microwave radar-based differential breast cancer 2003

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    MICROWAVE RADAR-BASED

    DIFFERENTIAL BREAST

    CANCER IMAGING

    Presented By

    PRIBIN CHACKO

    T7

    7941

    Guided By

    Mrs. Preetha

    Basu

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    ABSTRACT

    An improved antenna is presented for radar-basedbreast cancer imaging. The improvement was achievedby increasing the number of antennas in the array to 31elements, as well as by improving the antenna design

    itself. Using an experimental setup, with homogeneouscurved breast phantoms, we have demonstratedsubstantial imaging improvement with the newantenna array. The new system is also able to detect7mm-diameter tumour phantoms in any location withinthe breast, even as close as 4mm from the skin layer.

    Additionally, we have shown good imaging results inlow contrast scenarios, where the dielectric contrastbetween tumour and normal tissue was reduced to 2:1.Presented results clearly demonstrate the large impactof antennas characteristics on imaging performance. 2

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    CONTENTS

    INTRODUCTION

    UWB ANTENNA DESIGN

    ANTENNA ARRAY DESIGN

    3D RADAR IMAGING SETUP

    a. Measurement setup

    b. 3D breast phantom

    c. Differential imaging and focusing algorithm

    3D IMAGING RESULTS

    a. Comparison with previous antenna arrayb. Location-independent imaging using the new

    antenna array

    c. Low-contrast imaging using new antenna array

    CONCLUSIONS3

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    INTRODUCTION

    Breast cancer is cancer originating breast fromtissues.

    Most commonly found in middle-aged womens.

    This paper discusses an application of microwaves for

    medical imaging (for cancer detection).

    Two main approaches to microwave breast imaging:

    1. Microwave tomography and

    2. Radar-based imaging

    Radar based imaging technique is applied in theproposed method.

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    PRINCIPLE

    The cancer detection is based on a difference in theelectrical properties of normal and malignant breasttissues

    The early work on breast cancer detection was based

    on the assumptions of1. High (about 5:1) dielectric contrast, as well as

    2. Relatively homogeneous (electrically) internalbreast structure

    The most recent studies indicates that that the

    contrast might be significantly lower, and also thatthe breast interior is more inhomogeneous thanpreviously assumed.

    So breast imaging is much more challenging thanpreviously thought

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    PRINCIPLE (CONTD)

    Breast phantoms are developed from the MRIscanning images of the breast.

    The breast electrical properties differ at the same

    level as pixel intensity of MRI images.

    The more challenging process is to build a real breast

    phantom with the same tissue complexity as in

    numerical MRI-based phantoms.

    All experimental phantoms reported so far assume

    homogeneous breast tissue and only some include the

    very important skin layer. In this paper a new antenna array with 31 elements

    is presented, designed for microwave radar-based

    breast imaging. 6

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    PRINCIPLE (CONTD)

    System is based on multi-static radar operation Previous prototype used a 16-antenna array, formed

    on a section of a hemi-sphere to conform well to the

    breast shape.

    Here the no. of antenna is increased and antennadesign is improved.

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    UWB ANTENNADESIGN

    A new improved antenna is selected.

    Here we use UWB-Ultra Wide Band antenna.

    The main advantages of wide-slot UWB antenna

    are

    a. low-profile and excellent transientcharacteristics for a wide range of radiation

    angles.

    The main advantages of the new design are

    a. stable radiation pattern across the frequencyband of interest.

    b. extremely high fidelity (>95%) of radiated

    pulses for radiation angles even up to 600

    from bore-sight.

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    ANTENNA ARRAY DESIGN

    A. Old Array

    The old antenna array

    design is modified for

    improving the

    performance The old array contain

    only 16 antennas

    Arranged on a section of

    a hemi-sphere to conformwell to the breast shape.

    Old prototype: 16-element array based

    on the stacked-patch antenna 9

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    ANTENNA ARRAY DESIGN (CONTD)

    B. New Array

    New antenna array isformed around the lowerpart of a 85mm-radiussphere

    3D CAD software is used forthe new array design.

    To provide the best radiationcoverage of a breast, allantennas were positioned topoint towards a centre of

    curvature. A plastic shell, with

    openings for the antennas,has been manufactured toassure the best possibleaccuracy of positioning

    antennas

    New prototype: 31-element array based

    on

    the wide-slot antenna.

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    ANTENNA ARRAY DESIGN (CONTD)

    Schematic of the array modelled using CAD software11

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    3D RADAR IMAGING SETUP

    A. IMAGING SETUP The array is connected with coaxial cables to a

    custom-built network of electromechanical switches

    The bank of switches selects all possible pairs of

    antennas within the array, and connects them in turn

    to a vector network analyser (VNA)

    The VNA performs the radar measurement in the

    frequency-domain

    In a post-reception step, all measured data is

    transformed into the time-domain.

    With thirty one antenna elements in the array, four

    hundred and sixty five independent measurements

    (multistatic radar signals) are recorded. 13

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    IMAGING SETUP (CONTD)

    A computer controls both the VNA and the switch

    bank

    The measurement takes about 80 seconds to

    complete.

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    IMAGING SETUP (CONTD)

    Experimental setup of our imaging

    system.

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    3D BREASTPHANTOM

    For experimental testing a 3D model of thebreast is developed.

    during measurements the antennas are

    immersed in a matching liquid, to reduce

    reflections from the skin and for a more compactantenna design.

    The matching liquid must be able to simulate the

    properties of normal breast-fat.

    The matching and normal breast tissueequivalent liquid has a relative dielectric

    constant of about 10 and an attenuation of 1.2

    dB/cm at 6GHz. This material is also dispersive.16

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    ALTERNATIVE FOR MATCHING LIQUID

    As an alternative to the lossy matching liquid we canuse a ceramic shell to fill the distance between

    antennas and a breast skin.

    A 1mm thin layer of matching liquid still needs to be used

    between antennas and the ceramic shell.

    To accommodate breasts of different size, ceramic

    insert shells are used.

    The ceramic matching shell and inserts are designed,

    using low loss material with controlled dielectric

    constant (r=10) material Eccostock HiK500F fromEmerson&Cuming.

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    DEVELOPMENT OF SKIN PHANTOM

    The skin layer is 2mm thick, it is a part of a 67mm-

    radius hemi-sphere.

    When the skin phantom is fitted into the array it lies

    20mm above antenna elements. This distance betweenantennas and breast provides a full coverage of a

    breast by an antenna radiation pattern.

    The skin layer material is dispersive and, at 6 GHz, it

    has a relative dielectric constant of 30 and attenuation

    of 16 dB/cm.

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    CONSTRUCTION OF TUMOR PHANTOM

    Tumour phantom is constructed from a material with

    a relative dielectric constant close to 50.

    Conductivity of the material is 7 S/m (at 6GHz).

    The contrast between dielectric properties of breast

    fat and tumour phantom materials is around 1:5.

    Recently published data on the electromagnetic (EM)

    properties of breast tissues suggest that the contrast

    might be significantly lower, and also that the breastinterior is more inhomogeneous than previously thought

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    DIFFERENTIALIMAGING

    To obtain tumour response from the measured

    data we perform two measurements by rotating

    the array

    This method provides a differential signal, whichis used as an input into focusing algorithm.

    Advantage of this differential imaging is that it

    does not require a background measurement.

    Thus it could be used in realistic scenarios with

    breast cancer patients.

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    FOCUSING ALGORITHM

    A modified delay and sum (DAS) algorithm is

    used to form 3D images of scattered energy.

    The scattered energy at the given focal point,

    within the breast volume, can be expressed as:

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    FOCUSINGALGORITHM (CONTD)

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    FOCUSINGALGORITHM (CONTD)

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    3D IMAGING RESULTS

    Comparison with previous antenna array A 10mm (diameter) tumour phantom, located at a

    position P(x=20, y=20, z=-20) is considered. In both

    cases we have used breast phantom as described

    earlier

    Phantom used with the 31-elements array had 9mm

    bigger radius (skin had r=67mm,for 16 element array

    r=58mm only.)

    16-element array was slightly smaller due to the fact

    that the whole array was formed as a part of spherewith radius 78mm, and the radius of the 31-element

    array was 85mm.25

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    COMPARISON (CONTD)

    To quantitatively assess imaging results, we introduce

    a measure of detection quality: ratio of the clutterenergy to the tumour energy, above a certain threshold

    t (C/Tt).

    The clutter energy is calculated within the entire 3-D

    image (hemi-sphere with 67mm radius), and is simply

    the sum of focused values exceeding threshold t in all

    pixels.

    The tumour energy is calculated as the sum of focused

    values above the threshold, for pixels located within a

    cube of 24x24x24mm3, with the maximum focusedsignal located in the centre of the cube.(volume where wecalculate the clutter is about forty five times larger than that of

    the tumour)

    Another measure for quantitative assessment of

    imaging results is a ratio of peak clutter energy to apeak tumour energy (peakC/T ), calculated within a full

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    COMPARISON (CONTD) 3D IMAGES

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    COMPARISON (CONTD)

    Looking at figures for the

    16-element and the 31-elements arrays we cansee that in both casestumour has been detected.

    A single artifact is also

    visible for the 16-elementarray.

    ? HOW THE FIGURES

    ARE PLOT?

    3D images are shown ascontour plots at -1.5dBcut-off (all values smallerthan -1.5dB of a maximumvalue are not shown).

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    COMPARISON (CONTD)

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    COMPARISON (CONTD) 2D IMAGES

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    COMPARISON (CONTD)

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    COMPARISON (CONTD)

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    COMPARISON (CONTD)

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    COMPARISON (CONTD)

    Use only sixteen antenna for focusing with new

    array with the positions closest to those from theold array

    35

    Same as old

    figure

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    COMPARISON (CONTD)

    As expected, there is more clutter in the image But these results are still significantly better than

    for the old array with the same number of

    antennas.

    36Old array New array

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    COMPARISON (CONTD)

    The above results let us finally draw a conclusionthat the superior imaging performance is due to

    a. The better antenna design, and

    b. The larger number of antennas, which provideslarger array aperture and higher diversity of

    the radar data.

    This is encouraging and suggest that animprovement could still be achieved by further

    working on the better antenna and by adding more

    antennas to the array. 37

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    LOCATION-INDEPENDENT IMAGING

    USING THE NEWANTENNAARRAY

    A malignant tissue can be located anywherewithin a breast.

    So investigations are done at several locations ofthe breast.

    3 locations are picked within +x/+y quadrant (dueto symmetry of the array). They are

    1. P1 (x=0,y=50,z=-30),

    2. P2 (x=50,y=0,z=-30),

    3. P3 (x=40,y=40,z=-30).All three positions represent challenging cases of

    tumours in a close proximity of the skin layer.Any other locations further away from a skin areeasier to detect

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    RESULTS

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    LOCATION-INDEPENDENT IMAGING(CONTD)

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    LOW-CONTRAST IMAGING USING NEW

    ANTENNAARRAY

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    LOW-CONTRAST IMAGING : RESULTS

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    LOW-CONTRAST IMAGING (CONTD)

    In all the cases the tumor detected without anyproblems.

    However, as the dielectric contrast decreases, clutter

    increases.

    The obtained peak C/T values are

    0.36 for a 5:1 contrast,

    0.54 for a 2.7:1 contrast, and

    0.69 for a 2:1 contrast.

    This gives almost 100% increase in peak C/Tvalue,

    when dielectric contrast decreases from 5:1 to 2:1.

    However, it does not prohibit successful detection.

    These results confirm that

    The lower dielectric contrast imposes additional

    challenges for microwave imaging modalities

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    CONCLUSIONS

    This paper presents the new improved antenna array forradar-based breast cancer imaging.

    Improvement was achieved by increasing the number ofantennas in the array as well as by designing new UWBantenna.

    Comparing to the previously used stacked-patch antenna,which have a planar size of 18x23 mm2, the new wide-slotantenna has a size 14x14 mm2.

    The main advantages of the new design over the patch are

    Stable radiation pattern across a frequency band ofinterest

    extremely high fidelity (>95%) of radiated pulses forradiation angles even up to 600 from bore-sight.

    significant imaging improvement with the new 31-antennasystem over the previous 16-element array 44

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    CONCLUSIONS (CONTD)

    With the low threshold level (-7dB) in 3D images,

    the 16-element array provided a low quality images

    with high clutter. Targets often remain

    unrecognized.

    For the new array images consisted only of tumour

    response with no artifacts. This is achieved by modifying the antenna design.

    The new system is able to detect 7mm diameter

    tumour phantoms in any location within the

    breast, even as close as 4mm from the skin layer. Good imaging results in low-contrast scenarios

    (2:1).

    To the best of my knowledge, the system presented

    in this paper is the most advanced experimental

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    REFERENCES

    E.C. Fear, P.M. Meaney, M.A. Stuchly, "Microwaves for breast cancer detection?", IEEEPotentials, Volume 22, Issue 1, Feb-Mar 2003 Page(s):12 - 18

    P.M. Meaney, K.D. Paulsen, A. Hartov, R.K. Crane, "Microwave imaging for tissueassessment: initial evaluation in multitarget tissue-equivalent phantoms", IEEETransactions on Biomedical Engineering, Volume 43, Issue 9, Sept. 1996 Page(s):878 890

    P.M. Meaney, M.W. Fanning, D. Li, S.P. Poplack, K.D. Paulsen, "A clinical prototype foractive microwave imaging of the breast", IEEE Transactions on Microwave Theory andTechniques, Volume 48, Issue 11, Part 1, Nov. 2000 Page(s):1841 1853

    P. M. Meaney, Q. Fang, Ch. A. Kogel, S. P. Poplack, P. A. Kaufman, K. D. Paulsen,"Microwave imaging for neoadjuvant chemotherapy monitoring", Proceedings of The FirstEuropean Conference on Antennas and Propagation: EuCAP 2006, 6-10 November 2006,Nice, France

    S.C. Hagness, A. Taflove, J.E. Bridges; "Two-dimensional FDTD analysis of a pulsedmicrowave confocal system for breast cancer detection: fixed-focus and antenna-arraysensors", IEEE Transactions on Biomedical Engineering, Volume 45, Issue 12, Dec. 1998Page(s):1470 1479

    R. Benjamin, "Synthetic, post-reception focusing in near-field radar", EURELInternational Conference (Conf. Publ. No. 431) The Detection of Abandoned Land Mines: A

    Humanitarian Imperative Seeking a Technical Solution, 7-9 Oct. 1996 Page(s):133 137 R. Benjamin, "Detecting reflective object in reflective medium", UK patent, GB2313969,

    Publication date: 1997-12-10

    A.J. Surowiec, S.S. Stuchly, J.B. Barr, and A. Swarup, Dielectric properties of breastcarcinoma and the surrounding tissues", IEEE Transactions on Biomedical Engineering,35, 1988, pp. 257-263.

    W.T. Joines, Y. Zhang, C. Li, and R.L. Jirtle, "The measured electrical properties of normaland malignant human tissues from 50 to 900 MHz", Medical Physics, 21, 1994, pp. 547-550.

    A.M. Campbell and D.V. Land, "Dielectric properties of female human breast tissue" -

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