117 research outputs found
LHC High Beta* Runs: Transport and Unfolding Methods
The paper describes the transport of the elastically and diffractively
scattered protons in the proton-proton interactions at the LHC for the high
beta* runs. A parametrisation of the attered proton transport through the LHC
magnetic lattice is presented. The accuracy of the unfolding of the kinematic
variables of the scattered protons is discussed.Comment: 12 pages, 15 figure
Selected Issues on Histograming on GPUs
The contemporary large scale measuring systems in the real-time environment make extensive use of histogramming as a tool for the experimental data quality monitoring. The processing of a large number of data channels requires a suitable computing power where the graphical processors seem to be well suited. Histogramming operations run on the central and graphics processing units are discussed. Results of the performance measurements including various configurations of the allocation of the histograms in various parts of the memory of used devices are presented
Study of Diffraction with the ATLAS detector at the LHC
La thèse est consacrée à l étude de la diffraction en utilisant le détecteur ATLAS auprès du LHC. Après Une courte introduction à la physique diffractive incluant la diffraction dure et molle , nous présentons la production diffractive exclusive qui est particulièrement intéressante pour produire des jets et le boson de Higgs. Le mécanisme décrit par le formalisme de Khoze Martin et Ryskin et celui de CHIDe sont décrits en détail. Les sources d incertitude dans la description théorique sont encore importantes et une nouvelle mesure de la section efficace de production exclusive de jets au LHC permettra de réduire l incertitude de la production diffractive de boson de Higgs à un facteur 2 à trois. La mesure de la production exclusive de pions pp ! p_+_ p permet de contraindre les modèles de manière plus précise en utilisant les détecteurs ALFA, qui sont utilisés dans l expérience ATLAS pour la détection de protons diffusés dans les interactions élastiques et diffractives. Les détecteurs AFP décrits dans la dernière partie de la thèse, mesurant les protons dispersés après interaction diffractive sont présentés. Ils permettent d étendre le programme de physique d ATLAS, avec en particulier, la production centrale diffractive de boson W, ce qui rend possible une meilleure compréhension de la nature des échanges diffractifs.The thesis is devoted to the study of diffractive physics with the ATLAS detector at the LHC. After a short introduction to diffractive physics including soft and hard diffraction, we discuss diffractive exclusive production at the LHC whichis particularly interesting for Higgs and jet production. The QCD mechanism described by the Khoze Martin Ryskin and the CHIDe models are elucidated in detail. The uncertainties on these models are still large and a new possible exclusive jetmeasurement at the LHC will allow to reduce the uncertainty on diffarctive Higgs boson production to a factor 2 to 3. An additional measurement of exclusive pion production pp ! p_+_ p allows to constrain further exclusive model relying on theuse of the ALFA stations, which are used in the ATLAS Experiment for detection of protons scattered in elastic and diffractive interactions. In the last part of the thesis, the AFP detectors, aiming at measuring the protons scattered in diffractive interactions, are presented. They allow to extend substantially the ATLAS physics programme. In particular, the study of the central diffractive W boson production process makes possible a better determination of the nature of diffractive exchanges.PARIS11-SCD-Bib. électronique (914719901) / SudocSudocFranceF
Measurement of Jet Shapes in Photoproduction at HERA
The shape of jets produced in quasi-real photon-proton collisions at
centre-of-mass energies in the range GeV has been measured using the
hadronic energy flow. The measurement was done with the ZEUS detector at HERA.
Jets are identified using a cone algorithm in the plane with a
cone radius of one unit. Measured jet shapes both in inclusive jet and dijet
production with transverse energies GeV are presented. The jet
shape broadens as the jet pseudorapidity () increases and narrows
as increases. In dijet photoproduction, the jet shapes have been
measured separately for samples dominated by resolved and by direct processes.
Leading-logarithm parton-shower Monte Carlo calculations of resolved and direct
processes describe well the measured jet shapes except for the inclusive
production of jets with high and low . The observed
broadening of the jet shape as increases is consistent with the
predicted increase in the fraction of final state gluon jets.Comment: 29 pages including 9 figure
Measurement of the Diffractive Cross Section in Deep Inelastic Scattering using ZEUS 1994 Data
The DIS diffractive cross section, , has been measured in the mass range GeV for c.m. energies GeV and photon virtualities to 140 GeV. For fixed and , the diffractive cross section rises rapidly with , with corresponding to a -averaged pomeron trajectory of \bar{\alphapom} = 1.127 \pm 0.009 (stat)^{+0.039}_{-0.012} (syst) which is larger than \bar{\alphapom} observed in hadron-hadron scattering. The dependence of the diffractive cross section is found to be the same as that of the total cross section for scattering of virtual photons on protons. The data are consistent with the assumption that the diffractive structure function factorizes according to \xpom F^{D(3)}_2 (\xpom,\beta,Q^2) = (x_0/ \xpom)^n F^{D(2)}_2(\beta,Q^2). They are also consistent with QCD based models which incorporate factorization breaking. The rise of \xpom F^{D(3)}_2 with decreasing \xpom and the weak dependence of on suggest a substantial contribution from partonic interactions
Measurement of the F2 structure function in deep inelastic ep scattering using 1994 data from the ZEUS detector at HERA
We present measurements of the structure function \Ft\ in e^+p scattering at HERA in the range 3.5\;\Gevsq < \qsd < 5000\;\Gevsq. A new reconstruction method has allowed a significant improvement in the resolution of the kinematic variables and an extension of the kinematic region covered by the experiment. At \qsd < 35 \;\Gevsq the range in x now spans 6.3\cdot 10^{-5} < x < 0.08 providing overlap with measurements from fixed target experiments. At values of Q^2 above 1000 GeV^2 the x range extends to 0.5. Systematic errors below 5\perc\ have been achieved for most of the kinematic urray, W
- …