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W M Star

Publications and source records attributed to W M Star.

At least 55 records · Page 3Linked to original sources

Integrating sphere effect in whole-bladder-wall photodynamic therapy: II. The influence of urine at 458, 488, 514 and 630 nm optical irradiation.

Whole-bladder-wall (WBW) photodynamic therapy (PDT) performed with 458 nm instead of 630 nm wavelength might be advantageous. On the basis of Monte Carlo (MC) computer simulations using in vitro bladder optical properties, these wavelengths show an equally strong integrating sphere effect, while haematoporphyrin derivatives can be excited equally efficiently and more easily with an Ar+ laser at 458 nm. To test this, fluence rates were measured at the walls of two piglet bladders during in vivo and in vitro WBW optical irradiations at 458, 488, 514 and 630 nm. In the in vitro experiment, a controlled amount of urine with known absorption coefficient at the irradiation wavelengths was introduced in the bladder cavity. The optical absorption and scattering coefficients and anisotropy factor of the tissue of both piglet bladders were determined in vitro with a double integrating sphere set-up. MC simulations, using the in vitro optical properties, agree only partly with the measured bladder wall fluence rates. In the in vitro experiment with saline in the bladder cavity, the fluence rate at the bladder wall is lowest for 514 nm irradiation and highest for 458 and 630 nm irradiation. In the in vivo experiment and the in vitro experiment with light absorbing urine in the bladder cavity, which mimics the clinical situation, irradiation at 458 nm wavelength resulted in the lowest fluence rate for a given optical power emitted. It cannot be completely ruled out that in an in vivo bladder the light absorption by haemoglobin further reduces the integrating sphere effect at wavelengths shorter than 630 nm. Thus, WBW PDT with red light (630 nm) is technically more advantageous than that with green light (514 nm) or blue light (488 and 458 nm) as this gives the strongest integrating sphere effect.

Animals↗

In vivo fluorescence and photodynamic activity of zinc phthalocyanine administered in liposomes.

Zinc(II) phthalocyanine, a hydrophobic photosensitiser, was incorporated in unilamellar liposomes and studied in vivo for fluorescence kinetics and photodynamic activity. An observation chamber mounted in a dorsal skinfold of female WAG/Rij rats was used as a model system. In the chamber, an isogeneic mammary carcinoma was transplanted in the subcutaneous tissue. Phthalocyanine fluorescence was excited at 610 nm with a power density of 0.25 mW cm-2 and was detected above 665 nm through a high-pass filter using a two-stage image intensifier coupled to a charge-coupled device (CCD) camera. Following i.v. administration of 0.14 mg kg-1 of the drug, the fluorescence pharmacokinetics of the dye in vasculature, normal tissue and tumour tissue was determined as a function of time. Tumour fluorescence increased slowly to a maximum about 3 h post injection (p.i.), and remained well above the normal tissue fluorescence till 24 h p.i. Fluorescence in the circulation was always stronger than in the tissues. A treatment light dose at a wavelength of 675 nm was delivered 24 h p.i. One group of six animals received a total light dose of 150 J cm-2 (100 mW cm-2). A second group of six animals received a total light dose of 450 J cm-2 at the same dose rate. Vascular damage resulting from treatment was observed only at the final stages of the irradiation, despite the relatively high levels of fluorescence in the circulation. Immediate post-treatment (re)transplantation of the content of the chamber into the flank always resulted in tumour regrowth, confirming the presence of viable tumour cells following photodynamic therapy (PDT). When the chamber was left intact, the light dose of 450 J cm-2 yielded complete tissue necrosis. The role of the dye-carrier complex in shielding the vascular surrounding from photoproducts was studied in a third group of animals. The presence of peroxides was demonstrated in the serum of these animals after PDT with zinc phthalocyanine in liposomes (ZnPc-lip) using a total light dose of 450 J cm-2. This ex vivo observation supports the previously reported observations in vitro that the carrier complex is able to quench the photoproducts resulting from photoactivation of the photosensitiser which is present in the circulation.

Animals↗

In vivo fluorescence kinetics and photodynamic therapy using 5-aminolaevulinic acid-induced porphyrin: increased damage after multiple irradiations.

The kinetics of fluorescence in tumour (TT) and subcutaneous tissue (ST) and the vascular effects of photodynamic therapy (PDT) were studied using protoporphyrin IX (PpIX), endogenously generated after i.v. administration of 100 and 200 mg kg-1 5-aminolaevulinic acid (ALA). The experimental model was a rat skinfold observation chamber containing a thin layer of ST in which a small syngeneic mammary tumour grows in a sheet-like fashion. Maximum TT and ST fluorescence following 200 mg kg-1 ALA was twice the value after 100 mg kg-1 ALA, but the initial increase with time was the same for the two doses in both TT and ST. The fluorescence increase in ST was slower and the maximum fluorescence was less and appeared later than in TT. Photodynamic therapy was applied using green argon laser light (514.5 nm, 100 J cm-2). Three groups received a single light treatment at different intervals after administration of 100 or 200 mg kg-1 ALA. In these groups no correlation was found between the fluorescence intensities and the vascular damage following PDT. A fourth group was treated twice and before the second light treatment some fluorescence had reappeared after photobleaching due to the first treatment. Only with the double light treatment was lasting TT necrosis achieved, and for the first time with any photosensitiser in this model this was accomplished without complete ST necrosis.

Aminolevulinic Acid↗

Integrating sphere effect in whole bladder wall photodynamic therapy: I. 532 nm versus 630 nm optical irradiation.

The optical absorption, scattering and anisotropy coefficients of piglet bladder, with and without Photofrin, and of diseased human bladder were determined in vitro with a double integrating sphere set-up in the wavelength range 450-800 nm. Monte Carlo simulations were performed in a spherical geometry, representing the bladder, using the optical properties at 532 nm and 630 nm determined in vitro. The calculated fluence rates support the fluence rates that were measured at the bladder wall of a piglet during an in vivo whole bladder wall (WBW) irradiation at 532 nm and 630 nm. Fluence rates calculated and measured in vivo at 630 nm are in agreement with those measured previously in clinical photodynamic therapy (PDT) at 630 nm. WBW-PDT with red light (630 nm) will be technically more advantageous than with green light (532 nm) because of a stronger integrating sphere effect, which reduces the variations of the fluence rate at the bladder wall when the isotropic light source is moved away from the centre of the bladder. Since the optical properties show considerable variations from bladder to bladder, and since as a result the light fluence rate at the bladder wall can vary by a factor of 3 to 4 for the same non-scattered light fluence rate, we conclude that in situ light dosimetry during clinical WBW-PDT is a necessity.

Animals↗

Effect of photodynamic therapy on the endothelium-dependent relaxation of isolated rat aortas.

The early vascular effects of photodynamic therapy (PDT) include transient vasoconstriction and platelet aggregation. Since endothelium-derived relaxing factor (EDRF) is a potent vasodilator and inhibitor of platelet aggregation, we questioned whether PDT impairs the production of EDRF. To study this possible effect of PDT, endothelium-dependent relaxations of thoracic aortas obtained from male Wistar rats were determined. The aortic rings were connected to a isometric force transducer, exposed to various doses of Photofrin porfimer sodium (Photofrin) (0.1-1.0 microgram/ml), and illuminated with red light (wavelength > 610 nm, 14.6 +/- 1.5 mW/cm2) for different time periods (5-25 min). Endothelium-dependent relaxation was induced by acetylcholine in precontracted aortic rings. This EDRF-mediated relaxation was decreased after PDT in a light dose- and drug dose-dependent manner. Light microscopic examination did not show loss of endothelial cells. Similar results were obtained with rat aortas exposed to Photofrin in vivo and illuminated in vitro. Direct smooth muscle relaxation induced with sodium nitroprusside was not impaired, showing that PDT did not reduce the ability of smooth muscles to relax. No effect on the contractile responses was found either. We conclude that PDT impairs the production or release of EDRF by the endothelium. This could play an important role in the initial events occurring in vivo during and after PDT.

Acetylcholine↗

Fluorescence and photodynamic effects of bacteriochlorin a observed in vivo in 'sandwich' observation chambers.

Bacteriochlorin a (BCA), a derivative of bacteriochlorphyll a, is an effective photosensitiser in vitro and in vivo. BCA has a major absorption peak at 760 nm where tissue penetration is optimal. This property, together with rapid tissue clearance promises minor skin photosensitivity. The tissue localising and photodynamic properties of BCA were studied using isogeneic RMA mammary tumours, transplanted into subcutaneous tissue in transparent 'sandwich' observation chambers on the back of WAG/Rij rats. The fluorescence kinetics following an i.v. administration of 20 mg kg-1 BCA was assessed in blood vessels, tumour and normal tissue. Subsequently, the development of vascular- and tissue damage after a therapeutic light dose (760 nm, 600 J cm-2) was observed. Fifteen minutes post injection (p.i.), the fluorescence of BCA in the tumour reached a plateau value of 2.5 times the fluorescence in the normal tissue. From 1 h post injection the tumour fluorescence diminished gradually; after 24 h, the tumour fluorescence signal did not exceed that of the normal tissue. Following photodynamic therapy (PDT), 24 h p.i., complete vascular stasis was observed 2 h post treatment in the tumour only, with subsequent recovery. The presence of viable tumour cells following PDT was assessed by histology and re-transplantation of treated tumour tissue from the chamber into the flank immediately or 7 days after treatment. In both cases tumour regrowth was observed. BCA-PDT (20 mg kg-1, 760 nm, 100 J cm-2) 1 h after BCA administration, an interval which gives the optimal differential between tumour and normal tissue, was sufficient to prevent tumour regrowth. However, this only occurred when re-transplantation was performed 7 days after PDT. During PDT, 1 h p.i., vascular damage in tumour and normal tissue was considerable. Complete vascular shut-down was observed in the tumour 2 h after therapy and in the surrounding tissues at 24 h. Circulation damage was associated with vascular spasm and occlusion probably due to thrombi formation. Oedema was notable, especially following PDT with 600 J cm-2 at 24 h p.i.

Animals↗

In situ light dosimetry during whole bladder wall photodynamic therapy: clinical results and experimental verification.

Photodynamic therapy (PDT) using Photofrin IIR (PII) as a photosensitizer is currently being evaluated as a new treatment modality for superficial bladder cancer. An optimum therapeutic ratio requires uniform illumination of the whole bladder wall and accurate light dosimetry. The first clinical light dosimetry results (16 patients) are reported, obtained using a system which allows in situ measurement and control of the light fluence at the bladder wall. The true light fluence at the bladder wall (i.e. non-scattered incident light plus scattered light) appeared to be on the average a factor beta = 4.8 +/- 1.2 (mean +/- SD) larger than the non-scattered incident light fluence. The latter is often, but incorrectly, used in reporting light fluence. The factor beta varied between patients with extremes of 2.5 and 7.1. Because such large variations were unexpected, but may have significant clinical consequences, experiments in plastic bladder models were performed to study separately the various factors (e.g. bladder shape, air bubble) affecting the dosimetry in clinical treatments. The results imply that the clinical variations are most likely to be the result of variations in optical properties of the bladder wall mucosa, probably due to the disease and prior treatments. If light dosage is based on non-scattered light only (without in situ light dosimetry, according to a current clinical protocol) the present results indicate variations in the true (total) light fluence between patients by a factor of at least 2. At the least this may cause unnecessary discomfort to a number of patients.

Female↗

Pilot study on light dosimetry for endobronchial photodynamic therapy.

Endobronchial photodynamic therapy (EB-PDT) using photofrin as the photosensitizer is currently being evaluated as a new treatment modality for inoperable endobronchial tumors. One of the current problems with EB-PDT is the lack of adequate light dosimetry, which hampers proper interpretation of treatment results. In this study exploratory light dosimetry experiments were performed in plastic bronchus models using either a microlens-tipped fiber (suitable for illumination of small superficial tumors) or a cylindrical diffuser fiber (suitable for intraluminal illumination or interstitial illumination of partially obstructing tumors). It is shown that the light fluence prescriptions of current clinical protocols yield a different fluence in tissue for each illumination modality. Depending on the actual placement of the cylindrical diffuser within the lumen, the light fluence at 5 mm depth in the homogeneous tissue model may vary by a factor of 3. The results were confirmed by in vivo experiments in the trachea of a pig. There is a possibility of enhanced tissue response by accidental hyperthermia induced during EB-PDT. The temperature rise was therefore estimated in vivo using a rat tumor model to mimic clinical EB-PDT. Temperature rises of at least 5 degrees C and 10 degrees C can be expected for intraluminal and intratumoral illumination, respectively, at 3.5 +/- 1 mm depth in tissue and 400 mW/cm diffuser output. Light fluence and its distribution in the bronchus strongly depend on the geometry and the optical properties of the tissue as well as on the technique of illumination. As a result of inadequate dosimetry, significant variations in treatment response between patients may be expected.

Animals↗

In vivo photodynamic effects of phthalocyanines in a skin-fold observation chamber model: role of central metal ion and degree of sulfonation.

Six sulfonated metallophthalocyanines, chelated with either aluminum or zinc and sulfonated to different degrees, were studied in vivo for their photodynamic activity in a rat skin-fold chamber model. The chamber, located on the back of female WAG/Rij rats, contained a syngeneic mammary carcinoma implanted into a layer of subcutaneous tissue. Twenty-four hours after intravenous administration of 2.5 mumol/kg of one of the dyes, the chambers received a treatment light dose of 600 J/cm2 with monochromatic light of 675 nm at a power density of 100 mW/cm2. During light delivery and up to a period of 7 days after treatment, vascular effects of tumor and normal tissue were scored. Tumor cell viability was determined by histology and by reimplantation of the chamber contents into the skin of the same animal, either 2 h after treatment or after the 7 day observation period. Vascular effects of both tumor and subcutaneous tissue were strongest with dyes with the lowest degree of sulfonation and decreased with increasing degree of sulfonation. Tumor regrowth did not occur with aluminum phthalocyanine mono- and disulfonate and with zinc phthalocyanine monosulfonate. With the protocol that was used, complete necrosis without recovery was only observed when reimplantation took place at the end of the 7 day follow-up period. Reimplantation 2 h after treatment always resulted in tumor regrowth. At this interval, the presence of viable tumor cells was confirmed histologically. In general tumor tissue vasculature was more susceptible to photodynamic damage than vasculature of the normal tissue. The effect on the circulation of both tumor and normal tissue increased with decreasing degree of sulfonation.(ABSTRACT TRUNCATED AT 250 WORDS)

Animals↗

In vivo fluorescence kinetics of phthalocyanines in a skin-fold observation chamber model: role of central metal ion and degree of sulfonation.

The fluorescence pharmacokinetics of a series of metallosulfophthalocyanines, chelated with either aluminum or zinc and sulfonated to different degrees, was studied by fluorescence measurements in vivo. Dyes were administered systemically to female WAG/RIJ rats with an isogeneic mammary carcinoma transplanted into the subcutis in a transparent observation chamber located on their backs. Following an intravenous injection of 2.5 mumol/kg of the dye, fluorescence dynamics was observed up to 7 h postinjection. The phthalocyanines were excited at 610 nm with a power density of 0.1 mW/cm2 without causing photodynamic damage to the vasculature. Fluorescence was detected above 665 nm using a fluorescence imaging system based on an image intensifier. Dye retention in the blood vessels and tumor tissue was expressed as ratios relative to the fluorescence signal of the surrounding subcutaneous tissue. Phthalocyanines chelated with aluminum gave the highest fluorescence signal with tumor-over-subcutis ratios of up to a value of 4. The zinc complexes exhibited the highest vascular-over-subcutis ratios with maximum values exceeding a value of 6. They also displayed the longest retention times in the vascular system of well over 7 h. Overall, decreasing the degree of sulfonation of the metallophthalocyanines results in lower tumor-over-normal tissue fluorescence ratios, and furthermore aluminum-based dyes seem superior tumor localizers over zinc-based dyes. The advantages of phthalocyanines over porphyrins with respect to tumor localization and photodynamic therapy are discussed.

Animals↗

Optical properties of Intralipid: a phantom medium for light propagation studies.

Intralipid is an intravenous nutrient consisting of an emulsion of phospholipid micelles and water. Because Intralipid is turbid and has no strong absorption bands in the visible region of the electromagnetic spectrum, and is readily available and relatively inexpensive, it is often used as a tissue simulating phantom medium in light dosimetry experiments. In order to assist investigators requiring a controllable medium that over a finite range of wavelengths is optically equivalent to tissue, we have compiled previously published values of the optical interaction coefficients of Intralipid, most of which were measured at a wavelength of 633 nm. We have extended the measurements of the absorption and reduced scattering coefficients from 460 to 690 nm and the total attenuation coefficient from 500 to 890 nm. These measurements show that, for stock 10% Intralipid, the absorption coefficient varies from 0.015 to 0.001 cm-1 between 460 and 690 nm, the reduced scattering coefficient varies from 92 to 50 cm-1 between 460 and 690 nm, the total attenuation coefficient varies from 575 to 150 cm-1 between 500 and 890 nm, and the average cosine of scatter varies from 0.87 to 0.82 between 460 and 690 nm. With these data, we discuss the design of an optically tissue-equivalent phantom consisting of Intralipid and black India ink.

Absorption↗

Tumor and normal tissue response to interstitial photodynamic therapy of the rat R-1 rhabdomyosarcoma.

Interstitial photodynamic therapy (IPDT) using Photofrin II (PII) as photosensitizer has been studied in the rat rhabdomyosarcoma R-1, growing on the thigh or flank of WAG-Rij rats. A light dose-response relationship has been established, for 10 mg PII/kg i.v. and irradiation 24 hr later, with local tumor control as the end point for single IPDT treatments using four cylindrical diffusors simultaneously. A light energy fluence of 150-200 Joule/cm2 (wavelength 625 nm), measured in vivo at the tumor periphery, was required for tumor control. Comparison of tumor response at 5 and 2.5 mg PII/kg with the complete dose response relationship at 10 mg PII/kg suggests drug-light dose reciprocity and indicates that in our tumor model treatment failures are not likely to be caused by variations in (tumor) tissue photosensitizer level, but rather by insufficient light dose or inadequate light dose distribution. Increasing the interval between PII administration and irradiation from 24 hr to 48 hr had no great effect on tumor response to IPDT in this study. Inspection of the original tumor site 100 days after tumor control revealed obvious loss of thigh muscle tissue. Also, recurrent tumors showed a reduced growth rate. Therefore, the relationship between tumor (re)growth and PDT-induced normal tissue damage was studied and the existence of a tumor bed effect was confirmed. The present study indicates that tumor control after a single IPDT treatment is feasible, but that PDT induced damage to a margin of the adjacent normal tissue is probably required.

Animals↗

Whole bladder wall photodynamic therapy with in situ light dosimetry for carcinoma in situ of the bladder.

We report on the preliminary results of 12 patients with multifocal carcinoma in situ of the bladder treated with whole bladder wall photodynamic therapy. The total light dose (scattered plus nonscattered light) measured in situ was 100 joules per cm.2 in the first 6 patients (group 1) and 75 joules per cm.2 in the remaining 6 (group 2). These light doses correspond on the average to 27 joules per cm.2 and 15.5 joules per cm.2 nonscattered light as reported by other investigators. Followup ranged from 6 to 22 months (average 11.5). In group 1, 2 tumors recurred after 6 and 9 months, respectively, and 2 other patients had a permanently shrunken bladder without evidence of disease. In group 2, 1 tumor recurred 5 months after photodynamic therapy. In this group the bladder capacity increased on the average to 135% of the pretreatment value 3 months after photodynamic therapy. All recurrences were in patients with a history of invasive bladder cancer (stages T1 and T2). These preliminary results demonstrate the importance of in situ scattered light dosimetry for minimizing local side effects of whole bladder photodynamic therapy.

Aged↗

Interstitial photodynamic therapy in a rat liver metastasis model.

Photodynamic therapy (PDT) of hepatic tumours has been restricted owing to the preferential retention of photosensitizers in liver tissue. We therefore investigated interstitial tumour illumination as a means of selective PDT. A piece of colon carcinoma CC531 was implanted in the liver of Wag/Rij rats. Photofrin was administered (5 mg kg-1 i.v.) 2 days before laser illumination. Tumours with a mean (+/- s.e.) diameter of 5.7 +/- 0.1 mm (n = 106, 20 days after implantation) were illuminated with 625 nm light, at 200 mW cm-1 from a 0.5 cm cylindrical diffuser and either 100, 200, 400, 800 or 1600 J cm-1. Control groups received either laser illumination only, Photofrin only or diffuser insertion only. Short-term effects were studied on the second day after illumination by light microscopy and computer-assisted integration of the circumference of damaged areas. Long-term effects were studied on day 36. To determine the biochemistry of liver damage and function, serum ASAT and ALAT levels were measured on day 1 and 2, and antipyrine clearance on day 1. Tumour and surrounding liver necrosis increased with light dose delivered (P < 0.001). Best long-term results were obtained at 800 J cm-1 with complete tumour remission in 4 out of 6 animals. No deterioration in liver function was found. The results of this study show the ability of interstitial PDT to cause major destruction of tumour tissue in the liver combined with minimal liver damage.

Adenocarcinoma↗

Treatment system for whole bladder wall photodynamic therapy with in vivo monitoring and control of light dose rate and dose.

A system is described for in vivo monitoring and control of light dose rate and dose during whole bladder photodynamic therapy (PDT). A modified cystoscope admits an isotropic light source (fiber with diffusing tip, connected to a dye laser) and three translucent nylon catheters that are unfolded in three directions along the bladder wall. An isotropic light detector (0.8 mm. diameter probe on 200 microns. fiber) is inserted into each catheter and connected to an amplifier displaying light dose rate (in mW/cm.2) and integrated light dose (in J/cm.2) for each probe. Before treatment a low light level is used to optimize the position of the light source, requiring equal readings by each of the three dosimetry probes. Uniformity of irradiation is checked by moving the probes through their respective catheters along the bladder wall. With red light (wavelength 630 nm.) a dose rate uniformity of +/- 20% could be achieved in vivo in dog bladder. With green light (514.5 nm.) uniform irradiation was difficult, most likely due to a much smaller contribution of scattered light. Measurements during clinical PDT show that optimizing the light source position by suprapubic transvesical ultrasound may not secure uniform irradiation. Half-way into the treatment a difference of 100% between the readings of two probes was noted. Adjusting the position of the light source resulted in integrated light dose variations of less than 20% among the three probes at the end of treatment.

Animals↗

Skin optics.

Quantitative dosimetry in the treatment of skin disorders with (laser) light requires information on propagation of light in the skin related to the optical properties of the individual skin layers. This involves the solution of the integro-differential equation of radiative transfer in a model representing skin geometry, as well as experimental methods to determine the optical properties of each skin layer. These activities are unified under the name skin optics. This paper first reviews the current status of tissue optics, distinguishing between the cases of: dominant absorption, dominant scattering, and scattering about equal to absorption. Then, previously published data as well as some current unpublished data on (human) stratum corneum, epidermis and dermis, have been collected and/or (re)analyzed in terms of absorption coefficient, scattering coefficient, and anisotropy factor of scattering. The results are that the individual skin layers show strongly forward scattering (anisotropy factors between 0.7 and 0.9). The absorption and scattering data show that for all wavelengths considered scattering is much more important than absorption. Under such circumstances, solutions to the transport equation for a multilayer skin model and finite beam laser irradiation are currently not yet available. Hence, any quantitative dosimetry for skin treated with (laser) light is currently lacking.

Absorption↗

Interstitial hyperthermia using 27 MHz wire antennas and interstitial photodynamic therapy in a rat rhabdomyosarcoma: phantom and animal studies.

This paper deals with the interaction of interstitial hyperthermia (HT) and interstitial photodynamic therapy (PDT). Its main focus, however, is on a newly developed heating system; phantom studies as well as temperature-response data obtained from the in vivo experiments are presented. Heat was delivered by thin, flexible wire antennas operating at a frequency of 27 MHz. Measurements in muscle-equivalent phantom with infrared thermography were performed. Uniform heating over the inserted length of the antenna was obtained and impedance matching appears possible by simple variable air coils, thereby minimizing the reflected power to less than 20%. Light was obtained from an Argon-Dye laser system tuned to a wavelength of 625 nm at a dose rate of 75-100 mW per fiber to a total incident dose of 900 J from four linear light applicators. An experimental murine tumor (Rhabdomyosarcoma, type R-1) was transplanted in WAG/Rij rats and, after reaching an average diameter of 2 cm, the active component of haematoporphyrin derivative (HPD), Photofrin II, was injected intravenously. The tumors were subsequently implanted with four flexible catheters, through which either light or heat could be applied. Dose-response relationships for PDT alone, HT alone and PDT followed by HT were established with cure as endpoint. The animal experiments showed that with the use of low-frequency wires a good localized heat distribution in the tumors can be obtained. Moreover, this study showed that PDT and HT, in the proper sequence and only when optimal temperatures are reached, result in an augmented cytotoxicity on the tumor cells in vivo; i.e. a cure rate of 41% was obtained.

Animals↗

Interaction of interstitial photodynamic therapy and interstitial hyperthermia in a rat rhabdomyosarcoma--a pilot study.

Photodynamic therapy (PDT) involves the activation of photosensitizing drugs by light of appropriate wavelength. The photosensitive agent Hematoporphyrin Derivative (HPD) appears to be preferentially retained in malignant tumors; irradiation of HPD-containing tissue by light of appropriate wavelength (625 nm) and dose leads to (tumor) tissue destruction. The aim of this study is to achieve maximum tumor control probability with minimum normal tissue photosensitivity. In previous work from our laboratory it has been demonstrated that PDT has its fundamental effects on the tumor and normal tissue microcirculation. As it is well established that hyperthermia (HT) has its major effects in less well vascularized areas of the tumor, the combined modality of HT and PDT might prove to be advantageous. Moreover, suppression of sublethal damage repair by HT has been observed. To overcome the problem of poor light penetration into tissues and the high rate of recurrences following PDT with external irradiation, the combined effects of interstitial PDT with interstitial hyperthermia in a new line of animal experiments were studied in our laboratory. An experimental murine tumor (Rhabdomyosarcoma, type R-1) was transplanted in WAG/Rij rats and, after reaching an average diameter of 2 cm, the active component of HPD, that is Photofrin II, was injected intravenously in different dose schedules (5 mg/kg, 10 mg/kg). After 24 or 48 hrs the tumors were implanted with four flexible catheters, through which either light or heat could be applied. Light was obtained from an Argon-Dye laser system tuned to a wavelength of 625 nm at a dose rate of 75-100 mW per fiber to a dose level of 900 Joule from four linear light applicators. Heat (44 degrees C/30') was delivered by four 27 MHz radiofrequency antennas. Dose response relationships for PDT alone, HT alone and PDT combined with HT were established with cure as endpoint. This study showed that these two modalities, in the proper sequence and spacing, result in an augmented cytotoxicity on the tumor cells in vivo. With the combined modality treatment a cure rate of 41% (90 days) was obtained. As the implantation of flexible catheters is a well-known technique in radiation therapy practice, the potentiating effects of interstitial HT combined with interstitial PDT in solid tumors is very promising and clinical studies are warranted.

Animals↗