182 research outputs found
Digital Pixel Test Structures implemented in a 65 nm CMOS process
- Author
- Andronic Anton
- Antonelli Matias
- Aresti Mauro
- Baccomi Roberto
- Becht Pascal
- Beole Stefania
- Braach Justus
- Buckland Matthew Daniel
- Buschmann Eric
- Camerini Paolo
- Carnesecchi Francesca
- Cecconi Leonardo
- Charbon Edoardo
- Contin Giacomo
- Dannheim Dominik
- de Melo Joao
- Deng Wenjing
- di Mauro Antonello
- Hasenbichler Jan
- Hillemanns Hartmut
- Hong Geun Hee
- Isakov Artem
- Junique Antoine
- Kluge Alex
- Kotliarov Artem
- Křížek Filip
- Lautner Lukas
- Mager Magnus
- Marras Davide
- Martinengo Paolo
- Masciocchi Silvia
- Menzel Marius Wilm
- Munker Magdalena
- Piro Francesco
- Rachevski Alexandre
- Rebane Karoliina
- Reidt Felix
- Rinella Gianluca Aglieri
- Russo Roberto
- Sanna Isabella
- Sarritzu Valerio
- Senyukov Serhiy
- Snoeys Walter
- Sonneveld Jory
- Svihra Peter
- Tiltmann Nicolas
- Usai Gianluca
- Van Beelen Jacob Bastiaan
- Vassilev Mirella Dimitrova
- Vernieri Caterina
- Villani Anna
- Šuljić Miljenko
- Publication venue
- Publication date
- 14/02/2023
- Field of study
The ALICE ITS3 (Inner Tracking System 3) upgrade project and the CERN EP R&D
on monolithic pixel sensors are investigating the feasibility of the Tower
Partners Semiconductor Co. 65 nm process for use in the next generation of
vertex detectors. The ITS3 aims to employ wafer-scale Monolithic Active Pixel
Sensors thinned down to 20 to 40 um and bent to form truly cylindrical half
barrels. Among the first critical steps towards the realisation of this
detector is to validate the sensor technology through extensive
characterisation both in the laboratory and with in-beam measurements. The
Digital Pixel Test Structure (DPTS) is one of the prototypes produced in the
first sensor submission in this technology and has undergone a systematic
measurement campaign whose details are presented in this article.
The results confirm the goals of detection efficiency and non-ionising and
ionising radiation hardness up to the expected levels for ALICE ITS3 and also
demonstrate operation at +20 C and a detection efficiency of 99% for a DPTS
irradiated with a dose of 1015 1 MeV neq/cm2.
Furthermore, spatial, timing and energy resolutions were measured at various
settings and irradiation levels.Comment: Updated threshold calibration method. Implemented colorblind friendly
color palette in all figures. Updated reference
Digital Pixel Test Structures implemented in a 65 nm CMOS process
- Author
- Andronic Anton
- Antonelli Matias
- Aresti Mauro
- Baccomi Roberto
- Becht Pascal
- Beole Stefania
- Braach Justus
- Buckland Matthew Daniel
- Buschmann Eric
- Camerini Paolo
- Carnesecchi Francesca
- Cecconi Leonardo
- Charbon Edoardo
- Contin Giacomo
- Dannheim Dominik
- de Melo Joao
- Deng Wenjing
- Di Mauro Antonello
- Hasenbichler Jan
- Hillemanns Hartmut
- Hong Geun Hee
- Isakov Artem
- Junique Antoine
- Kluge Alex
- Kotliarov Artem
- Křížek Filip
- Lautner Lukas
- Mager Magnus
- Marras Davide
- Martinengo Paolo
- Masciocchi Silvia
- Menzel Marius Wilm
- Munker Magdalena
- Piro Francesco
- Rashevski Sasha
- Rebane Karoliina
- Reidt Felix
- Rinella Gianluca Aglieri
- Russo Roberto
- Sanna Isabella
- Sarritzu Valerio
- Senyukov Serhiy
- Snoeys Walter
- Sonneveld Jory
- Svihra Peter
- Tiltmann Nicolas
- Usai Gianluca
- van Beelen Jacob Bastiaan
- Vassilev Mirella Dimitrova
- Vernieri Caterina
- Villani Anna
- Šuljić Miljenko
- Publication venue
- HAL CCSD
- Publication date
- 16/12/2022
- Field of study
The ALICE ITS3 (Inner Tracking System 3) upgrade project and the CERN EP R&D on monolithic pixel sensors are investigating the feasibility of the Tower Partners Semiconductor Co. 65 nm process for use in the next generation of vertex detectors. The ITS3 aims to employ wafer-scale Monolithic Active Pixel Sensors thinned down to 20 to 40 um and bent to form truly cylindrical half barrels. Among the first critical steps towards the realisation of this detector is to validate the sensor technology through extensive characterisation both in the laboratory and with in-beam measurements. The Digital Pixel Test Structure (DPTS) is one of the prototypes produced in the first sensor submission in this technology and has undergone a systematic measurement campaign whose details are presented in this article. The results confirm the goals of detection efficiency and non-ionising and ionising radiation hardness up to the expected levels for ALICE ITS3 and also demonstrate operation at +20 C and a detection efficiency of 99% for a DPTS irradiated with a dose of 1015 1 MeV neq/cm2. Furthermore, spatial, timing and energy resolutions were measured at various settings and irradiation levels
Characterisation of analogue Monolithic Active Pixel Sensor test structures implemented in a 65 nm CMOS imaging process
- Author
- Alocco Giacomo
- Antonelli Matias
- Baccomi Roberto
- Beole Stefania Maria
- Blidaru Mihail Bogdan
- Buschmann Eric
- Buttwill Bent Benedikt
- Camerini Paolo
- Carnesecchi Francesca
- Chartier Marielle
- Choi Yongjun
- Colocci Manuel
- Contin Giacomo
- Dannheim Dominik
- Daza Sara Ruiz
- de Gruttola Daniele
- Di Mauro Antonello
- Donner Maurice Calvin
- Dubla Andrea
- Eberwein Gregor Hieronymus
- Egger Jan
- Fabbietti Laura
- Feindt Finn
- Gautam Kunal
- Gernhaeuser Roman
- Glover James Julian
- Gonella Laura
- Gregor Ingrid-Maria
- Grodaas Karl Gran
- Hillemanns Hartmut
- Huth Lennart
- Ilg Armin
- Isakov Artem
- Jones Daniel Matthew
- Junique Antoine
- Kaewjai Jetnipit
- Keil Markus
- Kim Jiyoung
- Kittimanapun Kritsada
- Kluge Alex
- Kobdaj Chinorat
- Kotliarov Artem
- Kucharska Gabriela
- Kushpil Svetlana
- Křížek Filip
- La Rocca Paola
- Laojamnongwong Natthawut
- Lautner Lukas
- Lemmon Roy Crawford
- Lemoine Corentin
- Li Long
- Librizzi Francesco
- Liu Jian
- Macchiolo Anna
- Mager Magnus
- Marras Davide
- Martinengo Paolo
- Masciocchi Silvia
- Mattiazzo Serena
- Menzel Marius Wilm
- Mulliri Alice
- Mylne Mia Rose
- Piro Francesco
- Rachevski Alexandre
- Rasà Marika
- Rebane Karoliina
- Reidt Felix
- Ricci Riccardo
- Rinella Gianluca Aglieri
- Saccà Gaspare
- Sanna Isabella
- Sarritzu Valerio
- Schlaadt Judith
- Schledewitz David
- Scioli Gilda
- Senyukov Serhiy
- Simancas Adriana
- Snoeys Walter
- Spannagel Simon
- Sturniolo Alessandro
- Tiltmann Nicolas
- Trifirò Antonio
- Usai Gianluca
- van Beelen Jacob Bastiaan
- Vanat Tomas
- Varga Laszlo
- Verdoglia Michele
- Viera Manuel del Rio
- Vignola Gianpiero
- Villani Anna
- Wennloef Haakan
- Witte Jonathan
- Wittwer Rebekka Bettina
- Šuljić Miljenko
- Publication venue
- HAL CCSD
- Publication date
- 27/03/2024
- Field of study
International audienceAnalogue test structures were fabricated using the Tower Partners Semiconductor Co. CMOS 65 nm ISC process. The purpose was to characterise and qualify this process and to optimise the sensor for the next generation of Monolithic Active Pixels Sensors for high-energy physics. The technology was explored in several variants which differed by: doping levels, pixel geometries and pixel pitches (10-25 μm). These variants have been tested following exposure to varying levels of irradiation up to 3 MGy and 1016 1 MeV neq cm−2. Here the results from prototypes that feature direct analogue output of a 4×4 pixel matrix are reported, allowing the systematic and detailed study of charge collection properties. Measurements were taken both using 55Fe X-ray sources and in beam tests using minimum ionizing particles. The results not only demonstrate the feasibility of using this technology for particle detection but also serve as a reference for future applications and optimisations
Annual Report 2023 and Phase-I Closeout
- Author
- Aglieri Rinella Gianluca
- Aleksa Martin
- Alfiero Daniele
- Alvarez Feito Diego
- Amatriain Carballo Aitor
- Andorno Marco
- Angeletti Massimo
- Antoszczuk Pablo Daniel
- Arena Maria Cristina
- Aretio Zarate Fernando
- Arpin Nathan Gaston
- Asbah Nedaa Alexandra
- Asensi Tortajada Ignacio
- Auffray Hillemanns Etiennette
- Ballabriga Sune Rafael
- Balutto Mattia
- Bandi Franco Nahuel
- Barba Higueras Maria
- Barney David
- Baron Sophie
- Baszczyk Mateusz Karol
- Benoit Philippe
- Bernardi Luca
- Biereigel Stefan
- Blomer Jakob
- Boelens Tonka
- Bordelius Aleksandar
- Borghello Giulio
- Bouvier Philippe
- Boyer Francois
- Braach Justus
- Brambilla Francesco Enrico
- Brandao De Souza Mendes Eduardo
- Bremer Johan
- Brondolin Erica
- Bruggeman Jurriaan
- Brunbauer Florian Maximilian
- Bugiel Szymon
- Bulling Anthony Frederick
- Buschmann Eric
- Buytaert Jan
- Byczynski Wiktor
- Cala' Roberto
- Campbell Michael
- Caratelli Alessandro
- Carceller Juan Miguel
- Carnesecchi Francesca
- Carnesecchi Riccardo
- Catinaccio Andrea
- Cecconi Leonardo
- Ceresa Davide
- Chalifour Michel
- Coco Victor
- Collins Paula
- Contiero Luca
- Cortes Fernandez Placido Martin
- Costanzi Ruddy
- Cure Benoit
- Curras Rivera Esteban
- D'Ambrosio Carmelo
- Dachs Florian
- Dannheim Dominik
- Dao Valerio
- De Benedetti Federico
- De Boer Jan
- De Melo Joao
- De Oliveira Rui
- Deelen Nikkie
- Deng Wenjing
- Detraz Stephane
- Dhaliwal Jashandeep
- Di Castro Mario
- Di Mauro Antonello
- Dias Matheo
- Dobrijevic Dominik
- Dorda Ana
- Dorosz Piotr Andrzej
- Dort Katharina
- Dudarev Alexey
- Dumps Raphael
- Eberwein Gregor Hieronymus
- Ellenbroek Veerle Jasmijn
- Emiliani Simone
- Faccio Federico
- Ferry Serge
- Flier Gerrit
- Floethner Karl Jonathan
- Francois Brieuc
- Frei Christoph
- Gabrielli Andrea
- Gargiulo Corrado
- Gawehn Anna
- Gerwig Hubert
- Gessinger-Befurt Paul
- Gkougkousis Vagelis
- Gluchowska Weronika
- Gris Alexandra
- Grodaas Karl Gran
- Groettvik Ola Slettevoll
- Guida Roberto
- Gustavino Carlo
- Gys Thierry
- Haimberger Jakob
- Hajheidari Mohammadtaghi
- Halvorsen Marius Mahlum
- Hasenbichler Jan
- Hawkings Richard
- Hellenschmidt Desiree
- Hillemanns Hartmut
- Himmerlich Anja
- Hoffmann Tobias
- Hong Geun Hee
- Howard Alexander
- Ijzermans Pieter
- Jaekel Martin
- Jakobsen Sune
- Jama Kacper
- Janot Patrick
- Janssens Djunes
- Joram Christian
- Junique Antoine
- Jurco Roberto
- Kaplon Jan
- Keizer Floris
- Kholodenko Sergey
- Kiehn Moritz
- Klaassen Dennis
- Klekotko Adam
- Kloukinas Kostas
- Kluge Alex
- Koppitz Martina Maria
- Krammer Manfred
- Kratochwil Nicolaus
- Kraus Veronika
- Kremastiotis Iraklis
- Kroeger Jens
- Kruyt Peter Martin
- Kucharska Gabriela
- Kuehn Susanne
- Kugathasan Thanushan
- Kulis Szymon
- Lalovic Milana
- Laudi Elisa
- LeBlanc Matt
- Lehmann Miotto Giovanna
- Lemoine Corentin
- Lemos Cid Edgar
- Lindner Rolf
- Linssen Lucie
- Lisowska Marta
- Lopez Gomez Javier
- Mager Magnus
- Malentacca Lorenzo
- Malinowski Filip
- Mandelli Beatrice
- Manolescu Florentina
- Martina Francesco
- Martinazzoli Loris
- Martinengo Paolo
- Mato Vila Pere
- Mazzei Francesco
- Mcalpine Lee
- Mcgreavy Chris
- Mehl Bertrand
- Mentink Matthias
- Menzel Marius Wilm
- Michelis Stefano
- Mlynarikova Michaela
- Molina Soledad
- Moll Michael
- Morant Johan
- Muller Hans
- Munker Magdalena
- Munzer Robert Helmut
- Musa Luciano
- Neroni Michela
- Nikiforou Nikiforos
- Nookala Anvesh
- Olantera Lauri
- Oliveri Eraldo
- Orlandini Giorgio
- Otarid Younes
- Pacifico Nicola
- Padulano Vincenzo Eduardo
- Pais Preema Rennee
- Pandey Awanish
- Pantaleo Felice
- Pape Sebastian
- Pazos Rial Eloi
- Pedano Medina Camila Rocio
- Pejasinovic Risto
- Pekkanen Juska
- Pernegger Heinz
- Petagna Paolo
- Piedigrossi Didier
- Piernas Diaz Francisco
- Piller Markus
- Piro Francesco
- Pizzichemi Marco
- Pizzirusso Olivier
- Poblocki Marcin Tadeusz
- Prousalidi Thenia
- Raikwar Piyush
- Ravasenga Ivan
- Raymond Michel
- Rebane Karolina
- Reichenbach Leonhard
- Reidt Felix
- Rembser Christoph
- Riedler Petra
- Riegler Werner
- Rigoletti Gianluca
- Ripamonti Giacomo
- Rodrigues Simoes Moreira Paulo
- Rodrigues Alexis
- Roloff Philipp Gerhard
- Ropelewski Leszek
- Rovere Marco
- Sailer Andre
- Sajdak Michal Jan
- Salamani Dalila
- Salomoni Matteo
- Salzburger Andreas
- Sanna Isabella
- Sasikumar Swathi
- Sauli Fabio
- Scaramuzzino Paolo Francesco
- Scarcella Carmelo
- Scharenberg Lucian
- Schindler Heinrich
- Schmidt Burkhard
- Schmidt Janis Viktor
- Schneider Thomas
- Schopper Andreas
- Secouet Pascal Jean
- Selvaggi Michele
- Sharma Abhishek
- Sicking Eva
- Sigaud Christophe
- Singh Shuvay
- Snoeys Walter
- Solans Sanchez Carlos
- Soos Csaba
- Sorgenfrei Niels
- Sriskaran Viros
- Stahl Sascha
- Stewart Graeme A
- Stumpert Valentin
- Subert Vendula
- Suljic Miljenko
- Svihra Peter
- Teixeira Antonio
- Teofili Lorenzo
- Termo Gennaro
- Tiltmann Nicolas
- Tong Qiaomu
- Troska Jan
- Tsiokanos Ioannis
- Utrobicic Antonija
- Van Beelen Jacob Bastiaan
- Van den Eijnden Joep
- Van Der Werf Jasper
- Van Rijnbach Milou
- Van Stenis Miranda
- Vanat Tomas
- Vasey Francois
- Vaskuri Anna
- Vazquez Nunez Marcos
- Veenhof Rob
- Verlaat Bart
- Verzeroli Mattia
- Vicente Barreto Pinto Mateus
- Vicente Leitao Pedro
- Vichoudis Paschalis
- Viqueira Rodriguez Manuel
- Volker Alexander
- Volkl Valentin
- Wanotayaroj Chaowaroj
- Weick Julian
- Wertelaers Piet
- Wiehe Moritz
- Wilkens Henric
- Williams Morag
- Yang Xiao
- Zaborowska Anna
- Publication venue
- Publication date
- 14/03/2024
- Field of study
This report summarises the activities of the CERN strategic R&D programme on technologies for future experiments during the year 2023, and highlights the achievements of the programme during its first phase 2020-2023
Measurement of the impact-parameter dependent azimuthal anisotropy in coherent ρ0 photoproduction in Pb–Pb collisions at √sNN = 5.02 TeV
- Author
- Abranches De Carvalho Leopoldo
- Acharya Shreyasi
- Adamová Dagmar
- Agarwal Apar
- Aglieri Rinella Gianluca
- Aglietta Luca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- Akishina Valentina
- Al-Turany Mohammad
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Mas’ud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Alici Andrea
- Alizadehvandchali Negin
- Alkin Anton
- Alme Johan
- Alocco Giacomo
- Alt Torsten
- Altamura Anna Rita
- Altsybeev Igor
- Alvarado Garcia Jesús Ricardo
- Amatriain Carballo Aitor
- Anaam Mustafa Naji
- Andrei Cristian
- Andreou Nicodemos
- Andronic Anton
- Andronov Evgeny
- Anguelov Venelin
- Antinori Federico
- Antonioli Pietro
- Apadula Nicole
- Aphecetche Laurent Bernard
- Appelshäuser Harald
- Arata Carolina
- Arcelli Silvia
- Aresti Mauro
- Arnaldi Roberta
- Arneiro Jhoao Gabriel Martins Campos Almeida
- Arsene Ionut Cristian
- Arslandok Mesut
- Arteche Diaz Raul
- Augustinus Andre
- Averbeck Ralf Peter
- Azmi Mohd Danish
- Baba Hitoshi
- Badalà Angela
- Bae Joonsuk
- Baek Yong Wook
- Bai Xiaozhi
- Bailhache Raphaëlle
- Bailung Yoshini
- Bala Renu
- Balbino Alessandro
- Baldisseri Alberto
- Balis Bartosz
- Banerjee Debjani
- Banoo Zarina
- Barbasova Veronika
- Barile Francesco
- Barioglio Luca
- Barlou Maria
- Barman Banajit
- Barnaföldi Gergely Gábor
- Barnby Lee Stuart
- Barreau Emilie Martine
- Barreto De Oliveira Campos Leonardo
- Bartels Clara
- Barth Klaus
- Bartsch Esther
- Bastid Nicole
- Basu Sumit
- Batigne Guillaume
- Battistini Daniel
- Batyunya Boris
- Bauri Dibakar
- Bazo Alba José Luis
- Bearden Ian Gardner
- Beattie Caitlin
- Becht Pascal
- Behera Debadatta
- Belikov Iouri
- Bell Hechavarria Ailec de la Caridad
- Bellini Francesca
- Bellwied Rene
- Belokurova Svetlana
- Bencédi Gyula
- Bensaoula Adel
- Beolè Stefania
- Berdnikov Yaroslav
- Berdnikova Anastasia
- Bergmann Luisa
- Bertran Ferrer Marta
- Besoiu Mihaela Gabriela
- Betev Latchezar
- Bhaduri Partha Pratim
- Bhasin Anju
- Bhattacharjee Buddhadeb
- Bianchi Livio
- Bianchi Nicola
- Bielčík Jaroslav
- Bielčíková Jana
- Bigot Alexandre Patrick
- Bilandzic Ante
- Biro Gabor
- Biswas Saikat
- Bize Nicolas Luc
- Blair Justin Thomas
- Blau Dmitry S.
- Blidaru Mihail-Bogdan
- Bluhme Nora
- Blume Christoph
- Boca Gianluigi
- Bock Friederike
- Bodova Tea
- Bok Jeongsu
- Boldizsar Laszlo
- Bombara Marek
- Bond Peter Matthew
- Bonomi Germano
- Borel Herve
- Borissov Alexander
- Borquez Carcamo Andres Gerardo
- Bossi Hannah
- Botta Elena
- Bratrud Lars
- Braun-Munzinger Peter
- Bregant Marco
- Broz Michal
- Bruno Giuseppe Eugenio
- Buchakchiev Valentin Dimitrov
- Buckland Matthew Daniel
- Budnikov Dmitry
- Bufalino Stefania
- Burmasov Nazar
- Buthelezi Edith Zinhle
- Bylinkin Alexander
- Bysiak Sebastian Adam
- Bühler Paul
- Büsching Henner
- Cabanillas Noris Juan Carlos
- Cai Mengke
- Caines Helen Louise
- Caliva Alberto
- Calvo Villar Ernesto
- Camerini Paolo
- Canedo Fabio de Moraes
- Carabas Mihai
- Carnesecchi Francesca
- Caron Robin Albert Andre
- Castillo Castellanos Javier Ernesto
- Castoldi Matteo
- Catalano Fabio
- Cattaruzzi Samuele
- Ceballos Sanchez Cesar
- Cerri Rebecca
- Chakaberia Irakli
- Chakraborty Pritam
- Chandra Sinjini
- Chapeland Sylvain
- Chartier Marielle
- Chattopadhay Souvik
- Chattopadhyay Subhasis
- Chattopadhyay Sukalyan
- Chen Meiyi
- Cheng Tiantian
- Cheshkov Cvetan Valeriev
- Chibante Barroso Vasco Miguel
- Chinellato David Dobrigkeit
- Chizzali Emma Sophia
- Cho Jaeyoon
- Cho Soyeon
- Chochula Peter
- Chochulska Zuzanna Anna
- Choudhury Dhrubajyoti
- Christakoglou Panagiotis
- Christensen Christian Holm
- Christiansen Peter L.
- Chujo Tatsuya
- Ciacco Mario
- Cicalò Corrado
- Ciupek Michael Rudolf
- Clai Giulia
- Colamaria Fabio Filippo
- Colburn Jonathan Samuel
- Colella Domenico
- Colocci Manuel
- Concas Matteo
- Conesa Balbastre Gustavo
- Conesa del Valle Zaida
- Contin Giacomo
- Contreras Nuno Jesus Guillermo
- Coquet Maurice
- Cortese Pietro
- Cosentino Mauro Rogerio
- Costa Filippo
- Costanza Susanna
- Cot Corentin
- Crkovská Jana
- Crochet Philippe
- Cruz Torres Reynier
- Cui Pengyao
- Cuveland Jan de
- Czarnynoga Maciej Marek
- Czeslaw Miskowiec Dariusz
- Dainese Andrea
- Dange Gautam
- Danisch Meike Charlotte
- Danu Andrea
- Das Prottay
- Das Prottoy
- Das Supriya
- Dash Archita Rani
- Dash Sadhana
- De Caro Annalisa
- De Cataldo Giacinto
- De Falco Alessandro
- De Gruttola Daniele
- De Marco Nora
- De Martin Chiara
- De Pasquale Salvatore
- Deb Rohaan
- Del Grande Raffaele
- Dello Stritto Luigi
- Deng Wenjing
- Devereaux Kyle Christian
- Dhankher Preeti
- Di Bari Domenico
- Di Mauro Antonio
- Diab Batoul
- Dietel Thomas
- Ding Yanchun
- Ditzel Janik
- Divià Roberto
- Djuvsland Øystein
- Dmitrieva Uliana
- Dobrin Alexandru Florin
- Dominguez Rosas Edgar
- Donigus Benjamin
- Doremalen Lennart Vincent Rogier van
- Duarte Galvan Carlos
- Dubiński Jan Michal
- Dubla Andrea
- Ducati Maria Beatriz de Leone Gay
- Dupieux Pascal
- Dzalaiova Natalia
- Eder Tabea Maria
- Ehlers Raymond James, III
- Eisenhut Florian
- Ejima Ren
- El Mard Bouziani Youssef
- Elia Domenico
- Erazmus Barbara Ewa
- Ercolessi Francesca
- Espagnon Bruno
- Espinoza Beltran Lucina Gabriela
- Eulisse Giulio
- Evans David
- Evdokimov Sergey
- Fabbietti Laura
- Faggin Mattia
- Faivre Julien
- Fan Feng
- Fan Wenqing
- Fantoni Alessandra
- Fasel Markus
- Feliciello Alessandro
- Feofilov Grigori A.
- Fernández Téllez Arturo
- Ferrandi De Oliveira Lucas
- Ferrero Andrea
- Ferrero Chiara
- Ferretti Alessandro
- Feuillard Victor Jose Gaston
- Filova Vendulka
- Finogeev Dmitry
- Fionda Fiorella Maria Celeste
- Flatland Erlend
- Flor Fernando Antonio
- Flores Amanda Nicole
- Foertsch Siegfried Valentin
- Fokin Ilya
- Fokin Sergey
- Follo Umberto
- Fragiacomo Enrico
- Frajna Eszter
- Fuchs Ulrich
- Funicello Nicola
- Furget Christophe
- Furs Artur
- Fusayasu Takahiro
- Gaardhøje Jens Jørgen
- Gagliardi Martino
- Gago Medina Alberto Martín
- Gahlaut Tanu
- Gameiro Munhoz Marcelo
- Gangadharan Dhevan Raja
- Ganoti Paraskevi
- Garabatos Cuadrado Jose Maria
- Garcia Guardiano Gabriel
- Garcia-Solis Edmundo Javier
- García Chávez Tonatiuh
- García Martínez Ginés
- Gargiulo Corrado
- Gasik Piotr
- Gaur Hari Mohan
- Gautam Amrit
- Germain Marie
- Ghosh Chandrasekhar
- Giacalone Marco
- Gioachin Giulia
- Giubellino Paolo
- Giubilato Piero
- Glaenzer Aude Marie Camille
- Glimos Ewa
- Glässel Peter
- Goh Daniel Jia Qin
- Gonzalez Sebastian Victor Luis
- Gordeev Pavel
- Gorgon Marek Boguslaw
- Goswami Kangkan
- Gotovac Sven
- Grabski Varlen
- Graczykowski Łukasz Kamil
- Grecka Ekaterina
- Grelli Alessandro
- Grigoraș Costin
- Grigoryan Smbat
- Grigoryev Vladislav
- Grosa Fabrizio
- Grosso Raffaele
- Große-Oetringhaus Jan Fiete
- Grund David
- Grünwald Nadine Alice
- Guernane Rachid
- Guilbaud Maxime Rene Joseph
- Gulbrandsen Kristjan Herlache
- Gunji Taku
- Guo Wenda
- Gupta Anik
- Gupta Ramni
- Gupta Rashi
- Gwizdziel Katarzyna
- Gyulai Laszlo
- Gündem Tuba
- Hachiya Shimomura Maya
- Hadjidakis Cynthia Marie
- Haider Fakhar Ul
- Haidlova Sara
- Haldar Mintu
- Haller Barthélémy von
- Hamagaki Hideki
- Hamdi Abdennacer
- Han Younghoon
- Hanley Brian Gerald
- Hannigan Ryan
- Hansen Joachim
- Haque Md Rihan
- Harris John William
- Harton Austin Vincent
- Hartung Michael Volker
- Hassan Hadi
- Hatzifotiadou Despina
- Hauer Philip
- Havener Laura Brittany
- Hellbär Ernst
- Helstrup Håvard
- Hemmer Marvin
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- Yu Zhi
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- Zaccolo Valentina
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- Zanone Federica
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- Zhalov Mikhail
- Zhang Biao
- Zhang Chi
- Zhang Liuyao
- Zhang Maolin
- Zhang Mingyu
- Zhang Song
- Zhang Xiaoming
- Zhang Yifei
- Zhang Zhen
- Zhao Mingrui
- Zherebchevskii Vladimir
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Senjie
- Zhu Ya
- Zugravel Stefan Cristi
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- Závada Petr
- Önnerstad Anna
- Šafařík Karel
- Šerkšnytė Laura
- Šuljić Miljenko
- Țăpuş Nicolae
- Publication venue
- Publication date
- 23/05/2024
- Field of study
The first measurement of the impact-parameter dependent angular anisotropy in the decay of coherently photoproduced ρ0 mesons is presented. The ρ0 mesons are reconstructed through their decay into a pion pair. The measured anisotropy corresponds to the amplitude of the cos(2ϕ) modulation, where ϕ is the angle between the two vectors formed by the sum and the difference of the transverse momenta of the pions, respectively. The measurement was performed by the ALICE Collaboration at the LHC using data from ultraperipheral Pb−Pb collisions at a center-of-mass energy of sNN−−−√ = 5.02 TeV per nucleon pair. Different impact-parameter regions are selected by classifying the events in nuclear-breakup classes. The amplitude of the cos(2ϕ) modulation is found to increase by about one order of magnitude from large to small impact parameters. Theoretical calculations, which describe the measurement, explain the cos(2ϕ) anisotropy as the result of a quantum interference effect at the femtometer scale that arises from the ambiguity as to which of the nuclei is the source of the photon in the interaction
Exclusive four pion photoproduction in ultraperipheral Pb-Pb collisions at sNN=5.02 TeV
- Author
- Abranches de Carvalho Leopoldo
- Acharya Shreyasi
- Adamova Dagmar
- Agarwal Apar
- Aglieri Rinella Gianluca
- Aglietta Luca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- Akishina Valentina
- Al-Turany Mohammad
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Masud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Alici Andrea
- Alizadehvandchali Negin
- Alkin Anton
- Alme Johan
- Alocco Giacomo
- Alt Torsten
- Altamura Anna Rita
- Altsybeev Igor
- Alvarado Garcia Jesus Ricardo
- Amatriain Carballo Aitor
- Anaam Mustafa
- Andrei Cristian
- Andreou Nicodemos
- Andronic Anton
- Andronov Evgeny
- Anguelov Venelin
- Antinori Federico
- Antonioli Pietro
- Apadula Nicole
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Arata Carolina
- Arcelli Silvia
- Aresti Mauro
- Arnaldi Roberta
- Arsene Ionut Cristian
- Arslandok Mesut
- Arteche Diaz Raul
- Augustinus Andre
- Averbeck Ralf Peter
- Azmi Mohd Danish
- Baba Hitoshi
- Badala Angela
- Badaro Saramela Thiago
- Bae Joonsuk
- Baek Yongwook
- Bai Xiaozhi
- Bailhache Raphaelle Marie
- Bailung Yoshini
- Bala Renu
- Balbino Alessandro
- Baldisseri Alberto
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- Banoo Zarina
- Barbasova Veronika
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- Barman Banajit
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- Wessels Johannes Peter
- Weyhmiller Sierra Lisa
- Wiechula Jens
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- Wilhelmi Alexander
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- Wilkinson Jeremy John
- Willems Guido Alexander
- Windelband Bernd Stefan
- Winn Michael Andreas
- Wright Josephina Rae
- Wu Wenya
- Wu Yitao
- Xiong Zhenjun
- Xu Ran
- Yadav Ankur
- Yadav Arun Kumar
- Yamaguchi Yorito
- Yang Shiming
- Yano Satoshi
- Yeats Emma Rose
- Yin Zhongbao
- Yoo In Kwon
- Yoon Jin Hee
- Yoval Pozos Irandheny
- Yu Hyeonjin
- Yu Zhi
- Yuan Shiming
- Yuncu Alperen
- Zaccolo Valentina
- Zampolli Chiara
- Zanone Federica
- Zardoshti Nima
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zhalov Mikhail
- Zhang Biao
- Zhang Chi
- Zhang Liuyao
- Zhang Maolin
- Zhang Mingyu
- Zhang Song
- Zhang Xiaoming
- Zhang Yifei
- Zhang Zhen
- Zhao Mingrui
- Zherebchevskii Vladimir
- Zhong Chen
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Senjie
- Zhu Ya
- Zugravel Stefan Cristi
- Zurlo Nicola
- Publication venue
- HAL CCSD
- Publication date
- 23/04/2024
- Field of study
International audienceThe intense photon fluxes from relativistic nuclei provide an opportunity to study photonuclear interactions in ultraperipheral collisions. The measurement of coherently photoproduced π+π−π+π− final states in ultraperipheral Pb-Pb collisions at sNN=5.02 TeV is presented for the first time. The cross section, dσ/dy, times the branching ratio (ρ→π+π+π−π−) is found to be 47.8±2.3 (stat.)±7.7 (syst.) mb in the rapidity interval ∣y∣<0.5. The invariant mass distribution is not well described with a single Breit-Wigner resonance. The production of two interfering resonances, ρ(1450) and ρ(1700), provides a good description of the data. The values of the masses (m) and widths (Γ) of the resonances extracted from the fit are m1=1385±14 (stat.)±3 (syst.) MeV/c2, Γ1=431±36 (stat.)±82 (syst.) MeV/c2, m2=1663±13 (stat.)±22 (syst.) MeV/c2 and Γ2=357±31 (stat.)±49 (syst.) MeV/c2, respectively. The measured cross sections times the branching ratios are compared to recent theoretical predictions
Measurement of Ωc0 baryon production and branching-fraction ratio BR(Ωc0→Ω−e+νe)/BR(Ωc0→Ω−π+) in pp collisions at s = 13 TeV
- Author
- Abranches de Carvalho Leopoldo
- Acharya Shreyasi
- Adamova Dagmar
- Agarwal Apar
- Aglieri Rinella Gianluca
- Aglietta Luca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- Akishina Valentina
- Al-Turany Mohammad
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Masud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Alici Andrea
- Alizadehvandchali Negin
- Alkin Anton
- Alme Johan
- Alocco Giacomo
- Alt Torsten
- Altamura Anna Rita
- Altsybeev Igor
- Alvarado Garcia Jesus Ricardo
- Amatriain Carballo Aitor
- Anaam Mustafa
- Andrei Cristian
- Andreou Nicodemos
- Andronic Anton
- Andronov Evgeny
- Anguelov Venelin
- Antinori Federico
- Antonioli Pietro
- Apadula Nicole
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Arata Carolina
- Arcelli Silvia
- Aresti Mauro
- Arnaldi Roberta
- Arsene Ionut Cristian
- Arslandok Mesut
- Arteche Diaz Raul
- Augustinus Andre
- Averbeck Ralf Peter
- Azmi Mohd Danish
- Baba Hitoshi
- Badala Angela
- Badaro Saramela Thiago
- Bae Joonsuk
- Baek Yongwook
- Bai Xiaozhi
- Bailhache Raphaelle Marie
- Bailung Yoshini
- Bala Renu
- Balbino Alessandro
- Baldisseri Alberto
- Balis Bartosz
- Banerjee Debjani
- Banoo Zarina
- Barbasova Veronika
- Barile Francesco
- Barioglio Luca
- Barlou Maria
- Barman Banajit
- Barnafoldi Gergely Gabor
- Barnby Lee Stuart
- Barreau Emilie Martine
- Barreto de Oliveira Campos Leonardo
- Bartels Clara
- Barth Klaus
- Bartsch Esther
- Bastid Nicole
- Basu Sumit
- Batigne Guillaume
- Battistini Daniel
- Batyunya Boris
- Bauri Dibakar
- Bazo Alba Jose Luis
- Bearden Ian Gardner
- Beattie Caitlin
- Becht Pascal
- Behera Debadatta
- Belikov Iouri
- Bell Hechavarria Ailec
- Bellini Francesca
- Bellwied Rene
- Belokurova Svetlana
- Bencedi Gyula
- Bensaoula Adel
- Beole Stefania Maria
- Berdnikov Yaroslav
- Berdnikova Anastasia
- Bergmann Luisa
- Bertran Ferrer Marta
- Besoiu Mihaela Gabriela
- Betev Latchezar
- Bhaduri Partha Pratim
- Bhasin Anju
- Bhattacharjee Buddhadeb
- Bianchi Livio
- Bianchi Nicola
- Bielcik Jaroslav
- Bielcikova Jana
- Bigot Alexandre Patrick
- Bilandzic Ante
- Biro Gabor
- Biswas Saikat
- Bize Nicolas Luc
- Blair Justin Thomas
- Blau Dmitry
- Blidaru Mihail Bogdan
- Bluhme Nora
- Blume Christoph
- Boca Gianluigi
- Bock Friederike
- Bodova Tea
- Bok Jeongsu
- Boldizsar Laszlo
- Bombara Marek
- Bond Peter Matthew
- Bonomi Germano
- Borel Herve
- Borissov Alexander
- Borquez Carcamo Andres Gerardo
- Bossi Hannah
- Botta Elena
- Bratrud Lars
- Braun-Munzinger Peter
- Bregant Marco
- Broz Michal
- Bruno Giuseppe Eugenio
- Buckland Matthew Daniel
- Budnikov Dmitry
- Buesching Henner
- Bufalino Stefania
- Buhler Paul Alois
- Burmasov Nazar
- Buthelezi Edith Zinhle
- Bylinkin Aleksandr
- Bysiak Sebastian Adam
- Cabanillas Noris Juan Carlos
- Cai Mengke
- Caines Helen Louise
- Caliva Alberto
- Calvo Villar Ernesto
- Camerini Paolo
- Carabas Mihai
- Carnesecchi Francesca
- Caron Robin Albert Andre
- Castillo Castellanos Javier Ernesto
- Castoldi Matteo
- Catalano Fabio
- Cattaruzzi Samuele
- Ceballos Sanchez Cesar
- Cerri Rebecca
- Chakaberia Irakli
- Chakraborty Pritam
- Chandra Sinjini
- Chapeland Sylvain
- Chartier Marielle
- Chattopadhay Souvik
- Chattopadhyay Subhasis
- Chattopadhyay Sukalyan
- Cheng Tiantian
- Cheshkov Cvetan Valeriev
- Chibante Barroso Vasco Miguel
- Chizzali Emma Sophia
- Cho Jaeyoon
- Cho Soyeon
- Chochula Peter
- Chochulska Zuzanna Anna
- Choudhury Dhrubajyoti
- Christakoglou Panagiotis
- Christensen Christian Holm
- Christiansen Peter
- Chujo Tatsuya
- Ciacco Mario
- Cicalo Corrado
- Ciupek Michael Rudolf
- Clai Giulia
- Colamaria Fabio Filippo
- Colburn Jonathan Samuel
- Colella Domenico
- Colocci Manuel
- Concas Matteo
- Conesa Balbastre Gustavo
- Conesa del Valle Zaida
- Contin Giacomo
- Contreras Nuno Jesus Guillermo
- Coquet Maurice
- Cortese Pietro
- Cosentino Mauro Rogerio
- Costa Filippo
- Costanza Susanna
- Cot Corentin
- Crkovska Jana
- Crochet Philippe
- Cruz Torres Reynier
- Cui Pengyao
- Czarnynoga Maciej Marek
- Czeslaw Miskowiec Dariusz
- Dainese Andrea
- Dange Gautam
- Danisch Meike Charlotte
- Danu Andrea
- Das Prottay
- Das Prottoy
- Das Supriya
- Dash Archita Rani
- Dash Sadhana
- de Caro Annalisa
- de Cataldo Giacinto
- de Cuveland Jan
- de Falco Alessandro
- de Gruttola Daniele
- de Leone Gay Maria Beatriz
- de Marco Nora
- de Martin Chiara
- de Melo Paulino Maria Monalisa
- de Moraes Canedo Fabio
- de Pasquale Salvatore
- Deb Rohaan
- del Grande Raffaele
- Dello Stritto Luigi
- Deng Wenjing
- Devereaux Kyle Christian
- Dhankher Preeti
- Di Bari Domenico
- Di Mauro Antonio
- Diab Batoul
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- Ding Yanchun
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- Divia Roberto
- Djuvsland Oeystein
- Dmitrieva Uliana
- Dobrigkeit Chinellato David
- Dobrin Alexandru Florin
- Dominguez Rosas Edgar
- Donigus Benjamin
- Duarte Galvan Carlos
- Dubinski Jan Michal
- Dubla Andrea
- Dupieux Pascal
- Dzalaiova Natalia
- Eder Tabea Maria
- Ehlers Raymond James
- Eisenhut Florian
- Ejima Ren
- El Mard Bouziani Youssef
- Elia Domenico
- Erazmus Barbara Ewa
- Ercolessi Francesca
- Espagnon Bruno
- Espinoza Beltran Lucina Gabriela
- Eulisse Giulio
- Evans David
- Evdokimov Sergey
- Fabbietti Laura
- Faggin Mattia
- Faivre Julien
- Fan Feng
- Fan Wenqing
- Fantoni Alessandra
- Fasel Markus
- Feliciello Alessandro
- Feofilov Grigorii
- Fernandez Tellez Arturo
- Ferrandi de Oliveira Lucas
- Ferrero Andrea
- Ferrero Chiara
- Ferretti Alessandro
- Feuillard Victor Jose Gaston
- Filova Vendulka
- Finogeev Dmitry
- Fionda Fiorella
- Fiorini da Silva Tiago
- Flatland Erlend
- Flor Fernando Antonio
- Flores Amanda Nicole
- Foertsch Siegfried Valentin
- Fokin Ilya
- Fokin Sergey
- Follo Umberto
- Fragiacomo Enrico
- Frajna Eszter
- Fuchs Ulrich
- Funicello Nicola
- Furget Christophe
- Furs Artur
- Fusayasu Takahiro
- Gaardhoeje Jens Joergen
- Gagliardi Martino
- Gago Medina Alberto Martin
- Gahlaut Tanu
- Gameiro Munhoz Marcelo
- Gangadharan Dhevan Raja
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- Gautam Amrit
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- Ghosh Chandrasekhar
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- Glaenzer Aude Marie Camille
- Glassel Peter
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- Gonzalez Sebastian Victor Luis
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- Graczykowski Lukasz Kamil
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- Grigoras Costin
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- Grigoryev Vladislav
- Grosa Fabrizio
- Grosse-Oetringhaus Jan Fiete
- Grosso Raffaele
- Gruenwald Nadine Alice
- Grund David
- Guernane Rachid
- Guilbaud Maxime Rene Joseph
- Gulbrandsen Kristjan Herlache
- Gundem Tuba
- Gunji Taku
- Guo Wenda
- Gupta Anik
- Gupta Ramni
- Gupta Rashi
- Gwizdziel Katarzyna
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- Hachiya Shimomura Maya
- Hadjidakis Cynthia Marie
- Haider Fakhar Ul
- Haidlova Sara
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- Hamagaki Hideki
- Hamdi Abdennacer
- Han Younghoon
- Hanley Brian Gerald
- Hannigan Ryan Patrick
- Hansen Joachim
- Haque Md Rihan
- Harris John William
- Harton Austin Vincent
- Hartung Michael Volker
- Hassan Hadi
- Hatzifotiadou Despina
- Hauer Philip
- Haugland Solheim Emilie
- Havener Laura Brittany
- Hellbar Ernst
- Helstrup Haavard
- Hemmer Marvin
- Herman Tomas
- Hernandez Sabrina Gabrielle
- Herrera Corral Gerardo Antonio
- Herrmann Sarah Nina Edwige
- Hetland Kristin Fanebust
- Heybeck Benedict
- Hillemanns Hartmut
- Hippolyte Boris
- Hoffmann Felix Willi
- Hofman Bas
- Hong Geun Hee
- Horst Maximilian
- Horzyk Adrian
- Hou Yongzhen
- Hristov Peter Zahariev
- Huhn Patrick
- Huhta Laura Maria
- Humanic Thomas
- Hutson Alek
- Hutter Dirk
- Hwang Minyoung Chris
- Ilkaev Radiy
- Inaba Motoi
- Innocenti Gian Michele
- Ippolitov Mikhail
- Isakov Artem
- Isidori Tommaso
- Islam Md Samsul
- Iurchenko Semen
- Ivanov Marian
- Ivanov Marian
- Ivanov Vladimir
- Iversen Kaare Endrup
- Jablonski Miroslaw
- Jacak Barbara
- Jacazio Nicolo
- Jacobs Peter Martin
- Jadlovska Slavka
- Jadlovsky Jan
- Jaelani Syaefudin
- Jahnke Cristiane
- Jakubcinova Zuzana
- Jakubowska Monika Joanna
- Janik Malgorzata Anna
- Janson Thomas
- Ji Su-Jeong
- Jia Shihai
- Jonas Florian
- Jones Daniel Matthew
- Jowett John
- Jung Jerome
- Jung Michael
- Junique Antoine Jean-Simon
- Jusko Anton
- Kaewjai Jetnipit
- Kalinak Peter
- Kalweit Alexander Philipp
- Karasu Uysal Ayben
- Karatovic David
- Karatzenis Nikolaos
- Karavichev Oleg
- Karavicheva Tatiana
- Karlsson Gumprecht Jesper Jan Walter
- Karpechev Evgeny
- Karwowska Maja Jadwiga
- Kebschull Udo Wolfgang
- Keidel Ralf
- Keil Markus
- Ketzer Bernhard Franz
- Khade Swapnesh Santosh
- Khan Ahsan Mehmood
- Khan Mohammed Mohisin
- Khan Shaista
- Khanzadeev Alexei
- Kharlov Yury
- Khatun Anisa
- Khuntia Arvind
- Khuranova Zhanna
- Kileng Bjarte
- Kim Beomkyu
- Kim Chong
- Kim Dong Jo
- Kim Eun Joo
- Kim Jaehyun
- Kim Jiyoung
- Kim Junlee
- Kim Minjung
- Kim Se Yong
- Kim Taejun
- Kimura Kento
- Kirkova Aleksandrina
- Kirsch Stefan
- Kisel Ivan
- Kiselev Sergey
- Kisiel Adam Ryszard
- Kitowski Jacek Pawel
- Klay Jennifer Lynn
- Klein Jochen
- Klein Spencer Robert
- Klein-Boesing Christian
- Kleiner Matthias
- Klemenz Thomas
- Kluge Alexander
- Kobdaj Chinorat
- Kohara Ryotaro
- Kollegger Thorsten Sven
- Kondratyev Andrey
- Kondratyeva Natalia
- Konig Joshua Leon
- Konigstorfer Stephan Alexander
- Konopka Piotr Jan
- Kornakov Van Georgui
- Korwieser Maximilian
- Koryciak Sebastian Dominik
- Koster Cornelia
- Kotliarov Artem
- Kovacic Nino
- Kovalenko Vladimir
- Kowalski Marek
- Kozhuharov Venelin Valeriev
- Kralik Ivan
- Kravcakova Adela
- Krcal Lubos
- Krivda Marian
- Krizek Filip
- Krizkova Gajdosova Katarina
- Krug Cristiano
- Kruger Mario
- Krupova Diana Maria
- Kryshen Evgeny
- Kucera Vit
- Kuhn Christian Claude
- Kuijer Paulus Gerardus
- Kumaoka Takuya
- Kumar Deekshit
- Kumar Lokesh
- Kumar Navneet
- Kumar Shyam
- Kundu Sourav
- Kurashvili Podist
- Kurepin Alexander
- Kurepin Alexey
- Kuryakin Alexey
- Kushpil Svetlana
- Kuskov Vladislav
- Kutyla Monika
- Kweon Min Jung
- Kwon Youngil
- La Pointe Sarah Louise
- La Rocca Paola
- Lafuente Mazuecos Antonio
- Lakrathok Anantachai
- Lamanna Massimo
- Landou Aimeric Robin
- Langoy Rune
- Larionov Pavel
- Laudi Elisa
- Lautner Lukas
- Lavicka Roman
- Lea Ramona
- Lee Hyungjun
- Legrand Iosif-Charles
- Legras Gauthier
- Lehrbach Johannes
- Lelek Tomasz Marcin
- Lemmon Roy Crawford
- Leon Monzon Ildefonso
- Lesch Marcel Markus
- Lesser Ezra Douglas
- Levai Peter
- Li Mingze
- Li Xiaomei
- Liang-Gilman Beatrice Eva
- Lien Jorgen Andre
- Lietava Roman
- Likmeta Iris
- Lim Bong-Hwi
- Lim Sanghoon
- Lindenstruth Volker
- Lindner Amelia
- Lippmann Christian
- Liu Donghai
- Liu Jian
- Loizides Constantinos
- Lokos Sandor
- Lomker Johanna
- Lopez Torres Ernesto
- Lopez Xavier Bernard
- Lu Pengzhong
- Lugo Fabiola Viridiana
- Luhder Jens Robert
- Lunardon Marcello
- Luparello Grazia
- Ma Yugang
- Mager Magnus
- Maire Antonin
- Majerz Emilia Maria
- Makariev Martin Vasilev
- Malaev Mikhail
- Malfattore Giovanni
- Malik Nasir Mehdi
- Malik Qasim Waheed
- Malik Salman Khurshid
- Malinina Liudmila
- Mallick Dukhishyam
- Mallick Neelkamal
- Mandaglio Giuseppe
- Mandal Sushobhan Kumar
- Manea Alexandru
- Manko Vladislav
- Manso Franck
- Mantovani Sarti Valentina
- Manzari Vito
- Mao Yaxian
- Marcjan Robert Waclaw
- Margagliotti Giacomo Vito
- Margotti Anselmo
- Marin Ana Maria
- Markert Christina
- Martinengo Paolo
- Martinez Garcia Josue
- Martinez Hernandez Mario Ivan
- Martinez-Garcia Gines
- Martins Campos Almeida Arneiro Jhoao Gabriel
- Martins Palhares Maria Paula
- Masciocchi Silvia
- Masera Massimo
- Masoni Alberto
- Massacrier Laure Marie
- Massen Olaf
- Mastroserio Annalisa
- Matonoha Oliver
- Mattiazzo Serena
- Matyja Adam Tomasz
- Mazzaschi Francesco
- Mazzilli Marianna
- Mckibben Lofnes Ingrid
- Mdhluli Joyful Elma
- Mejia Camacho Juan Manuel
- Melikyan Yury
- Menchaca-Rocha Arturo Alejandro
- Meninno Elisa
- Menzel Marius Wilm
- Meres Michal
- Mesa Perez Guillermo
- Miake Yasuo
- Micheletti Luca
- Mihaylov Dimitar Lubomirov
- Mikhaylov Konstantin
- Minafra Nicola
- Modak Abhi
- Mohanty Bedangadas
- Molander Mikael Andreas
- Monira Shirajum
- Mordasini Cindy
- Moreira de Godoy Willems Denise Aparecida
- Morozov Igor
- Morsch Andreas
- Mrnjavac Teo
- Muccifora Valeria
- Muhuri Sanjib
- Mulligan James Declan
- Mulliri Alice
- Munoz Mendez Jesus Eduardo
- Munzer Robert Helmut
- Murakami Hikari
- Murray Sean
- Musa Luciano
- Musinsky Jan
- Myrcha Julian Wojciech
- Naik Bharati
- Nambrath Anjali Ila
- Nandi Basanta Kumar
- Nania Rosario
- Nappi Eugenio
- Narcio Laveaga Rafael Angel
- Nassirpour Adrian Fereydon
- Nath Abhishek
- Nattrass Christine
- Naydenov Momchil Nikolaev
- Neagu Alexandra
- Negru Adrian-Eduard
- Nekrasova Evgeniia
- Nellen Lukas
- Nepeivoda Roman
- Nese Sigurd
- Neskovic Gvozden
- Nicassio Nicola
- Nielsen Borge Svane
- Nielsen Emil Gorm
- Nikolaev Sergey
- Nikulin Sergey
- Nikulin Vladimir
- Noferini Francesco
- Noh Seoyoung
- Nomokonov Petr
- Norman Jaime
- Novitzky Norbert
- Nowakowski Piotr
- Nyanin Alexander
- Nystrand Joakim Ingemar
- Oh Saehanseul
- Ohlson Alice Elisabeth
- Okorokov Vitaly
- Oleniacz Janusz
- Onnerstad Anna
- Oppedisano Chiara
- Ortiz Velasquez Antonio
- Otwinowski Jacek Tomasz
- Oya Motomi
- Oyama Ken
- Pachmayer Yvonne Chiara
- Padhan Sonali
- Pagano Davide
- Paic Guy
- Paisano Guzman Sergio
- Palasciano Antonio
- Panebianco Stefano
- Panikkassery Salvan Malavika
- Park Hanseo
- Park Hyebin
- Park Jonghan
- Parkkila Jasper Elias
- Patley Yash
- Paul Biswarup
- Paz Jimenez Alom Antonio
- Pei Hua
- Peitzmann Thomas
- Peng Xinye
- Pennisi Michele
- Perciballi Stefania
- Peresunko Dmitry Yurevich
- Pestov Yury
- Petersen Mikkel Tornhoj
- Petrov Vitalii
- Petrovici Mihai
- Piano Stefano
- Pikna Miroslav
- Pillot Philippe
- Pinazza Ombretta
- Pinsky Lawrence
- Pinto Chiara
- Pisano Silvia
- Planinic Mirko
- Pliatskas Stylianidis Christos
- Pliquett Fabian
- Ploskon Mateusz Andrzej
- Poghosyan Martin
- Polishchuk Boris
- Politano Stefano
- Poljak Nikola
- Pop Amalia
- Porteboeuf Sarah Julie
- Pozdniakov Valerii
- Pradhan Kshitish Kumar
- Prasad Sidharth Kumar
- Prasad Suraj
- Preghenella Roberto
- Prino Francesco
- Pruneau Claude Andre
- Pshenichnov Igor
- Puccio Maximiliano
- Pucillo Sara
- Qiu Shi
- Quaglia Luca
- Ragoni Simone
- Rai Ananya
- Rakotozafindrabe Andry Malala
- Ramello Luciano
- Rami Fouad
- Ramillien Barret Valerie
- Rasa Marika
- Rasanen Sami Sakari
- Rath Rutuparna
- Rauch Max Philip
- Ravasenga Ivan
- Read Kenneth Francis
- Reckziegel Christian
- Redelbach Andreas Ralph
- Redlich Krzysztof
- Reetz Carolina Anna
- Regules Medel Hector David
- Rehman Attiq Ur
- Reidt Felix
- Reme-Ness Haakon Andre
- Reygers Klaus Johannes
- Riabov Andrei
- Riabov Viktor
- Ricci Riccardo
- Richter Matthias Rudolph
- Riedel Anton Albert
- Riegler Werner
- Riffero Andrea Giovanni
- Ripoli Cristina
- Ristea Catalin-Lucian
- Rodriguez Cahuantzi Mario
- Rodriguez Ramirez Saul Anibal
- Roeed Ketil
- Roehrich Dieter
- Rogalev Roman
- Rogochaya Elena
- Rogoschinski Tim Sebastian
- Rohr David Michael
- Rojas Torres Solangel
- Rokita Przemyslaw Stefan
- Romanenko Gleb
- Ronchetti Federico
- Roslon Krystian
- Rossi Andrea
- Roy Ankhi
- Roy Subhadeep
- Rubini Nicola
- Rudolph Justus Arne
- Ruggiano Daniela
- Rui Rinaldo
- Russek Pawel Grzegorz
- Russo Roberto
- Rustamov Anar
- Ryabinkin Evgeny
- Ryabov Yury
- Rybicki Andrzej Krzysztof
- Ryu Jaehyeok
- Rzesa Wioleta
- Sadhu Samrangy
- Sadovskiy Sergey
- Saetre Jon-Are
- Safarik Karel
- Saha Sumit Kumar
- Saha Swati
- Sahoo Bhagyarathi
- Sahoo Raghunath
- Sahoo Sarita
- Sahu Dushmanta
- Sahu Pradip Kumar
- Saini Jogender
- Sakai Shingo
- Sambyal Sanjeev Singh
- Samitz Daniel
- Sanna Isabella
- Sarkar - Sinha Tinku
- Sarkar Debojit
- Sarma Pranjal
- Sarritzu Valerio
- Sas Mike
- Sasikumar Menon Anjaly
- Sawan Sawan
- Scapparone Eugenio
- Schambach Johann Joachim
- Scheid Horst Sebastian
- Schiaua Claudiu Cornel
- Schicker Rainer Martin
- Schlepper Felix
- Schmah Alexander
- Schmidt Christian Joachim
- Schmidt Hans Rudolf
- Schmidt Marten Ole
- Schmidt Martin
- Schmidt Nicolas
- Schmier Austin Robert
- Schotter Romain
- Schukraft Jurgen
- Schweda Kai Oliver
- Scioli Gilda
- Scomparin Enrico
- Seger Janet Elizabeth
- Sekiguchi Yuko
- Sekihata Daiki
- Selina Mariia
- Selyuzhenkov Ilya
- Senyukov Serhiy
- Seo Jin Joo
- Serebryakov Dmitry
- Serkin Leonid
- Serksnyte Laura
- Setoue Liveraro Gianni Shigeru
- Sevcenco Adrian
- Shaba Tebogo Joyce
- Shabetai Alexandre
- Shahoyan Ruben
- Shangaraev Artem
- Sharma Binti
- Sharma Deependra
- Sharma Himanshu
- Sharma Meenakshi
- Sharma Samarth
- Sharma Sheetal
- Sharma Upasana
- Shatat Afnan
- Sheibani Oveis
- Shigaki Kenta
- Shin Jaehyuck
- Shirinkin Sergey
- Shou Qiye
- Sibiryak Yury
- Siddhanta Sabyasachi
- Siemiarczuk Teodor
- Silvermyr David Olle Rickard
- Simantathammakul Tawanchat
- Simeonov Radoslav
- Singh Balwan
- Singh Bhawani
- Singh Kamaljeet
- Singh Ranbir
- Singh Randhir
- Singh Ravindra
- Singh Sweta
- Singh Vivek
- Singhal Vikas
- Sitar Branislav
- Sitta Mario
- Skaali Bernhard
- Skorodumovs Georgijs
- Smirnov Nikolai
- Snellings Raimond
- Song Jihye
- Sonnabend Christian
- Sonneveld Jorine
- Soramel Francesca
- Soto-Hernandez Analyce Bella
- Spijkers Rik
- Sputowska Iwona Anna
- Staa Joey
- Stachel Johanna
- Stan Ionel
- Steffanic Patrick John
- Stiefelmaier Stephan Friedrich
- Stocco Diego
- Storehaug Ida
- Strangmann Nicolas Justus
- Stratmann Peter
- Strazzi Sofia
- Sturniolo Alessandro
- Suire Christophe Pierre
- Sukhanov Mikhail
- Suljic Miljenko
- Sultanov Rishat
- Sumberia Vikash
- Sumowidagdo Suharyo
- Szarka Imrich
- Szymkowski Maciej
- Taghavi Seyed Farid
- Taillepied Guillaume
- Takahashi Jun
- Tambave Ganesh Jagannath
- Tang Siyu
- Tang Zebo
- Tapia Takaki Daniel Jesus
- Tapus Nicolae
- Tarasovicova Lucia Anna
- Tarzila Madalina-Gabriela
- Tassielli Giovanni Francesco
- Tauro Arturo
- Tavira Garcia Andrea
- Tejeda Munoz Guillermo
- Telesca Adriana
- Terlizzi Livia
- Terrevoli Cristina
- Thakur Sanchari
- Thomas Deepa
- Tikhonov Anatoly
- Tiltmann Nicolas
- Timmins Anthony Robert
- Tkacik Milan
- Tkacik Tomas
- Toia Alberica
- Tokumoto Ryoka
- Tomassini Sofia
- Tomohiro Keisuke
- Topilskaya Nataliya
- Toppi Marco
- Tork Theraa
- Torres Cabrera Maria Fernanda
- Torres Ramos Arianna Grisel
- Trifiro Antonio
- Triloki Triloki
- Triolo Andrea Sofia
- Tripathy Sushanta
- Tripathy Tulika
- Tropp Klaudia
- Trubnikov Victor
- Trzaska Wladyslaw Henryk
- Trzcinski Tomasz Piotr
- Tsolanta Christina
- Tumkin Alexandr
- Turrisi Rosario
- Tveter Trine Spedstad
- Ullaland Kjetil
- Ulukutlu Berkin
- Uras Antonio
- Urioni Marta
- Usai Gianluca
- Vala Martin
- Valencia Torres Victor
- Valle Nicolo
- van Doremalen Lennart
- van Leeuwen Marco
- van Veen Casper Arie
- van Weelden Roelof Jan Gijs
- Vande Vyvre Pierre
- Varga Dezso
- Varga Zoltan
- Vargas Torres Paola
- Vasileiou Maria
- Vasiliev Andrey
- Vasquez Beltran Yael Antonio
- Vazquez Doce Oton
- Vazquez Rueda Omar
- Vechernin Vladimir
- Vercellin Ermanno
- Vergara Limon Sergio
- Verma Rahul
- Vermunt Lucas Anne
- Vertesi Robert
- Verweij Marta
- Vickovic Linda
- Vilakazi Zabulon
- Villalobos Baillie Orlando
- Villani Anna
- Vinogradov Alexander
- Viqueira Rodriguez Manuel
- Virgili Tiziano
- Virta Maxim Mikael Olavi
- Vislavicius Vytautas
- Vodopyanov Alexander
- Voelkel Benedikt
- Volkl Martin Andreas
- Voloshin Sergey
- Volpe Giacomo
- von Haller Barthelemy
- Vorobyev Ivan
- Vozniuk Nikita
- Vrlakova Janka
- Wan Jie
- Wang Chunzheng
- Wang Dongfang
- Wang Yuanzhe
- Wang Yubiao
- Wegrzynek Adam Tadeusz
- Weiglhofer Felix Thomas
- Wenzel Sandro Christian
- Wessels Johannes Peter
- Weyhmiller Sierra Lisa
- Wiechula Jens
- Wikne Jon
- Wilhelmi Alexander
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Willems Guido Alexander
- Windelband Bernd Stefan
- Winn Michael Andreas
- Wright Josephina Rae
- Wu Wenya
- Wu Yitao
- Xiong Zhenjun
- Xu Ran
- Yadav Ankur
- Yadav Arun Kumar
- Yamaguchi Yorito
- Yang Shiming
- Yano Satoshi
- Yeats Emma Rose
- Yin Zhongbao
- Yoo In Kwon
- Yoon Jin Hee
- Yoval Pozos Irandheny
- Yu Hyeonjin
- Yu Zhi
- Yuan Shiming
- Yuncu Alperen
- Zaccolo Valentina
- Zampolli Chiara
- Zanone Federica
- Zardoshti Nima
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zhalov Mikhail
- Zhang Biao
- Zhang Chi
- Zhang Liuyao
- Zhang Maolin
- Zhang Mingyu
- Zhang Song
- Zhang Xiaoming
- Zhang Yifei
- Zhang Zhen
- Zhao Mingrui
- Zherebchevskii Vladimir
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Senjie
- Zhu Ya
- Zugravel Stefan Cristi
- Zurlo Nicola
- Publication venue
- HAL CCSD
- Publication date
- 29/04/2024
- Field of study
International audienceThe inclusive production of the charm-strange baryon Ωc0 is measured for the first time via its semileptonic decay into Ω−e+νe at midrapidity (∣y∣<0.8) in proton−proton (pp) collisions at the centre-of-mass energy s=13 TeV with the ALICE detector at the LHC. The transverse momentum (pT) differential cross section multiplied by the branching ratio is presented in the interval 2<pT<12 GeV/c. The branching-fraction ratio BR(Ωc0→Ω−e+νe)/BR(Ωc0→Ω−π+) is measured to be 1.12 ± 0.22 (stat.) ± 0.27 (syst.). Comparisons with other experimental measurements, as well as with theoretical calculations, are presented
Systematic study of flow vector decorrelation in sNN=5.02 TeV Pb-Pb collisions
- Author
- Abranches de Carvalho Leopoldo
- Acharya Shreyasi
- Adamova Dagmar
- Agarwal Apar
- Aglieri Rinella Gianluca
- Aglietta Luca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- Akishina Valentina
- Al-Turany Mohammad
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Masud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Alici Andrea
- Alizadehvandchali Negin
- Alkin Anton
- Alme Johan
- Alocco Giacomo
- Alt Torsten
- Altamura Anna Rita
- Altsybeev Igor
- Alvarado Garcia Jesus Ricardo
- Amatriain Carballo Aitor
- Anaam Mustafa
- Andrei Cristian
- Andreou Nicodemos
- Andronic Anton
- Andronov Evgeny
- Anguelov Venelin
- Antinori Federico
- Antonioli Pietro
- Apadula Nicole
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Arata Carolina
- Arcelli Silvia
- Aresti Mauro
- Arnaldi Roberta
- Arsene Ionut Cristian
- Arslandok Mesut
- Arteche Diaz Raul
- Augustinus Andre
- Averbeck Ralf Peter
- Azmi Mohd Danish
- Baba Hitoshi
- Badala Angela
- Badaro Saramela Thiago
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- Baek Yongwook
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- Torres Cabrera Maria Fernanda
- Torres Ramos Arianna Grisel
- Trifiro Antonio
- Triolo Andrea Sofia
- Tripathy Sushanta
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- Trubnikov Victor
- Trzaska Wladyslaw Henryk
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- Voloshin Sergey
- Volpe Giacomo
- von Haller Barthelemy
- Vorobyev Ivan
- Vozniuk Nikita
- Vrlakova Janka
- Wan Jie
- Wang Chunzheng
- Wang Dongfang
- Wang Yuanzhe
- Wang Yubiao
- Wegrzynek Adam Tadeusz
- Weiglhofer Felix Thomas
- Wenzel Sandro Christian
- Wessels Johannes Peter
- Weyhmiller Sierra Lisa
- Wiechula Jens
- Wikne Jon
- Wilhelmi Alexander
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Willems Guido Alexander
- Windelband Bernd Stefan
- Winn Michael Andreas
- Wright Josephina Rae
- Wu Wenya
- Wu Yitao
- Xiong Zhenjun
- Xu Ran
- Yadav Ankur
- Yadav Arun Kumar
- Yamaguchi Yorito
- Yang Shiming
- Yano Satoshi
- Yeats Emma Rose
- Yin Zhongbao
- Yoo In Kwon
- Yoon Jin Hee
- Yoval Pozos Irandheny
- Yu Hyeonjin
- Yu Zhi
- Yuan Shiming
- Yuncu Alperen
- Zaccolo Valentina
- Zampolli Chiara
- Zanone Federica
- Zardoshti Nima
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zhalov Mikhail
- Zhang Biao
- Zhang Chi
- Zhang Liuyao
- Zhang Maolin
- Zhang Mingyu
- Zhang Song
- Zhang Xiaoming
- Zhang Yifei
- Zhang Zhen
- Zhao Mingrui
- Zherebchevskii Vladimir
- Zhong Chen
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Senjie
- Zhu Ya
- Zugravel Stefan Cristi
- Zurlo Nicola
- Publication venue
- HAL CCSD
- Publication date
- 26/03/2024
- Field of study
International audienceMeasurements of the pT-dependent flow vector fluctuations in Pb-Pb collisions at sNN=5.02 TeV using azimuthal correlations with the ALICE experiment at the LHC are presented. A four-particle correlation approach [1] is used to quantify the effects of flow angle and magnitude fluctuations separately. This paper extends previous studies to additional centrality intervals and provides measurements of the pT-dependent flow vector fluctuations at sNN=5.02 TeV with two-particle correlations. Significant pT-dependent fluctuations of the V2 flow vector in Pb-Pb collisions are found across different centrality ranges, with the largest fluctuations of up to ∼15% being present in the 5% most central collisions. In parallel, no evidence of significant pT-dependent fluctuations of V3 or V4 is found. Additionally, evidence of flow angle and magnitude fluctuations is observed with more than 5σ significance in central collisions. These observations in Pb-Pb collisions indicate where the classical picture of hydrodynamic modeling with a common symmetry plane breaks down. This has implications for hard probes at high pT, which might be biased by pT-dependent flow angle fluctuations of at least 23% in central collisions. Given the presented results, existing theoretical models should be re-examined to improve our understanding of initial conditions, quark--gluon plasma (QGP) properties, and the dynamic evolution of the created system
Studying the interaction between charm and light-flavor mesons
- Author
- Abranches De Carvalho Leopoldo
- Acharya Shreyasi
- Adamova Dagmar
- Aglieri Rinella Gianluca
- Aglietta Luca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- Akishina Valentina
- Al-turany Mohammad
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Masud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Alici Andrea
- Alizadehvandchali Negin
- Alkin Anton
- Alme Johan
- Alocco Giacomo
- Alt Torsten
- Altamura Anna Rita
- Altsybeev Igor
- Alvarado Garcia Jesus Ricardo
- Amatriain Carballo Aitor
- Anaam Mustafa
- Andrei Cristian
- Andreou Nicodemos
- Andronic Anton
- Andronov Evgeny
- Anguelov Venelin
- Antinori Federico
- Antonioli Pietro
- Apadula Nicole
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Arata Carolina
- Arcelli Silvia
- Aresti Mauro
- Arnaldi Roberta
- Arsene Ionut Cristian
- Arslandok Mesut
- Arteche Diaz Raul
- Augustinus Andre
- Averbeck Ralf Peter
- Azmi Mohd Danish
- Baba Hitoshi
- Badala Angela
- Badaro Saramela Thiago
- Bae Joonsuk
- Baek Yongwook
- Bai Xiaozhi
- Bailhache Raphaelle Marie
- Bailung Yoshini
- Bala Renu
- Balbino Alessandro
- Baldisseri Alberto
- Balis Bartosz
- Banerjee Debjani
- Banoo Zarina
- Barile Francesco
- Barioglio Luca
- Barlou Maria
- Barman Banajit
- Barnafoldi Gergely Gabor
- Barnby Lee Stuart
- Barreau Emilie Martine
- Barreto De Oliveira Campos Leonardo
- Bartels Clara
- Barth Klaus
- Bartsch Esther
- Bastid Nicole
- Basu Sumit
- Batigne Guillaume
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- Wu Yitao
- Xu Ran
- Yadav Ankur
- Yadav Arun Kumar
- Yamaguchi Yorito
- Yang Shiming
- Yano Satoshi
- Yeats Emma Rose
- Yin Zhongbao
- Yoo In Kwon
- Yoon Jin Hee
- Yoval Pozos Irandheny
- Yu Hyeonjin
- Yu Zhi
- Yuan Shiming
- Yuncu Alperen
- Zaccolo Valentina
- Zampolli Chiara
- Zanone Federica
- Zardoshti Nima
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zhalov Mikhail
- Zhang Biao
- Zhang Chi
- Zhang Liuyao
- Zhang Mingyu
- Zhang Song
- Zhang Xiaoming
- Zhang Yifei
- Zhang Zhen
- Zhao Mingrui
- Zherebchevskii Vladimir
- Zhong Chen
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Ya
- Zugravel Stefan Cristi
- Zurlo Nicola
- Publication venue
- Publication date
- 19/01/2024
- Field of study
The two-particle momentum correlation functions between charm mesons (D∗± and D±) and charged light-flavor mesons (π± and K±) in all charge-combinations are measured for the first time by the ALICE Collaboration in high-multiplicity proton-proton collisions at a center-of-mass energy of s=13 TeV. For DK and D∗K pairs, the experimental results are in agreement with theoretical predictions of the residual strong interaction based on quantum chromodynamics calculations on the lattice and chiral effective field theory. In the case of Dπ and D∗π pairs, a tension between the calculations including strong interactions and the measurement is observed. For all particle pairs, the data can be adequately described by Coulomb interaction only, indicating a shallow interaction between charm and light-flavor mesons. Finally, the scattering lengths governing the residual strong interaction of the Dπ and D∗π systems are determined by fitting the experimental correlation functions with a model that employs a Gaussian potential. The extracted values are small and compatible with zero.The two-particle momentum correlation functions between charm mesons (D∗± and D±) and charged light-flavor mesons (π± and K±) in all charge-combinations are measured for the first time by the ALICE Collaboration in high-multiplicity proton-proton collisions at a center-of-mass energy of s=13 TeV. For DK and D∗K pairs, the experimental results are in agreement with theoretical predictions of the residual strong interaction based on quantum chromodynamics calculations on the lattice and chiral effective field theory. In the case of Dπ and D∗π pairs, tension between the calculations including strong interactions and the measurement is observed. For all particle pairs, the data can be adequately described by Coulomb interaction only, indicating a shallow interaction between charm and light-flavor mesons. Finally, the scattering lengths governing the residual strong interaction of the Dπ and D∗π systems are determined by fitting the experimental correlation functions with a model that employs a Gaussian potential. The extracted values are small and compatible with zero
Studying the interaction between charm and light-flavor mesons
- Author
- Abranches de Carvalho Leopoldo
- Acharya Shreyasi
- Adamova Dagmar
- Aglieri Rinella Gianluca
- Aglietta Luca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- Akishina Valentina
- Al-Turany Mohammad
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Masud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Alici Andrea
- Alizadehvandchali Negin
- Alkin Anton
- Alme Johan
- Alocco Giacomo
- Alt Torsten
- Altamura Anna Rita
- Altsybeev Igor
- Alvarado Garcia Jesus Ricardo
- Amatriain Carballo Aitor
- Anaam Mustafa
- Andrei Cristian
- Andreou Nicodemos
- Andronic Anton
- Andronov Evgeny
- Anguelov Venelin
- Antinori Federico
- Antonioli Pietro
- Apadula Nicole
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Arata Carolina
- Arcelli Silvia
- Aresti Mauro
- Arnaldi Roberta
- Arsene Ionut Cristian
- Arslandok Mesut
- Arteche Diaz Raul
- Augustinus Andre
- Averbeck Ralf Peter
- Azmi Mohd Danish
- Baba Hitoshi
- Badala Angela
- Badaro Saramela Thiago
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- Baek Yongwook
- Bai Xiaozhi
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- Wegrzynek Adam Tadeusz
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- Wilhelmi Alexander
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- Willems Guido Alexander
- Windelband Bernd Stefan
- Winn Michael Andreas
- Wright Josephina Rae
- Wu Wenya
- Wu Yitao
- Xu Ran
- Yadav Ankur
- Yadav Arun Kumar
- Yamaguchi Yorito
- Yang Shiming
- Yano Satoshi
- Yeats Emma Rose
- Yin Zhongbao
- Yoo In Kwon
- Yoon Jin Hee
- Yoval Pozos Irandheny
- Yu Hyeonjin
- Yu Zhi
- Yuan Shiming
- Yuncu Alperen
- Zaccolo Valentina
- Zampolli Chiara
- Zanone Federica
- Zardoshti Nima
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zhalov Mikhail
- Zhang Biao
- Zhang Chi
- Zhang Liuyao
- Zhang Mingyu
- Zhang Song
- Zhang Xiaoming
- Zhang Yifei
- Zhang Zhen
- Zhao Mingrui
- Zherebchevskii Vladimir
- Zhong Chen
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Ya
- Zugravel Stefan Cristi
- Zurlo Nicola
- Publication venue
- HAL CCSD
- Publication date
- 30/01/2024
- Field of study
International audienceThe two-particle momentum correlation functions between charm mesons (D∗± and D±) and charged light-flavor mesons (π± and K±) in all charge-combinations are measured for the first time by the ALICE Collaboration in high-multiplicity proton-proton collisions at a center-of-mass energy of s=13 TeV. For DK and D∗K pairs, the experimental results are in agreement with theoretical predictions of the residual strong interaction based on quantum chromodynamics calculations on the lattice and chiral effective field theory. In the case of Dπ and D∗π pairs, tension between the calculations including strong interactions and the measurement is observed. For all particle pairs, the data can be adequately described by Coulomb interaction only, indicating a shallow interaction between charm and light-flavor mesons. Finally, the scattering lengths governing the residual strong interaction of the Dπ and D∗π systems are determined by fitting the experimental correlation functions with a model that employs a Gaussian potential. The extracted values are small and compatible with zero
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