THE INFLUENCE OF AIR CAVITIES ON INTERFACE DOSES FOR PHOTON BEAMS

被引:68
作者
KLEIN, EE
CHIN, LM
RICE, RK
MIJNHEER, BJ
机构
[1] WASHINGTON UNIV,SCH MED,EDWARD MALLINCKRODT INST RADIOL,ST LOUIS,MO 63110
[2] HARVARD UNIV,SCH MED,JOINT CTR RADIAT THERAPY,DEPT RADIAT THERAPY,BOSTON,MA 02115
[3] UNIV CALIF SAN DIEGO,SAN DIEGO,CA 92103
[4] NETHERLANDS CANC INST,1066 CX AMSTERDAM,NETHERLANDS
来源
INTERNATIONAL JOURNAL OF RADIATION ONCOLOGY BIOLOGY PHYSICS | 1993年 / 27卷 / 02期
关键词
PHOTON DOSE DISTRIBUTION; TISSUE HETEROGENEITY; INTERFACE DOSIMETRY; AIR CAVITY; ELECTRONIC EQUILIBRIUM;
D O I
10.1016/0360-3016(93)90255-T
中图分类号
R73 [肿瘤学];
学科分类号
100214 ;
摘要
Purpose: As the quantification of dose in homogeneous media is now better understood, it is necessary to further quantify effects from heterogeneous media. The most extreme case is related to air cavities. Although dose corrections at large distances beyond a cavity are accountable by attenuation differences, perturbations at air-tissue interfaces are complex to measure or calculate. These measurements helps understand the physical processes that govern these perturbations. Methods and Materials: A thin window parallel-plate chamber and a special diode were used for measurements with various air cavity geometries (layer, channel, cubic cavity, triangle) in x-ray beams of 4 and 15 MV. Results: Underdosing effects occur at both the distal and proximal air cavity interfaces. The magnitude depends on geometry, energy, and field sizes. As the cavity thickness increases, the central axis dose at the distal interface decreases. Increasing field size remedied the underdosing, as did the introduction of lateral walls. Following a 2.0 cm wide air channel for a 4 MV, 4 x 4 cm2 field there was an 11% underdose at the distal interface, while a 2.0 cm cubic cavity yielded only a 3% loss. Measurements at the proximal interface showed losses of 5% to 8%. For a 4 MV parallel opposed beam irradiation the losses at the interfaces were 10% for a channel cavity (in comparison with the homogeneous case) and 1% for a cube. The losses were slightly larger for the 15 MV beam. Underdosage at the lateral interface was 4% and 8% for the 4 MV and 15 MV beams, respectively. Conclusion: Although reports suggest better clinical results using lower photon energies with the presence of air cavities, there is no reliable dose calculation algorithm to predict interface doses accurately. The measurements reported here can be used to guide the development of new calculation models under nonequilibrium conditions. This situation is of clinical concern when lesions such as larynx carcinoma beyond air cavities are irradiated.
引用
收藏
页码:419 / 427
页数:9
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