789 research outputs found

    Understanding the Kalman Filter: an Object Oriented Programming Perspective.

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    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

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    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

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    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

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    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

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    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

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    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 E×B 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.За ĐŽĐŸĐżĐŸĐŒĐŸĐłĐŸŃŽ ĐșŃ–ĐœĐ”Ń‚ĐžŃ‡ĐœĐŸĐłĐŸ ĐœĐ”ĐŸĐșĐ»Đ°ŃĐžŃ‡ĐœĐŸĐłĐŸ ĐșĐŸĐŽŃƒ XGC0 ĐŽĐ»Ń Ń€ĐŸĐ·Ń€ŃĐŽŃ–ĐČ ĐČ Ń‚ĐŸĐșĐ°ĐŒĐ°Đșах DIII-D і Alcator C-Mod ĐŽĐŸŃĐ»Ń–ĐŽĐ¶Đ”ĐœĐŸ сĐșĐ”ĐčĐ»Ń–ĐœĐł Đżâ€™Ń”ĐŽĐ”ŃŃ‚Đ°Đ»Ńƒ ĐČ ĐżĐ»Đ°Đ·ĐŒŃ–, Ń‰ĐŸ ĐżĐ”Ń€Đ”Đ±ŃƒĐČає ĐČ Ń€Đ”Đ¶ĐžĐŒŃ– ĐżĐŸĐ»Ń–ĐżŃˆĐ”ĐœĐŸĐłĐŸ ŃƒŃ‚Ń€ĐžĐŒĐ°ĐœĐœŃ, Đ· проĐșĐŸŃ€ĐŽĐŸĐœĐœĐžĐŒĐž Đ»ĐŸĐșĐ°Đ»Ń–Đ·ĐŸĐČĐ°ĐœĐžĐŒĐž ĐŒĐŸĐŽĐ°ĐŒĐž (ПЛМ) ĐżĐ”Ń€ŃˆĐŸĐłĐŸ топу, ĐČластОĐČĐŸŃŃ‚Ń– Đżâ€™Ń”ĐŽĐ”ŃŃ‚Đ°Đ»Ńƒ і ĐżĐŸŃ‚ĐŸĐșу тДпла ĐœĐ° ĐŽĐžĐČĐ”Ń€Ń‚ĐŸŃ€ ĐČ Đ·Đ°Đ»Đ”Đ¶ĐœĐŸŃŃ‚Ń– ĐČіЮ ĐČĐžŃ‚ŃĐłĐœŃƒŃ‚ĐŸŃŃ‚Ń– ĐżĐ»Đ°Đ·ĐŒĐž та ŃŃ‚Ń€ŃƒĐŒŃƒ ĐżĐ»Đ°Đ·ĐŒĐž. ĐŁ Ń€ĐŸĐ·Ń€Đ°Ń…ŃƒĐœĐșах ĐČĐžĐșĐŸŃ€ĐžŃŃ‚ĐŸĐČуються: Ń€Đ”Đ°Đ»Ń–ŃŃ‚ĐžŃ‡ĐœĐ° ĐłĐ”ĐŸĐŒĐ”Ń‚Ń€Ń–Ń ĐŽĐžĐČĐ”Ń€Ń‚ĐŸŃ€Đ°, ĐșŃ–ĐœĐ”Ń‚ĐžŃ‡ĐœĐ° ĐŒĐŸĐŽĐ”Đ»ŃŒ ĐŽĐ»Ń ĐœĐ”ĐŸĐșĐ»Đ°ŃĐžŃ‡ĐœĐžŃ… ДфДĐșтіĐČ, ĐŒĐŸĐŽĐ”Đ»ŃŒ Đ°ĐœĐŸĐŒĐ°Đ»ŃŒĐœĐŸĐłĐŸ Ń‚Ń€Đ°ĐœŃĐżĐŸŃ€Ń‚Ńƒ, яĐșĐ° ĐČŃ€Đ°Ń…ĐŸĐČує ДфДĐșто шора (ExB)-ĐżĐŸŃ‚ĐŸĐșіĐČ, і ŃƒĐŒĐŸĐČĐž Đ·Đ±ŃƒĐŽĐ¶Đ”ĐœĐœŃ ПЛМ-ĐœĐ”ŃŃ‚Ń–ĐčĐșĐŸŃŃ‚Đ”Đč. ĐŁ Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Ń– Ń€ĐŸĐ·Ń€Đ°Ń…ŃƒĐœĐșіĐČ ĐŸŃ‚Ń€ĐžĐŒĐ°ĐœŃ– сĐșĐ”ĐčĐ»Ń–ĐœĐłŃ– ĐŽĐ»Ń ŃˆĐžŃ€ĐžĐœĐž і ĐČĐžŃĐŸŃ‚Đž Đżâ€™Ń”ĐŽĐ”ŃŃ‚Đ°Đ»Ńƒ яĐș Ń„ŃƒĐœĐșції ĐżĐ°Ń€Đ°ĐŒĐ”Ń‚Ń€Ń–ĐČ ĐżĐ»Đ°Đ·ĐŒĐž. ĐĐ”Đ»Ń–ĐœŃ–ĐčĐœĐ° ĐČĐ·Đ°Ń”ĐŒĐŸĐŽŃ–Ń ĐœĐ”ĐŸĐșĐ»Đ°ŃĐžŃ‡ĐœĐžŃ… ДфДĐșтіĐČ Ń– ДфДĐșтіĐČ, ĐżĐŸĐČ'ŃĐ·Đ°ĐœĐžŃ… Đ· Đ°ĐœĐŸĐŒĐ°Đ»ŃŒĐœĐžĐŒ Ń‚Ń€Đ°ĐœŃĐżĐŸŃ€Ń‚ĐŸĐŒ, є ĐŒĐŸŃ‚ĐžĐČацією ĐŽĐ»Ń Ń€ĐŸĐ·Ń€ĐŸĐ±ĐșĐž ŃĐ°ĐŒĐŸŃƒĐ·ĐłĐŸĐŽĐ¶Đ”ĐœĐŸŃ— Ń‡ĐžŃĐ”Đ»ŃŒĐœĐŸŃ— ĐŒĐŸĐŽĐ”Đ»Ń–, яĐșĐ° ĐŸĐŽĐœĐŸŃ‡Đ°ŃĐœĐŸ ĐČĐșлючає ДфДĐșто Đ°ĐœĐŸĐŒĐ°Đ»ŃŒĐœĐŸĐłĐŸ і ĐœĐ”ĐŸĐșĐ»Đ°ŃĐžŃ‡ĐœĐŸĐłĐŸ Ń‚Ń€Đ°ĐœŃĐżĐŸŃ€Ń‚Ńƒ. ĐŸĐŸĐșĐ°Đ·Đ°ĐœĐŸ, Ń‰ĐŸ ĐżĐŸŃ‚ĐŸĐșĐž тДпла ĐœĐ° ĐŽĐžĐČĐ”Ń€Ń‚ĐŸŃ€ Đ·Đ°Đ»Đ”Đ¶Đ°Ń‚ŃŒ ĐČіЮ ĐżĐ»Đ°Đ·ĐŒĐŸĐČох ŃŃ‚Ń€ŃƒĐŒŃ–ĐČ. йаĐșĐŸĐ¶ прДЎстаĐČĐ»Đ”ĐœĐŸ Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Đž ĐŽĐŸŃĐ»Ń–ĐŽĐ¶Đ”ĐœĐœŃ Đ·Đ°Đ»Đ”Đ¶ĐœĐŸŃŃ‚Ń– ĐœĐ°ĐżŃ–ĐČŃˆĐžŃ€ĐžĐœĐž ĐżŃ€ĐŸŃ„Ń–Đ»Ń–ĐČ Ń‚Đ”ĐżĐ»Đ° ĐœĐ° ĐŽĐžĐČĐ”Ń€Ń‚ĐŸŃ€ ĐČіЮ ДфДĐșтіĐČ, ĐżĐŸĐČ'ŃĐ·Đ°ĐœĐžŃ… Đ· Đ°ĐœĐŸĐŒĐ°Đ»ŃŒĐœĐžĐŒ Ń‚Ń€Đ°ĐœŃĐżĐŸŃ€Ń‚ĐŸĐŒ і Đ·Ń–Ń‚ĐșĐœĐ”ĐœĐœŃĐŒĐž Đ· ĐœĐ”ĐčŃ‚Ń€Đ°Đ»ŃŒĐœĐžĐŒĐž Ń‡Đ°ŃŃ‚ĐžĐœĐșĐ°ĐŒĐž.ĐĄ ĐżĐŸĐŒĐŸŃ‰ŃŒŃŽ ĐșĐžĐœĐ”Ń‚ĐžŃ‡Đ”ŃĐșĐŸĐłĐŸ ĐœĐ”ĐŸĐșлассОчДсĐșĐŸĐłĐŸ ĐșĐŸĐŽĐ° XGC0 ĐŽĐ»Ń Ń€Đ°Đ·Ń€ŃĐŽĐŸĐČ ĐČ Ń‚ĐŸĐșĐ°ĐŒĐ°Đșах DIII-D Đž Alcator C-Mod ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœŃ‹ сĐșэĐčĐ»ĐžĐœĐł ĐżŃŒĐ”ĐŽĐ”ŃŃ‚Đ°Đ»Đ° ĐČ ĐżĐ»Đ°Đ·ĐŒĐ”, ĐœĐ°Ń…ĐŸĐŽŃŃ‰Đ”Đčся ĐČ Ń€Đ”Đ¶ĐžĐŒĐ” ŃƒĐ»ŃƒŃ‡ŃˆĐ”ĐœĐœĐŸĐłĐŸ ŃƒĐŽĐ”Ń€Đ¶Đ°ĐœĐžŃ, с ĐżŃ€ĐžĐłŃ€Đ°ĐœĐžŃ‡ĐœŃ‹ĐŒĐž Đ»ĐŸĐșĐ°Đ»ĐžĐ·ĐŸĐČĐ°ĐœĐœŃ‹ĐŒĐž ĐŒĐŸĐŽĐ°ĐŒĐž (ПЛМ) пДрĐČĐŸĐłĐŸ топа, Đž Đ·Đ°ĐČĐžŃĐžĐŒĐŸŃŃ‚ŃŒ сĐČĐŸĐčстĐČ ĐżŃŒĐ”ĐŽĐ”ŃŃ‚Đ°Đ»Đ° Đž ĐżĐŸŃ‚ĐŸĐșĐ° тДпла ĐœĐ° ĐŽĐžĐČĐ”Ń€Ń‚ĐŸŃ€ ĐŸŃ‚ ĐČŃ‹Ń‚ŃĐœŃƒŃ‚ĐŸŃŃ‚Đž ĐżĐ»Đ°Đ·ĐŒŃ‹ Đž Ń‚ĐŸĐșĐ° ĐżĐ»Đ°Đ·ĐŒŃ‹. В расчДтах ĐžŃĐżĐŸĐ»ŃŒĐ·ŃƒŃŽŃ‚ŃŃ: Ń€Đ”Đ°Đ»ĐžŃŃ‚ĐžŃ‡ĐœĐ°Ń ĐłĐ”ĐŸĐŒĐ”Ń‚Ń€ĐžŃ ĐŽĐžĐČĐ”Ń€Ń‚ĐŸŃ€Đ°, ĐșĐžĐœĐ”Ń‚ĐžŃ‡Đ”ŃĐșая ĐŒĐŸĐŽĐ”Đ»ŃŒ ĐŽĐ»Ń ĐœĐ”ĐŸĐșлассОчДсĐșох ŃŃ„Ń„Đ”ĐșŃ‚ĐŸĐČ, ĐŒĐŸĐŽĐ”Đ»ŃŒ Đ°ĐœĐŸĐŒĐ°Đ»ŃŒĐœĐŸĐłĐŸ Ń‚Ń€Đ°ĐœŃĐżĐŸŃ€Ń‚Đ°, ĐșĐŸŃ‚ĐŸŃ€Đ°Ń учотыĐČаДт ŃŃ„Ń„Đ”Đșты шора (ExB)-ĐżĐŸŃ‚ĐŸĐșĐŸĐČ, Đž ŃƒŃĐ»ĐŸĐČоя ĐČĐŸĐ·Đ±ŃƒĐ¶ĐŽĐ”ĐœĐžŃ ПЛМ-ĐœĐ”ŃƒŃŃ‚ĐŸĐčчоĐČĐŸŃŃ‚Đ”Đč. В Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Đ” Ń€Đ°ŃŃ‡Đ”Ń‚ĐŸĐČ ĐżĐŸĐ»ŃƒŃ‡Đ”ĐœŃ‹ сĐșэĐčĐ»ĐžĐœĐłĐž ĐŽĐ»Ń ŃˆĐžŃ€ĐžĐœŃ‹ Đž ĐČŃ‹ŃĐŸŃ‚Ń‹ ĐżŃŒĐ”ĐŽĐ”ŃŃ‚Đ°Đ»Đ° ĐșĐ°Đș Ń„ŃƒĐœĐșцоо ĐżĐ°Ń€Đ°ĐŒĐ”Ń‚Ń€ĐŸĐČ ĐżĐ»Đ°Đ·ĐŒŃ‹. ĐĐ”Đ»ĐžĐœĐ”ĐčĐœĐŸĐ” ĐČĐ·Đ°ĐžĐŒĐŸĐŽĐ”ĐčстĐČОД ĐœĐ”ĐŸĐșлассОчДсĐșох ŃŃ„Ń„Đ”ĐșŃ‚ĐŸĐČ Đž ŃŃ„Ń„Đ”ĐșŃ‚ĐŸĐČ, сĐČŃĐ·Đ°ĐœĐœŃ‹Ń… с Đ°ĐœĐŸĐŒĐ°Đ»ŃŒĐœŃ‹ĐŒ Ń‚Ń€Đ°ĐœŃĐżĐŸŃ€Ń‚ĐŸĐŒ, яĐČĐ»ŃĐ”Ń‚ŃŃ ĐŒĐŸŃ‚ĐžĐČацОДĐč Ń€Đ°Đ·Ń€Đ°Đ±ĐŸŃ‚ĐșĐž ŃĐ°ĐŒĐŸŃĐŸĐłĐ»Đ°ŃĐŸĐČĐ°ĐœĐœĐŸĐč Ń‡ĐžŃĐ»Đ”ĐœĐœĐŸĐč ĐŒĐŸĐŽĐ”Đ»Đž, ĐșĐŸŃ‚ĐŸŃ€Đ°Ń ĐŸĐŽĐœĐŸĐČŃ€Đ”ĐŒĐ”ĐœĐœĐŸ ĐČĐșлючаДт ŃŃ„Ń„Đ”Đșты Đ°ĐœĐŸĐŒĐ°Đ»ŃŒĐœĐŸĐłĐŸ Đž ĐœĐ”ĐŸĐșлассОчДсĐșĐŸĐłĐŸ Ń‚Ń€Đ°ĐœŃĐżĐŸŃ€Ń‚Đ°. ĐŸĐŸĐșĐ°Đ·Đ°ĐœĐŸ, Ń‡Ń‚ĐŸ ĐżĐŸŃ‚ĐŸĐșĐž тДпла ĐœĐ° ĐŽĐžĐČĐ”Ń€Ń‚ĐŸŃ€ Đ·Đ°ĐČосят ĐŸŃ‚ ĐżĐ»Đ°Đ·ĐŒĐ”ĐœĐœŃ‹Ń… Ń‚ĐŸĐșĐŸĐČ. йаĐșжД прДЎстаĐČĐ»Đ”ĐœŃ‹ Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Ń‹ ĐžŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœĐžŃ Đ·Đ°ĐČĐžŃĐžĐŒĐŸŃŃ‚Đž ĐżĐŸĐ»ŃƒŃˆĐžŃ€ĐžĐœŃ‹ ĐżŃ€ĐŸŃ„ĐžĐ»Đ”Đč тДпла ĐœĐ° ĐŽĐžĐČĐ”Ń€Ń‚ĐŸŃ€ ĐŸŃ‚ ŃŃ„Ń„Đ”ĐșŃ‚ĐŸĐČ, сĐČŃĐ·Đ°ĐœĐœŃ‹Ń… с Đ°ĐœĐŸĐŒĐ°Đ»ŃŒĐœŃ‹ĐŒ Ń‚Ń€Đ°ĐœŃĐżĐŸŃ€Ń‚ĐŸĐŒ Đž ŃŃ‚ĐŸĐ»ĐșĐœĐŸĐČĐ”ĐœĐžŃĐŒĐž с ĐœĐ”ĐčŃ‚Ń€Đ°Đ»ŃŒĐœŃ‹ĐŒĐž Ń‡Đ°ŃŃ‚ĐžŃ†Đ°ĐŒĐž

    Evidence of Color Coherence Effects in W+jets Events from ppbar Collisions at sqrt(s) = 1.8 TeV

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    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

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    The B0B^0-Bˉ0\bar B^0 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 Δmd=0.493±0.012(stat)±0.009(syst)\Delta m_d = 0.493 \pm 0.012{(stat)}\pm 0.009{(syst)} ps−1^{-1}.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

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    A measurement is presented of the ttˉt\bar{t} inclusive production cross-section in pppp collisions at a center-of-mass energy of s=8\sqrt{s}=8 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−1^{-1}. The cross-section was obtained using a likelihood discriminant fit and bb-jet identification was used to improve the signal-to-background ratio. The inclusive ttˉt\bar{t} production cross-section was measured to be 260±1(stat.)−23+22(syst.)±8(lumi.)±4(beam)260\pm 1{\textrm{(stat.)}} ^{+22}_{-23} {\textrm{(syst.)}}\pm 8{\textrm{(lumi.)}}\pm 4{\mathrm{(beam)}} pb assuming a top-quark mass of 172.5 GeV, in good agreement with the theoretical prediction of 253−15+13253^{+13}_{-15} pb. The ttˉ→(e,ÎŒ)+jetst\bar{t}\to (e,\mu)+{\mathrm{jets}} 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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