Mammography Tomosynthesis Using a Coupled Source And

Total Page:16

File Type:pdf, Size:1020Kb

Mammography Tomosynthesis Using a Coupled Source And MAMMOGRAPHY TOMOSYNTHESIS USING A COUPLED SOURCE AND DETECTOR IN A C-ARM CONFIGURATION JOSEPH TOBIAS RAKOWSKI MEDICAL COLLEGE OF OHIO 2004 ACKNOWLEDGEMENTS I want to express my gratitude to my advisor, Michael J. Dennis, for his guidance; to Patti McCann and Richard Lane in the Department of Anatomy for providing the specimens; to Diane Ammons for editing my dissertation; to the members of my dissertation committee; and to the Medical College for providing this opportunity. I dedicate this to my family who taught me the value of education, and to my loving and patient wife, Linda, and my super son, Joseph Aaron. ii TABLE OF CONTENTS Acknowledgements ii Table of Contents iii Introduction 1 Literature 6 Materials 8 Methods 10 Results 32 Discussion 99 Summary 109 Conclusions 111 Bibliography 112 Appendix A 120 Appendix B 133 Abstract 145 iii INTRODUCTION Mammography is, by far, the best diagnostic tool for detecting early stage breast cancer (Baker, 1982). Tabar et al. (1987) demonstrated the importance of early detection in saving lives (Tabar, 1987). However, despite the technological and quality improvements in recent years, 10 - 30% of breast cancers are not detected, while other cancers are not detected early enough to allow effective treatment (Bassett et al., 1987; Baines et al., 1986; Haug et al., 1987). The primary reason for missed diagnosis is that the cancer is often obscured by fibroglandular breast tissue that is radiographically dense (Holland et al., 1982, 1983; Martin et al., 1979; Feig et al., 1977; Ma et al.,1992; Jackson et al., 1993; Bird et al., 1992; Mandelson et al., 2000; White, 2000; Boyd et al., 1998; Rosenberg et al., 1998; van Gils et al., 1998). A tool that could potentially prove valuable at improving the detection of early stage breast cancer, especially in radiographically dense breasts, is tomosynthesis. Tomosynthesis is the process of reconstructing planes of interest at any level in an object from limited angle projection data in a manner similar to conventional focal plane tomography. Like conventional tomography, tomosynthesis allows the radiologist to focus on a selected image plane rather than a conventional two-dimensional (2D) static projection of all overlying tissue. Unlike conventional tomography, digital tomosynthesis makes possible two further enhancements: 1) partial removal of overlying structures that lie outside the plane of interest, and; 2) selection of any plane through the breast using a single set of projections, with only a small increase in dose over a conventional film/screen mammogram. 1 Tomosynthesis reconstruction differs from the reconstruction techniques of the widespread modality of axial computed tomography (CT) in several ways. First, the primary CT image plane is defined in the source-detector plane, while the tomosynthesis image plane is perpendicular to the source-detector plane. Second, CT uses a much greater number of projections, typically from 800 to 1500 to produce an image, and typically samples through an arc of at least 180 degrees. The tomosynthesis arc is limited to about 40 degrees, with the greatest number of projections in the literature at 64 (Sone et al., 1996), thereby producing an incomplete data set from which to reconstruct the subject. The data set is incomplete in that there are not enough data points to solve for the attenuation coefficients of each subject voxel along the beam rays. The approximate number of projections needed to produce a complete data set is equal to the circumference of the scanned subject divided by the size of the smallest object one desires to image. For example, a 10 cm diameter breast at 0.2 mm resolution would require 1,571 projections. Third, the reconstruction method in modern commercial CT scanners is filtered backprojection typically using the Fast Fourier Transform (FFT), an approach that has not been applied to tomosynthesis. The methods better suited for tomosynthesis are Algebraic Reconstruction Technique (ART) and pixel shifting with iterative summation/subtraction techniques, both of which are used in this project. The algebraic/iterative techniques produce higher quality images than the filtered backprojection technique when working with incomplete sets of data, or when there is a large statistical uncertainty from a relatively small number of photons contributing to the projection images. Fourier based reconstruction methods improve contrast, i.e., soft tissue discrimination, but generate significant reconstruction artifacts when used with a limited 2 number of projections over a limited angular range. The ART approach was used in the early scanners; However, because of its computational complexity, it was replaced by the filtered backprojection technique. Fourth, CT reconstruction creates a cross sectional map of the attenuation coefficients of the voxels in the subject tissue, which are translated proportionately to Hounsfield numbers for display purposes, scaled relative to the attenuation of water. This characteristic creates tremendous contrast relative to radiographic imaging, allowing discrimination of soft tissue. Conversely, radiography displays only the amount of radiation transmitted through the subject along each ray from the source to detector. Tomosynthesis, however, can improve contrast by focusing on individual planes in a subject and partially removing interfering out-of-plane structures, commonly referred to as blur in conventional film tomography. Finally, the quality and independence of tomosynthesis planes are compromised by blurring artifacts produced from unregistered details located outside the plane of reconstruction. Digital tomosynthesis methods will be implemented for use with isocentric stereotactic breast biopsy units with digital imaging capabilities. The methods used in this project provide for planar reconstruction orthogonal to the source-receptor axis, as well as tilted relative to that axis. The images are collected on a Lorad stereotactic prone breast biopsy unit. The imaging system comprises an x-ray source and image receptor coupled in a c-arm configuration. The image receptor comprises a scintillation screen that is lens-coupled to a Charged-Coupled Device (CCD) array with a 56 mm x 56 mm effective field of view. The CCD array size selections are 512 x 512 or 1024 x 1024. The general objective of this project was to quantify the imaging performance of the tomosynthesis process performed on an isocentric digital stereotactic digital breast 3 imaging system (Lorad Stereoguide with DSM digital image receptor). The image quality will be quantified in terms of the line spread function, the Modulation Transfer Function (MTF), the appearance of the ACR digital mammography phantom, and the Signal to Noise Ratio (SNR), Contrast to Noise Ratio (CNR) and Signal to Background Ratio (SBR) of a low contrast detectability tool developed for this project. Specific objectives were to: 1. Design C++ code to implement the tomosynthesis reconstruction methodology for the C-arm configuration. 2. Design C++ code to implement the tomosynthesis plane subtraction methodology for the c-arm configuration. The goal of plane subtraction is to remove the blur artifacts produced by structures positioned outside the reconstructed plane. a. Demonstrate a linear technique. b. Demonstrate a logarithmic technique. c. Demonstrate an iterative multiplane technique. d. Evaluate the effectiveness of each technique using the test phantoms and cadaver breast specimen. 3. Design C++ code to implement the iterative reconstruction methodology for the C-arm configuration, similar to ART. a. Evaluate the effectiveness of the ART using the test phantoms and cadaver breast specimen. 4. Evaluate the effect of reconstruction on system resolution through the Line Spread Function (LSF) and MTF using an edge phantom. 4 a. Compare the results from objective 4 with performance of the zero angle single projection image. 5. Develop a low contrast detectability phantom. a. Evaluate the effect of iterative and non-iterative reconstruction on Contrast, CNR, SNR, and SBR without structured noise. b. Modify the low contrast phantom with in-plane and out-of- plane structures designed to mimic fibroglandular breast tissue, i. e., structured noise. c. Evaluate the effect of iterative and non-iterative reconstruction with structured noise subtraction on Contrast, CNR, SNR, and SBR. d. Compare the results from objectives 5a. and c. with the performance of the zero angle single projection image. 6. Image a cadaver breast specimen. Perform both iterative and non- iterative reconstruction. Compare results with a single projection image. 7. Develop and image a step phantom to measure the effective slice thickness of a tomosynthesis plane. 5 LITERATURE Niklason et al. (1997), at Massachusetts General Hospital, using a full field digital General Electric (GE) mammographic system with a stationary detector geometry, demonstrated that tomosynthesis may improve the specificity of mammography with improved lesion margin visibility and may improve early breast cancer detection, especially in women with radiographically dense breasts. Webber, et al. (2000), at Wake Forest University in Winston-Salem, North Carolina, have developed an extension of tomosynthesis in their method of Three Dimensional Mammography Using Tuned Aperture Computed Tomography (TACT™). Webber et al. (1997) first presented their method in an earlier publication on dento-alveolar imaging. The TACT™ method produces a three-dimensional image of a limited slab by
Recommended publications
  • M.Sc.Medical Physics Ac18.Pdf
    Mangalore University Syllabus for the newly proposed course on M. Sc. in Medical Physics [Prepared as per new Regulations governing the Choice Based Credit System for the Two Years (Four Semester)] University Science Instrumentation Centre Mangalore University Mangalagangotri-574 199 20015-16 Internship: a. Internship is an option and not a part of the course work. b. Mangalore University will assist the students those who complete their M. Sc. in Medical Physics course in doing their internship in well-equipped radiation therapy departments or oncology centres/hospitals. c. The candidate would be eligible to work as Medical Physicist and becomes eligible to appear for Radiological Safety Officer (RSO) qualifying examination conducted by Atomic Energy Regulatory Board (AERB) in coordination with Radiological Physics & Advisory Division (RP&AD), Bhabha Atomic Research Centre (BARC) only on completion of one year internship. d. The institute/hospital/Centre where student(s) undergo 12 months internship and the supervising personnel will be certifying the completion of internship. Course Pattern Highlights: i. The M. Sc. in Medical Physics programme shall comprise “Core” and “Elective” courses. The “Core” courses shall further consists of “Hard” and “Soft” core courses. Hard core courses shall have 4 credits and soft core courses shall also have 4 credits. Further, there shall be two Open Electives carrying 3 credits each. Total credit for the programme shall be 91 including open electives. ii. Core courses are related to the discipline of the M.Sc. in Medical Physics programme. Hard core papers are compulsorily studied by a student as a core requirement to complete the programme of M.Sc.
    [Show full text]
  • Alternative Formats If You Require This Document in an Alternative Format, Please Contact: [email protected]
    University of Bath PHD The Application of X-RAY Computerised Tomography for the Advancement of Non- Invasive Imaging in Entomology Greco, Mark Award date: 2013 Awarding institution: University of Bath Link to publication Alternative formats If you require this document in an alternative format, please contact: [email protected] General rights Copyright and moral rights for the publications made accessible in the public portal are retained by the authors and/or other copyright owners and it is a condition of accessing publications that users recognise and abide by the legal requirements associated with these rights. • Users may download and print one copy of any publication from the public portal for the purpose of private study or research. • You may not further distribute the material or use it for any profit-making activity or commercial gain • You may freely distribute the URL identifying the publication in the public portal ? Take down policy If you believe that this document breaches copyright please contact us providing details, and we will remove access to the work immediately and investigate your claim. Download date: 25. Sep. 2021 THE APPLICATION OF X-RAY COMPUTERISED TOMOGRAPHY FOR THE ADVANCEMENT OF NON-INVASIVE IMAGING IN ENTOMOLOGY Mark Kerry Greco A thesis submitted for the degree of Doctor of Philosophy University of Bath Department of Electronic and Electrical Engineering February 2013 COPYRIGHT Attention is drawn to the fact that copyright of this thesis rests with the author. A copy of this thesis has been supplied on condition that anyone who consults it is understood to recognise that its copyright rests with the author and that they must not copy it or use material from it except as permitted by law or with the consent of the author.
    [Show full text]
  • Advertisement for Scientific Officer
    NATIONAL INSTITUTE OF SCIENCE EDUCATION AND RESEARCH (An Autonomous Institute under Dept. of Atomic Energy, Govt. of India) PO-Jatni, Dist- Khurda, Pin-752050, website: www.niser.ac.in Adv. No. FA-Rct./NA/02-2021 Advertisement for Scientific Officer Applications are invited from eligible Indian citizens for recruitment in the position of ‘Scientific Officer ‘D’ & Scientific Officer ‘C’ in the Centre for Medical and Radiation Physics, NISER. Sl # Positions with Pay Required Qualification & experience Category Age Vacancies Essential: Scientific Officer ‘D’ Ph.D (Physics/Medical Physics) with M.Sc in (Medical Physics) Medical Physics/ Post-MSc (Physics) Diploma in 40 1. UR 01 (One) Level-11, Index-1 Radiological Physics Years Pay `67,700/- Essential: Scientific Officer ‘D’ Ph.D. in Experimental Nuclear or Particle Physics 03 (Physics) with one year post-Ph.D. experience. 40 2 UR (Three) Level-11, Index-1 years Pay `67,700/- Essential: Scientific Officer ‘C’ B.E./B.Tech. in Electronics or Communication (Electronics) Engineering or Instrumentation with 4 years of 36 3 UR 01 (One) Level-10, Index-1 experience in reputed organisation years Pay `56,100/- Desirable: ME/M.Tech Essential: Scientific Officer ‘C’ M.Sc in Radiation Biology or MSc in Medical (Medical Physics) Physics or MSc in Life sciences with biological 36 4. Level-10, Index-1 effects of radiation as part of the course or MSc in UR 01 (One) Years Pay `56,100/- nuclear medicine or Post-MSc (Physics) Diploma in Radiological Physics with 04 years post-MSc experience. Applicants fulfilling the above eligibility criteria mentioned in brief should apply ONLINE (www.niser.ac.in) only.
    [Show full text]
  • Gary M. Glazer, M.D. 2005 LUCAS ANNUAL REPORT on May 21
    Gary M. Glazer, M.D. Emma Pfeiffer Merner Professor in the Medical Sciences Professor and Chairman Department of Radiology 2005 Lucas annuaL RepoRt septembeR 20, 2005 On May 21, 2005 the Stanford University Department of Radiology celebrated one hundred years of making ra- diology history. The centennial celebration began with historical and scientific exhibits presented by the faculty. A symposium was held to explore the potential of biomedical imaging and targeted therapies to lead the way in making personalized medicine a reality. Looking back over the past century, we feel immense pride in the stunning achievements of our Department. These legacies include harnessing the power of the linear accelerator to treat cancer, developing a cure for Hodgkin’s disease, and advancing non-invasive imaging using x-ray and magnetic resonance methods to better understand the structure and function of living systems. Our second century began on a high note with the opening of the expansion of the Lucas Center for Imaging. Together with the original Lucas Center, completed in 1992, both buildings constitute one of the world’s largest centers for imaging located on a University campus. The expansion involved the addition of two underground stories: the approximately 20,000 square feet of new space more than doubled the size of the Lucas Center. The expansion houses faculty and equipment associated with the Radiological Sciences Laboratory and Radiology’s Molecular Imaging Program. Major new installations include a 7T whole body magnet, a cyclotron and associ- ated radiochemistry facilities, wet labs for biology and chemistry and a unique education center with the latest technology for fully interactive learning.
    [Show full text]
  • Non—Destructive Testing of Industrial Materials
    APPLICATIONS OF GAMMA RAY TOMOGRAPHY TO NON—DESTRUCTIVE TESTING OF INDUSTRIAL MATERIALS A THESIS SUBMITTED FOR THE AWARD OF THE DEGREE OF DOCTOR OF PHILOSOPHY TO THE UNIVERSITY OF LONDON BY MOHAMED M. ENNAMI REACTOR CENTRE IMPERIAL COLLEGE OF SCIENCE, TECHNOLOGY AND MEDICINE SEPTEMBER 1988. This thesis is dedicated to my wife Mariam, my son Haroun and to our parents 1 ABSTRACT This study investigates the Possibility of applying computerised gamma—ray tomography in non—destructive testing o-f industrial materials in transmission and emission modes. Measurements -for tomography using gamma—rays and the operation of radiation detectors are based on photon interactions with matter. The theory governing these interactions is discussed. The theory o-f the mathematical reconstruction of a two dimensional distribution from its projections is shown? and reconstruction techniques and applications are reviewed. The principles of gamma—ray detection and measurements are presented in order that the physical significance of the data recorded can be assessed. Detection characteristics pertinent to imaging applications were measured for the horizontal dipstick Ge<Li> detector used in these experiments. The importance of these characteristics in determining the suitability of this detector for imaging applications is di scussed. A prototype scanning rig was designed for transmission and eiii i ssi on tamour aph y , T’.,; r i o wiii-, ‘ * • used with phantoms t o determine contrast and spatial resolution. The usefulness of line scans and contrast measurements in quantitative analysis is shown. The effect of scattering on image quality is discussed briefly in terms of the quality of the data used for reconstruction? and scatter subtraction is used for all reconstructions.
    [Show full text]
  • Biomedical Engineering
    BHARATH INSTITUTE OF HIGHER EDUCATION AND RESEARCH DEPARTMENT OF BIOMEDICAL ENGINEERING CURRICULUM AND SYLLABUS (R2018) CHOICE BASED CREDIT SYSTEM (Applicable to the batches admitted from July 2018) M.Tech - BIOMEDICAL ENGINEERING-R2018 DEPARTMENT VISION To create highly motivated, technologically competent engineers, be a benchmark and trend setter in Biomedical Engineering by imparting quality education with interwoven input from academic institutions, research organizations and industries to improve healthcare delivery to human in association with physicians and surgeons MISSION STATEMENTS MS1: Providing good academic ambience by adopting best teaching and learning practices through flexible student centric curriculum evolved continuously for student of BME with diverse backgrounds. MS2: Providing congenial ambience both for faculty members and students in inculcating critical thinking with a quest for creativity, innovation, research and development activities. MS3: Enhancing collaborative activities with academia, research institutions and industries by nurturing ethical entrepreneurship and leadership qualities. MS4: Nurturing continuous learning in the state-of-the art technologies and global outreach programmes resulting in competent world-class biomedical engineers PROGRAMME EDUCATIONAL OBJECTIVES (PEOs): PEO1: PREPARATION: To provide students with sound fundamental in Mathematical, Scientific and Engineering fundamentals necessary to formulate, analyse, and comprehend the fundamental concepts in Bio Medical Engineering. PEO2:
    [Show full text]
  • Draft Aerb Safety Guide No
    DRAFT AERB SAFETY GUIDE NO. AERB/RF-RQTL/SG-1 QUALIFICATION AND TRAINING OF PERSONS IN RADIATION FACILITIES AND THEIR APPROVAL/ LICENSING PROCESS Atomic Energy Regulatory Board Mumbai 400 094 India August 2018 1 This Page is intentionally kept Blank 2 FOREWORD Activities concerning establishment and utilization of nuclear facilities and use of radioactive sources are to be carried out in India in accordance with the provisions of the Atomic Energy Act, 1962. In pursuance of the objective of ensuring safety of occupational workers, members of the public and protection of the environment, the Atomic Energy Regulatory Board (AERB) has been entrusted with the responsibility of laying down safety standards and enforcing rules and regulations for such activities. The Board has, therefore, undertaken a programme of developing safety standards, safety codes, and related guides and manuals for the purpose. While come of these documents cover aspects such as siting, design, construction, operation, quality assurance and decommissioning of nuclear and radiation facilities, other documents cover regulatory aspects of these facilities. Safety codes and safety standards are formulated on the basis of internationally accepted safety criteria for design, construction and operation of specific equipment, structures, systems and components of nuclear and radiation facilities. Safety codes establish the objectives and set requirements that should be fulfilled to provide adequate assurance for safety in nuclear and radiation facilities. Safety guides elaborate various requirements and furnish approaches for their implementation. Safety manuals deal with specific topics and contain detailed scientific and technical information on the subject. These documents are prepared by experts in the relevant fields and are extensively reviewed by advisory committees of the Board before they are published.
    [Show full text]
  • Four Year Educational Residency Program of Diagnostic Radiology
    YEREVAN STATE MEDICAL UNIVERSITY (DEPARTMENT OF RADIOLOGY) FOUR YEAR EDUCATIONAL RESIDENCY PROGRAM OF DIAGNOSTIC RADIOLOGY The four-year diagnostic radiology residency program is designed to provide residents with direct clinical involvement at graduated levels of responsibility. Imaging has a great impact on disease diagnosis in all medical fields and new advents on different imaging tools have significantly changed the quality of medical diagnostic approaches. Interventional Radiology, or better to say “Image-Guided Microsurgical Procedures” have opened a new world for either diagnose or treat many of diseases in a safer, faster, and more effective way. Considering advances in medical knowledge, modern radiology has a great position. The specialists should acquire enough knowledge and expertise to answer diagnostic and therapeutic needs of patients in all fields and be capable for other colleagues to handle diagnostic and therapeutic procedures and use technology in this way. Obviously, the quality of radiology ward depends on residency programs. In regards to above needs, educational goals of diagnostic radiology are listed as below: A) General goals B) Specific goals: 1) Thorax 2) Musculoskeletal System 3) Digestive System (GI) 4) Genitourinary System (GU) 5) Nervous System 6) Head & Neck 7) Pediatrics 8) Breast 9) Interventional Radiology 10) Nuclear Medicine 11) Physics GENERAL GOALS: Residents initially interpret radiographic studies, which are subsequently reviewed by a faculty attending. Additionally, during most interventional procedures, residents are primary operators under direct supervision of attending physicians. All residents participate in a mentoring program in which they select a faculty member to provide guidance during the training process and to act as a resource for individual needs.
    [Show full text]
  • COMARE Sixteenth Report
    Committee on Medical Aspects of Radiation in the Environment (COMARE) SIXTEENTH REPORT Patient radiation dose issues resulting from the use of CT in the UK Chairman: Professor A Elliott © Crown copyright 2014 Produced by Public Health England for the Committee on Medical Aspects of Radiation in the Environment ISBN 978-0-85951-756-0 CONTENTS Page Foreword 5 Chapter 1 Introduction 7 Chapter 2 Applications and benefits of CT scanning 12 Chapter 3 Detriments associated with radiation dose from CT scans 19 Chapter 4 Developments in CT and technological strategies for dose reduction 31 Chapter 5 Dose measurements, dose surveys and diagnostic reference levels 41 Chapter 6 Clinical strategies for dose reduction 53 Chapter 7 Governance 61 Chapter 8 Conclusions 68 Chapter 9 Recommendations 69 References 71 Acknowledgements 82 Appendix A Glossary and Abbreviations 85 Appendix B CT versus MRI versus Ultrasound 91 Appendix C History of CT 92 Appendix D Letter from the Royal College of Radiologists 94 Appendix E COMARE Reports 95 Appendix F COMARE Membership 97 Appendix G Declarations of Interest 100 3 FOREWORD i The Committee on Medical Aspects of Radiation in the Environment (COMARE) was established in November 1985 in response to the final recommendation of the report of the Independent Advisory Group chaired by Sir Douglas Black (Black, 1984). The terms of reference for COMARE are: ‘to assess and advise government and the devolved authorities on the health effects of natural and man-made radiation and to assess the adequacy of the available data and the need for further research’ ii In the course of providing advice to government and the devolved authorities for over 28 years, COMARE has published to date 15 major reports and many other statements and documents mainly related to exposure to naturally occurring radionuclides, such as radon and its progeny, or to man- made radiation, usually emitted by major nuclear installations.
    [Show full text]
  • A X-Ray Scanning Machine for Imaging Atomic Elements
    A X-RAY SCANNING MACHINE FOR IMAGING ATOMIC ELEMENTS A.G.R. FENELON A THESIS FOR THE DEGREE OF MASTER OF SCIENCE PRESENTED TO THE NATIONAL COUNCIL FOR EDUCATIONAL AWARDS THE SCHOOL OF PHYSICAL SCIENCES NATIONAL INSTITUTE FOR HIGHER EDUCATION, DUBLIN RESEARCH SUPERVISOR JOSEPH FRYAR MAY 1988 DECLARATION This thesis is based on my own work. ABSTRACT X-ray computer axial tomography is a well established technique for producing images which show the spatial variation of X-ray linear attenuation coefficient within an object. X-ray differential K absorbtion edge tomography is the application of computer axial tomography to form images of selected atomic elements within an object, and these images show the distribution of specific atomic element concentration. The technique is to measure the attenuation of X-rays on either side of the K absorbtion edge of an atomic element with an energy dispersive X-ray detector, and then reconstruct an image of the location and concentration of that element in an object by means of a computer algorithm for display on a colour monitor. This method is able to image several atomic elements in one X-ray scan only of the object, in particular, consecutive elements in the Periodic Table of the Elements. One atomic element only within the object may be better selected by correcting for the X-ray attenuation of all the other elements, the matrix of the object, by extrapolating the measurements to the K absorbtion edge, thus measuring accurately the absorbtion coefficient of the analyte element only. The concentration of analyte element may O be measured down to about lkg/m in a water like matrix with a total of O 10 photons.
    [Show full text]
  • Medical Physics (2 Years Course)* (Choice Based Credit System)
    D.Y. PATIL EDUCATION SOCIETY KOLHAPUR DEEMED UNIVERSITY (Declared under section 3 of the UGC act 1956) 869, ‘E’ KasabaBawada, Kolhapur-416 006 Phone No. : (0231) 2601235-36, Fax : (0231) 2601595, Web: www.dypatilunikop.org , E-mail : [email protected] COURSE CURRICULUM M. Sc Medical Physics (2 Years Course)* (Choice based Credit System) (*On successful completion of M. Sc. Medical physics course, all students are required to undergo one year internship at AERB recognized institutes. This is a mandatory requirement for becoming qualified medical physicists and appearing in the RSO examination) 1 BL-MP-01- About the course M. Sc. Medical Physics course is basically a two years course which is approved by Atomic Energy Regulatory Board (AERB), Government of India. M. Sc. Medical Physics course, being a specialization course designed to train the young pool of PG students as qualified medical physicist and radiation safety officers (RSO) in the field of cancer radiation therapy. Medical physics is one of the fastest growing areas of employment for physicists. They play a crucial role in radiology, radiation therapy and nuclear medicine. These fields use very sophisticated and expensive equipment and medical physicist or responsible for much of its plan, execution, testing and quality assurance. The M.Sc. medical physics students are getting the exposures form the various cancer hospitals during practical and their M.Sc. Project work. Our students are exposed to field training in various cancer hospitals all over India. After completion of the 2 years course, students undergo one year internship according to AERB regulations in order to work as a Medical Physicist in the hospital.
    [Show full text]
  • A Thesis for the Degree of PHILOSOPHIAE DOCTOR
    A Study of the Imaging of Contrast Agents for use in Computerised Tomography. A thesis for the degree of PHILOSOPHIAE DOCTOR Presented to DUBLIN CITY UNIVERSITY By Neil John O'Hare B.Sc. The School of Physical Sciences Dublin City University Research Supervisor Joseph Fryar B.Sc. Ph.D August 1991 This thesis is dedicated to all my friends who, in one form or another, enabled me to finally finish school. Of these, four deserve special mention. Firstly my parents, John and Lucy, who , through times good and bad, offered continued support and encouragement. Secondly Jonie, the woman in my life, thanks for listening. Finally Joe Fryar, my supervisor. His enthusiasm for the subject made me start and his guidance enabled me to finish. No more could I ask for. Domo Arigato. He who krvama otheriA Lb wl&e He who. knomtx hlm&eig ¿6. entbqhtened He who. canqueria atherux atruaru}. He who. canquesux hlm&ei£ io. mlqhty He mho. knauM, contentm ent ¿a nich He w ha keep& on hl& cauAAe with enenqy. haA. uuM He wha dae& not deAsiate pxom h ia paapea p la c e wiM long, endarve He wha may die but not perdAh haci ¿cmqeAsity. Tao Te Ching Declaration This thesis is based on my own work. Table of Contents. C h a p te r I Introduction to Computerised Tomography and its applications. 1.1 Introduction 1 1.2 Principles and History of Computed Tomography. 2 1.3 Commercial Scanner Developments. 7 1.4 Computerised Tomography Applications. 1.4.1 Medical 11 1.4.2 Industrial 13 1.5 Other Forms of Computerised Tomography 1.5.1 Gamma-ray CT.
    [Show full text]