Radon measurements along active faults in the Langadas Basin, northern Greece

A network of three radon stations has been established in the Langadas Basin, northern Greece for radon monitoring by various techniques in earthquake prediction studies. Specially made devices with plastic tubes including Alpha Tracketch Detectors (ATD) were installed for registering alpha particles from radon and radon decay products exhaled from the ground, every 2 weeks, by using LR-115, type II, non-strippable Kodak films, starting from December 1996. Simultaneous measurements started using Lucas cells alpha spectrometer for instantaneous radon measurements in soil gas, before and after setting ATDs at the radon stations. Continuous monitoring of radon gas exhaling from the ground started from the middle of August 1999 by using silicon diode detectors, which simultaneously register meteorological parameters, such as rainfall, temperature and barometric pressure. The obtained data were studied together with the data of seismic events, such as the magnitude, <i>M_L</i>, of earthquakes that occurred at the Langadas Basin during the period of measurements, as registered by the Laboratory of Geophysics, Aristotle University of Thessaloniki, in order to find out any association between them

Radon measurements in association with earthquakes

A network of three radon stations has been established in the Langadas basin, North Greece. Newly made devices with plastic tubes are in operation with a-particle track detectors (ATDs) in registering a-particles from radon and radon decay products exhaled from the ground, every two weeks, starting from December 1996, by using LR-115, type II, nonstrippable Kodak films. Simultaneous measurements are made by using Lucas a-scintillation cells for instantaneous measurements of radon in soil gas, before and after setting the ATDs at the radon stations. The new devices used have the advantage of not using heating systems nor electrical power in the nearby area of the stations. Radon flux registrations ranged between 507 and 85880 tr cm22 or 1.5 and 188.9 tr cm22 h21, in the period of measurement, while radon concentrations in soil gas ranged between 528 and 35095 Bq m23 at the same time

Radon measurements along active faults in the Langadas Basin, northern Greece

International audienc

About the first experiment at JINR nuclotron deuteron beam with energy 2.52 gev on investigation of transmutation of I-129, NP-237, PU-238 and PU-239 in the field of neutrons generated in pbtarget with U-blanket

The experiment described in this communication is a part of the scientific program „Investigations of physical aspects of electronuclear method of energy production and transmutation of radioactive waste of atomic energetic using relativistic beams from the JINR Synchrophasotron/Nuclotron“ - the project „Energy plus Transmutation“. The performing of the first experiment at deuteron beam with energy 2.52 GeV at the electronuclear setup which consists of Pb-target with U-blanket (206.4 kg of natural uranium) and transmutation samples and its preliminary results are described. The hermetic samples of isotopes of I-129, Np-237, Pu-238 and Pu-239 which are produced in atomic reactors and industry setups which use nuclear materials and nuclear technologies were irradiated in the field of electronuclear neutrons produced in the Pbtarget surrounded with the U-blanket setup “Energy plus transmutation”. The estimations of its transmutations (radioecological aspect) were obtained in result of measurements of gamma activities of these samples. The information about space-energy distribution of neutrons in the volume of the Pb-target and the U-blanket was obtained with help of sets of activation threshold detectors (Al, V, Cu, Co, Y, In, I, Ta, Au, W, Bi and other), solid state nuclear track detectors, He-3 neutron detectors and nuclear emulsions

Izloženost genotoksičnim agensima iz životnog okoliša tijekom prenatalnog razvoja i djetinjstva

Health disorders and diseases related to environmental exposure in children such as cancer and immunologic disturbances (asthma, allergies) are on the rise. However, complex transplacental and prepubertal genotoxicology is given very limited consideration, even though intrauterine development and early childhood may be critical for elucidating the cancer aetiology. The foetus is transplacentally exposed to contaminants in food and environment such as various chemicals, drugs, radiochemically contaminated water and air. Target organs of xenobiotic action may differ between the mother and the foetus due to specific stage of developmental physiology and enzyme distribution. This in turn may lead to different levels of clastogenic and aneugenic metabolites of the same xenobiotic in the mother and the foetus. Adult’s protective behaviour is not sufficient to isolate children from radioisotopes, pesticides, toxic metals and metalloids, environmental tobacco smoke, endocrine disrupting chemicals, and various food contaminants, which are just a part of the stressors present in a polluted environment. In order to improve legislation related to foetus and child exposure to genotoxic and possibly carcinogenic agents, oncologists, paediatricians, environmental health specialists, and genotoxicologists should work together much more closely to make a more effective use of accumulated scientific data, with the final aim to lower cancer incidence and mortality.Unatoč velikim naporima da se smanji okolišna izloženost u djece se dalje bilježi trend porasta pojavnosti karcinoma i imunosnih poremećaja (astma, alergije). Premda su intrauterini razvoj i rano djetinjstvo kritično razdoblje za tumačenje etiologije nastanka karcinoma, transplacentalna i prepubertetna genotoksikologija do danas su slabo istražene. Fetus je transplacentalno izložen brojnim fizikalnim i kemijskim čimbenicima: kontaminantima iz hrane i okoliša, radiokemijski kontaminiranoj vodi, zraku te lijekovima. Ciljna tkiva za djelovanje ksenobiotika mogu biti različita u majke i fetusa zbog različitosti u razvojnoj fiziologiji i distribuciji enzima. Zbog toga u organizmu majke i fetusa mogu nastati različite razine klastogenih i aneugenih metabolita istog ksenobiotika. Zaštitna uloga odraslih u namjeri da spriječe negativne utjecaje onečišćenog okoliša na djetetovo zdravlje često je ograničena jer su radioizotopi, olovo, PCB, pasivno pušenje, živa, endokrino aktivne tvari, pesticidi i kontaminanti prisutni u svim životnim područjima tijekom razvoja i rasta djeteta. Kako bi se poboljšalo zakonodavstvo vezano uz izloženost djece genotoksičnim i vjerojatno kancerogenim tvarima, tijekom razvoja potrebna je bolja suradnja onkologa, pedijatara, stručnjaka zdravstvene ekologije i genotoksikologa. Na taj način ostvarilo bi se uspješnije iskorištavanje postojećih znanstvenih podataka u cilju smanjenja incidencije karcinoma i mortaliteta

Ytterbium (

The thick foils activation technique has been applied to estimate the average cross-sections of 168,170,176Yb $(\gamma, \mathrm{n})$ reaction near to photodisintegration threshold. The $(\gamma, \mathrm{n})$ cross-sections are derived using the integrated photon flux at any energy range from the reaction threshold to the bremsstrahlung end-point energy. The photon flux is estimated using a calibration photodisintegration set of foils and taking in advance the spectrum linearity at high energies. The p-nuclei 168Yb average cross-section is $106 \pm 21$ mb corresponding to $E_{\mathrm{mean}} = 10$ MeV. The 170Yb average cross section is $117 \pm 31$ mb matching $E_{\mathrm{mean}} = 9$ MeV while the 176Yb one is $123 \pm 36$ mb corresponding to $E_{\mathrm{mean}} = 8$ MeV. The experimental results associate to statistical model simulations performed by the TALYS code. The simulated data of 168Yb ranges 83–139 mb, while 170Yb and 176Yb vary between 89–152 and 84–170mb; which agree with the measurements within uncertainties. The simulated average cross-section of natYb $(\gamma, \mathrm{n})$ reaction is $127 \pm 25$ mb corresponding to energy ranges 6.6-14 MeV. The simulation results based on Lorentzian $\gamma$-strength considerations with the density level of Fermi gas plus the constant temperature model are closest to the average cross-sections measured

Photodisintegration average cross sections of dysprosium p-nuclei near (

First measured cross section data on ($\gamma$,n) reaction of dysprosium proton-rich nuclei 156Dy and 158Dy was experimentally determined via activation methods using a bremsstrahlung photons beam delivered by an electron medical accelerator. An integrated cross section of $144\pm 44$ mb is calculated for the 156Dy ($\gamma$,n) reaction at the energy interval 9.4-14MeV while for the 158Dy ($\gamma$,n) reaction at the energy interval 9.1-14 MeV is estimated as $168\pm 42$ mb. Moreover, theoretical calculations have been performed for all Dy isotopes employing the TALYS code. The effect of the nuclear-physics input parameters ($\gamma$-ray strength function, nuclear level densities) on the cross section calculations has been studied to successfully reproduce the experimental data. The effective cross section estimated using the TALYS code ranges between 115 and 206 mb for 156Dy ($\gamma$,n) and between 124 and 206mb for 158Dy ($\gamma$,n) reaction depending on the $\gamma$-ray strength function used