common to transmitter and receiver
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q19/00—Combinations of primary active antenna elements and units with secondary devices, e.g. with quasi-optical devices, for giving the antenna a desired directional characteristic
- H01Q19/06—Combinations of primary active antenna elements and units with secondary devices, e.g. with quasi-optical devices, for giving the antenna a desired directional characteristic using refracting or diffracting devices, e.g. lens
- H01Q19/062—Combinations of primary active antenna elements and units with secondary devices, e.g. with quasi-optical devices, for giving the antenna a desired directional characteristic using refracting or diffracting devices, e.g. lens for focusing
Definitions
- the invention is generally directed to radar systems.
- it provides an apparatus, method and system suitable for creating range-independent resolution radar.
- the spatial resolution of radar systems typically depends on the beamwidth, the size of the radar antennas, and the distance between the radar and the target. Consequently, there is typically a tradeoff between these factors and achievable resolution in radar sensing.
- phased arrays that use, for example, digital beamforming, or multi-static methods.
- phased array antennas add complexity in the form of individual feeds, transceivers, and phase shifters, and/or processing sections.
- FIG. 1 shows the effect of antenna size, target distance, and beamwidth on the spot size on the target.
- the spot size on the target (X) depends on the distance (R) between the target and the radar antenna.
- moving the antenna closer to the target is not always a practical approach, as one cannot always control the distance between the radar and the target.
- the spot size does not decrease with the radar- target distance when the distance becomes shorter than the far-field distance ⁇ 2/ ⁇ .
- the minimum spot size close to the antenna is of the order of the antenna aperture size itself, as is shown in FIG. 2.
- Super-resolution techniques can also be used to improve the resolution of radar systems.
- Super-resolution techniques may require increased processing power and
- the present invention provides an apparatus for imaging, the apparatus comprising: a radar transmitter configured to transmit a radar signal; a first cell comprising a first antenna and a first delay element, wherein the first cell is configured to receive the radar signal from the radar transmitter and to retransmit the radar signal after a first known time delay from the first delay element; and a radar receiver configured to receive the retransmitted radar signal from the first cell.
- the present invention provides a method for imaging, the method comprising: transmitting a first radar signal by a radar transmitter; receiving at least some portion of the radar signal at a first antenna of a first cell; generating, by a first delay element, a first time delayed signal based on the received at least some portion of the radar signal; retransmitting the first time delayed signal by the first antenna of the first cell; receiving the at least some portion of first time delayed signal by a radar receiver; and constructing an image, wherein constructing the image comprises determining the absence of a target based on the presence of the first time delayed signal and the presence of a target based on the absence of the first time delayed signal.
- the present invention provides a system for imaging, the system comprising: a radar, wherein the radar comprises: a radar transmitter configured to generate a radar signal, and a radar receiver; and a cell array, wherein the cell array comprises: a first cell, wherein the first cell comprises a first antenna and a first delay element connected to the first antenna, wherein the first antenna and the first delay element are configured to receive the radar signal, generate a first time delayed radar signal by the first delay element, and transmit the first time delayed radar signal such that at least some portion of the first time delayed radar signal is incident on the radar receiver, and a second cell, wherein the second cell comprises a second antenna and a second delay element connected to the second antenna, wherein the second antenna and the second delay element are configured to receive the radar signal, generate a second time delayed radar signal by the second delay element, and transmit the second time delayed radar signal such that at least some portion of the second time delayed radar signal is incident on the radar receiver.
- the present invention relates to improving the performance of radar, spectroscopy and imaging systems by (i) performing single or multi-pixel imaging with a single fixed beam radar regardless of the size of the radar-antenna, and (ii) providing a super-resolution of the target edges, at the order of a wavelength or less, that is independent from the target distance.
- the invention in an embodiment, further relates to a novel technique for radar imaging that achieves super-resolution of a target profile edges by placing an array of cells containing true delays or lumped delays behind the target.
- the resolution of the radar is determined, in part, by the size of the cells. Typical cells can be of the order of a wavelength, and the resolution of the radar is of the same order. This resolution can be achieved regardless of the size of the illuminating and receiving radar antennas, and regardless of the distance between the radar and the target.
- the cell structure is, in an embodiment, composed of an antennas (e.g., a horn, open ended waveguide, or patch antenna) connected to a lumped-delay (such as phase shifter, capacitors, inductors, etc.) with e.g. short circuit after the lumped element or true delay element (such as a waveguides, printed microstrip line, stripline, coaxial cable, coplanar waveguide, etc.) with generally varying length or delay for each cell by e.g. short-circuiting the delay element at the desired length.
- the cells are placed behind the target, and the overall design does not require significant changes in the radar system itself. With the described apparatus, the spatial resolution of the radar together with the cells is determined by the size of the cells and not by the size of the radar antennas or by the radar-target distance.
- the cell structure can be used with any radar system, such as continuous wave, pulsed, or other.
- FIG. 1 is a diagram showing the relation of the spot size from a radar to the distance to the target and the beamwidth, in accordance with the prior art
- FIG. 2 is a diagram showing the near-field and far-field components of the radar beam, in accordance with the prior art
- FIG. 3 is a schematic diagram of the range independent resolution radar system, according to an embodiment of the present invention.
- FIG. 4 is a schematic of the cell array with eighteen open-ended waveguides as antennas where each antenna is connected to a waveguide with different length by shortening the waveguide at the desired position, according to an embodiment the present invention
- FIG. 5 is a plot of the resulting beat frequencies of a continuous wave implementation of an embodiment of the present invention
- FIG. 6A is a schematic of a target present in front of the cell array, according to an embodiment of the present invention.
- FIG. 6B is a plot of the beat frequencies present for a frequency-modulated continuous-wave radar, according to an embodiment of the present invention.
- FIG. 6C is a reconstructed target image, according to an embodiment of the present invention.
- FIG. 7 is a schematic of a compact structure with flat waveguide meander tunnels, according to an embodiment of the present invention.
- FIG. 7 A is a schematic diagram of a top layer of a device, according to an embodiment of the present invention, with nine antennas;
- FIG. 7B is a schematic diagram of a middle signal distribution layer of a device, according to an embodiment of the present invention.
- FIG. 7C is a schematic diagram of a bottom true delay line layer of a device, according to an embodiment of the present invention.
- FIG. 7D is a schematic diagram of a multilayer device, according to an embodiment of the present invention.
- FIG. 8A is a schematic view of eight open ended waveguide antennas connected to eight waveguides with different lengths that are illuminated by an incident field, according to an embodiment of the present invention
- FIG. 8B is a plot of field intensities of a wave incident on the range independent resolution radar system's cell array, according to an embodiment of the present invention.
- FIG. 8C is a retransmitted signal directivity plot, according to an embodiment of the present invention.
- FIG. 9 is a barcode like device, according to an embodiment of the present invention.
- FIG. 10 is range independent resolution radar system incorporating lenses, according to an embodiment of the present invention.
- the range independent radar system 300 is composed of a radar 310 and an cell array 320.
- the radar 310 comprises a transmitter and a receiver.
- the target 390 is placed between the transmitter 310 and the cell array 320.
- Each cell 325 comprises a cell antenna 326 and a true delay 327.
- the cell antenna 326 can be any type of antenna suitable for transmitting and receiving signals in the radar frequency of operation, and may be an open ended waveguide, horn, patch, dipole, slot, miniaturized antenna, or reduced size dielectric surrounded antenna.
- the true delay 327 can be implemented as a microstrip line, stripline, waveguide, coplanar waveguide, or any other transmission line that can guide the incoming energy received by the cell-antenna and reflect it back to the radar.
- Other delay elements such as lumped elements, can be substituted for the true delay 327.
- the gain of each antenna the losses of the transmission line and the coupling between cells and the transmission line, one can reduce the antenna size and crowd the transmission line with no inherent physical limit determined by the wavelength.
- the radar transmitting antenna illuminating the target and the radar receiving antenna capturing the reflections from the target can be different or could be implemented by the same antenna.
- the target does not necessary block all of the cells.
- the apparatus, system, and method of embodiments of the present invention are applicable to all the cases where it is possible to put such cells behind the target.
- the target may also move within the area in front of the cells, and the imaging system may generate a series of images at various times when the time the target is present. Each cell produces a delay caused by its different length. For continuous-wave radars, such as frequency-modulated continuous-wave radar, each delay would be translated to different beat frequency ft in the radar receiver.
- the different delay will cause the reflected signal to arrive at a different times t r at the radar receiver.
- the cell will have a known delay from the true delay 327, by which it will delay the radar signal.
- the radar receiver can determine which cells are blocked based on the presence and/or amplitude of signal corresponding to the known time delay of the cell. Starting from a case where the array is illuminated by the radar's signal and there is no target obstructing the path, the radar will measure the delay associated with all the cells in the array. In case one or more cells are blocked by the target, the ft or t r associated with these cells will not appear at the radar output. Since the position of the cells can be known and predetermined, a high resolution image of the targets profile edges or the entire target can be formed. This high resolution is enabled regardless of the radar antenna size, target-radar distance, and without the need for traditional super-resolution methods.
- FIG. 4 shows an embodiment of the cell array 320 according to an embodiment of the present invention with eighteen open-ended waveguides as antennas where each antenna is connected to a waveguide with different length by shortening the waveguide at the desired position.
- eighteen beat frequencies will be generated in the radar receiver in correspondence with the delay of each cell.
- a plot of the resulting beat frequencies 510 can be seen in FIG. 5.
- the cell array 320 structure can contain any number of cells. This number can be chosen, for example, by considering the typical cell size, the target size and the frequency of operation.
- AL the range resolution of the radar
- the example here is for frequency-modulated continuous-wave radar, the same structure can be used with any continuous wave, pulsed, or other types of radar. In the case of pulsed radar, the length difference of each cell will generate different delays in the radar receiver.
- FIG. 6 A shows a schematic of a target 390 present in front of the cell array 320 according to an embodiment of the present invention.
- the target 390 will block some of the cells and other cells of the cell array 320 may be left open.
- the beat frequencies 510 (ft) or delays (t r ) that corresponds to the cells that were left open will produce corresponding signals at the radar receiver.
- the beat frequencies produced for a frequency- modulated continuous-wave radar are shown in FIG. 6B. Since the positions of the cells are known and pre-determined, an image 650 of the target can be formed, as shown in FIG. 6C.
- the distance between the target and the cells is not limited to any particular value. However, close distances are preferred so as to avoid diffraction effects in which cells that are blocked from direct view by the target would manage to reflect some of the energy back to the radar.
- the collective field reflected back from all the cells in the structure is, in fact, an aperture field of an antenna array. Therefore, one may randomly distribute the lengths of the true delays of each cell in order to create random phase distribution on this aperture. In such a way, we minimize the possibility of beam shifting that will reduce the power propagating towards the receiving antenna of the radar.
- FIG. 7D Other configurations of the array are also possible.
- the straight and long waveguides that appear in FIG. 4 can be replaced by a more compact structure with flat waveguide meander tunnels according to an embodiment of the present invention, as shown in FIG. 7D.
- the top layer 710 of the device is shown in FIG. 7A. This top layer 710 has a four by four set of open ended waveguides acting as the cell antennas.
- the middle layer 720 of the device is shown in FIG. 7B. This layer has distributing tunnels from the cell antennas to the true delays, which are waveguide tunnels in this embodiment. In this embodiment, the waveguide tunnels are thin tunnels.
- a bottom layer 730 of true delays can be seen in FIG. 7C.
- FIG. 8A shows a cell array 320 made up of eight open ended waveguide antennas connected to eight waveguides with different lengths that are illuminated by an incident field, according to an embodiment of the present invention.
- the illumination represents the signal transmitted by a radar.
- the different lengths of the waveguides are achieved by short-circuiting each waveguide to the desired length.
- the spatial pattern of the reflected wave is shown in FIG. 8B.
- This spatial pattern shows that each cell captured the illuminating wave and retransmitted a wave according to the length of the true delay.
- Illuminating a multi-cell structure with a radar signal such as a pulsed signal or a continuous wave signal, generates the various output signals, such as delayed pulses or beat frequencies, from which the radar image or target profile can be produced.
- the differences in length among the waveguides were chosen, in an embodiment, such that the retransmitted energy was steered by 30 degrees, as is seen in FIG. 8C. That is, a phase shift in each of the cells can be purposely introduced to change the direction of the retransmitted signal.
- the cells can be distributed randomly in terms of phase shifts between the cells in order to avoid beam steering of the reflected wave.
- the relatively high scattered field intensities behind the waveguides seen in FIG. 8B can be reduced as desired. This reduction can be achieved by placing radar absorbing materials around the cells aperture.
- the amplitude of the reflected wave can be used for attaining additional information about the target.
- the frequency received corresponding to a particular cell may have lower amplitude when the cell is partially blocked.
- the degree of the attenuation can aid in determining the extent of blockage by the target.
- the attenuated signal can also be used to further enhance the spatial resolution beyond the cell size.
- the signal attenuation can also be used for detecting material properties. For highly conducting metallic target, the blocked cells will emit little or no energy. If the target is made of other, only partially absorbing materials, cells that are blocked by the target may be able to reflect some of the energy back to the radar.
- the system can be used to characterize the material composition of the target, particularly at the radar operation frequency.
- a partially transparent object will not obstruct the radar beam, thereby allowing the corresponding returned signal (e.g., beat frequency components in frequency-modulated continuous-wave radar or delayed pulses in pulsed radar) to appear, although attenuated.
- the amplitude information is considered, the target object's image is still generated by noting that the corresponding frequencies return with lower power due to attenuation.
- the attenuated signal can provide information on the transparency of the object, which is determined by the material, its thickness, and its shape.
- the system can also aid in the determination of the target thickness.
- the characteristics of the returned signal will be dependent on the target thickness for some materials.
- reference frequency signals and additional beat frequencies signals that correspond to energy travelling back and forth multiple times to the cell are generated. This information can be used to determine the target thickness in these cases.
- cells that are partially blocked may generate frequencies that correspond to waves travelling back and forth multiple times to and from the cells before they are received by the radar. These frequencies will indicate that they are not fully blocked, improving the spatial resolution to a size below the cell size.
- Spatial resolution better than the wavelength can be obtained if the distance of the blocking object from the delay line aperture is shorter than a wavelength, and if the aperture size of the delay lines itself is smaller than a wavelength.
- the limit to the spatial resolution is the aperture dimension as long as the delay line is able to guide a wave at the given small aperture dimension.
- the cell array 320 may also be configured to create a barcode like device.
- the barcode like device according to an embodiment of the present invention, is shown in FIG. 9. This low- profile device has nine patch antennas and nine printed transmission lines with each
- FIG. 10 A method for improving the resolution for targets smaller than the cell array, according to an embodiment of the present invention, is shown in FIG. 10.
- the resolution of the formed image can be improved by adding a first lens 910 and a second lens 920, placing the target 390 between the lenses, and locating the cell array 320 after the second lens 920 as shown. In this way, the target's projected shape on the cells is larger, and more cells are effectively blocked. This lens system leads to improvement in the image resolution in comparison to the case without the lenses.
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- Radar, Positioning & Navigation (AREA)
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- General Physics & Mathematics (AREA)
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Abstract
Description
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Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP2018560025A JP6849897B2 (en) | 2016-05-18 | 2017-05-08 | Equipment, methods and systems for imaging |
| CN201780029983.3A CN109154650B (en) | 2016-05-18 | 2017-05-08 | Range-Independent Resolution Radar |
| DE112017000933.2T DE112017000933B4 (en) | 2016-05-18 | 2017-05-08 | Radar with range-independent resolution |
| GB1820374.5A GB2566848B (en) | 2016-05-18 | 2017-05-08 | Range-independent resolution radar |
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US15/157,425 | 2016-05-18 | ||
| US15/157,425 US10386478B2 (en) | 2016-05-18 | 2016-05-18 | Range-independent resolution radar |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| WO2017199125A1 true WO2017199125A1 (en) | 2017-11-23 |
Family
ID=60324921
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| PCT/IB2017/052670 Ceased WO2017199125A1 (en) | 2016-05-18 | 2017-05-08 | Range-independent resolution radar |
Country Status (6)
| Country | Link |
|---|---|
| US (1) | US10386478B2 (en) |
| JP (1) | JP6849897B2 (en) |
| CN (1) | CN109154650B (en) |
| DE (1) | DE112017000933B4 (en) |
| GB (1) | GB2566848B (en) |
| WO (1) | WO2017199125A1 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2018111810A1 (en) * | 2016-12-13 | 2018-06-21 | Duke University | Single-frequency dynamic metasurface microwave imaging systems and methods of use |
| US11555908B2 (en) | 2019-09-06 | 2023-01-17 | International Business Machines Corporation | Multi range radar system |
| US12276747B2 (en) * | 2021-06-25 | 2025-04-15 | Samsung Electronics Co., Ltd. | Radar for full-blockage detection of radio frequency modules in mobile devices |
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-
2016
- 2016-05-18 US US15/157,425 patent/US10386478B2/en active Active
-
2017
- 2017-05-08 GB GB1820374.5A patent/GB2566848B/en active Active
- 2017-05-08 WO PCT/IB2017/052670 patent/WO2017199125A1/en not_active Ceased
- 2017-05-08 CN CN201780029983.3A patent/CN109154650B/en active Active
- 2017-05-08 DE DE112017000933.2T patent/DE112017000933B4/en active Active
- 2017-05-08 JP JP2018560025A patent/JP6849897B2/en active Active
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| US6133989A (en) * | 1993-02-09 | 2000-10-17 | Advanced Scientific Concepts, Inc. | 3D imaging laser radar |
| US6414746B1 (en) * | 1999-11-24 | 2002-07-02 | Advanced Scientific Concepts, Inc. | 3-D imaging multiple target laser radar |
| US20140266866A1 (en) * | 2013-03-12 | 2014-09-18 | Nokia Corporation | Steerable transmit, steerable receive frequency modulated continuous wave radar transceiver |
| CN103744076A (en) * | 2013-12-25 | 2014-04-23 | 河海大学 | Non-convex optimization based MIMO radar moving object detection method |
| CN103941243A (en) * | 2014-04-03 | 2014-07-23 | 电子科技大学 | Spinning type aircraft height measuring method based on SAR three-dimensional imaging |
Also Published As
| Publication number | Publication date |
|---|---|
| CN109154650B (en) | 2023-05-26 |
| JP6849897B2 (en) | 2021-03-31 |
| DE112017000933B4 (en) | 2025-03-27 |
| GB2566848A (en) | 2019-03-27 |
| DE112017000933T5 (en) | 2019-02-28 |
| GB201820374D0 (en) | 2019-01-30 |
| CN109154650A (en) | 2019-01-04 |
| US10386478B2 (en) | 2019-08-20 |
| US20170336506A1 (en) | 2017-11-23 |
| JP2019516984A (en) | 2019-06-20 |
| GB2566848B (en) | 2020-03-18 |
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