Search results for " Generator"

showing 10 items of 328 documents

Gyrotron-driven high current ECR ion source for boron-neutron capture therapy neutron generator

2014

Abstract Boron-neutron capture therapy (BNCT) is a perspective treatment method for radiation resistant tumors. Unfortunately its development is strongly held back by a several physical and medical problems. Neutron sources for BNCT currently are limited to nuclear reactors and accelerators. For wide spread of BNCT investigations more compact and cheap neutron source would be much more preferable. In present paper an approach for compact D–D neutron generator creation based on a high current ECR ion source is suggested. Results on dense proton beams production are presented. A possibility of ion beams formation with current density up to 600 mA/cm 2 is demonstrated. Estimations based on obt…

PhysicsNuclear and High Energy Physicsta114Nuclear engineeringPhysics::Medical PhysicsNuclear TheoryRadiationIon sourcelaw.inventionNeutron captureNeutron generatorNeutron fluxlawGyrotronNeutron sourceNeutronNuclear ExperimentInstrumentationta217Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Two-photon widths of theχc0,2states and helicity analysis forχc2→γγ

2012

Based on a data sample of 106 X 10(6) psi' events collected with the BESIII detector, the decays psi' -> gamma chi(c0,2), chi(c0,2) -> gamma gamma are studied to determine the two-photon widths of the chi(c0,2) states. The two-photon decay branching fractions are determined to be B(chi(c0) -> gamma gamma) = (2.24 +/- 0.19 +/- 0.12 +/- 0.08) X 10(-4) and B(chi(c2) -> gamma gamma) = (3.21 +/- 0.18 +/- 0.17 +/- 0.13) X 10(-4) From these, the two-photon widths are determined to be Gamma(gamma gamma)(chi(c0)) = (2.33 +/- 0.20 +/- 0.13 +/- 0.17) keV, Gamma(gamma gamma)(chi(c2)) = (0.63 +/- 0.04 +/- 0.04 +/- 0.04) keV, and R = Gamma(gamma gamma)(chi(c2))/Gamma(gamma gamma)(chi(c0)) = 0.271 +/- 0.0…

PhysicsNuclear physicsNuclear and High Energy PhysicsAnnihilationElectron–positron annihilationLambdaWidth ratioHelicityEvent generatorGamma gammaPhysical Review D
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Correlations of intermediate mass fragments from Fe+Ta, Au, and Th collisions.

1995

Charge, velocity, and angular correlations between intermediate mass fragments (IMF) are presented for 50 and 100 MeV/nucleon Fe bombardments of Ta, Au, and Th targets. Correlation functions generated as a function of the relative velocity and the opening angle between two IMF's are qualitatively independent of the projectile energy and target mass and show a suppression at small relative velocities and opening angles due to the Coulomb repulsion between the fragments. The correlations are consistent with IMF's emitted primarily from a highly excited target residue following a rapid preequilibrium cascade. The correlation data are compared to model calculations using the event generator men…

PhysicsNuclear reactionNuclear and High Energy PhysicsProjectileNuclear TheoryRelative velocityCharge (physics)Nuclear matterNuclear physicsExcited stateAtomic physicsNuclear ExperimentNucleonEvent generatorPhysical review. C, Nuclear physics
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Electron-positron annihilation into three pions and the radiative return

2005

The Monte Carlo event generator PHOKHARA, which simulates hadron and muon production at electron-positron colliders through radiative return, has been extended to final states with three pions. A model for the form factor based on generalized vector dominance has been employed, which is consistent with presently available experimental observations.

PhysicsParticle physicsMuonPhysics and Astronomy (miscellaneous)Electron–positron annihilationHadronMonte Carlo methodForm factor (quantum field theory)FísicaFOS: Physical sciencesHigh Energy Physics - PhenomenologyPionHigh Energy Physics - Phenomenology (hep-ph)Radiative transferPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentEngineering (miscellaneous)Event generator
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The radiative return at phi- and B-factories: FSR for muon pair production at next-to-leading order

2004

Muon pair production through the radiative return is of importance for a measurement of the hadronic production cross section in two ways: it provides an independent calibration and it may give rise to an important background for a measurement of the pion form factor. With this motivation the Monte Carlo event generator PHOKHARA is extended to include next-to-leading order radiative corrections to the reaction $e^+e^-\to \mu^+\mu^-\gamma$. Furthermore, virtual ISR corrections to FSR from pions are introduced, which extends the applicability of the generator into a new kinematical regime. Finally, the effect of photon vacuum polarization is introduced into this new version of the generator.

PhysicsParticle physicsMuonPhysics and Astronomy (miscellaneous)Monte Carlo methodForm factor (quantum field theory)FOS: Physical sciencesFísicaHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Pair productionPionRadiative transferHigh Energy Physics::ExperimentVacuum polarizationNuclear ExperimentEngineering (miscellaneous)Particle Physics - PhenomenologyEvent generator
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Nucleon form factors, B-meson factories and the radiative return

2004

The feasibility of a measurement of the electric and magnetic nucleon form factors at $B$-meson factories through the radiative return is studied. Angular distributions allow a separation of the contributions from the two form factors. The distributions are presented for the laboratory and the hadronic rest frame, and the advantages of different coordinate systems are investigated. It is demonstrated that $Q^2$ values up to 8 or even 9 GeV$^2$ are within reach. The Monte Carlo event generator PHOKHARA is extended to nucleon final states, and results are presented which include Next-to-Leading Order radiative corrections from initial-state radiation. The impact of angular cuts on rates and d…

PhysicsParticle physicsPhysics and Astronomy (miscellaneous)Nuclear TheoryHadronMonte Carlo methodCoordinate systemFOS: Physical sciencesFísicaRest frameHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Radiative transferB mesonNuclear Experiment (nucl-ex)NucleonEngineering (miscellaneous)Nuclear ExperimentEvent generatorParticle Physics - Phenomenology
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Results from bottomonia production at the Tevatron and prospects for the LHC

2000

We extend our previous analysis on inclusive heavy quarkonia hadroproduction to the whole Upsilon(nS) (n=1,2,3) resonance family. We use a Monte Carlo framework with the colour-octet mechanism implemented in the PYTHIA event generator. We include in our study higher order QCD effects such as initial-state emission of gluons and Altarelli-Parisi evolution of final-state gluons. We extract some NRQCD colour-octet matrix elements relevant for Upsilon(nS) (n=1,2,3) hadroproduction from CDF data at the Fermilab Tevatron. Then we extrapolate to LHC energies to predict prompt bottomonia production rates. Finally, we examine the prospect to probe the gluon density in protons from heavy quarkonia in…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderHigh Energy Physics::LatticeMonte Carlo methodHigh Energy Physics::PhenomenologyTevatronFOS: Physical sciencesFísicaResonance (particle physics)GluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentFermilabNuclear ExperimentParticle Physics - PhenomenologyEvent generator
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Strongly super-Poisson statistics replaced by a wide-pulse Poisson process: The billiard random generator

2021

Abstract In this paper we present a study on random processes consisting of delta pulses characterized by strongly super-Poisson statistics and calculate its spectral density. We suggest a method for replacing a strongly super-Poisson process with a wide-pulse Poisson process, while demonstrating that these two processes can be set in such a way to have similar spectral densities, the same mean values, and the same correlation times. We also present a billiard system that can be used to generate random pulse noise of arbitrary statistical properties. The particle dynamics is considered in terms of delta and wide pulses simultaneously. The results of numerical experiments with the billiard s…

PhysicsSettore FIS/02 - Fisica Teorica Modelli E Metodi MatematiciStochastic processGeneral MathematicsApplied MathematicsGeneral Physics and AstronomySpectral densityStatistical and Nonlinear PhysicsPoisson distributionRenewal processPulse (physics)symbols.namesakeBilliard-like systemsStochastic processessymbolsHardware random number generatorFluctuation phenomenaStatistical physicsRenewal theoryHardware random number generatorDynamical billiardsSuper-Poisson statisticsGenerator (mathematics)Chaos, Solitons & Fractals
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Low-noise microvolt level calibrator for measurement of performance of biosignal recording systems

1997

A calibrator, the noise level of which is below the noise level generated in the preamplifier system, was needed for testing and development of a multichannel recording system. A multichannel preamplifier head assembly was used for recording cortical, subcortical, and cerebellar slow potentials and multiunit activity in freely moving cats and restrained rabbits. An inexpensive, battery-powered, lownoise voltage signal generator for calibration of the preamplifiers is described. The circuit provides a square-wave output at a frequency of 10 or 1000 Hz, and the peak-to-peak (p-p) amplitude can be selected at 10, 100, or 1000µV. The measured output noise of the calibrator is below 2µV (p-p, 0.…

PhysicsSignal generatorNoise (signal processing)Preamplifierbusiness.industryAcousticsExperimental and Cognitive PsychologyAmplitudeCalibrationPsychology (miscellaneous)BiosignalOscilloscopeTelecommunicationsbusinessGeneral PsychologyVoltageBehavior Research Methods, Instruments, & Computers
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Photonically assisted RF generator with incoherent sources

2008

An RF waveform generator operating with incoherent broadband light is successfully implemented. Complex RF ~10 GHz bandwidth waveforms are generated by means of incoherent wavelength-to-time mapping. Our technique can be scaled to the mm-wave range.

PhysicsSignal generatorbusiness.industryBandwidth (signal processing)ComputingMilieux_PERSONALCOMPUTINGElectrical engineeringBroadband communicationOpticsBroadbandHardware_INTEGRATEDCIRCUITSWaveformBroadband amplifiersRadio frequencyPhotonicsbusinessOECC/ACOFT 2008 - Joint Conference of the Opto-Electronics and Communications Conference and the Australian Conference on Optical Fibre Technology
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