Search results for "signal processing"

showing 10 items of 2451 documents

Constraints on doubly charged Higgs interactions at linear collider

1996

Production of a single doubly charged Higgs boson $Delta^{--}$ in polarized $e^+e^-$ and $e^+\gamma$ collision modes of the linear collider have been investigated. The mass range of $Delta^{--}$ to be probed extends up to the collision energy. The diagonal lepton number violating Yukawa coupling $h_{ee}$ will be tested at least three orders of magnitude more strictly than in present experiments.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesFísicaCoupling (probability)01 natural sciencesLepton number3. Good healthlaw.inventionHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Orders of magnitude (time)law0103 physical sciencesHiggs bosonProduction (computer science)High Energy Physics::Experiment010306 general physicsColliderEnergy (signal processing)
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Cross section measurements of high-p(T) dilepton final-state processes using a global fitting method

2008

We present a new method for studying high-$p_T$ dilepton events ($e^{\pm}e^{\mp}$, $\mu^{\pm}\mu^{\mp}$, $e^{\pm}\mu^{\mp}$) and simultaneously extracting the production cross sections of $p\bar{p} \to t\bar{t}$, $p\bar{p} \to W^+W^-$, and $p\bar{p} \to \ztt$ at a center-of-mass energy of $\sqrt{s} = 1.96$ TeV. We perform a likelihood fit to the dilepton data in a parameter space defined by the missing transverse energy and the number of jets in the event. Our results, which use $360 {\rm pb^{-1}}$ of data recorded with the CDF II detector at the Fermilab Tevatron Collider, are $\sigma(t\bar{t}) = 8.5_{-2.2}^{+2.7}$ pb, $\sigma(W^+W^-) = 16.3^{+5.2}_{-4.4}$ pb, and $\sigma(\ztt) =291^{+50}_…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologyGlobal fittingFOS: Physical sciencesddc:500.2State (functional analysis)Astronomy & Astrophysics;; Physics Particles & Fields01 natural sciences7. Clean energyHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)CrystallographyTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciences_High Energy Physics::ExperimentProduction (computer science)010306 general physicsEnergy (signal processing)Bar (unit)Lepton
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Gamow-Teller transitions in theA=40isoquintet of relevance for neutrino captures inAr40

2014

Background: The Gamow-Teller response of $^{40}\mathrm{Ar}$ is important for the use of liquid argon as a medium for neutrino detection. An ambiguity about the Gamow-Teller strength for the excitation of ${1}^{+}$ states at 2290 and 2730 keV in $^{40}\mathrm{K}$ results in a significant uncertainty for neutrino capture rates. This ambiguity is caused by the large discrepancy observed between strengths extracted from $^{40}\mathrm{Ar}$($p$, $n$) charge-exchange data and the transition strengths for the analog transitions studied in the $\ensuremath{\beta}$ decay of $^{40}\mathrm{Ti}$.Purpose: This study was aimed at resolving the ambiguity between the results from the $^{40}\mathrm{Ar}$($p$,…

PhysicsNuclear and High Energy PhysicsParticle physicsAmplitudeSHELL modelLiquid argonNeutrinoBorn approximationEnergy (signal processing)ExcitationNeutrino scatteringPhysical Review C
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Charged current weak electroproduction of the Delta resonance

1998

We study the weak production of $\ensuremath{\Delta}$ (i.e., ${e}^{\ensuremath{-}}+\stackrel{\ensuremath{\rightarrow}}{p}{\ensuremath{\Delta}}^{0}+{\ensuremath{\nu}}_{e}$ and ${e}^{+}+\stackrel{\ensuremath{\rightarrow}}{p}{\ensuremath{\Delta}}^{++}+{\overline{\ensuremath{\nu}}}_{e})$ in the intermediate energy range corresponding to the Mainz and TJNAF electron accelerators. The differential cross sections $\ensuremath{\sigma}(\ensuremath{\theta})$ are found to be of the order of ${10}^{\ensuremath{-}39}$ cm${}^{2}$/sr, over a range of angles which increases with energy. The possibility of observing these reactions with the high luminosities available at these accelerators, and studying the…

PhysicsNuclear and High Energy PhysicsParticle physicsAngular distributionIntermediate energyOrder (ring theory)FísicaProduction (computer science)ElectronResonance (particle physics)Energy (signal processing)Charged current
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Measurement of in oscillation using quantum correlations in at

2015

We report a measurement of the parameter y(CP) in D-0-(D) over bar (0) oscillations performed by taking advantage of quantum coherence between pairs of D-0(D) over bar (0) mesons produced in e(+)e(-) annihilations near threshold. In this work, doubly-tagged D-0(D) over bar (0) events, where one D decays to a CP eigenstate and the other D decays in a semileptonic mode, are reconstructed using a data sample of 2.92 fb(-1) collected with the BESIII detector at the center-of-mass energy of root s = 3.773 GeV. We obtain y(CP) = (-2.0 +/- 1.3 +/- 0.7)%, where the first uncertainty is statistical and the second is systematic. This result is compatible with the current world average.

PhysicsNuclear and High Energy PhysicsParticle physicsAnnihilationMeson010308 nuclear & particles physicsOscillationQuantum correlation01 natural sciencesNuclear physicsPion0103 physical sciencesCP violationCoherence (signal processing)High Energy Physics::Experiment010306 general physicsEigenvalues and eigenvectors
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Resonant conversion of massless neutrinos in supernovae

1996

It has been noted for a long time that, in some circumstances, {\sl massless} neutrinos may be {\sl mixed} in the leptonic charged current. Conventional neutrino oscillation searches in vacuum are insensitive to this mixing. We discuss the effects of resonant massless-neutrino conversions in the dense medium of a supernova. In particular, we show how the detected $\bar\nu_e$ energy spectra from SN1987a and the supernova $r$-process nucleosynthesis may be used to provide very stringent constraints on the mixing of {\sl massless} neutrinos.

PhysicsNuclear and High Energy PhysicsParticle physicsAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaAstrophysicsNuclear physicsMassless particleSupernovaHigh Energy Physics - PhenomenologyGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)NucleosynthesisHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationMixing (physics)Charged currentEnergy (signal processing)
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Improved determination of the electroweak penguin contribution to ϵ′/ϵ in the chiral limit

2003

We perform a finite energy sum rule analysis of the flavor ud two-point V-A current correlator, Delta Pi (Q^2). The analysis, which is performed using both the ALEPH and OPAL databases for the V-A spectral function, Delta rho, allows us to extract the dimension six V-A OPE coefficient, a_6, which is related to the matrix element of the electroweak penguin operator, Q_8, by chiral symmetry. The result for a_6 leads directly to the improved (chiral limit) determination epsilon'/epsilon = (- 15.0 +- 2.7) 10^{-4}. Determination of higher dimension OPE contributions also allows us to perform an independent test using a low-scale constrained dispersive analysis, which provides a highly nontrivial…

PhysicsNuclear and High Energy PhysicsParticle physicsCurrent (mathematics)010308 nuclear & particles physicsOperator (physics)High Energy Physics::PhenomenologyElectroweak interaction01 natural sciencesDimension (vector space)Consistency (statistics)0103 physical sciencesHigh Energy Physics::ExperimentLimit (mathematics)Sum rule in quantum mechanics010306 general physicsEnergy (signal processing)Physics Letters B
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Generalized Bounds on Majoron-neutrino couplings

2001

We discuss limits on neutrino-Majoron couplings both from laboratory experiments as well as from astrophysics. They apply to the simplest class of Majoron models which covers a variety of possibilities where neutrinos acquire mass either via a seesaw-type scheme or via radiative corrections. By adopting a general framework including CP phases we generalize bounds obtained previously. The combination of complementary bounds enables us to obtain a highly non-trivial exclusion region in the parameter space. We find that the future double beta project GENIUS, together with constraints based on supernova energy release arguments, could restrict neutrino-Majoron couplings down to the 10^{-7} leve…

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesParameter spaceSupernovaHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Radiative transferCP violationNeutrinoVariety (universal algebra)Energy (signal processing)Majoron
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Is charged lepton flavor violation a high energy phenomenon?

2013

Searches for rare processes such as mu --> e gamma put stringent limits on lepton flavour violation expected in many Beyond the Standard Model physics scenarios. This usually precludes the observation of flavour violation at high energy colliders such as the LHC. We here discuss a scenario where right-handed neutrinos are produced via a Z' portal but which can only decay via small flavour violating couplings. Consequently, the process rate is unsuppressed by the small couplings and can be visible despite unobservably small mu --> e gamma rates.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh energyLarge Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciences01 natural sciencesProcess rateHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::ExperimentNeutrino010306 general physicsEnergy (signal processing)FlavorLeptonPhysical Review D
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On total muon capture rates and the average neutrino energy

1973

A method of avoiding the uncertainty associated with the average neutrino energy nu in the usual closure approach to muon capture rates is discussed. Instead of neglecting the kinematic dependence on each particular channel, the partial capture rate is approximated by a first-order expansion around nu . After the sum over the final states is performed, the result is quite independent of the specific value of nu . Application to /sup 3/He, /sup 6/Li and closed-shell nuclei is given, as an effective test of the nuclear models used. (17 refs).

PhysicsNuclear and High Energy PhysicsParticle physicsIsotopes of lithiumFísicaKinematicsMuon captureNuclear physicsHelium-4Closure (computer programming)Helium-3NeutrinoEnergy (signal processing)Nuclear PhysicsNuclear Physics A
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