Organ Dose estimates for Radio-Isotope Therapy treatment planning purposes

Size: px
Start display at page:

Download "Organ Dose estimates for Radio-Isotope Therapy treatment planning purposes"

Transcription

1 GE Healthcare Organ Dose estimates for Radio-Isotope Therapy treatment planning purposes Dosimetry toolkit package White Paper

2 Content Introduction... 3 Dosimetry Toolkit... 4 Purpose... 4 Input... 4 Content... 4 Output... 4 SPECT Reconstruction... 4 Quantitative Reconstruction... 5 Registration... 5 Organs definition... 6 Segmentation operations... 6 ROI/VOI tools:... 6 System sensitivity calibration standard dose syringe... 7 Time Activity Curves and fitting... 8 Saving results... 8 Algorithms and clinical examples used... 9 Registration Algorithm... 9 Registration stages in Multi WB SPECT/CT scenario... 9 Registration stages in Hybrid scenario... 9 Segmentation algorithms...10 Threshold criterion for NM image...10 Threshold criterion for CT image...10 Segmentation Propagation...11 Inner segmentation...11 Coronal Overlap (Hybrid scenario)...11 System suggested organs Segmentation:...12 Lungs segmentation...12 Liver segmentation...12 All bone cavities segmentation...13 Additional tools for Non-contiguous volumes...13 System sensitivity calibration standard dose syringe...14 References...15

3 Introduction Radio Isotope therapy is defined as a radiation therapy that uses administered radiopharmaceutical to transfer radiation energy to a pathological target tissue in order to achieve a destructive tissue effect. The destructive tissue effect depends on the amount of transferred energy to the tissue, i.e the absorbed radiation dose, which is measured in units of gray (Gy). It is essential to be able to calculate the absorbed radiation dose to a targeted tissue at any stage of treatment in order to enable safe and effective therapy planning and monitoring. Note: The term dose refers to the radiation dose in the SI unit grays. It should not be confused with the frequently used dose to describe the administered activity in GBq or mci. Targeted Radio Isotope Therapy is used today for single focal lesion of tumors: breast, lung, prostate, etc. The aim in the near future is to have personalized therapy based on patients genetic or protein profiles. Targeted Radio Isotope therapies will be prescribed based on molecular signatures. Individual patient dosimetry may support the following goals: To determine minimum effective and maximum tolerated absorbed doses per individual patient To monitor tumor response and organ toxicity during treatment To predict tumor response and normal organ toxicity based on pre-therapy dosimetry To compare the dose response results of different therapy strategies Radiation in radionuclide therapy is directed to the target tissue by the radiopharmaceutical. This dynamic metabolic process creates a complex spatial and temporal radiation distribution with biochemical and physical variations over time. Pharmacokinetics as well as biological or physical bystander effects (on non-target organs) influence the amount of the radiation dose to the target. In contrast to externalbeam radiation therapy, which uses a controlled and time limited radiation, radionuclide therapy delivers a low and continuously decreasing dose rate. Therefore the calculation of the accumulated radiation dose for radionuclide therapy is complex. Nuclear Medicine (NM) imaging is used to measure the activity distribution over time. The calculation of the absorbed dose in each organ is based on these scans. Due to the limited spatial resolution of the NM scans, the dosimetry calculations are always an approximation. Radiation doses to target organs are usually calculated using the MIRD formalism by commercially available software such as MIRDOSE3 or OLINDA/EXM. These models are based on assumptions about anatomy (standard man and woman) and radiopharmaceutical distribution (uniformity of uptake in source and target) that are not necessarily valid in individual patients. Nevertheless they provide a practical and standardized model for clinical practice [1]. The aim of the dosimetry toolkit is to simplify the procedure for quantifying radiopharmaceutical dose, reduce the processing time and improve accuracy of results, compared to the manual tools currently used. The Dosimetry toolkit creates an essential input to other radiotherapy planning SW.

4 Dosimetry Toolkit Purpose Dosimetry Toolkit uses multi WB SPECT/CT and/or WB planar datasets for quantifying changes in radiopharmaceutical uptake over time and calculating residence time per organ for Radio-Isotope Therapy treatment planning purposes. The purpose of the Dosimetry Toolkit is to define and report the patient organs volume, activity and residence time of radiopharmaceutical concentration within patient organs. These results are based on consecutive patient scans and can be used as input for Radio-Isotope Therapy planning applications (such as OLINDA or similar). The organs of interest in this respect are large organs (more than 50cc), such as liver, lungs, kidneys, spleen, and heart. Note: This toolkit is intended to replace tedious manual tools for organs definition and activity calculations, in order to enable improved processing workflow and productivity. The accuracy of the dosimetry toolkit results depends heavily on user provided quantitative input: injected activity, organ definition, system sensitivity and reconstruction parameters. The user is encouraged to verify the dosimetry toolkit results vs. the existing tools used by the facility. This verification should be performed prior to the clinical use of the dosimetry Toolkit. Input The toolkit supports the following types of input: Series of whole body SPECT/CT scans Series of Whole Body Planar scans with single SPECT/CT (Hybrid scenario) Series of planar WB (for which Volume results can not be provided) A single time sample of SPECT/CT can be used to determine the organs volume and activity. Content The Dosimetry toolkit includes tools that can help the user to perform in a quick and convenient way the following tasks: Reconstruction of all raw SPECT/CT data, including accurate SPECT/CT registration adjustment and quality control, along with patient motion detection and correction, attenuation, scatter and collimator blurring corrections. Image reconstruction is performed using iterative algorithm (OSEM). Registrations of all the scans to one common reference with semi-automatic/manual tools that enable the user to perform local organ registration Segmentation of the different organs (such as heart, liver, lungs, kidneys, spleen, bone marrow), with semi-automatic/ manual tools to differentiate between overlapping organs Create time activity curves for each of the organs Curve fitting Calculate imaging agent Residence time in each organ Output The toolkit can export: Organs volumes Organs activities Organs imaging agent time activity curves Organs imaging agent residence time Individual or combined organ masked volumes as datasets. These datasets can be exported in Dicom format All numerical values (volumes, activities, residence time) can be exported to MS Excel file Time and Percentage of injected dose can be saved in format suitable for input to OLINDA, avoiding the need to type all the results in OLINDA interface SPECT Reconstruction The quality and quantitative accuracy of SPECT reconstructed images are affected by noise in the projection data, resolution degradation caused by the collimator-detector response (CDR) function of the imaging system, photon attenuation, and scatter in the patient s body. Recently, there has been significant progress in the development of model-based corrective SPECT image reconstruction methods that include correction for these image quality-degrading factors. The corrective image reconstruction package (also referred to as Resolution Recovery) developed by Johns Hopkins University (JHU) provides improved SPECT images by including physical models of the imaging process into iterative image reconstruction algorithms. In particular, it provides accurate 3D models of the collimator-detector response functions for a variety of clinical applications. This results in a significant

5 enhancement in image quality and potential improvement in diagnostic properties. Clinical application of these techniques are available and can be applied to reduce SPECT acquisition time with equal or better image characteristics when compared to standard reconstructions [5]. Collimatordetector blur is the main factor affecting the resolution and noise properties of nuclear medicine images. In reconstructed SPECT images, these characteristics are strongly affected by the applied reconstruction algorithm and its parameters. Collimator Detector Response (CDR) consists of four main components: intrinsic response (system without collimator), the geometric, septal penetration and septal scatter components of the collimator parameters. The geometric component of CDR results from photons passing through the collimator holes without interacting with the collimator itself. The septal penetration component describes the portion of the CDR where photons reaching the detector after passing through one or more septa do not scatter. The scatter component refers to photons that scatter in the septa and are detected. For the majority of clinically used collimator designs, the last two components are generally significant for only mediumand high-energy imaging. For each combination of acquisition system, radiopharmaceutical and particular acquisition protocol, the collimator detector response function provides the probability that a photon emitted from any point of the imaged object will contribute to a pixel of the resulting image. By including an accurate model of the collimator-detector response function in an iterative SPECT reconstruction algorithm, the blurring effect may be included in the iterative reconstruction process, resulting in improved spatial resolution. Current estimate Update Update coefficients Project Physics of the imaging prosess Back project Figure: Scheme of iterative reconstruction process. Estimated projection Compare Error Projection Measured projection (Date) A CDR compensation technique was developed at the University of North Carolina-Chapel Hill (UNC) and JHU [6,7,8]. The effect of CDR compensation on reconstructed images has been studied from qualitative [9], quantitative [10,11,12], and clinical task-based [13, 14, 15] perspectives. It has been found that CDR corrected images demonstrate not only improved resolution and signal-to-noise ratio, but also lower noise variability in reconstructed images. Significant improvement of the resolution properties requires more iterations of the reconstruction method with compensation than are usually recommended for the same data when no compensation is applied. On the other hand, image noise level tends to amplify with the number of iterations. Taking into account the differences in the iterative reconstruction process, with and without CDR, application-specific optimization of acquisition and processing parameters is essential to successful utilization of the corrective reconstruction method [14, 15, 16,17]. Quantitative Reconstruction Usually the reconstruction used for visualization purposes is done with limited number of iterations and with postfiltering. For more accurate quantitative results the number of iterations should be increased and postfiltering should be avoided. The resulting image is quantitatively more accurate, but also noisier and less suitable for visualization purposes. The reconstruction parameters (number of iterations, number of subsets) for accurate quantitation should be optimized per each radiopharmaceutical, collimator and clinical protocol (scan time, number of views etc ). For example, for quantitative reconstruction of In111 scans with MEGP collimator, it is recommended to use 30 iterations with 5 subsets [18,19]. In order to optimize reconstruction parameters per specific Isotope/ Collimator/Camera combination, the user should use phantom studies of Jaszczak and/or anthropomorphic phantom(s). In order to improve quantitative accuracy, reconstruction should include corrections for patient motion, attenuation, scatter and collimator blurring. Registration The application includes two stages of registration: WB registration and organ registration. First all the WB scans (SPECT/CT or WB planar) are registered, to achieve optimal registration of the complete patient body (or all the scanned parts of it) between all scans. Although the whole body, registered as rigid body, may be properly registered, internal organs may be slightly mis-registered due to local shifts/ rotation. Once the scans are registered, the user can correct location and shape of each Organ VOI (SPECT/CT) or ROI (Planar) on each of the images, if needed.

6 Organs definition Note: The following is applicable to multiple SPECT/CT or Hybrid Scenarios Only. Defining an Organ on Multiple Planar WBs scenario is freehand ROI drawing based on the operator experience. Organs are defined using the CT and NM slices interchangeably, using threshold-based algorithms. Some organs may have an initial automated proposal or semiautomatic proposal; some organs are defined manually. The defined organ is superimposed over CT and NM slices. All organs are saved in a mask volume, each with a new color. The user must confirm that organs are accurately defined. In some cases the system may suggest initial segmentation for specific organs, nevertheless the responsibility always lies on the user to confirm that the organ volume is delineated correctly. Results are more accurate for large volumes (more than 50cc). For smaller volumes (of organs or lesions), accuracy of activity quantitation is degraded due to partial volume effects that are inherent because of the limited gamma camera spatial resolution. The discrepancy between NM and CT resolution causes organ s activity to spill over the organs contours as depicted in the CT image. In order to include all the organ s activity within the VOI, the organ VOI definition may be expanded slightly beyond the organ s limits as depicted in the CT image. For organs that are defined based on the CT image, the user may consider slight dilatation of the organ VOI beyond the CT limits in order to get more accurate organ s activity estimation (note that in this case the volume measurement is less accurate). To project the SPECT organs accurately over the WB planar images, their frontal outline is created. Some organs may overlap, mostly with the lungs. Overlapped areas may be removed when projected over the planar images. Computation of organ activities in the planar images is extrapolated by the ratio of used/removed volumes. Segmentation operations are based on the underlying data and use threshold operators to segment the data. The selected viewport, CT or NM, is the basis for the threshold segmentation. For both NM and CT images, the segmentation process starts at a user selected seed point and propagates in 2D/3D (ROI or VOI). The segmentation propagates when some or all the adjacent voxels withstand the threshold criterion. The propagation is stopped when none of the adjacent voxels comply with the threshold criterion. ROI/VOI tools: ROI tools are working on a single slice (2D). VOI tools act similar to the ROI tools, extended to 3D. The VOI tools cover large volumes without the need to go over slice by slice, however the visualization and ability to control their expansion are more complex as the screen display is 2D. Segmentation ROI/VOI Tools available: Draw automatic ROI/VOI starting at a user selected seed point, Draw semi automatic ROI/VOI starting at a seed point ( growing ROI/VOI ), Draw manual ROI/VOI starting at a seed point (acts as a pencil), Erase automatic ROI/VOI starting at a seed point, Erase semi automatic ROI/VOI starting at a seed point, Erase manual ROI/VOI starting at a seed point (acts as an eraser). Dilate Region/Volume voxels Erode Region/Volume voxels Open Bridges Close Gaps Auto NM segmentation Segmentation operations The application segments the WB SPECT/CT image volume into different organs this means that each organ is enclosed by a VOI. This segmentation is done based on the CT and NM images and serves as first approximation of the organs volumes. The user has various tools to correct/improve this automated segmentation prior to confirming the organ segmentation.

7 System sensitivity calibration standard dose syringe System sensitivity should be measured for each combination of camera, collimator and radioisotope used. Accurate measurement of the patient injected activity dose in a calibrated dosimeter is required. Time of dosimeter measurement must be recorded to allow accurate decay correction. In order to accurately measure system sensitivity and compensate for variations in system sensitivity between scans, a standard dose syringe can be used. A syringe with small amount of dose is placed near to and outside the patient during the sequence of acquisitions. The initial syringe activity should be measured by an external dosimeter (time of measurement should be recorded) and should also be imaged in a separate scan on the camera. The same syringe (with its decaying activity) should be used in all patient scans. The user fills a dialog (see below) with patient and syringe information. The standard dose syringe images are used to calibrate the patient counts acquired, based on the known half-life of the isotope used. If there is no syringe image the application activates a dialog to specify the system sensitivity by the user. Commercially available OLINDA software package can be used for calculation of NM radiopharmaceuticals internal absorbed doses in organs and tumors.

8 Time Activity Curves and fitting Time activity curve is created for each of the organs defined. These curves are fitted to an exponential function of the form: y = A e BX Usually exponential fit is done by taking the logarithm of the function and looking for the parameters that give the least square fit. This fit gives greater weights to small y values so, in order to weight the points equally, it is often better to minimize the function n y i (ln y i -a-bx i ) 2 i =1 See reference [4] The equal weight exponential fit is used in Dosimetry Toolkit. Saving results The picture below shows the final report The results are saved on the Xeleris workstation. The user is able to save segmented data and organ names, as part of a results series. Data recorded at the Xeleris database is DICOM compatible. It can be exported, backed up and retrieved, and is transferable between Xeleris 3 Systems. A template for MS Excel spread sheet is provided for the numerical results. Time and Percentage of injected dose can be saved in format suitable for input to OLINDA, avoiding the need to type all the results in OLINDA interface. Commercially available OLINDA software package can be used for calculation of NM radiopharmaceuticals internal absorbed doses in organs and tumors.

9 Algorithms and clinical examples used Registration Algorithm The registration is performed automatically with a rigid registration algorithm that utilizes the NLM Insight Segmentation & Registration Toolkit (ITK). Tools for manual adjustment of the scans are provided, for small modifications of the automatic registration results, in order to get the optimal registration. Automatic Image registration is an iterative process that is performed on coarse resampled image with a gradual increase in resolution, in a stepwise manner to determine the final translation and rotation parameters. This stepwise algorithm results in improved registration (over one step registration ) both in terms of reducing processing time, in its convergence to accurate true solution and the robustness of the solution. The automatic registration is based on the following components: The transformation of the image voxel positions to new 3D coordinates (x, y, z position). For rigid registration this will include translation and rotation. A cost function-a metric depicting the adequacy of the registration. The optimizer-determines how to update the transformation parameters after each iteration, based on the change in values of the cost function. Regular Step Gradient Descent optimizer and least mean Squares cost function are used in all the steps. In the first coarse steps the transformation include translation operation only, while in the later finer steps the transformation include both translation and rotation operators. Registration stages in Multi WB SPECT/CT scenario In the Multi WB SPECT/CT scenario that includes a Series of Whole Body SPECT/CT scans, there are two stages of registration: WB Registration of all SPECT/CT sets to a common reference this stage is performed before organs are defined Organs local registration on each of the WB SPECT/CT images WB registration After all the NM & CT scans were reconstructed (using standard Volumetrix MI UI) to create set of 3D whole-body images of the patient in various time points, all the scans are registered to one common reference. The reference image is the CT image of the latest scan, while the moving images (the images that are moved in order to be registered to the reference) are the CT images of all the other scans. Organ registration After all organs have been defined on the earliest SPECT/CT image, the organs masks are copied onto all the other SPECT/CT images (sets) and the user is required to check organs positions on each set. These sets are already rigidly registered to a common reference. The program loads the user selected set of registered NM & CT images. Organs defined on the first set are copied onto this set. The user has to review and adjust each organ in the loaded set, if needed. The same operation is repeated for all SPECT/CT sets. Registration stages in Hybrid scenario In the hybrid scenario that includes a Series of Whole Body Planar scans with single SPECT/CT, there are three stages of registration: Registration of the SPECT scan with the nearest in time planar WB scan. This stage is performed before organs are defined Registration of all WBs to common planar reference (used in the previous stage) this stage is performed after organs are defined Organs local registration on each of the WB planar images For all these registration stages, the application suggests initial registration and the user can confirm or modify the registration.

10 Registration of SPECT image with its conjugate WB planar image When the automatic registration is completed, the registered images are displayed in the order they were acquired. Manual adjustment of registration is supported via a screen based user interface to match every pair of WB planar images, for small modifications of the automatic registration, in order to get optimal match. Organ specific registration between consecutive scans After all the WB planar images are registered to a common reference, the user is able to manually correct residual local (organ specific) mis-registration. Segmentation algorithms Threshold criterion for NM image The reference image is the summed coronal slices of the SPECT image while the moving image is the nearest in time WB planar image. This WB scan serves as a common reference for all the other WB scans. Manual adjustment of registration is supported via a screen based user interface, for small modifications of the automatic registration, in order to get optimal match of SPECT 3D scan (single or multi fields of view) with the Wholebody 2D image. Registration of all WBs to common planar reference The threshold value is defined by the counts at the seed point multiplied by the NM Threshold (in the range of 0-1). All the voxels with counts above the threshold pass the threshold criterion. Threshold criterion for CT image The CT range in Hounsfield Units (HU) is divided into 3 ranges: Lungs values all values below a predefined, customizable value (default=-400). If the seed point is in the lungs range, all the voxels in the lungs range (HU <-400) pass the threshold criterion. Bones values all values above a predefined, customizable value (default=200). If the seed point is in the Bones range, all the voxels in the Bones range (HU > 200) pass the threshold criterion. Soft tissue values all values between the Lungs and the Bones. If the seed point is in the soft tissue range (-400 < HU < 200), the threshold criterion is defined as follows: The reference value is equal to HU Value at the Seed point , and the CT percents from the reference value define the threshold (in units of HU+1000). All the voxels with HU values in the range of the reference value +/-CT percent pass the threshold criterion. After all organs are segmented and defined on the WB SPECT/CT image, the 3D organs masks are projected onto the conjugate WB planar image. All the WB planar images have to be registered in order to project the organ ROIs at their correct location over the scans at all times. Initial registration of all WBs to common planar reference is performed automatically, without user intervention. The same WB scan that was already registered to the SPECT image (the WB planar image nearest to the SPECT image) is used as a reference for the other WB planar scans to register to. Example: for a seed of HU=100 with a CT percent threshold of 8%, all voxels in the range of 12HU to 188HU are searched, as 12 =( )*(1-0.08)-1000, 188 =( )*(1+0.08)-1000

11 Segmentation Propagation The segmentation process starts at the seed point. All neighbors within a specified square/cube are checked. Voxels that comply with the threshold criterion are entered into the cache and added to organ VOI. When all neighbors of current voxel were tested, the current voxel is removed from the cache. This process continues for the neighbors of all the voxels within the cache and stops when the cache is empty. This process is referred to as outer segmentation (the default). The square/cube size to each side of the current voxel is defined by the Neighbors parameter. The default value for outer segmentation neighbors is 1 so neighbors cube size is 3*3*3 voxels (3 voxels include the current voxel and one neighbor at each side). The picture below demonstrates the segmentation propagation on an NM image. The segmentation process starts at the seed point (the left image) and is built up according to the threshold criterion as shown on the images to the right. Manual mode-holding and moving left mouse button ( drag ), starts to paint the segmentation manually, with the current setting of pen size. (0 5 pixels to each side of the pointer tip). This mode also holds when one moves the mouse while the Semi Automatic iteration is in place, as described above. Inner segmentation Holding the [Shift] key prior to starting the automatic and semiautomatic modes activates an inner search. This continues the propagation only when the full square/cube around the voxel is passing the threshold criterion (as defined above). To stop the propagation it is enough to have one voxel within the cube that does not meet the threshold criterion. The default value for inner neighbors is 3 (defining 7*7*7 cube). A practical example: Using outer segmentation by [Alt]+Clicking on a point inside the Left lung in a CT slice (left image) will look for all points below 400HU (the default lung threshold) and continue as long as one of neighbors (a 3*3*3 cube) is less than-400. This catches the trachea as part of the lung as shown on the center image below. Using the inner segmentation technique ([Alt]+[Shift]+Clicking on a point inside the Left lung), the resultant segmentation avoids the trachea as shown on the right image below. There are 3 modes for Segmentation Propagation: Semi-Automatic mode-holding left mouse button continuously, without moving it, starts the semi-automatic segmentation propagation, as shown above. The process stops on one of the following: -- when the segmentation ceases to find new points withstanding the segmentation criterion (empty cache). An audible note will notify the end of the process. -- the user releases the mouse button. -- the user starts to move the mouse. Automatic mode-holding the [Alt] key while clicking the left mouse button, starts the automatic segmentation propagation. The process stops when no new points withstanding the segmentation criterion are found (empty cache). During the propagation the user does not see the progress of the segmentation. The automatic segmentation result is shown only when it is completed (an hourglass cursor indicates the process). Coronal Overlap (Hybrid scenario) In the case of Hybrid Scenario the 3D organs masks are projected to the WB planar 2D image. In this case overlap between projected 2D organs may occur. The toolkit enables handling this overlap. The 3D presentation menu includes the [coronal overlap] menu entry. When selected, the 3D image is projected to the anterior view and all the regions, which contain more than one organ, are painted in white. The areas in white do not represent the depth, contradictory to the other surface rendered parts of this image. They symbolize the fact that there are overlapped organs along this coronal line. Hovering over these areas print the organs involved and the Volume/counts of the overlapped volumes.

12 A voxel within lung is searched. The algorithm looks for a sequence of 6 cms of continuous lung voxels all with HU<- 200, that follows a sequence of 4 cms of tissue voxels over 200HU. The next lung voxel that follows the lung sequence is determined as the seed point. 8 vectors, starting at the seed point, along the 8 diagonals, must hit a soft tissue before reaching the edge of the image. If any vector hits the border, this seed is not within the lung and a new seed is searched for. By default, the volumes of these overlapped areas are removed from the planar coronal ROIs. The counts (activities) and volume of the remaining partial organs are extrapolated by the ratio of the known full volume to the partial volume, assuming that the organ has uniformly distributed activity. As this may not be the case, the user has to determine which organ this sub volume belongs to. System suggested organs Segmentation: The system can suggest automatic segmentation for several organs: Lungs Liver All Bone Cavities (bone marrow + spinal cord) In order to initiate the automatic segmentation the workspace must be empty (no voxel has been segmented yet). The user can request automatic segmentation for the 3 organs above by selecting the organ from the Organ Pick list and click [Confirm]. The organ is not declared automatically, allowing the user to edit the VOI before confirming it by pressing Confirm button again. Additional tools for non contiguous volumes (soft tissue, fat, soft tissue + fat etc ) are available. Lungs segmentation The system suggested lung segmentation is based on the clear lung boundaries on the CT image. Use of the standard semiautomatic or automatic propagation segmentation will usually include the trachea and other air cavities. In order to avoid the air cavities outside the lungs, the automatic lung segmentation works as follows: Once such a seed point is found, an inwards segmentation below 200 is performed with 3 neighbors. The segmentation propagation collects only voxels having the full 7*7*7 voxels (15.4 mm3) cube around them passing the threshold criterion of HU<-200. As the mainstem bronchial diameter is less than 15mm (see reference [2,3]), an inward segmentation with neighborhood of 15.4mm will not include the mainstem bronchial. Once such inner part of the lung is found, dilation of 3 voxels below 200HU fills back the missing boundaries. This is first done for right lung and then for the left. The picture below displays automatic lung detection Coronal, sagittal, transaxial and 3D presentation. Liver segmentation Liver is considered to have uniform HU values and slow edges. It is also assumed that the boundaries of the liver and other surrounding soft tissues are well defined. As there are many soft tissue organs that fill these criteria, the user should triangulate at the center of the liver prior to call for the automatic segmentation. This defines both the seed and the mean HU to look for. An inwards segmentation with 4 neighbors is applied, defining a neighborhood of 9*9*9 voxels (19.8mm 3 ) cube. As the boundaries depend on patient motion during the CT scan, e.g. heavy strikes initiated from breathing, Liver Heart

13 it requires a bit of experience to define a good seed point to get accurate liver delineation as in the picture below Inverse of the result above gives the bone cavities voxels. and not erroneous liver segmentation that includes other organs (see picture below) The following slices show both marrow in the sternum and spinal cord. All bone cavities segmentation Automatic segmentation of all bone cavities can be used to define bone marrow The automatic search for bone cavities is performed as follows: The segmentation is performed on the CT image. The segmentation does not separate between Red and Yellow Marrow tissues. The quality of the detected cavities depends mostly on the thickness of the CT slices. Thick slices, such as the above (4.26mm) will interpolate axial cavities, affecting both the HU values and the axial resolution. Additional tools for Non-contiguous volumes Tools are available for enabling non-standard segmentation in cases where the volume of interest is not contiguous. At first stage all the voxels above 100HU are marked regardless of continuity. Adding to these voxels additional voxels by starting a segmentation from a seed point at the top left corner, to include all the voxels having HU below 100HU (i.e. Soft tissue and air) with requirement for Continuity. Full Tissue segmentation enables segmentation of spatially non-contiguous voxels within selected density (HU) range. It is activated on the CT image by holding the [Alt]+[F]. The HU range is defined by the HU value of the seed point and the CT percent threshold. The segmentation marks all voxels that comply with the threshold criterion based on the seed point and the CT percent. There is no requirement for continuity of voxels. Left image shows bone segmentation-seed point selected on bone, bone CT threshold criterion is used. Center image shows soft tissue segmentation. Seed point selected on soft tissue, soft tissue CT threshold criterion is used. Right image shows fat segmentation. Seed point selected on fat, soft tissue CT threshold criterion is used. Bone tissue fat Previously found voxels (HU>100) block segmentation propagation from penetrating the bone. The new segmentation includes all voxels except bone cavities.

14 Further segmentation is available by adding to the current segments: Below an example of adding fat to soft tissue: First performing soft tissue segmentation (as described above) then add fat by holding the [Alt]+[F] while clicking on fat voxel. System sensitivity calibration standard dose syringe The user fills a dialog with patient and standard dose syringe information. The standard dose syringe images are used to calibrate the patient counts acquired, based on the known half-life of the isotope used. If there is no calibration image the application activates a dialog to specify the system sensitivity by the user. For Hybrid and WB scenarios If a standard dose syringe is scanned within the patient WB planar scans, the application detects its location over all the geometrical mean images, and place ROIs over them. The syringe activity (counts per pixel) is assumed to be much higher than patient activity. The user can review and edit these ROIs as needed. In order to avoid decrease of patient image color dynamic range, the system finds the maximal count outside the standard dose and uses it as initial window level. Note that each of the patient scans are displayed with a different window level, thus the display does not reflect the relative intensity between scans. Using the standard dose permits longer late scans to get clearer organs silhouettes while maintaining accurate dose calculations. Multi SPECT/CT scenario A separate standard dose syringe image may be acquired. The user has to enter the syringe activity dose used for the calibration image as part of the patient activity Dialog. Calibration scan should be acquired as a static dual head image of the standard dose syringe. The application detects the source using 1% of its maximum value as the threshold, and the average counts of the 2 images are used to compute the Calibration factor.

15 References 1. B. Brans & L. Bodei & F. Giammarile & O. Linden &M. Luster &W. J. G. Oyen & J. Tennvall. Clinical radionuclide therapy dosimetry: the quest for the Holy Gray. Eur J Nucl Med Mol Imaging (2007) 34: Estimating the diameter of the left main bronchus. Anaesth Intensive Care Oct;28(5): The relationship between left mainstem bronchial diameter and patient size Journal of Cardiothoracic and Vascular Anesthesis, Volume 9, Issue 2, Pages (April 1995) 4. LeastSquaresFittingExponential.html#eqn10 5. Volokh, L., et al., Efficacy of corrective reconstruction with collimator detector response compensation for short Tc-99m bone SPECT acquisition in a bone lesion detection task./abstract presented at SNM Meeting, Tsui, B.M.W., et al., Implementation of simultaneous attenuation and detector response correction in SPECT. IEEE Transactions on Nuclear Science, (1): p Tsui, B.M.W., et al., The importance and implementation of accurate three-dimensional compensation methods for quantitative SPECT. Phys Med Biol, (3): p Tsui, B.M.W., et al., Characteristics of reconstructed point response in three-dimensional spatially variant detector response compensation in SPECT, in Three-Dimensional Image Reconstruction in Radiology and Nuclear Medicine, P. Grangeat and J.-L. Amans, Editors. 1996, Kluwer Academic Publishers. p Tsui BMW, Zhao XD*, Frey EC and McCartney WH. Quantitative SPECT: Basics and Clinical Considerations. Seminar in Nuclear Medicine, Vol. XXIV, No 1 (January), pp 38-65, Pretorius, P.H., et al., Reducing the influence of the partial volume effect on SPECT activity quantitation with 3D modelling of spatial resolution in iterative reconstruction. Physics in Medicine and Biology, (2): p Kohli, V., et al., Compensation for distance-dependent resolution in cardiac-perfusion SPECT: impact on uniformity of wall counts and wall thickness. Nuclear Science, IEEE Transactions on, (3): p Pretorius, P.H., et al., Comparison of detection accuracy of perfusion defects in SPECT for different reconstruction strategies using polar-map quantitation. Ieee Transactions on Nuclear Science, (5): p Narayanan, M.V., et al., Human-observer receiveroperating-characteristic evaluation of attenuation, scatter, and resolution compensation strategies for Tc-99m myocardial perfusion imaging. Journal of Nuclear Medicine, (11): p Frey, E.C., K.L. Gilland, and B.M.W. Tsui, Application of task-based measures of image quality to optimization and evaluation of three-dimensional reconstruction-based compensation methods in myocardial perfusion SPECT. IEEE Transactions on Medical Imaging, (9): p He, X, et al., A mathematical observer study for the evaluation and optimization of compensation methods for Myocardial SPECT using a phantom population that realistically models patient variability. IEEE Transactions on Nuclear Science, (1): Sankaran, S., et al., Optimum compensation method and filter cutoff frequency in myocardial SPECT: A human observer study. Journal of Nuclear Medicine, (3): p Gifford, H.C., et al., LROC analysis of detector-response compensation in SPECT. IEEE Transactions on Medical Imaging, (5): p He B, Wahl RL, Du Y, Sgouros G, Jacene H, Flinn I and Frey EC. Comparison of Residence Time Estimation Methods for Radioimmunotherapy Dosimetry and Treatment Planning : Monte Carlo Simulation Studies. IEEE Trans Med Imaging Apr;27(4): He B, Wahl RL, Sgouros G, Du Y, Jacene H, Kasecamp WR, Flinn I, Hammes RJ, Bianco J, Kahl B, Frey EC. Comparison of organ residence time estimation methods for radioimmunotherapy dosimetry and treatment planningpatient studies. Med Phys May;36(5):

16 2011 General Electric Company-All rights reserved. General Electric Company reserves the right to make changes in specifications and features shown herein, or discontinue any products described at any time without notice or obligation. Please contact your GE representative for the most current information. *GE, GE Monogram and imagination at work are trademarks of General Electric Company. GE Healthcare is a division of General Electric Company. About GE Healthcare GE Healthcare provides transformational medical technologies and services that are shaping a new age of patient care. Our broad expertise in medical imaging and information technologies, medical diagnostics, patient monitoring systems, drug discovery, biopharmaceutical manufacturing technologies, performance improvement and performance solutions services help our customers to deliver better care to more people around the world at a lower cost. In addition, we partner with healthcare leaders, striving to leverage the global policy change necessary to implement a successful shift to sustainable healthcare systems. Our healthymagination vision for the future invites the world to join us on our journey as we continuously develop innovations focused on reducing costs, increasing access and improving quality around the world. Headquartered in the United Kingdom, GE Healthcare is a unit of General Electric Company (NYSE: GE). Worldwide, GE Healthcare employees are committed to serving healthcare professionals and their patients in more than 100 countries. For more information about GE Healthcare, visit our website at GE Healthcare 3000 North Grandview Blvd Waukesha, WI U.S.A DOC

Validation of GEANT4 for Accurate Modeling of 111 In SPECT Acquisition

Validation of GEANT4 for Accurate Modeling of 111 In SPECT Acquisition Validation of GEANT4 for Accurate Modeling of 111 In SPECT Acquisition Bernd Schweizer, Andreas Goedicke Philips Technology Research Laboratories, Aachen, Germany bernd.schweizer@philips.com Abstract.

More information

Monte-Carlo-Based Scatter Correction for Quantitative SPECT Reconstruction

Monte-Carlo-Based Scatter Correction for Quantitative SPECT Reconstruction Monte-Carlo-Based Scatter Correction for Quantitative SPECT Reconstruction Realization and Evaluation Rolf Bippus 1, Andreas Goedicke 1, Henrik Botterweck 2 1 Philips Research Laboratories, Aachen 2 Fachhochschule

More information

Quantitative imaging for clinical dosimetry

Quantitative imaging for clinical dosimetry Quantitative imaging for clinical dosimetry Irène Buvat Laboratoire d Imagerie Fonctionnelle U678 INSERM - UPMC CHU Pitié-Salpêtrière, Paris buvat@imed.jussieu.fr http://www.guillemet.org/irene Methodology

More information

Ch. 4 Physical Principles of CT

Ch. 4 Physical Principles of CT Ch. 4 Physical Principles of CT CLRS 408: Intro to CT Department of Radiation Sciences Review: Why CT? Solution for radiography/tomography limitations Superimposition of structures Distinguishing between

More information

3/27/2012 WHY SPECT / CT? SPECT / CT Basic Principles. Advantages of SPECT. Advantages of CT. Dr John C. Dickson, Principal Physicist UCLH

3/27/2012 WHY SPECT / CT? SPECT / CT Basic Principles. Advantages of SPECT. Advantages of CT. Dr John C. Dickson, Principal Physicist UCLH 3/27/212 Advantages of SPECT SPECT / CT Basic Principles Dr John C. Dickson, Principal Physicist UCLH Institute of Nuclear Medicine, University College London Hospitals and University College London john.dickson@uclh.nhs.uk

More information

Concepts, Applications, and Requirements for Quantitative SPECT/CT. Conflict of Interest Disclosure

Concepts, Applications, and Requirements for Quantitative SPECT/CT. Conflict of Interest Disclosure Concepts, Applications, and Requirements for Quantitative SPECT/CT Eric C. Frey, Ph.D. (efrey@jhmi.edu) Division of Medical Imaging Physics Russell H. Morgan Department of Radiology and Radiological Science

More information

GE Healthcare. Vivid 7 Dimension 08 Cardiovascular ultrasound system

GE Healthcare. Vivid 7 Dimension 08 Cardiovascular ultrasound system GE Healthcare Vivid 7 Dimension 08 Cardiovascular ultrasound system ltra Definition. Technology. Performance. Start with a system that s proven its worth in LV quantification and 4D imaging. Then add even

More information

Optimization of CT Simulation Imaging. Ingrid Reiser Dept. of Radiology The University of Chicago

Optimization of CT Simulation Imaging. Ingrid Reiser Dept. of Radiology The University of Chicago Optimization of CT Simulation Imaging Ingrid Reiser Dept. of Radiology The University of Chicago Optimization of CT imaging Goal: Achieve image quality that allows to perform the task at hand (diagnostic

More information

multimodality image processing workstation Visualizing your SPECT-CT-PET-MRI images

multimodality image processing workstation Visualizing your SPECT-CT-PET-MRI images multimodality image processing workstation Visualizing your SPECT-CT-PET-MRI images FUSION FUSION is a new visualization and evaluation software developed by Mediso built on state of the art technology,

More information

Conflicts of Interest Nuclear Medicine and PET physics reviewer for the ACR Accreditation program

Conflicts of Interest Nuclear Medicine and PET physics reviewer for the ACR Accreditation program James R Halama, PhD Loyola University Medical Center Conflicts of Interest Nuclear Medicine and PET physics reviewer for the ACR Accreditation program Learning Objectives 1. Be familiar with recommendations

More information

Proton dose calculation algorithms and configuration data

Proton dose calculation algorithms and configuration data Proton dose calculation algorithms and configuration data Barbara Schaffner PTCOG 46 Educational workshop in Wanjie, 20. May 2007 VARIAN Medical Systems Agenda Broad beam algorithms Concept of pencil beam

More information

Tomographic Reconstruction

Tomographic Reconstruction Tomographic Reconstruction 3D Image Processing Torsten Möller Reading Gonzales + Woods, Chapter 5.11 2 Overview Physics History Reconstruction basic idea Radon transform Fourier-Slice theorem (Parallel-beam)

More information

Effects of the difference in tube voltage of the CT scanner on. dose calculation

Effects of the difference in tube voltage of the CT scanner on. dose calculation Effects of the difference in tube voltage of the CT scanner on dose calculation Dong Joo Rhee, Sung-woo Kim, Dong Hyeok Jeong Medical and Radiological Physics Laboratory, Dongnam Institute of Radiological

More information

James R Halama, PhD Loyola University Medical Center

James R Halama, PhD Loyola University Medical Center James R Halama, PhD Loyola University Medical Center Conflicts of Interest Nuclear Medicine and PET physics reviewer for the ACR Accreditation program Learning Objectives Be familiar with the tests recommended

More information

Design and Fabrication of Kidney Phantoms for Internal Radiation Dosimetry Using 3D Printing Technology

Design and Fabrication of Kidney Phantoms for Internal Radiation Dosimetry Using 3D Printing Technology Design and Fabrication of Kidney Phantoms for Internal Radiation Dosimetry Using 3D Printing Technology Johannes Tran-Gia, PhD NPL MEMPHYS Workshop Applications of 3D Printing for Medical Phantoms Klinik

More information

Philips SPECT/CT Systems

Philips SPECT/CT Systems Philips SPECT/CT Systems Ling Shao, PhD Director, Imaging Physics & System Analysis Nuclear Medicine, Philips Healthcare June 14, 2008 *Presented SNM08 Categorical Seminar - Quantitative SPECT and PET

More information

Mathematical methods and simulations tools useful in medical radiation physics

Mathematical methods and simulations tools useful in medical radiation physics Mathematical methods and simulations tools useful in medical radiation physics Michael Ljungberg, professor Department of Medical Radiation Physics Lund University SE-221 85 Lund, Sweden Major topic 1:

More information

Deviceless respiratory motion correction in PET imaging exploring the potential of novel data driven strategies

Deviceless respiratory motion correction in PET imaging exploring the potential of novel data driven strategies g Deviceless respiratory motion correction in PET imaging exploring the potential of novel data driven strategies Presented by Adam Kesner, Ph.D., DABR Assistant Professor, Division of Radiological Sciences,

More information

Implementation and evaluation of a fully 3D OS-MLEM reconstruction algorithm accounting for the PSF of the PET imaging system

Implementation and evaluation of a fully 3D OS-MLEM reconstruction algorithm accounting for the PSF of the PET imaging system Implementation and evaluation of a fully 3D OS-MLEM reconstruction algorithm accounting for the PSF of the PET imaging system 3 rd October 2008 11 th Topical Seminar on Innovative Particle and Radiation

More information

Prostate Detection Using Principal Component Analysis

Prostate Detection Using Principal Component Analysis Prostate Detection Using Principal Component Analysis Aamir Virani (avirani@stanford.edu) CS 229 Machine Learning Stanford University 16 December 2005 Introduction During the past two decades, computed

More information

Spiral CT. Protocol Optimization & Quality Assurance. Ge Wang, Ph.D. Department of Radiology University of Iowa Iowa City, Iowa 52242, USA

Spiral CT. Protocol Optimization & Quality Assurance. Ge Wang, Ph.D. Department of Radiology University of Iowa Iowa City, Iowa 52242, USA Spiral CT Protocol Optimization & Quality Assurance Ge Wang, Ph.D. Department of Radiology University of Iowa Iowa City, Iowa 52242, USA Spiral CT Protocol Optimization & Quality Assurance Protocol optimization

More information

3-D Monte Carlo-based Scatter Compensation in Quantitative I-131 SPECT Reconstruction

3-D Monte Carlo-based Scatter Compensation in Quantitative I-131 SPECT Reconstruction 3-D Monte Carlo-based Scatter Compensation in Quantitative I-131 SPECT Reconstruction Yuni K. Dewaraja, Member, IEEE, Michael Ljungberg, Member, IEEE, and Jeffrey A. Fessler, Member, IEEE Abstract- we

More information

Technical aspects of SPECT and SPECT-CT. John Buscombe

Technical aspects of SPECT and SPECT-CT. John Buscombe Technical aspects of SPECT and SPECT-CT John Buscombe What does the clinician need to know? For SPECT What factors affect SPECT How those factors should be sought Looking for artefacts For SPECT-CT Issues

More information

GPU implementation for rapid iterative image reconstruction algorithm

GPU implementation for rapid iterative image reconstruction algorithm GPU implementation for rapid iterative image reconstruction algorithm and its applications in nuclear medicine Jakub Pietrzak Krzysztof Kacperski Department of Medical Physics, Maria Skłodowska-Curie Memorial

More information

REMOVAL OF THE EFFECT OF COMPTON SCATTERING IN 3-D WHOLE BODY POSITRON EMISSION TOMOGRAPHY BY MONTE CARLO

REMOVAL OF THE EFFECT OF COMPTON SCATTERING IN 3-D WHOLE BODY POSITRON EMISSION TOMOGRAPHY BY MONTE CARLO REMOVAL OF THE EFFECT OF COMPTON SCATTERING IN 3-D WHOLE BODY POSITRON EMISSION TOMOGRAPHY BY MONTE CARLO Abstract C.S. Levin, Y-C Tai, E.J. Hoffman, M. Dahlbom, T.H. Farquhar UCLA School of Medicine Division

More information

Corso di laurea in Fisica A.A Fisica Medica 5 SPECT, PET

Corso di laurea in Fisica A.A Fisica Medica 5 SPECT, PET Corso di laurea in Fisica A.A. 2007-2008 Fisica Medica 5 SPECT, PET Step 1: Inject Patient with Radioactive Drug Drug is labeled with positron (β + ) emitting radionuclide. Drug localizes

More information

(RMSE). Reconstructions showed that modeling the incremental blur improved the resolution of the attenuation map and quantitative accuracy.

(RMSE). Reconstructions showed that modeling the incremental blur improved the resolution of the attenuation map and quantitative accuracy. Modeling the Distance-Dependent Blurring in Transmission Imaging in the Ordered-Subset Transmission (OSTR) Algorithm by Using an Unmatched Projector/Backprojector Pair B. Feng, Member, IEEE, M. A. King,

More information

Fits you like no other

Fits you like no other Fits you like no other BrightView X and XCT specifications The new BrightView X system is a fully featured variableangle camera that is field-upgradeable to BrightView XCT without any increase in room

More information

Image Acquisition Systems

Image Acquisition Systems Image Acquisition Systems Goals and Terminology Conventional Radiography Axial Tomography Computer Axial Tomography (CAT) Magnetic Resonance Imaging (MRI) PET, SPECT Ultrasound Microscopy Imaging ITCS

More information

If it matters to you, it matters to us

If it matters to you, it matters to us If it matters to you, it matters to us Philips clinical innovations in nuclear medicine Innovation with insight We understand that clinical innovations are only as valuable as the day-to-day difference

More information

RT_Image v0.2β User s Guide

RT_Image v0.2β User s Guide RT_Image v0.2β User s Guide RT_Image is a three-dimensional image display and analysis suite developed in IDL (ITT, Boulder, CO). It offers a range of flexible tools for the visualization and quantitation

More information

A Comparison of the Uniformity Requirements for SPECT Image Reconstruction Using FBP and OSEM Techniques

A Comparison of the Uniformity Requirements for SPECT Image Reconstruction Using FBP and OSEM Techniques IMAGING A Comparison of the Uniformity Requirements for SPECT Image Reconstruction Using FBP and OSEM Techniques Lai K. Leong, Randall L. Kruger, and Michael K. O Connor Section of Nuclear Medicine, Department

More information

IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 53, NO. 1, FEBRUARY

IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 53, NO. 1, FEBRUARY IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 53, NO. 1, FEBRUARY 2006 181 3-D Monte Carlo-Based Scatter Compensation in Quantitative I-131 SPECT Reconstruction Yuni K. Dewaraja, Member, IEEE, Michael Ljungberg,

More information

Diagnostic imaging techniques. Krasznai Zoltán. University of Debrecen Medical and Health Science Centre Department of Biophysics and Cell Biology

Diagnostic imaging techniques. Krasznai Zoltán. University of Debrecen Medical and Health Science Centre Department of Biophysics and Cell Biology Diagnostic imaging techniques Krasznai Zoltán University of Debrecen Medical and Health Science Centre Department of Biophysics and Cell Biology 1. Computer tomography (CT) 2. Gamma camera 3. Single Photon

More information

REAL-TIME ADAPTIVITY IN HEAD-AND-NECK AND LUNG CANCER RADIOTHERAPY IN A GPU ENVIRONMENT

REAL-TIME ADAPTIVITY IN HEAD-AND-NECK AND LUNG CANCER RADIOTHERAPY IN A GPU ENVIRONMENT REAL-TIME ADAPTIVITY IN HEAD-AND-NECK AND LUNG CANCER RADIOTHERAPY IN A GPU ENVIRONMENT Anand P Santhanam Assistant Professor, Department of Radiation Oncology OUTLINE Adaptive radiotherapy for head and

More information

DUAL energy X-ray radiography [1] can be used to separate

DUAL energy X-ray radiography [1] can be used to separate IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 53, NO. 1, FEBRUARY 2006 133 A Scatter Correction Using Thickness Iteration in Dual-Energy Radiography S. K. Ahn, G. Cho, and H. Jeon Abstract In dual-energy

More information

Image-based Monte Carlo calculations for dosimetry

Image-based Monte Carlo calculations for dosimetry Image-based Monte Carlo calculations for dosimetry Irène Buvat Imagerie et Modélisation en Neurobiologie et Cancérologie UMR 8165 CNRS Universités Paris 7 et Paris 11 Orsay, France buvat@imnc.in2p3.fr

More information

DUE to beam polychromacity in CT and the energy dependence

DUE to beam polychromacity in CT and the energy dependence 1 Empirical Water Precorrection for Cone-Beam Computed Tomography Katia Sourbelle, Marc Kachelrieß, Member, IEEE, and Willi A. Kalender Abstract We propose an algorithm to correct for the cupping artifact

More information

Hidenobu Tachibana The Cancer Institute Hospital of JFCR, Radiology Dept. The Cancer Institute of JFCR, Physics Dept.

Hidenobu Tachibana The Cancer Institute Hospital of JFCR, Radiology Dept. The Cancer Institute of JFCR, Physics Dept. 2-D D Dose-CT Mapping in Geant4 Hidenobu Tachibana The Cancer Institute Hospital of JFCR, Radiology Dept. The Cancer Institute of JFCR, Physics Dept. Table of Contents Background & Purpose Materials Methods

More information

Spatio-Temporal Registration of Biomedical Images by Computational Methods

Spatio-Temporal Registration of Biomedical Images by Computational Methods Spatio-Temporal Registration of Biomedical Images by Computational Methods Francisco P. M. Oliveira, João Manuel R. S. Tavares tavares@fe.up.pt, www.fe.up.pt/~tavares Outline 1. Introduction 2. Spatial

More information

SPECT QA and QC. Bruce McBride St. Vincent s Hospital Sydney.

SPECT QA and QC. Bruce McBride St. Vincent s Hospital Sydney. SPECT QA and QC Bruce McBride St. Vincent s Hospital Sydney. SPECT QA and QC What is needed? Why? How often? Who says? QA and QC in Nuclear Medicine QA - collective term for all the efforts made to produce

More information

CT vs. VolumeScope: image quality and dose comparison

CT vs. VolumeScope: image quality and dose comparison CT vs. VolumeScope: image quality and dose comparison V.N. Vasiliev *a, A.F. Gamaliy **b, M.Yu. Zaytsev b, K.V. Zaytseva ***b a Russian Sci. Center of Roentgenology & Radiology, 86, Profsoyuznaya, Moscow,

More information

Biomedical Image Analysis based on Computational Registration Methods. João Manuel R. S. Tavares

Biomedical Image Analysis based on Computational Registration Methods. João Manuel R. S. Tavares Biomedical Image Analysis based on Computational Registration Methods João Manuel R. S. Tavares tavares@fe.up.pt, www.fe.up.pt/~tavares Outline 1. Introduction 2. Methods a) Spatial Registration of (2D

More information

Fits you like no other

Fits you like no other Fits you like no other Philips BrightView X and XCT specifications The new BrightView X system is a fully featured variableangle camera that is field-upgradeable to BrightView XCT without any increase

More information

Structured Light II. Thanks to Ronen Gvili, Szymon Rusinkiewicz and Maks Ovsjanikov

Structured Light II. Thanks to Ronen Gvili, Szymon Rusinkiewicz and Maks Ovsjanikov Structured Light II Johannes Köhler Johannes.koehler@dfki.de Thanks to Ronen Gvili, Szymon Rusinkiewicz and Maks Ovsjanikov Introduction Previous lecture: Structured Light I Active Scanning Camera/emitter

More information

BME I5000: Biomedical Imaging

BME I5000: Biomedical Imaging 1 Lucas Parra, CCNY BME I5000: Biomedical Imaging Lecture 4 Computed Tomography Lucas C. Parra, parra@ccny.cuny.edu some slides inspired by lecture notes of Andreas H. Hilscher at Columbia University.

More information

Joint CI-JAI advanced accelerator lecture series Imaging and detectors for medical physics Lecture 1: Medical imaging

Joint CI-JAI advanced accelerator lecture series Imaging and detectors for medical physics Lecture 1: Medical imaging Joint CI-JAI advanced accelerator lecture series Imaging and detectors for medical physics Lecture 1: Medical imaging Dr Barbara Camanzi barbara.camanzi@stfc.ac.uk Course layout Day AM 09.30 11.00 PM 15.30

More information

The Emory Reconstruction Toolbox Version 1.0

The Emory Reconstruction Toolbox Version 1.0 The Emory Reconstruction Toolbox Version 1.0 Operating Instructions Revision 02 (April, 2008) Operating Instructions The Emory Reconstruction Toolbox Application Copyrights, Trademarks, Restrictions

More information

Automated segmentation methods for liver analysis in oncology applications

Automated segmentation methods for liver analysis in oncology applications University of Szeged Department of Image Processing and Computer Graphics Automated segmentation methods for liver analysis in oncology applications Ph. D. Thesis László Ruskó Thesis Advisor Dr. Antal

More information

An Automated Image-based Method for Multi-Leaf Collimator Positioning Verification in Intensity Modulated Radiation Therapy

An Automated Image-based Method for Multi-Leaf Collimator Positioning Verification in Intensity Modulated Radiation Therapy An Automated Image-based Method for Multi-Leaf Collimator Positioning Verification in Intensity Modulated Radiation Therapy Chenyang Xu 1, Siemens Corporate Research, Inc., Princeton, NJ, USA Xiaolei Huang,

More information

CT Basics Principles of Spiral CT Dose. Always Thinking Ahead.

CT Basics Principles of Spiral CT Dose. Always Thinking Ahead. 1 CT Basics Principles of Spiral CT Dose 2 Who invented CT? 1963 - Alan Cormack developed a mathematical method of reconstructing images from x-ray projections Sir Godfrey Hounsfield worked for the Central

More information

SISCOM (Subtraction Ictal SPECT CO-registered to MRI)

SISCOM (Subtraction Ictal SPECT CO-registered to MRI) SISCOM (Subtraction Ictal SPECT CO-registered to MRI) Introduction A method for advanced imaging of epilepsy patients has been developed with Analyze at the Mayo Foundation which uses a combination of

More information

Three Dimensional Dosimetry Analyses In Radionuclide Therapy Using IDL And MCNP-based Software Tools

Three Dimensional Dosimetry Analyses In Radionuclide Therapy Using IDL And MCNP-based Software Tools Three Dimensional Dosimetry Analyses In Radionuclide Therapy Using IDL And MCNP-based Software Tools M. G. Stabin 1, H. Yoriyaz 2, R. Li 1, A. B. Brill 1 1 Vanderbilt University, Nashville, TN, USA 2 Instituto

More information

8/3/2017. Contour Assessment for Quality Assurance and Data Mining. Objective. Outline. Tom Purdie, PhD, MCCPM

8/3/2017. Contour Assessment for Quality Assurance and Data Mining. Objective. Outline. Tom Purdie, PhD, MCCPM Contour Assessment for Quality Assurance and Data Mining Tom Purdie, PhD, MCCPM Objective Understand the state-of-the-art in contour assessment for quality assurance including data mining-based techniques

More information

Q.Clear. Steve Ross, Ph.D.

Q.Clear. Steve Ross, Ph.D. Steve Ross, Ph.D. Accurate quantitation (SUV - Standardized Uptake Value) is becoming more important as clinicians seek to utilize PET imaging for more than just diagnosing and staging disease, but also

More information

Is deformable image registration a solved problem?

Is deformable image registration a solved problem? Is deformable image registration a solved problem? Marcel van Herk On behalf of the imaging group of the RT department of NKI/AVL Amsterdam, the Netherlands DIR 1 Image registration Find translation.deformation

More information

TomoTherapy Related Projects. An image guidance alternative on Tomo Low dose MVCT reconstruction Patient Quality Assurance using Sinogram

TomoTherapy Related Projects. An image guidance alternative on Tomo Low dose MVCT reconstruction Patient Quality Assurance using Sinogram TomoTherapy Related Projects An image guidance alternative on Tomo Low dose MVCT reconstruction Patient Quality Assurance using Sinogram Development of A Novel Image Guidance Alternative for Patient Localization

More information

CT Protocol Review: Practical Tips for the Imaging Physicist Physicist

CT Protocol Review: Practical Tips for the Imaging Physicist Physicist CT Protocol Review: Practical Tips for the Imaging Physicist Physicist Dianna Cody, Ph.D., DABR, FAAPM U.T.M.D. Anderson Cancer Center August 8, 2013 AAPM Annual Meeting Goals Understand purpose and importance

More information

Basics of treatment planning II

Basics of treatment planning II Basics of treatment planning II Sastry Vedam PhD DABR Introduction to Medical Physics III: Therapy Spring 2015 Dose calculation algorithms! Correction based! Model based 1 Dose calculation algorithms!

More information

Hybrid Imaging for Patient-Specific Dosimetry in Radionuclide Therapy

Hybrid Imaging for Patient-Specific Dosimetry in Radionuclide Therapy Hybrid Imaging for Patient-Specific Dosimetry in Radionuclide Therapy Ljungberg, Michael; Sjögreen Gleisner, Katarina Published in: Diagnostics DOI: 10.3390/diagnostics5030296 Published: 2015-01-01 Link

More information

Estimating 3D Respiratory Motion from Orbiting Views

Estimating 3D Respiratory Motion from Orbiting Views Estimating 3D Respiratory Motion from Orbiting Views Rongping Zeng, Jeffrey A. Fessler, James M. Balter The University of Michigan Oct. 2005 Funding provided by NIH Grant P01 CA59827 Motivation Free-breathing

More information

Workshop on Quantitative SPECT and PET Brain Studies January, 2013 PUCRS, Porto Alegre, Brasil Corrections in SPECT and PET

Workshop on Quantitative SPECT and PET Brain Studies January, 2013 PUCRS, Porto Alegre, Brasil Corrections in SPECT and PET Workshop on Quantitative SPECT and PET Brain Studies 14-16 January, 2013 PUCRS, Porto Alegre, Brasil Corrections in SPECT and PET Físico João Alfredo Borges, Me. Corrections in SPECT and PET SPECT and

More information

A Study of Medical Image Analysis System

A Study of Medical Image Analysis System Indian Journal of Science and Technology, Vol 8(25), DOI: 10.17485/ijst/2015/v8i25/80492, October 2015 ISSN (Print) : 0974-6846 ISSN (Online) : 0974-5645 A Study of Medical Image Analysis System Kim Tae-Eun

More information

College of the Holy Cross. A Topological Analysis of Targeted In-111 Uptake in SPECT Images of Murine Tumors

College of the Holy Cross. A Topological Analysis of Targeted In-111 Uptake in SPECT Images of Murine Tumors College of the Holy Cross Department of Mathematics and Computer Science A Topological Analysis of Targeted In- Uptake in SPECT Images of Murine Tumors Author: Melissa R. McGuirl Advisor: David B. Damiano

More information

Corso di laurea in Fisica A.A Fisica Medica 4 TC

Corso di laurea in Fisica A.A Fisica Medica 4 TC Corso di laurea in Fisica A.A. 2007-2008 Fisica Medica 4 TC Computed Tomography Principles 1. Projection measurement 2. Scanner systems 3. Scanning modes Basic Tomographic Principle The internal structure

More information

Slide 1. Technical Aspects of Quality Control in Magnetic Resonance Imaging. Slide 2. Annual Compliance Testing. of MRI Systems.

Slide 1. Technical Aspects of Quality Control in Magnetic Resonance Imaging. Slide 2. Annual Compliance Testing. of MRI Systems. Slide 1 Technical Aspects of Quality Control in Magnetic Resonance Imaging Slide 2 Compliance Testing of MRI Systems, Ph.D. Department of Radiology Henry Ford Hospital, Detroit, MI Slide 3 Compliance Testing

More information

ANALYSIS OF CT AND PET/SPECT IMAGES FOR DOSIMETRY CALCULATION

ANALYSIS OF CT AND PET/SPECT IMAGES FOR DOSIMETRY CALCULATION 2009 International Nuclear Atlantic Conference - INAC 2009 Rio de Janeiro,RJ, Brazil, September27 to October 2, 2009 ASSOCIAÇÃO BRASILEIRA DE ENERGIA NUCLEAR - ABEN ISBN: 978-85-99141-03-8 ANALYSIS OF

More information

Gradient-Based Differential Approach for Patient Motion Compensation in 2D/3D Overlay

Gradient-Based Differential Approach for Patient Motion Compensation in 2D/3D Overlay Gradient-Based Differential Approach for Patient Motion Compensation in 2D/3D Overlay Jian Wang, Anja Borsdorf, Benno Heigl, Thomas Köhler, Joachim Hornegger Pattern Recognition Lab, Friedrich-Alexander-University

More information

Introduction to Medical Image Processing

Introduction to Medical Image Processing Introduction to Medical Image Processing Δ Essential environments of a medical imaging system Subject Image Analysis Energy Imaging System Images Image Processing Feature Images Image processing may be

More information

1. Deployment of a framework for drawing a correspondence between simple figure of merits (FOM) and quantitative imaging performance in CT.

1. Deployment of a framework for drawing a correspondence between simple figure of merits (FOM) and quantitative imaging performance in CT. Progress report: Development of assessment and predictive metrics for quantitative imaging in chest CT Subaward No: HHSN6801000050C (4a) PI: Ehsan Samei Reporting Period: month 1-18 Deliverables: 1. Deployment

More information

Overview of Proposed TG-132 Recommendations

Overview of Proposed TG-132 Recommendations Overview of Proposed TG-132 Recommendations Kristy K Brock, Ph.D., DABR Associate Professor Department of Radiation Oncology, University of Michigan Chair, AAPM TG 132: Image Registration and Fusion Conflict

More information

CT NOISE POWER SPECTRUM FOR FILTERED BACKPROJECTION AND ITERATIVE RECONSTRUCTION

CT NOISE POWER SPECTRUM FOR FILTERED BACKPROJECTION AND ITERATIVE RECONSTRUCTION CT NOISE POWER SPECTRUM FOR FILTERED BACKPROJECTION AND ITERATIVE RECONSTRUCTION Frank Dong, PhD, DABR Diagnostic Physicist, Imaging Institute Cleveland Clinic Foundation and Associate Professor of Radiology

More information

Determination of Three-Dimensional Voxel Sensitivity for Two- and Three-Headed Coincidence Imaging

Determination of Three-Dimensional Voxel Sensitivity for Two- and Three-Headed Coincidence Imaging IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 50, NO. 3, JUNE 2003 405 Determination of Three-Dimensional Voxel Sensitivity for Two- and Three-Headed Coincidence Imaging Edward J. Soares, Kevin W. Germino,

More information

Implementation of Advanced Image Guided Radiation Therapy

Implementation of Advanced Image Guided Radiation Therapy Image Acquisition Course Outline Principles, characteristics& applications of the available modalities Image Processing in the T x room Image guided treatment delivery What can / can t we do in the room

More information

LOGIQ. V2 Ultrasound. Part of LOGIQ Vision Series. Imagination at work LOGIQ is a trademark of General Electric Company.

LOGIQ. V2 Ultrasound. Part of LOGIQ Vision Series. Imagination at work LOGIQ is a trademark of General Electric Company. TM LOGIQ V2 Ultrasound Part of LOGIQ Vision Series Imagination at work The brilliance of color. The simplicity of GE. Now you can add the advanced capabilities of color Doppler to patient care with the

More information

3D Computer Vision. Structured Light II. Prof. Didier Stricker. Kaiserlautern University.

3D Computer Vision. Structured Light II. Prof. Didier Stricker. Kaiserlautern University. 3D Computer Vision Structured Light II Prof. Didier Stricker Kaiserlautern University http://ags.cs.uni-kl.de/ DFKI Deutsches Forschungszentrum für Künstliche Intelligenz http://av.dfki.de 1 Introduction

More information

Shadow casting. What is the problem? Cone Beam Computed Tomography THE OBJECTIVES OF DIAGNOSTIC IMAGING IDEAL DIAGNOSTIC IMAGING STUDY LIMITATIONS

Shadow casting. What is the problem? Cone Beam Computed Tomography THE OBJECTIVES OF DIAGNOSTIC IMAGING IDEAL DIAGNOSTIC IMAGING STUDY LIMITATIONS Cone Beam Computed Tomography THE OBJECTIVES OF DIAGNOSTIC IMAGING Reveal pathology Reveal the anatomic truth Steven R. Singer, DDS srs2@columbia.edu IDEAL DIAGNOSTIC IMAGING STUDY Provides desired diagnostic

More information

GPU applications in Cancer Radiation Therapy at UCSD. Steve Jiang, UCSD Radiation Oncology Amit Majumdar, SDSC Dongju (DJ) Choi, SDSC

GPU applications in Cancer Radiation Therapy at UCSD. Steve Jiang, UCSD Radiation Oncology Amit Majumdar, SDSC Dongju (DJ) Choi, SDSC GPU applications in Cancer Radiation Therapy at UCSD Steve Jiang, UCSD Radiation Oncology Amit Majumdar, SDSC Dongju (DJ) Choi, SDSC Conventional Radiotherapy SIMULATION: Construciton, Dij Days PLANNING:

More information

664 IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 52, NO. 3, JUNE 2005

664 IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 52, NO. 3, JUNE 2005 664 IEEE TRANSACTIONS ON NUCLEAR SCIENCE, VOL. 52, NO. 3, JUNE 2005 Attenuation Correction for the NIH ATLAS Small Animal PET Scanner Rutao Yao, Member, IEEE, Jürgen Seidel, Jeih-San Liow, Member, IEEE,

More information

A closer look at CT scanning

A closer look at CT scanning Vet Times The website for the veterinary profession https://www.vettimes.co.uk A closer look at CT scanning Author : Charissa Lee, Natalie Webster Categories : General, Vets Date : April 3, 2017 A basic

More information

Constructing System Matrices for SPECT Simulations and Reconstructions

Constructing System Matrices for SPECT Simulations and Reconstructions Constructing System Matrices for SPECT Simulations and Reconstructions Nirantha Balagopal April 28th, 2017 M.S. Report The University of Arizona College of Optical Sciences 1 Acknowledgement I would like

More information

PMOD Features dedicated to Oncology Research

PMOD Features dedicated to Oncology Research While brain research using dynamic data has always been a main target of PMOD s developments, many scientists working with static oncology data have also found ways to leverage PMOD s unique functionality.

More information

Integrated proton-photon treatment planning

Integrated proton-photon treatment planning Pinnacle 3 Proton Planning Integrated proton-photon treatment planning Philips Pinnacle 3 Proton Planning specifications Pinnacle 3 Proton Planning is designed to simplify treatment planning for proton

More information

UNIVERSITY OF SOUTHAMPTON

UNIVERSITY OF SOUTHAMPTON UNIVERSITY OF SOUTHAMPTON PHYS2007W1 SEMESTER 2 EXAMINATION 2014-2015 MEDICAL PHYSICS Duration: 120 MINS (2 hours) This paper contains 10 questions. Answer all questions in Section A and only two questions

More information

Super-resolution Reconstruction of Fetal Brain MRI

Super-resolution Reconstruction of Fetal Brain MRI Super-resolution Reconstruction of Fetal Brain MRI Ali Gholipour and Simon K. Warfield Computational Radiology Laboratory Children s Hospital Boston, Harvard Medical School Worshop on Image Analysis for

More information

Introduction to Positron Emission Tomography

Introduction to Positron Emission Tomography Planar and SPECT Cameras Summary Introduction to Positron Emission Tomography, Ph.D. Nuclear Medicine Basic Science Lectures srbowen@uw.edu System components: Collimator Detector Electronics Collimator

More information

Learn Image Segmentation Basics with Hands-on Introduction to ITK-SNAP. RSNA 2016 Courses RCB22 and RCB54

Learn Image Segmentation Basics with Hands-on Introduction to ITK-SNAP. RSNA 2016 Courses RCB22 and RCB54 Learn Image Segmentation Basics with Hands-on Introduction to ITK-SNAP RSNA 2016 Courses RCB22 and RCB54 RCB22 Mon, Nov 28 10:30-12:00 PM, Room S401CD RCB54 Thu, Dec 1 2:30-4:30 PM, Room S401CD Presenters:

More information

AAPM Standard of Practice: CT Protocol Review Physicist

AAPM Standard of Practice: CT Protocol Review Physicist AAPM Standard of Practice: CT Protocol Review Physicist Dianna Cody, Ph.D., DABR, FAAPM U.T.M.D. Anderson Cancer Center September 11, 2014 2014 Texas Radiation Regulatory Conference Goals Understand purpose

More information

Introduction to Emission Tomography

Introduction to Emission Tomography Introduction to Emission Tomography Gamma Camera Planar Imaging Robert Miyaoka, PhD University of Washington Department of Radiology rmiyaoka@u.washington.edu Gamma Camera: - collimator - detector (crystal

More information

Automated Image Analysis Software for Quality Assurance of a Radiotherapy CT Simulator

Automated Image Analysis Software for Quality Assurance of a Radiotherapy CT Simulator Automated Image Analysis Software for Quality Assurance of a Radiotherapy CT Simulator Andrew J Reilly Imaging Physicist Oncology Physics Edinburgh Cancer Centre Western General Hospital EDINBURGH EH4

More information

Motion artifact detection in four-dimensional computed tomography images

Motion artifact detection in four-dimensional computed tomography images Motion artifact detection in four-dimensional computed tomography images G Bouilhol 1,, M Ayadi, R Pinho, S Rit 1, and D Sarrut 1, 1 University of Lyon, CREATIS; CNRS UMR 5; Inserm U144; INSA-Lyon; University

More information

Digital Image Processing

Digital Image Processing Digital Image Processing SPECIAL TOPICS CT IMAGES Hamid R. Rabiee Fall 2015 What is an image? 2 Are images only about visual concepts? We ve already seen that there are other kinds of image. In this lecture

More information

The Near Future in Cardiac CT Image Reconstruction

The Near Future in Cardiac CT Image Reconstruction SCCT 2010 The Near Future in Cardiac CT Image Reconstruction Marc Kachelrieß Institute of Medical Physics (IMP) Friedrich-Alexander Alexander-University Erlangen-Nürnberg rnberg www.imp.uni-erlangen.de

More information

Fundamentals of CT imaging

Fundamentals of CT imaging SECTION 1 Fundamentals of CT imaging I History In the early 1970s Sir Godfrey Hounsfield s research produced the first clinically useful CT scans. Original scanners took approximately 6 minutes to perform

More information

RADIOMICS: potential role in the clinics and challenges

RADIOMICS: potential role in the clinics and challenges 27 giugno 2018 Dipartimento di Fisica Università degli Studi di Milano RADIOMICS: potential role in the clinics and challenges Dr. Francesca Botta Medical Physicist Istituto Europeo di Oncologia (Milano)

More information

Intraoperative Prostate Tracking with Slice-to-Volume Registration in MR

Intraoperative Prostate Tracking with Slice-to-Volume Registration in MR Intraoperative Prostate Tracking with Slice-to-Volume Registration in MR Sean Gill a, Purang Abolmaesumi a,b, Siddharth Vikal a, Parvin Mousavi a and Gabor Fichtinger a,b,* (a) School of Computing, Queen

More information

ADVANCING CANCER TREATMENT

ADVANCING CANCER TREATMENT 3 ADVANCING CANCER TREATMENT SUPPORTING CLINICS WORLDWIDE RaySearch is advancing cancer treatment through pioneering software. We believe software has un limited potential, and that it is now the driving

More information

Basic Radiation Oncology Physics

Basic Radiation Oncology Physics Basic Radiation Oncology Physics T. Ganesh, Ph.D., DABR Chief Medical Physicist Fortis Memorial Research Institute Gurgaon Acknowledgment: I gratefully acknowledge the IAEA resources of teaching slides

More information

VALIDATION OF DIR. Raj Varadhan, PhD, DABMP Minneapolis Radiation Oncology

VALIDATION OF DIR. Raj Varadhan, PhD, DABMP Minneapolis Radiation Oncology VALIDATION OF DIR Raj Varadhan, PhD, DABMP Minneapolis Radiation Oncology Overview Basics: Registration Framework, Theory Discuss Validation techniques Using Synthetic CT data & Phantoms What metrics to

More information

Auto-Segmentation Using Deformable Image Registration. Disclosure. Objectives 8/4/2011

Auto-Segmentation Using Deformable Image Registration. Disclosure. Objectives 8/4/2011 Auto-Segmentation Using Deformable Image Registration Lei Dong, Ph.D. Dept. of Radiation Physics University of Texas MD Anderson Cancer Center, Houston, Texas AAPM Therapy Educational Course Aug. 4th 2011

More information