Willi A. Kalender

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Willi A. Kalender (born 1 August 1949) is a German medical physicist and professor and former chairman of the Institute of Medical Physics of the University of Erlangen-Nuremberg. [1] Kalender has produced several new technologies in the field of diagnostic radiology imaging.

Contents

Kalender is a Fellow of the American Association of Physicists in Medicine (AAPM) and Honorary Fellow of the British Institute of Radiology (BIR) and of the Institute of Physics and Engineering in Medicine (IPEM). Kalender was also elected a member of the National Academy of Engineering (2016) for the development of spiral computed tomography methods that enable modern high-speed 3D medical imaging with X-rays.

Education

Kalender started his studies in physics and mathematics at the University of Bonn, Germany. He completed his master's and Ph.D. degree in medical physics at the University of Wisconsin in 1974 and 1979, respectively. In 1988 he completed all postdoctoral lecturing qualifications (Habilitation) at the University of Tübingen, Germany. In order to get a better grasp of the subject, he took and successfully completed all courses in the pre-clinical medicine curriculum.

Career

From 1979 to 1995 Kalender worked in the research laboratories of Siemens Medical Systems in Erlangen, Germany; he was appointed head of the Medical Physics group in 1988. In 1995 he was appointed full professor and chairman of the newly established Institute of Medical Physics at the Friedrich-Alexander-University Erlangen-Nuremberg, Germany. In 1999 he became distinguished visiting professor to the Department of Radiology at Stanford University, Stanford, CA, US.

Research and Development Achievements

Kalender has conducted research mainly in the area of diagnostic radiology imaging with a clear focus on special CT applications. The goals of and motivation for his projects were mostly derived from observations during patient exams in clinical radiology.

Kalender was involved in the development of the world's first product options for dual-energy CT [1] in 1983 and for metal artifact reduction (MAR) in 1987. [2]

Kalender developed volumetric spiral computed tomography; the world's first clinical spiral CT studies were presented at RSNA 1989. [3] The combination of continuous data acquisition with slip-ring-based data transmission and continuous table translation led to considerable reduction of examination times, to an essential reduction of motion artifacts and image quality significantly improved by providing isotropic spatial resolution as a decisive feature.

Kalender developed angio-CT [4] and heart phase-specific cardiac imaging. [4]

Other highly important fields of W. Kalender's research have been radiation protection and the development of intelligent and very efficient dose reduction approaches such as tube current modulation [7] and the optimization of the choice of x-ray spectra. [5] They allow reducing the patient dose by an order of magnitude in many cases without impairing image quality.

2008-2019 Kalender's research was focused on the development of an efficient breast-CT system to improve the early detection of breast cancer. [6] The scanner and in particular the development of its high-resolution photon-counting detector design allow scanning the breast with a dose similar to that of digital mammography, but with much higher resolution and clarity than mammography due to superposition-free fully 3D-resolution of breast-CT. [7] The introduction into clinical practice was performed in 2018 at the University Spital Zurich (Swiss).

Kalender has founded several university spinoff companies to transfer scientific results into products and small business.

Selected Honours & Awards

Publications

Kalender has authored 963 publications, including 286 original scientific papers; his Hirsch-index is cited with a 69 (ISI-Web of Knowledge, 2018)

Related Research Articles

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A computed tomography scan is a medical imaging technique used to obtain detailed internal images of the body. The personnel that perform CT scans are called radiographers or radiology technologists.

<span class="mw-page-title-main">Radiography</span> Imaging technique using ionizing and non-ionizing radiation

Radiography is an imaging technique using X-rays, gamma rays, or similar ionizing radiation and non-ionizing radiation to view the internal form of an object. Applications of radiography include medical and industrial radiography. Similar techniques are used in airport security,. To create an image in conventional radiography, a beam of X-rays is produced by an X-ray generator and it is projected towards the object. A certain amount of the X-rays or other radiation are absorbed by the object, dependent on the object's density and structural composition. The X-rays that pass through the object are captured behind the object by a detector. The generation of flat two-dimensional images by this technique is called projectional radiography. In computed tomography, an X-ray source and its associated detectors rotate around the subject, which itself moves through the conical X-ray beam produced. Any given point within the subject is crossed from many directions by many different beams at different times. Information regarding the attenuation of these beams is collated and subjected to computation to generate two-dimensional images on three planes which can be further processed to produce a three-dimensional image.

<span class="mw-page-title-main">Radiology</span> Branch of Medicine

Radiology is the medical specialty that uses medical imaging to diagnose diseases and guide their treatment, within the bodies of humans and other animals. It began with radiography, but today it includes all imaging modalities, including those that use no electromagnetic radiation, as well as others that do, such as computed tomography (CT), fluoroscopy, and nuclear medicine including positron emission tomography (PET). Interventional radiology is the performance of usually minimally invasive medical procedures with the guidance of imaging technologies such as those mentioned above.

Medical physics deals with the application of the concepts and methods of physics to the prevention, diagnosis and treatment of human diseases with a specific goal of improving human health and well-being. Since 2008, medical physics has been included as a health profession according to International Standard Classification of Occupation of the International Labour Organization.

<span class="mw-page-title-main">Medical imaging</span> Technique and process of creating visual representations of the interior of a body

Medical imaging is the technique and process of imaging the interior of a body for clinical analysis and medical intervention, as well as visual representation of the function of some organs or tissues (physiology). Medical imaging seeks to reveal internal structures hidden by the skin and bones, as well as to diagnose and treat disease. Medical imaging also establishes a database of normal anatomy and physiology to make it possible to identify abnormalities. Although imaging of removed organs and tissues can be performed for medical reasons, such procedures are usually considered part of pathology instead of medical imaging.

<span class="mw-page-title-main">Nuclear medicine</span> Medical specialty

Nuclear medicine or nucleology is a medical specialty involving the application of radioactive substances in the diagnosis and treatment of disease. Nuclear imaging, in a sense, is "radiology done inside out" because it records radiation emitted from within the body rather than radiation that is transmitted through the body from external sources like X-ray generators. In addition, nuclear medicine scans differ from radiology, as the emphasis is not on imaging anatomy, but on the function. For such reason, it is called a physiological imaging modality. Single photon emission computed tomography (SPECT) and positron emission tomography (PET) scans are the two most common imaging modalities in nuclear medicine.

The Hounsfield scale, named after Sir Godfrey Hounsfield, is a quantitative scale for describing radiodensity. It is frequently used in CT scans, where its value is also termed CT number.

<span class="mw-page-title-main">CT pulmonary angiogram</span>

A CT pulmonary angiogram (CTPA) is a medical diagnostic test that employs computed tomography (CT) angiography to obtain an image of the pulmonary arteries. Its main use is to diagnose pulmonary embolism (PE). It is a preferred choice of imaging in the diagnosis of PE due to its minimally invasive nature for the patient, whose only requirement for the scan is an intravenous line.

Image-guided radiation therapy is the process of frequent imaging, during a course of radiation treatment, used to direct the treatment, position the patient, and compare to the pre-therapy imaging from the treatment plan. Immediately prior to, or during, a treatment fraction, the patient is localized in the treatment room in the same position as planned from the reference imaging dataset. An example of IGRT would include comparison of a cone beam computed tomography (CBCT) dataset, acquired on the treatment machine, with the computed tomography (CT) dataset from planning. IGRT would also include matching planar kilovoltage (kV) radiographs or megavoltage (MV) images with digital reconstructed radiographs (DRRs) from the planning CT.

<span class="mw-page-title-main">Tomosynthesis</span>

Tomosynthesis, also digital tomosynthesis (DTS), is a method for performing high-resolution limited-angle tomography at radiation dose levels comparable with projectional radiography. It has been studied for a variety of clinical applications, including vascular imaging, dental imaging, orthopedic imaging, mammographic imaging, musculoskeletal imaging, and chest imaging.

The computed tomography dose index (CTDI) is a commonly used radiation exposure index in X-ray computed tomography (CT), first defined in 1981. The unit of CTDI is the gray (Gy) and it can be used in conjunction with patient size to estimate the absorbed dose. The CTDI and absorbed dose may differ by more than a factor of two for small patients such as children.

<span class="mw-page-title-main">Flat-panel detector</span> Class of solid-state x-ray digital radiography devices

Flat-panel detectors are a class of solid-state x-ray digital radiography devices similar in principle to the image sensors used in digital photography and video. They are used in both projectional radiography and as an alternative to x-ray image intensifiers (IIs) in fluoroscopy equipment.

<span class="mw-page-title-main">PET-MRI</span>

Positron emission tomography–magnetic resonance imaging (PET–MRI) is a hybrid imaging technology that incorporates magnetic resonance imaging (MRI) soft tissue morphological imaging and positron emission tomography (PET) functional imaging.

<span class="mw-page-title-main">Cone beam computed tomography</span> Medical imaging technique

Cone beam computed tomography is a medical imaging technique consisting of X-ray computed tomography where the X-rays are divergent, forming a cone.

<span class="mw-page-title-main">Photon counting</span> Counting photons using a single-photon detector

Photon counting is a technique in which individual photons are counted using a single-photon detector (SPD). A single-photon detector emits a pulse of signal for each detected photon. The counting efficiency is determined by the quantum efficiency and the system's electronic losses.

Proton computed tomography (pCT), or proton CT, is an imaging modality first proposed by Cormack in 1963 and initial experiment explorations identified several advantages over conventional X-ray CT (xCT). However, particle interactions such as multiple Coulomb scattering (MCS) and (in)elastic nuclear scattering events deflect the proton trajectory, resulting in nonlinear paths which can only be approximated via statistical assumptions, leading to lower spatial resolution than X-ray tomography. Further experiments were largely abandoned until the advent of proton radiation therapy in the 1990s which renewed interest in the topic due to the potential benefits of imaging and treating patients with the same particle.

<span class="mw-page-title-main">Operation of computed tomography</span>

X-ray computed tomography operates by using an X-ray generator that rotates around the object; X-ray detectors are positioned on the opposite side of the circle from the X-ray source.

Jeffrey Harold Siewerdsen is an American physicist and biomedical engineer who is a Professor of Imaging Physics at The University of Texas MD Anderson Cancer Center as well as Biomedical Engineering, Computer Science, Radiology, and Neurosurgery at Johns Hopkins University.He is among the original inventors of cone-beam CT-guided radiotherapy as well as weight-bearing cone-beam CT for musculoskeletal radiology and orthopedic surgery. His work also includes the early development of flat-panel detectors on mobile C-arms for intraoperative cone-beam CT in image-guided surgery. He developed early models for the signal and noise performance of flat-panel detectors and later extended such analysis to dual-energy imaging and 3D imaging performance in cone-beam CT. He founded the ISTAR Lab in the Department of Biomedical Engineering, the Carnegie Center for Surgical Innovation at Johns Hopkins Hospital, and the Surgical Data Science Program at the Institute for Data Science in Oncology at The University of Texas MD Anderson Cancer Center.

Photon-counting computed tomography (PCCT) is a form of X-ray computed tomography (CT) in which X-rays are detected using a photon-counting detector (PCD) which registers the interactions of individual photons. By keeping track of the deposited energy in each interaction, the detector pixels of a PCD each record an approximate energy spectrum, making it a spectral or energy-resolved CT technique. In contrast, more conventional CT scanners use energy-integrating detectors (EIDs), where the total energy deposited in a pixel during a fixed period of time is registered. These EIDs thus register only photon intensity, comparable to black-and-white photography, whereas PCDs register also spectral information, similar to color photography.

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References

  1. Franzeurl, Kristian. "Institute of Medical Physics, Erlangen". www.imp.uni-erlangen.de. Retrieved 2017-08-11.
  2. Kalender, W.A.; Hebel, R. (1986). "Fast routine for the reduction of artifacts caused by metallic implants in CT images". 161 (P). Radiological Society of North America Inc: 345.{{cite journal}}: Cite journal requires |journal= (help)
  3. Kalender, W A; Seissler, W; Klotz, E; Vock, P (July 1990). "Spiral volumetric CT with single-breath-hold technique, continuous transport, and continuous scanner rotation". Radiology. 176 (1): 181–183. doi:10.1148/radiology.176.1.2353088. ISSN   0033-8419.
  4. Kachelrieß, M; Kalender, WA (2000). "ECG-correlated image reconstruction from sub second multi-slice spiral CT scans of the heart". Med. Phys. 27 (8): 1881–1902.
  5. Kalender, Willi A.; Deak, Paul; Kellermeier, Markus; van Straten, Marcel; Vollmar, Sabrina V. (March 2009). "Application- and patient size-dependent optimization of x-ray spectra for CT". Medical Physics. 36 (3): 993–1007. doi:10.1118/1.3075901. ISSN   0094-2405.
  6. Kalender, Willi A.; Beister, Marcel; Boone, John M.; Kolditz, Daniel; Vollmar, Sabrina V.; Weigel, Michaela C. C. (1 January 2012). "High-resolution spiral CT of the breast at very low dose: concept and feasibility considerations". European Radiology. 22 (1): 1–8. doi:10.1007/s00330-011-2169-4. ISSN   1432-1084.
  7. Kalender, Willi A.; Kolditz, Daniel; Steiding, Christian; Ruth, Veikko; Lück, Ferdinand; Rößler, Ann-Christin; Wenkel, Evelyn (1 March 2017). "Technical feasibility proof for high-resolution low-dose photon-counting CT of the breast". European Radiology. 27 (3): 1081–1086. doi:10.1007/s00330-016-4459-3. ISSN   1432-1084.

[1] Kalender WA, Klotz E, Süß C. An integral approach to vertebral bone mineral analysis by X-ray computed tomography. Radiology 1987; 164:419-423

Further reading