The paper deals with the recent improvements introduced in the most usual method applied in the Institut Gustave Roussy radiotherapy department for obtaining the anatomical data of patients treated ...for head and neck tumors. For each of these patients, five to seven transverses slices and a lateral radiographic film are taken from a Mecaserto simulator-CT. The anatomical representation of the patient sagittal plane is carried out from the digitalisation of the radiographic film on a Vidar Vxr-12 Plus film scanner and integrated into the Dosigray dose calculation programme in order to be used as a support for the laying out of the dose distribution in reference to the treatment. The sagittal anatomical representation obtained from the radiographic film digitalisation is compared with the one resulting from the interpolation between a limited number of irregularly-spaced transverse slices taken on the simulator-CT. The method using the simulator-scanner transverse slices and the radiographic film digitalisation represents an interesting alternative for obtaining an anatomy simulation representative of the patient in hospitals where a scanner is not available full-time for the needs of the radiotherapy process.
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GEOZS, IJS, IMTLJ, KILJ, KISLJ, NUK, OILJ, PNG, SAZU, SBCE, SBJE, UL, UM, UPCLJ, UPUK
A study of identification properties of a Si-Si DE-E telescope exploiting an underdepleted residual-energy detector has been performed. Five different bias voltages have been used, one corresponding ...to full depletion, the others associated with a depleted layer ranging from 90% to 60% of the detector thickness. Fragment identification has been performed using either the DE-E technique or Pulse Shape Analysis (PSA). Both detectors are reverse mounted: particles enter from the low field side, to enhance the PSA performance. The achieved charge and mass resolution has been quantitatively expressed using a Figure of Merit (FoM). Charge collection efficiency has been evaluated and the possibility of energy calibration corrections has been considered. We find that the DE-E performance is not affected by incomplete depletion even when only 60% of the wafer is depleted. Isotopic separation capability improves at lower bias voltages with respect to full depletion, though charge identification thresholds are higher than at full depletion. Good isotopic identification via PSA has been obtained from a partially depleted detector whose doping uniformity is not good enough for isotopic identification at full depletion.
The novel, potential anxiolytic, S 15535 (4-(benzodioxan-5-yl)1-(indan-2-yl)piperazine), is an agonist and antagonist (weak partial agonist) at pre- and postsynaptic serotonin (5-HT)1A receptors, ...respectively. Herein, we characterized its influence on dialysate levels of 5-HT, dopamine (DA) and NAD simultaneously determined in single samples of the frontal cortex (FCX) of freely moving rats, and compared its activity in several other models of potential antidepressant (AD) properties with those of the 5-HT reuptake inhibitor (SSRI), fluoxetine. S 15535 displayed high affinity at cloned human (h) 5-HT1A receptors (Ki = 0.7 nM) and >250-fold lower affinity at cloned hD2 (400 nM), hD3 (248 nM) and h alpha2A-adrenergic (AR) (190 nM) receptors. S 15535 (0.08-5.0 mg/kg s.c.) markedly and dose-dependently suppressed dialysate levels of 5-HT in the FCX, nucleus accumbens and striatum of freely moving rats, whereas fluoxetine (10.0 mg/kg s.c.) elevated levels of 5-HT in each structure. In contrast to 5-HT, dialysate levels of DA and NAD in the FCX were dose-dependently increased by S 15535, and this effect was mimicked by fluoxetine. The influence of S 15535 and fluoxetine on FCX levels of DA was regionally specific inasmuch as dialysate levels of DA in the accumbens and striatum were not modified. The selective 5-HT1A antagonist, WAY 100,635 (N-2-4-(2-methoxyphenyl)-1-piperazinylethyl-N-(2-pyridinyl) cyclohexanecarboxamide (0.16) transiently elicited a slight increase in cortical levels of 5-HT, an action opposite to that of S 15535. Further, in the presence of WAY 100,635 (0.16), the influence of S 15535 (0.63) on cortical levels of 5-HT, DA and NAD was markedly attenuated. Upon chronic administration of S 15535 or fluoxetine (10.0 mg/kg s.c. daily for 14 days, in each case), there was no significant alteration in the density of beta-AR receptors in the FCX. However, in contrast to fluoxetine, S 15535 elicited a significant (25%) decrease in the density (Bmax) of 5-HT2A receptors labeled by 3Hketanserin in the cortex; there was no alteration in Kd. In a learned helplessness paradigm in rats, S 15535 (0.63-40.0 mg/kg p.o.) markedly reduced escape deficits on each of three consecutive days of testing. Fluoxetine (2.0-8.0 mg/kg i.p.) was also active in each session, but presented a biphasic dose-response curve. Finally, under the conditions used, neither S 15535 (0.63-10.0) nor fluoxetine (0.63-10.0) decreased immobility time in the forced swim test. In conclusion, S 15535 is a selective ligand of cloned, h5-HT1A receptors. Its agonist actions at 5-HT1A autoreceptors underlie its ability to decrease extracellular levels of 5-HT in the FCX, and likely contribute to the increase in extracellular levels of DA and NAD evoked by S 15535 in this structure. Further, S 15535 is active in several other, although not all, models of potential AD activity. Thus, although S 15535 is under development as an anxiolytic agent, a further characterization of its putative AD actions would be of interest.
In this study, we attempted to identify of the subtype(s) of alpha-2 adrenergic receptor (AR) involved in the control of motor behavior, nociception and the hippocampal synthesis of noradrenaline ...(NA) in the rat. The high efficacy alpha-2 AR agonists, xylazine and UK 14,304 5-bromo-6-2-imidazolin-2-yl-aminoquinoxaline, inhibited striatal accumulation of L-dopa in rats pretreated with NSD 1015 (an inhibitor of aromatic amino acid-decarboxylase), elicited a loss of the righting reflex in rats, provoked ataxia in the rotarod test in mice and elicited antinociception in the writhing and hot-plate tests in mice. Guanfacine and guanabenz, agonists acting preferentially at rat alpha-2A (R alpha-2A)/human alpha-2A (H alpha-2A) AR, mimicked the antinociceptive and motor actions of xylazine and UK 14,304 and likewise inhibited NA synthesis. The preferential R alpha-2A/H alpha-2A AR antagonist, 2-(2H-(1-methyl-1, 3-dihydroisoindole)methyl)-4, 5-dihydro-imidazole (BRL 44408), enhanced hippocampal synthesis of NA and blocked the antinociceptive and motor effects of UK 14,304, xylazine, guanfacine and guanabenz. Similarly, fluparoxan and des-fluorofluparoxan, preferential antagonists at R alpha-2A AR as compared to H alpha-2A AR, were highly active. In contrast, the preferential alpha-2B/alpha-2C AR antagonists, ARC 239 2-(2-(4-o-methoxyphenyl)piperazine-1-yl)-ethyl)-4,4-dimethyl-1,3- (2H,4H)-isoquinolinedione prazosin, corynanthine, spiroxatrine and 1,2-dimethyl-2,3,9,13-betetrahydro-1H-dibenzo(c,f)- imidazo(1,5-a)azepine (BRL 41992), as well as the preferential H alpha-2A AR antagonist, 2-(2,6-dimethoxyphenoxyethyl)- aminomethyl-1,4-benzodioxane (WB 4101), were only weakly active. Based on the actions of a total of 16, structurally diverse alpha-2 AR antagonists, a correlation matrix was constructed. This revealed a strong correlation among the tests (median r = 0.82) and allowed for a comparison between drug potency in inhibiting these alpha-2 AR-mediated actions and affinity at various populations of alpha-2 AR subtypes (see companion paper). Correlations for potency in the two motor tests were pronounced with R alpha-2A sites (0.85), modest with H alpha-2A sites (0.60) and alpha-2B sites (0.58) and poor with alpha-2C sites (0.35). For the two antinociceptive tests, correlations were likewise pronounced with R alpha-2A sites (0.80) but less marked with H alpha-2A sites (0.73), alpha-2B sites (0.62) and alpha-2C sites (0.62).
Peripheral collisions involving heavy ions at relativistic energies have been extensively studied for the last years. Such reactions lead to generally hot fragments 1,2, however the excitation energy ...is subject to large fluctuations and can reach low values 3. The study of the energy dissipation, its coupling to other quantities such as the isospin and momentum of fragments are of interest because they carry information on the underlying mechanism, governing to a large extent production yields.
Up to now this excitation energy has been essentially assessed from the effect of the evaporation stage on the
N
Z
ratio of fragments 1,2. We report in this contribution on a direct measurement, in coincidence with heavy fragments, of particles which mainly come from the deexcitation stage of the quasi-projectile. This type of measurement provides information not only on the mean deposited energy, but also on the excitation spectrum.
The experimental results will be discussed in view of two questions: are neutron-rich isotopes produced either by fluctuations in the energy deposition (low energy tail) or by fluctuations in the decay stage for hot primary fragments? Does a Glodhaber-type mechanism 4 (recoil effects) fully accounts for the width of the longitudinal momentum spectrum?
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IJS, IMTLJ, KILJ, KISLJ, NUK, SBCE, SBJE, UL, UM, UPCLJ, UPUK
The quasi-projectile (QP) properties are investigated in the Ar+Ni collisions at 95 A.MeV taking into account the intermediate velocity emission. Indeed, in this reaction, between 52 and 95 A.MeV ...bombarding energies, the number of particles emitted in the intermediate velocity region is related to the overlap volume between projectile and target. Mean transverse energies of these particles are found particularly high. In this context, the mass of the QP decreases linearly with the impact parameter from peripheral to central collisions whereas its excitation energy increases up to 8 A.MeV. These results are compared to previous analyses assuming a pure binary scenario.
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GEOZS, IJS, IMTLJ, KILJ, KISLJ, NUK, OILJ, SAZU, SBCE, SBJE, UL, UM, UPCLJ, UPUK
The odd-even staggering of the yield of final reaction products has been studied as a function of proton (Z) and neutron (N) numbers for the collisions 84 Kr+112 Sn and 84 Kr+124 Sn at 35 ...MeV/nucleon, in a wide range of elements (up to Z ~ 20). The experimental data show that staggering effects rapidly decrease with increasing size of the fragments. Moreover the staggering in N is definitely larger than the one in Z. Similar general features are qualitatively reproduced by the GEMINI code. Concerning the comparison of the two systems, the staggering in N is in general rather similar, being slightly larger only for the lightest fragments produced in the n-rich system. In contrast the staggering in Z, although smaller than that in N, is sizably larger for the n-poor system with respect to the n-rich one.
Isospin transport phenomena in dissipative heavy ion collisions have been investigated at Fermi energies with a beam of 84Kr at 35AMeV. A comparison of the /Z of light and medium products ...forward-emitted in the centre of mass frame when the beam impinges on a n-poor 112Sn and a n-rich 124Sn targets is presented. Data were collected by means of a three-layer telescope with very good performances in terms of mass identification (full isotopic resolution up to Z about 20 for ions punching through the first detector layer) built by the FAZIA Collaboration and located just beyond the grazing angle for both reactions. The /Z of the decay products emitted when the n-rich target is used is always higher than that associated to the n-poor one. Since the detector was able to measure only fragments coming from the QuasiProjectile decay and/or neck emission, the observed behaviour can be ascribed to the isospin diffusion, driven by the isospin gradient between QuasiProjectile and QuasiTarget. Moreover, for light fragments the /Z as a function of the lab velocity of the fragment increases when we move from the QuasiProjectile velocity to the centre of mass (neck zone). This effect can be interpreted as an evidence of isospin drift driven by the density gradient between the QuasiProjectile zone (at normal density) and the more diluted neck zone.
The european Fazia collaboration aims at building a new modular array for charged product identification to be employed for heavy-ion studies. The elementary module of the array is a ...Silicon-Silicon-CsI telescope, optimized for ion identification also via pulse shape analysis. The achievement of top performances imposes specific electronics which has been developed by FAZIA and features high quality charge and current preamplifiers, coupled to fully digital front-end. During the initial R&D phase, original and novel solutions have been tested in prototypes, obtaining unprecedented ion identification capabilities. FAZIA is now constructing a demonstrator array consisting of about two hundreds telescopes arranged in a compact and transportable configuration. In this contribution, we mainly summarize some aspects studied by FAZIA to improve the ion identification. Then we will briefly discuss the FAZIA program centered on experiments to be done with the demonstrator. First results on the isospin dynamics obtained with a reduced set-up demonstrate well the performance of the telescope and represent a good starting point towards future investigations with both stable and exotic beams.
The water content, relative ratio of bound water, mean 1H NMR spin-lattice relaxation time T1, and T1 of bound water fraction were studied on rat liver during the course of cancer induction by ...diethylnitrosamine. Using the FETS model proposed by Fung, the results were discussed according to histology. Liver T1 increase was correlated with water content and a regular decrease of T1b was observed during the course of hepatocarcinogenesis, associated with a shift of the position of the minimum of T1b toward the negative temperatures. A biphasic decay of T1b was also noticed in the presence of hepatocarcinoma nodules.
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