Multi-modal Adaptive Land Mine Detection Using Ground-Penetrating Radar (GPR) and Electro-Magnetic...
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Transcript of Multi-modal Adaptive Land Mine Detection Using Ground-Penetrating Radar (GPR) and Electro-Magnetic...
Multi-modal Adaptive Land Mine Detection UsingGround-Penetrating Radar (GPR) and
Electro-Magnetic Induction (EMI)
METAL
PLASTIC
DARPA-AROMURI
Jay A. Marble and Andrew E. Yagle
Outline
1. Application Overview 1.1 Data Collection 1.2 Metal and Plastic Landmines2. Sensor Phenomenology 2.1 Ground Penetrating Radar (GPR) 2.2 Electromagnetic Induction (EMI) 2.3 Overview of Approach3. Metal Landmine Detection 3.1 GPR Signature Features 3.2 EMI Signature Features4. Plastic Landmine Detection 4.1 Plastic Landmine Detection Difficulty 4.2 Hyperbola Flattening Transform 4.3 GPR Signature of Plastic Landmines 4.4 Metal Firing Pin Detection5. Adapting to Changes in Environment6. Current Progress
Bandwidth: 500MHz - 2GHz
Depth Resolution: Free Space - 10cm (4”) Soil (r=3) - 5.7cm (2.3”)
1. Application Overview1.1 Data Collection
GPR Facts EMI Facts
8
111 3 5 7 9 13 15 17 19
2 4 6 10 12 14 16 18
1 2 873 4 5 6 9 10 161511 12 13 14
20
Sampling: Along Track: 5cm Cross Track: 17.5cm Swath: 2.8m
Sampling: Along Track: 5cm (2”) Cross Track: 15cm (6”) Swath: 3.0m
Operating: 75 HzFrequency
EMICoils
GPRAntennae
USArmy Mine Hunter / Killer System
Database: 11000m2
1. Application Overview1.1 Data Collection
Type: M-15Metal CasingBurial Depth: 3”Width: 13”Height: 5.9”
M-21Metal CasingBurial Depth: 1”Width: 13”Height: 8.1”
Type: TM-62MMetal CasingBurial Depth: 2”Width: 13”Height: 5.9”
Metal Landmines
1. Application Overview1.2 Metal Mines
Database Contains: 70 metal cased mines buried from 0” to 3” (Shallow). 93 metal cased mines buried from 3” to 6” (Deep).
Type: VS1.6Plastic CasingBurial Depth: 6”Width: 8.6”Height: 3.5”
Type: TMA-4Plastic CasingBurial Depth: 2”Width: 11”Height: 4.3”
Type: TM-62PPlastic CasingBurial Depth: 2”Width: 13”Height: 5.9”
Type: VS2.2Plastic CasingBurial Depth: 1”Width: 9” (.23m)Height: 4.5” (.115m)
Type: M-19PlasticWidth: 0.33mHeight: 3.5”
Plastic Landmines
1. Application Overview1.2 Plastic Mines
Database Contains: 156 Shallow 265 Deep
NOT LANDMINES
LANDMINES
How to discriminate between landminesand other objects using GPR and EMI ?
GOAL: To determine presence vs. absence of land mines vs. other metal objectsUSING: Both GPR and EMI data (multi-modal detection algorithm)
1. Application Overview
Outline
1. Application Overview 1.1 Data Collection 1.2 Metal and Plastic Landmines2. Sensor Phenomenology 2.1 Ground Penetrating Radar (GPR) 2.2 Electromagnetic Induction (EMI) 2.3 Overview of Approach3. Metal Landmine Detection 3.1 GPR Signature Features 3.2 EMI Signature Features4. Plastic Landmine Detection 4.1 Plastic Landmine Detection Difficulty 4.2 Hyperbola Flattening Transform 4.3 GPR Signature of Plastic Landmines 4.4 Metal Firing Pin Detection5. Adapting to Changes in Environment6. Current Progress
-0.5 0 0.5 1 1.5
Tx RxAntenna Module
Target
Layer 2
Air
f1 f2 fNf3
SampledFrequencies
DepthProfile
FourierTransform
Target
TransmitPulse
GroundInterface
PulseLaunch
SampleTime
Transmitted Frequencies
f1
f2
fN
2.1 GPR Phenomenology
Continuous, Stepped Frequency Radar500MHz – 1.5GHz
128 Frequency Steps
h
d
[m]
khjdjd
RCSRT eeeTTdh
GGE 222
2112
2
220 44
2.1 GPR Phenomenology
khjRT
R eRh
GGEE 2
12
2
220 44
(echo from air-ground interface)
(echo from buried target)
GT – Gain of transmit antennaGR – Gain of receive antennaER – Electric field strength at the receiver E0 – Transmitted Electric field strength.h – Height of antenna above groundd – Depth of target below the surface – Wavelength in Free SpaceRCS – Target Radar Cross Section
002 k (Propagation Constant
Above the ground)
*This model is for the antenna directly above the buried object.
2.1 GPR Phenomenology
2
1
22
2
112
1
2
1
22
2
112
1
r
rR
1
1
11
12
r
T
1
221
r
T
1
1
212
r Slightly-
Conducting Media
Approximation
-
Along Track [m]
Dep
th [
inch
es]
-0.5 0 0.5 1
-15
-12
-9
-6
-3
0
3
Synthetic Aperture
AntennaPattern
Data collected in time and space.
2.1 GPR Phenomenology
-
Along Track [m]
Dep
th [
inch
es]
-0.5 0 0.5 1
-15
-12
-9
-6
-3
0
3
Simulated Data(“x-t” domain)
-Earth’s
Surface x
z
(0,0.5)
x
z
Point Target
(0,6”)
-
2.1 GPR Phenomenology
Unimaged Signature
Metal CasingHeight: 6”Width: 13”Depth: 6”
TM-62M Landmine
X
Z
TM-62M at 6”
2.2 EMI Phenomenology
Air
Ground
Primary MagneticField
BuriedSphere
CurrentSource
Electronics& Sampler
DataStorage
I
V+
_
EMI Wire Coil
I
V+
_
EMI Wire Coil Simplified EMISystem Concept
Air
Ground
Source
SecondaryMagnetic
Field
Source H-field Incident Field at Object Metal Object Reaction
duruJeum
zyxH hd
u
z )(2
),,( 0)(
0 21
30
021
duruJeum
zyxH hd
u
r )(2
),,( 1)(
0 21
210
021
)( 111122
1 ju
)( 222222
2 ju
Air
Ground
Source
Source H-field
(x,y,-d)
(x,y,h)
2.2 EMI Phenomenology
),,(),,,(2 03
ssszssz zyxHaPam
),,(),,,(2 03
sssrssr zyxHaPam
))sinh()cosh()(sinh())cosh()(sinh(
))sinh()cosh()(sinh())cosh()(sinh(2),,,(
20
20
s
sss aP
)( ssia
Metal Object Reaction
SecondaryMagnetic
Field
pr
pz
duruJeum
zyxH hz
u
zzz )(
2),,( 0
)(
0 21
321
duruJeum
zyxH hz
u
rrz )(
2),,( 1
)(
0 21
21 21
2.2 EMI Phenomenology
* Model assumes a solid spherical target.
zzzzxxzx pHHpHHv 00
InducedMagnetic
Sources
px
pz
* Model no longer assumes a solid spherical target.
H0x – Horizontal magnetic field at the center of the target produced by the source magnetic dipole.
Hxz – Vertical magnetic field at the receive coil produced by the horizontal induced magnetic dipole.
H0z – Vertical magnetic field at the center of the target produced by the source magnetic dipole.
Hzz – Vertical magnetic field at the receive coil produced by the vertical induced magnetic dipole.
z
x
p
p TargetMagneticPolarizabilityVector
2.2 EMI Phenomenology
EMI Spatial
Signature
2.2 EMI Phenomenology
Coi
l Num
ber
(Acr
oss
Tra
ck)
Along Track
12345678910111213141516
Depth: 1”
Depth: 3”
EMI Spatial
Signature
2.2 EMI Phenomenology
Screener Stage
FeatureExtraction Stage
Discriminant Stage
Feature Vector
2.3 Overview of Approach
Screener: Points-of-Interest (POI) are detected and reported. This stage must be fast and must detect all landmines, but can have false-alarms.
Discriminant: Combines object features into a test statistic.
Features: Aspects of the detected objects are characterized in a vector of feature values.
POI
2.3 Overview of Approach:Screener Stage
Point-of-InterestList
2.3 Overview of Approach:Feature Extraction
Index X Location Y Location
1 291456.6558 4227053.1692
2 291382.6225 4227053.3659
3 291354.7422 4227052.5429
.
.
.
N 291309.1396 4227060.2448
GPR Features Depth Width Height RCS
EMI Features Magnetic Dipole Moments Decay Rates
Extracted EMI Chip
EMI Data
4227052.5429291354.7422
POI List EMI Data
Extracted GPR Cube
To Discriminant
Function
Feature Vector
Tra
ined
Sta
tistic
2.3 Overview of Approach:Discriminant Function
• The QPD can be thought of as a mapping. The feature vector (x1,x2) is mapped into a statistic “s” based on the training of the coefficients (c1,c2,c3,c4,c5,c6).
• The feature values are scalar numbers describing object: X1 - Feature Value 1 (Like: object diameter) X2 – Feature Value 2 (Like: object depth)
OutputStatistic
Quadratic Polynomial Discriminant Function(Shown here for 2 features.)
Outline
1. Application Overview 1.1 Data Collection 1.2 Metal and Plastic Landmines2. Sensor Phenomenology 2.1 Ground Penetrating Radar (GPR) 2.2 Electromagnetic Induction (EMI) 2.3 Overview of Approach3. Metal Landmine Detection 3.1 GPR Signature Features 3.2 EMI Signature Features4. Plastic Landmine Detection 4.1 Plastic Landmine Detection Difficulty 4.2 Hyperbola Flattening Transform 4.3 GPR Signature of Plastic Landmines 4.4 Metal Firing Pin Detection5. Adapting to Changes in Environment6. Current Progress
EMISimple
Threshold -kImaging
(Size/Depth)
EMIPolarization
Vector& Decay
Rate DetectionList
GPR DataDiscriminant
Function
EMI Data
Y/N
Proposed Architecture for Metal Landmine Detection
Feature Extractor
3. Metal Mines: Algorithm
POI Detector
Adaptive EnvironmentalParameter Estimation
Azimuth
FFT
After Azimuth FFT
-60 -40 -20 0 20 40 60
30
40
50
60
70
80
After 2D Phase Compensation
-60 -40 -20 0 20 40 60
30
40
50
60
70
80
(Kx,Kz) Domain after Stolt Interpolation
-60 -40 -20 0 20 40 60
20
30
40
50
60
70
80
Focused Image
-1.5 -1 -0.5 0 0.5 1 1.5
-1.6
-1.4
-1.2
-1
-0.8
-0.6
-0.4
-0.2
0
0.2
0.4
2D
Phase
Comp
Stolt
Interp
2D
FFT
After Azimuth FFT
-60 -40 -20 0 20 40 60
30
40
50
60
70
80
After 2D Phase Compensation
-60 -40 -20 0 20 40 60
30
40
50
60
70
80
(Kx,Kz) Domain after Stolt Interpolation
-60 -40 -20 0 20 40 60
20
30
40
50
60
70
80
Mechanics ofWavenumber
Migration
3. WavenumberMigration Imaging
Place in -k
Format
2D Phase Comp.
StoltInterp.
2DFFT
HyperbolicPointTarget
FocusedPoint
Target
R(kx,) D(kx,kz)R(kx,)F(kx,,)
Metal CaseHeight: 6”Width: 13”Depth: 6”
TM-62M Landmine Depth and Azimuth Resolution
r r d
variation median inches
Air 1 1 3.94
Dry Sand 4-6 5 1.76
Wet Sand 10-30 20 0.88
Dry Clay 2-5 3 2.27Wet Clay 15-40 27 0.76
B
c rd 2
/
02
/
f
c ra
3.1 GPR Signature
B = 1.5GHzf0 = 1.25GHz = 60°
Unimaged Signature
De
pth
[In
che
s]
Along Track [Inches]
Signature before imaging is dominated by the standard hyperbola.
Depth can be determined if data is properly calibrated. Size requires imaging to estimate.
“Convexity” of signatures is determined by the speed of propagation in the medium.
3.1 GPR Signature
Image
De
pth
[In
che
s]
Along Track [Inches]
Imaged signature shows reflections from the top and bottom of the landmine.
Length of the object can now be estimated from the length of the top and bottom reflections.
Height of the object can be estimated from the distance between the two reflections.
Depth has been calibrated during the imaging process.
3.1 GPR Signature
Image
De
pth
[In
che
s]
Along Track [Inches]
BottomReflection
TopReflection
6”
13”
Estimated Depth and Size
Depth: 5.7” Length: 11.3” Height: 6.8”
Ground Truth
Depth: 6” Length: 13” Height: 6”
3r (Dry Clay)
About 3 res. cells across target in depth.
3.1 GPR Signature
Objects Reported
BottomObject
TopObject
De
pth
[In
che
s]
Along Track [Inches]
2
3
1
4
Four objects are identified by setting a threshold and clustering connected pixels.
Objects 1 and 2 are clearly above the ground and can be eliminated.
Objects 3 and 4 are the top and bottom reflections.
3.1 GPR Signature
6.8”
Objects Reported
De
pth
[In
che
s]
Along Track [Inches]
10.8”
12.5”
Length is estimated by averaging the lengths of the two reflections. (Est. Length: 11.3”)
Height is the distance between the two reflections. (Est. Height: 6.8”)
Depth is the distance from the ground surface (0”) to the top reflection. (Est. Depth: 5.7”)
5.7”
3.1 GPR Signature
Repeatability Study
Ten SignaturesBefore Imaging
3.1 GPR Signature
Repeatability Study
Ten SignaturesAfter Imaging
3.1 GPR Signature
3.1 GPR Signature
Repeatability Study
Ten SignaturesBinarized
Length [inches]
Height[inches]Number
1 12 6.8 6.7
2 11.3 6.8 5.6
3 11.3 6.8 5.6
4 18 6.8 5.6
5 14 6.8 6.7
6 11.3 5.7 6.7
7 10.7 5.7 6.7
8 9.3 6.8 6.7
9 11.3 5.7 6.7
10 10.7 6.8 6.7
Note: Depth Sample Spacing: 1.1”
Depth[inches]
Ground Truth: Depth: 6” Length: 13” Height: 6”
3.1 GPR Signature
Repeatability Study
Magnetic Polarizability
npHv
vHHHp
pTT
y
x 1
ˆ
ˆ
np
pHHHHv
z
xzzzxzx
00
(signal model)
(N Samples)
(Least Squares Estimator)
zzzzxxzx pHHpHHv 00
•To compute the H matrix, we must know the depth of the target.
3.2 EMI Signature
z
x
p
p
• GPR (Radar) gives depth information
• EMI (Dipole models) give H matrix values
• Combining these: Multi-modal detection
• Synergy: Each helps the other work better
3.2 EMI Signature
InducedMagnetic
Sources
px
pz
0.669ˆ xp
5.324ˆ zp
3.2 EMI Signature
3.2 EMI Signature
Iron Sphere
Aluminum Plate
No Target Present
time
AmpsTarget Present
Decay Rate Discriminant
3.2 EMI Signature
Aluminum Objects
Iron Objects
Time [ms]
No
rma
lize
d R
esp
on
se
tN
nn
neAtr
1
)(
• Sum of Decaying Exponentials (Prony):
• N=2 is usually enough
• Decay Rate Features:
1A
2A12
3. Metal Mines Summary
• Decay Rate Features:
1A
2A12
xp zp• Magnetic Polarizability:
EMI Features
Depth Length
Height
GPR Features
• -k Imaging Features:
• Other Features:
RCS
Outline
1. Application Overview 1.1 Data Collection 1.2 Metal and Plastic Landmines2. Sensor Phenomenology 2.1 Ground Penetrating Radar (GPR) 2.2 Electromagnetic Induction (EMI) 2.3 Overview of Approach3. Metal Landmine Detection 3.1 GPR Signature Features 3.2 EMI Signature Features4. Plastic Landmine Detection 4.1 Plastic Landmine Detection Difficulty 4.2 Hyperbola Flattening Transform 4.3 GPR Signature of Plastic Landmines 4.4 Metal Firing Pin Detection5. Adapting to Changes in Environment6. Current Progress
HFTDetectionAlgorithm
-kImaging
(Size/Depth)
EMI(Firing Pin)
DetectionList
GPR Data
DiscriminantFunction
EMI Data
Y/N
POI Detector
Proposed Architecture for Plastic Landmine Detection
Feature Extractor
4. Plastic Mines: Algorithm
Adaptive EnvironmentalParameter Estimation
4.1 Plastic Mine Detection
GPR Standard Detection Statistic – Standard Deviation Over Depth Bins
• The standard detection approach is to create the “plan view” image below by taking a standard deviation over depth.
• Using this statistic there are many false alarms, but most mines are detected. Deeply buried plastic mines, however, are often missed.
3x10-3
34 Deeply Buried VS1.6 Mines
VS1.6 Max Pixel Histogram
3x10-3
34 Deeply Buried VS1.6 Mines
VS1.6 Max Pixel Histogram3x10-3
PDF Estimated from Histogram
3x10-43x10-4
3x10-3
Background StatisticsPDF Estimated from Histogram
3x10-43x10-4
4.1 Plastic Mine Detection
Pro
babi
lity
of
Det
ecti
on
Probability of False Alarm
ROC Curve
Deeply Buried VS1.6(Depth <3”)
• About 80% of deep VS1.6 plastic mines are detectable.
4.1 Plastic Mine Detection
Plastic Landmine (VS1.6)Surface
Top ofMine at 6”
SoilStratum
Deeply buried plastic landmines face a low signal-to-noise ratio (SNR).
Strata in the ground can create large radar returns that lead to false alarms.
The Hyperbola Flattening Transform seeks to exploit all the “energy” of the hyperbolic signature.
4.1 Plastic Mine Detection
Simulation Simulation
Original Hyperbola 45° Rotation
Simulation Simulation
Remapping: 1/yy
12
2
2
2
a
x
d
y 1xy 1y
x
The Hyperbola Flattening Transform converts a hyperbolic signature into a straight line at 45°.
4.2 Hyperbola Flattening
Mathematical Description
180°
90°
0°
120° Radon Transform illustration
shows a projection for 120° from a circle.
4.2 Hyperbola Flattening
Application to Simulated Data
The RADON transform creates “projections” by summing along lines.
Projections are oriented for 0° to 180°.
Radon Transform of the “flattened” hyperbola has a strong maximum at 45° corresponding to the “energy” contained in the hyperbola.
4.2 Hyperbola Flattening
Application to Simulated Data
4.2 HyperbolaFlattening
Application to Real Data
Transform Location ofHyperbolic Signature
4.2 Hyperbola Flattening
4.2 HyperbolaFlattening
VS1.6
Along Track
Dep
th
The HFT will now be applied as a detector.
A small kernel is moved throughout the scene. At each location, the HFT is applied.,
At each point the HFT is run for several values of the “a” parameter. The maximum result is placed into a detection image.
Original Image
4.2 HyperbolaFlattening
Algorithm Application
VS1.6
The HFT is applied to all locations in the scene. The detection image shown here is the result.
Bright pixels correspond to hyperbolas. Hyperbolic signatures have been contrast enhanced, while non-hyperbolas are suppressed.Along Track
Dep
th
Hyperbola Detection Image
4.2 HyperbolaFlattening
Algorithm Application
VS1.6
Along Track
Dep
th
Pixels that break a certain threshold are shown. These pixels reveal the locations of the “most hyperbola-like” signals in the scene.
The region corresponding to the VS1.6 has been enhanced by the HFT detector.
Algorithm ApplicationHyperbola-like Regions
4.2 HyperbolaFlattening
VS1.6 at 1”
4.3 GPR Signature
M19 at 5”
4.3 GPR Signature
12345678910111213141516
Coi
l Num
ber
(Acr
oss
Tra
ck)
Along Track
Firing PinDetection
Landmines contain a small amount of metal in the firing pin.
*The data here has been non- linearly altered. (That is, 3 square roots have been applied.)
Plastic Metal Metal
EMI Data
4.4 Firing Pin
VS2.2 at 1” TM-62P at 2” VS1.6 at 1”
Firing PinDetection
All These Landmines are Plastic.Nevertheless, an EMI signal is attainable.The sensor sled was lowered to just 2” above the ground.
EMI Spatial Signature EMI Spatial Signature EMI Spatial Signature
4.4 Firing Pin
4. Plastic MineSummary
• Decay Rate Features:
1A
2A12
xp zp• Magnetic Polarizability:
EMI Features
Depth? Length
Height
GPR Features
• -k Imaging Features:
• Other Features:
RCS
0
1fp
• Firing Pin Detection (binary):
(detected)
(not-detected)
Outline
1. Application Overview 1.1 Data Collection 1.2 Metal and Plastic Landmines2. Sensor Phenomenology 2.1 Ground Penetrating Radar (GPR) 2.2 Electromagnetic Induction (EMI) 2.3 Overview of Approach3. Metal Landmine Detection 3.1 GPR Signature Features 3.2 EMI Signature Features4. Plastic Landmine Detection 4.1 Plastic Landmine Detection Difficulty 4.2 Hyperbola Flattening Transform 4.3 GPR Signature of Plastic Landmines 4.4 Metal Firing Pin Detection5. Adapting to Changes in Environment6. Current Progress
EiEs
Et
R12 = Ei
Es
10
2 = r 0
r
rR
1
1
11
12
5. Adapting to Environmental Changes
• Measuring Dielectric Constant of a material is done using the reflection coefficient.
• Reflection Coefficient
r r
variation medianAir 1 1
Dry Sand 4-6 5
Wet Sand 10-30 20Dry Clay 2-5 3
Wet Clay 15-40 27
• r is frequency independent for 500 MHz < f < 2.0GHz
2
12
12
11
11
R
Rr
Reflection Coefficient
• Solving for r is non-linear
• Therefore, estimates of r are very sensitive to noise in the observations of R12.
5. Adapting to Environmental Changes
4rnR 33.012
128 Frequencies
r After Conversion to r:
3.4ˆ r
'4ˆ nr
Sample Mean – Biased Estimate
5. Adapting to Environmental Changes
Example – Dry Soil (r small)
• Reflection Coefficient for 128 Frequencies is contaminated with Gaussian Noise.
• Variance at a single frequency is large, so all 128 must be combined in some way to reduce the estimate variance.
222.0128
)ˆvar()ˆvar( r
r
n~N(0,0.01) (SNR = 10dB)
n’~X1?(0,3.6)
40r4r
• Simple First Attempt at Adaptive Filter
• Averages r of 50 locations along track
• Performed acceptably for r = 4
r rEstimateFrom 128Frequencies
AdaptiveFilter Output
5. Adapting to Environmental Changes
• Estimation of r is a challenge.
• Utilize all available information:• 128 Frequencies• 20 Antennas• Multiple Locations Along Track
• Characterize Noise after Conversion to r
X[i] = r + n[i] n~? (How is “n” distributed?)
5. Adapting to Environmental Changes
• Determine Unbiased Estimator for r given non-Gaussian nature of noise using 128 frequencies (maximum likelihood)
• Possibly incorporate a priori information (max. a posteriori)
Approach to Adaptive Processing of r Changes
Outline
1. Application Overview 1.1 Data Collection 1.2 Metal and Plastic Landmines2. Sensor Phenomenology 2.1 Ground Penetrating Radar (GPR) 2.2 Electromagnetic Induction (EMI) 2.3 Overview of Approach3. Metal Landmine Detection 3.1 GPR Signature Features 3.2 EMI Signature Features4. Plastic Landmine Detection 4.1 Plastic Landmine Detection Difficulty 4.2 Hyperbola Flattening Transform 4.3 GPR Signature of Plastic Landmines 4.4 Metal Firing Pin Detection5. Adapting to Changes in Environment6. Current Progress
6. Current Progress
Wavenumber Migration Processor GPR Point Target Simulator Successful Imaging of Metal Landmines Successful Imaging of Plastic Landmines
GPR Feature Set Identify Metal Landmine GPR Feature Set Identify Plastic Landmine GPR Feature Set Automated Extraction of GPR Metal Features Automated Extraction of GPR Plastic Features
Plastic Landmine Detection Evaluate Baseline Performance with ROC Curve
Implement the Hyperbola Flattening Transform Enhance Processing Speed of the HFT Evaluate HFT Performance using ROC Curves
6. Current Progress
Physical Signal Modeling EMI Simple Target Simulator (dipole induction) Study effect of soil conductivity on measured signature.
EMI Feature Set Identify Metal Landmine EMI Feature SetP Use Least Squares to Estimate Magnetic Polarization FeaturesP Measure decay rates of iron and aluminum objects. Identify Firing Pin Detection Features Spectral Noise Whitener for Firing Pin Detection Automated Extraction of EMI Metal Features Automated Extraction of EMI Firing Pin Features
Adaptive Estimation of r
Estimation of r from GPR scattering measurements.
Determine statistical model of noise in r observations.
Investigate MLE and MAP estimators for r
6. Current Progress