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Biomedical subjects

M A Astrahan

Publications and source records attributed to M A Astrahan.

32 records · Page 2Linked to original sources
PubMedDate not supplied

Regional silver content of radiographic film determined by x-ray fluorescence compared with optical densitometry.

The regional silver content of radiographic film measured by x-ray fluorescence is compared to light absorption measured by a densitometer. Silver content analysis appears to permit a greater dynamic range of useful exposure levels than does light absorption densitometry. This improvement in latitude, however, is not considered great enough to warrant development of a complex system for scanning silver distribution in radiographic applications.

Densitometry↗
PubMedDate not supplied

Characteristics of the high-energy photon beam of a 25-MeV accelerator.

The CGR Saturne 25 is an isocentrically mounted standing wave medical linear accelerator that produces dual-energy photon beams and a scanned electron beam with six selectable energies between 4 and 25 MeV. The highest energy photon beam is nominally referred to as 23 MV. For this beam the mean energy of the accelerated electron beam on the 1.3 radiation length (4 mm) tungsten x-ray target is found to be approximately 21 MeV, with the energy acceptance stated to be +/- 5%. The electron beam traverses a 270 degrees bending magnet upstream of the x-ray production target. The resulting bremsstrahlung beam passes through a combination steel and lead flattening filter, 4-cm maximum thickness. Dosimetric data for the 23-MV beam are presented with respect to rectangular field output factor, depth of maximum dose as a function of field size, surface and buildup dose, central axis percent depth dose, tissue-phantom ratios, beam profile, applicability of inverse square, and block transmission. Some data are also presented on the effect of different flattening filter designs on apparent beam energy.

Electrons↗
PubMedDate not supplied

Backscatter measurements from a single seed of 125I for ophthalmic plaque dosimetry.

To determine the dosimetric effect of a gold plaque applicator used in 125I ophthalmic irradiation, relative dose rates at points 2-18 mm transverse to the axis of a single seed of 125I were measured in an acrylic phantom under three different measurement conditions. The detectors were 1-mm diameter X 3-mm length LiF thermoluminescent dosimeters (TLD's). Conditions corresponded to the following: (i) full scatter, (ii) the presence of an ophthalmic gold plaque, and (iii) no scatter material on the side of the seed opposite to the TLD's. The dose rate with the gold plaque is less than that with full scatter phantom. There is no significant decrease in dose rate at 2.2 mm from the seed. Dose rate is significantly reduced at greater distances. The does rate decrease ranges from 4% at 5 mm to 10% at 18 mm. The 125I seed in the gold plaque gives 3%-5% higher dose rate than in the absence of backscatter material.

Brachytherapy↗
PubMedDate not supplied

Output factor constituents of a high-energy photon beam.

Measurements designed to separate primary and various scatter components of central axis dose of the highest energy photon beam of the CGR Saturne 25 linear accelerator are described. This beam has an unusually large output variation with field size. The measurements are performed both in air and in a water phantom, with and without an aperture external to the collimator system. Results are presented in the form of relative output factors for different field sizes due to (i) flattening filter scatter, (ii) water phantom scatter, (iii) collimator backscatter into the monitor chamber, and (iv) collimator forward scatter onto the central axis. It is found that the flattening filter is the single largest scatter component, but that each of the other factors is significant in determining the output dose per monitor unit as a function of field size.

Humans↗
PubMedDate not supplied

Optimization of 125I ophthalmic plaque brachytherapy.

Episcleral plaques containing 125I sources are often used in the treatment of ocular melanoma. Within four years post-treatment, however, the majority of patients experience some visual loss due to radiation retinopathy. The high incidence of late complications suggests that careful treatment optimization may lead to improved outcome. The goal of optimization would be to reduce the magnitude of vision-limiting complications without compromising tumor control. We have developed a three-dimensional computer model for ophthalmic plaque therapy which permits us to explore the potential of various optimization strategies. One simple strategy which shows promise is to maximize the ratio of dose to the tumor apex (T) compared to dose to the macula (M). By modifying the parameters of source location, activity distribution, source orientation, and shielding we find that the calculated T:M ratio can be varied by a factor of 2 for a common plaque design and posterior tumor location. Margins and dose to the tumor volume remain essentially unchanged.

Biophysical Phenomena↗
PubMedDate not supplied

Algorithm for dosimetry of multiarc linear-accelerator stereotactic radiosurgery.

Treatment planning for multiarc radiosurgery is an inherently complex three-dimensional dosimetry problem. Characteristics of small-field x-ray beams suggest that major simplification of the dose computation algorithm is possible without significant loss of accuracy compared to calculations based on large-field algorithms. The simplification makes it practical to efficiently implement accurate multiplanar dosimetry calculations on a desktop computer. An algorithm is described that is based on data from fixed-beam tissue-maximum-ratio (TMR) and profile measurements at isocenter. The profile for each fixed beam is scaled geometrically according to distance from the x-ray source. Beam broadening due to scatter is taken into account by a simple formula that interpolates the full width at half maximum (FWHM) between profiles at isocenter at different depths in phantom. TMR and profile data for two representative small-field collimators (10- and 25-mm projected diameter) were obtained by TLD and film measurements in a phantom. The accuracy of the calculational method and the associated computer program were verified by TLD and film measurements of noncoplanar multiarc irradiations from these collimators on a 4-MV linear accelerator. Comparison of film measurements in two orthogonal planes showed close agreement with calculations in the shape of the dose distribution. Maximal separation of measured and calculated 90%, 80%, and 50% isodose curves was less than or equal to 0.5 mm for all planes and collimators. All TLD and film measurements of dose to isocenter agreed with calculations to within 2%.

Algorithms↗
PubMedDate not supplied

Tumor localization using fundus view photography for episcleral plaque therapy.

The accurate localization of ophthalmic tumors on the scleral surface is important when calculating radiation dose to the tumor and adjacent structures from episcleral I-125 plaques. This is particularly true for tumors close to the fovea or optic nerve. A fundus view diagram of the eye is often used by ophthalmologists to describe the size and shape of the tumor perimeter as well as its geographical location on the retinal surface. There is, however, an inherent inaccuracy associated with the use of a hand drawn diagram to obtain physical measurements. A computer planning program has been developed which uses CT and a digitized photographic montage of the posterior hemisphere to estimate the size and location of posteriorly located tumors. A simple phantom was constructed to test the software and a direct comparison made between planned versus measured tumor size and location in an excised eye.

Brachytherapy↗
PubMedDate not supplied

The accuracy of temperature measurement from within an interstitial microwave antenna.

Temperature measurement from within microwave interstitial antennas is a promising new development for hyperthermia. These antennas could enable the development of multipoint temperature regulation, leading to improved control of temperature distributions and therefore more effective hyperthermia treatments. In the complex environment of an antenna within a plastic catheter, measured temperatures were found to differ from the estimated local tissue temperature by up to 8 degrees C. In the design evaluated in this report the primary source of this error appears to be self-heating distal to the antenna junction, particularly in the outer copper conductor. The magnitude of self-heating is directly proportional to applied microwave power. Catheter wall thickness, tissue perfusion, and longitudinal temperature gradient also influence the measured temperature.

Humans↗
PubMedDate not supplied

A technique for combining microwave hyperthermia with intraluminal brachytherapy of the oesophagus.

A technique for combining microwave hyperthermia with 192Ir brachytherapy for the treatment of oesophageal carcinoma is described. This approach uses an intraluminal afterloading applicator and up to six microwave antennae to deliver both hyperthermia and brachytherapy, with minimal modification of the existing procedure for brachytherapy alone. Each microwave antenna includes a built-in thermistor to control temperature and balance power. Longitudinal temperature distributions were measured in situ from within the applicator, and at the applicator-tissue interface in vivo. Two-dimensional SAR and steady-state temperature distributions measured in muscle-equivalent phantom are presented and discussed. The technique appears to be capable of elevating tissue temperature to greater than 42 degrees C in a radially symmetric volume of length greater than 5 cm, with radial penetration of 0.5 cm. The clinical technique is relatively simple and well tolerated.

Brachytherapy↗
PubMedDate not supplied

Microwave applicator for transurethral hyperthermia of benign prostatic hyperplasia.

An applicator for heating the prostate gland using a transurethral approach is described. This technique uses three microwave antennas and a thermometry sensor attached to the outer surface of a balloon (Foley) type urological catheter. Each microwave antenna also includes a built-in thermistor to control temperature and balance power. The balloon catheter assures rapid and reproducible localization of the antennas in the prostatic urethra. The two-dimensional SAR and steady-state temperature distributions surrounding the applicator in tissue equivalent phantom are reported. Longitudinal temperature distributions measured in situ at the applicator-urethral interface and the longitudinal and radial temperature distributions measured in normal canine prostate are presented and discussed. The technique appears to be capable of elevating temperature to greater than 42 degrees C in a cylindrically symmetrical volume up to 5 cm length and 0.5 cm radial penetration surrounding the applicator.

Hot Temperature↗
PubMedDate not supplied

Adjuvant pelvic hyperthermia in advanced cervical carcinoma. I. Feasibility, thermometry and device comparison.

From 1981 to 1989, a total of 26 women with locally or regionally advanced carcinoma of the uterine cervix were treated with radiotherapy (RT) and pelvic regional hyperthermia (HT), in the Divisions of Radiation Oncology at the University of Utah Medical Center (UU) and the Kenneth Norris Jr Cancer Hospital of the University of Southern California (USC). HT was produced by the BSD-1000 HT system and the annular phased array (AA) applicator usually driven at 60-65 MHz, or the BSD-2000 HT system and the Sigma-60 (S60) applicator usually driven at 70-85 MHz. During the HT sessions acute toxicity was common, particularly because of pain within or outside the applicator, which was power-limiting in 43% of the patients overall. Pain was more easily manipulated, but more commonly power-limiting with the S60. Systemic stress was power-limiting in 22% of patients treated with the AA, but in no patients with the S60. Detailed thermal mapping and temperature analysis were performed on 26 patients. The mean overall average intratumour temperature achieved was 41 +/- 1.1 degrees C for 30 min; 5% and 35% of the monitored intratumour loci exceeded 43 degrees C and 42 degrees C, respectively. Temperatures recorded in the cervical os and proximal vagina appeared lower relative to the monitored normal structures in the region. Subacute treatment related toxicities occurred in five patients and included protracted pain (three) and superficial second degree burns (one), all of which resolved with supportive non-surgical therapy.

Adenocarcinoma↗
PubMedDate not supplied

Transurethral hyperthermia for benign prostatic hyperplasia: long term results.

Transurethral resection of the prostate (TURP) is the only recognized treatment in patients with benign prostatic hyperplasia (BPH). Transurethral hyperthermia (TUHT) was used as an alternative treatment in patient who refused TURP. From 1987 to 1988, 21 BPH patients with moderate to severe symptoms and signs of prostatism were treated with TUHT in a phase I trial. Mean pre-treatment subjective and objective values were: total symptom score (TSS) 13.5, obstructive symptom score (OSS) 6.5, irritative symptom score (TSS) 7.0, peak flow rate (PFR) 11.6 cc/sec, post-voiding residual volume (PRV) 187 cc, and prostate volume (PV) 93 cc. TUHT was given for a total of 177 sessions (mean 8.4), each of 60 min duration at a steady state. Temperature was recorded continuously on the urethral surface, in all treatments. It ranged from Tmin 40.3 degrees C to Tmax = 49.2 degrees C and Tmean = 44.1 degrees C. The mean minimum temperature of > or = 42 degrees C was obtained in 98% of the TUHT sessions. Treatments were given on an outpatient basis without sedation or anaesthesia. Treatment tolerance was excellent with minor acute toxicity common (71% of patients), of no clinical importance and with no late complications. Of the 21 patients treated, 17 (81%) had an objective and 15 (71%) a subjective improvement recorded at 6 months post-treatment. This statistically highly significant improvement included: 61% decrease in TSS; 66% decrease in OSS; 55% decrease in ISS; 42% increase in PFR; 55% decrease in PRV; and 21% decrease in PV. Of the 17 patients with objective improvement, nine have maintained their response to TUHT for a minimum period of over six years, two relapsed at 11 and 40 months, respectively, and six patients died of cardiovascular causes maintaining their response to death. This study has demonstrated TUHT treatment efficacy with no major or clinically important toxicity in BPH patients. A relative weakness of this report is a lack of verification of objective study parameters in the patients at seven years post-treatment. Prospective randomized trials are needed to define the role of TUHT in the management of BPH patients.

Aged↗