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Dive into the research topics where Edward C. Pennington is active.

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Featured researches published by Edward C. Pennington.


International Journal of Radiation Oncology Biology Physics | 1990

Analysis of movement of intrathoracic neoplasms using ultrafast computerized tomography

Cynthia S. Ross; David H. Hussey; Edward C. Pennington; William Stanford; J. Fred Doornbos

Twenty patients with intrathoracic neoplasms were evaluated with ultrafast (cine) computerized tomography to determine the contribution of tumor motion to geographic errors. The treatment portals were setup with conventional simulation techniques and then scanned with cine computerized tomography. Eight tomographic levels were studied, 10 images per level over 7 seconds time. Major geographic misses were detected in three patients (15%), and minor geographic misses in an additional three (15%). The greatest tumor movement was noted in lesions located adjacent to the heart or aorta or near the diaphragm. Five of six hilar lesions showed significant lateral motion (average = 9.2 mm) with cardiac contraction, and three of four lower lobe lesions showed significant craniocaudal movement with respiration. Mediastinal lesions moved an average of 8.7 mm laterally. Lesions in the upper lobes showed minimal movement (average = 2.2 mm), and tumors attached to the chest wall showed no measurable movement.


International Journal of Radiation Oncology Biology Physics | 2001

Initial clinical experience with frameless stereotactic radiosurgery: Analysis of accuracy and feasibility

Timothy C. Ryken; Sanford L. Meeks; Edward C. Pennington; Patrick W. Hitchon; Vincent C. Traynelis; Nina A. Mayr; Frank J. Bova; William A. Friedman; John M. Buatti

PURPOSE To report on preliminary clinical experience with a novel image-guided frameless stereotactic radiosurgery system. METHODS AND MATERIALS Fifteen patients ranging in age from 14 to 81 received radiosurgery using a commercially available frameless stereotactic radiosurgery system. Pathologic diagnoses included metastases (12), recurrent primary intracranial sarcoma (1), recurrent central nervous system (CNS) lymphoma (1), and medulloblastoma with supratentorial seeding (1). Treatment accuracy was assessed from image localization of the stereotactic reference array and reproducibility of biteplate reseating. We chose 0.3 mm vector translation error and 0.3 degree rotation about each axis as the maximum tolerated misalignment before treating each arc. RESULTS The biteplates were found on average to reseat with a reproducibility of 0.24 mm. The mean registration error from CT localization was found to be 0.5 mm, which predicts that the average error at isocenter was 0.82 mm. No patient treatment was delivered beyond the maximum tolerated misalignment. The radiosurgery treatment was delivered in approximately 25 min per patient. CONCLUSION Our initial clinical experience with stereotactic radiotherapy using the infrared camera guidance system was promising, demonstrating clinical feasibility and accuracy comparable to many frame-based systems.


International Journal of Radiation Oncology Biology Physics | 2003

Ultrasound-guided extracranial radiosurgery: technique and application.

Sanford L. Meeks; John M. Buatti; Lionel G. Bouchet; Francis J. Bova; Timothy C. Ryken; Edward C. Pennington; Kathleen M Anderson; William A. Friedman

PURPOSE Stereotactic radiosurgery is an effective treatment modality for many intracranial lesions, but target mobility limits its utility for extracranial applications. We have developed a new technique for extracranial radiosurgery based on optically guided three-dimensional ultrasound (3DUS). The 3DUS system provides the ability to image the target volume and critical structures in real time and determine any misregistration of the target volume with the linear accelerator. In this paper, we describe the system and its initial clinical application in the treatment of localized metastatic disease. METHODS AND MATERIALS The extracranial stereotactic system consists of an ultrasound unit that is optically tracked and registered with the linear accelerator coordinate system. After an initial patient positioning based on computed tomographic (CT) simulation, stereotactic ultrasound images are acquired and correlated with the CT-based treatment plan to determine any soft-tissue shifts between the time of the planning CT and the actual treatment. Optical tracking is used to correct any patient offsets that are revealed by the real-time imaging. RESULTS Preclinical testing revealed that the ultrasound-based stereotactic navigation system is accurate to within 1.5 mm in comparison with an absolute coordinate phantom. Between March 2001 and March 2002, the system was used to deliver extracranial radiosurgery to 17 metastatic lesions in 16 patients. Treatments were delivered in 1 or 2 fractions, with an average fractional dose of 16 Gy (range 12.5-24 Gy) delivered to the 80% isodose surface. Before each fraction, the target misalignment from isocenter was determined using the 3DUS system and the misalignments averaged over all patients were anteroposterior = 4.8 mm, lateral = 3.6 mm, axial = 2.1 mm, and average total 3D displacement = 7.4 mm (range = 0-21.0 mm). After correcting patient misalignment, each plan was delivered as planned using 6-11 noncoplanar fields. No acute complications were reported. CONCLUSIONS A system for high-precision radiosurgical treatment of metastatic tumors has been developed, tested, and applied clinically. Optical tracking of the ultrasound probe provides real-time tracking of the patient anatomy and allows computation of the target displacement before treatment delivery. The patient treatments reported here suggest the feasibility and safety of the technique.


Journal of Applied Clinical Medical Physics | 2009

Radiation therapy plan checks in a paperless clinic

Ramon Alfredo Carvalho Siochi; Edward C. Pennington; Timothy J. Waldron; John E. Bayouth

Traditional quality assurance checks of a patients radiation therapy plan involve printing out treatment parameters from the treatment planning system and the “record and verify” (R&V) system and visually checking the information for one‐to‐one correspondence. In a paperless environment, one can automate this process through independent software that can read the treatment planning data directly and compare it against the parameters in the R&V systems database. In addition to verifying the data integrity, it is necessary to check the logical consistency of the data and the accuracy of various calculations. The results are then imported into the patients electronic medical record. Appropriate workflows must be developed to ensure that no steps of the QA process are missed. This paper describes our electronic QA system (EQS), consisting of in‐house software and workflows. The EQS covers 3D conformal and intensity modulated radiation therapy, electrons, stereotactic radiosurgery, total body irradiation, and clinical set ups with and without virtual simulation. The planning systems handled by our EQS are ADAC Pinnacle and Varian FASTPLAN, while the R&V systems are LANTIS and VARIS. The improvement in our plan check process over the paperless system is described in terms of the types of detected errors. The potential problems with the implementation and use of the EQS, as well as workarounds for data that are not easily accessible through electronic means, are described. PACS numbers: 87.55.Qr, 87.55.tg, 87.55.tm


Radiotherapy and Oncology | 2002

In vivo determination of extra-target doses received from serial tomotherapy

Sanford L. Meeks; Arnold C. Paulino; Edward C. Pennington; James H. Simon; Mark Skwarchuk; John M. Buatti

BACKGROUND AND PURPOSE The purpose of this study was to perform in-vivo measurements of extracranial doses received by patients undergoing serial tomotherapy of the head and neck. MATERIAL AND METHODS Intensity modulated radiotherapy treatment (IMRT) plans were designed for nine patients using the CORVUS treatment planning system (NOMOS Corp.). These plans were delivered using a tertiary collimator dedicated for serial tomotherapy attached to a 10-MV linear accelerator. For each patient, one optically stimulated luminescence dosimeter (OSLD) was placed on the sternum and one on the lower abdomen. The OSLDs were then processed, thereby estimating the in vivo absorbed doses to the sternum and gonads as a function of distance from the treatment site. RESULTS The OSLDs were shown to measure known doses to within 5%, thereby validating their accuracy for this dose and energy range. In the patient studies, the dose received by the OSLDs varied in direct proportion to the number of monitor units delivered and inversely with the distance from the target volume; the patient dose at a distance of 15 cm from the target is approximately 0.4% of the total monitor units delivered, and drops to below 0.1% of the total MUs at approximately 40 cm from the center of the target. The average sternal dose was 1353 mSv and the average abdominal dose was 327 mSv for an average prescribed dose of 60.1 Gy. This can be attributed, at least partially, to the inefficient treatment delivery that on average required 9.9 MU/0.01 Gy. CONCLUSIONS While IMRT reduces the normal tissue volume in the high-dose region, it also increases the overall monitor units delivered, and hence the whole-body dose, when compared with conventional treatment delivery. As has been noted in existing literature, these increases in whole-body dose from radiotherapy delivery may increase the likelihood of a radiation-induced secondary malignancy. Therefore, it is important to assess the risk of secondary malignancies from IMRT delivery, and compare this relative risk against the potential benefits of decreased normal tissue complication probabilities.


Medical Physics | 2009

Dosimetric characterization and application of an imaging beam line with a carbon electron target for megavoltage cone beam computed tomography.

R Flynn; Julia Hartmann; Ali Bani-Hashemi; Earl Nixon; R. Alfredo; C. Siochi; Edward C. Pennington; John E. Bayouth

Imaging dose from megavoltage cone beam computed tomography (MVCBCT) can be significantly reduced without loss of image quality by using an imaging beam line (IBL), with no flattening filter and a carbon, rather than tungsten, electron target. The IBL produces a greater keV-range x-ray fluence than the treatment beam line (TBL), which results in a more optimal detector response. The IBL imaging dose is not necessarily negligible, however. In this work an IBL was dosimetrically modeled with the Philips Pinnacle3 treatment planning system (TPS), verified experimentally, and applied to clinical cases. The IBL acquisition dose for a 200 degrees gantry rotation was verified in a customized acrylic cylindrical phantom at multiple imaging field sizes with 196 ion chamber measurements. Agreement between the measured and calculated IBL dose was quantified with the 3D gamma index. Representative IBL and TBL imaging dose distributions were calculated for head and neck and prostate patients and included in treatment plans using the imaging dose incorporation (IDI) method. Surface dose was measured for the TBL and IBL for four head and neck cancer patients with MOSFETs. The IBL model, when compared to the percentage depth dose and profile measurements, had 97% passing gamma indices for dosimetric and distance acceptance criteria of 3%, 3 mm, and 100% passed for 5.2%, 5.2 mm. For the ion chamber measurements of phantom image acquisition dose, the IBL model had 93% passing gamma indices for acceptance criteria of 3%, 3 mm, and 100% passed for 4%, 4 mm. Differences between the IBL- and TBL-based IMRT treatment plans created with the IDI method were dosimetrically insignificant for both the prostate and head and neck cases. For IBL and TBL beams with monitor unit values that would result in the delivery of the same dose to the depth of maximum dose under standard calibration conditions, the IBL imaging surface dose was higher than the TBL imaging surface dose by an average of 18%, with a standard deviation of 8% (p = 2 x 10(-6)). The IBL can be modeled with acceptable accuracy using a standard TPS, and accounting for IBL dose in treatment plans with the IDI method is straightforward. The resulting composite dose distributions, assuming similar imaging doses, are negligibly different from those of the TBL. The increased IBL surface dose relative to the TBL is likely clinically insignificant.


Medical Physics | 1988

Leakage radiation from electron applicators on a medical accelerator

Edward C. Pennington; Shirish K. Jani; B-Chen Wen

The leakage characteristics of electron applicators on our Clinac 2500 linear accelerator have been measured. The leakage radiation in the patient plane and at the surface of the electron applicators has been measured for applicator sizes from 6 cm×6 cm to 25 cm×25 cm and beam energies from 6 to 22 MeV. For certain applicator/energy combinations the leakage radiation was significant. The leakage radiation, relative to the central axis dose, was found to be up to 7% in the patient plane and up to 39% at the applicator surface. Reducing the collimator setting or adding lead at select locations on the applicator surface was effective in reducing the magnitude of the radiation leakage.


IEEE Transactions on Biomedical Engineering | 2003

Effects of vessel geometry and catheter position on dose delivery in intracoronary brachytherapy

Andreas Wahle; John J. Lopez; Edward C. Pennington; Sanford L. Meeks; Kathleen C. Braddy; James M. Fox; Theresa M. H. Brennan; John M. Buatti; James D. Rossen; Milan Sonka

In-stent restenosis is commonly observed in coronary arteries after intervention. Intravascular brachytherapy has been found effective in reducing the recurrence of restenosis after stent placement. Conventional dosing models for brachytherapy with beta (/spl beta/) radiation neglect vessel geometry as well as the position of the delivery catheter. This paper demonstrates in computer simulations on phantoms and on in vivo patient data that the estimated dose distribution varies substantially in curved vessels. In simulated phantoms of 50-mm length with a shape corresponding to a 60/spl deg/-180/spl deg/ segment of a respectively sized torus, the average dose in 2-mm depth was decreased by 2.70%-7.48% at the outer curvature and increased by 2.95%-9.70% at the inner curvature as compared with a straight phantom. In vivo data were represented in a geometrically correct three-dimensional model that was derived by fusion of intravascular ultrasound (IVUS) and biplane angiography. These data were compared with a simplified tubular model reflecting common assumptions of conventional dosing schemes. The simplified model yielded significantly lower estimates of the delivered radiation and the dose variability as compared with a geometrically correct model (p < 0.001). The estimated dose in ten vessel segments of eight patients was on average 8.76% lower at the lumen/plaque and 6.52% lower at the media/adventitia interfaces (simplified tubular model relative to geometrically correct model). The differences in dose estimates between the two models were significantly higher in the right coronary artery as compared with the left coronary artery (p < 0.001).


Medical Dosimetry | 1998

Dosimetric considerations of water-based bolus for irradiation of extremities

Cheng B. Saw; B-Chen Wen; Kathleen M. Anderson; Edward C. Pennington; David H. Hussey

The dosimetry of high-energy photon beams in the treatment of superficial lesions occurring in extremities was examined. Large parallel-opposed fields with different photon beam energies were used. The extremity was immersed in water contained in a commercially available plastic wastebasket. The water bolus serves to even out the surface irregularities of the extremities and to remove the skin sparing effect. A polystyrene block was placed at the floor of the wastebasket to ensure that the extremity was encompassed in the radiation fields. The photon beam energies considered were 4 MV, 6 MV, 10 MV, and 24 MV. The results show that the dose distributions are more homogeneous with higher photon beam energies. The isodose lines are more constricted at mid-plane for low energy photon beams. Higher energy photon beams, 10 MV and up would be preferable for the treatment of superficial lesions of the extremities immersed in water bolus contained in a typical wastebasket size.


Medical Physics | 1989

Dose anisotropy around an Au-198 seed source

Shirish Jani; Edward C. Pennington; Boyd M. Knosp

For interstitial implants with radioactive Au-198 seeds, the dosimetric calculations usually ignore the finite source size and employ a point source approximation, resulting in a computed isotropic dose distribution. However, the measured radiation fluence from Au-198 seeds is reported to be anisotropic, suggesting some amount of dose anisotropy in tissue. We have measured this dose anisotropy around Au-198 seeds (2.5 X 0.8 mm2) using Kodak X-OMAT XV-2 films placed in contact with individual seeds in a phantom. Autoradiographs obtained for various exposure times were digitized and studied with an image analysis computer network. The networks overall spatial resolution was about 0.01 cm. The optical isodensity contours around the seed were obtained. The useful range of optical density (OD) for the system was found to be 1 to 2 OD units. Within this range, the shape of an optical isodensity contour would be identical to an isodose contour. Proximal to the source, the contours were elliptical in shape, elongated along the seed axis. However, further away, the elongation was in the direction normal to the seed axis. This was in agreement with the reported data on the radiation fluence around Au-198 seeds. It was concluded that measurable dose anisotropy existed around Au-198 seeds. However, it was too small to be of any clinical significance.

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Sanford L. Meeks

University of Texas MD Anderson Cancer Center

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Shirish K. Jani

University of Iowa Hospitals and Clinics

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John E. Bayouth

University of Wisconsin-Madison

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Kathleen M. Anderson

University of Iowa Hospitals and Clinics

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Shirish Jani

Sharp Memorial Hospital

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