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RSNA 2010, Chicago, Nov. 28 - Dec Dec.. 2, 2010 Update Course in Diagnostic Radiology Physics Physics:: CT and MR Imaging Directors:: Directors Willi A. Kalender, Ph.D. (CT) Ed Jackson, Ph.D. (MR) Categorical Course in Diagnostic Radiology Physics: Physics: CT and MR RSNA 2010, Chicago, Nov. 28, 2010, RC 132A CT Image Generation: From MultiMulti-Slice to ConeCone-Beam CT A. Advances in CT Technology Willi A. Kalender, Ph.D. Institute of Medical Physics University of Erlangen http://www.imp.uni--erlangen.de http://www.imp.uni AuntMinnie http://www.auntminnie.com On Nov. 16, 2009 AuntMinnie wrote: It‘s not for nothing that CT is able to maintain its star status at the RSNA show year after year. Extraordinary flexibility in head-to-toe head to toe imaging applications, combined with rapid technological advancement, make CT the modality to beat once again in 2009. This year’s Chicago meeting will highlight several powerful technical innovations …. Seite 1 1 CT Development: from fan beam to cone beam z RSNA 1998 1×5 mm 4×1 mm 0.75 s 0.5 s 1995 1998 RSNA 2001 RSNA 2004 RSNA 2008 16×0.75 mm 64×0.6 mm 320×0.5 mm 0.42 s 0.33 s 0.3 s 2001 2004 2009 RSNA 20?? 2048×0.4 mm 0.2 s 20?? Advances in CT Technology • State of the art in clinical CT • CT Technology • Flat detector CT Spiral CT: Scanning Principle Start of spiral scan Path of continuously rotating x-ray tube and detector RSNA 1989 Direction of continuous patient transport 0 z, mm 0 t, s Kalender WA et al. Radiology 1989; 173(P):414 and 1990; 176:181-183 Seite 2 2 State of the Art in Multi Multi--slice Spiral CT RSNA 2009 Rotation time per 360° 0.27 - 0.35 s Slice width 0.5 - 0.6 mm simultaneously scanned slices 64 (- 320) z-coverage per rotation 40 - 160 mm Scan times „whole body“ 2 - 20 s Scan range >1000 mm Isotropic spatial resolution 0.4 - 0.6 mm Effective dose <1 - 10 mSv Typical values for high-performance scanners Spiral CT Angiography in 2004 • 64-slice scanner • 3 s total scan time • 0.5 mm isotropic spatial resolution • 2.4 mSv effective dose Advances in CT Technology • State of the art in CT • Technology - X-ray sources - X-ray detectors - Scanner design - Dual source CT - Dual energy CT - Dose management • Flat detector CT Seite 3 3 X-ray Sources for CT • Limited x-ray power was a severe problem in the 1980s and 1990s. • Peak power values of up to 120 kW are available today. • Shorter and shorter rotation times demand higher power values. • Reduced weight and size of tubes would be very welcome. Rotating Anode XX-ray Tubes The principle of x-ray tube developments for CT over the years: Increase the anode‘s mass to allow for higher heat capacity ”Rotating Vacuum Vessel“ XX-ray Tube Technology with zz-flying focal spot ((zFFS zFFS)) Rotating vacuum vessel Oil for HV insulation and cooling Emitter Straton tube Motor Deflection coils Housing Ball bearings Electron beam X-rays Schardt et al. Medical Physics 2004; 31:2699-2706 Seite 4 4 A high-power X-ray tube Double z-Sampling Technology z-Flying Focal Spot Electromagnetic Control of the Electron Beam Rotating Anode z 0,6 mm 0,6 mm 32 detector rows (64 slices scanned) Sampling distance: 0.3 mm Kalender WA. Computed Tomography. 2nd ed. Wiley, New York 2005 Impact of the zFFS on z-Resolution MTFs in the z-direction x 1.2 without zFFS 0.4 mm 1 0.4 mm with zFFS z M TFz 0.8 0.6 04 0.4 0.5mm 0.2 0.5 mm 0 0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2 lp/mm 0.6 mm 0.6 mm without zFFS with zFFS Kyriakou … Kalender. Eur Radiol 2006; 16:1206-1215 Seite 5 5 Impact of the zFFS on windmill artifacts without zFFS with zFFS ASSR reconstruction, p=1.2 X-ray Detectors for CT • Detectors remain to be the most critical and most costly component of CT scanners. • Single- and dual row detectors were used for nearly three decades. decades • Multi-row or array detector technology, introduced in 1998, dominates today. • 64-slice scanners may offer the optimum solution for clinical CT. Multi--row Detectors for Multi Multi Multi--slice Spiral CT D # rows M Smin # slices mm z-extent Mm GE 64 64 0.625 40.0 Philips 128 256* 0.625* 80.0 Siemens 64 128* 0.6* 38.4 Toshiba 320 Example 320 of a 64-row 0.5 detector 160.0 T. spiral 64 (of 320) 64 (55 modules with 16 channels) 0.5 32.0 *overlapping slices at 0.3 mm increments Seite 6 6 Standard 6464-slice Multi Multi--Row CT detector grid anti-scatter protect gaps 64 x16 module scintillator reflector optical coupling photodiode amplifiers and digitizers 55 × 16 channels, 64 rows Problems associated with wider detectors (higher number of rows, greater zz-coverage) • Potential image quality problems • Higher scattered radiation intensities • X-ray tube heel effect • Reduced potential for dose optimisation • Dose increase in step-and-shoot mode • Cost • …. Î There are many reasons against a continuation of the “slice race“ Advantages of wider detectors (higher number of rows, greater zz-coverage) • Dynamic scanning, in case all the anatomy of interest is covered in a single rotation, e.g. for brain perfusion measurements. However, • modern 64-slice scanners offer shuttle modes which allow fast and repeated measurements with the scan range freely adapted to needs even for wider ranges. Seite 7 7 Advances in CT Technology • State of the art in CT • Technology - X-ray sources - Detectors - Scanner design - Dual source CT - Dual energy CT - Dose management • Flat detector CT Demands on faster scanners • Mechanic design has to withstand very fast rotation. Centrifugal forces acting on the x-ray tube Î 30 g for trot d = 300 ms = 65 cm rotation time per 360° distance to center of rotation “Air--borne“ CT Gantry “Air offering very high rotation speed with no wear on components Schleifring Seite 8 8 Demands on faster scanners • Mechanic design has to withstand very fast rotation. Centrifugal forces acting on the x-ray tube Î 30 g for trot d = 300 ms = 65 cm rotation time per 360° distance to center of rotation • X-ray power has to increase with higher speed Î by 1/trot for trot < 300 ms P > 100 kW are required A DualDual-Source CT (DSCT) System Dual Source CT (DSCT) * • System set-up – 2 Straton tubes and 2 x 128-slice acquisition with double z-sampling – 280 ms gantry rotation – 50 and 33 cm field of view • X-ray power – Acquisition with up to 2 x 100 kW • Cardiac CT – 75 ms temporal resolution (trot/4) • Dual Energy CT – Simultaneous acquisition with 80 kV / 140 KV with 0.5 mm tin filter added for the 140 kV beam * SOMATOM Definition Flash, Siemens Healthcare, Forchheim, Germany Seite 9 9 Temporal Resolution Phase-correlated reconstructions for heart rates of 40 – 120 bpm 60 bpm 80 bpm 100 bpm 120 bpm DSCT SSC CT Sphere at rest 40 bpm Ertel … Kalender. Radiology 2008; 248:1013-1017 Dual Source Cardiac CT DIASTOLE SYSTOLE Achenbach et al., Eur J Radiol 2006; 57(3):331-335 How about a cardiac exam in about a quarter of a second? Scan range Collimation Rotation time Pitch 12 cm 38.4 mm 280 ms 3.4 Î Table speed Scan time 46.6 cm/s 0.26 s = 1.59 km/h !! Seite 10 10 High--pitch dual High dual--source CT 0.26 s Flash Cardiac Scan direction 75 ms per slice Scan only for one heart phase and only during one heart beat and at minimum radiation dose !!! Cardiac DSCT with high pitch 100 kV 320 mAs 59 bpm triphasic CM injection 60 ml Ultravist 370 + 50 ml saline bolus Effective dose 0.98 mSv Courtesy of S. Achenbach, University of Erlangen Flash performance: High speed Spiral CT angiography scan range pitch rot. time Î scan time dose 700 mm 2.8 280 ms 1.8 s 1.4 mSv Seite 11 11 Spatial resolution Pitch factor: 3.0 Pitch factor: 1.0 0.4 mm 0.4 mm Ertel D, … Kalender WA. Eur Radiol 2009 Thoracic CT with Flash Chest Pain – Pulmonary Embolism 100 kV 370 mAs 51 bpm triphasic CM injection 60 ml Ultravist 370 + 50 ml saline bolus Scan time 0.7 s Courtesy of M. Lell, University of Erlangen Dual Energy CT Applications approved by the FDA 2007 1. 2. 3. 4 4. 5. 6. 7. 8. 9. 10. Direct subtraction of bone Differentiation between plaque and contrast agent Virtual unenhanced abdominal organ imaging Kidney stone characterization Visualization of cartillage, tendons, ligaments Evaluation of lung perfusion defects Heart perfusion blood volume Uric acid crystal visualization Lung vessel emblisation Brain hemorrhage differentiation Seite 12 12 Dual Energy CT: 1. Direct Bone Removal Courtesy of C. Becker, Munich, Germany Dual Energy CT: 2. Differentiation between hard plaques and contrast Courtesy of F.Civaia, Centre Cardiothoracique de Monaco Dual Energy CT: 2. Differentiation of hard plaques and contrast Plaque Plaque ON OFF Courtesy of M. Lell, Erlangen, Germany Seite 13 13 Dual Energy CT: 7. Cardiac Perfusion I di Iodine concentration in the myocardium depicting perfusion deficit vs. Angiography and SPECT Courtesy of J. Schoepf, Charleston, SC, USA (Circulation, 2008) Technical Implementations of DECT • 1970s ff.: Separate scans obtain 2 successive scans at high and low voltage, possibly with different filtration • 1980s: Rapid kV-switching obtain data at high and low voltage values in a single scan with fixed filtration • 1990s ff.: Novel detectors photon-counting energy-discriminating detectors & sandwich detectors • 2000s: Dual Source CT obtain data simultaneously in a single scan with mA values and filtration adapted separately DECT will be covered in RC 432 on Tue at 04:30 p.m. Dose Management in Modern CT (RC 732 on Thu at 16:30 a.m.) Tube current modulation (TCM) and automated exposure control (AEC) (AEC),, introduced in the late 1990ies and generally available since a few years years,, are the essential building blocks. blocks. The principle simply is is:: Adapt the tube current and thereby the x-ray intensity to the attenuation given for any projection as a function of rotation angle and z-position Seite 14 14 In--plane TCM (α In (α-TCM) Attenuation (central ray) 3603 43 0° 0 projection angle α 360° 360 Tube current (for central ROI) max Attenuation for the central ray: in a.p. direction: 43 in lateral direction: 3603 min 0° projection angle α 360° Tube Current Modulation (TCM) and Automatic Exposure Control (AEC) Standard CT re el. image noise re el. tube current re el. image noise re el. tube current TCM & AEC α-TCM z-TCM z C 40/W 500 z C 40/W 500 Principle of operation Detectors with smaller z-extent yield better performance! Kalender WA. Computed Tomography. 2nd ed. Wiley, New York 2005 Advances in CT Technology • State of the art in CT • Technology • Flat detector CT - C-arm-based CT - Facio-mandibular skull CT - Breast CT - Micro-CT -… 3D Angio (since <2000) Seite 15 15 CT Imaging using rotating C-arm Systems Image Intensifiers Flat-Panel Detectors CT Imaging using rotating C-arm Systems 3D Angio (since <2000) after intraarterial injection with image intensifiers Dyna CT (since >2000) after intravenous injection with flat panel detectors Interventional Radiology: Vertebroplasty Images: Courtesy of Arnd Dörfler, Erlangen Seite 16 16 Interventionl Radiology: Vertebroplasty Images: Courtesy of Arnd Dörfler, Erlangen FD-CT is still inferior to clinical CT with respect to image quality and dose utilisation, but itt offers o e s excellent e ce e t co conditions dto s for interventional procedures and for intraoperative imaging! Hepatocellular Carcinoma; Embolization Embolisation of a hepatocellular carcinoma Images: Courtesy of PD R. Loose, Nuremberg 3D Patient Dose Distributions calculated by Monte Carlo methods methods** Kyriakou Y, Dörfler A, Kalender WA. AJNR 2008 * Deak, van Straten, Shrimpton, Zankl, Kalender. Eur Radiol 2008; 18:759-772 Seite 17 17 Robot--driven C-arm Systems Robot Prototype in operation since June 2006 Product installation in November 2007 Large Volume Coverage with Robot--driven C Robot C--arm CT 30× 30 ×40 cm² detector Conventional mechanics: < 25 cm diameter, <20 cm height Courtesy of M. Reiser Munich, Germany … and Fluoroscopy UFE: 3D vascular anatomy Courtesy of M. Reiser Munich, Germany Seite 18 18 C-arm system rotating at 100 100°°/s to make perfusion measurements C-arm system rotating at 100 100°°/s to make perfusion measurements 0~2 s 4~6 s 8~10 s 12~14 s 16~18 s 20~22 s 24~26 s t High--Resolution CT of the Breast High Micro--CT scan of surgical specimens Micro DCIS specimen embedded in paraffine HiRes Micro-CT 40 µm resolution Kalender WA. Eur Radiol 2009; 19(S4):849-852 Seite 19 19 Breast CT scanner concept Transition from single-circle singleto flat detector spiral CT detector Pre-clinical testing expected for the end of 2011 Kalender WA. Eur Radiol 2009; 19(S4):849-852 Thank you for your attention! attention! [email protected] [email protected] -erlangen.de Seite 20 20