Lecture 1: Development of the Analog Gamma Camera

Slides:



Advertisements
Similar presentations
Topic 8. Gamma Camera (II)
Advertisements

Instruments for Radiation Detection and Measurement Lab # 4.
NUCP 2371 Radiation Measurements II
Dante Nakazawa with Prof. Juan Collar
Chapter 8 Planar Scintigaraphy
Nuclear Medicine Spring 2009 FINAL. 2 NM Team Nuclear medicine MD Nuclear medicine MD Physicist Physicist Pharmacist Pharmacist Technologist Technologist.
Gamma Camera Technology
Computed Tomography RAD309
Unit I: Physics Associated with Nuclear Medicine Instrumentation Part A: Atomic Structure and Radiation’s Interaction with Matter Lecture 2 CLRS 321 Nuclear.
Session 3: Atomic Structure and Ionizing Radiation (cont’d) Lecture 3
Lecture 2-Building a Detector George K. Parks Space Sciences Laboratory UC Berkeley, Berkeley, CA.
Instruments for Radiation Detection and Measurement
Planar scintigraphy produces two-dimensional images of three dimensional objects. It is handicapped by the superposition of active and nonactive layers.
Instruments for Radiation Detection and Measurement Lab # 3 (1)

1 Scintillators  One of the most widely used particle detection techniques Ionization -> Excitation -> Photons -> Electronic conversion -> Amplification.
Innovation is in our genes. 1 Siemens Medical Solutions Molecular Imaging What are SPECT basics?
Scintillation Detectors
Nuclear Medicine: Planar Imaging and the Gamma Camera Katrina Cockburn Nuclear Medicine Physicist.
Nuclear Medicine Principles & Technology_I
R. Pani Department of Experimental Medicine and Pathology University of Rome La Sapienza-Italy. Flat Panel PMT: advances in position sensitive photodetection.
NASA 2001 Mars Odyssey page 1 Workshop HEND Russian Aviation and Space Agency Institute for Space Research Present knowledge of HEND efficiency.
Medical applications of particle physics General characteristics of detectors (5 th Chapter) ASLI YILDIRIM.
CAT scanners and gamma cameras Unit 16 Waves. Learning objectives Describe how CAT scanners can produce a much more detailed image than conventional X-rays.
Lecture 12  Last Week Summary  Sources of Image Degradation  Quality Control  The Sinogram  Introduction to Image Processing.
Nuclear Medicine Physics and Equipment 243 RAD 1 Dr. Abdo Mansour Assistant Professor of radiology
Nuclear Medicine Instrumentation 242 NMT 1 Dr. Abdo Mansour Assistant Professor of radiology
Nuclear Medicine Physics & Instrumentation I
Chapter-2 The Planar Imaging Gamma Camera
Introduction to Gamma Camera
Chapter-2 The Planar Imaging Important points in chapter 2 (chapter 13 from the book) The gamma camera (the basic principles of the gamma camera) The types.
Unit II: Nuclear Medicine Measuring Devices Part A: Gas-filled Detectors "Enrico Fermi," Microsoft® Encarta® Online Encyclopedia
PET Imaging Positron Emission Tomography
Muhammad Musaddiq.
Chapter-5 Positron emission tomography (PET)
Gamma Camera Technology
Radiation detectors Ion chamber 2. Geiger Muller counter (GM).
Nuclear Medicine Physics Jerry Allison, Ph.D. Department of Radiology Medical College of Georgia Radiation Detectors.
CLRS 321 Nuclear Medicine Physics and Instrumentation 1
Nuclear Medicine Physics
Computed Tomography Data Acquisition
MoNA detector physics How to detect neutrons. Thomas Baumann NSCL.
Image quality and Performance Characteristics
Image quality and Performance Characteristics
Gamma Camera.
Function and Structure in
Unit V: Introduction to Gamma Camera
Lecture 2—Associated Electronics and Energy Spectrum
Lecture 4(Unit II): Gas-Filled Detector Quality Control
Lecture 2: Basic Operation of Gas-filled Detectors Unit II, Gas-filled Detectors "Enrico Fermi," Microsoft® Encarta® Online Encyclopedia
CLRS 321 Nuclear Medicine Physics & Instrumentation I
Lecture 3 (Unit II): Gas-Filled Detector Operation and Use
Neutron Detection with MoNA LISA
Nuclear Medicine Physics & Instrumentation I
Gamma-Gamma Correlations in Na-22
Lecture 3: Modes of Radioactive Decay
Lecture 6: Attenuation and Transmission of Photons
Scintillation Counter
Nuclear Medicine Physics & Instrumentation I
Lecture 1—Basic Principles of Scintillation
CLRS 321 Nuclear Medicine Physics and Instrumentation 1
Gamma Camera & Basic Principles
Function and Structure in
Gamma Camera Ilker Ozsahin Oct
Development of a Large Area Gamma-ray Detector
HE instrument and in-orbit performance
Assist. Prof. Dr. Ilker Ozsahin Oct
Remote sensing in meteorology
Fiber Optic Transmission
Status Report on MCP PET Simulation
Presentation transcript:

Lecture 1: Development of the Analog Gamma Camera Unit V: Introduction to Gamma Camera Lecture 1: Development of the Analog Gamma Camera http://www.petnm.unimelb.edu.au/nucmed/overview/history.html

Objectives Describe the major components of the Anger gamma camera and the development and concept of positioning logic, including the requirement for energy normalization Discuss later improvements to the Anger camera’s design

Circa 1950s Rectilinear Scanner http://www.petnm.unimelb.edu.au/nucmed/overview/history.html

Anger Camera—circa 1958 http://www.rsna.org/Publications/rsnanews/jan06/people_jan06.cfm

Hal Anger’s original plan using 7 PMTs Paul Early, D. Bruce Sodee, Principles and Practice of Nuclear Medicine, 2nd Ed., (St. Louis: Mosby 1995), pg. 253.

Cross-sectional Schematic of Gamma Camera PMTs NaI (Tl) Crystal

What we want to get is…

But the schematic says we’ll get…

Because of its particulate, high energy, nature, we can only use High “Z” material to “absorb” gamma radiation (i.e. lead).

… adding a multi-hole collimator to the exterior-facing portion of the large scintillation crystal

Collimators…”discriminate based on direction of flight…” (NM & PET/CT, 7th Ed). Collimators allow only gamma photons traveling in a desired direction to be detected. Collimators themselves cannot discriminate different photon energies from one another.

Position Logic Circuitry

Position Logic Circuitry with normalization of event energy Sum circuit totals all output to create the Z pulse The Z pulse is sent to the PHA and the division circuit to normalize X and Y output for positioning

Related positioning logic concept: edge packing Picture from: http://www.medimaging.gr/cd/pages/par4.htm accessed 11/11/12

NaI(Tl) Crystals Usually 3/8 to 5/8 inch thick Hygroscopic so hermetically sealed Surrounded by inward reflective cover

Thicker crystal : more sensitive crystal Gamma photon Less likely gamma photon will pass through undetected But PMTs will see it more as a foggy diffuse light

Thinner crystal : better resolution Gamma photons But PMTs will see a gamma photon as a more distinct point of light More gamma photons will pass through undetected

3/8 inch crystal required to efficiently detect gamma photons up to 200 keV Most modern gamma cameras have 38 x 50 cm rectangular FOVs

More resolute thicker crystals are possible for higher photon energies. Paul Christian, Donald Bernier, James Langan, Nuclear Medicine and Pet: Technology and Techniques, 5th Ed. (St. Louis: Mosby 2004) pg 69.

Paul Christian, Donald Bernier, James Langan, Nuclear Medicine and Pet: Technology and Techniques, 5th Ed. (St. Louis: Mosby 2004) pg 69.

Putting It All Together

Putting It All Together Collimator – Only allows direct path photon to interact with NaI(Tl) crystal.

Putting It All Together Crystal – Emits visible light when energy from gamma photon is deposited within in

Putting It All Together Light Pipe— Anger’s original design included a thick clear plastic sheet between crystal & PMT. The photoemissive material is thicker at the center of the photo anode resulting in making the PMTs shapes visible on a uniform image. This was an attempt to reduce this effect. Newer cameras correct this digitally and no longer use light pipes.

Putting It All Together PMTs – Generate electric pulse in response to visible light from crystal. (Closest PMT to light generates greatest pulse) Modern cameras have an array of 60-120 PMTs More recently produced systems include software for thresholding PMT responses for more accurate positioning

Putting It All Together Position Logic Circuit – Compares PMT pulses and assigns a location on an image matrix that corresponds with the event detected by the crystal.

Putting It All Together Position Logic Circuit – Sends location signals in terms of x and y values

Putting It All Together DIVISION CIRCUITRY Z Pulse Sum of PMT pulses generated by a detection event (represents total energy deposited on the crystal). The Z pulse is also used in the “Division Circuitry” to “normalize” the X & Y positioning signals.

Putting It All Together Pulse Height Analyzer- As with any scintillation detector, allows us to select pulses of a certain height and reject others.

-y +y +x -x Paul Early, D. Bruce Sodee, Principles and Practice of Nuclear Medicine, 2nd Ed., (St. Louis: Mosby 1995), pg. 253 & 255.

Paul Early, D. Bruce Sodee, Principles and Practice of Nuclear Medicine, 2nd Ed., (St. Louis: Mosby 1995), pg. 255.

Multiformatter High quality CRT Can direct image to multiple spots on film 2, 4, 8, 16, 30 images on one film Works great, but NO MISTAKES! Paul Early, D. Bruce Sodee, Principles and Practice of Nuclear Medicine, 2nd Ed., (St. Louis: Mosby 1995), pg. 255.

Variable Persistance Scope (P-Scope) More commonly digitized now Screen is “refreshed” based on time or counts Paul Early, D. Bruce Sodee, Principles and Practice of Nuclear Medicine, 2nd Ed., (St. Louis: Mosby 1995), pg. 256.

Next time: Modern Gamma Cameras