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IMAGE RECONSTRUCTION

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Title: IMAGE RECONSTRUCTION


1
IMAGE RECONSTRUCTION
  • A brief background
  • By DINESHBABU V DINAKARABABU
  • 15th October 2007

2
What is Digital Image Processing?
  • Can any one of you come up with a simple
    definition?

3
What is Digital Image Processing?
  • Processing of a 2-D picture by a digital
    computer.
  • In a broader context, it is the digital
    processing of a 2D-data.
  • Digital image is an array of real or complex
    numbers represented by a finite number of bits.

Remote Sensing
Robotics
Medical Imaging
Radar
4
Classes of problems
  • Many applications but lots of problems
    associated with image processing
  • 1. Image representation and modeling
  • 2. Image Enhancement
  • 3. Image restoration
  • 4. Image Analysis
  • 5. Image Reconstruction
  • 6.Image Data Compression

Image Analysis
Image Data Compression
Image Reconstruction
5
Image reconstruction from projections
  • Special class of image restoration problems
  • 2 or higher dimensional object is reconstructed
    from several 1-D projections
  • Projection obtained by projecting X-ray beam
    through object
  • Important in medical imaging ( CT Scanners ),
    astronomy, radar imaging, geological exploration
    and non-destructive testing of assemblies
  • We focus on the medical imaging applications.
  • Lots of algorithms available.
  • This problem can be set up mathematically in the
    framework of Radon transform theory ( We will
    deal with it in a short while )

6
What is projection?
  • Shadowgram obtained by illuminating an object by
    penetrating radiation
  • Each pixel on the projected image represents the
    total absorption of the X-ray along its path from
    source to detector
  • Rotate the source-detector assembly around the
    object projection views for several different
    angles can be obtained.
  • Reconstructing a cross-section of an object from
    several images of its transaxial projections an
    important problem to be addressed in image
    processing
  • Goal of image reconstruction is to obtain an
    image of a cross-section of the object from these
    projections.

7
CT Scanners
  • Imaging systems that generate such slice views
    are called computerized tomography scanners
  • Resolution lost along path of X-rays while
    obtaining projections
  • CT restores this resolution by using information
    from multiple projections.
  • Special case of image restoration

8
Imaging Techniques
  • Transmission Tomography
  • Reflection Tomography
  • Emission Tomography
  • Magnetic Resonance Imaging
  • Projection-based image processing

9
Radon Transform
  • Provides mathematical framework for going back
    and forth between the spatial coordinates (x,y)
    and projection-space coordinates (s,?)
  • Radon transform of f(x,y) is g(s,?)
  • Line integral along a line inclined at an angle ?
    from the y-axis and at a distance s from the
    origin.
  • Mathematical expression

10
Radon Transform
  • Rotated coordinate system (s,u)
  • G(s,?) is called ray-sum
  • Represents summation of f(x,y) along a ray at a
    distance s and at an angle ?
  • Each point in (s,?) domain corresponds to a line
    in (x,y) domain
  • (s,?) Not polar coordinates

11
The Back Projection Operator
  • Defined by the mathematical expression
  • b(x,y) called the back-projection of g(s,?)
  • Can be written in polar co-ordinates as
  • Represents the accumulation of the ray sums of
    all of the rays that pass through (x,y) or (r,F)

12
Parallel-Beam Backprojection An FPGA
ImplementationOptimized for Medical Imaging
  • Radon Transform and Back-Projection Operator
  • Mathematical Frameworks needed for Image
    Reconstruction
  • Lets proceed to the Reconstruction Algorithm and
    the FPGA implementation

13
What the authors present?
  • FPGA implementation of the parallel-beam
    backprojection algorithm
  • Explore a number of quantization issues
  • Minimizing error while maximizing efficiency
  • Reference
  • Parallel-Beam Backprojection An FPGA
    Implementation Optimized for Medical Imaging
  • by Srdjan Coric, Miriam Leeser, Eric Miller
  • Department of Electrical and Computer
    Engineering
  • Northeastern University
  • Boston, MA 02115

14
Filtered Backprojection
  • Called Filtered Backprojection (FBP) as we are
    filtering the projections using a high-pass
    filter before the actual backprojection.
  • Most commonly used approach for image
    reconstruction
  • Dense projection data
  • Parallel-beam and fan-beam variations depends
    on x-ray beam
  • we focus on parallel-beam Backprojection
  • Computationally intensive process
  • Highly parallelizable process

15
Challenges facing FBP
  • Computationally intensive process
  • - an image of size n n complexity is O(n3)
  • - upto order n2log2 n
  • Difficulty in producing high resolution images
  • - density of each projection
  • - total number of projections be large
  • High precision reconstructions difficult
  • - analyze the effects of quantization
  • - fixed-point implementation with properly
    chosen bit-widths
  • - bit reduction of intermediate results for
    different rounding schemes

16
Parallel-Beam Backprojection
  • Finds widespread application in medical imaging
  • Computationally intensive algorithms requiring
    the rapid
  • processing of large amounts of data
  • Can benefit greatly from hardware acceleration
  • Reconfigurable hardware has not been applied to
    this important area
  • Efficient implementation and maximum speedup -
    fixed-point implementations are required
  • Associated quantization errors must be carefully
    balanced against the requirements
  • Visual quality of image not compromised.

17
PARALLEL-BEAM FILTEREDBACKPROJECTION
  • Parallel-beam CT scanning system
  • an array of equally spaced unidirectional sources
    of focused X-ray beams
  • radiation reaches a collinear array of detectors
  • Spatial variation of the absorbed energy in the
    two-dimensional plane through the object is
    expressed by the attenuation coefficient µ(x, y).
  • set of values given by all detectors comprises a
    one-dimensional projection of the attenuation
    coefficient, P(t, ?)
  • t is the detector distance from the origin
  • ? is the angle at which the measurement is taken

18
Radon and Inverse Radon Transform
  • Io is the source intensity
  • Id is the detected intensity
  • d() is the Dirac delta function
  • Radon transform represents an operator that maps
    an image µ(x, y) to a sinogram P(t, ?)
  • Inverse mapping-Inverse Radon transform which
    when applied to a sinogram gives an image
  • FBP algorithm uses this mapping

19
Discrete formulation of Backprojection and the
algorithm
  • ??(t) is a filtered projection at angle ?
  • K is the number of projections taken during CT
    scanning at angles ?i over a 180
  • Algorithmically, this equation is implemented as
    a triple nested for loop
  • Outermost loop is over projection angle, ?
  • For each ?, we update every pixel in the image in
    raster-scan order starting in the upper left
    corner and looping first over columns, c, and
    next over rows, r.
  • the pixel at location (r,c) is incremented by the
    value of ??(t) where t is a function of r and c

20
Linear Interpolation
  • The issue here is that the X-ray going through
    the currently reconstructed pixel, in general,
    intersects the detector array between detectors.
  • So, use linear interpolation.
  • point of intersection is calculated as an address
    corresponding to detectors numbered from 0 to
    1023 (i)
  • fractional part of this address is the
    interpolation factor
  • interpolation can be performed beforehand in
    software or it can be a part of the
    backprojection hardware itself
  • Implementation in hardware done
  • - reduces the amount of data that must be
    transmitted to the reconfigurable board
  • - interpolation in hardware is much faster
  • equation that performs linear interpolation is
    given by

21
Illustration of the coordinate system used in
parallel-beam backprojection
22
Geometrical explanation of the incremental
spatial address calculation
23
Quantization
  • Quantization here indicates the conversion of
    floating point variables to fixed point variables
    of proper bit-width.
  • Quantize all our data and calculations to
    increase the speed and decrease the resources
    required for implementation.
  • Determining allowable quantization is based on a
    software simulation of the tomographic process.
  • Quantization error compare a fixed-point image
    reconstruction with a floating a fixed-point
    image reconstruction with a floating-point one.
  • Quantization should not result in loss of
    numerical accuracy and hence a change in the
    visual quality of the image.
  • Possibilities for bit reduction on the outputs of
    certain functional units

24
Representation of fixed point variables
  • V is an arbitrary real number
  • Va is its fixed-point approximation
  • Q is an integer that encodes V
  • S is the slope
  • B is the bias
  • Fixed-point versions of the sinogram and the
    filtered sinogram use slope/bias scaling where
    the slope and bias are calculated to give maximal
    precision

25
Quantization of two variables
  • ws is the word size in bits of integer Q
  • Round represents rounding to nearest
  • min(V) min(Q) B 0 for unsigned numbers
  • For a given sinogram, S and B are constants and
    they do not show up in the hardware only the
    quantization value Q is a part of the hardware
    implementation
  • Interpolation factor is an unsigned fractional
    number - uses radix point-only scaling

26
Relative Error
  • N is the total number of pixels
  • xi and yiFP are the values of the i-th pixel in
    the quantized and floating-point reconstructions

27
Simulation steps for quantization
  • Reproject Generates a sinogram of 1024
    projections and 1024 samples per projection.
  • Filter Sinogram data convolved with the impulse
    response of the ramp filter generating a filtered
    sinogram.
  • Backproject Backprojecting the filtered
    sinogram to give a reconstructed image.

28
Detailed flowchart of the simulation process
  • Different quantization steps possible are shown
    in the figure above
  • Each path represents a separate simulation cycle.

29
Hardware Organization
  • Hardware acceleration in reconfigurable hardware
    - parallel processing
  • Two basic sources of parallelism
  • Pixel parallelism - image can be divided into
    subsections which can be reconstructed
    simultaneously
  • Projection parallelism simultaneously
    processing individual projections
  • Pixel parallelism limited by available memory
    bandwidth
  • We concentrate on projection parallelism.

30
Data flow of backprojection hardware
  • Three flows of data going on simultaneously
  • - Pipeline flow
  • - Sinogram data flow
  • - Accumulation data flow

31
Datapath implementation of the non-parallel
backprojection hardware
32
Datapath of the implemented 4-way parallel
backprojection hardware
33
Image comparison grayscale range mapped to a
part of the pixel value range
34
RESULTS AND PERFORMANCE
35
CONCLUSION
  • FPGA implementation of parallel-beam
    backprojection algorithm
  • Analysis of quantization effects caused by finite
    bit-widths
  • Paid special attention not to compromise the high
    precision requirements
  • 20 times speed-up over a similar software
    implementation
  • Worst case relative error of 0.015 compared to a
    floating-point implementation
  • Real time image reconstruction is easily
    attainable by exploiting parallelism.
  • Hardware architecture presented can easily be
    modified to different bit-widths for different
    sensors and applications
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