Abstract:A cylindrical balloon was developed to improve delivery of circumferential light for photodynamic therapy (PDT) of esophageal carcinoma. The balloon consisted of a 36-mm-long clear cylindrical membrane and a central tube to hold a cylindrical diffuser in the center of the lumen. Three isotropic probes were placed on the outside of the balloon to allow measurement of delivered light dose to the esophageal mucosa. The balloon was tested in the normal esophagus of 8 dogs that were injected with 4.0 mg/kg of PHOTO… Show more
“…This may explain the difference in fluence rate build-up factor between the two diffuser lengths. Panjehpour et al [19,20] also measured the fluence (rate) in a normal canine esophagus model using isotropic detectors. They found relatively small variations of approximately AE 12% between the (n ¼ 8) different animals.…”
Background and Objectives: Previous studies with PhotoDynamic Therapy (PDT) in bladder and bronchi have shown that due to scattering and reflection, the actually delivered fluence rate on the surface in a hollow organ can be significantly higher than expected. In this pilot study, we investigated the differences between the primary calculated and the actual measured fluence rate during PDT of Barrett's Esophagus (BE) using 23 independent clinical measurements in 15 patients. Study Design/Materials and Methods: A KTP-dye module laser at 630 nm was used as light source. Light delivery was performed using a cylindrical light diffuser inserted in the center of an inflatable transparent balloon with a length corresponding to the length of the Barrett's epithelium. The total light output power of the cylindrical diffuser was calibrated using an integrating sphere to deliver a primary fluence rate of 100 mW cm À2 . Two fiber-optic pseudo sphere isotropic detectors were placed on the balloon and were used to measure fluence rate at the surface of the esophageal wall during PDT. Results and Conclusions: The actual fluence rate measured was 1.5-3.9 times higher than the primary fluence rate for 630 nm. In general, the fluence rate amplification factor decreased with increasing redness of the tissue and was less for shorter diffusers. Fluence rate variations in time were observed which coincided with patients coughing, movement, and esophageal spasms. These factors combined with inter patient variability of the fluence rate measured appears to justify the routine application of this technique in PDT of BE.
“…This may explain the difference in fluence rate build-up factor between the two diffuser lengths. Panjehpour et al [19,20] also measured the fluence (rate) in a normal canine esophagus model using isotropic detectors. They found relatively small variations of approximately AE 12% between the (n ¼ 8) different animals.…”
Background and Objectives: Previous studies with PhotoDynamic Therapy (PDT) in bladder and bronchi have shown that due to scattering and reflection, the actually delivered fluence rate on the surface in a hollow organ can be significantly higher than expected. In this pilot study, we investigated the differences between the primary calculated and the actual measured fluence rate during PDT of Barrett's Esophagus (BE) using 23 independent clinical measurements in 15 patients. Study Design/Materials and Methods: A KTP-dye module laser at 630 nm was used as light source. Light delivery was performed using a cylindrical light diffuser inserted in the center of an inflatable transparent balloon with a length corresponding to the length of the Barrett's epithelium. The total light output power of the cylindrical diffuser was calibrated using an integrating sphere to deliver a primary fluence rate of 100 mW cm À2 . Two fiber-optic pseudo sphere isotropic detectors were placed on the balloon and were used to measure fluence rate at the surface of the esophageal wall during PDT. Results and Conclusions: The actual fluence rate measured was 1.5-3.9 times higher than the primary fluence rate for 630 nm. In general, the fluence rate amplification factor decreased with increasing redness of the tissue and was less for shorter diffusers. Fluence rate variations in time were observed which coincided with patients coughing, movement, and esophageal spasms. These factors combined with inter patient variability of the fluence rate measured appears to justify the routine application of this technique in PDT of BE.
“…Among them, the concentration of photosensitizer inside the tissue at the time of light application, the presence of oxygen and the light irradiance itself play a major role. When considering the treatment of the esophagus, several studies have already considered the difficulty in obtaining an optimal irradiance [9,10]. The comparison of PDT results in the esophagus between groups following protocols that are more or less optimized and with reasonably well-adapted light distributing devices clearly indicates that optimal devices (such as balloon) lead to much improved therapy [11].…”
Our results could explain side effects sometimes observed when performing PDT. 'Endoscopic' illumination, however, could also represent an interesting alternative to the 630 nm diode laser. When using white light, superficial efficacy of PDT could be reinforced and transmural necrosis leading to perforation or stenoses reduced, since there is less red light in depth compared with a diode laser.
“…The delivery of light energy was performed with a cylindrical diffuser inserted into a specially designed balloon catheter similar to previously designed models for esophageal PDT (31–33). This has the advantage of improved centering of the diffuser, leading to a more homogenous light delivery.…”
Section: Discussionmentioning
confidence: 99%
“…This has the advantage of improved centering of the diffuser, leading to a more homogenous light delivery. In addition, the exact surface area treated is known, so that fluence can be calculated on a square centimeter basis instead of solely on the basis of the length of the diffuser, allowing more precise light dosimetry (31).…”
Photodynamic therapy (PDT) has been used for many years for both palliative and curative treatment of bronchial carcinomas. However, prolonged skin phototoxicity and reduced depth of penetration has limited the widespread use of PDT. We studied the endobronchial phototoxicity of a novel photosensitizer, WST 09 (Tookad Ò ). Fourteen pairs of Large White-Landrace male piglets were given intravenous WST 09 followed by laser light illumination of the left mainstem bronchus. Different settings for light dose (fluence), fluence rate (FR), drug dose (D) and drug-light interval (DLI) were applied to each pair. Bronchial toxicity was assessed with repeat bronchoscopic photographic evaluation as well as by pathologic examination following autopsy. Animals developed no toxicity, moderate toxicity or severe toxicity. Increased toxicity was seen with increasing D and fluence and decreasing DLI, whereas no increased toxicity was seen with higher FR. PDT-related histological changes in the normal bronchus confirm the vascular effect of WST 09. Depending on the parameter settings for fluence, D and DLI, the lesions ranged from focal intramucosal ischemia to transmural infarction with subsequent acute inflammation and fibrosis. Clinically feasible parameters for drug and light dosimetry were documented. These data will be important in determining safe starting doses for human phase I/II studies.
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