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Published byBenjamin Clarke Modified over 9 years ago
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CT “Computer tomography”
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Contrast mechanisms in X-ray imaging: X-ray absorption X-ray absorption mechanisms: 1. Photoelectric effect 2. Compton scatter 3. Pair formation Problem: X-ray image is a summation image
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CT History 1972 Godfrey Hounsfield „Siretom” head scanner (1974) 128x128 image recorded using the Siretom scanner (1975) Allan Cormack 1979 Nobel Prize in Medicine
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CT Foundations I source detector
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CT Foundations II µ x : linear attenuation coefficient
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Scanning I I. generation Single moving source Single moving detector II. generation Single moving source Narrow fan-beam Multiple moving detectors
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Scanning II III-IV. generation Single moving source Wide fan-beam Multiple detectors or detector ring closed gantry open gantry
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CT Image Reconstruction 1. Algebraic reconstruction techniques 2. Direct Fourier reconstruction 3. „Filtered Back Projection” CT-image: 4000 detectors 1000 projections 512x512 matrix 16 bit depth
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CT Image: Density matrix Density (“CT Number”): Hounsfield units µ: attenuation coefficient of voxel µ w : attenuation coefficient of water
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Contrast Manipulation of CT Image: „windowing”
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Spiral CT New CT Developments, Trends Virtual endoscopy Angiography 3D reconstruction
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MRI “Magnetic Resonance Imaging”
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Nuclei with nuclear spin: elementary magnets Magnetic moment: =magnetogyric ratio L=angular momentum
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In absence of magnetic field: Random orientation of elementary magnets In magnetic field: elementary magnetsenergy levels orientsplit B0B0 parallel antiparallel EE B0B0 E B
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Precession Precession or Larmor frequency:
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B0B0 M Low energy state parallel in case of proton High energy state antiparallel in case of proton Net magnetization (M) due to spin excess in different energy states
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Excitation using radio frequency (RF) radiation Resonance condition: Larmor frequency M Net magnetization
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Spin-lattice relaxation T1 or longitudinal relaxation t MzMz T1 relaxation time: depends on interaction between elementary magnet (proton) and its environment
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Spin-spin relaxation T2 or transverse relaxation M xy t “free induction decay” (FID) T2 relaxation time: depends on interaction between elementary magnets (protons)
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1970: detection of lengthened relaxation times in cancerous tissues 1972: theoretical development of human in vivo 3D NMR 1977: first human MRI image Inventor of MRI: Raymond V. Damadian (1936-)
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MRI: Net magnetization of the human body takes place “indomitable”
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Paul C. Lauterbur (1929-) 1971: development of spatially resolved NMR
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voxel: volume element pixel: picture element Image MRI imaging I: Spatial resolution
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Definition and addressing of elementary 3D image points (voxels): by using gradient magnetic fields MRI imaging I: Spatial resolution ByBy BxBx BzBz
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MRI imaging II: Color (grayscale) resolution (contrast) Based on relaxation times
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MRI imaging II: Color (grayscale) resolution (contrast) Based on spin density and relaxation times T1-weighing T2-weighing Proton density- weighing
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MRI technology Magnet: superconducting (liquid He) Resolution enhancement: with surface RF coils Excitation with pulse sequences 90˚ Detection and analysis: Fourier transform of temporal signal t
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MRI: Image manipulation I Reslicing in perpendicular plane
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MRI: Image manipulation II Spatial projection („volume rendering”)
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Blood flow Image slice Saturated spins Unsaturated spins MRI: Non-invasive angiography
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MRI: Non-invasive angiography arteria carotis Circulus arteriosus Willisii
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MRI movie Based on high time resolution images Opening and closing of aorta valve
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Functional MRI fMRI High time resolution image sequences recorded synchronously with physiological processes Effect of light pulses on visual cortex
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MRI információ szuperponálása egyéb információval (PET)
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Superposed MRI and PET image sequence PET activity: during eye movement Volume rendering
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