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AbstractAbstract
[en] The NOMAD experiment has been searching for νμ ↔ ντ oscillations by looking for the appearance of τ- in events from the CERN-SPS neutrino beam. With some improvements in the analysis techniques with respect to the previous published results and including data from 1995 to 1997, no evidence for oscillations is found, resulting in an updated limit in the oscillation probability of P(νμ ↔ ντ) < 0.6 x 10-3 at 90% C.L. This corresponds to a limit on the oscillation mixing angle of sin2 2Θμτ < 1.2 x 10-3 for large Δm2
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6. topical seminar on neutrino and astroparticle physics; Pisa (Italy); 17-21 May 1999; S0920563200004886; Copyright (c) 2000 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.; Country of input: International Atomic Energy Agency (IAEA)
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AbstractAbstract
[en] The dijet cross section in photoproduction has been measured with the ZEUS detector at HERA using an integrated luminosity of 38.6 pb-1. The events were required to have a virtuality of the incoming photon, Q2, of less than 1 GeV2 and a photon-proton centre-of-mass energy in the range 134 < Wγp < 277 GeV. Each event contains at least two jets satisfying transverse-energy requirements of Ejet1T > 14 GeV and Ejet2T > 11 GeV and pseudorapidity requirements of -1 < ηjet1,2 < 2.4. The measurements are compared to next-to-leading-order QCD predictions. The data show particular sensitivity to the density of partons in the photon, allowing the validity of the current parameterizations to be tested. (author)
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10. International Workshop on Deep Inelastic Scattering (DIS2002); Cracow (Poland); 30 Apr - 4 May 2002; 5 refs., 4 figs.
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Acta Physica Polonica. Series B; ISSN 0587-4254; ; v. 33(10); p. 3105-3110
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BASIC INTERACTIONS, BOSONS, ELECTROMAGNETIC INTERACTIONS, ELEMENTARY PARTICLES, ENERGY, FIELD THEORIES, FUNCTIONS, INELASTIC SCATTERING, INTERACTIONS, KINETIC ENERGY, LEPTON-BARYON INTERACTIONS, LEPTON-HADRON INTERACTIONS, LEPTON-LEPTON INTERACTIONS, LEPTON-NUCLEON INTERACTIONS, MASSLESS PARTICLES, MOMENTUM TRANSFER, PARTICLE INTERACTIONS, PARTICLE PRODUCTION, POSTULATED PARTICLES, QUANTUM FIELD THEORY, SCATTERING, STORAGE RINGS
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AbstractAbstract
[en] Respiratory gated PET/CT (positron emission tomography/computed tomography) of the lung is expected to increase the accuracy of quantitative determinations in lesional activities, regardless of the gating method used; reasonably, respiratory gating should increase standard uptake value (SUV; and possibly decrease lesional size), on the basis of the reduction of the smearing effect.'' However, literature data are very limited, particularly for in vivo studies. The objective of this article is to test the SUV variations in a large group of lung lesion studies. A group of 26 consecutive positive studies (21 men, 5 women, age 36-84, mean 68), performed on patients referred to our institution for known or suspected lung cancer, are examined. All studies were performed both with conventional PET/CT total body scan and with Real-Time Position Management (RPM) triggered selective gated study of the thorax. Four studies were considered technically unsatisfactory and were discarded; the remaining 22 studies are the object of this work. Max lesional SUVs were evaluated in both settings by semi-automated algorithms; for the gated studies, both values of the bin that showed more relevant variations from the clinical routinary study (''best bin'') and an average value that was calculated over all bins were determined. Results were compared on a one-to-one basis. In conventional, SUV showed a mean±standard deviation (SD) value of 9.2±6.9 (range 0.9-26). In the averaged gated studies, the mean±SD value was 13.4±11.7 (range 1.4-47); in the ''best bin'' dataset the mean±SD was 14.9±12.9, ranging from 1.6 to 53.1. In general, the use of respiratory trigger induced rather variable but overall consistent increases in SUV. If the percentage variations in the average trigger dataset are considered, there is an average increase of +60%, SD ±97 (P<0.05). Similar results are found in the ''best bin'' dataset, the average percentage increase in SUV values being +77.2% (SD±04.6). In lung cancer, triggering procedures increase the signal to noise ratio. The increase in SUV determined by gating is very variable, but generally relevant. This could lead to an SUV values cut-off revision, and may have an impact on smaller lesions detection. (author)
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Journal Article
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Annals of Nuclear Medicine; ISSN 0914-7187; ; v. 23(2); p. 191-196
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ANTIMETABOLITES, BETA DECAY RADIOISOTOPES, BETA-PLUS DECAY RADIOISOTOPES, BODY, COMPUTERIZED TOMOGRAPHY, DIAGNOSTIC TECHNIQUES, DIMENSIONLESS NUMBERS, DISEASES, DRUGS, EMISSION COMPUTED TOMOGRAPHY, FLUORINE ISOTOPES, HOURS LIVING RADIOISOTOPES, ISOMERIC TRANSITION ISOTOPES, ISOTOPES, LIGHT NUCLEI, METABOLISM, NANOSECONDS LIVING RADIOISOTOPES, NEOPLASMS, NUCLEI, ODD-ODD NUCLEI, ORGANS, RADIOISOTOPES, RESPIRATORY SYSTEM, TOMOGRAPHY
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AbstractAbstract
[en] In this paper we present a study of the signal produced by electrons and pions of energies ranging between 1 GeV and 180 GeV in modules of ATLAS Tile Calorimeter. Results are compared to Geant4 simulation by analyzing linearity, resolution, e/π ratio and shower profile. The final goal is to tune and validate, in the simple Test Beam geometry, the Geant4 simulation program
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9. topical seminar on innovative particle and radiation detectors; Siena (Italy); 23-26 May 2004; S0920-5632(05)00820-0; Copyright (c) 2005 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.; Country of input: International Atomic Energy Agency (IAEA)
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AbstractAbstract
[en] The precision of the final jet energy scale is a fundamental ingredient for important physics measurements, like the top-quark mass, or even for new discoveries (SUSY). The ATLAS calorimeter requirements in terms of uniformity and resolution have been achieved and verified in many years of tests on beam at CERN. The key issues for the jet reconstruction and calibration in ATLAS (agreement between test beam data and the Geant 4 predictions, clustering strategies, reconstruction and calibration algorithms) will be briefly discussed and reviewed
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10. Pisa meeting on advanced detectors: Frontier detectors for frontier physics; La Biodola, Elba (Italy); 21-27 May 2006; S0168-9002(06)02032-8; Copyright (c) 2006 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.; Country of input: International Atomic Energy Agency (IAEA)
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Nuclear Instruments and Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment; ISSN 0168-9002; ; CODEN NIMAER; v. 572(1); p. 154-156
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External URLExternal URL
AbstractAbstract
[en] Four surface reflectance models of solar radiation were determined by examining several sets of field measurements taken for clear-sky conditions at various sites in Antarctica. Each model consists of the mean spectral curve of surface reflectance in the 0.25-2.7 μm wavelength range and of the dependence curve of total abedo on the solar elevation angle h, within the range from 50 to 550. The TNB (Terra Nova Bay) model refers to a rocky terrain where granites are predominant; the NIS (Nansen Ice Sheet) model to a glacier surface made uneven by sastrugi and streaked by irregular fractures; the HAP (High Altitude Plateau) model to a flat ice surface covered by fresh snow and scored by light sastrugi; and the RIS (Ross Ice Shelf) model to an area covered by the sea ice pack presenting many discontinuities in the reflectance features, due to melt water lakes, puddles, refrozen ice and snow pots. The reflectance curve obtained for the TNB model presents gradually increasing values as wavelength increases through the visible spectral range and almost constant values at infrared wavelengths, giving a total albedo value equal to 0.264 at = 300, which increases by about 80% through the lower range of h and decreases by 12% through the upper range. The reflectance curves of the NIS, HAP and RIS models are all peaked at visible wavelengths and exhibit decreasing values throughout the infrared spectral range, giving values of total albedo equal to 0.464, 0.738 and 0.426 at h 300, respectively. These values were estimated to increase by 8-14% as h decreases from 300 to 50 and to decrease by 2-4% only as h increases from 300 to 550
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Barichello, G.; Cervera-Villanueva, A.; Daniels, D.C.; Couto e Silva, E. do; Ellis, M.; Ferrere, D.; Gomez-Cadenas, J.J.; Goessling, C.; Gouanere, M.; Hernando, J.A.; Huta, W.; Kokkonen, J.; Kuznetsov, V.E.; Linssen, L.; Lisowski, B.; Long, J.; Lupi, A.; Runolfsson, Oe.; Schmidt, B.; Soler, F.J.P.; Steele, D.; Stipcevic, M.; Vidal-Sitjes, G.; Veltri, M., E-mail: p.soler@rl.ac.uk2003
AbstractAbstract
[en] The NOMAD-STAR detector is a silicon vertex detector installed in the NOMAD spectrometer at the CERN SPS neutrino beam. It consists of four layers of a passive boron carbide target with a total mass of 45 kg and five layers of 600 single-sided silicon microstrip detectors covering a total area of 1.14 m2. About 11,500νμ charged current interactions were reconstructed in the fiducial volume of NOMAD-STAR from the neutrino run in 1998. The potential use of silicon detectors for νμ(νe)↔ντ oscillations depends on the observation of the τ candidates by the experimental signature of a large impact parameter, in the case of the one prong decay of the τ, or a double vertex, in the case of the three prong decay. The main aim of NOMAD-STAR is to measure the impact parameter and vertex distributions of charged current interactions, which constitute the main backgrounds for the oscillation signals, to understand the significance of a potential signal in a future experiment. The present paper describes the experience gained in the operation of this silicon vertex detector, and the performance achieved with it
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S0168900203013792; Copyright (c) 2003 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.; Country of input: International Atomic Energy Agency (IAEA)
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Nuclear Instruments and Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment; ISSN 0168-9002; ; CODEN NIMAER; v. 506(3); p. 217-237
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Autiero, D.; Baldo-Ceolin, M.; Bobisut, F.; Cattaneo, P.W.; Cavasinni, V.; Collazuol, G.; Conforto, G.; Contalbrigo, M.; Conta, C.; Prete, T. Del; Santo, A. De; Ferrari, R.; Flaminio, V.; Fraternali, M.; Gibin, D.; Gninenko, S.N.; Graziani, G.; Guglielmi, A.; Iacopini, E.; Lacaprara, S.; Lupi, A.; Kirsanov, M.M.; Kovzelev, A.V.; Rotonda, L. La; Lanza, A.; Laveder, M.; Marchionni, A.; Martelli, F.; Mezzetto, M.; Orestano, D.; Pastore, F.; Pennacchio, E.; Petti, R.; Polesello, G.; Renzoni, G.; Roda, C.; Salvatore, F.; Sconza, A.; Toropin, A.N.; Valdata-Nappi, M.; Veltri, M.; Vercesi, V.; Volkov, S.A.1999
AbstractAbstract
[en] A description of the response of the NOMAD electromagnetic calorimeter to electrons and photons is discussed. In particular, the dependence of the two-dimensional shower shape on the angle and energy of the incident particle is parametrized by analytical functions. Some applications to the neutrino event reconstruction are also reported
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S0168900298013527; Copyright (c) 1999 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.; Country of input: Syrian Arab Republic
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Nuclear Instruments and Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment; ISSN 0168-9002; ; CODEN NIMAER; v. 425(1-2); p. 188-209
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Autiero, D.; Baldo-Ceolin, M.; Bobisut, F.; Cattaneo, P.W.; Camilleri, L.; Cavasinni, V.; Collazuol, G.; Conforto, G.; Conta, C.; Contalbrigo, M.; Del Prete, T.; De Santo, A.; Ferrari, R.; Fraternali, M.; Gibin, D.; Gninenko, S.N.; Graziani, G.; Guglielmi, A.; Iacopini, E.; Kovzelev, A.V.; La Rotonda, L.; Lacaprara, S.; Lanza, A.; Laveder, M.; Lupi, A.; Martelli, F.; Mezzetto, M.; Orestano, D.; Pastore, F.; Pennacchio, E.; Petti, R.; Polesello, G.; Rimoldi, A.; Salvatore, F.; Sconza, A.; Valdata-Nappi, M.; Veltri, M.; Vercesi, V.; Volkov, S.A.1997
AbstractAbstract
[en] Test beam results of the NOMAD electromagnetic calorimeter are presented showing linearity, signal uniformity, energy and position resolution measured in an electron beam. Tests were also performed placing the calorimeter in a magnetic field of 0.4 T. Results on the π rejection obtained using a combined measurement of preshower/electromagnetic calorimeter are found to be in good agreement with the project expectations. Finally the calorimeter response to the muons is discussed. (orig.)
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Nuclear Instruments and Methods in Physics Research. Section A, Accelerators, Spectrometers, Detectors and Associated Equipment; ISSN 0168-9002; ; CODEN NIMAER; v. 387(3); p. 352-364
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Astier, P.; Autiero, D.; Baldisseri, A.; Baldo-Ceolin, M.; Banner, M.; Bassompierre, G.; Benslama, K.; Besson, N.; Bird, I.; Blumenfeld, B.; Bobisut, F.; Bouchez, J.; Boyd, S.; Bueno, A.; Bunyatov, S.; Camilleri, L.; Cardini, A.; Cattaneo, P.W.; Cavasinni, V.; Cervera-Villanueva, A.; Collazuol, G.; Conforto, G.; Conta, C.; Contalbrigo, M.; Cousins, R.; Daniels, D.; Degaudenzi, H.; Del Prete, T.; De Santo, A.; Dignan, T.; Di Lella, L.; Couto e Silva, E. do; Dumarchez, J.; Ellis, M.; Fazio, T.; Feldman, G.J.; Ferrari, R.; Ferrere, D.; Flaminio, V.; Fraternali, M.; Gaillard, J.-M.; Gangler, E.; Geiser, A.; Geppert, D.; Gibin, D.; Gninenko, S.; Godley, A.; Gomez-Cadenas, J.-J.; Gosset, J.; Goessling, C.; Gouanere, M.; Grant, A.; Graziani, G.; Guglielmi, A.; Hagner, C.; Hernando, J.; Hubbard, D.; Hurst, P.; Hyett, N.; Iacopini, E.; Joseph, C.; Juget, F.; Kirsanov, M.; Klimov, O.; Kokkonen, J.; Kovzelev, A.; Krasnoperov, A.; Kuznetsov, V.; Lacaprara, S.; Lachaud, C.; Lakic, B.; Lanza, A.; LaRotonda, L.; Laveder, M.; Letessier-Selvon, A.; Levy, J.-M.; Linssen, L.; Ljubicic, A.; Long, J.; Lupi, A.; Marchionni, A.; Martelli, F.; Mechain, X.; Mendiburu, J.-P.; Meyer, J.-P.; Mezzetto, M.; Mishra, S.R.; Moorhead, G.F.; Naumov, D.; Nedelec, P.; Nefedov, Yu.; Nguyen-Mau, C.; Orestano, D.; Pastore, F.; Peak, L.S.; Pennacchio, E.; Pessard, H.; Petti, R.; Placci, A.; Polesello, G.; Pollmann, D.; Polyarush, A.; Popov, B.; Poulsen, C.; Rathouit, P.; Rico, J.; Roda, C.; Rubbia, A.; Salvatore, F.; Schahmaneche, K.; Schmidt, B.; Sevior, M.; Sillou, D.; Soler, F.J.P.; Sozzi, G.; Steele, D.; Stiegler, U.; Stipcevic, M.; Stolarczyk, Th.; Tareb-Reyes, M.; Taylor, G.N.; Tereshchenko, V.; Toropin, A.; Touchard, A.-M.; Tovey, S.N.; Tran, M.-T.; Tsesmelis, E.; Ulrichs, J.; Vacavant, L.; Valdata-Nappi, M.; Valuev, V.; Vannucci, F.; Varvell, K.E.; Veltri, M.; Vercesi, V.; Vidal-Sitjes, G.; Vieira, J.-M.; Vinogradova, T.; Weber, F.V.; Weisse, T.; Wilson, F.F.; Winton, L.J.; Yabsley, B.D.; Zaccone, H.; Zuber, K.; Zuccon, P., E-mail: mikhail.kirsanov@cern.ch
NOMAD Collaboration2001
NOMAD Collaboration2001
AbstractAbstract
[en] The inclusive production of the meson resonances ρ0(770), f0(980) and f2(1270) in neutrino-nucleus charged current interactions has been studied with the NOMAD detector exposed to the wide band neutrino beam generated by 450 GeV protons at the CERN SPS. For the first time the f0(980) meson is observed in neutrino interactions. The statistical significance of its observation is 6 standard deviations. The presence of f2(1270) in neutrino interactions is reliably established. The average multiplicity of these three resonances is measured as a function of several kinematic variables. The experimental results are compared to the multiplicities obtained from a simulation based on the Lund model. In addition, the average multiplicity of ρ0(770) in antineutrino-nucleus interactions is measured
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S0550321301000542; Copyright (c) 2001 Elsevier Science B.V., Amsterdam, The Netherlands, All rights reserved.; Country of input: International Atomic Energy Agency (IAEA)
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ANTINEUTRINOS, CERN SPS SYNCHROTRON, CHARGED-CURRENT INTERACTIONS, COMPARATIVE EVALUATIONS, COMPUTERIZED SIMULATION, F0-980 MESONS, F2-1270 MESONS, GEV RANGE 100-1000, INCLUSIVE INTERACTIONS, MULTIPLICITY, MUON NEUTRINOS, NEUTRINO REACTIONS, NEUTRINO-NUCLEON INTERACTIONS, PARTICLE PRODUCTION, PROTONS, RESONANCE PARTICLES, RHO-770 MESONS, STANDARD MODEL
ACCELERATORS, ANTILEPTONS, ANTIMATTER, ANTIPARTICLES, BARYONS, BOSONS, CYCLIC ACCELERATORS, ELEMENTARY PARTICLES, ENERGY RANGE, EVALUATION, FERMIONS, FIELD THEORIES, GEV RANGE, GRAND UNIFIED THEORY, HADRONS, INTERACTIONS, LEPTON REACTIONS, LEPTON-BARYON INTERACTIONS, LEPTON-HADRON INTERACTIONS, LEPTON-NUCLEON INTERACTIONS, LEPTONS, MASSLESS PARTICLES, MATHEMATICAL MODELS, MATTER, MESONS, NEUTRINOS, NUCLEAR REACTIONS, NUCLEONS, PARTICLE INTERACTIONS, PARTICLE MODELS, QUANTUM FIELD THEORY, SCALAR MESONS, SIMULATION, SYNCHROTRONS, TENSOR MESONS, UNIFIED GAUGE MODELS, VECTOR MESONS
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