RESUMO
The treatment of superficial skin lesions via daylight activated photodynamic therapy (PDT) has been explored theoretically with three dimensional (3D) Monte Carlo radiation transfer simulations. For similar parameters and conditions, daylight activated PDT was compared to conventional PDT using a commercially available light source. Under reasonable assumptions for the optical properties of the tissue, protoporphyrin IX (PpIX) concentration and a treatment dose of 75 J cm(-2), it was found that during a clear summer day an effective treatment depth of over 2 mm can be achieved after 30 min of daylight illumination at a latitude of 56 degrees North. The same light dose would require 2.5 h of daylight illumination during an overcast summer day where a treatment depth of about 2 mm can be achieved. For conventional PDT the developed model suggests that 15 min of illumination is required to deliver a light dose of 75 J cm(-2), which would result in an effective treatment depth of about 3 mm. The model developed here allows for the determination of photo-toxicity in skin tissue as a function of depth for different weather conditions as well as for conventional light sources. Our theoretical investigation supports clinical studies and shows that daylight activated PDT has the potential for treating superficial skin lesions during different weather conditions.
Assuntos
Algoritmos , Luz/efeitos adversos , Fotoquimioterapia/métodos , Doses de Radiação , Ácido Aminolevulínico/efeitos adversos , Humanos , Método de Monte Carlo , Fármacos Fotossensibilizantes/efeitos adversos , Protoporfirinas/efeitos adversos , Pele/efeitos dos fármacos , Pele/efeitos da radiaçãoRESUMO
The choice of light source is important for the efficacy of photodynamic therapy (PDT) of non-melanoma skin cancer. We simulated the photodynamic dose (PDD) delivered to a tumour during PDT using theoretical radiation transfer simulations performed via our 3D Monte Carlo radiation transfer (MCRT) model for a range of light sources with light doses up to 75 J cm(-2). The PDD delivered following superficial irradiation from (A) non-laser light sources, (B) monochromatic light, (C) alternate beam diameters and (D) re-positioning of the tumour within the tissue was computed. (A) The final PDD deposited to the tumour at a depth of 2 mm by the Paterson light source was 2.75, 2.50 and 1.04 times greater than the Waldmann 1200, Photocure and Aktilite, respectively. (B) Tumour necrosis occurred at a depth of 2.23 mm and increased to 3.81 mm for wavelengths 405 and 630 nm, respectively. (C) Increasing the beam diameter from 10 to 50 mm had very little effect on depth of necrosis. (D) As expected, necrosis depths were reduced when the tumour was re-positioned deeper into the tissue. These MCRT simulations show clearly the importance of choosing the correct light source to ensure optimal light delivery to achieve tumour necrosis.