Effect of porcine placental extract on the mild menopausal symptoms of climacteric women.

OBJECTIVES: This study assessed the effects of oral porcine placental extract (PPE) on the mild menopausal symptoms of climacteric women. METHODS: In this 12-week, multicenter, randomized, double-blind, placebo-controlled, parallel-group study, 50 climacteric Japanese women were randomized 1 : 1 to oral PPE (300 mg/day) or placebo. Menopausal symptoms were evaluated by using the Simplified Menopausal Index (SMI), as were serum estradiol (E2) and follicle stimulating hormone (FSH) levels. Blood biochemical and cellular and urinary tests were done to evaluate safety aspects of repeated oral administration of PPE. RESULTS: The total SMI score of the PPE group was significantly more improved after 12 weeks than that of the placebo group (p = 0.031). This score and three subscores (vasomotor, psychological, and somatic symptoms) were significantly improved at 8 and/or 12 weeks compared with the initial values in the PPE group (p < 0.05). E2 and FSH levels were not improved in either group. No adverse events were observed. CONCLUSIONS: Oral PPE at 300 mg/day improved the mild menopausal symptoms of climacteric women. Since oral PPE did not improve serum E2 and FSH levels, PPE is thought not to ameliorate hormonal balance itself but to improve subjective feelings of climacteric women.

Electron-phonon superconductivity in C-doped topological nodal-line semimetal Zr5Pt3: a muon spin rotation and relaxation (µSR) study.

In the present work, we demonstrate that C-doped Zr5Pt3is an electron-phonon superconductor (with critical temperatureTC= 3.8 K) with a nonsymmorphic topological Dirac nodal-line semimetal state, which we report here for the first time. The superconducting properties of Zr5Pt3C0.5have been investigated by means of magnetization, resistivity, specific heat, and muon spin rotation and relaxation (µSR) measurements. We find that at low temperatures, the depolarization rate is almost constant and it can be well described by a single-bands-wave model with a superconducting gap of 2Δ(0)/kBTC= 3.84, somewhat higher than the value of BCS theory. From the transverse field µSR analysis, we estimate the London penetration depthλL= 469 nm, superconducting carrier densityns= 1.83 × 1026 m-3, and effective massm* = 1.428me. The zero field µSR confirms the absence of any spontaneous magnetic field in the superconducting ground state. In order to gain additional insights into the electronic ground state of C-doped Zr5Pt3, we also performed first-principles calculations within the framework of density functional theory (DFT). The observed homogenous electronic character of the Fermi surface as well as the mutual decrease ofTCand density of states at the Fermi level are consistent with the experimental findings of this study. However, the band structure reveals the presence of robust, gapless fourfold-degenerate nodal lines protected by 63screw rotations and glide mirror planes. Therefore, Zr5Pt3represents a novel, unprecedented condensed matter system to investigate the intricate interplay between superconductivity and topology.

Role of the dipolar interaction on the macroscopic state of magnetic nanoparticle systems: a Monte Carlo study.

We have performed Monte Carlo simulations to treat the effect of the dipolar interaction in assemblies of superparamagnetic nanoparticles. Our simulations reproduce correctly the increase of the blocking temperature (T(B)) as the concentration increases, as observed experimentally. Interestingly, we have observed a progressive displacement of the M2 versus H/M isotherms (Arrott plots) from the origin as the concentration of nanoparticles increases. Moreover, the curvature of the isotherms at T > T(B) changes from positive to negative slope at high sample concentrations, resembling the shape of a first order phase transition. These results are surprisingly similar to that found in a conventional magnetic phase transition under the effect of a random anisotropy or a random field.

Evaluation of PHITS for microdosimetry in BNCT to support radiobiological research.

The aim of this paper is to validate the microdosimetric functionality of the Monte Carlo code, PHITS, and verify its use for estimating dose and RBE for radiobiological studies performed at Kyoto University Institute for Integrated Radiation and Nuclear Science (KURNS). Lineal energy spectra produced by the KUR mixed irradiation mode were measured with a tissue equivalent proportional counter (TEPC) place in free air. The Monte Carlo calculation showed a good agreement with the measured data. In the second part of the study, a realistic set-up of a typical in-vivo radiobiological experiment was simulated with PHITS and the simulation results were compared against TLD and gold foil activation measurements. The Monte Carlo simulation results and the measured data showed an agreement within 3%. The calculated RBE also showed a close value to clinically utilised values. This study shows that PHITS can be utilised to evaluate thermal neutron fluxes and gamma ray absorbed dose rates inside a tumour like medium.

Source identification and concentration distribution of polychlorinated biphenyls in environmental media around industrial complexes.

In order to grasp the concentration distribution and identify sources of PCBs, air and soil samples around Sihwa and Banwol industrial area in Korea were analyzed. In result, the polychlorinated biphenyls (PCBs) concentration of air and soil was ranged from 2.08 to 5.82 ng/m3 (0.0686­1.01 pg WHO-TEQ/m3) and 2.43 to 274 ng/g dry (0.116­60.5 pg WHO-TEQ/g dry), respectively. Air and soil samples showed the very similar isomer composition pattern in each homologue by matrix, respectively. As a result of MLR for soil samples, the whole contribution rate of PCBs products (Aroclor) to soil was ~2 times higher than combustion.

Note: Development of real-time epithermal neutron detector for boron neutron capture therapy.

The real-time detection of epithermal neutrons forms an important aspect of boron neutron capture therapy. In this context, we developed an epithermal neutron detector based on the combination of a small Eu:LiCaAlF6 scintillator and a quartz fiber in order to fulfill the irradiation-field requirements for boron neutron capture therapy. The irradiation test is performed with the use of a reactor-based neutron source. The thermal and epithermal neutron sensitivities of our epithermal neutron detector are estimated to be 9.52 × 10-8 ± 1.59 × 10-8 cm2 and 1.20 × 10-6 cm2 ± 8.96 × 10-9 cm2, respectively. We also subject the developed epithermal neutron detector to actual irradiation fields, and we confirm that the epithermal neutron flux can be measured in realtime.

Histological analysis of the effect of hyperthermia on normal rabbit hepatic vasculature.

The effects of hyperthermia on rabbit hepatic vasculature were studied histologically. To investigate heat-induced vascular damage in the central veins, portal veins, and hepatic arterioles, the left lobes of rabbit liver were heated locally for 30 min in the range of 40-46 degrees C. Hyperthermia was induced by an 8-MHz radiofrequency current heating device using a needle type interstitial applicator. This device allowed application of heat to a central area of 10 x 10 mm no more than 1 degree C below the preset temperature. Within the area of 1 cm2, the percentage of damaged (ruptured or thrombosed) vessels was estimated for each type of hepatic vasculature. Vascular damage following hyperthermia continued up to 24 h after heating for the three types of hepatic vasculature. Central veins were the most thermosensitive followed by portal veins, whereas hepatic arterioles were the most thermoresistant. The temperature causing 50% vascular damage 24 h after heating was 41.5-42.5 degrees C, 42.5-43.5 degrees C, and 44-45 degrees C for central veins, portal veins, and arterioles, respectively. This differential thermal responsiveness of hepatic vasculature may be attributed to the histological structure of the vessels.

Improvement of depth dose distribution using multiple-field irradiation in boron neutron capture therapy.

It is important that improvements are made to depth dose distribution in boron neutron capture therapy, because the neutrons do not reach the innermost regions of the human body. Here, we evaluated the dose distribution obtained using multiple-field irradiation in simulation. From a dose volume histogram analysis, it was found that the mean and minimum tumor doses were increased using two-field irradiation, because of improved dose distribution for deeper-sited tumors.

Radiobiological characteristics of solid tumours depending on the p53 status of the tumour cells, with emphasis on the response of intratumour quiescent cells.

Human head and neck squamous cell carcinoma cells transfected with mutant TP53 (SAS/mTP53) or with a neo vector as a control (SAS/neo) were inoculated subcutaneously (s.c.) into both hind legs of Balb/cA nude mice. Mice bearing tumours received 5-bromo-2'-deoxyuridine (BrdU) continuously to label all proliferating (P) cells in the tumours. The mice then received gamma-ray irradiation. Another group of mice received a series of test doses of gamma-rays while alive or after tumour clamping to obtain hypoxic fractions (HFs) in the tumours. Right after irradiation, the tumour cells were isolated and incubated with a cytokinesis blocker. The micronucleus (MN) frequency in the cells without BrdU labelling (=quiescent (Q) cells) was determined using immunofluorescence staining for BrdU. Meanwhile, 6 h after irradiation, tumour cell suspensions obtained in the same manner were used for determining the frequency of apoptosis in the Q cells. The MN frequency and apoptosis frequency in total (P+Q) tumour cells were determined from the tumours that were not pretreated with BrdU. In total cell populations, SAS/mTP53 cells were more radioresistant than SAS/neo cells in clonogenic survival. Q tumour cells exhibited a significantly lower apoptosis and MN frequency, probably due to their much larger HF, than total cells. In both total and Q cell fractions, SAS/mTP53 cells were less susceptible to apoptosis and more susceptible to micronucleation than SAS/neo cells. Obviously, TP53 status had the potential to influence the radiosensitivity of not only the total cells, but also the Q cells. However, irrespective of the TP53 status, significant differences in radiosensitivity between total and Q tumour cells were consistently observed. From the viewpoint of tumour control as a whole, including intratumour Q tumour cell control, a treatment modality for enhancing the Q cell response has to be considered.

Enhancement of the therapeutic outcome of radio-immunotherapy by combination with whole-body mild hyperthermia.

To enhance the effect of radio-immunotherapy for solid cancers, whole-body mild hyperthermia was added, and its effects on the pharmacokinetics of radiolabelled antibody, outcome of radio-immunotherapy, and radiosensitivity of the tumour were investigated. Nude mice bearing human colon cancer xenografts were heated to 40 degrees C for 3 or 6 h. After heating, mice received intravenous (i.v.) injections of [131I]-labelled anti-carcinoembryonic antigen (CEA) monoclonal antibody. Although 6-h heating did not alter the biodistribution of the radiolabelled antibody, and alone did not show any therapeutic effect on tumour growth, when combined with radio-immunotherapy, the therapeutic effect on tumour growth was significantly enhanced. Three-hour heating also significantly enhanced the effect of radio-immunotherapy. Colony formation assay showed that the radiosensitivity of the tumour was significantly enhanced after heating, which was achieved by a reduction of the hypoxic fraction of the tumour. In conclusion, the addition of whole-body mild hyperthermia significantly enhanced the therapeutic effect of radio-immunotherapy by increasing the radiosensitivity of the tumour.

Potentially lethal damage repair by quiescent cells in murine solid tumors.

We investigated potentially lethal damage repair by quiescent tumor cells in vivo. SCC VII tumor-bearing C3H/He mice were irradiated after being given 10 injections of 5-bromo-2'-deoxyuridine (BUdR) to label all the proliferating cells in their tumors, and the tumors were then excised and trypsinized. The tumor cell suspensions thus obtained were incubated with cytochalasin-B (Cyt-B, a cytokinesis blocker), and the micronucleus frequency in cells without BUdR labelling was determined using immunofluorescence staining to BUdR. The micronucleus frequency was then used to determine the surviving fraction of unlabelled cells on the basis of the regression line obtained for the micronucleus frequency and the surviving fraction of all tumor cells not labeled by BUdR, which can be regarded as the quiescent cells in a tumor for all practical purposes. Assessment performed 0, 3, 6, 9, and 24 hr after irradiation showed that quiescent cells had more potentially lethal damage repair capacity than the tumor cell population as a whole. Assays were also performed immediately after irradiation alone, 24 hr after the injection of cis-diamminedichloroplatinum(II) (CDDP), mitomycin C (MMC), or misonidazole [1-(2-nitro-1-imidazolyl)-3-methoxy-2-propanol] (MISO) following irradiation, and 24 hr after irradiation alone. It was found that CDDP and MISO (especially the latter) inhibited potentially lethal damage repair more strongly in quiescent cells than in the tumor cell population as a whole. This assay method thus appears to be quite useful for detecting the responses of quiescent tumor cells to various chemical agents.

Middle dose rate irradiation in combination with carbogen inhalation selectively and more markedly increases the responses of SCCVII tumors.

PURPOSE: Carbogen increases the radiation response of tumors and reduced dose rate irradiation spares the damage of normal tissues. The purpose in this paper is to investigate the possibility of selective radiosensitization of tumors by reduced dose rate irradiation in combination with carbogen inhalation. METHODS AND MATERIALS: SCCVII tumors in C3H/He mice were irradiated at middle dose rate (0.1 Gy/min) or high dose rate irradiation (3.0 Gy/min) in combination with carbogen inhalation. The mice were enclosed in a box with carbogen flushing at 1.01/min. The tumor response was measured by a cytokinesis block micronucleus assay. The effects on intestinal crypt cells and bone marrow cells were investigated by microcolony assay or Hendry's method, respectively. RESULTS: The anti-tumor effect of middle dose rate irradiation was equal to that of a high dose rate irradiation. Carbogen inhalation, more efficiently, increased the antitumor effect when combined with middle and high dose rate irradiation, and yielded enhancement ratios of 1.6 at around 2 Gy. Middle dose rate irradiation produced less damage on intestinal crypt cells and bone marrow cells in comparison with high dose rate irradiation, and carbogen inhalation never enhanced the responses of these normal tissues in combination with middle dose rate irradiation. Dose modifying factors were 1.3-2.0. CONCLUSION: Since middle dose rate irradiation in combination with carbogen inhalation gave the therapeutic gain factors of 2.0-3.2, which were much larger than those obtained with any other radiosensitizers, this combination has a potential as a new modality for improving the results of cancer radiotherapy.

Electroporation increases the effect of borocaptate (10B-BSH) in neutron capture therapy.

PURPOSE: The cell membrane permeability of borocaptate (10B-BSH) and its extent of accumulation in cells are controversial. This study was performed to elucidate these points. METHODS AND MATERIALS: Two different treatments were applied to SCCVII tumor cells. The first group of tumor cells was incubated in culture medium with 10B-BSH or 10B-enriched boric acid, and was exposed to neutrons from the heavy water facility of the Kyoto University Reactor (KUR). More than 99% of neutrons were thermal neutrons at flux base. The second group was pretreated by electroporation in combination with 10B-BSH, and thereafter the cells were irradiated with neutrons. The cell killing effects of boron neutron capture therapy (BNCT) using BSH were investigated by colony formation assay. RESULTS: Surviving cell fraction decreased exponentially with neutron fluence, and addition of BSH significantly enhanced the cell killing effect of neutron capture therapy (NCT) depending on 10B concentration. The effect of BSH-BNCT also increased with preincubation time of cells in the medium containing BSH. The electroporation of cells with BSH at 10 ppm 10B markedly enhanced BSH-BNCT effects in comparison with that of preincubation alone. The effect of BSH-BNCT with electroporation was equal to that of BNCT using 10B-boric acid at a same 10B concentration (10 ppm). CONCLUSIONS: BSH is suggested to penetrate the cells slowly and remained after washing. Electroporation can introduce BSH into the cells very efficiently, and BSH stays in the cells and is not lost by washing. Therefore, if electroporation is applied to tumors after BSH injection, 10B remains in tumors but is cleared from normal tissues, and selective accumulation of 10B in tumors will be achieved after an adequate waiting time.

Hyperthermia enhances thermal-neutron-induced cell death of human glioblastoma cell lines at low concentrations of 10B.

PURPOSE: To examine the ability of pre- vs. post-irradiation hyperthermia to enhance the effectiveness of thermal neutrons to kill human glioblastoma cells. METHODS AND MATERIALS: Human glioblastoma cell lines, T98G, A7, A172, and U 87MG, were exposed to thermal neutrons from the Kyoto University Research (KUR) reactor or to 60Co gamma-rays. Hyperthermia was tested before and after irradiation of T98G (44 degrees C, 15 min) and A7 cells (44 degrees C, 40 min), and with different concentrations (0-30 ppm) of 10B-boric acid. The biological end point of all experiments was cell survival measured by a colony formation assay. RESULTS: The relative biological effectiveness (RBE) values of thermal neutrons for these cell lines compared with 60Co gamma-rays were 1.8-2.0 at their D(0) values. When T98G and A7 cells were heated after thermal neutron irradiation, there was a synergistic effect at low 10B concentrations (up to 5 ppm for T98G and up to 10 ppm for A7 cells). With high concentrations of boron (10-30 ppm for T98G and 20-30 ppm for A7 cells), hyperthermia and neutron irradiation interact additively rather than synergistically. There was no enhancement when cells were heated before thermal neutron irradiation. These results suggest that the radiosensitizing effect of hyperthermia may be attributed to partial inhibition of the repair of the potentially lethal damage caused by neutron irradiation.

Radiobiologic significance of apoptosis and micronucleation in quiescent cells within solid tumors following gamma-ray irradiation.

PURPOSE: To determine the frequency of apoptosis in quiescent (Q) cells within solid tumors following gamma-ray irradiation, using four different tumor cell lines. In addition, to assess the significance of detecting apoptosis in these cell lines. METHODS AND MATERIALS: C3H/He mice bearing SCC VII or FM3A tumors, Balb/c mice bearing EMT6/KU tumors, and C57BL mice bearing EL4 tumors received 5-bromo-2'-deoxyuridine (BrdU) continuously for 5 days via implanted mini-osmotic pumps to label all proliferating (P) cells. The mice then received gamma-ray irradiation at a dose of 4--25 Gy while alive or after tumor clamping. Immediately after irradiation, the tumors were excised, minced, and trypsinized. The tumor cell suspensions thus obtained were incubated with cytochalasin-B (a cytokinesis blocker), and the micronucleus (MN) frequency in cells without BrdU labeling (= Q cells) was determined using immunofluorescence staining for BrdU. Meanwhile, 6 hours after irradiation, tumor cell suspensions obtained in the same manner were fixed. The apoptosis frequency in Q cells was also determined with immunofluorescence staining for BrdU. The MN and apoptosis frequency in total (P + Q) tumor cells were determined from the tumors that were not pretreated with BrdU. RESULTS: In total cells, SCC VII, FM3A, and EMT6/KU cells showed reasonable relationships between MN frequency and surviving fraction (SF). However, fewer micronuclei were induced in EL4 cells than the other cell lines. In contrast, a comparatively close relationship between apoptosis frequency and SF was found in total cells of EL4 cell line. Less apoptosis was observed in the other cell lines. Quiescent tumor cells exhibited significantly lower values of MN and apoptosis frequency probably due to their large hypoxic fraction, similar to total tumor cells on clamped irradiation. CONCLUSION: gamma-ray irradiation induced MN formation in SCC VII, FM3A, and EMT6/KU tumor cells, and the apoptosis was marked in EL4 cells compared with the other cell lines. Our method for detecting the Q cell response to gamma-ray irradiation using P cell labeling with BrdU and the MN frequency assay was also applicable to apoptosis detection assay.

Dimethyl sulfoxide protects against thermal and epithermal neutron-induced cell death and mutagenesis of Chinese hamster ovary (CHO) cells.

PURPOSE: To investigate the protective effects of dimethyl sulfoxide (DMSO) on cell killing and mutagenicity at the HPRT locus in Chinese hamster ovary (CHO) cells against thermal and epithermal neutrons produced at the Kyoto University Research (KUR) reactor. METHODS AND MATERIALS: DMSO was added to cells 15 min before irradiation and removed 15 min after irradiation. Cells were irradiated by thermal and epithermal neutrons with or without boron at 10 ppm. The biological endpoint of cell survival was measured by colony formation assay. The mutagenicity was measured by the mutant frequency in the HPRT locus. A total of 378 independent neutron-induced mutant clones were isolated in separate experiments. The molecular structure of HPRT mutations was determined by analysis by multiplex polymerase chain reaction of all nine exons. RESULTS: The D(0) values of epithermal and thermal neutrons in three different modes, i.e., thermal, epithermal, and mixtures of thermal and epithermal, were 0.8-1.2 Gy. When cells were treated with DMSO, the D(0) values increased to 1.0-2.3, especially in the absence of boron. DMSO showed a protective effect against mutagenesis of the HPRT locus induced by epithermal and thermal neutron irradiation. After DMSO treatment, the mutagenicity was decreased, especially when the cells were irradiated in epithermal neutron mode. Molecular structure analysis indicated that total and partial deletions were dominant and the incidence of total deletions was increased in the presence of boron in the thermal neutron and mixed modes. In the epithermal neutron mode, more than half of the mutations were total deletions. When cells were treated with DMSO, the incidence of total deletions by thermal neutron irradiation with boron and epithermal irradiation decreased. CONCLUSIONS: Our results suggest that DMSO has various protective effects against cytotoxic and mutagenic effects of thermal and epithermal neutrons, and that the extent of protection is reflected by the percentage of absorbed dose distribution for each neutron irradiation mode.

Hyperthermia combined with radiation therapy for primarily unresectable and recurrent colorectal cancer.

The value of adjuvant hyperthermia to radiotherapy in the treatment of locally advanced colorectal cancers was investigated. Between 1981 and 1989, 71 primarily unresectable or recurrent colorectal tumors were treated with radiotherapy at the Department of Radiology, Kyoto University Hospital. Of the 71 tumors, 35 were treated with radiotherapy plus hyperthermia (group I), while 36 tumors (group II) were unsuitable for hyperthermia mainly because of difficulties with the insertion of temperature probes or the thickness of the patient's subcutaneous fat (greater than 2 cm). The mean total radiation dose was 58 Gy and 57 Gy for groups I and II, respectively. Thirty deep-seated pelvic tumors were treated with an 8 MHz radiofrequency capacitive heating device, and five subsurface tumors were treated with a 430 MHz microwave hyperthermia system. Hyperthermia was given following radiotherapy for 30-60 min for a total of 2-14 sessions (mean 5.7). In 32 of the 35 tumors heated, direct measurement of tumor temperature was performed. For the five tumors treated with the microwave heating device, the means of the mean maximum, average, and minimum measured intratumoral temperatures were 45.4 degrees C, 43.3 degrees C, and 40.6 degrees C, respectively. The corresponding values were 42.2 degrees C, 41.3 degrees C, and 40.3 degrees C for the 27 tumors treated with the capacitive heating device. Effective heating of deep-seated pelvic tumors was more difficult than heating of abdominal wall or perineal tumors. The local control rate at 6 months after the treatment, which was defined as absence of local progression of the tumors, was 59% (17/29) and 37% (11/30) for groups I and II, respectively. The objective tumor response rate (complete regression plus partial response) evaluated by computed tomography was 54% (19/35) in group I, whereas it was 36% (10/28) in group II. A better response rate of 67% was obtained in the 15 tumors with a mean average tumor temperature of greater than 42 degrees C. Although limitation of our current heating devices exist, the combination of hyperthermia with radiotherapy is a promising treatment modality in the treatment of locally advanced colorectal cancer.

Alteration of sensitivity of intratumor quiescent and total cells to gamma-rays following thermal neutron irradiation with or without 10B-compound.

PURPOSE: Changes in the sensitivity of intratumor quiescent (Q) and total cells to gamma-rays following thermal neutron irradiation with or without 10B-compound were examined. METHODS AND MATERIALS: 5-Bromo-2'-deoxyuridine (BrdU) was injected to SCC VII tumor-bearing mice intraperitoneally 10 times to label all the proliferating (P) tumor cells. As priming irradiation, thermal neutrons alone or thermal neutrons with 10B-labeled sodium borocaptate (BSH) or dl-p-boronophenylalanine (BPA) were administered. The tumor-bearing mice then received a series of gamma-ray radiation doses, 0 through 24 h after the priming irradiation. During this period, no BrdU was administered. Immediately after the second irradiation, the tumors were excised, minced, and trypsinized. Following incubation of tumor cells with cytokinesis blocker, the micronucleus (MN) frequency in cells without BrdU labeling (= Q cells at the time of priming irradiation) was determined using immunofluorescence staining for BrdU. The MN frequency in the total (P + Q) tumor cells was determined from the tumors that were not pretreated with BrdU before the priming irradiation. To determine the BrdU-labeled cell ratios in the tumors at the time of the second irradiation, each group also included mice that were continuously administered BrdU until just before the second irradiation using mini-osmotic pumps which had been implanted subcutaneously 5 days before the priming irradiation. RESULTS: In total cells, during the interval between the two irradiations, the tumor sensitivity to gamma-rays relative to that immediately after priming irradiation decreased with the priming irradiation ranking in the following order: thermal neutrons only > thermal neutrons with BSH > thermal neutrons with BPA. In contrast, in Q cells, during that time the sensitivity increased in the following order: thermal neutrons only < thermal neutrons with BSH < thermal neutrons with BPA. The longer the interval between the two irradiations, the higher was the BrdU-labeled cell ratio at the second irradiation. The labeled cell ratio at the same time point after each priming irradiation increased in the following order: thermal neutrons only < thermal neutrons with BSH < thermal neutrons with BPA. CONCLUSION: These findings indicated that the use of 10B-compound, especially BPA, in thermal neutron irradiation causes the recruitment from the Q to P population.

The combined effect of boronophenylalanine and borocaptate in boron neutron capture therapy for SCCVII tumors in mice.

PURPOSE: To increase the effect of boron neutron capture therapy (BNCT) on tumors in vivo, the combined effects of para-boronophenylalanine (BPA) and borocaptate sodium (BSH) were investigated. METHODS AND MATERIALS: 10B-enriched BPA and BSH were administered to C3H/He mice bearing SCCVII tumors by intragastric and intravenous injections, respectively. The colony formation and tumor control assays were employed for investigating antitumor effects of BNCT. The extent of homogeneity of tumor cell killing effect was examined by the distribution of frequencies of binuclear cells (BNC) producing a certain number of micronuclei (0,1,2,--,> or =5) to total number of BNC and by the comparison between surviving cell fraction (SF) in colony formation assay and the normal nuclear division fraction (NNDF) at first mitosis following BNCT. RESULTS: The relationships between SF and radiation dose in Gy (D) at around 10 ppm of 10B in tumors were as follow: -InSF = -0.101 + 0.648 Gy(-1) x D, 0.0606+0.435 Gy(-1) x D, and -0.0155 + 0.342 Gy(-1) x D for BPA, BPA + BSH, and BSH, respectively. In tumor control assay, BPA was also more effective than BSH, but the difference of effectiveness significantly decreased: 1.9 times more effective in colony assay vs. 1.2 times in tumor control assay. The most effective treatment to achieve tumor cure was BNCT using BPA + BSH, and it was 1.9 times more effective than BSH-BNCT. In BSH-BNCT, NNDF decreased exponentially with radiation dose and was equal to SF. However, NNDF following BPA-BNCT showed a biphasic decrease with radiation dose, and SF was much lower than NNDF. In the combination of BPA and BSH, the discrepancy between NNDF and SF decreased in comparison with BPA-BNCT. The distribution of frequency of BNC with a certain number of micronuclei to total BNC was very close to Poisson distribution in BSH-BNCT tumors; however, it deviated from the Poisson in BPA-BNCT tumors. In combination with BPA and BSH, the distribution showed an intermediate pattern. These findings indicate that BSH distributes homogeneously with a heterogeneous distribution of BPA in tumors, and the heterogeneous effect of BPA-BNCT was improved by the combination of two boron compounds. CONCLUSION: The heterogeneous cell killing effect of BPA-BNCT was improved by the combination of BSH, and increased tumor control rates. Therefore, this combination may improve clinical outcome of BNCT although the effects on normal tissues have to be examined before clinical application.

Radiobiological evidence suggesting heterogeneous microdistribution of boron compounds in tumors: its relation to quiescent cell population and tumor cure in neutron capture therapy.

PURPOSE: The heterogeneous microdistribution of boron compounds in tumors and its significance on tumor cure were examined by a radiobiological procedure. The role of quiescent (Q) cells in tumor was especially investigated. METHODS AND MATERIALS: 10B-enriched paraboronophenylalanine (BPA) and mercaptoundecahydrododecaborate (BSH) were administered to SCCVII tumor bearing C3H/He mice by intragastric and i.v. injections, respectively. The continued effects of these boron compounds with thermal irradiations were studied by using colony formation and tumor control assays. Their effects on Q cells were also analyzed by the combined method of micronucleus frequency assay and an identification of proliferating (P) cells by BUdR and anti-BUdR monoclonal antibody. RESULTS: 10B-concentration after BPA (1,500 mg/kg) and BSH (75 mg/kg) administration were 11 ppm at 3 h and 10.5 ppm at 30 min, respectively. Cell survival decreased exponentially with an increment of neutron fluence (phi). The exponential parts of the curves were: -InSF = -0.052+ 13.0x10(13)phi, -InSF = -0.032+7.68X10(-13)phi, and -InSF = -0.0005+2.68x10(-13)phi for BPA-BNCT, BSH-BNCT, and NCT alone, respectively. Fifty percent tumor control was obtained at the influence of 10.2 x 10(12) n/cm2 in BPA-BNCT. On the other hand, 11.4 x 10(12) n/cm2 of neutrons had to be delivered in BSH-BNCT. The normal nuclear division fraction defined as the cell fraction that did not express micronuclei at first mitosis after treatment was investigated. The surviving cell fraction and the normal nuclear division fraction were regarded as equal in NCT alone. However, the normal nuclear division factor following BPA-BNCT was greater than the surviving cell fraction, and the difference increased with an increase in neutron fluence. In Q cells, BSH-BNCT yielded higher micronucleus frequency than BPA-BNCT and NCT alone. The frequencies in Q cells following BPA-BNCT and NCT alone were almost same as that in total cell population after NCT alone. CONCLUSIONS: Our data suggested that BPA distributed in tumors hetergeneously. Q cells especially might not accumulate BPA. To decrease the possible disadvantage of BPA-BNCT, the combination of BPA and BSH or other neutron capture element that emit particles with longer ranges, for example, gadolinium, would have to be investigated.