Search for pair-produced three-jet resonances in proton-proton collisions at $sqrt{s}= $ 13 TeV
Albert M Sirunyan,Robin Erbacher, Camilo Andres Carrillo Montoya, Wagner Carvalho,Maciej Górski,Danek Kotlinski,Balazs Ujvari, Samila Muthumuni, Ayse Polatoz,Shaaban Khalil,Nicholas Smith, Basile Vermassen,Young-Il Choi, Roumyana Hadjiiska, Amitabh Lath,Willard Johns, Lorenzo Uplegger, Pierre Van Hove, Mohammad Alhusseini, Alberto Orso Maria Iorio, Ulrich Heintz, Alessandro Thea,Giuseppe Latino,Andrew Hart, Federico Vazzoler, Teppo Mäenpää,Sinan Sagir, Georgios Tsipolitis,Jennifer Chu,Cristian Pena,Jozsef Molnar,Soureek Mitra,Torben Dreyer,Dominik Nowatschin, Sergei Slabospitskii,Shamik Ghosh, Mircho Rodozov,Michael Tytgat, Dooyeon Gyun, Robert Schöfbeck,Luc Pape, James Hirschauer, Burak Bilki, Shane Breeze, Francisco Yumiceva, Mustafa Numan Bakirci, Evrim Ersin Kangal,Reza Goldouzian,Ram Krishna Dewanjee, Chiara Rovelli, Daniele Fasanella,Wei Shi,Robert Hirosky, Santeri Laurila,Arnd Meyer,Hans Reithler,Lalit Mohan Pant, Danila Tlisov, Austin Baty, Tomas Lindén,Zachary Lesko, Gail Hanson,Giovanna Selvaggi, Furkan Dolek,Fabio Colombo,Jaehoon Lim, Christos Roskas, Bhawandeep Bhawandeep, Catherine Kirsty Mackay,Weifeng Ji, Wolfram Dietrich Zeuner,Tiziano Camporesi, Raphael Granier de Cassagnac,Georgios Daskalakis,Kin Ho Lo,Ernesto Migliore, Giacomo Ortona, Paul Schütze,Ece Asilar, Marcos Correa Martins Junior, Alexander Morton, Nicola Cavallo, Anne-Marie Magnan, Christopher Mcginn, Chanwook Hwang, Yasser Assran,André Holzner, Ta-Yung Ling,Kai-Feng Chen,Matthew Nguyen,David Stickland,Giorgio Apollinari,Marta Felcini,Damir Lelas,Xinmei Niu,Michal Olszewski,Scarlet Norberg, Oleksandr Zenaiev,Paul Lujan, Dennis Roy,Martijn Mulders,Fabrizio Palla,Satoshi Hasegawa,David Curry,Elena Popova, Roberval Walsh,Christopher Palmer, Kristan Allan Hahn,Tao Huang,Piotr Traczyk, Juozas Vaitkus,Prakash Thapa, Chia-Ming Kuo,Olena Karacheban, Alicia Calderon, Akshansh Singh,Pawan Kumar Netrakanti,Thomas Kress, Georgia Karapostoli,Fotios Ptochos,Noemi Beni, Anna Zanetti, Marc M Baarmand, Achille Petrilli, Bhargav Madhusudan Joshi, De Hua Zhu, Andreas Kornmayer, Clint Richardson,Maria Cepeda, Mauricio Thiel, Cécile Caillol, John Paul Chou,Linwei Li,Peicho Petkov,Natale Demaria,Davide Piccolo, Pawel de Barbaro,Nural Akchurin, Olaf Behnke,Russell Richard Betts,Vincenzo Innocente, Laura Dodd,Hyunchul Kim, Attila Racz,Paul Baillon, Viktor Savrin, Jyothsna Rani Komaragiri, Mario Masciovecchio, Jakob Salfeld-Nebgen, Rylan Conway,Kaya Tatar, Alexx Perloff, Dustin Anderson, Lukas Bäni,Viktor Khristenko, Dirk Krücker, Slawek Tkaczyk,Alan Campbell,Arabella Martelli, Devdatta Majumder,Isidro Gonzalez Caballero, Inna Kucher, Bernard Ille,Sudeshna Banerjee,Salvatore Buontempo, Silvia Taroni, Seh Wook Lee,Evangelos Paradas, Andrea Massironi, Candan Isik,David Lange,Ryan Mueller, Claus Kleinwort,Jingyu Zhang, Robert Fischer, Kuntal Mondal,Ivan Shvetsov,Samet Lezki, Joscha Knolle, Maximilian Heindl,Peter Wittich, Giovanni Abbiendi, Hao Qiu,Manfred Paulini, Diego Matos Figueiredo,Altan Cakir,Paolo Lariccia,Stefan Piperov,Jose M Hernandez,Huaqiao Zhang, Yutaro Iiyama, Konstantinos Vellidis,Vladimir Petrov, Cristina Martin Perez, Mario Galanti, Alberto Sánchez Hernández, Gilvan Alves,Iurii Antropov, Florian Michael Pitters, Alexander Nikitenko,Nikkie Deelen, Kevin Burkett,Seth Cooper,Regina Demina,Arun Kumar,Wuming Luo,Jay Dittmann,Till Arndt,Elvire Bouvier, David Krofcheck,Francesca Cenna,Zainol Abidin Ibrahim,Margaret Zientek, Timo Peltola, Adish Vartak,Marcus Hohlmann, Helen F Heath, Alberto Bragagnolo,Usama Hussain, Pedro Silva, Alexander Titterton,Julie Malcles, Erik Butz, Paul Kyberd, Richard Loveless, Alexander Dermenev,Dezso Horvath,Andrea Delgado, Andres Tiko,Sicheng Wang, Jens Multhaup,Andrei Gritsan, Rachel Yohay,Wolfgang Lohmann, Riccardo Andrea Manzoni,Francesco Fiori, Benjamin Charles Radburn-Smith,Yi Chen, Apostolos Panagiotou, Laszlo Gutay,Igor Smirnov, Frank Jm Geurts,Carlos Florez, Prafulla Kumar Behera, Martin Lipinski, Charles Harrington,Claudio Caputo,Muhammad Waqas, Evan Wolfe, Giancarlo Mantovani, Antonio María Pérez-Calero Yzquierdo, Brieuc Francois,Philip Chang, Renato Campanini, Pieter David,Francesco Navarria, Matthias Schröder, Federica Primavera, Max Philip Rauch, Ashim Roy, Mohd Adli Bin Ali, Klaas Padeken, Carlo Civinini,Alexey Kamenev,Maksym Titov, Matthieu Marionneau,Rizki Syarif,Manoj Sharan,Ioannis Papadopoulos, Michael Henry Schmitt,Unki Yang, Marina Kolosova, Pierluigi Paolucci, Abhisek Datta, Deniz Sunar Cerci, Christian Schnaible, Luigi Moroni, Boaz Klima,Mate Csanad,Etiennette Auffray, Kenyi Hurtado Anampa,John Conway, Zhangqier Wang, Pablo Martinez Ruiz del Arbol, Sang Il Pak,Hasan Ogul,Oliver Gutsche, Alexis Fagot,Evan Ranken, Christopher Rogan, Burin Asavapibhop, Andreas Güth, Quentin Ingram,Thomas Eichhorn, Gianluca Cerminara,Stefano Lacaprara, Matteo Sani, Amina Zghiche,Duccio Abbaneo,Paraskevas Sphicas, Willis Lin, Nairit Sur, Garyfallia Paspalaki, Suman Chatterjee,Silvia 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Kirsanov, Shahram Rahatlou, Daniel Salerno, Cameron Bravo, John Perry Cumalat, Giuseppe Iaselli, Loukas Gouskos, Paolo Capiluppi, Alessandro Di Mattia, Süleyman Durgut, Robert M Brown, Anirban Saha, Cristóvão Beirão Da Cruz E Silva, Maria Elena Pol, Lovedeep Kaur Saini, Maria Margherita Obertino, Panagiotis Kokkas, Igor Azhgirey, Thomas Ferguson, Kerstin Borras, Daniel Treille, Felicitas Pauss, Shashikant Dugad, Manjit Kaur, Ashley Parker, Monika Grothe, Allison Reinsvold, Benoit Courbon, Kevin Sung
PHYSICAL REVIEW D（2019）
引用 6|浏览55
摘要
A search has been performed for pair-produced resonances decaying into three jets. The proton-proton collision data used for this analysis were collected with the CMS detector in 2016 at a center-of-mass energy of 13 TeV and correspond to an integrated luminosity of 35.9 fb(-1). The mass range from 200 to 2000 GeV is explored in four separate mass regions. The observations show agreement with standard model expectations. The results are interpreted within the framework of R-parity violating SUSY, where pair-produced gluinos decay to a six quark final state. Gluino masses below 1500 GeV are excluded at 95% confidence level. An analysis based on data with multijet events reconstructed at the trigger level extends the reach to masses as low as 200 GeV. Improved analysis techniques have led to enhanced sensitivity, allowing the most stringent limits to date to be set on gluino pair production.
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