Search results for "Lung"

showing 10 items of 2389 documents

Measurement of matter-antimatter differences in beauty baryon decays

2017

Differences in the behaviour of matter and antimatter have been observed in $K$ and $B$ meson decays, but not yet in any baryon decay. Such differences are associated with the non-invariance of fundamental interactions under the combined charge-conjugation and parity transformations, known as $C\!P$ violation. Using data from the LHCb experiment at the Large Hadron Collider, a search is made for $C\!P$-violating asymmetries in the decay angle distributions of $\Lambda^0_b$ baryons decaying to $p\pi^-\pi^+\pi^-$ and $p\pi^-K^+K^-$ final states. These four-body hadronic decays are a promising place to search for sources of $C\!P$ violation both within and beyond the Standard Model of particle…

Physics beyond the Standard ModelHadrontransformation [parity]General Physics and Astronomy7000 GeV-cms8000 GeV-cmsviolation [CP]decay [meson]01 natural sciencesHigh Energy Physics - ExperimentSettore FIS/04 - Fisica Nucleare e SubnucleareHigh Energy Physics - Experiment (hep-ex)antimatterscattering [p p][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]AntimatèriaDecays of bottom mesons Flavor symmetriesB mesonLHCb - Abteilung HintonPhysicsLarge Hadron Collider02 Physical Sciencesnew physicsCabibbo–Kobayashi–Maskawa matrixPhysicsparity: transformationParticle physicsFlavor symmetriesCharge conjugation parity time reversal and other discrete symmetrieDecays of bottom mesonsasymmetry: CPCERN LHC CollCP-VIOLATION; LAMBDA(B)meson: decayangular distribution [decay]AntimatterPhysical SciencesCP violationLHCcolliding beams [p p]Lambda/b0: hadronic decayParticle Physics - Experimentp p: scatteringParticle physicsAntimatterFluids & PlasmasPhysics MultidisciplinaryLambda/b0 --> p pi- K+ K-FOS: Physical scienceshadronic decay [Lambda/b0]Lambda/b0 --> p pi+ 2pi-CP [asymmetry]530Lambda/b0 --> p pi+ 2pi-Determination of Cabibbo-Kobayashi & Maskawa (CKM) matrix elementNONuclear physicsPhysics and Astronomy (all)LAMBDA(B)TheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciencesCP: violationdecay: angular distributionddc:530010306 general physicsLarge Hadron Collider (France and Switzerland)01 Mathematical SciencesScience & Technologycharge conjugation010308 nuclear & particles physicshep-exLambda/b0 --> p pi- K+ K-High Energy Physics::PhenomenologyGran Col·lisionador d'HadronsLHC-BHEPBaryonLHCbCP-VIOLATIONCKM matrixHadronic decays of baryonBottom baryons (|B|>0)High Energy Physics::ExperimentFísica de partículesExperimentsp p: colliding beamsstatisticalexperimental results
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X-ray emitting hot plasma in solar active regions observed by the SphinX spectrometer

2012

Aims. The detection of very hot plasma in the quiescent corona is important for diagnosing heating mechanisms. The presence and the amount of such hot plasma is currently debated. The SphinX instrument on-board the CORONAS-PHOTON mission is sensitive to X-ray emission of energies well above 1 keV and provides the opportunity to detect the hot plasma component. Methods. We analysed the X-ray spectra of the solar corona collected by the SphinX spectrometer in May 2009 (when two active regions were present). We modelled the spectrum extracted from the whole Sun over a time window of 17 days in the 1.34− 7k eV energy band by adopting the latest release of the APED database. Results. The SphinX …

Physics010504 meteorology & atmospheric sciencesSpectrometerX-rayBremsstrahlungAstronomy and AstrophysicsPlasmaAstrophysics01 natural sciencesCoronaSpectral lineSun: corona methods: observational techniques: spectroscopicStars13. Climate actionSpace and Planetary Science0103 physical sciencesCalibration010303 astronomy & astrophysics0105 earth and related environmental sciencesAstronomy & Astrophysics
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A model of M87 nuclear emission without ADAF

2007

We present a simple physical model of the central source emission in the M87 galaxy. It is well known that the observed X‐ray luminosity from this galactic nucleus is much lower than the predicted one, if a standard radiative efficiency is assumed. Up to now the main model invoked to explain such a luminosity is the ADAF (Advection‐Dominated‐Accretion‐Flow) model. Our approach supposes only a simple axis‐symmetric adiabatic accretion with a low angular momentum together with the bremsstrahlung emission process in the accreting gas. With no other special hypothesis on the dynamics of the system, this model agrees well enough with the luminosity value measured by Chandra.

PhysicsAngular momentumActive galactic nucleusAstrophysics::High Energy Astrophysical PhenomenaBremsstrahlungAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsGalactic nucleiGalaxyAccretion (astrophysics)Radiative efficiencyAstrophysics::Solar and Stellar AstrophysicsAdiabatic processAstrophysics::Galaxy Astrophysics
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A Simple Model of Radiative Emission in M87

2005

We present a simple physical model of the central source emission in the M87 galaxy. It is well known that the observed X-ray luminosity from this galactic nucleus is much lower than the predicted one, if a standard radiative efficiency is assumed. Up to now the main model invoked to explain such a luminosity is the ADAF (Advection-Dominated-Accretion-Flow) model. Our approach supposes only a simple axis-symmetric adiabatic accretion with a low angular momentum together with the bremsstrahlung emission process in the accreting gas. With no other special hypothesis on the dynamics of the system, this model agrees well enough with the luminosity value measured by Chandra.

PhysicsAngular momentumAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)BremsstrahlungFOS: Physical sciencesAstronomy and AstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsAstrophysicsaccretion accretion disks black hole physics hydrodynamicsGalaxyAccretion (astrophysics)Space and Planetary ScienceRadiative efficiencyRadiative transferAstrophysics::Solar and Stellar AstrophysicsAdiabatic processAstrophysics::Galaxy AstrophysicsThe Astrophysical Journal
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Atomic physics of positronium with intense slow positron beams

2002

Abstract The theory of quantum electrodynamics has presented a complete calculation of the energy levels of positronium (Ps, e + e − ) up to the order R ∞ α 4 . The annihilation rates for para -Ps (1 1 S 0 ) and ortho -Ps (1 1 S 1 ) are completely known up to the order R ∞ α 5 and R ∞ α 6 , respectively. The present experimental uncertainty for spectroscopic results is 5–100 times larger than the theoretical uncertainty. For the annihilation rates the experimental situation is even worse. The theoretical predictions have presently reached a level of precision which is a challenge to experimentalists! The experimental uncertainty for the fine- and hyperfine transitions in the Ps atom is dete…

PhysicsAnnihilationBremsstrahlungGeneral Physics and AstronomySurfaces and InterfacesGeneral ChemistryElectronCondensed Matter PhysicsSurfaces Coatings and Filmslaw.inventionPositroniumNuclear physicsPositronlawAtomBeam dumpAtomic physicsHyperfine structureApplied Surface Science
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High-precision comparison of the antiproton-to-proton charge-to-mass ratio

2015

Invariance under the charge, parity, time-reversal (CPT) transformation$^{1}$ is one of the fundamental symmetries of the standard model of particle physics. This CPT invariance implies that the fundamental properties of antiparticles and their matter-conjugates are identical, apart from signs. There is a deep link between CPT invariance and Lorentz symmetry—that is, the laws of nature seem to be invariant under the symmetry transformation of spacetime—although it is model dependent$^{2}$. A number of high-precision CPT and Lorentz invariance tests—using a co-magnetometer, a torsion pendulum and a maser, among others—have been performed$^{3}$, but only a few direct high-precision CPT tests …

PhysicsAntiparticleParticle physicsMultidisciplinaryCPT symmetryLorentz transformationLorentz covarianceBaryonsymbols.namesakeStandard-Model ExtensionAntiprotonQuantum mechanicsAntimattersymbolsPräzisionsexperimente - Abteilung BlaumParticle Physics - Experiment
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The 0.1-100 keV Spectrum of LMC X-4 in the High State: Evidence for a High Energy Cyclotron Absorption Line

2001

We report on the spectral analysis of the X-ray pulsar LMC X-4 in its high state out of eclipse observed by BeppoSAX. During this observation no coherent pulsations are detected. The primary continuum is well described by a power law with a high energy cutoff (E_cutoff ~ E_fold ~ 18 keV). The addition of a cyclotron absorption line at ~100 keV improves the fit significantly. The inferred magnetic moment is 1.1 10^{31} Gauss cm^3, in agreement with the value estimated assuming that the neutron star is at the spin equilibrium, as it has been proposed for this source. The remaining excess at low energies can be fitted by a Comptonization of soft photons by moderately hot electrons (kT ~0.9 keV…

PhysicsAstrophysics::High Energy Astrophysical PhenomenaContinuum (design consultancy)Astrophysics (astro-ph)BremsstrahlungFOS: Physical sciencesAstronomy and AstrophysicsRadiusAstrophysicsAstrophysicsSpectral lineNeutron starPulsarSpace and Planetary ScienceOptical depth (astrophysics)Astrophysics::Solar and Stellar AstrophysicsBlack-body radiationAstrophysics::Earth and Planetary Astrophysics
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Plasma emission at the laser tripled frequency

2003

The third harmonic generation in the skin-layer of a dense hot plasma due to inverse bremsstrahlung is investigated for regimes having increasing experimental relevance. New analytical dependencies of the radiation flux density at the frequency 3ω on the plasma and fundamental wave parameters are established.

PhysicsBremsstrahlungGeneral Physics and AstronomyInversePlasmaLaserElectromagnetic radiationlaw.inventionRadiation fluxPhysics::Plasma PhysicslawHigh harmonic generationThird harmonicAtomic physicsPhysics Letters A
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Isobar excitation in proton-proton bremsstrahlung

1978

Abstract The contribution of intermediate nucleon isobars to proton-proton bremsstrahlung is calculated in a relativistic model. Using conventional coupling constants and form factors for the exchange of π - and ρ-mesons we find that for photon energies ω > 100 MeV isobar excitation increases the cross section markedly over the prediction of soft-photon calculations. Our results agree well with recent experiments at incident proton energy T lab =730 MeV.

PhysicsCoupling constantNuclear and High Energy PhysicsSoft photonPhotonProtonNuclear TheoryBremsstrahlungNuclear physicsIsobarPhysics::Accelerator PhysicsAtomic physicsNuclear ExperimentNucleonExcitationNuclear Physics A
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Efficiency and dynamic range of the photostimulable x-ray storage material KBr:In

1997

By calibrating the photostimulated luminescence (PSL) response with the known intensity of a standard light source, efficiency of the KBr:In powder material to the x- ray bremsstrahlung exposure at room temperature is estimated. At 44 and 85 kV voltages on the x-ray tube, the values of (8 plus or minus 2) multiplied by 10 5 and (18 plus or minus 4) multiplied by 10 5 photons from 1 mm 2 area of the 1 mm thick material are obtained as PSL responses on a 1 mR x-ray exposure, respectively. Under an assumption of the uniform x-ray excitation within the material, the maximum values for the x-ray irradiation dose and the PSL response both corresponding to the upper limit of linearity range are te…

PhysicsDynamic rangePhotostimulated luminescenceAnalytical chemistryBremsstrahlungX-rayIrradiationLuminescenceSaturation (chemistry)PSLSPIE Proceedings
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