Search results for "positron"

showing 10 items of 1346 documents

Improved measurements of the branching fractions forB0→π+π−andB0→K+π−, and a search forB0→K+K−

2007

We present measurements of the branching fractions for the charmless two-body decays B0→π+π- and B0→K+π-, and a search for the decay B0→K+K-. We include the effects of final-state radiation from the daughter mesons for the first time, and quote branching fractions for the inclusive processes B0→h+h′-nγ, where h and h′ are pions or kaons. The maximum value of the sum of the energies of the n undetected photons, Eγmax, is mode-dependent. Using a data sample of approximately 227×106 Υ(4S)→BB decays collected with the BABAR detector at the PEP-II asymmetric-energy e+e- collider at SLAC, we measure: B(B0→π+π-nγ;Eγmax =150MeV)=(5.1±0.4±0.2) ×10-6, B(B0→K+π-nγ;Eγmax =105MeV)=(18.1±0. 6±0.6)×10-6, …

PhysicsNuclear and High Energy PhysicsPhotonMeson010308 nuclear & particles physicsBranching fractionElectron–positron annihilationTwo-body problem01 natural sciencesNuclear physicsParticle decayPionPair production0103 physical sciences010306 general physicsPhysical Review D
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Timing results using an FPGA-based TDC with large arrays of 144 SiPMs

2015

Silicon photomultipliers (SiPMs) have become an alternative to traditional tubes due to several features. However, their implementation to form large arrays is still a challenge especially due to their relatively high intrinsic noise, depending on the chosen readout. In this contribution, two modules composed of SiPMs with an area of roughly mm mm are used in coincidence. Coincidence resolving time (CRT) results with a field-programmable gate array, in combination with a time to digital converter, are shown as a function of both the sensor bias voltage and the digitizer threshold. The dependence of the CRT on the sensor matrix temperature, the amount of SiPM active area and the crystal type…

PhysicsNuclear and High Energy PhysicsPixelbusiness.industryDetectorBiasingNoise (electronics)Time-to-digital converterFull width at half maximumSilicon radiation detectorsSilicon photomultiplierOpticsNuclear Energy and EngineeringGate arrayPositron emission tomography (PET)Nuclear medicineTEORIA DE LA SEÑAL Y COMUNICACIONESElectronic engineeringTrigger circuitsElectrical and Electronic Engineeringbusiness
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The binding energy of 184 476 X in the droplet model

1985

The positron spectrum emitted in the U-U-reaction at subthreshold energy could be interpreted in terms of the formation of a giant nucleus if the binding of the latter is 100 MeV stronger than predicted by the usual droplet model parametrisation. We analyse the extrapolation to giant nuclei by accounting properly for the error propagation when the parameters are fitted to measured binding energies and radii. The influence of higher order terms is discussed.

PhysicsNuclear and High Energy PhysicsPropagation of uncertaintySubthreshold conductionNuclear TheoryBinding energyExtrapolationmedicine.anatomical_structurePositronmedicineNuclear fusionAtomic physicsNuclear ExperimentNucleusZeitschrift f�r Physik A Atoms and Nuclei
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Recoil-beta tagging: A novel technique for studying proton-drip-line nuclei

2006

Abstract Tagging with charged particles and γ -rays at the focal plane of recoil separators has proven, over the last two decades, to be a very powerful tool for the identification of excited states in exotic nuclei produced with very low cross-sections. One of the key areas so far unexplored in terms of the tagging methodology has been performing correlations with β -particles at the focal plane of a recoil separator. A new technique entitled Recoil-Beta Tagging (RBT) has been developed, this technique exploits the unusual properties of Fermi super-allowed β emitters, which have both a short half-life ( ∼ 100 ms ) and high β + -endpoint energy. Correlating with such β -particles using a do…

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsDetector[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesCharged particleSemiconductor detectorNuclear physicsRecoilPositronExcited state27.50.þe; 29.30.Kv; 29.40.Wk0103 physical sciencesAtomic physics010306 general physicsNuclear ExperimentInstrumentationFermi Gamma-ray Space Telescope
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Measurement of the proton form factor by studyinge+e−→pp¯

2015

Using data samples collected with the BESIII detector at the BEPCII collider, we measure the Born cross section of e(+)e(-) -> p (p) over tilde at 12 center-of-mass energies from 2232.4 to 3671.0 MeV. The corresponding effective electromagnetic form factor of the proton is deduced under the assumption that the electric and magnetic form factors are equal (vertical bar G(E)vertical bar = vertical bar G(M)vertical bar). In addition, the ratio of electric to magnetic form factors, vertical bar G(E)/G(M)vertical bar, and vertical bar G(M)vertical bar are extracted by fitting the polar angle distribution of the proton for the data samples with larger statistics, namely at root s = 2232.4 and 240…

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsElectron–positron annihilationHigh Energy Physics::PhenomenologyForm factor (quantum field theory)01 natural sciences7. Clean energyVertical barlaw.inventionNuclear physicsCross section (physics)Distribution (mathematics)law0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsNucleonColliderPhysical Review D
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A device to measure the effects of strong magnetic fields on the image resolution of PET scanners

2009

Abstract Very high resolution images can be achieved in small animal PET systems utilizing solid state silicon pad detectors. As these systems approach sub-millimeter resolutions, the range of the positron is becoming the dominant contribution to image blur. The size of the positron range effect depends on the initial positron energy and hence the radioactive tracer used. For higher energy positron emitters, such as Ga 68 and Tc 94 m , which are gaining importance in small animal studies, the width of the annihilation point distribution dominates the spatial resolution. This positron range effect can be reduced by embedding the field of view of the PET scanner in a strong magnetic field. In…

PhysicsNuclear and High Energy PhysicsRadioactive tracerAnnihilationPhysics::Instrumentation and Detectorsbusiness.industryResolution (electron density)DetectorField of viewlaw.inventionMagnetic fieldOpticsNuclear magnetic resonancePositronlawPhysics::Accelerator PhysicsbusinessInstrumentationImage resolutionNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Initial-state radiation measurement of thee+e−→π+π−π+π−cross section

2012

We study the process e+e- -> pi+pi-pi+pi-gamma, with a photon emitted from the initial-state electron or positron, using 454.3 fb^-1 of data collected with the BABAR detector at SLAC, corresponding to approximately 260,000 signal events. We use these data to extract the non-radiative sigma(e+e- ->pi+pi-pi+pi-) cross section in the energy range from 0.6 to 4.5 Gev. The total uncertainty of the cross section measurement in the peak region is less than 3%, higher in precision than the corresponding results obtained from energy scan data.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Photon010308 nuclear & particles physicsDetectorElectron01 natural sciencesNuclear physicsCross section (physics)Positron0103 physical sciencesPiHigh Energy Physics::ExperimentAtomic physics010306 general physicsEnergy (signal processing)Physical Review D
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High energy gamma ray counterparts of astrophysical sources of ultra-high energy cosmic rays

2004

If ultra-high energy cosmic rays (UHECRs) are accelerated at astrophysical point sources, the identification of such sources can be achieved if there is some kind of radiation at observable wavelengths that may be associated with the acceleration and/or propagation processes. No radiation of this type has so far been detected or at least no such connection has been claimed. The process of photopion production during the propagation of UHECRs from the sources to the Earth results in the generation of charged and neutral pions. The neutral (charged) pions in turn decay to gamma quanta and electrons that initiate an electromagnetic cascade in the universal photon background. We calculate the f…

PhysicsNuclear and High Energy PhysicsRange (particle radiation)PhotonAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)Astrophysics::Instrumentation and Methods for AstrophysicsGamma rayFOS: Physical sciencesAstronomy and AstrophysicsCosmic rayElectronAstrophysicsRadiationAstrophysicsAtomic and Molecular Physics and OpticsNuclear physicsPositronPionIntergalactic travelUltra-high-energy cosmic rayAstroparticle Physics
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Preliminary assessment of the imaging capability of the YAP–(S)PET small animal scanner in neuroscience

2006

The new and fully engineered version of the YAP–(S)PET small animal scanner has been tested at the University of Mainz for preliminary assessment of its imaging capability for studies related to neuropharmacology and psychiatry. The main feature of the scanner is the capability to combine PET and SPECT techniques. It allows the development of new and interesting protocols for the investigation of many biological phenomena, more effectively than with PET or SPECT modalities alone. The scanner is made up of four detector heads, each one composed of a 4 � 4c m 2 of YAlO3:Ce (or YAP:Ce) matrix, and has a field of view (FOV) of 4 cm axially � 4c m + transaxially. In PET mode, the volume resoluti…

PhysicsNuclear and High Energy PhysicsScannermedicine.medical_specialtymedicine.diagnostic_testDetectorCollimatorField of viewSingle-photon emission computed tomographylaw.inventionFeature (computer vision)lawPositron emission tomographySmall animalmedicineMedical physicsInstrumentationBiomedical engineeringNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Weak magnetic dipole moments in two-Higgs-doublet models

1995

We investigate the effects of the new scalars in a two-Higgs-doublet model on the weak magnetic dipole moments of the fermions at the $Z$ peak. Proportionality of the Yukawa couplings to the fermion masses, and to $\tan{\beta}$, makes such effects more important for the third family, and potentially relevant. For the $\tau$ lepton, the new diagrams are suppressed by $v_\tau = 2 \sin^2 \theta_W - 1/2$, or by powers of $m_\tau/M_Z$, but may still be comparable to the SM electroweak contributions. In contrast, we find that the new contributions for the bottom quark may be much larger than the SM electroweak contributions. These new effects may even compete with the gluonic contribution, if the…

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsElectron–positron annihilationHigh Energy Physics::LatticeElectroweak interactionHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesFísicaFermionBottom quarkHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentLepton
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