13 research outputs found

    Search for 22^{22}Na in novae supported by a novel method for measuring femtosecond nuclear lifetimes

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    Classical novae are thermonuclear explosions in stellar binary systems, and important sources of 26^{26}Al and 22^{22}Na. While gamma rays from the decay of the former radioisotope have been observed throughout the Galaxy, 22^{22}Na remains untraceable. The half-life of 22^{22}Na (2.6 yr) would allow the observation of its 1.275 MeV gamma-ray line from a cosmic source. However, the prediction of such an observation requires good knowledge of the nuclear reactions involved in the production and destruction of this nucleus. The 22^{22}Na(p,γp,\gamma)23^{23}Mg reaction remains the only source of large uncertainty about the amount of 22^{22}Na ejected. Its rate is dominated by a single resonance on the short-lived state at 7785.0(7) keV in 23^{23}Mg. In the present work, a combined analysis of particle-particle correlations and velocity-difference profiles is proposed to measure femtosecond nuclear lifetimes. The application of this novel method to the study of the 23^{23}Mg states, combining magnetic and highly-segmented tracking gamma-ray spectrometers, places strong limits on the amount of 22^{22}Na produced in novae, explains its non-observation to date in gamma rays (flux < 2.5x10−410^{-4} ph/(cm2^2s)), and constrains its detectability with future space-borne observatories.Comment: 18 pages, 3 figures, 1 tabl

    Lung cancer risk and occupational exposures in crop farming: results from the AGRIculture and CANcer (AGRICAN) cohort

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    International audienceOBJECTIVES:Farmers are considered at lower risk of lung cancer. However, specific tasks can expose them to hazardous air contaminants such as pesticides, diesel exhaust and mineral dust. This study aimed to assess the associations between various crops and related tasks and the risk of lung cancer, overall and by histological subtypes.METHODS:AGRIculture and CANcer is a prospective French cohort of individuals affiliated to the agricultural health insurance scheme. Incident lung cancers (n=897) were identified by cancer registries from enrolment (2005-2007) to 2013. Data on crop and livestock exposure during lifetime were obtained from the enrolment questionnaire. We used a Cox model with attained age as timescale, adjusted for gender, smoking history and exposure to cattle and horses. Effects of duration and surface were assessed and analyses stratified on gender and smoking status were performed.RESULTS:Winegrowers were at higher risk of adenocarcinoma (HR=1.27 (95% CI 0.94 to 1.72)). We also found an association between pea growing and small cell lung cancer: significant effect of duration (ptrend=0.04) and the suggestion of a surface-effect relationship (ptrend=0.06); increased risk (HR=2.38 (95% CI 1.07 to 5.28)) for pesticide users; and significant effect of duration (ptrend=0.01) for harvesters. The risk of squamous cell carcinoma was increased for sunflower growing (HR=1.59 (95% CI 0.97 to 2.62), fruit-tree pruning (HR=1.44 (95% CI 0.92 to 2.27)) and pesticide use on beets (HR=1.47 (95% CI 0.92 to 2.34)). Corn and/or wheat/barley growers were at lower risk of lung cancer.CONCLUSIONS:Our results suggest associations between lung cancer and several crop-related tasks, even if we cannot rule out some chance findings due to multiple comparisons

    Lifetime Measurements Using RDDS Method in the Vicinity of 78^{78}Ni

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    International audienceReduced quadrupole transition probabilities for low-lying transitions in neutron-rich N = 52 isotones 88Kr and 86Se were investigated with a recoil distance Doppler shift (RDDS) experiment. The experiment was performed at GANIL (Caen, France) using the Orsay Universal Plunger System (OUPS) for the RDDS technique and the AGATA array for the γ-ray detection coupled to the VAMOS++ magnetic spectrometer for an event-by-event particle identification. In 88Kr, the lifetimes of seven levels were determined and in 86Se, the lifetimes of five levels were determined. The deduced B(E2; 2+ 1 → 0 + 1 ) are compared with mean-field and shellmodel calculations

    Excitations of the magic N=50 neutron-core revealed in Ga 81

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    none41The high-spin states of the neutron-rich Ga81, with three valence protons outside a Ni78 core, were measured. The measurement involved prompt Îł-ray spectroscopy of fission fragments isotopically identified using the combination of the variable mode spectrometer (VAMOS++) and the advanced gamma tracking array (AGATA). The new Îł-ray transitions, observed in coincidence with Ga81 ions, and the corresponding level scheme do not confirm the high-spin levels reported earlier. The newly observed high-spin states in Ga81 are interpreted using the results of state-of-the-art large-scale shell model (LSSM) calculations. The lower excitation energy levels are understood as resulting from the recoupling of three valence protons to the closed doubly magic core, while the highest excitation energy levels correspond to excitations of the magic N=50 neutron core. These results support the doubly magic character of Ni78 and the persistence of the N=50 shell closure but also highlight the presence of strong proton-neutron correlations associated with the promotion of neutrons across the magic N=50 shell gap, only few nucleons away from Ni78.restrictedDudouet J.; Lemasson A.; Maquart G.; Nowacki F.; Verney D.; Rejmund M.; Duchene G.; Stezowski O.; Clement E.; Michelagnoli C.; Korichi A.; Andreoiu C.; Astier A.; De Angelis G.; De France G.; Delafosse C.; Deloncle I.; Didierjean F.; Dombradi Z.; Ducoin C.; Gadea A.; Gottardo A.; Guinet D.; Jacquot B.; Jones P.; Konstantinopoulos T.; Kuti I.; Le Blanc F.; Lenzi S.M.; Li G.; Lozeva R.; Million B.; Napoli D.R.; Navin A.; Perez-Vidal R.M.; Petrache C.M.; Ralet D.; Ramdhane M.; Redon N.; Schmitt C.; Sohler D.Dudouet, J.; Lemasson, A.; Maquart, G.; Nowacki, F.; Verney, D.; Rejmund, M.; Duchene, G.; Stezowski, O.; Clement, E.; Michelagnoli, C.; Korichi, A.; Andreoiu, C.; Astier, A.; De Angelis, G.; De France, G.; Delafosse, C.; Deloncle, I.; Didierjean, F.; Dombradi, Z.; Ducoin, C.; Gadea, A.; Gottardo, A.; Guinet, D.; Jacquot, B.; Jones, P.; Konstantinopoulos, T.; Kuti, I.; Le Blanc, F.; Lenzi, S. M.; Li, G.; Lozeva, R.; Million, B.; Napoli, D. R.; Navin, A.; Perez-Vidal, R. M.; Petrache, C. M.; Ralet, D.; Ramdhane, M.; Redon, N.; Schmitt, C.; Sohler, D

    High-resolution spectroscopy of neutron-rich Br isotopes and signatures for a prolate-to-oblate shape transition at N=56

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    International audienceThe first systematic experimental study of the neutron-rich Br isotopes with two complementary state-of-the-art techniques is presented. These isotopes have been populated in the fission process at two different facilities, GANIL and ILL. New spectroscopic information has been obtained for odd-even 87−93^{87-93}Br isotopes and the experimental results have been compared with state-of-the-art Large-Scale Shell-Model and DNO Shell-Model calculations. As a result of such theoretical approaches, a transition from prolate (87,89^{87,89}Br) to oblate (91,93^{91,93}Br) shapes is obtained from the subtle balance between proton and neutron quadrupole deformations, as a clear signature of pseudo-SU3 quadrupole regime

    Structure of 83^{83}As, 85^{85}As and 87^{87}As: from semi-magicity to Îł\gamma-softness

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    International audienceThe structure of 83^{83}As, 85^{85}As and 87^{87}As have been studied in fusion-fission reaction 238^{238}U+9^9Be. Fission fragments were identified in mass and atomic number using the VAMOS++ spectrometer and the coincident Îł\gamma-rays were detected in the Îł\gamma-ray tracking array AGATA. New transitions in 83^{83}As and 85^{85}As are reported and placed in the level schemes. A level scheme of the excited states in 87^{87}As is proposed for the first time. The data are interpreted in frame of Large-Scale Shell-Model calculations, SU3 symmetries and Beyond Mean-Field frameworks. A spherical regime at magic number NN=50 is predicted and the location of the proton g9/2g_{9/2} orbital is proposed for the first time. Development of collectivity in a prolate deformed, Îł\gamma-soft regime in the open shell cases 85^{85}As and 87^{87}As, most neutron-rich isotopes beyond NN=50, is concluded. Data and theoretical calculations give confidence to a relatively high extrapolated excitation energy about 4 MeV of the 9/2+9/2^+ state in 79^{79}Cu, one proton above 78^{78}Ni

    Structure of 83^{83}As, 85^{85}As and 87^{87}As: from semi-magicity to Îł\gamma-softness

    No full text
    The structure of 83^{83}As, 85^{85}As and 87^{87}As have been studied in fusion-fission reaction 238^{238}U+9^9Be. Fission fragments were identified in mass and atomic number using the VAMOS++ spectrometer and the coincident Îł\gamma-rays were detected in the Îł\gamma-ray tracking array AGATA. New transitions in 83^{83}As and 85^{85}As are reported and placed in the level schemes. A level scheme of the excited states in 87^{87}As is proposed for the first time. The data are interpreted in frame of Large-Scale Shell-Model calculations, SU3 symmetries and Beyond Mean-Field frameworks. A spherical regime at magic number NN=50 is predicted and the location of the proton g9/2g_{9/2} orbital is proposed for the first time. Development of collectivity in a prolate deformed, Îł\gamma-soft regime in the open shell cases 85^{85}As and 87^{87}As, most neutron-rich isotopes beyond NN=50, is concluded. Data and theoretical calculations give confidence to a relatively high extrapolated excitation energy about 4 MeV of the 9/2+9/2^+ state in 79^{79}Cu, one proton above 78^{78}Ni

    Search for 22Na in novae supported by a novel method for measuring femtosecond nuclear lifetimes

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    Abstract Classical novae are thermonuclear explosions in stellar binary systems, and important sources of 26Al and 22Na. While γ rays from the decay of the former radioisotope have been observed throughout the Galaxy, 22Na remains untraceable. Its half-life (2.6 yr) would allow the observation of its 1.275 MeV γ-ray line from a cosmic source. However, the prediction of such an observation requires good knowledge of its nucleosynthesis. The 22Na(p, γ)23Mg reaction remains the only source of large uncertainty about the amount of 22Na ejected. Its rate is dominated by a single resonance on the short-lived state at 7785.0(7) keV in 23Mg. Here, we propose a combined analysis of particle-particle correlations and velocity-difference profiles to measure femtosecond nuclear lifetimes. The application of this method to the study of the 23Mg states, places strong limits on the amount of 22Na produced in novae and constrains its detectability with future space-borne observatories
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