419 research outputs found
Results of the NEMO3 experiment
The purpose of the NEMO3 experiment is to detect neutrinoless double beta
decay in order to determine the nature of neutrino and its absolute mass. We
analysed the 389 effective days of data from the kg of Mo and
kg of Se and obtained the following limits on the half-life for
the \bb process: years (Mo) and
years (Se). The corresponding
limits on the neutrino effective mass are 0.7 - 2.8 eV (Mo) and
1.7 - 4.9 eV (Se) at 90% Confident Level. We also performed a
detailled analysis on the double beta decay of Mo into the excited
states , of Ru. The results are: years,
years,
years,
years.Comment: 4 pages, 5 figures, Proceeding of the Moriond 2006 EW conferenc
Atenció a la diversitat d’altes capacitats
El propòsit del treball és el d’analitzar el procés d’aprenentatge dels alumnes actuals a l’educació secundària obligatòria amb altes capacitats. En primer lloc s’estudien les diferents teories sobre la intel·ligència per arribar a una definició d’es d’on es parteix per a determinar les altes capacitat i posteriorment s’estudia la influència de les noves tecnologies en el desenvolupament cognitiu; s’estudia quines habilitats desenvolupen els alumnes, quins talents afavoreixen, i si es podria parlar d’una nova intel·ligència tecnològica.
En segon lloc es relaciona la intel·ligència tecnològica amb les altes capacitats; es comparen les característiques d’aprenentatge de les altes capacitats amb les habilitats que les noves tecnologies potencien en els alumnes i es proposa un esbós del que podrien ser les característiques cognitives dels alumnes amb altes capacitats en l’etapa d’educació secundària influenciats cognitivament per les noves tecnologies d’es de sempre.
Per últim, es proposa una programació anual per l’assignatura de Tecnologia per al curs de tercer de l’educació secundària obligatòria tenint en compte les necessitats educatives dels alumnes amb altes capacitats d’una manera integradora en una aula ordinària
A new method to improve photometric redshift reconstruction. Applications to the Large Synoptic Survey Telescope
In the next decade, the LSST will become a major facility for the
astronomical community. However accurately determining the redshifts of the
observed galaxies without using spectroscopy is a major challenge.
Reconstruction of the redshifts with high resolution and well-understood
uncertainties is mandatory for many science goals, including the study of
baryonic acoustic oscillations. We investigate different approaches to
establish the accuracy that can be reached by the LSST six-band photometry. We
construct a realistic mock galaxy catalog, based on the GOODS survey luminosity
function, by simulating the expected apparent magnitude distribution for the
LSST. To reconstruct the photometric redshifts (photo-z's), we consider a
template-fitting method and a neural network method. The photo-z reconstruction
from both of these techniques is tested on real CFHTLS data and also on
simulated catalogs. We describe a new method to improve photo-z reconstruction
that efficiently removes catastrophic outliers via a likelihood ratio
statistical test. This test uses the posterior probability functions of the fit
parameters and the colors. We show that the photometric redshift accuracy will
meet the stringent LSST requirements up to redshift after a selection
that is based on the likelihood ratio test or on the apparent magnitude for
galaxies with in at least 5 bands. The former selection has the
advantage of retaining roughly 35% more galaxies for a similar photo-z
performance compared to the latter. Photo-z reconstruction using a neural
network algorithm is also described. In addition, we utilize the CFHTLS
spectro-photometric catalog to outline the possibility of combining the neural
network and template-fitting methods. We conclude that the photo-z's will be
accurately estimated with the LSST if a Bayesian prior probability and a
calibration sample are used.Comment: 19 pages, 25 figures, accepted for publication in Astronomy and
Astrophysics Astronomy and Astrophysics, 201
Identification and characterization of an inhibitory fibroblast growth factor receptor 2 (FGFR2) molecule, up-regulated in an Apert Syndrome mouse model
AS (Apert syndrome) is a congenital disease composed of skeletal, visceral and neural abnormalities, caused by dominant-acting mutations in FGFR2 [FGF (fibroblast growth factor) receptor 2]. Multiple FGFR2 splice variants are generated through alternative splicing, including PTC (premature termination codon)-containing transcripts that are normally eliminated via the NMD (nonsense-mediated decay) pathway. We have discovered that a soluble truncated FGFR2 molecule encoded by a PTC-containing transcript is up-regulated and persists in tissues of an AS mouse model. We have termed this IIIa–TM as it arises from aberrant splicing of FGFR2 exon 7 (IIIa) into exon 10 [TM (transmembrane domain)]. IIIa–TM is glycosylated and can modulate the binding of FGF1 to FGFR2 molecules in BIAcore-binding assays. We also show that IIIa–TM can negatively regulate FGF signalling in vitro and in vivo. AS phenotypes are thought to result from gain-of-FGFR2 signalling, but our findings suggest that IIIa–TM can contribute to these through a loss-of-FGFR2 function mechanism. Moreover, our findings raise the interesting possibility that FGFR2 signalling may be a regulator of the NMD pathway
Measurement of double beta decay of 100Mo to excited states in the NEMO 3 experiment
The double beta decay of 100Mo to the 0^+_1 and 2^+_1 excited states of 100Ru
is studied using the NEMO 3 data. After the analysis of 8024 h of data the
half-life for the two-neutrino double beta decay of 100Mo to the excited 0^+_1
state is measured to be T^(2nu)_1/2 = [5.7^{+1.3}_{-0.9}(stat)+/-0.8(syst)]x
10^20 y. The signal-to-background ratio is equal to 3. Information about energy
and angular distributions of emitted electrons is also obtained. No evidence
for neutrinoless double beta decay to the excited 0^+_1 state has been found.
The corresponding half-life limit is T^(0nu)_1/2(0^+ --> 0^+_1) > 8.9 x 10^22 y
(at 90% C.L.).
The search for the double beta decay to the 2^+_1 excited state has allowed
the determination of limits on the half-life for the two neutrino mode
T^(2nu)_1/2(0^+ --> 2^+_1) > 1.1 x 10^21 y (at 90% C.L.) and for the
neutrinoless mode T^(0nu)_1/2(0^+ --> 2^+_1) > 1.6 x 10^23 y (at 90% C.L.).Comment: 23 pages, 7 figures, 4 tables, submitted to Nucl. Phy
Measurement of the 8B Solar Neutrino Flux with the KamLAND Liquid Scintillator Detector
We report a measurement of the neutrino-electron elastic scattering rate from
8B solar neutrinos based on a 123 kton-day exposure of KamLAND. The
background-subtracted electron recoil rate, above a 5.5 MeV analysis threshold
is 1.49+/-0.14(stat)+/-0.17(syst) events per kton-day. Interpreted as due to a
pure electron flavor flux with a 8B neutrino spectrum, this corresponds to a
spectrum integrated flux of 2.77+/-0.26(stat)+/-0.32(syst) x 10^6 cm^-2s^-1.
The analysis threshold is driven by 208Tl present in the liquid scintillator,
and the main source of systematic uncertainty is due to background from
cosmogenic 11Be. The measured rate is consistent with existing measurements and
with Standard Solar Model predictions which include matter enhanced neutrino
oscillation.Comment: 6 pages, 3 figure
Results of the BiPo-1 prototype for radiopurity measurements for the SuperNEMO double beta decay source foils
The development of BiPo detectors is dedicated to the measurement of
extremely high radiopurity in Tl and Bi for the SuperNEMO
double beta decay source foils. A modular prototype, called BiPo-1, with 0.8
of sensitive surface area, has been running in the Modane Underground
Laboratory since February, 2008. The goal of BiPo-1 is to measure the different
components of the background and in particular the surface radiopurity of the
plastic scintillators that make up the detector. The first phase of data
collection has been dedicated to the measurement of the radiopurity in
Tl. After more than one year of background measurement, a surface
activity of the scintillators of (Tl) 1.5
Bq/m is reported here. Given this level of background, a larger BiPo
detector having 12 m of active surface area, is able to qualify the
radiopurity of the SuperNEMO selenium double beta decay foils with the required
sensitivity of (Tl) 2 Bq/kg (90% C.L.) with a six
month measurement.Comment: 24 pages, submitted to N.I.M.
Measurement of Neutrino Oscillation with KamLAND: Evidence of Spectral Distortion
We present results of a study of neutrino oscillation based on a 766 ton-year
exposure of KamLAND to reactor anti-neutrinos. We observe 258 \nuebar\
candidate events with energies above 3.4 MeV compared to 365.2 events expected
in the absence of neutrino oscillation. Accounting for 17.8 expected background
events, the statistical significance for reactor \nuebar disappearance is
99.998%. The observed energy spectrum disagrees with the expected spectral
shape in the absence of neutrino oscillation at 99.6% significance and prefers
the distortion expected from \nuebar oscillation effects. A two-neutrino
oscillation analysis of the KamLAND data gives \DeltaMSq =
7.9 eV. A global analysis of data from KamLAND
and solar neutrino experiments yields \DeltaMSq =
7.9 eV and \ThetaParam =
0.40, the most precise determination to date.Comment: 5 pages, 4 figures; submitted to Phys.Rev.Letter
Measurement of double beta decay of ¹⁰⁰Mo to excited states in the NEMO 3 experiment
The double beta decay of ¹⁰⁰Mo to the 0_{1}^{+} and 2_{1}^{+} excited states of ¹⁰⁰Ru is studied using the NEMO 3 data. After the analysis of 8024 h of data the half-life for the two-neutrino double beta decay of ¹⁰⁰Mo to the excited 0_{1}^{+} state is measured to be T_{1/2}^{2v} = [5.7_{-0.9}^{+1.3} (stat.) ± 0.8 (syst.)] x 10²⁰ y. The signal-to-background ratio is equal to 3. Information about energy and angular distributions of emitted electrons is also obtained. No evidence for neutrinoless double beta decay to the excited 0_{1}^{+} state has been found. The corresponding half-life limit is T_{1/2}^{0v} (0⁺→0_{1}^{+}) > 8.9 x 10²² y (at 90% C.L.). The search for the double beta decay to the 2_{1}^{+} excited state has allowed the determination of limits on the half-life for the two neutrino mode T_{1/2}^{0v} (0⁺→2_{1}^{+}) > 1.1 x 10²¹ y (at 90% C.L.) and for the neutrinoless mode T_{1/2}^{0v} (0⁺→2_{1}^{+}) > 1.6 x 10²³ y (at 90% C.L.)
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