Search for a new scalar resonance decaying to a pair of Z bosons in proton-proton collisions at √s=13 TeV
2018
- Robin Erbacher
- C. A. Carrillo Montoya
- Dave M Newbold
- Wagner Carvalho
- Maciej Górski
- Danek Kotlinski
- Balázs Ujvári
- Samila Muthumuni
- Richard Lander
- Nicholas Smith
- Basile Vermassen
- Young-Il Choi
- Roumyana Hadjiiska
- Amitabh Lath
- Willard Johns
- Lorenzo Uplegger
- Pierre Van Hove
- Alberto Orso Maria Iorio
- Ulrich Heintz
- Alessandro Thea
- Giuseppe Latino
- Andrew Hart
- Teppo Mäenpää
- Sinan Sagir
- Jyothsna Rani Komaragiri
- Jennifer Chu
- Olga Driga
- Cristian Peña
- József Molnár
- Soureek Mitra
- Torben Dreyer
- Dominik Nowatschin
- Shamik Ghosh
- Mircho Rodozov
- Michael Tytgat
- Dooyeon Gyun
- Robert Schöfbeck
- Luc Pape
- James Hirschauer
- Burak Bilki
- Francisco Yumiceva
- 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
- Fabio Colombo
- Jaehoon Lim
- Christos Roskas
- Bhawandeep Bhawandeep
- Weifeng Ji
- Wolfram Dietrich Zeuner
- Tiziano Camporesi
- Raphael Granier de Cassagnac
- Georgios Daskalakis
- Kin Ho Lo
- Ernesto Migliore
- Ilknur Hos
- Giacomo Ortona
- Lothar At Bauerdick
- Ece Asilar
- Alexander Morton
- Nicola Cavallo
- Anne-Marie Magnan
- Christopher McGinn
- Chanwook Hwang
- Andre Holzner
- Ta-Yung Ling
- Kai-Feng Chen
- Matthew Nguyen
- David Stickland
- Giorgio Apollinari
- Marta Felcini
- Damir Lelas
- Esraa El-Khateeb
- Michał Olszewski
- Scarlet Norberg
- Oleksandr Zenaiev
- Jorge Luis Rodriguez
- Paul Lujan
- Martijn Mulders
- Fabrizio Palla
- Satoshi Hasegawa
- David Curry
- Sunil Bansal
- Roberval Walsh
- Christopher Palmer
- Kristan Allan Hahn
- Tao Huang
- Piotr Traczyk
- Willi Bertl
- Prakash Thapa
- George Stephans
- Olena Karacheban
- Alicia Calderón
- Thomas Peiffer
- Pawan Kumar Netrakanti
- Georgia Karapostoli
- Fotios Ptochos
- Noemi Beni
- Anna Zanetti
- Valerio Calvelli
- Achille Petrilli
- Bhargav Madhusudan Joshi
- De Hua Zhu
- Andreas Kornmayer
- Clint Richardson
- María Cepeda
- Mauricio Thiel
- J William Gary
- Cecile Caillol
- John Paul Chou
- Mohammed Mahmoud
- Peicho Petkov
- Natale Demaria
- Davide Piccolo
- Pawel de Barbaro
- Fabrizio Odorici
- Nural Akchurin
- Olaf Behnke
- Russell Richard Betts
- Vincenzo Innocente
- Hyunchul Kim
- Attila Rácz
- Paul Baillon
- Viktor Savrin
- Kunal Kothekar
- Mario Masciovecchio
- Adam Dishaw
- Rylan Conway
- Kaya Tatar
- Alexx Perloff
- Dustin Anderson
- Alexei Safonov
- Bibhuprasad Mahakud
- Viktor Khristenko
- Dirk Krücker
- Slawek Tkaczyk
- Alan Campbell
- Arabella Martelli
- Devdatta Majumder
- Isidro González Caballero
- Inna Kucher
- Bernard Ille
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- Salvatore Buontempo
- Silvia Taroni
- Seh Wook Lee
- Evangelos Paradas
- Andrea Massironi
- David Lange
- Ryan Mueller
- Claus Kleinwort
- Jingyu Zhang
- Robert Fischer
- Kuntal Mondal
- Ivan Shvetsov
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- Joscha Knolle
- Maximilian Heindl
- Peter Wittich
- Giovanni Abbiendi
- Hao Qiu
- Manfred Paulini
- Kenyi Hurtado Anampa
- Altan Çakir
- Paolo Lariccia
- Stefan Piperov
- Ka Hei Martin Kwok
- Huaqiao Zhang
- Yutaro Iiyama
- Vladimir Petrov
- Emine Gürpinar
- Mario Galanti
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- Florian Michael Pitters
- Eddi A. De Wolf
- Alexander Nikitenko
- Nikkie Deelen
- Kevin Burkett
- Seth Cooper
- Regina Demina
- Arun Kumar
- Wuming Luo
- Jay Dittmann
- Chunjie Wang
- Till Arndt
- Elvire Bouvier
- David Krofcheck
- Francesca Cenna
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- Marcus Hohlmann
- Sudha Ahuja
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- Matthew Carver
- Wolfgang Lohmann
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- Francesco Fiori
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- Apostolos Panagiotou
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- Igor Smirnov
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- Prafulla Kumar Behera
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- Walter Van Doninck
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- Paul Edmund Karchin
- Peter Raics
- Saeid Paktinat Mehdiabadi
- Maria Hempel
- Roberto Chierici
- James Bowen
- Anastasia Karavdina
- Sarmad Masood Shaheen
- Mareike Meyer
- Gaetano-Marco Dallavalle
- Ron Lipton
- Adolf Bornheim
- Felice Pantaleo
- Vineet Kumar
- Jason Sang Hun Lee
- Joze Zobec
- Semiray Girgis
- Joshua Hardenbrook
- Michael Plagge
- Yongbin Feng
- Mani Tripathi
- Cristina Oropeza Barrera
- Siarhei Shulha
- Achim Stahl
- Robert Klanner
- Andrew Melo
- Roberto Leonardi
- Sergey Polikarpov
- Leander Litov
- Tiziano Rovelli
- Maciej Misiura
- Brian Dorney
- Stephan Linn
- Mark Raymond Adams
- Urs Langenegger
- Marco Musich
- Philippe Busson
- Ioannis Papakrivopoulos
- Pushpalatha C. Bhat
- Mohammad Abrar Wadud
- Carlo Battilana
- Navid Rad
- Daniel Troendle
- Ulrich Husemann
- Hans-Jürgen Simonis
- Dong Hee Kim
- Gian Mario Bilei
- Heriberto Castilla Valdez
- Yi-ting Duh
- Niels Dupont-Sagorin
- Aashaq Shah
- Enrico Robutti
- Tanvi Wamorkar
- Nadja Strobbe
- Steven Lowette
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- Jing Wang
- D. De Jesus Damiao
- Jeremy Andrea
- Paolo Azzurri
- Maria Aldaya Martin
- Sergio Cittolin
- Maksat Haytmyradov
- Si Xie
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- Patrizia Azzi
- Jesús Marco
- Marco Cuffiani
- Arnaud Steen
- Vincent J Smith
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- Sébastien Viret
- Jiyeon Han
- Simone Gelli
- Katja Klein
- Diego Alejandro Sanz Becerra
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- David Michael Morse
- Giovanni Organtini
- Heiner Tholen
- Dave Pellett
- Justin Pilot
- Jeffrey Roskes
- Hualin Mei
- Yeonju Go
- Manfred Krammer
- Pietro Vischia
- Andre Rosowsky
- Dmitry Sosnov
- Yiwen Wen
- Armando Bermúdez Martínez
- Yi Wang
- Qiang Li
- Roberto Salerno
- Humberto Antonio Salazar Ibarguen
- Alessandra Romero
- Dmitry Hits
- Kevin Pedro
- Artur Apresyan
- Stefano Marcellini
- Vladimir Rekovic
- Otman Charaf
- Fábio Lúcio Alves
- Steven Kaplan
- Fengwangdong Zhang
- George Wei-Shu Hou
- Matthew Herndon
- Isabell-Alissandra Melzer-Pellmann
- Nathaniel Odell
- Jim Hanlon
- Vasile Mihai Ghete
- Paul Sheldon
- Jacobo Konigsberg
- Bahareh Roozbahani
- Jean Fay
- Thomas Ferbel
- Giulia Negro
- Genius Walia
- Jian Sun
- Marc Osherson
- Robert Harr
- Alessandro Degano
- Natalia Lychkovskaya
- Atanu Modak
- Abdollah Mohammadi
- Ozgun Kara
- Georg Sieber
- David Stuart
- Xavier Janssen
- Saranya Ghosh
- Jane Nachtman
- Mara Senghi Soares
- Borislav Pavlov
- Luca Pacher
- Raffaele Gerosa
- Tanmay Mudholkar
- Michael Benjamin Andrews
- Merve Nazlim Agaras
- Gervasio Gomez
- Vuko Brigljević
- Anne Dabrowski
- Francesco Fallavollita
- Livio Fano
- Antonio Ranieri
- Anton Karneyeu
- Gaël Perrin
- Ajay Kumar
- Anadi Canepa
- Marco Cipriani
- Aruna Nayak
- Giovanni Franzoni
- James Faulkner
- Soham Bhattacharya
- Andromachi Tsirou
- Ennio Monteil
- Agostino Di Francesco
- Stephen Mrenna
- Alexis Kalogeropoulos
- Andreas Mussgiller
- Manuel Alejandro Segura Delgado
- Nicola Pozzobon
- Suyong Choi
- Pietro Govoni
- Tagir Aushev
- Gurpreet Singh
- Shuichi Kunori
- Andreas Psallidas
- Rajdeep Mohan Chatterjee
- Francesco Micheli
- Stephan Lammel
- Alexander Schmidt
- Christopher Neu
- Min Suk Kim
- Mikhail Kirsanov
- Shahram Rahatlou
- Daniel Salerno
- Cameron Bravo
- John Perry Cumalat
- Loukas Gouskos
- Paolo Capiluppi
- Alessandro Di Mattia
- Suleyman Durgut
- Benjamin Stieger
- Ivan Kresimir Furic
- Anirban Saha
- Elias Pree
- Cristovao Beirao Da Cruz E Silva
- Maria Elena Pol
- David Ja Cockerill
- Lovedeep Kaur Saini
- Maria Margherita Obertino
- Panagiotis Kokkas
- Stefano Casasso
- Igor Azhgirey
- Thomas Ferguson
- Kerstin Borras
- Daniel Treille
- Felicitas Pauss
- Shashikant Dugad
- Manjit Kaur
- Christophe Royon
- Ashley Parker
- Monika Grothe
- Allison Reinsvold
- Benoit Courbon
- Kevin Sung
A search for a new scalar resonance decaying to a pair of Z bosons is performed in the mass range from 130 GeV to 3 TeV, and for various width scenarios. The analysis is based on proton-proton collisions recorded by the CMS experiment at the LHC in 2016, corresponding to an integrated luminosity of 35.9 fb^(−1) at a center-of-mass energy of 13 TeV. The Z boson pair decays are reconstructed using the 4l, 2l2q, and 2l2ν final states, where l = e or μ. Both gluon fusion and electroweak production of the scalar resonance are considered, with a free parameter describing their relative cross sections. A dedicated categorization of events, based on the kinematic properties of associated jets, and matrix element techniques are employed for an optimal signal and background separation. A description of the interference between signal and background amplitudes for a resonance of an arbitrary width is included. No significant excess of events with respect to the standard model expectation is observed and limits are set on the product of the cross section for a new scalar boson and the branching fraction for its decay to ZZ for a large range of masses and widths.
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