Search results for "PARTICLE PHYSICS"

showing 10 items of 6826 documents

New constraints on R-parity violation from μ–e conversion in nuclei

1998

We derive new constraints on the products of explicitly R-parity violating couplings $\lambda$ and $\lambda'$ in MSSM from searches for \mu-e conversion in nuclei. We concentrate on the loop induced photonic coherent conversion mode. For the combinations $|\lambda\lambda|$ which in \mu-e conversion can be probed only at loop level our constraints are in many cases more stringent than the previous ones due to the enhancement of the process by large $\ln(m^2_f/m^2_{\tilde f}).$ For the combinations of $|\lambda'\lambda'|$ the tree-level \mu-e conversion constraints are usually more restrictive than the loop ones except for two cases which involve the third generation. With the expected improv…

Loop (topology)PhysicsHigh Energy Physics - PhenomenologyNuclear and High Energy PhysicsParticle physicsR-paritySensitivity (control systems)Simetria (Física)LambdaPartícules (Física nuclear)Third generationPhysics Letters B
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Effect ofmconbquark chromomagnetic interaction and on-shell two-loop integrals with two masses

1999

The effect of non-zero c quark mass on b quark HQET Lagrangian, up to 1/mb level, is calculated at two loops. The results are expressed in terms of dilogarithmic functions of mc/mb. This calculation involves on-shell two-loop propagator-type diagrams with two different masses, mb and mc. A general algorithm for reducing such Feynman integrals to the basis of two nontrivial and two trivial integrals is constructed.

Loop (topology)PhysicsNuclear and High Energy PhysicsParticle physicsBasis (linear algebra)BibliographyShell (structure)PropagatorCharm (quantum number)Bottom quarkCharm quarkPhysical Review D
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μ-e conversion in nuclei versus μ→e γ: an effective field theory point of view

1998

Using an effective lagrangian description we analyze possible new physics contributions to the most relevant muon number violating processes: $\mu \to e \gamma$ and $\mu$--$e$ conversion in nuclei. We identify a general class of models in which those processes are generated at one loop level and in which $\mu$--$e$ conversion is enhanced with respect to $\mu \to e \gamma$ by a large $\ln(m^2_\mu/\Lambda^2),$ where $\Lambda$ is the scale responsible for the new physics. For this wide class of models bounds on $\mu$--$e$ conversion constrain the scale of new physics more stringently than $\mu \to e \gamma$ already at present and, with the expected improvements in $\mu$--$e$ conversion experim…

Loop (topology)PhysicsNuclear and High Energy PhysicsParticle physicsMuonViolació CP (Física nuclear)Physics beyond the Standard ModelScalar (mathematics)Effective field theoryScale (descriptive set theory)Order of magnitudePartícules (Física nuclear)Lepton
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Two-loop QED Corrections to Bhabha Scattering

2006

Recent developments in the calculation of the NNLO corrections to the Bhabha scattering differential cross section in pure QED are briefly reviewed and discussed.

Loop (topology)Scattering cross-sectionPhysicsHigh Energy Physics - PhenomenologyNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - Phenomenology (hep-ph)Nuclear TheoryFOS: Physical sciencesPhysics::History of PhysicsAtomic and Molecular Physics and OpticsBhabha scatteringNuclear Physics B - Proceedings Supplements
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Three-gluon Green functions: low-momentum instanton dominance and zero-crossing

2016

International audience; We will report on a some efforts recently made in order to gain a better understanding of some IR properties of the 3-point gluon Green function by following both lattice and continuum QCD approaches.

Low-momentumParticle physicsInstantonQC1-999High Energy Physics::Lattice01 natural sciencesGluonTheoretical physicsLattice (order)quantum chromodynamics0103 physical sciencesddc:530010306 general physicsGreen functionslatticePhysicsQuantum chromodynamics010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologygluonZero crossingGluonZero-crossing[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]instantonHigh Energy Physics::Experimentmomentum: lowEPJ Web of Conferences
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Interaction Control of Robotic Manipulators Without Force Measurement

2010

This paper deals with a new adaptive force-position control of a robotic manipulator based on force estimation. Based on Lyapunov techniques will be proved that the control law guaranties tracking of the desired Cartesian trajectory along the contact plane and of a constant desired force along reciprocal direction, without force measuring. Extensive simulations with 2-DOF manipulator illustrates the followed approach.

Lyapunov functionAdaptive controlRobotic manipulators control adaptive control interaction control.Computer scienceRobot manipulatorControl engineeringTracking (particle physics)Computer Science::Roboticssymbols.namesakeSettore ING-INF/04 - AutomaticaControl theoryTrajectorysymbolsManipulatorConstant (mathematics)
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Adaptive predictor control for stabilizing pressure in a managed pressure drilling system under time-delay

2016

Abstract In this paper, we address adaptive predictor feedback design for a simplified ODE drilling system in the presence of unknown parameter, disturbance and time-delay. The main objective is to stabilize the bottomhole pressure at a critical depth at a desired set-point directly. The time-delay in the transmission line of the drilling systems is considered. The stabilization of the dynamic system and the asymptotic tracking are demonstrated by the proposed predictor control, where the adaptation employs Lyapunov update law design with normalization. The proposed method is evaluated using a high fidelity drilling simulator and cases from a North Sea drilling operation are simulated. The …

Lyapunov functionNormalization (statistics)0209 industrial biotechnologyEngineeringAdaptive controlbusiness.industryOde0102 computer and information sciences02 engineering and technologyTracking (particle physics)01 natural sciencesIndustrial and Manufacturing EngineeringComputer Science ApplicationsCompensation (engineering)symbols.namesake020901 industrial engineering & automation010201 computation theory & mathematicsControl and Systems EngineeringTransmission lineControl theoryModeling and SimulationsymbolsbusinessSimulationJournal of Process Control
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On eleven-dimensional supergravity and chern?SIMONS Theory

2012

We probe in some depth into the structure of eleven-dimensional, osp(32|1)-based Chern-Simons supergravity, as put forward by Troncoso and Zanelli (TZ) in 1997. We find that the TZ Lagrangian may be cast as a polynomial in 1/l, where l is a length, and compute explicitly the first three dominant terms. The term proportional to 1/l^9 turns out to be essentially the Lagrangian of the standard 1978 supergravity theory of Cremmer, Julia and Scherk, thus establishing a previously unknown relation between the two theories. The computation is nontrivial because, when written in a sufficiently explicit way, the TZ Lagrangian has roughly one thousand non-explicitly Lorentz-covariant terms. Specially…

M-theoryPhysicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsPolynomialSupergravityChern–Simons theoryStructure (category theory)FOS: Physical sciencesMathematical Physics (math-ph)Term (logic)High Energy Physics - Theory (hep-th)Higher-dimensional supergravityAlgebraic numberMathematical PhysicsMathematical physics
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New analysis of ηπ tensor resonances measured at the COMPASS experiment

2018

We present a new amplitude analysis of the $\eta\pi$ $D$-wave in $\pi^- p\to \eta\pi^- p$ measured by COMPASS. Employing an analytical model based on the principles of the relativistic $S$-matrix, we find two resonances that can be identified with the $a_2(1320)$ and the excited $a_2^\prime(1700)$, and perform a comprehensive analysis of their pole positions. For the mass and width of the $a_2$ we find $M=(1307 \pm 1 \pm 6)$~MeV and $\Gamma=(112 \pm 1 \pm 8)$~MeV, and for the excited state $a_2^\prime$ we obtain $M=(1720 \pm 10 \pm 60)$~MeV and $\Gamma=(280\pm 10 \pm 70)$~MeV, respectively.

M012M311.80.EtCOMPASS01 natural sciencesHigh Energy Physics - ExperimentUNITARITYSubatomär fysikPomeronCompassexcited stateSubatomic PhysicsNuclear and high energy physics; peripheral photoproduction; physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]COMPASS experimentEXCHANGEa2(1320)Nuclear Experimenta2(1700)Quantum chromodynamicsPhysicsUnitarityPP INTERACTIONShep-phamplitude analysisMESONSlcsh:QC1-999analytic propertiesHigh Energy Physics - PhenomenologyAmplitudeS-matrixphysicsParticle Physics - ExperimentAMPLITUDE ANALYSISNuclear and High Energy PhysicsParticle physicsMeson530CONNECTIONPHYSICS14.40.Be[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]pomeron0103 physical sciencesperipheral photoproductionddc:530Tensor010306 general physicsM012W3Particle Physics - PhenomenologyPOMERONhep-ex010308 nuclear & particles physicsM162M11.55.Bq11.55.Fvmeson resonanceM162WPhysics and Astronomy450 GEV/C[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph][ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::ExperimentMATRIXlcsh:PhysicsPhysics Letters B
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NEXT-100 Technical Design Report (TDR). Executive summary

2012

[EN] In this Technical Design Report (TDR) we describe the NEXT-100 detector that will search for neutrinoless double beta decay (ßß0v) in 136XE at the Laboratorio Subterráneo de Canfranc (LSC), in Spain. The document formalizes the design presented in our Conceptual Design Report (CDR): an electroluminescence time projection chamber, with separate readout planes for calorimetry and tracking, located, respectively, behind cathode and anode. The detector is designed to hold a maximum of about 150 kg of xenon at 15 bar, or 100 kg at 10 bar. This option builds in the capability to increase the total isotope mass by 50% while keeping the operating pressure at a manageable level. The readout pla…

MECANICA DE LOS MEDIOS CONTINUOS Y TEORIA DE ESTRUCTURASPhotomultiplierPhysics - Instrumentation and DetectorsBar (music)Time projection chambersFOS: Physical scienceschemistry.chemical_elementWavelength shifterTracking (particle physics)7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentTECNOLOGIA ELECTRONICAHigh Energy Physics - Experiment (hep-ex)chemistry.chemical_compoundXenonOptics0103 physical sciences010306 general physicsInstrumentationMathematical PhysicsPhysicsTime projection chamber010308 nuclear & particles physicsbusiness.industryDetectorFísicaTetraphenyl butadieneDetectorsInstrumentation and Detectors (physics.ins-det)Gas detectorsDetectors de gasoschemistryDetector design and construction technologies and materialsbusinessJournal of Instrumentation
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