238 research outputs found
Quality assessment of an interferon-gamma release assay for tuberculosis infection in a resource-limited setting
- Author
- A Lalvani
- AAO Varma
- AH Peruski
- C Ricós
- CC Heuck
- D Menzies
- Do B Tam
- GW Williams
- HG Endres
- Ikumi Matsushita
- J Coloma
- JL Fleiss
- JO Westgard
- JO Westgard
- Kazue Higuchi
- Le T Hong
- Luu T Lien
- M Pai
- Naoki Ishizuka
- Naoto Keicho
- Nguyen TL Hang
- Nobuyuki Harada
- P Armitage
- PG Smith
- RJ Lock
- RW Peeling
- SC Kazmierczak
- Shinsaku Sakurada
- V Marks
- Vu TX Thu
- Publication venue
- BioMed Central
- Publication date
- 01/01/2009
- Field of study
<p>Abstract</p> <p>Background</p> <p>When a test for diagnosis of infectious diseases is introduced in a resource-limited setting, monitoring quality is a major concern. An optimized design of experiment and statistical models are required for this assessment.</p> <p>Methods</p> <p>Interferon-gamma release assay to detect tuberculosis (TB) infection from whole blood was tested in Hanoi, Viet Nam. Balanced incomplete block design (BIBD) was planned and fixed-effect models with heterogeneous error variance were used for analysis. In the first trial, the whole blood from 12 donors was incubated with nil, TB-specific antigens or mitogen. In 72 measurements, two laboratory members exchanged their roles in harvesting plasma and testing for interferon-gamma release using enzyme linked immunosorbent assay (ELISA) technique. After intervention including checkup of all steps and standard operation procedures, the second trial was implemented in a similar manner.</p> <p>Results</p> <p>The lack of precision in the first trial was clearly demonstrated. Large within-individual error was significantly affected by both harvester and ELISA operator, indicating that both of the steps had problems. After the intervention, overall within-individual error was significantly reduced (<it>P </it>< 0.0001) and error variance was no longer affected by laboratory personnel in charge, indicating that a marked improvement could be objectively observed.</p> <p>Conclusion</p> <p>BIBD and analysis of fixed-effect models with heterogeneous variance are suitable and useful for objective and individualized assessment of proficiency in a multistep diagnostic test for infectious diseases in a resource-constrained laboratory. The action plan based on our findings would be worth considering when monitoring for internal quality control is difficult on site.</p
Nasopharyngeal Pneumococcal Colonization Density Is Associated With Severe Pneumonia in Young Children in the Lao People's Democratic Republic
- Author
- Publication venue
- 'Oxford University Press (OUP)'
- Publication date
- 11/05/2021
- Field of study
BACKGROUND: No studies have explored the association between pneumococcal nasopharyngeal density and severe pneumonia using the World Health Organization (WHO) 2013 definition. In Lao People's Democratic Republic (Lao PDR), we determine the association between nasopharyngeal pneumococcal density and severe pneumonia in children. METHODS: A prospective observational study was undertaken at Mahosot Hospital, Vientiane, from 2014 to mid-2018. Children <5 years admitted with acute respiratory infections (ARIs) were included. Clinical and demographic data were collected alongside nasopharyngeal swabs for pneumococcal quantification by lytA real-time quantitative polymerase chain reaction. Severe pneumonia was defined using the 2013 WHO definition. For pneumococcal carriers, a logistic regression model examined the association between pneumococcal density and severe pneumonia, after adjusting for potential confounders including demographic and household factors, 13-valent pneumococcal conjugate vaccine status, respiratory syncytial virus co-detection, and preadmission antibiotics. RESULTS: Of 1268 participants with ARI, 32.3% (n = 410) had severe pneumonia and 36.9% (n = 468) had pneumococcal carriage. For pneumococcal carriers, pneumococcal density was positively associated with severe pneumonia (adjusted odds ratio, 1.4 [95% confidence interval, 1.1-1.8]; P = .020). CONCLUSIONS: Among children with ARIs and pneumococcal carriage, pneumococcal carriage density was positively associated with severe pneumonia in Lao PDR. Further studies may determine if pneumococcal density is a useful marker for pneumococcal conjugate vaccine impact on childhood pneumonia
Long-range angular correlations on the near and away side in p–Pb collisions at
- Author
- Abdiel Ramirez Reyes
- Adam Ryszard Kisiel
- Adam Tomasz Matyja
- Adam Wlodzimierz Jacholkowski
- Adam Szczepankiewicz
- Adela Kravcakova
- Aditya Nath Mishra
- Adrian Sevcenco
- Adriana Telesca
- Airton Deppman
- Ajay Kumar Dash
- Alberica Toia
- Alberto Baldisseri
- Alberto Collu
- Alberto Gago
- Alberto Masoni
- Alejandro Szanto de Toledo
- Alessandra Maria Mazzoni
- Alessandra Fantoni
- Alessandro De Falco
- Alessandro Feliciello
- Alessandro Grelli
- Alessandro Pesci
- Alexander Philipp Kalweit
- Alexander Akindinov
- Alexander Borissov
- Alexander Hansen
- Alexander Kluge
- Alexander Mamonov
- Alexander Nedosekin
- Alexander Ochirov
- Alexander Vinogradov
- Alexander Vodopianov
- Alexander Wilk
- Alexandr Tumkin
- Alexandre Alarcon do Passo Suaide
- Alexandre Nyanin
- Alexandre Rachevski
- Alexandre Shabetai
- Alexandru Florin Dobrin
- Alexandru Bercuci
- Alexei Kaidalov
- Alexei Khanzadeev
- Alexei Pavlinov
- Alexey Bogdanov
- Alexey Kuryakin
- Alexey Vyushin
- Alexis Jean Michel Mas
- Alfonso Tarazona Martinez
- Alfredo Musso
- Alice Zimmermann
- Alina Gabriela Grigoras
- Alis Rodriguez Manso
- Alla Maevskaya
- Alphonse Rademakers
- Amalia Pop
- Amaya Ofelia Casanova Diaz
- Ana Maria Marin
- Anais Annick Erica Bergognon
- Anand Kumar Dubey
- Anatoly Kolojvari
- Anders Garritt Knospe
- Anders Nils Erik Oskarsson
- Andras Gabor Agocs
- Andre Augustinus
- Andre Mischke
- Andrea Agostinelli
- Andrea Alici
- Andrea Dainese
- Andrea Danu
- Andrea Dubla
- Andrea Festanti
- Andrea Francescon
- Andrea Rossi
- Andreas Arend
- Andreas Morsch
- Andrei Geae Gheata
- Andrei Ionut Herghelegiu
- Andres Sandoval
- Andrew Marshall Adare
- Andrey Ivanov
- Andrey Kazantsev
- Andrey Reshetin
- Andrey Vasiliev
- Andrey Zarochentsev
- Andry Malala Rakotozafindrabe
- Andrzej Deloff
- Andrzej Rybicki
- Andzhey Asryan
- Angela Badala
- Anik Gupta
- Anitha Nyatha
- Anju Bhasin
- Ankita Goswami
- Anna Rita Reolon
- Annalisa De Caro
- Annalisa Mastroserio
- Annika Passfeld
- Anselmo Margotti
- Ante Bilandzic
- Anthony Timmins
- Antoine Xavier Lardeux
- Anton Alkin
- Anton Andronic
- Anton Jusko
- Antonin Maire
- Antonino Zichichi
- Antonio Carlos Oliveira Da Silva
- Antonio Di Mauro
- Antonio Juan Rubio Montero
- Antonio Ortiz Velasquez
- Antonio Uras
- Ara Grigoryan
- Armando Palmeri
- Arnaldi Roberta
- Arnulfo Martinez Davalos
- Arsen Hayrapetyan
- Arshad Ahmad
- Artem Konevskih
- Artur Krzysztof Szostak
- Arturo Alejandro Menchaca Rocha
- Arturo Fernandez Tellez
- Arturo Tauro
- Arvinder Singh Palaha
- Ashok Kumar Bhati
- Astrid Morreale
- Attilio Tarantola Peloni
- Attiq Ur Rehman
- Aurora Diozcora Vargas
- Austin Harton
- Ayben Karasu Uysal
- Baba Potukuchi
- Bae Svane Nielsen
- Barbara Erazmus
- Barbara Guerzoni
- Barthelemy von Haller
- Basanta Kumar Nandi
- Bastian Bathen
- Bedangadas Mohanty
- Benjamin Andreas Hess
- Benjamin Donigus
- Beole&apos
- Beomkyu Kim
- Beomsu Chang
- Bernard Hicks
- Bernd Stefan Windelband
- Bernhard Skaali
- Berzano Dario Carlo Domenico
- Betty Abelev
- Bianchi Livio
- Bikash Sinha
- Biswarup Paul
- Bjarte Kileng
- Bjorn Steven Nilsen
- Blahoslav Pastircak
- Blanco F.
- Bo Fenton Olsen
- Bogdan Theodor Rascanu
- Bogdan Vulpescu
- Boris Batyunya
- Boris Grinyov
- Boris Hippolyte
- Boris Polichtchouk
- Boris Wagner
- Bossu&apos
- Botta Elena
- Branislav Sitar
- Brigitte Cheynis
- Brijesh Kumar Srivastava
- Bruno Alessandro
- Bruno Espagnon
- Bruno Ghidini
- Bufalino Stefania
- Byounghee Han
- Cai Xu
- Camilo Ernesto Lara
- Carlos Albert Salgado
- Carlos Eugenio Perez Lara
- Carlos Pajares
- Carmelo Di Giglio
- Carsten Sogaard
- Casper Nygaard
- Catherine Silvestre
- Catia Petta
- Cenek Zach
- Cesar Ceballos Sanchez
- Chiara Zampolli
- Christelle Sophie Roy
- Christian Claude Kuhn
- Christian Holm Christensen
- Christian Joachim Schmidt
- Christian Klein Bosing
- Christian Lippmann
- Christina Markert
- Christine Nattrass
- Christoph Heinrich Baumann
- Christoph Blume
- Christoph Mayer
- Christophe Pierre Suire
- Christophe Furget
- Christopher Daniel Anson
- Cinzia Luzzi
- Ciprian Mihai Mitu
- Claude Andre Pruneau
- Claudio Geuna
- Claudiu Cornel Schiaua
- Constantinos Loizides
- Corrado Cicalo
- Corrales Morales Yasser
- Costanza Cavicchioli
- Costin Grigoras
- Crispin Williams
- Cristian Geae Ivan
- Cristian Andrei
- Cristina Terrevoli
- Csaba Soos
- Cvetan Cheshkov
- Cynthia Marie Hadjidakis
- Dae Sung Hwang
- Dagmar Adamova
- Daicui Zhou
- Daniel Jesus Tapia Takaki
- Daniel Berenyi
- Daniel Felea
- Daniel Lohner
- Daniela Fabris
- Daniele De Gruttola
- Danilo Vranic
- Danthasinghe Piyarathna
- Dariusz Miskowiec
- David Christopher Truesdale
- David Olle Rickard Silvermyr
- David Philip Emschermann
- David Chinellato
- David Evans
- David Rohr
- David Tlusty
- Davide Caffarri
- Davide Falchieri
- Davide Perrino
- Debasish Das
- Deepa Thomas
- Deepika Rathee
- Deeptanshu Manu Jha
- Denise Aparecida Moreira De Godoy
- Despoina Hatzifotiadou
- Dhevan Raja Gangadharan
- Diego Caballero Orduna
- Diego Perini
- Diego Stocco
- Dieter Rohrich
- Dilan Minthaka Madagodahettige Don
- Dmitri Ivanovich Patalakha
- Dmitri Peresunko
- Dmitry Aleksandrov
- Dmitry Blau
- Dmitry Budnikov
- Dmitry Finogeev
- Dmitry Malʼ
- Do Won Kim
- Domenico Di Bari
- Domenico Colella
- Domenico Elia
- Dominik Fehlker
- Dong Jo Kim
- Dong Wang
- Dosatsu Sakata
- Durga Prasad Mahapatra
- Dutta Majumdar A. K.
- Edith Zinhle Buthelezi
- Edmundo Garcia Solis
- Eleazar Cuautle
- Elena Gonzalez Ferreiro
- Elena Bruna
- Elienos Pereira De Oliveira Filho
- Elisa Incani
- Elisabetta Crescio
- Emanuele Quercigh
- Emilia Cruz Alaniz
- Emmanuel Floratos
- Enrichetta Maria Fiore
- Enrico Fragiacomo
- Erick Jonathan Almaraz Avina
- Ermes Braidot
- Ernesto Belmont Moreno
- Ernesto Calvo Villar
- Ernesto Lopez Torres
- Ervin Denes
- Ester Anna Rita Casula
- Esther Montes
- Eugen Mudnic
- Eugenio Nappi
- Eugenio Scapparone
- Eulogio Serradilla
- Eva Sicking
- Evert Anders Stenlund
- Evgeny Karpechev
- Evgeny Kryshen
- Evgeny Ryabinkin
- Ewa Gladysz Dziadus
- Fabio Colamaria
- Fabrizio Coccetti
- Fatima Padilla
- Federico Antinori
- Federico Carminati
- Federico Cindolo
- Federico Ronchetti
- Fedor Guber
- Felix Vincenz Rettig
- Fengchu Zhou
- Fernando Baltasar Dos Santos Pedrosa
- Fernando Scarlassara
- Ferretti Alessandro
- Filip Krizek
- Filippo Costa
- Fiorella Fionda
- Florian Painke
- Francesca Bellini
- Francesca Soramel
- Francesco Barile
- Francesco Blanco
- Francesco Carena
- Francesco Noferini
- Francesco Prino
- Francesco Riggi
- Franck Manso
- Franco Meddi
- Frederick Kramer
- Gabriel de Barros
- Gagliardi Martino
- Galina Shabratova
- Gallio Mauro
- Gennady Zinovjev
- Gerardo Antonio Herrera Corral
- Gerardus Nooren
- Gergely Gabor Barnafoldi
- Gergoe Hamar
- Giacinto de Cataldo
- Giacomo Vito Margagliotti
- Giacomo Contin
- Giacomo Volpe
- Gianfranco Segato
- Gianluca Aglieri Rinella
- Gianluca Santagati
- Gianluca Usai
- Gideon Francois Steyn
- Gilda Scioli
- Gines Martinez Garcia
- Ginevra Dʼ
- Giovanna Puddu
- Giovanni Cara Romeo
- Giuseppe Eugenio Bruno
- Giuseppe Pappalardo
- Giuseppe Simonetti
- Giuseppe Viesti
- Goran Simatovic
- Graham Richard Lee
- Grazia Luparello
- Greeshma Koyithatta Meethaleveedu
- Grigory Feofilov
- Grzegorz Andrzej Wilk
- Grzegorz Stefanek
- Guido Marie Urciuoli
- Guillaume Batigne
- Guillermo Tejeda Munoz
- Gunnar Lovhoiden
- Gustavo Conesa Balbastre
- Guy Paic
- Gyula Bencedi
- Gyulnara Eyyubova
- Haavard Helstrup
- Haeng Jin Jang
- Haitao Zhang
- Hanna Paulina Zbroszczyk
- Hans Hjersing Dalsgaard
- Hans Martin Ljunggren
- Hans Rudolf Schmidt
- Hans Beck
- Hans Boggild
- Hans Muller
- Harald Appelshauser
- Hege Austrheim Erdal
- Heiko Engel
- Helen Louise Caines
- Helmut Oskar Oeschler
- Henner Buesching
- Henning Kvaerno
- Henrik Qvigstad
- Hermes Leon Vargas
- Hermes Leon
- Herve Borel
- Hideki Hamagaki
- Hiroaki Sakaguchi
- Hisayuki Torii
- Hongsheng Zhu
- Hongyan Yang
- Hrant Gulkanyan
- Hugo Denis Antonio Pereira Da Costa
- Hugues Delagrange
- Hyung Taik Jung
- Hyungsuk Son
- Ian Gardner Bearden
- Igor Altsybeev
- Igor Kulakov
- Igor Lakomov
- Igor Pshenichnov
- Igor Yushmanov
- Ildefonso Leon Monzon
- Ilya Selyuzhenkov
- Imrich Szarka
- In Kwon Yoo
- Indranil Das
- Innocenti Gian Michele
- Ionel Stan
- Ionela Berceanu
- Ionut Cristian Arsene
- Iosif Legrand
- Iouri Belikov
- Irakli Garishvili
- Irakli Martashvili
- Iryna Ilkiv
- Isha Chawla
- Ismael Cortes Maldonado
- Ivan Kisel
- Ivan Kralik
- Ivan Vorobyev
- Ivana Hrivnacova
- Ivonne Alicia Maldonado Cervantes
- Iwona Sputowska
- Jacek Tomasz Otwinowski
- Jae Mercado Perez
- Jaen Lien
- Jai Salzwedel
- Jan de Cuveland
- Jan Fiete Grosse Oetringhaus
- Jan Marian Pluta
- Jan Cepila
- Jan Figiel
- Jan Musinsky
- Jan Rak
- Jana Bielcikova
- Janka Vrlakova
- Janusz Oleniacz
- Jaroslav Adam
- Jaroslav Ban
- Jaroslav Bielcik
- Jason Glyndwr Ulery
- Javier Ernesto Castillo Castellanos
- Jean Luc Fernand Charvet
- Jean Pierre Revol
- Jean Sebastien Real
- Jean Willy Andre Cleymans
- Jean Yves Grossiord
- Jeewon Seo
- Jennifer Lynn Klay
- Jens Joergen Gaardhoje
- Jens Wiechula
- Jerzy Gustaw Bartke
- Jesus Guillermo Contreras
- Jianhui Zhu
- Jianlin Zhu
- Jiebin Luo
- Jihye Song
- Jihyun Bhom
- Jin Sook Kim
- Jiri Kral
- Jiri Mares
- Jitendra Kumar
- Joakim Ingemar Nystrand
- Jocelyn Mlynarz
- Jochen Mathias Thader
- Jochen Gerhard
- Jochen Klein
- Jochen Ulrich
- Joel Mazer
- Joerg Walter Lehnert
- Jogender Saini
- Johan Alme
- Johanna Stachel
- Johannes Hendrik Stiller
- Johannes Wessels
- John William Harris
- Jon Wikne
- Jonas Anielski
- Jonghyun Kim
- Jongik Yoon
- Jorn Henning Putschke
- Jose Garabatos
- Jovan Milosevic
- Jozef Urban
- Ju Hwan Kang
- Juan Francisco Castillo Hernandez
- Juha Heikki Aysto
- Juho Jaako Sarkamo
- Julian Book
- Julien Faivre
- Jun Takahashi
- JunGyu Yi
- Jurgen Schukraft
- Jussi Viinikainen
- Kai Krister Loo
- Kai Oliver Schweda
- Kamal Hussain Khan
- Karel Polak
- Karel Safarik
- Ke Ma
- Ken Oyama
- Kengo Watanabe
- Kenneth Francis Read
- Kenta Shigaki
- Ketil Roed
- Ki Sang Lee
- Kilian Eberhard Schwarz
- Kirill Voloshin
- Kjetil Ullaland
- Klaus Johannes Reygers
- Kristin Fanebust Hetland
- Kristjan Herlache Gulbrandsen
- Krzysztof Redlich
- Kurepin A.
- Kurepin A. B.
- Kushal Das
- Kyoichiro Ozawa
- Kyrre Skjerdal
- Ladislav Sandor
- Lalit Kumar Mangotra
- Laszlo Boldizsar
- Latchezar Betev
- Laura Helena Gonzalez Trueba
- Laure Marie Massacrier
- Laurent Bernard Aphecetche
- Laurent Ducroux
- Lawrence Pinsky
- Lee Stuart Barnby
- Leonid Vinogradov
- Leonidas Xaplanteris Karampatsos
- Leticia Cunqueiro
- Levente Molnar
- Linda Vickovic
- Linus Feldkamp
- Lizardo Valencia Palomo
- Lodovico Riccati
- Loic Henri Antoine Manceau
- Luca Toscano
- Luciano Musa
- Ludmila Malinina
- Luigi Vannucci
- Luis Manuel Montano Zetina
- Luisa Cifarelli
- Lukasz Kamil Graczykowski
- Luke David Hanratty
- Maciej Szymanski
- Madan Aggarwal
- Mads Stormo Nilsson
- Magali Danielle Estienne
- Magnus Mager
- Maitreyee Mukherjee
- Maksym Zyzak
- Malgorzata Anna Janik
- Manuel Enrique Cotallo
- Marcel Figueredo
- Marcello Lunardon
- Marcelo Munhoz
- Marchisone Massimiliano
- Marco van Leeuwen
- Marco Boccioli
- Marco Bregant
- Marco Marquard
- Marco Monteno
- Marek Bombara
- Marek Chojnacki
- Marek Kowalski
- Maria Haiduc
- Maria Nicassio
- Maria Vasileiou
- Marian Ivanov
- Marian Krivda
- Marian Putis
- Mariana Petris
- Marie Germain
- Mario Fusco Girard
- Mario Ivan Martinez
- Mario Rodriguez Cahuantzi
- Markus Ansgar Heide
- Markus Fasel
- Markus Kohler
- Marta Verweij
- Martha Spyropoulou Stassinaki
- Martijn Reicher
- Martin Alfonso Subieta Vasquez
- Martin Robert Girard
- Martin Rudolf Wilde
- Martin Poghosyan
- Martin Vala
- Masato Sano
- Masera Massimo
- Massimo Venaruzzo
- Mateusz Andrzej Ploskon
- Mateusz Lechman
- Matthew Steinpreis
- Matthias Jakob Bach
- Matthias Rudolph Richter
- Matthias Hartig
- Matthias Kretz
- Matthieu Laurent Lenhardt
- Maurizio Basile
- Maurizio Morando
- Mauro Rogerio Cosentino
- Maxime Rene Joseph Guilbaud
- Megan Elizabeth Connors
- Meidana Huang
- Mengliang Wang
- Mesut Arslandok
- Michael Annan Lisa
- Michael Gerard Cherney
- Michael Linus Knichel
- Michael Kliemant
- Michael Weber
- Michal Broz
- Michal Krelina
- Michal Meres
- Michal Petran
- Michal Sumbera
- Michal Vajzer
- Michelangelo Agnello
- Michele Floris
- Michiel Botje
- Miguel Angel Diaz Corchero
- Mihaela Gheata
- Mihai Niculescu
- Mihai Petrovici
- Mikhail Bogolyubsky
- Mikhail Ippolitov
- Mikhail Kompaniets
- Mikhail Malaev
- Mikhail Stolpovskiy
- Mikhail Zhalov
- Mikolaj Krzewicki
- Milano Leonardo
- Milos Pachr
- Mimae Kim
- Min Jung Kweon
- Minwoo Kim
- Mirko Planinic
- Miroslav Krus
- Miroslav Pikna
- Misha Veldhoen
- Mohd Danish Azmi
- Mohisin Mohammed Khan
- Motoi Inaba
- Muhammad Ajaz
- Muhammad Irfan
- Mykhaylo Zynovyev
- Myunggeun Song
- Natalia Kondratyeva
- Natasha Sharma
- Nazeer Ahmad
- Nelson Carlin Filho
- Nestor Armesto
- Nevio Grion
- Nicola Bianchi
- Nicolas Arbor
- Nicole Alice Martin
- Nicole Bastid
- Nikolai Smirnov
- Nikolai Zaviyalov
- Nirbhay Kumar Behera
- Nora De Marco
- Nora Pitz
- Norbert Herrmann
- Norbert Novitzky
- Oeystein Djuvsland
- Oleg Karavichev
- Oleksii Ivanytskyi
- Olga Driga
- Oliver Busch
- Olja Dordic
- Ombretta Pinazza
- Oppedisano Chiara
- Orlando Villalobos Baillie
- Oystein Senneset Haaland
- Palash Khan
- Panagiota Foka
- Panagiotis Christakoglou
- Paola La Rocca
- Paola Gianotti
- Paola Pagano
- Paolo Camerini
- Paolo Giubellino
- Paolo Martinengo
- Paraskevi Ganoti
- Pascal Dupieux
- Pasquale Di Nezza
- Patrick Aaron Scott
- Patrick Reichelt
- Paul Kuijer
- Pedro Gonzalez Zamora
- Pedro Ladron de Guevara
- Pedro Luis Manuel Podesta Lerma
- Per Ivar Loenne
- Peter Braun Munzinger
- Peter Graham Jones
- Peter Zahariev Hristov
- Peter Chochula
- Peter Christiansen
- Peter Glassel
- Peter Jacobs
- Peter Kalinak
- Peter Levai
- Peter Malzacher
- Peter Strmen
- Petr Nomokonov
- Petr Zavada
- Petra Riedler
- Philipp Luettig
- Philippe Crochet
- Philippe Gros
- Philippe Pillot
- Philippe Rosnet
- Pier Giaio Innocenti
- Piergiaio Cerello
- Pierre Vande Vyvre
- Pierre Zelnicek
- Pietro Antonioli
- Pietro Cortese
- Piotr Krystian Ostrowski
- Plamen Rumenov Petrov
- Podist Kurashvili
- Pradip Kumar Roy
- Pradip Kumar Sahu
- Predrag Buncic
- Premomoy Ghosh
- Rachid Guernane
- Radek Smakal
- Radiy Ilkaev
- Raffaele Grosso
- Raghava Varma
- Raghunath Sahoo
- Raimond Snellings
- Rainer Arno Ernst Renfordt
- Rainer Martin Schicker
- Ralf Peter Averbeck
- Ralf Keidel
- Rama Chandra Baral
- Rama Narayana Singaraju
- Ramello Luciano
- Ramni Gupta
- Ramon Gomez
- Ramona Lea
- Ranbir Singh
- Raoul Stefan de Rooij
- Raphael Noel Tieulent
- Raphaelle Marie Bailhache
- Raphaelle Ichou
- Rashmi Raniwala
- Raul Tonatiuh Jimenez Bustamante
- Rebecca Scott
- Renato Angelo Ricci
- Renaud Vernet
- Rene Bellwied
- Rene Brun
- Renu Bala
- Renzhuo Wan
- Rigoberto Cruz Albino
- Rinaldo Baldini Ferroli
- Rinaldo Rui
- Rishat Sultanov
- Robert Grajcarek
- Roberto Barbera
- Roberto Divia
- Roberto Preghenella
- Roger Worsley Fearick
- Rohini Sharma
- Rolf Paul Scharenberg
- Roman Lietava
- Romualdo Santoro
- Ron Ariel Soltz
- Rongrong Ma
- Rosa Romita
- Rosario Nania
- Rosario Turrisi
- Rosi Jan Reed
- Ruben Shahoyan
- Rudiger Haake
- Rudolf Janik
- Rune Langoy
- Russo Riccardo
- Sabyasachi Siddhanta
- Sadhana Dash
- Saehanseul Oh
- Salvatore De Pasquale
- Sami Sakari Rasanen
- Sandra Moretto
- Sandro Bjelogrlic
- Sandun Jayarathna
- Sang Un Ahn
- Sanjeev Singh Sambyal
- Sanjib Muhuri
- Sanshiro Mizuno
- Sara Vallero
- Sarah Louise La Pointe
- Sarah Porteboeuf Houssais
- Satish Sharma
- Satyajit Jena
- Scomparin Enrico
- Se Yong Kim
- Sean Murray
- Sebastian Kalcher
- Sedat Altinpinar
- Serge Kox
- Sergey Filchagin
- Sergey Fokin
- Sergey Gorbunov
- Sergey Kiselev
- Sergey Nazarenko
- Sergey Nikolaev
- Sergey Nikulin
- Sergey Sadovsky
- Sergey Voloshin
- Sergey Zaporozhets
- Sergio Di Liberto
- Sergio Serci
- Sergio Vergara
- Serhiy Senyukov
- Shiming Yang
- Shingo Sakai
- Shinichi Esumi
- Shinichi Hayashi
- Shtejer Diaz Katherin
- Shuaib Ahmad Khan
- Shuang Li
- Sidharth Kumar Prasad
- Siegfried Valentin Foertsch
- Silvia Arcelli
- Silvia Masciocchi
- Simone Schuchmann
- Sitta Mario
- Smbat Grigoryan
- Sona Pochybova
- Sorin Ion Zgura
- Stanislav Yasnopolsky
- Stefan Thomas Heckel
- Stefan Boettger
- Stefan Kirsch
- Stefan Rossegger
- Stefano Piano
- Subhash Singha
- Subhasis Chattopadhyay
- Subikash Choudhury
- Sudhir Raniwala
- Sudipan De
- Suh Urk Chung
- Sukalyan Chattopadhyay
- Sul Ah Ahn
- Sumit Basu
- Sun Kun Oh
- Sung Chul Lee
- Supriya Das
- Susanta Kumar Pal
- Svein Lindal
- Sven Gotovac
- Svetlana Kushpil
- Sylvain Chapeland
- Tadeusz Antoni Dobrowolski
- Taebong Moon
- Taesoo Kim
- Takafumi Niida
- Taku Gunji
- Tapan Kumar Nayak
- Tatiana Karavicheva
- Tatjana Susa
- Tatsuya Chujo
- Teodor Siemiarczuk
- Terry Awes
- Thanushan Kugathasan
- Theo Alexander Broker
- Thomas Michael Cormier
- Thomas Dietel
- Thomas Humanic
- Thomas Peitzmann
- Thorsten Kollegger
- Tim Schuster
- Timo Gunther Breitner
- Timothy Symons
- Timur Pocheptsov
- Tinku Sinha
- Tiziano Virgili
- Tobias Krawutschke
- Tomas Robert Aronsson
- Tomasz Jan Pawlak
- Tome Anticic
- Tomi Samuli Raiha
- Tomoya Tsuji
- Torsten Alt
- Toru Sugitate
- Trine Spedstad Tveter
- Tuomo Esa Aukusti Kalliokoski
- Tuva Richert
- Tyler Allen Browning
- Udo Wolfgang Kebschull
- Ulrich Michael Frankenfeld
- Ulrich Fuchs
- Uwe Westerhoff
- Valentina Zaccolo
- Valeria Muccifora
- Valerie Barret
- Valerio Altini
- Valery Kondratiev
- Valery Punin
- Vardanush Papikyan
- Vasco Miguel Chibante Barroso
- Vasile Catanescu
- Vasily Kushpil
- Vedran Nikolic
- Venelin Anguelov
- Vera Loggins
- Vercellin Ermanno
- Veronica Canoa Roman
- Victor Trubnikov
- Vikas Singhal
- Vincenzo Paticchio
- Vitaly Loginov
- Vito Lenti
- Vito Manzari
- Vladimir Ivanov
- Vladimir Kaplin
- Vladimir Kovalenko
- Vladimir Nikulin
- Vladimir Peskov
- Vladimir Pospisil
- Vladimir Samsonov
- Vladimir Vechernin
- Vladimir Wagner
- Vladislav Grigoriev
- Vladislav Manko
- Vojtech Petracek
- Volker Lindenstruth
- Weilin Yu
- Werner Riegler
- Wiktor Stanislaw Peryt
- Wisla Carena
- Wladyslaw Henryk Trzaska
- Woo Jin Park
- Xavier Bernard Lopez
- Xianbao Yuan
- Xiangrong Zhu
- Xianguo Lu
- Xiaoming Zhang
- Xitzel Sanchez Castro
- Yaldo Chris G.
- Yannick Denis Zoccarato
- Yaping Wang
- Yaroslav Berdnikov
- Yasuo Miake
- Yasuto Hori
- Yaxian Mao
- Yevgen Martynov
- Yifei Wang
- Yogendra Viyogi
- Yong Wook Baek
- Yorito Yamaguchi
- You Zhou
- Youngil Kwon
- Yury Kharlov
- Yury Kucheriaev
- Yury Pestov
- Yury Sibiriak
- Yury Vinogradov
- Yves Roland Schutz
- Yvonne Chiara Pachmayer
- Zabulon Vilakazi
- Zaida Conesa del Valle
- Zhongbao Yin
- Zubayer Ahammed
- Zuzana Harmanova
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2013
- Field of study
Combination of searches for heavy spin-1 resonances using 139 fb−1 of proton-proton collision data at s = 13 TeV with the ATLAS detector
- Author
- Aad G
- Aakvaag E
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboelela M
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Ackermann A
- Adam Bourdarios C
- Adamczyk L
- Addepalli SV
- Addison MJ
- Adelman J
- Adiguzel A
- Adye T
- Affolder AA
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- Aggarwal A
- Agheorghiesei C
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahuja S
- Ai X
- Aielli G
- Aikot A
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- Aitbenchikh B
- Aizenberg I
- Akbiyik M
- Akimov AV
- Akiyama D
- Akolkar NN
- Aktas S
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Albouy GL
- Alderweireldt S
- Alegria ZL
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Alfonsi F
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- Ali B
- Ali HMJ
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- Alimonti G
- Alkakhi W
- Allaire C
- Allbrooke BMM
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- Aloisio A
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- Alviggi MG
- Aly M
- Amaral Coutinho Y
- Ambler A
- Amelung C
- Amerl M
- Ames CG
- Amidei D
- Amirie KJ
- Amor Dos Santos SP
- Amos KR
- An S
- Ananiev V
- Anastopoulos C
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
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- Cerqueira AS
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- Chapon E
- Chargeishvili B
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- Chekulaev SV
- Chelkov GA
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- Ciocio A
- Cirotto F
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- Zhemchugov A
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 19/04/2024
- Field of study
A combination of searches for new heavy spin-1 resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons or quarks, is presented. The data sample used corresponds to 139 fb−1 of proton-proton collisions at
= 13 TeV collected during 2015–2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb,
, and tb) or third-generation leptons (τν and ττ) are included in this kind of combination for the first time. A simplified model predicting a spin-1 heavy vector-boson triplet is used. Cross-section limits are set at the 95% confidence level and are compared with predictions for the benchmark model. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The complementarity of the various analyses increases the sensitivity to new physics, and the resulting constraints are stronger than those from any individual analysis considered. The data exclude a heavy vector-boson triplet with mass below 5.8 TeV in a weakly coupled scenario, below 4.4 TeV in a strongly coupled scenario, and up to 1.5 TeV in the case of production via vector-boson fusion
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
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- Shrif EM
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- Sideras Haddad E
- Sidoti A
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- Sjölin J
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- Soldatov EY
- Soldevila U
- Solodkov AA
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- Solovyanov OV
- Solovyev V
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- Sonay A
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- Sopczak A
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- Sánchez J
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- Taffard A
- Tafirout R
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- Talyshev AA
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- Tanaka A
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- Tanaka R
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- Tao Z
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- Tarek Abouelfadl Mohamed A
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- Trischuk DA
- Trocmé B
- Troncon C
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- Tskhadadze EG
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- Tsukerman II
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- Vasquez GA
- Vasyukov A
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- Veatch J
- Vecchio V
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- Vergis C
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- Vermeulen JC
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- Vgenopoulos A
- Viaux Maira N
- Vickey Boeriu OE
- Vickey T
- Viehhauser GHA
- Vigani L
- Villa M
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- Villhauer EM
- Vilucchi E
- Vincter MG
- Virdee GS
- Vishwakarma A
- Visibile A
- Vittori C
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- Vladimirov V
- Voevodina E
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- Weingarten J
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- Wiedenmann W
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- Wiglesworth C
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- Wilkens HG
- Williams DM
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- Willocq S
- Wilson BJ
- Windischhofer PJ
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- Winter BT
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- Wobisch M
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- Worm SD
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- Wu SL
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- Xu D
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- Xu R
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- Xu Z
- Yabsley B
- Yacoob S
- Yamaguchi Y
- Yamashita E
- Yamauchi H
- Yamazaki T
- Yamazaki Y
- Yan J
- Yan S
- Yan Z
- Yang HJ
- Yang HT
- Yang S
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- Yang X
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- Yang Y
- Yang Y
- Yang Z
- Yao W-M
- Yap YC
- Ye H
- Ye H
- Ye J
- Ye S
- Ye X
- Yeh Y
- Yeletskikh I
- Yeo BK
- Yexley MR
- Yin P
- Yorita K
- Younas S
- Young C
- Young CJS
- Yu C
- Yu Y
- Yuan M
- Yuan R
- Yue L
- Zaazoua M
- Zabinski B
- Zaid E
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zamora Saa JA
- Zang J
- Zanzi D
- Zaplatilek O
- Zeitnitz C
- Zeng H
- Zeng JC
- Zenger DT
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhai M
- Zhang B
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- Zhang K
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- Zhang R
- Zhang S
- Zhang T
- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
- Zhou Y
- Zhu CG
- Zhu J
- Zhu Y
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- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 01/04/2024
- Field of study
This paper presents the measurement of fducial and diferential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets (W±W±jj) using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of √s = 13 TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity diference. The measured fducial cross sections for electroweak and inclusive W±W±jj production are 2.92 ± 0.22 (stat.) ± 0.19 (syst.)fb and 3.38±0.22 (stat.)±0.19 (syst.)fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95% confdence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons H±± that are produced in vector-boson fusion processes and decay into a same-sign W boson pair is performed. The largest deviation from the Standard Model occurs for an H±± mass near 450 GeV, with a global signifcance of 2.5 standard deviations
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- Abadie WM
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- Kowalski ML
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- Krause HF
- Kreindler JL
- Kreindler JL
- Krings JG
- Kristin J
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- Lai X
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- Larivée N
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- Lazar RH
- Le Bon SD
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- Lechien JR
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- Lee S
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- Lennard CM
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- Liu CM
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- Lowery AS
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- Mariano ER
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- Marshall AH
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- Masterson L
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- Maxfield AZ
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- McMains KC
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- Melen I
- Melroy C
- Meltzer EO
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- Meltzer EO
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- Melvin TA
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- Messerklinger W
- Metson R
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- Mfuna EL
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- Middleton PG
- Miglani A
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- Mortazavi N
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- Mostafa BE
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- Mozzanica F
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- Nagarkar DR
- Nagata Y
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- Namyslowski G
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- Ngoc Ha T
- Nguyen BK
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- Nicolai P
- Nimsakul S
- Nino G
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- Nisa L
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- Nocera AL
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- Nomura K
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- Nyenhuis SM
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- Oakley GM
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- Ocampo CJ
- Odat H
- Ogasawara N
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- Ooi EH
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- Orb Q
- Ordovas‐Montanes J
- Ordovas‐Montanes J
- Organization WH
- Orlandi R
- Orlandi RR
- Orlandi RR
- Orlandi RR
- Orlandi RR
- Orlandi RR
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- Orlandi RR
- Orlandi RR
- Ostovar A
- Ou J
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- Ozdek A
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- Ozturan A
- Ozturk F
- Paderno A
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- Pang YT
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- Papagiannopoulos P
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- Paramasivan S
- Parasher AK
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- Parikh A
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- Parikh SL
- Parikh SR
- Paris G.
- Park D‐Y
- Park M
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- Park SK
- Park SK
- Park SM
- Parma V
- Parsek MR
- Pasaje CF
- Pasaje CF
- Pasaje CF
- Passali D
- Passali D
- Passali D
- Passàli D
- Passàli D
- Passàli D
- Patel NA
- Patel NN
- Patel VS
- Patel ZM
- Patel ZM
- Patou J
- Patro SK
- Pauli C
- Pavlin JD
- Payne SC
- Payne SJ
- Pearlman AN
- Pearlman AN
- Peng Y
- Peng Y
- Penttila M
- Perez‐Novo CA
- Peric A
- Peric A
- Perica A
- Perić A
- Perkasa MF
- Perloff JR
- Persson EK
- Peters AT
- Peña MT
- Pfaar O
- Pfaar O
- Pfaar O
- Pham V
- Phillips KM
- Phillips KM
- Phillips KM
- Phillips KM
- Phillips KM
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- Philpott C
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- Picado C
- Piccirillo JF
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- Pimenta F
- Pincus RL
- Pinther S
- Pinto Bezerra Soter AC
- Pinto JM
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- Pipolo C
- Plebani A
- Plonk DP
- Poachanukoon O
- Poetker DM
- Poetker DM
- Poetker DM
- Poetker DM
- Poletti SC
- Ponikau JU
- Ponikau JU
- Ponikau JU
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- Porter PC
- Pothoven KL
- Prajapati DP
- Prickett KK
- Prince AA
- Principi N
- Promsopa C
- Psaltis AJ
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- Pumhirun P
- Pundir V
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- Purcell PL
- Purkey MT
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- Pynnonen M
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- Qualliotine JR
- Quintanilla‐Dieck L
- Quinti I
- Qvarnberg Y
- Rabago D
- Rabago D
- Rabbe R
- Rachelefsky GS
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- Ragab A
- Ragab A
- Ragab S
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- Raghunandhan S
- Rahbar R
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- Rains BM
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- Raithatha R
- Rajan JP
- Rajiv S
- Ramadan HH
- Ramadan HH
- Ramadan HH
- Ramadan HH.
- Ramadan HH.
- Ramakrishnan V
- Ramakrishnan VR
- Ramakrishnan VR
- Ramakrishnan VR
- Ramakrishnan VR
- Ramakrishnan VR
- Ramakrishnan VR
- Ramakrishnan VR
- Ramanathan M
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- Rantala A
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- Rawal RB
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- Rawlings BA
- Reardon E.
- Reddel HK
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- Regev E
- Reg‐entSM MIPS 2018 Reporting ‐ Quality Measures
- Reh DD
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- Revai K
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- Ricciardolo FLM
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- Rosen PL
- Rosenfeld RM
- Rosenfeld RM
- Rosenfeld RM
- Rostkowska‐Nadolska B
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- Rostkowska‐Nadolska BLM
- Rotenberg BW
- Roth M
- Rowan NR
- Rowan NR
- Rowan NR
- Rowe SM
- Rowe‐Jones JM
- Roxbury CR
- Rozsasi A
- Rudack C
- Rudmik L
- Rudmik L
- Rudmik L
- Rudmik L
- Rudmik L
- Rudmik L
- Rudmik L
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- Saidi IS
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- Salama ER
- Salama N
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- Sawhney S
- Sawicki GS
- Saylam G
- Scadding GK
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- Scangas GA
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- Scarpignato C
- Schaper C
- Scheinberg PA
- Schenkel E
- Schenkel EJ
- Scheuller MC
- Schiappoli M
- Schicht M
- Schlosser RJ
- Schlosser RJ
- Schlosser RJ
- Schlosser RJ
- Schlosser RJ
- Schlosser RJ
- Schmidt F
- Schneider S
- Schreiber CP
- Schubert MS
- Schwartz HJ
- Schwartz JS
- Schwarzbach HL
- Schwitzguébel AJ‐P
- Scott JR
- Scott JR
- Sedaghat AR
- Sedaghat AR
- Sedaghat AR
- Seiberling K
- Seiberling KA
- Seiberling KA
- Seiberling KA
- Sejima T
- Sella GCP
- Sener M
- Senior BA
- Senior BA
- Senturk M
- Seppanen M
- Seresirikachorn K
- Servat JJ
- Seshadri S
- Sethi DS
- Sethi N
- Sethi RKV
- Sethi S
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- Settipane RA
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- Shah GB
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- Shaikh N
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- Shanbhag S
- Shapiro AJ
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- Sharif‐Askari FS
- Sharma P
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- Sharp HJ
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- Shen J
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- Shin HW KD
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- Shinkwin CA
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- Siedek V
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- Siegel GJ
- Sieskiewicz A
- Sikand A
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- Silva MP
- Silveira MLC
- Silverman RA
- Sindwani R
- Singhal D
- Singla G
- Sintobin I
- Sirikci A
- Sitarek P
- Siu J
- Sivaci R
- Sjogren PP
- Slavin RG
- Sleigh MA
- Sleigh MA
- Small CB
- Smith A
- Smith KA
- Smith KA
- Smith KA
- Smith KA
- Smith KA
- Smith KA
- Smith SS
- Smith SS
- Smith T
- Smith TL
- Smith TL
- Smith TL
- Smith TL
- Smith TL
- Smith TL
- Smith TL
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snidvongs K
- Snow DG
- Snyderman CH
- Sohn HG
- Sohn JH
- Soler ZM
- Soler ZM
- Soler ZM
- Soler ZM
- Soler ZM
- Soler ZM
- Soler ZM
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- Song W
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- Southwood JE
- Sowerby LJ
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- Steinke JW
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- Stelter K
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- Stentzel S
- Stern‐Shavit S
- Stevens PR
- Stevens WW
- Stevens WW
- Stevens WW
- Stevens WW
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- Stevens WW
- Stevenson DD
- Stevenson DD
- Stewart RA
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- Stokken J
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- Stolovitzky JP
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- Strauss G
- Stringer SP
- Stryjewska‐Makuch G
- Su MC
- Subramanian HN
- Succar EF
- Sugimoto I
- Sugino T
- Suh JD
- Sullivan PW
- Sultan B
- Sunadome H
- Sundaresan AS
- Sunkaraneni VS
- Suzuki S
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- Sylvester DC
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- Szczeklik A
- Szczygielski K
- Tabaee A
- Tabaee A
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- Tabrizi R
- Taccariello M
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- Tahkokallio O
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- Takabayashi T
- Takabayashi T
- Takabayashi T
- Takahashi T
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- Tammemagi CM
- Tan BK
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- Tan KS
- Tan KS
- Tan NC
- Tan NC
- Tan NC
- Tanaka S
- Tang C
- Tanner SB
- Tarrant BJ
- Tas M
- Taschieri S
- Taulu R
- Taulu R
- Tay TR
- Taylor MJ
- Telmesani LM
- Tesche S
- Teufelberger AR
- Tewfik MA
- Thacker NM
- Thamboo A
- Thamboo A
- Thamboo A
- Tharakan A
- Theodoraki MN
- Thilsing T
- Thomas AJ
- Thomas JK
- Thomas M
- Thomas WW
- Thulasidas P
- Tieu DD
- Tipirneni KE
- Tipirneni KE
- Tipirneni KE
- Tirelli G
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- Tirumandas M
- Tizzano M
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- Todman MS
- Tomassen P
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- Tomassen P
- Tomassen P
- Toppila‐Salmi S
- Tos M
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- Tosca MA
- Toskala E
- Tosun F
- Tournas A
- Tran Khai Hoan N
- Tripathi A
- Trompette A
- Tscopp KP
- Tsetsos N
- Turan A
- Turan A
- Turfe Z
- Turner JH
- Turner JH
- Turner JH
- Turner JH
- Turner JH
- Tyler MA
- Tyler MA
- Tyler MA
- Tyler MA
- Tzelnick S
- Ualiyeva S
- Ueda D
- Ulualp SO
- Ulualp SO
- Unlu HH
- Unsal AA
- Ural A
- Uri N
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- Vaezi MF
- Vaidyanathan S
- Vaiman M
- Vaira LA
- Vaira LA
- Valdes CJ
- Valentine R
- Valentine R
- Valentine R
- Valera FCP
- Van Bruaene N
- Van Crombruggen K
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- Van Der Veen J
- Van der Veken P
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- Varshney R
- Varvyanskaya A
- Vashishta R
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- Vceva A
- Velasquez N
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- Venekamp RP
- Venekamp RP
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- Veskitkul J
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- Villari CR
- Virgin F
- Virgin FW
- Virgin FW
- Vlastarakos PV
- Vlckova I
- Vleming M
- Voegels RL
- Von Buchwald C
- Vreugdenburg TD
- Vultaggio A
- Vuralkan E
- Wadwongtham W
- Wagener JS
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- Wald ER
- Wald ER
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- Wald ER.
- Walker A
- Wallwork B
- Walsh JE
- Walsh TJ
- Wan H
- Wandell GM
- Wang CS
- Wang EW
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- Wang F
- Wang F
- Wang J
- Wang JH
- Wang LF
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- Wang L‐F
- Wang L‐F
- Wang M
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- Wang PC
- Wang TT
- Wang W
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- Wang X
- Wang X
- Wang X
- Wasan A
- Watelet J‐B
- Watts WJ
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- Weakley J
- Weber R
- Weber R
- Wechsler ME
- Wei CC
- Wei JL
- Weinberg EA
- Weinhold B
- Weissman JD
- Weitzel EK
- Welch KC
- Welch KC
- Welch KC.
- Wellborn PS
- Wen W LW
- Wen YS
- Wentzel JL
- Weschta M
- Westman M
- Westrin KM
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- Williamson IG
- Wilson AM
- Wilson KF
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- Wise SK
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- Wise SK
- Won HK
- Wong AYS
- Wong D
- Wong IW
- Wong IW
- Wong SJ
- Wood AJ
- Wood AJ
- Woodard T
- Woodhouse BM
- Woods CM
- Woodworth BA
- Woodworth BA
- Woodworth BA
- Woodworth BA
- Woodworth BA.
- Workman AD
- Workman AD
- Workman AD
- Workman AD
- Workman AD
- Workman AD
- Wormald PJ
- Wormald PJ
- Wright ED
- Wu AW
- Wu AW
- Wu D
- Wu D
- Wu D
- Wu J
- Wu Y‐X
- Wuister AM
- Wuokko‐Landén A
- Xia Z
- Xian M
- Xu J
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- Xu Z
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- Yamasaki A
- Yan C
- Yan CH
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- Yan CH
- Yan CH
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- Yancey KL
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- Yang C
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- Yayik AM
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- Yohai RA
- Yoo F
- Yoo HS
- Yoon H
- Yoon HY
- Yoshida K
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- Young LC
- Yousefi J
- Yu MS
- Yu X
- Yu XM
- Zabner J
- Zacharek M
- Zainine R
- Zajac AE
- Zalmanovici Trestioreanu A
- Zalmanovici Trestioreanu A
- Zariwala MA
- Zeiger J
- Zeng M
- Zeng M
- Zhai GT
- Zhang L
- Zhang ML
- Zhang N
- Zhang N
- Zhang N
- Zhang Q
- Zhang S
- Zhang S
- Zhang S
- Zhang Y
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhang Z
- Zhang Z
- Zhang Z
- Zhao CY
- Zhao K
- Zhao K
- Zhao L
- Zhao YC
- Zhao YC
- Zheng C
- Zheng Z
- Zhou B
- Zia S
- Ziegler CGK
- Zielinska‐Blizniewska H
- Zou L
- Zuckerman JD
- Zurlo JJ
- Zuskin E
- Čulig J
- Publication venue
- 'Wiley'
- Publication date
- 01/01/2021
- Field of study
Background: The 5 years since the publication of the first International Consensus Statement on Allergy and Rhinology: Rhinosinusitis (ICAR‐RS) has witnessed foundational progress in our understanding and treatment of rhinologic disease. These advances are reflected within the more than 40 new topics covered within the ICAR‐RS‐2021 as well as updates to the original 140 topics. This executive summary consolidates the evidence‐based findings of the document. Methods: ICAR‐RS presents over 180 topics in the forms of evidence‐based reviews with recommendations (EBRRs), evidence‐based reviews, and literature reviews. The highest grade structured recommendations of the EBRR sections are summarized in this executive summary. Results: ICAR‐RS‐2021 covers 22 topics regarding the medical management of RS, which are grade A/B and are presented in the executive summary. Additionally, 4 topics regarding the surgical management of RS are grade A/B and are presented in the executive summary. Finally, a comprehensive evidence‐based management algorithm is provided. Conclusion: This ICAR‐RS‐2021 executive summary provides a compilation of the evidence‐based recommendations for medical and surgical treatment of the most common forms of RS
Accuracy versus precision in boosted top tagging with the ATLAS detector
- Author
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- Aakvaag E
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- Abdelhameed S
- Abeling K
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- Huang Y
- Huang Y
- Huang Z
- Hubacek Z
- Huebner M
- Huegging F
- Huffman TB
- Hugli CA
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- Hurrell LTB
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- Joos HL
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- Juzek MK
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- Kalaitzidou I
- Kalderon CW
- Kang NJ
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- Kareem MJ
- Karentzos E
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- Karyukhin AN
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- Klimentov A
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- Koch SF
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- Kodyš P
- Koeck DM
- Koenig PT
- Koffas T
- Kolay O
- Koletsou I
- Komarek T
- Kong AXY
- Kono T
- Konstantinidis N
- Kontaxakis P
- Konya B
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- Koperny S
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- Kostyukhin VV
- Kotsokechagia A
- Kotwal A
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- Kourkoumeli-Charalampidi A
- Kourkoumelis C
- Kourlitis E
- Kovanda O
- Kowalewski R
- Kozanecki W
- Kozhin AS
- Kramarenko VA
- Kramberger G
- Kramer P
- Krasny MW
- Krasznahorkay A
- Kraus AC
- Kraus JW
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- Kurdysh O
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- Kurova A
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- Kuze M
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- Kyriacou NG
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- Ladygin E
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- Lahbabi FZ
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- Lang VS
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- Lankford AJ
- Lanni F
- Lantzsch K
- Lanza A
- Lançon E
- Laporte JF
- Lari T
- Lassnig M
- Latonova V
- Latour BMD
- Laurier A
- Lawlor SD
- Lawrence Z
- Lazaridou R
- Lazzaroni M
- Le Boulicaut EM
- Le Pottier LT
- Le B
- Leban B
- Lebedev A
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- Lee S
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- Leeuw LL
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- Leinonen W
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- Leite MAL
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- Leitner R
- Leney KJC
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- Leone S
- Leonidopoulos C
- Leopold A
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- Li K
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- Li Z
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- Liberti B
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- Lima VF
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- Lindley RE
- Lindon JH
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- Lipeles E
- Lipniacka A
- Lister A
- Little JD
- Liu B
- Liu BX
- Liu D
- Liu EHL
- Liu JB
- Liu JKK
- Liu K
- Liu K
- Liu M
- Liu MY
- Liu P
- Liu Q
- Liu X
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- Liu Y
- Liu YL
- Liu YW
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- Llácer MM
- Lobodzinska EM
- Loch P
- Lohse T
- Lohwasser K
- Loiacono E
- Lokajicek M
- Lomas JD
- Long JD
- Longarini I
- Longo R
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- Lopez-canelas NA
- Lory AM
- Losada M
- Loseva O
- Lou X
- Lou X
- Lounis A
- Love PA
- Lu G
- Lu M
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- Lu YJ
- Lubatti HJ
- Luci C
- Luehring F
- Luengo SIF
- Luise I
- Lukianchuk O
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- Lundberg O
- Luongo NA
- Lutz MS
- Lux AB
- Lynn D
- Lysak R
- Lytken E
- Lyubushkin V
- Lyubushkina T
- Lyukova MM
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- Maeno T
- Maguire H
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- Maio A
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- Zhemchugov A
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- IOP Publishing
- Publication date
- 01/08/2024
- Field of study
Abstract
The identification of top quark decays where the top quark has a large momentum transverse to the beam axis, known as top tagging, is a crucial component in many measurements of Standard Model processes and searches for beyond the Standard Model physics at the Large Hadron Collider.
Machine learning techniques have improved the performance of top tagging algorithms, but the size of the systematic uncertainties for all proposed algorithms has not been systematically studied.
This paper presents the performance of several machine learning based top tagging algorithms on a dataset constructed from simulated proton-proton collision events measured with the ATLAS detector at √
s
= 13 TeV.
The systematic uncertainties associated with these algorithms are estimated through an approximate procedure that is not meant to be used in a physics analysis, but is appropriate for the level of precision required for this study.
The most performant algorithms are found to have the largest uncertainties, motivating the development of methods to reduce these uncertainties without compromising performance.
To enable such efforts in the wider scientific community, the datasets used in this paper are made publicly available.</jats:p
Combination and summary of ATLAS dark matter searches interpreted in a 2HDM with a pseudo-scalar mediator using 139 fb−1 of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" altimg="si157.svg"><mml:mrow><mml:msqrt><mml:mrow><mml:mi>s</mml:mi></mml:mrow></mml:msqrt><mml:mo linebreak="goodbreak" linebreakstyle="after">=</mml:mo><mml:mn>13</mml:mn></mml:mrow></mml:math> TeV pp collision data
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- Abbott B
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- Abidi SH
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- Yamauchi H
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- Yao W-M
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- Yeo BK
- Yexley MR
- Yin P
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- Young CJS
- Yu Y
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- Yue L
- Zaazoua M
- Zabinski B
- Zaid E
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zang J
- Zanzi D
- Zaplatilek O
- Zeitnitz C
- Zeng H
- Zeng JC
- Zenger DT
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhai M
- Zhang B
- Zhang DF
- Zhang J
- Zhang J
- Zhang K
- Zhang L
- Zhang P
- Zhang R
- Zhang S
- Zhang T
- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
- Zhou Y
- Zhu CG
- Zhu J
- Zhu Y
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Elsevier BV
- Publication date
- 01/07/2024
- Field of study
Results from a wide range of searches targeting different experimental signatures with and without missing transverse momentum (
) are used to constrain a Two–Higgs-Doublet Model (2HDM) with an additional pseudo-scalar mediating the interaction between ordinary and dark matter (2HDM + a). The analyses use up to 139 fb−1 of proton–proton collision data at a centre-of-mass energy
TeV recorded with the ATLAS detector at the Large Hadron Collider during 2015–2018. The results from three of the most sensitive searches are combined statistically. These searches target signatures with large
and a leptonically decaying Z boson; large
and a Higgs boson decaying to bottom quarks; and production of charged Higgs bosons in final states with top and bottom quarks, respectively. Constraints are derived for several common and new benchmark scenarios in the 2HDM + a
Search for dark photons in rare Z boson decays with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Adam Bourdarios C
- Adamczyk L
- Adamek L
- Addepalli SV
- Addison MJ
- Adelman J
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahuja S
- Ai X
- Aielli G
- Ait Tamlihat M
- Aitbenchikh B
- Aizenberg I
- Akbiyik M
- Akimov AV
- Akiyama D
- Akolkar NN
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Albouy GL
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Algren M
- Alhroob M
- Ali B
- Ali HMJ
- Ali S
- Alibocus SW
- Aliev M
- Alimonti G
- Alkakhi W
- Allaire C
- Allbrooke BMM
- Allen JF
- Allendes Flores CA
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alvarez Estevez M
- Alvarez Fernandez A
- Alves Cardoso M
- Alviggi MG
- Aly M
- Amaral Coutinho Y
- Ambler A
- Amelung C
- Amerl M
- Ames CG
- Amidei D
- Amor Dos Santos SP
- Amos KR
- Ananiev V
- Anastopoulos C
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
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- Zeng H
- Zeng JC
- Zenger DT
- Zenin O
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- Zerradi S
- Zerwas D
- Zhai M
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- Zhang J
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- Zhang X
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- Zhang Z
- Zhang Z
- Zhao H
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- Zhemchugov A
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
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- Zhu CG
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- Zhu Y
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- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2023
- Field of study
A search for events with a dark photon produced in association with a dark Higgs boson via rare decays of the standard model
Z
boson is presented, using
139
fb
−
1
of
√
s
=
13
TeV
proton-proton collision data recorded by the ATLAS detector at the Large Hadron Collider. The dark boson decays into a pair of dark photons, and at least two of the three dark photons must each decay into a pair of electrons or muons, resulting in at least two same-flavor opposite-charge lepton pairs in the final state. The data are found to be consistent with the background prediction, and upper limits are set on the dark photon’s coupling to the dark Higgs boson times the kinetic mixing between the standard model photon and the dark photon,
α
D
ϵ
2
, in the dark photon mass range of [5, 40] GeV except for the
Υ
mass window [8.8, 11.1] GeV. This search explores new parameter space not previously excluded by other experiments
Combined measurement of the Higgs boson mass from the H → γγ and H → ZZ∗ → 4ℓ decay channels with the ATLAS detector using √s = 7, 8, and 13 TeV pp collision data
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adam Bourdarios C
- Adamczyk L
- Addepalli SV
- Addison MJ
- Adelman J
- Adiguzel A
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- Affolder AA
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- Agaras MN
- Agarwala J
- Aggarwal A
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- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahuja S
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- Aizenberg I
- Akbiyik M
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- Akolkar NN
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- Aleksandrov IN
- Alexa C
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- Ali B
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- Allaire C
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- Zenger DT
- Zenin O
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- Zhang Z
- Zhao H
- Zhao P
- Zhao T
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- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
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- Zhu CG
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- Zhu Y
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- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2023
- Field of study
A measurement of the mass of the Higgs boson combining the
H
→
Z
Z
∗
→
4
ℓ
and
H
→
γ
γ
decay channels is presented. The result is based on
140
fb
−
1
of proton-proton collision data collected by the ATLAS detector during LHC run 2 at a center-of-mass energy of 13 TeV combined with the run 1 ATLAS mass measurement, performed at center-of-mass energies of 7 and 8 TeV, yielding a Higgs boson mass of
125.11
±
0.09
(
stat
)
±
0.06
(
syst
)
=
125.11
±
0.11
GeV
. This corresponds to a 0.09% precision achieved on this fundamental parameter of the Standard Model of particle physics
- …