789 research outputs found
Understanding the Kalman Filter: an Object Oriented Programming Perspective.
The basic ideals underlying the Kalman filter are outlined in this paper without direct recourse to the complex formulae normally associated with this method. The novel feature of the paper is its reliance on a new algebraic system based on the first two moments of the multivariate normal distribution. The resulting framework lends itself to an object-oriented implementation on computing machines and so many of the ideas are presented in these terms. The paper provides yet another perspective of Kalman filtering, one that many should find relatively easy to understand.Time series analysis, forecasting, Kalman filter, dynamic linear statistical models, object oriented programming.
Noncommutative Scalar Field Coupled to Gravity
A model for a noncommutative scalar field coupled to gravity is proposed via
an extension of the Moyal product. It is shown that there are solutions
compatible with homogeneity and isotropy to first non-trivial order in the
perturbation of the star-product, with the gravity sector described by a flat
Robertson-Walker metric. We show that in the slow-roll regime of a typical
chaotic inflationary scenario, noncommutativity has negligible impact.Comment: Revtex4, 6 pages. Final version to appear at Phys. Rev.
Time-Space Noncommutativity in Gravitational Quantum Well scenario
A novel approach to the analysis of the gravitational well problem from a
second quantised description has been discussed. The second quantised formalism
enables us to study the effect of time space noncommutativity in the
gravitational well scenario which is hitherto unavailable in the literature.
The corresponding first quantized theory reveals a leading order perturbation
term of noncommutative origin. Latest experimental findings are used to
estimate an upper bound on the time--space noncommutative parameter. Our
results are found to be consistent with the order of magnitude estimations of
other NC parameters reported earlier.Comment: 7 pages, revTe
phosphorus and potassium fertilizer effects on alfalfa and soil in a non limited soil
Fertilization strategies for high-yielding alfalfa (Medicago sativa L.) should take in account the increase in soil nutritional status that occurred during the last decades in areas with intensive agricultural use. A field study was conducted at the University of Padova, northeastern Italy, to determine the response of alfalfa yield and nutritive value to various combinations of P and K rates in a soil lacking nutrient deficiency. Alfalfa cultivar Delta was seeded in March 2005 on a silt loam soil having 38 mg kg -1 available P and 178 mg kg -1 exchangeable K. Nine treatments deriving from the combination of three P fertilization rates (0, 100, and 200 kg ha -1 P 2 O 5 ) and three K rates (0, 300, and 600 kg ha -1 K 2 O) were compared in a randomized complete block design. Plots were harvested at bud stage during three growing seasons (2005-2007) and dry matter (DM) yield, forage nutritive value, P and K contents, canopy height, and stem density were measured at each harvest. Soil samples were collected at the end of the research period for determination of available P and exchangeable K. The results demonstrated that P application had no impact on yield and did not interact with K in determining productivity, while K had a positive effect on yield. However, the 300 kg ha -1 K 2 O rate appeared sufficient to maximize yield, without adverse effects on the forage nutritive value. Data from soil analyses showed that alfalfa has a high K uptake even when it is fertilized at high rates
Ecological Invasion, Roughened Fronts, and a Competitor's Extreme Advance: Integrating Stochastic Spatial-Growth Models
Both community ecology and conservation biology seek further understanding of
factors governing the advance of an invasive species. We model biological
invasion as an individual-based, stochastic process on a two-dimensional
landscape. An ecologically superior invader and a resident species compete for
space preemptively. Our general model includes the basic contact process and a
variant of the Eden model as special cases. We employ the concept of a
"roughened" front to quantify effects of discreteness and stochasticity on
invasion; we emphasize the probability distribution of the front-runner's
relative position. That is, we analyze the location of the most advanced
invader as the extreme deviation about the front's mean position. We find that
a class of models with different assumptions about neighborhood interactions
exhibit universal characteristics. That is, key features of the invasion
dynamics span a class of models, independently of locally detailed demographic
rules. Our results integrate theories of invasive spatial growth and generate
novel hypotheses linking habitat or landscape size (length of the invading
front) to invasion velocity, and to the relative position of the most advanced
invader.Comment: The original publication is available at
www.springerlink.com/content/8528v8563r7u2742
Kinetic modeling of H-mode pedestal with effects from anomalous transport and MHD stability
Scaling of the H-mode pedestal in tokamak plasmas with type I ELMs and dependence of the pedestal properties and the resulting divertor head load width with the plasma elongation and plasma current are investigated using the kinetic neoclassical XGC0 code for DIII-D and Alcator C-Mod tokamaks. The simulations in this study use realistic diverted geometry and are self-consistent with the inclusion of kinetic neoclassical physics, theory-based anomalous transport models with the EĂB flow shearing effects, as well as an MHD ELM triggering criterion. Scalings for the pedestal width and height are developed as a function of the scanned plasma parameters. The nonlinear interplay between anomalous and neoclassical effects motivates the development of a self-consistent simulation model that includes neoclassical and anomalous effects simultaneously. It is demonstrated that the divertor heat load width depend on the plasma currents. In the development of this dependence, effects of neutral collisions and anomalous transport are taken into account. Changes in the neoclassical divertor heat load fluxes associated with the introduction of the neutral collision and anomalous transport effects are described.ĐĐ° ĐŽĐŸĐżĐŸĐŒĐŸĐłĐŸŃ ĐșŃĐœĐ”ŃĐžŃĐœĐŸĐłĐŸ ĐœĐ”ĐŸĐșлаŃĐžŃĐœĐŸĐłĐŸ ĐșĐŸĐŽŃ XGC0 ĐŽĐ»Ń ŃĐŸĐ·ŃŃĐŽŃĐČ ĐČ ŃĐŸĐșĐ°ĐŒĐ°ĐșĐ°Ń
DIII-D Ń Alcator C-Mod ĐŽĐŸŃĐ»ŃĐŽĐ¶Đ”ĐœĐŸ ŃĐșĐ”ĐčĐ»ŃĐœĐł ĐżâŃĐŽĐ”ŃŃĐ°Đ»Ń ĐČ ĐżĐ»Đ°Đ·ĐŒŃ, ŃĐŸ пДŃДбŃĐČĐ°Ń ĐČ ŃĐ”Đ¶ĐžĐŒŃ ĐżĐŸĐ»ŃĐżŃĐ”ĐœĐŸĐłĐŸ ŃŃŃĐžĐŒĐ°ĐœĐœŃ, Đ· ĐżŃĐžĐșĐŸŃĐŽĐŸĐœĐœĐžĐŒĐž Đ»ĐŸĐșĐ°Đ»ŃĐ·ĐŸĐČĐ°ĐœĐžĐŒĐž ĐŒĐŸĐŽĐ°ĐŒĐž (ĐĐĐ) пДŃŃĐŸĐłĐŸ ŃОпŃ, ĐČлаŃŃĐžĐČĐŸŃŃŃ ĐżâŃĐŽĐ”ŃŃĐ°Đ»Ń Ń ĐżĐŸŃĐŸĐșŃ ŃДпла ĐœĐ° ĐŽĐžĐČĐ”ŃŃĐŸŃ ĐČ Đ·Đ°Đ»Đ”Đ¶ĐœĐŸŃŃŃ ĐČŃĐŽ ĐČĐžŃŃĐłĐœŃŃĐŸŃŃŃ ĐżĐ»Đ°Đ·ĐŒĐž ŃĐ° ŃŃŃŃĐŒŃ ĐżĐ»Đ°Đ·ĐŒĐž. ĐŁ ŃĐŸĐ·ŃĐ°Ń
ŃĐœĐșĐ°Ń
ĐČĐžĐșĐŸŃĐžŃŃĐŸĐČŃŃŃŃŃŃ: ŃДалŃŃŃĐžŃĐœĐ° ĐłĐ”ĐŸĐŒĐ”ŃŃŃŃ ĐŽĐžĐČĐ”ŃŃĐŸŃĐ°, ĐșŃĐœĐ”ŃĐžŃĐœĐ° ĐŒĐŸĐŽĐ”Đ»Ń ĐŽĐ»Ń ĐœĐ”ĐŸĐșлаŃĐžŃĐœĐžŃ
Đ”ŃĐ”ĐșŃŃĐČ, ĐŒĐŸĐŽĐ”Đ»Ń Đ°ĐœĐŸĐŒĐ°Đ»ŃĐœĐŸĐłĐŸ ŃŃĐ°ĐœŃĐżĐŸŃŃŃ, ŃĐșĐ° ĐČŃĐ°Ń
ĐŸĐČŃŃ Đ”ŃĐ”ĐșŃĐž ŃĐžŃĐ° (ExB)-ĐżĐŸŃĐŸĐșŃĐČ, Ń ŃĐŒĐŸĐČĐž збŃĐŽĐ¶Đ”ĐœĐœŃ ĐĐĐ-ĐœĐ”ŃŃŃĐčĐșĐŸŃŃĐ”Đč. ĐŁ ŃДзŃĐ»ŃŃĐ°ŃŃ ŃĐŸĐ·ŃĐ°Ń
ŃĐœĐșŃĐČ ĐŸŃŃĐžĐŒĐ°ĐœŃ ŃĐșĐ”ĐčĐ»ŃĐœĐłŃ ĐŽĐ»Ń ŃĐžŃĐžĐœĐž Ń ĐČĐžŃĐŸŃĐž ĐżâŃĐŽĐ”ŃŃĐ°Đ»Ń ŃĐș ŃŃĐœĐșŃŃŃ ĐżĐ°ŃĐ°ĐŒĐ”ŃŃŃĐČ ĐżĐ»Đ°Đ·ĐŒĐž. ĐДлŃĐœŃĐčĐœĐ° ĐČĐ·Đ°ŃĐŒĐŸĐŽŃŃ ĐœĐ”ĐŸĐșлаŃĐžŃĐœĐžŃ
Đ”ŃĐ”ĐșŃŃĐČ Ń Đ”ŃĐ”ĐșŃŃĐČ, ĐżĐŸĐČ'ŃĐ·Đ°ĐœĐžŃ
Đ· Đ°ĐœĐŸĐŒĐ°Đ»ŃĐœĐžĐŒ ŃŃĐ°ĐœŃĐżĐŸŃŃĐŸĐŒ, Ń ĐŒĐŸŃĐžĐČĐ°ŃŃŃŃ ĐŽĐ»Ń ŃĐŸĐ·ŃĐŸĐ±ĐșĐž ŃĐ°ĐŒĐŸŃĐ·ĐłĐŸĐŽĐ¶Đ”ĐœĐŸŃ ŃĐžŃДлŃĐœĐŸŃ ĐŒĐŸĐŽĐ”Đ»Ń, ŃĐșĐ° ĐŸĐŽĐœĐŸŃĐ°ŃĐœĐŸ ĐČĐșĐ»ŃŃĐ°Ń Đ”ŃĐ”ĐșŃĐž Đ°ĐœĐŸĐŒĐ°Đ»ŃĐœĐŸĐłĐŸ Ń ĐœĐ”ĐŸĐșлаŃĐžŃĐœĐŸĐłĐŸ ŃŃĐ°ĐœŃĐżĐŸŃŃŃ. ĐĐŸĐșĐ°Đ·Đ°ĐœĐŸ, ŃĐŸ ĐżĐŸŃĐŸĐșĐž ŃДпла ĐœĐ° ĐŽĐžĐČĐ”ŃŃĐŸŃ Đ·Đ°Đ»Đ”Đ¶Đ°ŃŃ ĐČŃĐŽ ĐżĐ»Đ°Đ·ĐŒĐŸĐČĐžŃ
ŃŃŃŃĐŒŃĐČ. йаĐșĐŸĐ¶ ĐżŃДЎŃŃĐ°ĐČĐ»Đ”ĐœĐŸ ŃДзŃĐ»ŃŃĐ°ŃĐž ĐŽĐŸŃĐ»ŃĐŽĐ¶Đ”ĐœĐœŃ Đ·Đ°Đ»Đ”Đ¶ĐœĐŸŃŃŃ ĐœĐ°ĐżŃĐČŃĐžŃĐžĐœĐž ĐżŃĐŸŃŃĐ»ŃĐČ ŃДпла ĐœĐ° ĐŽĐžĐČĐ”ŃŃĐŸŃ ĐČŃĐŽ Đ”ŃĐ”ĐșŃŃĐČ, ĐżĐŸĐČ'ŃĐ·Đ°ĐœĐžŃ
Đ· Đ°ĐœĐŸĐŒĐ°Đ»ŃĐœĐžĐŒ ŃŃĐ°ĐœŃĐżĐŸŃŃĐŸĐŒ Ń Đ·ŃŃĐșĐœĐ”ĐœĐœŃĐŒĐž Đ· ĐœĐ”ĐčŃŃĐ°Đ»ŃĐœĐžĐŒĐž ŃĐ°ŃŃĐžĐœĐșĐ°ĐŒĐž.ĐĄ ĐżĐŸĐŒĐŸŃŃŃ ĐșĐžĐœĐ”ŃĐžŃĐ”ŃĐșĐŸĐłĐŸ ĐœĐ”ĐŸĐșлаŃŃĐžŃĐ”ŃĐșĐŸĐłĐŸ ĐșĐŸĐŽĐ° XGC0 ĐŽĐ»Ń ŃĐ°Đ·ŃŃĐŽĐŸĐČ ĐČ ŃĐŸĐșĐ°ĐŒĐ°ĐșĐ°Ń
DIII-D Đž Alcator C-Mod ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœŃ ŃĐșŃĐčĐ»ĐžĐœĐł ĐżŃДЎДŃŃала ĐČ ĐżĐ»Đ°Đ·ĐŒĐ”, ĐœĐ°Ń
ĐŸĐŽŃŃĐ”ĐčŃŃ ĐČ ŃĐ”Đ¶ĐžĐŒĐ” ŃĐ»ŃŃŃĐ”ĐœĐœĐŸĐłĐŸ ŃĐŽĐ”ŃĐ¶Đ°ĐœĐžŃ, Ń ĐżŃОгŃĐ°ĐœĐžŃĐœŃĐŒĐž Đ»ĐŸĐșĐ°Đ»ĐžĐ·ĐŸĐČĐ°ĐœĐœŃĐŒĐž ĐŒĐŸĐŽĐ°ĐŒĐž (ĐĐĐ) пДŃĐČĐŸĐłĐŸ ŃОпа, Đž Đ·Đ°ĐČĐžŃĐžĐŒĐŸŃŃŃ ŃĐČĐŸĐčŃŃĐČ ĐżŃДЎДŃŃала Đž ĐżĐŸŃĐŸĐșĐ° ŃДпла ĐœĐ° ĐŽĐžĐČĐ”ŃŃĐŸŃ ĐŸŃ ĐČŃŃŃĐœŃŃĐŸŃŃĐž ĐżĐ»Đ°Đ·ĐŒŃ Đž ŃĐŸĐșĐ° ĐżĐ»Đ°Đ·ĐŒŃ. Đ ŃĐ°ŃŃĐ”ŃĐ°Ń
ĐžŃĐżĐŸĐ»ŃĐ·ŃŃŃŃŃ: ŃДалОŃŃĐžŃĐœĐ°Ń ĐłĐ”ĐŸĐŒĐ”ŃŃĐžŃ ĐŽĐžĐČĐ”ŃŃĐŸŃĐ°, ĐșĐžĐœĐ”ŃĐžŃĐ”ŃĐșĐ°Ń ĐŒĐŸĐŽĐ”Đ»Ń ĐŽĐ»Ń ĐœĐ”ĐŸĐșлаŃŃĐžŃĐ”ŃĐșĐžŃ
ŃŃŃĐ”ĐșŃĐŸĐČ, ĐŒĐŸĐŽĐ”Đ»Ń Đ°ĐœĐŸĐŒĐ°Đ»ŃĐœĐŸĐłĐŸ ŃŃĐ°ĐœŃĐżĐŸŃŃĐ°, ĐșĐŸŃĐŸŃĐ°Ń ŃŃĐžŃŃĐČĐ°Đ”Ń ŃŃŃĐ”ĐșŃŃ ŃĐžŃĐ° (ExB)-ĐżĐŸŃĐŸĐșĐŸĐČ, Đž ŃŃĐ»ĐŸĐČĐžŃ ĐČĐŸĐ·Đ±ŃĐ¶ĐŽĐ”ĐœĐžŃ ĐĐĐ-ĐœĐ”ŃŃŃĐŸĐčŃĐžĐČĐŸŃŃĐ”Đč. Đ ŃДзŃĐ»ŃŃĐ°ŃĐ” ŃĐ°ŃŃĐ”ŃĐŸĐČ ĐżĐŸĐ»ŃŃĐ”ĐœŃ ŃĐșŃĐčĐ»ĐžĐœĐłĐž ĐŽĐ»Ń ŃĐžŃĐžĐœŃ Đž ĐČŃŃĐŸŃŃ ĐżŃДЎДŃŃала ĐșĐ°Đș ŃŃĐœĐșŃОО паŃĐ°ĐŒĐ”ŃŃĐŸĐČ ĐżĐ»Đ°Đ·ĐŒŃ. ĐĐ”Đ»ĐžĐœĐ”ĐčĐœĐŸĐ” ĐČĐ·Đ°ĐžĐŒĐŸĐŽĐ”ĐčŃŃĐČОД ĐœĐ”ĐŸĐșлаŃŃĐžŃĐ”ŃĐșĐžŃ
ŃŃŃĐ”ĐșŃĐŸĐČ Đž ŃŃŃĐ”ĐșŃĐŸĐČ, ŃĐČŃĐ·Đ°ĐœĐœŃŃ
Ń Đ°ĐœĐŸĐŒĐ°Đ»ŃĐœŃĐŒ ŃŃĐ°ĐœŃĐżĐŸŃŃĐŸĐŒ, ŃĐČĐ»ŃĐ”ŃŃŃ ĐŒĐŸŃĐžĐČĐ°ŃОДĐč ŃĐ°Đ·ŃĐ°Đ±ĐŸŃĐșĐž ŃĐ°ĐŒĐŸŃĐŸĐłĐ»Đ°ŃĐŸĐČĐ°ĐœĐœĐŸĐč ŃĐžŃĐ»Đ”ĐœĐœĐŸĐč ĐŒĐŸĐŽĐ”Đ»Đž, ĐșĐŸŃĐŸŃĐ°Ń ĐŸĐŽĐœĐŸĐČŃĐ”ĐŒĐ”ĐœĐœĐŸ ĐČĐșĐ»ŃŃĐ°Đ”Ń ŃŃŃĐ”ĐșŃŃ Đ°ĐœĐŸĐŒĐ°Đ»ŃĐœĐŸĐłĐŸ Đž ĐœĐ”ĐŸĐșлаŃŃĐžŃĐ”ŃĐșĐŸĐłĐŸ ŃŃĐ°ĐœŃĐżĐŸŃŃĐ°. ĐĐŸĐșĐ°Đ·Đ°ĐœĐŸ, ŃŃĐŸ ĐżĐŸŃĐŸĐșĐž ŃДпла ĐœĐ° ĐŽĐžĐČĐ”ŃŃĐŸŃ Đ·Đ°ĐČĐžŃŃŃ ĐŸŃ ĐżĐ»Đ°Đ·ĐŒĐ”ĐœĐœŃŃ
ŃĐŸĐșĐŸĐČ. йаĐșжД ĐżŃДЎŃŃĐ°ĐČĐ»Đ”ĐœŃ ŃДзŃĐ»ŃŃĐ°ŃŃ ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžŃ Đ·Đ°ĐČĐžŃĐžĐŒĐŸŃŃĐž ĐżĐŸĐ»ŃŃĐžŃĐžĐœŃ ĐżŃĐŸŃОлДĐč ŃДпла ĐœĐ° ĐŽĐžĐČĐ”ŃŃĐŸŃ ĐŸŃ ŃŃŃĐ”ĐșŃĐŸĐČ, ŃĐČŃĐ·Đ°ĐœĐœŃŃ
Ń Đ°ĐœĐŸĐŒĐ°Đ»ŃĐœŃĐŒ ŃŃĐ°ĐœŃĐżĐŸŃŃĐŸĐŒ Đž ŃŃĐŸĐ»ĐșĐœĐŸĐČĐ”ĐœĐžŃĐŒĐž Ń ĐœĐ”ĐčŃŃĐ°Đ»ŃĐœŃĐŒĐž ŃĐ°ŃŃĐžŃĐ°ĐŒĐž
Evidence of Color Coherence Effects in W+jets Events from ppbar Collisions at sqrt(s) = 1.8 TeV
We report the results of a study of color coherence effects in ppbar
collisions based on data collected by the D0 detector during the 1994-1995 run
of the Fermilab Tevatron Collider, at a center of mass energy sqrt(s) = 1.8
TeV. Initial-to-final state color interference effects are studied by examining
particle distribution patterns in events with a W boson and at least one jet.
The data are compared to Monte Carlo simulations with different color coherence
implementations and to an analytic modified-leading-logarithm perturbative
calculation based on the local parton-hadron duality hypothesis.Comment: 13 pages, 6 figures. Submitted to Physics Letters
Measurement of the B0-anti-B0-Oscillation Frequency with Inclusive Dilepton Events
The - oscillation frequency has been measured with a sample of
23 million \B\bar B pairs collected with the BABAR detector at the PEP-II
asymmetric B Factory at SLAC. In this sample, we select events in which both B
mesons decay semileptonically and use the charge of the leptons to identify the
flavor of each B meson. A simultaneous fit to the decay time difference
distributions for opposite- and same-sign dilepton events gives ps.Comment: 7 pages, 1 figure, submitted to Physical Review Letter
Measurement of the top pair production cross section in 8 TeV proton-proton collisions using kinematic information in the lepton plus jets final state with ATLAS
A measurement is presented of the inclusive production
cross-section in collisions at a center-of-mass energy of TeV
using data collected by the ATLAS detector at the CERN Large Hadron Collider.
The measurement was performed in the lepton+jets final state using a data set
corresponding to an integrated luminosity of 20.3 fb. The cross-section
was obtained using a likelihood discriminant fit and -jet identification was
used to improve the signal-to-background ratio. The inclusive
production cross-section was measured to be
pb assuming a top-quark mass of 172.5 GeV, in good agreement with the
theoretical prediction of pb. The production cross-section in the fiducial region
determined by the detector acceptance is also reported.Comment: Published version, 19 pages plus author list (35 pages total), 3
figures, 2 tables, all figures including auxiliary figures are available at
http://atlas.web.cern.ch/Atlas/GROUPS/PHYSICS/PAPERS/TOPQ-2013-06
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