Search results for "loop"

showing 10 items of 608 documents

Dynamics for a 2-vertex Quantum Gravity Model

2010

We use the recently introduced U(N) framework for loop quantum gravity to study the dynamics of spin network states on the simplest class of graphs: two vertices linked with an arbitrary number N of edges. Such graphs represent two regions, in and out, separated by a boundary surface. We study the algebraic structure of the Hilbert space of spin networks from the U(N) perspective. In particular, we describe the algebra of operators acting on that space and discuss their relation to the standard holonomy operator of loop quantum gravity. Furthermore, we show that it is possible to make the restriction to the isotropic/homogeneous sector of the model by imposing the invariance under a global …

PhysicsPhysics and Astronomy (miscellaneous)[PHYS.GRQC] Physics [physics]/General Relativity and Quantum Cosmology [gr-qc]010308 nuclear & particles physicsHolonomyHilbert spaceFOS: Physical sciencesLoop quantum gravityGeneral Relativity and Quantum Cosmology (gr-qc)01 natural sciencesGeneral Relativity and Quantum CosmologyVertex (geometry)symbols.namesakeOperator (computer programming)0103 physical sciencesPhysical Sciencessymbols[PHYS.GRQC]Physics [physics]/General Relativity and Quantum Cosmology [gr-qc]Quantum gravitySpin network010306 general physicsLoop quantum cosmologyMathematical physics
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TIME-RESOLVED EMISSION FROM BRIGHT HOT PIXELS OF AN ACTIVE REGION OBSERVED IN THE EUV BAND WITH SDO/AIA AND MULTI-STRANDED LOOP MODELING

2015

Evidence for small amounts of very hot plasma has been found in active regions and might be the indication of an impulsive heating, released at spatial scales smaller than the cross section of a single loop. We investigate the heating and substructure of coronal loops in the core of one such active region by analyzing the light curves in the smallest resolution elements of solar observations in two EUV channels (94 A and 335 A) from the Atmospheric Imaging Assembly on-board the Solar Dynamics Observatory. We model the evolution of a bundle of strands heated by a storm of nanoflares by means of a hydrodynamic 0D loop model (EBTEL). The light curves obtained from the random combination of tho…

PhysicsPixelSun: coronaExtreme ultraviolet lithographyFOS: Physical sciencesAstronomy and AstrophysicsPlasmaCoronal loopAstronomy and AstrophysicLight curveSun: UV radiationPower lawNanoflaresComputational physicsSettore FIS/05 - Astronomia E AstrofisicaAstrophysics - Solar and Stellar AstrophysicsSun: activitySpace and Planetary ScienceSubstructureSolar and Stellar Astrophysics (astro-ph.SR)
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Quantum Search with Multiple Walk Steps per Oracle Query

2015

We identify a key difference between quantum search by discrete- and continuous-time quantum walks: a discrete-time walk typically performs one walk step per oracle query, whereas a continuous-time walk can effectively perform multiple walk steps per query while only counting query time. As a result, we show that continuous-time quantum walks can outperform their discrete-time counterparts, even though both achieve quadratic speedups over their corresponding classical random walks. To provide greater equity, we allow the discrete-time quantum walk to also take multiple walk steps per oracle query while only counting queries. Then it matches the continuous-time algorithm's runtime, but such …

PhysicsQuantum PhysicsSpeedupLoop-erased random walkFOS: Physical sciencesRandom walk01 natural sciencesAtomic and Molecular Physics and OpticsOracleQuantum search010305 fluids & plasmasQuadratic equationMathematics::Probability0103 physical sciencesKey (cryptography)Quantum walkQuantum Physics (quant-ph)010306 general physicsAlgorithmComputer Science::Databases
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Three-loop relation of quark $$\overline {MS} $$ and pole masses

1990

We calculate, exactly, the next-to-leading correction to the relation between the $$\overline {MS} $$ quark mass, $$\bar m$$ , and the scheme-independent pole mass,M, and obtain $$\begin{gathered} \frac{M}{{\bar m(M)}} \approx 1 + \frac{4}{3}\frac{{\bar \alpha _s (M)}}{\pi } + \left[ {16.11 - 1.04\sum\limits_{i = 1}^{N_F - 1} {(1 - M_i /M)} } \right] \hfill \\ \cdot \left( {\frac{{\bar \alpha _s (M)}}{\pi }} \right)^2 + 0(\bar \alpha _s^3 (M)), \hfill \\ \end{gathered} $$ as an accurate approximation forN F−1 light quarks of massesM i <M. Combining this new result with known three-loop results for $$\overline {MS} $$ coupling constant and mass renormalization, we relate the pole mass to the…

PhysicsQuantum chromodynamicsCoupling constantQuarkParticle physicsPhysics and Astronomy (miscellaneous)High Energy Physics::PhenomenologyPropagatorElementary particleLoop (topology)RenormalizationHigh Energy Physics::ExperimentEngineering (miscellaneous)Bar (unit)Zeitschrift für Physik C Particles and Fields
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Soft-virtual corrections to Higgs production atN3LO

2015

The authors compute certain (soft-virtual) corrections to the Higgs boson production in the gluon-gluon fusion at next-to-next-to-next-to-leading order in QCD. Such higher loop calculations are essential for comparing the theoretical predictions with the experimental results of the Higgs boson production at LHC.

PhysicsQuantum chromodynamicsLoop (topology)Nuclear and High Energy PhysicsHiggs fieldParticle physicsLarge Hadron ColliderHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHiggs bosonDrell–Yan processHigh Energy Physics::ExperimentProduction (computer science)Physical Review D
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Infrared singularities in one-loop amplitudes

2010

In this talk we discuss a purely numerical approach to next-to-leading order calculations in QCD. We present a simple formula, which provides a local infrared subtraction term for the integrand of a one-loop amplitude. In addition we briefly comment on local ultraviolet subtraction terms and on the required deformation of the contour of integration.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsInfraredSubtractionFOS: Physical sciencesTerm (logic)Atomic and Molecular Physics and OpticsLoop (topology)High Energy Physics - PhenomenologyAmplitudeClassical mechanicsHigh Energy Physics - Phenomenology (hep-ph)Simple (abstract algebra)Gravitational singularity
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Combined relativistic and static analysis for all DB = 2 operators

2001

We analyse matrix elements of Delta B=2 operators by combining QCD results with the ones obtained in the static limit of HQET. The matching of all the QCD operators to HQET is made at NLO order. To do that we have to include the anomalous dimension matrix up to two loops, both in QCD and HQET, and the one loop matching for all the Delta B=2 operators. The matrix elements of these operators are relevant for the prediction of the B-\bar B mixing, B_s meson width difference and supersymmetric effects in Delta B=2 transitions.

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesStatic analysisAtomic and Molecular Physics and OpticsLoop (topology)High Energy Physics - PhenomenologyMatrix (mathematics)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Mixing (mathematics)Dimension (vector space)Física nuclearHigh Energy Physics::ExperimentLimit (mathematics)
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N3LOHiggs boson and Drell-Yan production at threshold: The one-loop two-emission contribution

2014

In this paper, we study phenomenologically interesting soft radiation distributions in massless QCD. Specifically, we consider the emission of two soft partons off of a pair of lightlike Wilson lines, in either the fundamental or the adjoint representation, at next-to-leading order. Our results are an essential component of the next-to-next-to-next-to-leading order threshold corrections to both Higgs boson production in the gluon fusion channel and Drell-Yan lepton production. Our calculations are consistent with the recently published results for Higgs boson production. As a nontrivial cross-check on our analysis, we rederive a recent prediction for the Drell-Yan threshold cross section us…

PhysicsQuantum chromodynamicsNuclear and High Energy PhysicsParticle physicsWilson loop010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyDrell–Yan process01 natural sciencesGluonMassless particleDimensional regularization0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsLeptonPhysical Review D
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Foundations of the Quantum Chromodynamics

2015

Quantum chromodynamics (QCD) is a theory to describe the strong interaction in hadrons. It was developed in the history of understanding the structure of the hadrons. In the 1950s, a large number of hadrons were discovered in experiments.

PhysicsQuantum chromodynamicsParticle physicsHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyHadronStrong interactionStructure (category theory)High Energy Physics::ExperimentNuclear ExperimentLoop integral
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Quark mass dependence of the one-loop three-gluon vertex in arbitrary dimension

2001

The one-loop off-shell massive quark contribution to the three-gluon vertex is calculated in an arbitrary space-time dimension. The results for all relevant on-shell and symmetric limits are obtained directly from the general off-shell results. The analytic structure of the results for the relevant massive scalar integrals is also discussed.

PhysicsQuarkNuclear and High Energy PhysicsLoop (graph theory)Particle physicsScalar (mathematics)Nuclear TheoryStructure (category theory)FOS: Physical sciencesGluonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Dimension (vector space)Vertex (curve)Physics::Atomic and Molecular ClustersMathematical physics
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