Fluorescence photobleaching of ALA and ALA-heptyl ester induced protoporphyrin IX during photodynamic therapy of normal hairless mouse skin: a comparison of two light sources and different illumination schemes

This study investigated photobleaching of protoporphyrin IX (PpIX) induced by 5-aminolevulinic acid (ALA) and ALA-heptyl ester during superficial photodynamic therapy (PDT) in normal skin of the female BALB/c-nu/nu athymic mouse. We examined the effects of two light sources (laser and broadband lamp) and two different illumination schemes (fractionated light and continuous irradiation) on the kinetics of photobleaching. Our results show that light exposure (0-30 minutes, 10 mW/cm2) of wavelengths of approximately 420 nm (blue light) and 635 nm (red light) induced time-dependent PpIX photobleaching for mouse skin of 2% ALA and ALA-heptyl ester. Blue light (10 mW/cm2) caused more rapid PpIX photobleaching than did red light (100 mW/cm2), which is attributed to stronger absorption at 407 nm than at 632 nm for PpIX. In the case of light fractionation, fractionated light induced faster photobleaching compared with continuous light exposure after topical application of 2% ALA and ALA-heptyl ester in vivo. These have been suggested to allow reoxygenation of the irradiated tissue, with a consequent enhancement of singlet oxygen production in the second and subsequent fractions.     

Protoporphyrin IX fluorescence photobleaching increases with the use of fractionated irradiation in the esophagus

Fluorescence measurements have been used to track the dosimetry of photodynamic therapy (PDT) for many years, and this approach can be especially important for treatments with aminolevulinic-acid-induced protoporphyrin IX (ALA-PpIX). PpIX photobleaches rapidly, and the bleaching is known to be oxygen dependent, and at the same time, fractionation or reduced irradiance treatments have been shown to significantly increase efficacy. Thus, in vivo measurement of either the bleaching rate and/or the total bleaching yield could be used to track the deposited dose in tissue and determine the optimal treatment plans. Fluorescence in rat esophagus and human Barrett's esophagus are measured during PDT in both continuous and fractionated light delivery treatment, and the bleaching is quantified. Reducing the optical irradiance from 50 to 25 mWcm did not significantly alter photobleaching in rat esophagus, but fractionation of the light at 1-min on and off intervals did increase photobleaching up to 10% more (p value=0.02) and up to 25% more in the human Barrett's tissue (p value<0.001). While two different tissues and two different dosimetry systems are used, the data support the overall hypothesis that light fractionation in ALA-PpIX PDT esophageal treatments should have a beneficial effect on the total treatment effect.     

Fluorescence detection of protoporphyrin IX in living cells: a comparative study on single- and two-photon excitation

Photodynamic therapy (PDT) involves a combination of a lesion-localizing photosensitizer with light and has been established as a new modality for some medical indications. Much evidence has shown the correlation between subcellular localization of a photosensitizer with its photodynamic efficiency. However, the fluorescence of most photosensitizers in cells is weak and easily photobleached. We compare the effect of single-photon excitation (SPE) with that of two-photon excitation (TPE) on fluorescence detection of protoporphyrin IX (PpIX), a potent photosensitizer, in the PLC hepatoma cells in vitro. By using laser scanning confocal fluorescence microscopy, both fluorescence images and spectra of intracellular PpIX are studied with SPE of 405- and 488-nm lasers, and TPE of 800-nm femtosecond laser. The 405-nm laser is more efficient at exciting PpIX fluorescence than the 488-nm laser, but causes a considerable photobleaching of the PpIX fluorescence and induces weak autofluorescence signals of native flavins in the cells as well. The 800-nm TPE is found to significantly improve the quality of PpIX fluorescence images with negligible PpIX photobleaching and minimized endogenous autofluorescence, indicating the potential of 800-nm TPE for studying cellular localization of porphyrin photosensitizers for PDT.     

Spectroscopic measurements of photoinduced processes in human skin after topical application of the hexyl ester of 5-aminolevulinic acid.

Although 5-aminolevulinic acid, ALA, and its derivatives, have been widely studied and applied in clinical photodynamic therapy (PDT), there is still a lack of reliable and non-invasive methods and technologies to evaluate physiological parameters of relevance for the therapy, such as erythema, melanogenesis, and oxygen level. We have investigated the kinetics of these parameters in human skin in vivo during and after PDT with the hexyl ester of ALA, ALA-Hex. Furthermore, the depth of photosensitizer (protoporphyrin IX, PpIX) production after different application times was investigated. It was found that the depth increased with increasing application time of ALA-Hex. We also investigated the depth of PpIX before and after light exposure causing 50% photobleaching at 407 nm. The PpIX localized in superficial layers of the normal tissue was removed during the bleaching. Thus, after bleaching, the remaining PpIX was localized mainly in the deeper layers of normal tissue. We have applied fluorescence emission spectroscopy, fluorescence excitation spectroscopy, and reflectance spectroscopy in the study of the above-mentioned parameters. In conclusion, fluorescence excitation spectroscopy and reflectance spectroscopy are simple, useful, reliable, and noninvasive techniques in the evaluation of the processes taking place in human skin in vivo during and after PDT. Using these methods we were able to quantify melanogenesis, O2 level, erythema, vasoconstriction, and vasodilatation.     

Effect of (R)L-sulforaphane on 5-aminolevulinic acid-mediated photodynamic therapy

Topical photodynamic therapy (PDT) with 5-aminolevulinic acid (ALA), or so-called ALA-PDT, is a standard procedure in the clinical practice. For optimal treatment of nonmelanoma skin cancer, actinic keratoses and other dermatoses improvements are required because of adverse side effects, which include pruritus, erythema, edema, and pain. (R)L-sulforaphane (SF) is a compound that protects against erythema, but it can also induce DNA fragmentation that leads to cell death by apoptosis. The aim of our study was to investigate whether SF has any impact on protoporphyrin IX (PpIX) production and on PDT effectiveness. We have investigated some relevant properties of SF: its photostability in dimethyl sulfoxide (DMSO), its effect on ALA-induced production of PpIX in A431 human squamous carcinoma cells and in human skin, its effect on the photoinactivation of PpIX sensitized cells, and its effect on the rate of photobleaching of PpIX. SF had no influence on PpIX photodegradation, neither in solution nor in A431 cells. The synthesis of PpIX was increased by SF in human skin, but not in A431 cells. The average increase in PpIX fluorescence in human skin was 18% +/- 6% and 43% +/- 10% for ALA combined with 80 nmol/L SF and 120 nmol/L SF, respectively. Pretreatment with (R)L-sulforaphane before topical ALA-PDT may improve penetration of ALA through the stratum corneum, and, subsequently, increase PpIX synthesis.     

Induction of apoptosis by hexaminolevulinate-mediated photodynamic therapy in human colon carcinoma cell line 320DM.

Photodynamic therapy (PDT) typically involves systemic or topical administration of a tumor-localizing photosensitizer or prodrug and its subsequent activation by visible light. This results primarily in singlet oxygen-induced photodamage to the tumor. 5-Aminolevulinic acid (ALA) and its derivatives have recently been widely used for PDT due to their selective induction in tumor of endogenous protoporphyrin IX (PpIX), a potent photosensitizer. Although ALA-PDT has achieved successful results in the treatment of several clinical oncological and nononcological diseases, the mechanisms of this modality are still not fully elucidated. In the present study, the human colon carcinoma cell line 320DM was treated in vitro with PDT using hexaminolevulinate (HAL), a hexylester of ALA known to be 50 to 100 times more efficient at producing PpIX formation than ALA itself. PpIX production increased with increasing HAL concentrations in the cells and phototoxicity of the cells was enhanced with increasing light (450 nm) doses. HAL-PDT induced apoptotic cell death, as measured by nuclear staining of Hoechst 33342 for fluorescence microscopy, DNA electrophoresis and TdT staining for flow cytometry. PDT with 5 muM of HAL and a light dose of 640 mJ/cm2 produced a 75% apoptotic cell population 40 hr after the treatment. Furthermore, the loss of mitochondrial membrane potential coincident with the release of cytochrome c from the mitochondria into the cytosol led to a rapid activation of caspase-9 and caspase-3 (an executioner), indicating that the selective damage to the mitochondria by HAL-PDT can induce a cytochrome-c-mediated apoptotic response in the 320DM cells.     

Correlation of in vivo photosensitizer fluorescence and photodynamic-therapy-induced depth of necrosis in a murine tumor model

We compared light-induced fluorescence (LIF) to nominal injected drug dose for predicting the depth of necrosis response to photodynamic therapy (PDT) in a murine tumor model. Mice were implanted with radiation-induced fibrosarcoma (RIF) and were injected with 0, 5, or 10 mg/kg Photofrin. 630-nm light (30 J/cm(2), 75 mW/cm(2)) was delivered to the tumor after 24 hours. Fluorescence emission (lambda(excitation)=545 nm, lambda( emission)=628 nm) from the tumor was measured. The LIF data had less scatter than injected drug dose, and was found to be at least as good as an injected drug dose for predicting the depth of necrosis after PDT. Our observations provide further evidence that fluorescence spectroscopy can be used to quantify tissue photosensitizer uptake and to predict PDT tissue damage.     

Comparison of noninvasive photodynamic therapy dosimetry methods using a dynamic model of ALA-PDT of human skin

A numerical model of ALA photodynamic therapy of human skin was used to calculate photosensitizer fluorescence and singlet-oxygen luminescence (SOL) observable at the skin surface during treatment. From the emissions, three practical dose metrics were calculated: the fractional fluorescence bleaching metric (FFBM) given by F(0)/F, where F is photosensitizer protoporphyrin IX (PpIX) fluorescence and F(0) is its initial value, the absolute fluorescence bleaching metric (AFBM) given by F(0)-F, and the cumulative SOL (CSOL). These three metrics can be measured during clinical PDT treatment, but their relation to actual singlet-oxygen distribution in the skin is complex and may depend on treatment parameters such as irradiance. Using the model, the three metrics were compared to the average singlet-oxygen dose in the dermis. Despite the complex dependence of (1)O(2) concentration on depth, a roughly linear correlation was found for all three dose metrics. The correlation for the FFBM was not robust when treatment parameters were varied and this metric was especially sensitive to the initial PpIX concentration and its depth dependence. The AFBM was less sensitive to treatment conditions but CSOL demonstrated the best overall performance.     

Repetitive photodynamic therapy of malignant brain tumors.

The probability of achieving local control with current single-shot, intraoperative photodynamic therapy (PDT) treatments of intracerebral gliomas seems improbable due to the length of time required to deliver adequate light fluences to depths of 1-2 cm in the resection margin. Additionally, due to the short doubling time of many malignant gliomas, the kill rate per cell doubling indicates that it seems unlikely that a single treatment would be sufficient to prevent tumor recurrence. Multiple repetitive treatments would therefore seem required. In this publication we primarily review our work examining the effects of repetitive PDT on malignant brain tumor cells both in vitro and in vivo. The in vitro therapy response of human and rat glioma spheroids to 5-aminolevulinic acid (ALA)-mediated PDT in repetitive form was investigated. The results indicated that PDT repeated at relatively long intervals (weeks) was more effective at inhibiting spheroid growth than either daily fractionated PDT or single-treatment regimes. The in vivo response to repetitive treatment was evaluated in a rodent glioma model where BT4C cell line tumors were established in the brains of inbred BD-IX rats. Microfluorometry of frozen tissue sections showed that PpIX is produced with a 10-20:1 tumor to normal tissue selectivity ratio 4 hr after ALA injection. Preliminary evidence of increased efficacy of repetitive PDT and low fluence rate treatment is presented.     

Development of a new illumination procedure for photodynamic therapy of the abdominal cavity

A homogeneous illumination of intra-abdominal organs is essential for successful photodynamic therapy of the abdominal cavity. Considering the current lack of outstanding light-delivery systems, a new illumination procedure was assessed. A rat model of peritoneal carcinomatosis was used. Four hours after intraperitoneal injection of hexaminolevulinate, a square illuminating panel connected to a 635-nm laser source was inserted vertically into the abdominal cavity. The abdominal incision was sutured and a pneumoperitoneum created prior to illumination. Light dosimetry was based on the calculation of the peritoneal surface by MRI. The rats were treated with a light dose of 20, 10, 5 or 2.5 J/cm(2) administered continuously with an irradiance of 7 mW/cm(2). The homogeneity of the cavity illumination was assessed by quantification of the photobleaching of the tumor lesions according to their localization and by scoring of that of the liver and of the bowel immediately after treatment. Photobleaching quantification for tumor lesions relied on the calculation of the fluorescence intensity ratio (after/before treatment) after recording of the lesions during blue-light laparoscopy and determination of their fluorescence intensity with Sigmascan Pro software. The procedure led to a homogeneous treatment of the abdominal cavity. No statistical difference was observed for the photobleaching values according to the localization of the lesions on the peritoneum (p=0.59) and photobleaching of the liver and of the intestine was homogeneous. We conclude that this procedure can successfully treat the major sites involved in peritoneal carcinomatosis.     

Characterization of Photofrin photobleaching for singlet oxygen dose estimation during photodynamic therapy of MLL cells in vitro

A singlet oxygen dose model is developed for PDT with Photofrin. The model is based on photosensitizer photobleaching kinetics, and incorporates both singlet oxygen and non-singlet oxygen mediated bleaching mechanisms. To test our model, in vitro experiments were performed in which MatLyLu (MLL) cells were incubated in Photofrin and then irradiated with 532 nm light. Photofrin fluorescence was monitored during treatment and, at selected fluence levels, cell viability was determined using a colony formation assay. Cell survival correlated well to calculated singlet oxygen dose, independent of initial Photofrin concentration or oxygenation. About 2 x 10(8) molecules of singlet oxygen per cell were required to reduce the surviving fraction by 1/e. Analysis of the photobleaching kinetics suggests that the lifetime of singlet oxygen in cells is 0.048 +/- 0.005 micros. The generation of fluorescent photoproducts was not a result of singlet oxygen reactions exclusively, and therefore did not yield additional information to aid in quantifying singlet oxygen dose.     

Monitoring Pc 4 photodynamic therapy in clinical trials of cutaneous T-cell lymphoma using noninvasive spectroscopy

Silicon phthalocyanine Pc 4 photodynamic therapy (Pc 4-PDT) has emerged as a potentially effective treatment for cutaneous T-cell lymphoma (CTCL). Noninvasive reflectance and fluorescence spectroscopy before, during, and after PDT may provide useful dose metrics and enable therapy to be tailored to individual lesions. We present the design and implementation of a portable bedside spectroscopy system for initial clinical trials of Pc 4-PDT of CTCL. Reflectance and fluorescence spectra were obtained from an early stage CTCL patient throughout the course of the PDT treatment. Preliminary patient data show a significant effect of Pc 4 on the tissue absorption, modest Pc 4 photobleaching, and heterogeneity of Pc 4 within and between the lesions.     

Immune response against angiosarcoma following lower fluence rate clinical photodynamic therapy.

Tumor response to photodynamic therapy (PDT) is dependent on treatment parameters used. In particular, the light fluence rate may be an important determinant of the treatment outcome. In this clinical case report, we describe the response of angiosarcoma to PDT carried out using different fluence rates and drug and light doses. A patient with recurrent multifocal angiosarcoma of the head and neck was recruited for PDT. A new generation chlorin-based photosensitizer, Fotolon, was administered at a dose of 2.0 to 5.7 mg/kg. The lesions were irradiated with 665 nm laser light for a light dose of 65 to 200 J/cm2 delivered at a fluence rate of 80 or 150 mW/cm2. High dose PDT carried out at a high fluence rate resulted in local control of the disease for up to a year; however, the disease recurred and PDT had to be repeated. PDT of new lesions carried out at a lower fluence rate resulted in tumor eradication. More significantly, it also resulted in spontaneous remission of neighboring and distant untreated lesions. Repeat PDT carried out on a recurrent lesion at a lower fluence rate resulted in eradication of both treated and untreated lesions despite the lower total light dose delivered. Immunohistochemical examination of biopsy samples implies that PDT could have activated a cell-mediated immune response against untreated lesions. Subsequent histopathological examination of the lesion sites showed negative for disease. Our clinical observations show that lower fluence rate PDT results in better outcome and also indicate that the fluence rate, rather than the total light dose, is a more crucial determinant of the treatment outcome. Specifically, lower fluence rate PDT appears to activate the body's immune response against untreated lesions.     

Morphological changes of the dermatophyte Trichophyton rubrum after photodynamic treatment: a scanning electron microscopy study.

Treatment strategies for superficial mycosis caused by the dermatophyte Trichophyton rubrum consist of the use of topical or oral antifungal preparations. We have recently discovered that T. rubrum is susceptible to photodynamic treatment (PDT), with 5,10,15-tris(4-methylpyridinium)-20-phenyl-[21H,23H]-porphine trichloride (Sylsens B) as a photosensitizer. The susceptibility appeared to depend on the fungal growth stage, with PDT efficacy higher with microconidia when compared to mycelia. The aim of this study was to investigate, with the use of scanning electron microscopy, the morphological changes caused by a lethal PDT dose to T. rubrum when grown on isolated human stratum corneum. Corresponding dark treatment and light treatment without photosensitizer were used as controls. A sub-lethal PDT dose was also included in this investigation The morphologic changes were followed at various time points after the treatment of different fungal growth stages. Normal fungal growth was characterized by a fiber-like appearance of the surface of the hyphae and microconidia with the exception of the hyphal tips in full mycelia and the microconidia shortly after attachment to the stratum corneum. Here, densely packed globular structures were observed. The light dose (108 J/cm2) in the absence of Sylsens B, or the application of the photosensitizer in the absence of light, caused reversible fungal wall deformations and bulge formation. However, after a lethal PDT, a sequence of severe disruptions and deformations of both microconidia and the mycelium were observed leading to extrusion of cell material and emptied fungal elements. In case of a non-lethal PDT, fungal re-growth started on the remnants of the treated mycelium.     

Total skin electron therapy treatment verification: Monte Carlo simulation and beam characteristics of large non-standard electron fields

Total skin electron therapy (TSET) is a complex technique which requires non-standard measurements and dosimetric procedures. This paper investigates an essential first step towards TSET Monte Carlo (MC) verification. The non-standard 6 MeV 40 x 40 cm2 electron beam at a source to surface distance (SSD) of 100 cm as well as its horizontal projection behind a polymethylmethacrylate (PMMA) screen to SSD = 380 cm were evaluated. The EGS4 OMEGA-BEAM code package running on a Linux home made 47 PCs cluster was used for the MC simulations. Percentage depth-dose curves and profiles were calculated and measured experimentally for the 40 x 40 cm2 field at both SSD = 100 cm and patient surface SSD = 380 cm. The output factor (OF) between the reference 40 x 40 cm2 open field and its horizontal projection as TSET beam at SSD = 380 cm was also measured for comparison with MC results. The accuracy of the simulated beam was validated by the good agreement to within 2% between measured relative dose distributions, including the beam characteristic parameters (R50, R80, R100, Rp, E0) and the MC calculated results. The energy spectrum, fluence and angular distribution at different stages of the beam (at SSD = 100 cm, at SSD = 364.2 cm, behind the PMMA beam spoiler screen and at treatment surface SSD = 380 cm) were derived from MC simulations. Results showed a final decrease in mean energy of almost 56% from the exit window to the treatment surface. A broader angular distribution (FWHM of the angular distribution increased from 13 degrees at SSD = 100 cm to more than 30 degrees at the treatment surface) was fully attributable to the PMMA beam spoiler screen. OF calculations and measurements agreed to less than 1%. The effect of changing the electron energy cut-off from 0.7 MeV to 0.521 MeV and air density fluctuations in the bunker which could affect the MC results were shown to have a negligible impact on the beam fluence distributions. Results proved the applicability of using MC as a treatment verification tool for complex radiotherapy techniques.     

Quantitative fluorescence imaging of protoporphyrin IX through determination of tissue optical properties in the spatial frequency domain

The ability to quantitatively determine tissue fluorescence is of interest for the purpose of better understanding the details of photodynamic therapy of skin cancer. In particular, we are interested in quantifying protoporphyrin IX (PpIX) in vivo. We present a method of correcting fluorescence for effects of native tissue absorption and scattering properties in a spatially resolved manner that preserves the resolution of the fluorescence imaging system, based off a homogeneous representation of tissue. Validation was performed using a series of liquid turbid phantoms having varying concentrations of absorber, scatterer, and fluorophore (PpIX). Through the quantification of tissue optical properties via spatial frequency domain imaging, an empirical model based on Monte Carlo simulations was deployed to successfully decouple the effects of absorption and scattering from fluorescence. From this we were able to deduce the concentration of the PpIX to within 0.2 μg/ml of the known concentration. This method was subsequently applied to the determination of PpIX concentration from in vivo normal skin where the model-based correction determined a concentration of 1.6 μg/ml, which is in agreement with literature.     

Comparison of merocyanine 540-mediated photodynamic action on leukemia cells between pulsed and continuous wave light sources.

Whether a pulsed laser is superior to a continuous wave (CW) light source in photodynamic therapy (PDT) of cancer is still unclear and contradictory in the literature. Although photosaturation of a sensitizer and oxygen depletion in tumor have been considered to be involved during pulsed laser irradiation, there is a lack of experimental data. In the present work several parameters such as the amount of merocyanine 540 (MC540) in cells, the oxygen concentration in cells, and the amount of photos reaching cells during pulsed laser irradiation, were studied to compare the MC540-mediated PDT effects of a pulsed laser and a CW light source on murine myeloid WEH-3B (JCS) cells in vitro. The results showed that the pulsed laser was less effective at cell inactivation than the CW light under the same irradiation dose. However, when the energy of the pulsed laser was reduced from 0.25 to 0.06 mJ/cm2 while keeping the total irradiation dose unchanged, the photoinactivation of cells was increased significantly. Based on the measurements and calculations for the present experimental conditions, each cell has about 108 MC540 molecules bound (5 microg/ml MC540 for 1 hr) and receives about 109 photos from 0.25 mJ/cm2 of the pulsed laser. The results indicate that the photosaturation of MC540 occurs in the present conditions due to the fact that the photons received by one cell in one laser pulse were much more than the numbers of MC540 molecules bound to one cell. Thus, the photosaturation of the photosensitizer is one of the reasons to explain the different efficiency in cell inactivation between the pulsed laser and CW light.     

A comprehensive mathematical model of microscopic dose deposition in photodynamic therapy

We have developed a comprehensive theoretical model for rigorously describing the spatial and temporal dynamics of oxygen (3O2) consumption and transport and microscopic photodynamic dose deposition during photodynamic therapy (PDT) in vivo. Previously published models have been improved by considering perfused vessels as a time-dependent 3O2 source and linking the 3O2 concentration in the vessel to that within the tissue through the Hill equation. The time-dependent photochemical 3O2 consumption rate incorporates sensitizer photobleaching effects and an experimentally determined initially nonuniform photosensitizer distribution. The axial transport of 3O2 is provided for in the capillaries and in the surrounding tissue. A self-sensitized singlet oxygen (1O2)-mediated bleaching mechanism and the measured, initially nonuniform distribution of mesotetrahydroxyphenyl chlorin at 3 h after intravascular administration were used to demonstrate the capabilities of the model. Time-evolved distributions of 3O2 concentration were obtained by numerically solving two-dimensional diffusion-with-reaction equations both in the capillary and the adjacent tissue. Using experimentally established physiological and photophysical parameters, the mathematical model allows computation of the dynamic variation of hemoglobin-3O2 saturation (SO2) within the vessels, irreversible sensitizer degradation due to photobleaching, and the microscopic distributions of 3O2, sensitizer concentration, and 1O2 dose deposition under various irradiation conditions. The simulations reveal severe axial gradients in 3O2 and in photodynamic dose deposition in response to a wide range of clinically relevant treatment parameters. Thus, unlike former Krogh cylinder-based models, which assume a constant 3O2 concentration at the vessel, this new model identifies conditions in which 3O2 depletion and minimal deposition of reacting 1O2 exist near the end of axial segments of vessels and shows that treatment-limiting 3O2 depletion is induced at fluence rates as low as 10 mW cm(-2). These calculations also demonstrate that intercapillary heterogeneity of photosensitizer contributes significantly to the distribution of photodynamic dose. This more rigorous mathematical model enables comparison with experimentally observable, volume-averaged quantities such as SO2 and the loss of sensitizer fluorescence through bleaching that have not been included in previous analyses. Further, it establishes some of the intrinsic limitations of such measurements. Specifically, our simulations demonstrate that tissue measurements of SO2 and of photobleaching are necessarily insensitive to microscopic heterogeneity of photodynamic dose deposition and are sensitive to intercapillary spacing. Because prior knowledge of intercapillary distances in tumors is generally unavailable, these measurements must be interpreted with caution. We anticipate that this model will make useful dosimetry predictions that should inform optimal treatment conditions and improve current clinical protocols.     

Monte Carlo techniques for scattering foil design and dosimetry in total skin electron irradiations

Total skin electron irradiation (TSEI) with single fields requires large electron beams having good dose uniformity, dmax at the skin surface, and low bremsstrahlung contamination. To satisfy these requirements, energy degraders and scattering foils have to be specially designed for the given accelerator and treatment room. We used Monte Carlo (MC) techniques based on EGS4 user codes (BEAM, DOSXYZ, and DOSRZ) as a guide in the beam modifier design of our TSEI system. The dosimetric characteristics at the treatment distance of 382 cm source-to-surface distance (SSD) were verified experimentally using a linear array of 47 ion chambers, a parallel plate chamber, and radiochromic film. By matching MC simulations to standard beam measurements at 100 cm SSD, the parameters of the electron beam incident on the vacuum window were determined. Best match was achieved assuming that electrons were monoenergetic at 6.72 MeV, parallel, and distributed in a circular pattern having a Gaussian radial distribution with full width at half maximum = 0.13 cm. These parameters were then used to simulate our TSEI unit with various scattering foils. Two of the foils were fabricated and experimentally evaluated by measuring off-axis dose uniformity and depth doses. A scattering foil, consisting of a 12 x 12 cm2 aluminum plate of 0.6 cm thickness and placed at isocenter perpendicular to the beam direction, was considered optimal. It produced a beam that was flat within +/-3% up to 60 cm off-axis distance, dropped by not more than 8% at a distance of 90 cm, and had an x-ray contamination of <3%. For stationary beams, MC-computed dmax, Rp, and R50 agreed with measurements within 0.5 mm. The MC-predicted surface dose of the rotating phantom was 41% of the dose rate at dmax of the stationary phantom, whereas our calculations based on a semiempirical formula in the literature yielded a drop to 42%. The MC simulations provided the guideline of beam modifier design for TSEI and estimated the dosimetric performance for stationary and rotational irradiations.     

Heat shock protein 27 protects against aminolevulinic acid-mediated photodynamic therapy-induced apoptosis and necrosis in human breast cancer cells.

This study utilized two breast cancer cell lines differing only in their expression of heat shock protein 27 (hsp27). The DB46 cell line was engineered to express high constitutive levels of hsp27, while the DC4 cell line expresses normal low levels of hsp27. The cells were incubated in 1 mM aminolevlinic acid (ALA) 4 hr prior to light exposures (635 nm) ranging from 1 to 20 J/cm2. Both cell lines displayed a dose response to photodynamic therapy (PDT) as assayed by clonogenic survival. LD50s of 2.68 and 1.27 J/cm2 were observed for DB46 and DC4 cells respectively. ALA-PDT-induced resistance to both apoptosis and necrosis in the DB46 cell line was found from TUNEL assays and fluorescence microscopy studies using propidium iodide and Hoechst staining.