M. Tytgat
Ghent University
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Featured researches published by M. Tytgat.
Physics Letters B | 2016
Khachatryan; Albert M Sirunyan; A. Tumasyan; W. Adam; E. Asilar; T. Bergauer; J. Brandstetter; M. Dragicevic; J. Erö; Martin Flechl; M. Friedl; R. Frühwirth; Vasile Mihai Ghete; C. Hartl; N. Hörmann; J. Hrubec; M. Jeitler; Axel König; I. Krätschmer; D. Liko; T. Matsushita; I. Mikulec; D. Rabady; Navid Rad; B. Rahbaran; H. Rohringer; Jochen Schieck; J. Strauss; W. Treberer-Treberspurg; W. Waltenberger
A search for new physics is performed based on all-hadronic events with large missing transverse momentum produced in proton-proton collisions at √ s = 13 TeV. The data sample, corresponding to an integrated luminosity of 2.3 fb−1, was collected with the CMS detector at the CERN LHC in 2015. The data are examined in search regions of jet multiplicity, tagged bottom quark jet multiplicity, missing transverse momentum, and the scalar sum of jet transverse momenta. The observed numbers of events in all search regions are found to be consistent with the expectations from standard model processes. Exclusion limits are presented for simplified supersymmetric models of gluino pair production. Depending on the assumed gluino decay mechanism, and for a massless, weakly interacting, lightest neutralino, lower limits on the gluino mass from 1440 to 1600 GeV are obtained, significantly extending previous limits. Published in Physics Letters B as doi:10.1016/j.physletb.2016.05.002. c
Journal of Instrumentation | 2013
D. Abbaneo; M. Abbrescia; M. Abi Akl; C Armaingaud; P. Aspell; Y. Assran; S. Bally; Y. Ban; P. Barria; L. Benussi; V. Bhopatkar; S. Bianco; Jelte E. Bos; O. Bouhali; J. Cai; Cesare Calabria; A. Castaneda; S. Cauwenbergh; Ali Celik; J. Christiansen; S. Colafranceschi; Anna Colaleo; A. Conde Garcia; G. De Lentdecker; R. De Oliveira; G. De Robertis; S. Dildick; S. Ferry; W. Flanagan; J. Gilmore
The CMS GEM collaboration is performing a feasibility study to install triple-GEM detectors in the forward region of the muon system (1.6 < vertical bar eta vertical bar < 2.4) of the CMS detector at the LHC. Such micro-pattern gas detectors are able to cope with the extreme particle rates that are expected in that region during the High Luminosity phase of the LHC. With their spatial resolution of order 100 micron GEMs would not only provide additional benefits in the CMS muon High Level Trigger, but also in the muon identification and track reconstruction, effectively combining tracking and triggering capabilities in one single device. The present status of the full project will be reviewed, highlighting all importants steps and achievements since the start of the R& D in 2009. Several small and full-size prototypes were constructed with different geometries and techniques. The baseline design of the triple-GEM detector for CMS will be described, along with the results from extensive test measurements of all prototypes both in the lab and in test beams at the CERN SPS. The proposed on-and off-detector electronics for the final system will be presented.
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 Instrumentation | 2013
D. Abbaneo; M. Abbrescia; M. Abi Akl; C Argamaingaud; P. Aspell; Y. Assran; S. Bally; Y. Ban; P. Barria; L. Benussi; V. Bhopatkar; S. Bianco; Jelte E. Bos; O. Bouhali; J. Cai; C. Calabria; A. Castaneda; S. Cauwenbergh; A. Celik; J. Christiansen; S. Colafranceschi; Anna Colaleo; A. Conde Garcia; G. De Lentdecker; R. De Oliveira; G. De Robertis; S. Dildick; S. Ferry; W. Flanagan; J. Gilmore
The international CMS GEM collaboration is studying the feasibility of upgrading the CMS forward muon system by adding layers of triple GEM based detectors. After successful tests of small size tripe-GEM chambers in the period of 2010-2011, the collaboration has designed, built and tested full-size GEM chambers for the upgrade purpose. We report on results from test beam and simulation that were conducted to study the performance of the GEM chambers.
Journal of Instrumentation | 2014
D. Abbaneo; M. Abbrescia; M. Abi Akl; C Armaingaud; P. Aspell; Y. Assran; S. Bally; Y. Ban; S. Banerjee; P. Barria; L. Benussi; V. Bhopatkar; S. Bianco; Jelte E. Bos; O. Bouhali; J. Cai; Cesare Calabria; A. Castaneda; S. Cauwenbergh; Ali Celik; J. Christiansen; S. Colafranceschi; Anna Colaleo; A. Conde Garcia; G. De Lentdecker; R. De Oliveira; G. De Robertis; S. Dildick; S. Ferry; W. Flanagan
The LHC data-taking will resume in 2015 with energy of 13-14 TeV and luminosity of 2 divided by 5 x 10(34) cm(-2) s(-1). At those energies, a considerable fraction of the particles produced propagate in the high pseudo-rapidity regions. The proposal for the upgrade of the CMS muon forward system involves Gas Electron Multiplier (GEM) chambers to be installed during the second LHC Long Shutdown (LS2) covering the pseudorapidity range 1 : 5 < vertical bar h vertical bar < 2.2. This detector is able to handle the extreme particle rates expected in this region when the LHC will be running at higher luminosity. The GEM is an excellent choice, as its high spatial resolution (order of 100 m m) allows to combine tracking and triggering capabilities, which will improve the CMS muon High Level Trigger, the muon identification and the track reconstruction. Intense R&D has been going on since 2009 and it has lead to the development of several GEM prototypes and associated detector electronics. These GEM prototypes have been subjected to extensive tests in the laboratory and in test beams at the CERN Super Proton Synchrotron (SPS). This contribution will review the status of the CMS upgrade project with GEMs, discussing also the trigger performance.
Journal of Instrumentation | 2016
K. S. Lee; Sungwoong Cho; S. Choi; B. Hong; Y. Go; M. Kang; Jaehoon Lim; Sue Kyung Park; A. Cimmino; S. Crucy; A. Fagot; M. Gul; Aao Rios; M. Tytgat; N. Zaganidis; S. Aly; Y. Assran; A. Radi; A. Sayed; G. Singh; M. Abbrescia; G. Iaselli; M. Maggi; G. Pugliese; P. Verwilligen; W. Van Doninck; S. Colafranceschi; Archana Sharma; L. Benussi; S. Bianco
We report on a systematic study of double-gap and four-gap phenolic resistive plate chambers (RPCs) for future high-{eta} RPC triggers in the CMS. In the present study, we constructed real-sized double-gap and four-gap RPCs with gap thicknesses of 1.6 and 0.8 mm, respectively, with 2-mm-thick phenolic high-pressure-laminated (HPL) plates. We examined the prototype RPCs for cosmic rays and 100 GeV muons provided by the SPS H4 beam line at CERN. We applied maximum gamma rates of 1.5 kHz cm-2 provided by 137Cs sources at Korea University and the GIF++ irradiation facility installed at the SPS H4 beam line to examine the rate capabilities of the prototype RPCs. In contrast to the case of the four-gap RPCs, we found the relatively high threshold was conducive to effectively suppressing the rapid increase of strip cluster sizes of muon hits with high voltage, especially when measuring the narrow-pitch strips. The gamma-induced currents drawn in the four-gap RPC were about one-fourth of those drawn in the double-gap RPC. The rate capabilities of both RPC types, proven through the present testing using gamma-ray sources, far exceeded the maximum rate expected in the new high-{eta} endcap RPCs planned for future phase-II LHC runs.We report on a systematic study of double-gap and four-gap phenolic resistive plate chambers (RPCs) for the Phase-2 upgrade of the CMS muon system at high eta. In the present study, we constructed real-sized double-gap and four-gap RPCs with gap thicknesses of 1.6 and 0.8 mm, respectively, with 2-mm-thick phenolic high-pressure-laminated (HPL) plates. We examined the prototype RPCs with cosmic rays and with 100-GeV muons provided by the SPS H4 beam line at CERN. To examine the rate capability of the prototype RPCs both at Korea University and at the CERN GIF++ facility, the chambers were irradiated with Cs-137 sources providing maximum gamma rates of about 1.5 kHz cm(-2). For the 1.6-mm-thick double-gap RPCs, we found the relatively high threshold on the produced detector charge was conducive to effectively suppressing the rapid increase of strip cluster sizes of muon hits with high voltage, especially when measuring the narrow-pitch strips. The gamma-induced currents drawn in the four-gap RPC were about one-fourth of those drawn in the double-gap RPC. The rate capabilities of both RPC types, proven through the present testing using gamma-ray sources, far exceeded the maximum rate expected in the new high-eta endcap RPCs planned for future phase-II runs of the Large Hadron Collider (LHC).
Journal of Instrumentation | 2016
M. Abbrescia; S. Muhammad; F. Primavera; S. Bianco; D. Pierluigi; Antonio Russo; P. Van Auwegem; D. Piccolo; M. Ferrini; L. Benussi; L. Passamonti; S. Cauwenbergh; G. Saviano; M. Tytgat
The operations of Resistive Plate Chambers in LHC experiments require Fluorine based (F-based) gases for optimal performance. Recent European regulations demand the use of environmentally unfriendly F-based gases to be limited or banned. In view of the CMS experiment upgrade, several tests are ongoing to measure the performance of the detector with these new ecological gas mixtures, in terms of efficiency, streamer probability, induced charge and time resolution. Prototype chambers with readout pads and with the standard CMS electronic setup are under test. In this paper preliminary results on performance of RPCs operated with a potential eco-friendly gas candidate 1,3,3,3-Tetrafluoropropene, commercially known as HFO-1234ze, with CO2 and CF3I based gas mixtures are presented and discussed for the possible application in the CMS experiment.
Journal of Instrumentation | 2016
A. Fagot; A. Cimmino; S. Crucy; M. Gul; Aao Rios; M. Tytgat; N. Zaganidis; S. Aly; Y. Assran; A. Radi; A. Sayed; G. Singh; M. Abbrescia; G. Iaselli; M. Maggi; G. Pugliese; P. Verwilligen; W. Van Doninck; S. Colafranceschi; Archana Sharma; L. Benussi; S. Bianco; D. Piccolo; F. Primavera; V. Bhatnagar; R. Kumari; A. Mehta; J. B. Singh; A. Ahmad; W. Ahmed
The high pseudo-rapidity region of the CMS muon system is covered by Cathode Strip Chambers (CSC) only and lacks redundant coverage despite the fact that it is a challenging region for muons in terms of backgrounds and momentum resolution. In order to maintain good efficiency for the muon trigger in this region additional RPCs are planned to be installed in the two outermost stations at low angle named RE3/1 and RE4/1. These stations will use RPCs with finer granularity and good timing resolution to mitigate background effects and to increase the redundancy of the system.
Journal of Instrumentation | 2016
M. Gul; A. Braghieri; A. Magnani; I. Crotty; A. Dimitrov; J. Vaitkus; P. Vitulo; A. Fagot; F. Thyssen; C. Avila; Y. Assran; G. Pugliese; S. Buontempo; N. Zaganidis; S. Crucy; G. Lanza; G. Singh; J. B. Singh; P. Petkov; S. Muhammad; M. I. Asghar; K. S. Lee; C U Estrada; J. Goh; S. Aly; I. Bagaturia; L. Lista; Min Suk Kim; C. Riccardi; D. Kim
In the framework of the High Luminosity LHC upgrade program, the CMS muon group built several different RPC prototypes that are now under test at the new CERN Gamma Irradiation Facility (GIF++). A dedicated Detector Control System (DCS) has been developed using the WinCC-OA tool to control and monitor these prototype detectors and to store the measured parameters data. Preliminary efficiency studies that set the base performance measurements of CMS RPC for starting aging studies are also presented.
nuclear science symposium and medical imaging conference | 2012
I. Laktineh; L. Caponetto; S. Cauwenbergh; C. Combret; I. Crotty; Y. Haddad; G. Grenier; R. Guida; R. Kieffer; N. Lumb; L. Mirabito; F. Schirra; N. Seguin; M. Tytgat; M. Vander Donckt; Y. Wang; Nicolas Zaganidis
The limitation of the detection rate of standard bakelite resistive plate chambers (RPC) used as muon detector in LHC experiments is behind the absence of such detectors in the high η regions in both CMS and ATLAS detectors. RPCs made with low resistivity glass plates (1010 Ω.cm) could be an adequate solution to equip the high TJ regions extending thus both the trigger efficiency and the physics performance. Different beam tests with single and multi-gap configurations using the new glass have shown that such detectors can operate at few thousands Hzlcm2 with high efficiency(>90%).