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Factors associated with smoking among tuberculosis patients in Spain

  • Jiménez-Fuentes, María Ángeles
  • Rodrigo, Teresa
  • Altet, María Neus
  • Jiménez-Ruiz, Carlos A.
  • Casals, Martí
  • Penas, Antón
  • Mir, Isabel
  • Solano Reina, Segismundo
  • Riesco-Miranda, Juan Antonio
  • Caylá, Joan A.
Altres ajuts: This work was made possible by a grant from the Spanish Society of Pneumology and Thoracic Surgery, SEPAR 2011., To determine the prevalence of smoking and analyze associated factors in a cohort of patients diagnosed with tuberculosis (TB) in Spain between 2006 and 2013. Multicenter, cross-sectional, descriptive, observational study using a national database of TB patients, using logistic regression to calculate odds ratios (OR) and confidence intervals (CI). We analyzed 5,846 cases (62 % men, mean age 39 years, 33 % foreigners). 23.4 % were alcohol abuser, 1.3 % were injected drug users (IDU), 4.6 % were co-infected with HIV, and 7.5 % had a history of TB treatment. 6.6 % and 0.8 % showed resistance to one and multiple drugs, respectively. The predominant clinical presentation was pulmonary (71 %) with a cavitary radiological pattern in 32.8 % of cases. 82 % of cases were confirmed microbiologically, and 54 % were smear-positive microscopy. 2,300 (39.3 %) patients were smokers. The following factors were associated with smoking: male sex (OR = 2.26;CI:1.97;2.60), Spanish origin (OR = 2.79;CI:2.40-3.24), alcoholism (OR = 2.85;CI:2.46;3.31), IDU (OR = 2.78;CI:1.48;5.52), homelessness (OR = 1.99;CI:1.14-3.57), pulmonary TB (OR = 1.61;CI:1.16;2.24), cavitary radiological pattern (OR = 1.99;CI:1.43;2.79) and a smear-positive microscopy at the time of diagnosis (OR = 1.39;CI:1.14;1.17). The prevalence of smoking among TB patients is high. Smokers with TB have a distinct sociodemographic, clinical, radiological and microbiological profile to non-smokers.
Proyecto:


Azimuthal anisotropy of charged particles with transverse momentum up to 100 GeV/c in PbPb collisions at √sNN= 5.02 TeV

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  • Dragicevic, M.
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  • Scheuch, F.
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  • Locci, E.
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  • Qu,H.
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  • Gouskos, J.
  • Konyushikhin, M.
  • Albrow, M.
  • Malberti, M.
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  • Hart, A.
  • Sekmen, S.
  • Adams, M. R.
  • Gran, J.
  • Heller, R.
  • Pieri, M.
  • Singh, G.
  • Tiras, E.
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  • Kalsi, A. K.
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  • Shi, M.
  • Fisk, I.
  • Sobol, A.
  • Heindl, M.
  • Bahinipati, S.
  • Mullin, S. D.
  • Mcginn, C.
  • Romero, L.
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  • Casal, Bruno
  • Musienko, Y.
  • Eerola, P.
  • Steinbrueck, Georg
The Fourier coeffcients v2and v3characterizing the anisotropy of the azimuthal distribution of charged particles produced in PbPb collisions at √sNN= 5.02 TeV are measured with data collected by the CMS experiment. The measurements cover a broad transverse momentum range, 1 < pT< 100 GeV/c. The analysis focuses on the pT> 10 GeV/c range, where anisotropic azimuthal distributions should reflect the path-length dependence of parton energy loss in the created medium. Results are presented in several bins of PbPb collision centrality, spanning the 60% most central events. The v2coeffcient is measured with the scalar product and the multiparticle cumulant methods, which have different sensitivities to initial-state fluctuations. The values from both methods remain positive up to pT∼ 60–80 GeV/c, in all examined centrality classes. The v3coeffcient, only measured with the scalar product method, tends to zero for pT>~ 20 GeV/c. Comparisons between theoretical calculations and data provide new constraints on the path-length dependence of parton energy loss in heavy ion collisions and highlight the importance of the initial-state fluctuations., Individuals have received support from the Marie-Curie program and the European Research Council and EPLANET (European Union); the Leventis Foundation; the A.P. Sloan Foundation; the Alexander von Humboldt Foundation; the Belgian Federal Science Policy Office; the Fonds pour la Formation à la Recherche dans l'Industrie et dans l'Agriculture (FRIA-Belgium); the Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium); the Ministry of Education, Youth and Sports (MEYS) of the Czech Republic; the Council of Science and Industrial Research, India; the HOMING PLUS program of the Foundation for Polish Science, cofinanced from European Union, Regional Development Fund, the Mobility Plus program of the Ministry of Science and Higher Education, the National Science Center (Poland), contracts Harmonia 2014/14/M/ST2/00428, Opus 2014/13/B/ST2/02543, 2014/15/B/ST2/03998, and 2015/19/B/ST2/02861, Sonata-bis 2012/07/E/ST2/01406; the National Priorities Research Program by Qatar National Research Fund; the Programa Clarín-COFUND del Principado de Asturias; the Thalis and Aristeia programs cofinanced by EU-ESF and the Greek NSRF; the Rachadapisek Sompot Fund for Postdoctoral Fellowship, Chulalongkorn University and the Chulalongkorn Academic into Its 2nd Century Project Advancement Project (Thailand); and the Welch Foundation, contract C-1845., Peer Reviewed
Proyecto:


The network of photodetectors and diode lasers of the CMS Link alignment system

  • Arce, Pedro
  • Barcala, J. M.
  • Calvo, E.
  • Ferrando, A.
  • Josa, M. I.
  • Molinero, A.
  • Navarrete, J.
  • Oller, J. C.
  • Brochero Cifuentes, J. A.
  • Calderon, Alicia
  • Fernández, M. G.
  • Gómez, G.
  • González Sánchez, J.
  • Martínez-Rivero, Celso
  • Matorras, Francisco
  • Rodrigo, Teresa
  • Martínez Ruiz del Arbol, P.
  • Scodellaro, Luca
  • Sobron Sañudo, M.
  • Vila, Iván
  • López Virto, A.
  • Fernández, J.
  • Raics, P.
  • Szabó, Z.
  • Trócsnyi, Z.
  • Ujvari, B.
  • Zilizi, G.
  • Beni, N.
  • Christian, G.
  • Imrek, J.
  • Molnar, J.
  • Novak, D.
  • Pálinkás, J.
  • Székely, G.
  • Szillási, Z.
  • Bencze, G.
  • Vestergombi, G.
  • Benettoni, M.
  • Gasparini, F.
  • Montecassiano, F.
  • Rampazzo, M.
  • Zago, M.
  • Benvenuti, A. C.
  • Reithler, H.
  • Jiang, C. H.
The central feature of the CMS Link alignment system is a network of Amorphous Silicon Position Detectors distributed throughout the muon spectrometer that are connected by multiple laser lines. The data collected during the years from 2008 to 2015 is presented confirming an outstanding performance of the photo sensors during more than seven years of operation. Details of the photo sensor readout of the laser signals are presented. The mechanical motions of the CMS detector are monitored using these photosensors and good agreement with distance sensors is obtained., Open Access funded by CERN., Peer Reviewed
Proyecto:


Observation of the rare Bs0 →µ+µ− decay from the combined analysis of CMS and LHCb data

  • CMS Collaboration
  • Khachatryan, V.
  • Martínez-Vidal, Fernando
  • Ruiz Valls, Pablo
  • Oyanguren, Arantza
  • Sánchez Mayordomo, Carlos
  • Brochero Cifuentes, J. A.
  • Calderon, Alicia
  • Cabrillo, I. J.
  • Duarte Campderros, J.
  • Fernández, M.
  • Gómez, G.
  • Graziano, A.
  • López Virto, A.
  • Marco, Jesús
  • Marco, Rafael
  • Martínez-Rivero, Celso
  • Matorras, Francisco
  • Muñoz Sánchez, F. J.
  • Piedra, Jonatan
  • Rodrigo, Teresa
  • Rodríguez Marrero, Ana Y.
  • Ruiz Jimeno, Alberto
  • Scodellaro, Luca
  • Vila, Iván
  • Vilar, Rocío
This work is licensed under a Creative Commons Attribution-NonCommercial-ShareAlike 3.0 Unported licence.-- et al., The standard model of particle physics describes the fundamental particles and their interactions via the strong, electromagnetic and weak forces. It provides precise predictions for measurable quantities that can be tested experimentally. The probabilities, or branching fractions, of the strange B meson (B-s(0)) and the B-0 meson decaying into two oppositely charged muons (mu(+) and mu(-)) are especially interesting because of their sensitivity to theories that extend the standard model. The standard model predicts that the B-s(0)->mu(+)mu(-) and B-0 ->mu(+)mu(-) decays are very rare, with about four of the former occurring for every billion B-s(0) mesons produced, and one of the latter occurring for every ten billion B-0 mesons(1). A difference in the observed branching fractions with respect to the predictions of the standard model would provide a direction in which the standard model should be extended. Before the Large Hadron Collider (LHC) at CERN2 started operating, no evidence for either decay mode had been found. Upper limits on the branching fractions were an order of magnitude above the standard model predictions. The CMS (Compact Muon Solenoid) and LHCb(Large Hadron Collider beauty) collaborations have performed a joint analysis of the data from proton-proton collisions that they collected in 2011 at a centre-of-mass energy of seven teraelectronvolts and in 2012 at eight teraelectronvolts. Here we report the first observation of the B-s(0)->mu(+)mu(-) decay, with a statistical significance exceeding six standard deviations, and the best measurement so far of its branching fraction. Furthermore, we obtained evidence for the B-0 ->mu(+)mu(-) decay with a statistical significance of three standard deviations. Both measurements are statistically compatible with standard model predictions and allow stringent constraints to be placed on theories beyond the standard model. The LHC experiments will resume taking data in 2015, recording proton-proton collisions at a centre-of-mass energy of 13 teraelectronvolts, which will approximately double the production rates of B-s(0) and B-0 mesons and lead to further improvements in the precision of these crucial tests of the standard model., We express our gratitude to colleagues in the CERN accelerator departments for the excellent performance of the LHC. We thank the technical and administrative staff at CERN, at the CMS institutes and at the LHCb institutes. In addition, we gratefully acknowledge the computing centres and personnel of the Worldwide LHC Computing Grid for delivering so effectively the computing infrastructure essential to our analyses. Finally, we acknowledge the enduring support for the construction and operation of the LHC, the CMS and the LHCb detectors provided by CERN and by many funding agencies. The following agencies provide support for both CMS and LHCb: CAPES, CNPq, FAPERJ and FINEP (Brazil); NSFC (China); CNRS/IN2P3 (France); BMBF, DFG and HGF (Germany); SFI (Ireland); INFN (Italy); NASU (Ukraine); STFC (UK); and NSF (USA). Agencies that provide support for CMS only are BMWFW and FWF (Austria); FNRS and FWO (Belgium); FAPESP (Brazil); MES (Bulgaria); CAS and MoST (China); COLCIENCIAS (Colombia); MSES and CSF (Croatia); RPF (Cyprus); MoER, ERC IUT and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA (France); GSRT (Greece); OTKA and NIH (Hungary); DAE and DST (India); IPM (Iran); NRF and WCU (Republic of Korea); LAS (Lithuania); MOE and UM (Malaysia); CINVESTAV, CONACYT, SEP, and UASLP-FAI (Mexico); MBIE (New Zealand); PAEC (Pakistan); MSHE and NSC (Poland); FCT (Portugal); JINR (Dubna); MON, RosAtom, RAS and RFBR (Russia); MESTD (Serbia); SEIDI and CPAN (Spain); Swiss Funding Agencies (Switzerland); MST (Taipei); ThEPCenter, IPST, STAR and NSTDA (Thailand); TUBITAK and TAEK (Turkey); SFFR (Ukraine); and DOE (USA). Agencies that provide support for only LHCb are: FINEP (Brazil); MPG (Germany); FOM and NWO (The Netherlands); MNiSW and NCN (Poland); MEN/IFA (Romania); MinES and FANO (Russia); MinECo (Spain); SNSF and SER (Switzerland). Individuals from the CMS collaboration have received support from the Marie-Curie programme and the European Research Council and EPLANET (European Union); the Leventis Foundation; the A. P. Sloan Foundation; the Alexander von Humboldt Foundation; the Belgian Federal Science Policy Office; the Fonds pour la Formation a la Recherche dans l'Industrie et dans l'Agriculture (FRIABelgium); the Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium); the Ministry of Education, Youth and Sports (MEYS) of the Czech Republic; the Council of Science and Industrial Research, India; the HOMING PLUS programme of Foundation for Polish Science, cofinanced from European Union, Regional Development Fund; the Compagnia di San Paolo (Torino); the Consorzio per la Fisica (Trieste); MIUR project 20108T4XTM (Italy); the Thalis and Aristeia programmes cofinanced by EU-ESF and the Greek NSRF; and the National Priorities Research Program by Qatar National Research Fund. Individual groups or members of the LHCb collaboration have received support from EPLANET, Marie Sklodowska-Curie Actions and ERC (European Union), Conseil general de Haute-Savoie, Labex ENIGMASS and OCEVU, Region Auvergne (France), RFBR (Russia), XuntaGal and GENCAT (Spain), Royal Society and Royal Commission for the Exhibition of 1851 (UK). LHCb is also thankful for the computing resources and the access to software R&D tools provided by Yandex LLC (Russia). The CMS and LHCb collaborations are indebted to the communities behind the multiple open source software packages on which they depend., Peer reviewed
Proyecto:
Ver en: http://hdl.handle.net/10261/126468, http://dx.doi.org/10.13039/501100002322, http://dx.doi.org/10.13039/501100003593, http://dx.doi.org/10.13039/501100003141, http://dx.doi.org/10.13039/100007388, http://dx.doi.org/10.13039/501100004794, http://dx.doi.org/10.13039/501100001822, http://dx.doi.org/10.13039/100000879, http://dx.doi.org/10.13039/100005156, http://dx.doi.org/10.13039/501100002341, http://dx.doi.org/10.13039/501100004117, http://dx.doi.org/10.13039/501100005324, http://dx.doi.org/10.13039/501100000781, http://dx.doi.org/10.13039/501100000782, http://dx.doi.org/10.13039/501100002347, http://dx.doi.org/10.13039/501100004809, http://dx.doi.org/10.13039/501100002661, http://dx.doi.org/10.13039/501100004586, http://dx.doi.org/10.13039/501100001871, http://dx.doi.org/10.13039/501100003448, http://dx.doi.org/10.13039/501100002809, http://dx.doi.org/10.13039/501100001659, http://dx.doi.org/10.13039/501100001656, http://dx.doi.org/10.13039/501100003329, http://dx.doi.org/10.13039/501100003407, http://dx.doi.org/10.13039/501100001809, http://dx.doi.org/10.13039/501100003725, http://dx.doi.org/10.13039/501100004281, http://dx.doi.org/10.13039/100000001, http://dx.doi.org/10.13039/501100008687, http://dx.doi.org/10.13039/501100002674, http://dx.doi.org/10.13039/501100002261, http://dx.doi.org/10.13039/501100001602, http://dx.doi.org/10.13039/501100008202, http://dx.doi.org/10.13039/501100000780, http://dx.doi.org/10.13039/501100000271, http://dx.doi.org/10.13039/501100001409, http://dx.doi.org/10.13039/100000015, http://dx.doi.org/10.13039/501100001502


Search for heavy resonances in the W/Z-tagged dijet mass spectrum in pp collisions at 7 TeV

  • Chatrchyan, S.
  • Brochero Cifuentes, J. A.
  • Cabrillo, I. J.
  • Calderon, Alicia
  • Chuang, S. H.
  • Duarte Campderros, J.
  • Felcini, Marta
  • Fernández, M.
  • Gómez, G.
  • González Sánchez, J.
  • Graziano, A.
  • Jorda, C.
  • López Virto, A.
  • Marco, Jesús
  • Marco, Rafael
  • Martínez-Rivero, Celso
  • Matorras, Francisco
  • Muñoz Sánchez, F. J.
  • Rodrigo, Teresa
  • Rodríguez Marrero, Ana Y.
  • Ruiz Jimeno, Alberto
  • Scodellaro, Luca
  • Vila, Iván
  • Vilar, Rocío
  • CMS Collaboration
This article is published Open Access at sciencedirect.com.It is distributed under the terms of the Creative Commons Attribution License 3.0.-- et al., A search has been made for massive resonances decaying into a quark and a vector boson, qW or qZ, or a pair of vector bosons, WW, WZ, or ZZ, where each vector boson decays to hadronic final states. This search is based on a data sample corresponding to an integrated luminosity of 5.0 fb−15.0 fb−1 of proton–proton collisions collected in the CMS experiment at the LHC in 2011 at a center-of-mass energy of 7 TeV. For sufficiently heavy resonances the decay products of each vector boson are merged into a single jet, and the event effectively has a dijet topology. The background from QCD dijet events is reduced using recently developed techniques that resolve jet substructure. A 95% CL lower limit is set on the mass of excited quark resonances decaying into qW (qZ) at 2.38 TeV (2.15 TeV) and upper limits are set on the cross section for resonances decaying to qW, qZ, WW, WZ, or ZZ final states., We acknowledge support from BMWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MEYS (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES (Croatia); RPF (Cyprus); MoER, SF0690030s09 and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); NRF and WCU (Korea); LAS (Lithuania); CINVESTAV, CONACYT, SEP, and UASLPFAI (Mexico); MSI (New Zealand); PAEC (Pakistan); MSHE and NSC (Poland); FCT (Portugal); JINR (Armenia, Belarus, Georgia, Ukraine Uzbekistan); MON, RosAtom, RAS and RFBR (Russia); MSTD (Serbia); SEIDI and CPAN (Spain); Swiss Funding Agencies (Switzerland); NSC (Taipei); ThEP, IPST and NECTEC (Thailand); TUBITAK and TAEK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (USA)., Peer Reviewed
Proyecto:


Search for heavy narrow dilepton resonances in pp collisions at √s=7 TeV and √s=8 TeV

  • Chatrchyan, S.
  • Brochero Cifuentes, J. A.
  • Cabrillo, I. J.
  • Cabrillo, I. J.
  • Calderon, Alicia
  • Chuang, S. H.
  • Duarte Campderros, J.
  • Felcini, Marta
  • Fernández, M.
  • Gómez, G.
  • González Sánchez, J.
  • Graziano, A.
  • Jorda, C.
  • López Virto, A.
  • Marco, Jesús
  • Marco, Rafael
  • Martínez-Rivero, Celso
  • Matorras, Francisco
  • Muñoz Sánchez, F. J.
  • Rodrigo, Teresa
  • Rodríguez Marrero, Ana Y.
  • Ruiz Jimeno, Alberto
  • Scodellaro, Luca
  • Vila, Iván
  • Vilar, Rocío
  • CMS Collaboration
This article is published Open Access at sciencedirect.com. It is distributed under the terms of the Creative Commons Attribution License 3.0.-- et al., An updated search for heavy narrow resonances decaying to muon or electron pairs using the CMS detector is presented. Data samples from pp collisions at √s = 7 TeV and 8 TeV at the LHC, with integrated luminosities of up to 5.3 and 4.1 fb−1, respectively, are combined. No evidence for a heavy narrow resonance is observed. The analysis of the combined data sets excludes, at 95% confidence level, a Sequential Standard Model Z'SSM resonance lighter than 2590 GeV, a superstring-inspired Z'ψ lighter than 2260 GeV, and Kaluza–Klein gravitons lighter than 2390 (2030) GeV, assuming that the coupling parameter k/MPl is 0.10 (0.05). These are the most stringent limits to date., We acknowledge support from BMWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MEYS (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES (Croatia); RPF (Cyprus); MoER, SF0690030s09 and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); NRF and WCU (Korea); LAS (Lithuania); CINVESTAV, CONACYT, SEP, and UASLPFAI (Mexico); MSI (New Zealand); PAEC (Pakistan); MSHE and NSC (Poland); FCT (Portugal); JINR (Armenia, Belarus, Georgia, Ukraine Uzbekistan); MON, RosAtom, RAS and RFBR (Russia); MSTD (Serbia); SEIDI and CPAN (Spain); Swiss Funding Agencies (Switzerland); NSC (Taipei); ThEP, IPST and NECTEC (Thailand); TUBITAK and TAEK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (USA)., Peer Reviewed
Proyecto:


Search for narrow resonances using the dijet mass spectrum in pp collisions at √s=8 TeV

  • Chatrchyan, S.
  • Brochero Cifuentes, J. A.
  • Cabrillo, I. J.
  • Calderon, Alicia
  • Chuang, S. H.
  • Duarte Campderros, J.
  • Felcini, Marta
  • Fernández, M.
  • Gómez, G.
  • González Sánchez, J.
  • Graziano, A.
  • Jorda, C.
  • López Virto, A.
  • Marco, Jesús
  • Marco, Rafael
  • Martínez-Rivero, Celso
  • Matorras, Francisco
  • Muñoz Sánchez, F. J.
  • Rodrigo, Teresa
  • Rodríguez Marrero, Ana Y.
  • Ruiz Jimeno, Alberto
  • Scodellaro, Luca
  • Vila, Iván
  • Vilar, Rocío
  • CMS Collaboration
Results are presented of a search for the production of new particles decaying to pairs of partons (quarks, antiquarks, or gluons), in the dijet mass spectrum in proton-proton collisions at √s=8 TeV. The data sample corresponds to an integrated luminosity of 4.0 fb-1, collected with the CMS detector at the LHC in 2012. No significant evidence for narrow resonance production is observed. Upper limits are set at the 95% confidence level on the production cross section of hypothetical new particles decaying to quark-quark, quark-gluon, or gluon-gluon final states. These limits are then translated into lower limits on the masses of new resonances in specific scenarios of physics beyond the standard model. The limits reach up to 4.8 TeV, depending on the model, and extend previous exclusions from similar searches performed at lower collision energies. For the first time mass limits are set for the Randall-Sundrum graviton model in the dijet channel., We acknowledge support from BMWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MEYS (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES (Croatia); RPF (Cyprus); MoER, SF0690030s09 and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); NRF and WCU (Korea); LAS (Lithuania); CINVESTAV, CONACYT, SEP, and UASLPFAI (Mexico); MSI (New Zealand); PAEC (Pakistan); MSHE and NSC (Poland); FCT (Portugal); JINR (Armenia, Belarus, Georgia, Ukraine Uzbekistan); MON, RosAtom, RAS and RFBR (Russia); MSTD (Serbia); SEIDI and CPAN (Spain); Swiss Funding Agencies (Switzerland); NSC (Taipei); ThEP, IPST and NECTEC (Thailand); TUBITAK and TAEK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (USA)., Peer Reviewed
Proyecto:


Search for fractionally charged particles in pp collisions at √s=7 TeV

  • Chatrchyan, S.
  • Brochero Cifuentes, J. A.
  • Cabrillo, I. J.
  • Cabrillo, I. J.
  • Calderon, Alicia
  • Chuang, S. H.
  • Duarte Campderros, J.
  • Felcini, Marta
  • Fernández, M.
  • Gómez, G.
  • González Sánchez, J.
  • Graziano, A.
  • Jorda, C.
  • López Virto, A.
  • Marco, Jesús
  • Marco, Rafael
  • Martínez-Rivero, Celso
  • Matorras, Francisco
  • Muñoz Sánchez, F. J.
  • Rodrigo, Teresa
  • Rodríguez Marrero, Ana Y.
  • Ruiz Jimeno, Alberto
  • Scodellaro, Luca
  • Vila, Iván
  • Vilar, Rocío
  • CMS Collaboration
A search is presented for free heavy long-lived fractionally charged particles produced in pp collisions at √s=7 TeV. The data sample was recorded by the CMS detector at the LHC and corresponds to an integrated luminosity of 5.0 fb-1. Candidate fractionally charged particles are identified by selecting tracks with associated low charge measurements in the silicon tracking detector. Observations are found to be consistent with expectations for background processes. The results of the search are used to set upper limits on the cross section for pair production of fractionally charged, massive spin-1/2 particles that are neutral under SU(3)C and SU(2)L. We exclude at 95% confidence level such particles with electric charge ±2e/3 with masses below 310 GeV, and those with charge ±e/3 with masses below 140 GeV. © 2013 CERN. Published by the American Physical Society under the terms of the http://creativecommons.org/ licenses/by/3.0/Creative Commons Attribution 3.0 License. Further distribution of this work must maintain attribution to the author(s) and the published article's title, journal citation, and DOI., We acknowledge support from BMWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MEYS (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES (Croatia); RPF (Cyprus); MoER, SF0690030s09 and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); NRF and WCU (Korea); LAS (Lithuania); CINVESTAV, CONACYT, SEP, and UASLPFAI (Mexico); MSI (New Zealand); PAEC (Pakistan); MSHE and NSC (Poland); FCT (Portugal); JINR (Armenia, Belarus, Georgia, Ukraine Uzbekistan); MON, RosAtom, RAS and RFBR (Russia); MSTD (Serbia); SEIDI and CPAN (Spain); Swiss Funding Agencies (Switzerland); NSC (Taipei); ThEP, IPST and NECTEC (Thailand); TUBITAK and TAEK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (USA)., Peer Reviewed
Proyecto:


Search for gluino mediated bottom- and top-squark production in multijet final states in pp collisions at 8 TeV

  • Chatrchyan, S.
  • Brochero Cifuentes, J. A.
  • Cabrillo, I. J.
  • Calderon, Alicia
  • Chuang, S. H.
  • Duarte Campderros, J.
  • Fernández, M.
  • Gómez, G.
  • González Sánchez, J.
  • Graziano, A.
  • Jorda, C.
  • López Virto, A.
  • Marco, Jesús
  • Marco, Rafael
  • Martínez-Rivero, Celso
  • Matorras, Francisco
  • Muñoz Sánchez, F. J.
  • Rodrigo, Teresa
  • Rodríguez Marrero, Ana Y.
  • Ruiz Jimeno, Alberto
  • Scodellaro, Luca
  • Vila, Iván
  • Vilar, Rocío
  • CMS Collaboration
This article is published Open Access at sciencedirect.com. It is distributed under the terms of the Creative Commons Attribution License 3.0.-- et al., A search for supersymmetry is presented based on events with large missing transverse energy, no isolated electron or muon, and at least three jets with one or more identified as a bottom-quark jet. A simultaneous examination is performed of the numbers of events in exclusive bins of the scalar sum of jet transverse momentum values, missing transverse energy, and bottom-quark jet multiplicity. The sample, corresponding to an integrated luminosity of 19.4fb-1, consists of proton-proton collision data recorded at a center-of-mass energy of 8TeV with the CMS detector at the LHC in 2012. The observed numbers of events are found to be consistent with the standard model expectation, which is evaluated with control samples in data. The results are interpreted in the context of two simplified supersymmetric scenarios in which gluino pair production is followed by the decay of each gluino to an undetected lightest supersymmetric particle and either a bottom or top quark-antiquark pair, characteristic of gluino mediated bottom- or top-squark production. Using the production cross section calculated to next-to-leading-order plus next-to-leading-logarithm accuracy, and in the limit of a massless lightest supersymmetric particle, we exclude gluinos with masses below 1170GeV and 1020GeV for the two scenarios, respectively. © 2013 CERN., We acknowledge support from BMWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MEYS (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES (Croatia); RPF (Cyprus); MoER, SF0690030s09 and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); NRF and WCU (Korea); LAS (Lithuania); CINVESTAV, CONACYT, SEP, and UASLPFAI (Mexico); MSI (New Zealand); PAEC (Pakistan); MSHE and NSC (Poland); FCT (Portugal); JINR (Armenia, Belarus, Georgia, Ukraine Uzbekistan); MON, RosAtom, RAS and RFBR (Russia); MSTD (Serbia); SEIDI and CPAN (Spain); Swiss Funding Agencies (Switzerland); NSC (Taipei); ThEP, IPST and NECTEC (Thailand); TUBITAK and TAEK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (USA). Individuals have received support from the Marie-Curie programme and the European Research Council and EPLANET(EuropeanUnion); the Leventis Foundation; the A.P. Sloan Foundation; the Alexander von Humboldt Foundation; the Belgian Federal Science Policy Office; the Fonds pour la Formation à la Recherche dans l’Industrie et dansl’Agriculture (FRIA-Belgium); the Agentschap voor Innovatie door Wetenschapen Technologie (IWT-Belgium); the Ministry of Education, Youth and Sports(MEYS) of Czech Republic; the Council of Science and Industrial Research, India; the Compagnia di San Paolo(Torino); the HOMINGPLUS programme of Foundation for PolishScience, cofinanced by EU,Re-gional Development Fund; and the Thalis and Aristeia programmes cofinanced byEU-ESFand the Greek NSRF., Peer Reviewed
Proyecto:


Search for new physics in final states with a lepton and missing transverse energy in pp collisions at the LHC

  • Chatrchyan, S.
  • Brochero Cifuentes, J. A.
  • Cabrillo, I. J.
  • Cabrillo, I. J.
  • Calderon, Alicia
  • Chuang, S. H.
  • Duarte Campderros, J.
  • Fernández, M.
  • Gómez, G.
  • González Sánchez, J.
  • Graziano, A.
  • Jorda, C.
  • López Virto, A.
  • Marco, Jesús
  • Marco, Rafael
  • Martínez-Rivero, Celso
  • Matorras, Francisco
  • Muñoz Sánchez, F. J.
  • Rodrigo, Teresa
  • Rodríguez Marrero, Ana Y.
  • Ruiz Jimeno, Alberto
  • Scodellaro, Luca
  • Vila, Iván
  • Vilar, Rocío
  • CMS Collaboration
This Letter describes the search for an enhanced production rate of events with a charged lepton and a neutrino in high-energy pp collisions at the LHC. The analysis uses data collected with the CMS detector, with an integrated luminosity of 5.0 fb-1 at √s=7 TeV, and a further 3.7 fb -1 at √s=8 TeV. No evidence is found for an excess. The results are interpreted in terms of limits on a heavy charged gauge boson (W ′) in the sequential standard model, a split universal extra dimension model, and contact interactions in the helicity-nonconserving model. For the last, values of the binding energy below 10.5 (8.8) TeV in the electron (muon) channel are excluded at a 95% confidence level. Interpreting the ℓν final state in terms of a heavy W′ with standard model couplings, masses below 2.90 TeV are excluded. © 2013 CERN., We acknowledge support from BMWF and FWF (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MEYS (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES (Croatia); RPF (Cyprus); MoER, SF0690030s09 and ERDF (Estonia); Academy of Finland, MEC, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); NRF and WCU (Korea); LAS (Lithuania); CINVESTAV, CONACYT, SEP, and UASLPFAI (Mexico); MSI (New Zealand); PAEC (Pakistan); MSHE and NSC (Poland); FCT (Portugal); JINR (Armenia, Belarus, Georgia, Ukraine Uzbekistan); MON, RosAtom, RAS and RFBR (Russia); MSTD (Serbia); SEIDI and CPAN (Spain); Swiss Funding Agencies (Switzerland); NSC (Taipei); ThEP, IPST and NECTEC (Thailand); TUBITAK and TAEK (Turkey); NASU (Ukraine); STFC (United Kingdom); DOE and NSF (USA)., Peer Reviewed
Proyecto:


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