--> D*(2010)- muon+ neutrino/mu
Search for the rare decay $B^{+} \rightarrow {\mu}^{+}{\mu}^{-}{\mu}^{+}{\nu}_{{\mu}}$
... the neutrino in the decay. At most one hit in the muon stations is allowed to be shared between two different muon ...a muon of the same sign in the ...
20
Measurement of the atmospheric $\nu_e$ and $\nu_\mu$ energy spectra with the ANTARES neutrino telescope
... Abstract This letter presents a combined measurement of the energy spectra of atmospheric ν e and ν µ in the energy range between ∼100 GeV and ∼50 TeV with the ANTARES neutrino telescope. The analysis uses 3012 ...
13
Measurement of Angular and CP Asymmetries in $D^0\to\pi^+\pi^-\mu^+\mu^-$ and $D^0\to K^+K^-\mu^+\mu^-$ decays
... a muon and an undetected ...multivariate muon-identification discriminant that combines the information from the Cherenkov detectors, the calorimeters and the muon system [22, ...the muon- ...
15
Physique du Higgs aux collisionneurs $e^+e^-$ et $\mu^+\mu^-$
... pas necessaire de refroidir les muons autant que pour le premier collisionneur : en general, une dispersion en energie de 0.1% est plus que susante, ce qui permet d'atteindre une lu[r] ...
128
First observations of the rare decays $B^+\!\rightarrow K^+\pi^+\pi^-\mu^+\mu^-$ and $B^+\!\rightarrow\phi K^+\mu^+\mu^-$
... momentum to 0.6% at 100 GeV/c. The minimum distance of a track to a primary pp interaction vertex (PV), the impact parameter (IP), is measured with a resolution of (15 + 29/p T ) µm, where p T is the the component of p ...
20
Search for the rare decay B_s^0->mu^+mu^-
... the 95% C.L. [17]. The D0 detector [18] has a central tracking system, consisting of a silicon microstrip tracker (SMT) [19] and a central fiber tracker (CFT), both located within a 2 T su- perconducting solenoidal ...
7
Search for the lepton flavour violating decay $\tau^-\to \mu^-\mu^+\mu^-$
... well-reconstructed muon candidates with p T > 300 MeV/c that have a significant separation from the ...same-sign muon pairs with mass lower than 250 MeV/c 2 ...
22
Deviations of exact neutrino textures using radiative neutrino masses
... S 3 1 0 + F i 1 0 - Table 2. Particle content. A Z 2 symmetry needs to be included to avoid FCNC [ 36 – 38 ]. To do so, any doublet scalar of the model with the same quantum numbers as the Higgs needs to be odd under ...
10
Search for $A'\to\mu^+\mu^-$ Decays
... each muon would hit active sensors, and thus, have recorded hits in the ...each muon track, though this dependence is largely geometric, making rescaling the resolution of prompt tracks ...
30
Measurement of $C\!P$ asymmetries in the decays $B^0 \rightarrow K^{*0} \mu^+ \mu^-$ and $B^+ \rightarrow K^{+} \mu^+ \mu^-$
... criteria. A requirement on the B candidate vertex fit χ 2 per degree of freedom is applied to provide a good quality vertex fit. Additionally, the angle between the momentum vector of the B candidate and the vector ...
19
Constraints on the $K^0_S \rightarrow \mu^+ \mu^-$ Branching Fraction
... S → π + π − branching fraction are found to be smaller than 5%. The total systematic uncertainty is between 19% and 23%, depending on the trigger category and the BDT bin. It tends to be lower in the TIS trigger category ...
18
Understanding untyped $\overline{\lambda}\mu\widetilde{\mu}$ calculus
... Continuation semantics of λµe µ T is given by the interpretation in the category of negated domains of [ 22 ], whereas λµe µ Q is interpreted in Moggi’s Kleisli category over predomains [r] ...
16
Constraints on neutrino lifetime from the Sudbury Neutrino Observatory
... The neutron capture efficiency was found to be strongly correlated with the neutrino parameters and is floated in the fit to correctly account for correlations with the final results. Less correlated parameters ...
11
Search for lepton number violating decays $B^{+}\rightarrow \pi^- \mu^+ \mu^+$ and $B^{+}\rightarrow K^- \mu^+ \mu^+$
... The search for B + → h − µ + µ + is carried out with data from the LHCb experiment at the Large Hadron Collider at CERN. The data corresponds to 36 pb −1 of integrated luminosity of proton-proton collisions at √ s = 7 ...
7
First observation of the decay $B^{+} \rightarrow \pi^{+} \mu^{+} \mu^{-}$
... 30 Institute for Nuclear Research of the Russian Academy of Sciences (INR RAN), Moscow, Russia 31 Budker Institute of Nuclear Physics (SB RAS) and Novosibirsk State University, Novosibir[r] ...
20
Introducing HR-$\mu$MAS NMR probe for $\mu$g-scale samples
... The excellent NMR spectroscopic capabilities of HR-IiMAS shown here for NMR metabolic profiling on Ilg/nL samples have demonstrated that HR-IIMAS could have an impact on future NMR-b[r] ...
2
Model-independent search for neutrino sources with the ANTARES neutrino telescope
... of neutrino emission models or assumptions on the topology of emission regions, this analysis is not intended to discover potential sources with the highest achievable significance, nor to analyse the properties ...
33
Search for the rare decay $\Lambda_{c}^{+} \to p\mu^+\mu^-$
... For the final selection a second BDT is trained, which includes additional variables related to Λ + c -baryon decay properties and the isolation of the proton and muons in the detector. The final discrimination is ...
17
Evidence for the rare decay $\Sigma^+ \to p \mu^+ \mu^-$
... Cherenkov detectors, an electromagnetic and a hadronic calorimeter, and a muon system composed of alternating layers of iron and multiwire proportional chambers. The online event selection is performed by a ...
17
Search for the decay D0 to \pi+ \pi- \mu+ \mu-
... A search for the D 0 → π + π − µ + µ − decay, where the muon pair does not originate from a resonance, is performed using proton-proton collision data corresponding to an integrated luminosity of 1.0 fb −1 ...
21