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AMTA Paper Archive

ISAR RCS editing via modern spectral estimation methods
S.R. DeGraaf,E. LeBaron, G. Fliss, K. Quinlan, S. Li-Fliss, November 1995

ERIM is investigating the use of modem spectral esti­ mation techniques for extracting (editing) desired or undesired contributions to RCS and ISAR measurements in two ways. The first approach involves using parametric spectral estimators to perform frequency sweep range compression and signal history editing, while the second involves using the associated stabilized linear prediction filters to extrapolate sweep data and perform "enhanced resolution" Fourier image editing. This paper summarizes our editing algorithms and illustrates RCS editing results using measurements of a conesphere target contaminated by a metal rod and foam support. The reconstructed "clean" conesphere measurements are compared quantitatively against numerically simulated ground truth. Editing was performed using three bandwidths at two center fre­ quencies to provide insight into the impacts of nominal resolution and scatterer amplitude variation with fre­ quency on editing efficacy, and to assess the degree to which superresolution algorithms can offset reduced nominal resolution.

Super-resolution for SAR/ISAR RCS measurement using spatially variant apodization
H. Stankwitz,M. Kosek, November 1995

Spatially Variant Apodization (SVA) [l] is nonlinear image domain algorithm which effectively eliminates finite-aperture sidelobes from SAR/ISAR imagery without degrading mainlobe resolution, unlike traditional methods of sidelobe suppression (e.g. Taylor weighting). Dezellum et. al. [2] demonstrated at the 16th AMTA symposium the benefits of SVA for improving RCS analysis of ISAR data. The purpose of this paper is to show that robust super-resolution via bandwidth extrapolation can be obtained in a relatively simple, straightforward manner using SVA, providing further improvement in RCS measurements from SAR/ISAR data. This new super-resolution algorithm (called Super-SVA) can extrapolate the signal bandwidth for an arbitrary set of scatterers by a factor of two or more, with a commensurate improvement in resolution. Super-resolution techniques have been traditionally limited to problems where a-priori knowledge is available and/or the scene content is suitably constrained. Using Super-SVA, no a-priori knowledge of scene content is required. Super-SVA exploits the fact that SVA applied to an image results in finite image-domain support on the scale of the system resolution for an arbitrary set of complex scatterers. Extrapolation of the frequency-domain signal data is then simply a matter of applying frequency-domain inverse amplitude weighting. The fidelity of the deconvolution process can be improved by embedding the original signal data in the extrapolated data and performing further iterations of the process.

Generalized geometry for ISAR imaging, A
C. Malek, November 1995

Traditional range/doppler ISAR techniques have inherent geometric limitations. By using concepts of microwave holography and tomography, a vector-based k space approach allows a more generalized geometry of the sampled Fourier space. By constructing a complete annulus in the polar sampling space, arbitrary apertures up to 360 degrees can be processed for "full body" two dimensional images. This processing also typically exhibits better resolution. The algorithm relies on linear interpolation for potar­ Cartesian conversion. The general geometric formulation is also readily adaptable to arbitrary antenna configurations.

Flexible high speed antenna measurement data acquisition system for the outdoor antenna range, A
J.S. DeRosa, November 1995

Rome Laboratory has recently designed and implemented a state of the art automated antenna measurement data acquisition system at the Rome Lab/Newport antenna test facility. A generalized approach to the antenna data acquisition hardware and software was implemented which allows sequencing, control and measurement of test variables in virtually any order without test specific software modifications. The hardware design is based on distributed computers in which real-time data acquisition tasks and near real-time operator control and data analysis tasks are performed independently. The computers operate in a remote client/server configuration in which control information and data are transferred via fiber optic local area network. In this paper, the fundamental approach to the data acquisition system design is discussed and the antenna measurement hardware and software that comprises the final system are described.

Triband radome measurement system: installation and testing results, A
V. Jory,G.W. Pearson, J.R. Jones, L.L. Oh, S.J. Manning, T.L. Norin, V. Farr, November 1995

In an earlier paper ("System Engineering for a Radome Test System," John R. Jones, et al, AMTA, October 1994) the system level design of a compact range enhancement for the testing of the Triband Radome was presented. This paper will discuss the installation and testing of the radome measurement system in the compact range. The purpose of the radome measurement system is to determine (within close tolerances) boresight shift, transmission loss, antenna pattern changes and polarization effects caused by the radome. Unique features include novel coordinate transformation and correction by means of a laser autocollimator and data reduction algorithms. Also featured is the tracking subsystem which consists of a specially designed two-axis track pedestal, an autotrack controller, and three five-horn compact range feed arrays operating at X, K, and Q-bands. The performance of the triband radome measurement system in the compact range setting will be presented.

Bistatic coherent measurement system (BICOMS), A
R.O. Jernejcic,W.L. Cassaday, November 1995

The U.S. Air Force 46 Test Group, Radar Target Scattering Division (RATSCAT), at Holloman AFB, NM, in conjunction with the US Army, Navy and Georgia Tech Research Institute (GTRI), has developed a concept for a bistatic coherent radar measurement system (BICOMS). It will be used to measure both the monostatic and bistatic RCS of targets, as well as create two-dimensional images of monostatic and bistatic signature data. It will consist of two mobile radar units, each of which is capable of simultaineously collecting coherent monostatic and bistatic RCS data. This paper will cover the systetn design specificatiovs, layout and design of equipment, and discuss the operating parameters for the radar (power, antenna sizes, sensitivities, timing, etc.).

Portable 4.5m x 2.0m near-field scanner, A
D.S. Fooshe, November 1995

Portable scanners used for near-field antenna measurements are usually incapable of providing a large scan area with a high degree of probe position accuracy. This paper discusses a 4.5m x 2.0m portable scanner developed by NSI with a probe position accuracy on the order of 2 mils (0.050 mm) rms. An NSI patented optical measurement system measures the X, Y, and Z position, and provides real­ time position correction capability. This lightweight, portable scanner combined with optical correction provides enhanced accuracy while reducing overall antenna measurement system costs and improving test chamber flexibility.

2095P pulsed microwave measurement system for the Naval Surface Warfare Center, Crane Division
R.S. Sauerman,A.R. Tillerson, November 1995

Modem pulsed phased array radar systems bring new challenges to antenna measurement. These antennas generally consist of hundreds of Transmit-Receive (TR) modules controlled via a beam steering computer to fonn the antenna beam. Attempting to operate these modules with a CW wavefonn will not only quickly damage the mod­ ules but will not properly characterize the antenna. The Navel Surface Warfare Center, Crane Division, recog­ nized the need to add pulsed capability when specifying their latest antenna measurement system. Scientific­ Atlanta met these requirements by integrating their newly introduced Model l 795P Pulsed Microwave Receiver into their proven 2095 Microwave Measurement System to make the Model 2095P Pulsed Microwave Measurement System.

Planar near-field measurements and microwave holography for measuring aperture distribution on a 60 GHz active array antenna
J. Guerrieri,D. Tamura, K. MacReynolds, N. Canales, November 1995

This paper discusses results of a recent attempt to measure aperture distribution of a small active steerable array antenna at 60 GHz using planar near-field measurements and the back transform. Using a procedure which exercises every phase shifter without steering the antenna beam, it is possible to isolate problems with individual bits in the phase shifters. From calculation of the aperture fields for each case we hope to infer the individual phase shifter bit loss. We will also discuss problems which arose in the measurement because of the short wavelength, signal-to-noise ratio and small number of elements.

High power superposition for active array transmit pattern measurement
J. Hoffman,B.L. Galebach, K. Thompson, November 1995

Measurement of active array high-power transmit patterns in an indoor near-field facility raises significant issues concerning safe microwave power levels and absorber power-handling capability. An extension of the planar near-field measurement technique for the safe and accurate measurement of active array high power transmit patterns is considered to address these issues. This new technique involves sequentially turning on groups of elements around each probe position while making measurements for each group of activated elements. Simulation results indicate that this technique is potentially feasible for safely and accurately measuring low sidelobe active array transmit patterns.

Beam pointing method in a deployable phased array antenna for satellite use
R. Yonezawa,I. Chiba, T. Katagi, T. Takahashi, November 1995

Deployable phased array antennas for satellite use have been of recent concern[ 11[2]. In a phased array antenna, the excitation phase is the most important factor. For the case when the observation point coincides with the point towards which the beam should be directed, the method for determining the excitation phase is presented in reference [1]. In this case, deflection of the main beam due to a change of the satellite attitude or distortion of the antenna surface can be corrected. However, in an antenna in which the shape of the main beam has to be maintained, the observation point should be placed apart from the main beam region. In this paper, we investigate the necessary number of observation points to correct main beam deflection and present a method that makes it possible not only to correct the deflection of the main beam but also to measure displacement of relative element positions.

Measurement of complex permittivity of dielectric material at microwave frequency using waveguide measurements
M.D. Deshpande,C.J. Reddy, R. Cravey, November 1995

A simple waveguide measurement technique is presented to determine the complex dielectric constant of a dielectric material. Using a network analyzer, the reflection coefficient of the shorted waveguide (loaded with sample ) is measured. Using the Finite Element Method the exact reflection coefficient of the shorted waveguide (loaded with the sample) is deter­ mined as a function of the dielectric constant. Matching the measured value of the reflection coefficient with the reflection coefficient calculated using the FEM and utilizing the Newton-Raphson Method, an estimate of dielectric constant of a dielectric material is obtained. Comparison of estimated values of dielectric constant obtained from simple waveguide modal theory and the present approach is presented.

INTA's free space NRL arch system and calibration for absorber material characterization
I. Montiel, November 1995

In order to measure the performance of microwave absorbing materials a broadband free- space measurement system constructed in INTA. The is a kind of N RL Arch that gives us the possibility of measurements in d ifferent configurations. It comprises a set of dielect ric loaded rectangular waveguide antennas, coaxial vector analyzer, sample support and a computer. A TRL calibration technique in the plate near field is developed taking advantage of the calibration functions implemented in the network analyzer and the time domain gating. We introduce the use of typical RCS calibration standards as the calibration reflect standards. It gives us the possibility of performing the near field free space calibration in the same way that it is usually done in waveguide, but for directions di fferent to the normal. This calibration allows us to check the edge diffraction behaviour of the samples in the measurement and is thought to be adecuated for thin materials.

General order N analytic correction of probe-position errors in planar near-field measurements
L.A. Muth, November 1995

An analytic technique recently developed at NIST [1] [2] to correct for probe position errors in planar near-field measurements has been implemented to arbitrary accuracy. The nth-order correction scheme is composed of an mth-order ordered expansion and an n - m higher-order approximation, where both n and m are arbitrary. The technique successfully removes very large probe position errors in the near-field, so the residual near-field probe position errors are substantially below levels that can be measured on a near-field range. Only the error-contaminated near-field measurements and an accurate probe position error function are needed for implementation of the correction technique. The method also requires the ability to obtain derivatives of the error-contaminated near field defined on an error-free regular grid with respect to the coordi­ nates. In planar geometry the derivatives are obtained using FFTs [1], giving an approximate operation count of (3 • 2=- 1 - 1 + (n - m)) N log N, where N is the number of data points. Efficient computer codes have been developed to demonstrate the technique. The results of simulations are more accurate than those obtained us­ ing the well-known k correction [3), which can correct for position errors in some direction in k space, but further contaminates the sidelobe levels.

Simulation of errors in near-field facilities
D.J. Janse van Rensburg,G. Seguin, S. Mishra, November 1995

A technique for estimating measurement errors in near­ field facilities is presented. Known mechanical and electrical errors can be accounted for in simulation and such results are presented here. Unknown factors like chamber reflection and instrumentation drift can be estimated via selective measurement and the error induced by such anomalies may be combined with the simulated findings to provide error patterns for a particular test antenna and facility. Results are shown where these patterns are used to calculate measurement error limits. The software presented here also allows the generation of parametric curves which show the impact of a parameter of interest.

Comparison of K-correction and Taylor-series correction for probe-position errors in planar near-field scanning, A
M.H. Francis, November 1995

We investigated two methods of probe-position error correction to determine how well the corrected results compare to the uncorrupted far field: the k-correction method and the Taylor-series method. For this investigation, we measured a 1.2 m dish at 4 GHz and a 1.2m by 0.9m phased array at 2.2 GHz. Measurements were made first without position errors and then with deliberate z-position errors. We perfonned probe­ position error correction using both methods and compared the results to the error-free far field. For errors up to A/4, the fifth-order implementation of the Taylor­ series correction was slightly better than the k-correction. For errors of ')..J2, the k-correction was better than the Taylor-series correction.

Hologram accuracy determination
G. Masters, November 1995

Hologram measurements are becoming more and more popular as a reliable method for identifying bad elements and the tuning of active phased array antennas. Relying on holographic data to adjust phase shifters and attenuators in these antennas can give undesired results if the accuracy of the data is poor. Often measurements can be improved if the error sources can be isolated and quantified. This paper presents an approach to producing a hologram accuracy budget based on the NIST 18-term error budget created for near-field measurements. A set of hologram accuracy terms is identified and data is presented showing the typical hologram accuracy that can be expected from a near-field scanner.

Method to transform measured Fresnel patterns to far-field based on a least-squares algorithm with probe correction, A
F. Las Heras,B. Galocha, J.L. Besada, November 1995

A method to transform Fresnel field data to far-field data with probe correction, based on a non linear least­ squares algorithm, is presented. The functional to be considered is the expression of the Fresnel field radiated by an array of isotropic sources located on the antenna aperture, and the complex excitations are the coefficients that minimize the rms error between the measured data and the functional values. The intermediate step of determining the complex excitations can be used as a diagnostic tool. Probe pattern correction has been included in the method, improving the performances of antenna measurement systems placed in small size anechoic chambers.

Calibrated real-time RCS measurements using the DDRE modular radar system (MRS)
O.S. Friis, November 1995

The Modular Radar System has been developed at the Danish Defence Research Establishment (DDRE) in cooperation with the Danish company CRIMP. The unique system is capable of performing nearly all types of calibrated radar measurements. The modularized highly flexible system is presented along with a number of measurement. RCS of very small targets at short ranges 400'- l 000', medium range measurements of Navy targets, aircraft and chaff at ranges from 1-10 nautical miles. The real time high resolution range profiles are used for positive identification of "hot spots" on Navy vessels leading to very efficient RCS reductions.

3-D high resolution radar imaging using the MUSIC algorithm
M. Baquero,A.J. Sieber, G. Nesti, J. Fortuny, November 1995

Superresolution techniques based on the Multiple Signal Classification (MUSIC) have recently been applied to two-dimensional (2-D) Inverse Synthetic Aperture Radar (ISAR) imaging with demonstrated results. These techniques exhibit much higher spa­ tial resolution than other approaches using a 2-D Fourier transform. This paper a MUSIC­ based superresolution algorithm for 3-D radar imaging, which is especially useful for measurements with both small frequency and aspect angle (in azimuth and elevation) spans. This algorithm models the measured 3-D data set as a sum of point source emissions plus noise. Once the positions in the 3-D space of such scattering centers are obtained using the MU­ SIC algorithm, the weights (or RCS) of the scattering centers are obtained through a pseudo-inverse matrix inversion computed by means of a Singular Value De­ composition (SYD).







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