E. Cortina Gil
Université catholique de Louvain
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by E. Cortina Gil.
Journal of Instrumentation | 2015
G. Baulieu; M. Bedjidian; K. Belkadhi; J. Berenguer; V. Boudry; P. Calabria; S. Callier; E. Calvo Almillo; S. Cap; L. Caponetto; C. Combaret; R. Cornat; E. Cortina Gil; B. De Callatay; F. Davin; C. de la Taille; R. Dellanegra; D. Delaunay; F. Doizon; F. Dulucq; A. Eynard; M. C. Fouz; F. Gastaldi; L. Germani; G. Grenier; Y. Haddad; R. Han; J. C. Ianigro; R. Kieffer; I. Laktineh
A large prototype of 1.3m3 was designed and built as a demonstrator of the semi-digital hadronic calorimeter (SDHCAL) concept proposed for the future ILC experiments. The prototype is a sampling hadronic calorimeter of 48 units. Each unit is built of an active layer made of 1m2 Glass Resistive Plate Chamber(GRPC) detector placed inside a cassette whose walls are made of stainless steel. The cassette contains also the electronics used to read out the GRPC detector. The lateral granularity of the active layer is provided by the electronics pick-up pads of 1cm2 each. The cassettes are inserted into a self-supporting mechanical structure built also of stainless steel plates which, with the cassettes walls, play the role of the absorber. The prototype was designed to be very compact and important efforts were made to minimize the number of services cables to optimize the efficiency of the Particle Flow Algorithm techniques to be used in the future ILC experiments. The different components of the SDHCAL prototype were studied individually and strict criteria were applied for the final selection of these components. Basic calibration procedures were performed after the prototype assembling. The prototype is the first of a series of new-generation detectors equipped with a power-pulsing mode intended to reduce the power consumption of this highly granular detector. A dedicated acquisition system was developed to deal with the output of more than 440000 electronics channels in both trigger and triggerless modes. After its completion in 2011, the prototype was commissioned using cosmic rays and particles beams at CERN.
Journal of High Energy Physics | 2010
V. Khachatryan; S. Basegmez; G. Bruno; J. Caudron; E. Cortina Gil; J. De Favereau De Jeneret; C. Delaere; P. Demin; D. Favart; A. Giammanco; Ghislain Grégoire; Jonathan Hollar; V. Lemaitre; Fabio Maltoni; Otilia Militaru; S. Ovyn; K. Piotrzkowski; L. Quertenmont; N. Schul
Transverse momentum and pseudorapidity distributions of charged hadrons in pp collisions at
Journal of Instrumentation | 2015
G. Aglieri Rinella; E. Cortina Gil; M. Fiorini; J. Kaplon; A. Kluge; F. Marchetto; M.E. Martin Albarran; M. Morel; M. Noy; L. Perktold; S. Tiuraniem; Bob Velghe
\sqrts = 0.9
Journal of Instrumentation | 2012
E. Martin; G. Aglieri Rinella; V. Carassiti; A. Ceccucci; E. Cortina Gil; A. Cotta Ramusino; G. Dellacasa; M Fiorini; S. Garbolino; P. Jarron; J. Kaplon; A. Kluge; F. Marchetto; A. Mapelli; G. Mazza; M. Morel; M. Noy; Georg Nuessle; P. Petagna; F. Petrucci; L. Perktold; P. Riedler; A. Rivetti; M. Statera; Bob Velghe
and 2.36 TeVMeasurements of inclusive charged-hadron transverse-momentum and pseudorapidity distributions are presented for proton-proton collisions at
Physics Procedia | 2012
M. Fiorini; G. Aglieri Rinella; V. Carassiti; A. Ceccucci; E. Cortina Gil; A. Cotta Ramusino; G. Dellacasa; S. Garbolino; P. Jarron; J. Kaplon; A. Kluge; F. Marchetto; A. Mapelli; E. Martin; G. Mazza; M. Morel; M. Noy; Georg Nuessle; P. Petagna; F. Petrucci; L. Perktold; P. Riedler; A. Rivetti; M. Statera; Bob Velghe
\sqrt{s} = 0.9
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2017
G. Aglieri Rinella; D. Alvarez Feito; Roberta Arcidiacono; Cristina Biino; S. Bonacini; A. Ceccucci; S. Chiozzi; E. Cortina Gil; A. Cotta Ramusino; J. Degrange; M. Fiorini; E. Gamberini; A. Gianoli; J. Kaplon; Alexander Kluge; A. Mapelli; F. Marchetto; E. Minucci; M. Morel; Jérôme Noël; M. Noy; L. Perktold; M. Perrin-Terrin; P. Petagna; F. Petrucci; K. Poltorak; G. Romagnoli; G. Ruggiero; Bob Velghe; H. Wahl
and 2.36 TeV. The data were collected with the CMS detector during the LHC commissioning in December 2009. For non-single-diffractive interactions, the average charged-hadron transverse momentum is measured to be 0.46 ± 0.01 (stat.) ± 0.01 (syst.) GeV/c at 0.9 TeV and 0.50 ± 0.01 (stat.) ± 0.01 (syst.) GeV/c at 2.36 TeV, for pseudorapidities between --2.4 and +2.4. At these energies, the measured pseudorapidity densities in the central region, dNch/dη||η|<0.5, are 3:48 ± 0:02 (stat.) ± 0.13 (syst.) and 4:47 ± 0:04 (stat.) ± 0.16 (syst.), respectively. The results at 0.9 TeV are in agreement with previous measurements and confirm the expectation of near equal hadron production in
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2018
L. Federici; G. Aglieri Rinella; D. Alvarez Feito; Roberta Arcidiacono; Cristina Biino; S. Bonacini; A. Ceccucci; S. Chiozzi; E. Cortina Gil; A. Cotta Ramusino; J. Degrange; M. Fiorini; E. Gamberini; A. Gianoli; J. Kaplon; A. Kleimenova; A. Kluge; A. Mapelli; F. Marchetto; E. Migliore; E. Minucci; M. Morel; Jérôme Noël; M. Noy; L. Perktold; M. Perrin-Terrin; P. Petagna; F. Petrucci; K. Poltorak; G. Romagnoli
\overline p p
Archive | 2015
Viacheslav Duk; G. Aglieri Rinella; R. Aliberti; F. Ambrosino; B. Angelucci; A. Antonelli; G. Anzivino; Roberta Arcidiacono; I. Azhinenko; S. Balev; J. Bendotti; Andrea Biagioni; Cristina Biino; A. Bizzeti; T. Blazek; A. Blik; B. Bloch-Devaux; V. Bolotov; V. Bonaiuto; M. Bragadireanu; D. Britton; G. Britvich; F. Bucci; F. Butin; E. Capitolo; C. Capoccia; T. Capussela; V. Carassiti; Nicolo Cartiglia; A. Cassese
and pp collisions. The results at 2.36 TeV represent the highest-energy measurements at a particle collider to date.Measurements of inclusive charged-hadron transverse-momentum and pseudorapidity distributions are presented for proton-proton collisions at √ s = 0.9 and 2.36 TeV. The data were collected with the CMS detector during the LHC commissioning in December 2009. For non-single-diffractive interactions, the average charged-hadron transverse momentum is measured to be 0.46 ± 0.01 (stat.) ± 0.01 (syst.) GeV/c at 0.9 TeV and 0.50 ± 0.01 (stat.) ± 0.01 (syst.) GeV/c at 2.36 TeV, for pseudorapidities between −2.4 and +2.4. At these energies, the measured pseudorapidity densities in the central region, dNch/dη||η|<0.5, are 3.48± 0.02 (stat.) ± 0.13 (syst.) and 4.47± 0.04 (stat.) ± 0.16 (syst.), respectively. The results at 0.9 TeV are in agreement with previous measurements and confirm the expectation of near equal hadron production in pp̄ and pp collisions. The results at 2.36 TeV represent the highest-energy measurements at a particle collider to date. ∗See Appendix A for the list of collaboration members ar X iv :1 00 2. 06 21 v2 [ he pex ] 8 F eb 2 01 0
Journal of Instrumentation | 2015
E. Cortina Gil; L. Soung-Yee
A time-tagging hybrid silicon pixel detector developed for beam tracking in the NA62 experiment has been tested in a dedicated test-beam at CERN with 10 GeV/c hadrons. Measurements include time resolution, detection efficiency and charge sharing between pixels, as well as effects due to bias voltage variations. A time resolution of less than 150 ps has been measured with a 200 μm thick silicon sensor, using an on-pixel amplifier-discriminator and an end-of-column DLL-based time-to-digital converter.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2010
O. Militaru; T. Bergauer; M. Bergholz; Philipp Blum; W. De Boer; K. Borras; E. Cortina Gil; A. Dierlamm; M. Dragicevic; D. Eckstein; J. Erfle; M. Fernandez; Lutz Feld; M. Frey; M. Friedl; E. Fretwurst; E. Gaubas; F.J. Gonzalez; P. Grabiec; M. Grodner; F. Hartmann; S. Hänsel; K. H. Hoffmann; J. Hrubec; R. Jaramillo; W. Karpinski; V. Kazukauskas; K. Klein; V. Khomenkov; R. Klanner
The Gigatracker (GTK) is a hybrid silicon pixel detector developed for NA62, an experiment studying ultra-rare kaon decays at the CERN SPS. The main characteristics are a time-tagging resoluion of 150ps, with low material budget per station (0.5% X0) and a fluence comparable to the one expected for the inner trackers of LHC detectors in 10 years of operation. To compensate the time-walk, two read-out architectures have been designed and produced. The first architecture is based on a Constant Fraction Discriminator (CFD) followed by an on-pixel Time-to-Digital-Converter (TDC). The second architecture is based on a on-pixel group shared TDC. The GTK system developments are described: the integration steps (assembly and cooling) and the results obtained from the prototypes fabricated for the two read-out architectures.