A5084010480- Greenhouse Technology and Climate Control
- Nuclear Physics and Applications
- Plant Water Relations and Carbon Dynamics
- Neural dynamics and brain function
- Nuclear reactor physics and engineering
- Light effects on plants
- EEG and Brain-Computer Interfaces
- Radioactive contamination and transfer
- Magnetic and transport properties of perovskites and related materials
- Radioactivity and Radon Measurements
- Radioactive Decay and Measurement Techniques
- Nuclear physics research studies
- Nuclear and radioactivity studies
- Fluid Dynamics and Turbulent Flows
- Computational Fluid Dynamics and Aerodynamics
- Plant and animal studies
- Neuroscience and Neural Engineering
- Radiation Detection and Scintillator Technologies
- Guidance and Control Systems
- Graphite, nuclear technology, radiation studies
- Nuclear Materials and Properties
- Dementia and Cognitive Impairment Research
- Plasma and Flow Control in Aerodynamics
- Advanced Chemical Physics Studies
- Sleep and Wakefulness Research
Centre Hospitalier Universitaire de Rennes
2024
Franche-Comté Électronique Mécanique Thermique et Optique - Sciences et Technologies
2013-2023
Centre National de la Recherche Scientifique
1986-2022
Université de technologie de belfort-montbéliard
2017-2022
Université de franche-comté
1999-2017
Université de Sherbrooke
2013-2015
Bhabha Atomic Research Centre
2011
Université Laval
1981-2007
Université de Lille
1981-1998
Laboratoire de Neurosciences Cognitives
1993
Although green consumption is increasingly popular in the academic literature, practice still far from commonplace among consumers. Few studies have been conducted to explain consumer reluctance adopt products (GPs), particularly with regard roles of various risks consumers perceive their purchases. However, perceived towards GPs could be one explanations for ‘green gap’ – difference between pro-environmental attitudes and purchase behaviour. We used a means-end chain (MEC) approach explore...
The long-lived radionuclide Fe 60 has been observed through extraction of its disintegration product, 10-minute Co 60m , from the iron fraction isolated a copper target bombarded with ~400-Mev. protons. Direct observation was prevented by 59 present. Yield considerations indicate half-life to be ~3 × 10 5 years, uncertain factor 3.
1. In anaesthetized rats, recordings were made within the medullary subnucleus reticularis dorsalis (SRD) from neurones that exhibited convergence of nociceptive inputs entire surface body. Neurones with total responded to supramaximal percutaneous electrical stimuli (2 ms duration) early and late peaks due activation A delta C fibres, respectively, no matter which part body was stimulated. partial identical an peak regardless stimulated a some, mainly contralateral, parts The...
ISHS International Conference on Sustainable Greenhouse Systems - Greensys2004 CFD PREDICTION OF THE NATURAL VENTILATION IN A TUNNEL-TYPE GREENHOUSE: INFLUENCE WIND DIRECTION AND SENSIBILITY TO TURBULENCE MODELS
The yields of 53-day Be 7 , 21.3-hour Mg 28 and 56.6-hour Ni 66 from the slow neutron fission U 235 have been investigated. Upper limits 3 × 10 −7 % 4.2 −9 set for respectively. A yield 2.0 ± 1.0 −8 has found formation . These results are compared with current knowledge frequency triple
The half-lives of Au 195 , Pt 195m and 197 have been measured. radionuclides were produced by neutron irradiation in the NRX reactor at Chalk River radiochemically purified after irradiation. decay X rays γ-radiations from was observed with a NaI (Tl) detector, β-decay an anthracene detector. are:[Formula: see text]The errors quoted are estimated reliability measurement include statistical counting error plus systematic error.
A new radioisotope of platinum, ${\mathrm{Pt}}^{200}$, with an 11.5-hr half-life has been produced by successive neutron capture in ${\mathrm{Pt}}^{198}$. It was identified milking its daughter, ${\mathrm{Au}}^{200}$. The activation cross section for the reaction ${\mathrm{Pt}}^{199}(n, \ensuremath{\gamma}){\mathrm{Pt}}^{200}$ is approximately 15 barns.
The reactor neutron-capture cross section of 18-minute Rb 88 has been determined by an activation method. yield 89 formed successive neutron capture in 87 was counting the beta rays emitted its daughter, 51-day Sr . In these experiments is also produced (n, γ)Sr reaction from contamination rubidium target and decay Corrections for contributions sources to have measured experimentally. be 5.8 mb. conditions experiment. Taking 0.12 ± 0.3 barn thermal , found 1.0 neutrons.
The half-life of Au 200 has been measured to be 48.4 ± 0.3 minutes. beta radiations emitted in the decay have studied by absorption aluminum, and gamma with a multichannel scintillation spectrometer. Two rays end-point energies 2.25 0.20 0.7 0.1 Mev respective abundance (75 3)% (25 were detected. Three 0.367, 1.23, 1.60 observed. It was established that 0.367- 1.23-Mev are coincidence. A scheme for is proposed.