378 research outputs found
A study of the properties and development in technology for obtaining multi-component systems of particle reinforced aluminum and titanium alloys
- Publication venue
- Politechnika Częstochowska
- Publication date
- 01/01/2022
- Field of study
The article analyzes the groundwork on the influence of alloying contaminants on the structure and mechanical properties of aluminum alloys. Aluminum has become widely used in various parts of machine-building due to its physical properties. However, the main task of modern material science is to increase the strength of aluminum alloys. Therefore, today there is the development of materials and alloys based on aluminum with alloying constituents (copper, silicon, magnesium, zinc, mangan), which are administered in aluminum mainly to increase its strength. Especially attractive are properties of aluminum-doped by transition metals, in particular scandium, zirconium, iron, etc. Finally, conclusions are drawn in order to develop a material based on aluminum with increased hardness, durability, and crack resistance
The first in-beam reaction measurement at CRYRING@ESR using the CARME array
- Author
- Andelkovic Zoran
- Bruno Carlo G.
- Bräuning-Demian Angela
- Chen Rui-Jui
- Davinson Thomas
- Dellmann Sophia F.
- Erbacher Phillip
- Fedotova Svetlana
- Forstner Oliver
- Freire-Fernandez David
- Glorius Jan
- Gumberidze Alexandre
- Hall Oscar
- Herfurth Frank
- Hillenbrand Pierre-Michel
- Hudson-Chang George
- Kalinin Anton
- Lestinsky Michael
- Litvinov Yuri A.
- Marsh Jordan J.
- Menz Esther B.
- Nociforo Chiara
- Petridis Nikolaos
- Psaltis Athanasios
- Sanjari Shahab
- Selina Mariia
- Sidhu Ragandeep S.
- Spillman Uwe
- Stöhlker Thomas
- Varga Laszlo
- Vorobjev Gleb
- Woods Philip J.
- Publication venue
- Springer
- Publication date
- 01/01/2024
- Field of study
In the last decade nuclear reaction measurements using heavy ion storage rings became an important tool for nuclear astrophysics studies. The new CRYRING Array for Reaction MEasurements (CARME), recently commissioned at the low energy CRYRING@ESR storage ring (GSI/FAIR), is designed to take this novel approach one step further and perform direct nuclear reaction measurements at stellar energies, as well as indirect studies of nuclear properties of interest for nuclear astrophysics. CRYRING is unique worldwide in being able to store high quality, isotopically pure, radioactive beams produced in-flight at the low energies required for nuclear astrophysics. This paper describes the first in-beam reaction measurement with CARME at CRYRING, the first beam on (conventional) target measurement for FAIR Phase-0, and the data analysis approach required by this unprecedented, unique experimental approach
Time performance of Analog Pixel Test Structures with in-chip operational amplifier implemented in 65 nm CMOS imaging process
- Author
- Aglietta Luca
- Antonelli Matias
- Barile Francesco
- Benotto Franco
- Beolè Stefania Maria
- Botta Elena
- Bruno Giuseppe Eugenio
- Carnesecchi Francesca
- Colella Domenico
- Colelli Angelo
- Contin Giacomo
- de Robertis Giuseppe
- Dumitrache Florina
- Elia Domenico
- Ferrero Chiara
- Fransen Martin
- Kluge Alex
- Kumar Shyam
- Lemoine Corentin
- Licciulli Francesco
- Lim Bong-Hwi
- Loddo Flavio
- Mager Magnus
- Marras Davide
- Martinengo Paolo
- Pastore Cosimo
- Patra Rajendra Nath
- Perciballi Stefania
- Piro Francesco
- Prino Francesco
- Ramello Luciano
- Ramos Arianna Grisel Torres
- Reidt Felix
- Rinella Gianluca Aglieri
- Russo Roberto
- Sarritzu Valerio
- Savino Umberto
- Schledewitz David
- Selina Mariia
- Senyukov Serhiy
- Sitta Mario
- Snoeys Walter
- Sonneveld Jory
- Suljic Miljenko
- Triloki Triloki
- Turcato Andrea
- Publication venue
- HAL CCSD
- Publication date
- 07/08/2024
- Field of study
International audienceIn the context of the CERN EP R&D on monolithic sensors and the ALICE ITS3 upgrade, the Tower Partners Semiconductor Co (TPSCo) 65 nm process has been qualified for use in high energy physics, and adopted for the ALICE ITS3 upgrade. An Analog Pixel Test Structure (APTS) featuring fast per pixel operational-amplifier-based buffering for a small matrix of four by four pixels, with a sensor with a small collection electrode and a very non-uniform electric field, was designed to allow detailed characterization of the pixel performance in this technology. Several variants of this chip with different pixel designs have been characterized with a (120 GeV/c) positive hadron beam. This result indicates that the APTS-OA prototype variants with the best performance achieve a time resolution of 63 ps with a detection efficiency exceeding 99% and a spatial resolution of 2 μm, highlighting the potential of TPSCo 65nm CMOS imaging technology for high-energy physics and other fields requiring precise time measurement, high detection efficiency, and excellent spatial resolution
Time performance of Analog Pixel Test Structures with in-chip operational amplifier implemented in 65 nm CMOS imaging process
- Author
- Aglietta Luca
- Antonelli Matias
- Barile Francesco
- Benotto Franco
- Beolè Stefania Maria
- Botta Elena
- Bruno Giuseppe Eugenio
- Carnesecchi Francesca
- Colella Domenico
- Colelli Angelo
- Contin Giacomo
- De Robertis Giuseppe
- Dumitrache Florina
- Elia Domenico
- Ferrero Chiara
- Fransen Martin
- Kluge Alex
- Kumar Shyam
- Lemoine Corentin
- Licciulli Francesco
- Lim Bong-Hwi
- Loddo Flavio
- Mager Magnus
- Marras Davide
- Martinengo Paolo
- Pastore Cosimo
- Patra Rajendra Nath
- Perciballi Stefania
- Piro Francesco
- Prino Francesco
- Ramello Luciano
- Ramos Arianna Grisel Torres
- Reidt Felix
- Rinella Gianluca Aglieri
- Russo Roberto
- Sarritzu Valerio
- Savino Umberto
- Schledewitz David
- Selina Mariia
- Senyukov Serhiy
- Sitta Mario
- Snoeys Walter
- Sonneveld Jory
- Suljic Miljenko
- Triloki Triloki
- Turcato Andrea
- Publication venue
- Publication date
- 26/07/2024
- Field of study
In the context of the CERN EP R&D on monolithic sensors and the ALICE ITS3 upgrade, the Tower Partners Semiconductor Co (TPSCo) 65 nm process has been qualified for use in high energy physics, and adopted for the ALICE ITS3 upgrade. An Analog Pixel Test Structure (APTS) featuring fast per pixel operational-amplifier-based buffering for a small matrix of four by four pixels, with a sensor with a small collection electrode and a very non-uniform electric field, was designed to allow detailed characterization of the pixel performance in this technology. Several variants of this chip with different pixel designs have been characterized with a (120 GeV/c) positive hadron beam. This result indicates that the APTS-OA prototype variants with the best performance achieve a time resolution of 63 ps with a detection efficiency exceeding 99% and a spatial resolution of 2 μm, highlighting the potential of TPSCo 65nm CMOS imaging technology for high-energy physics and other fields requiring precise time measurement, high detection efficiency, and excellent spatial resolution
Probing the Chiral Magnetic Wave with charge-dependent flow measurements in Pb-Pb collisions at the LHC
- Author
- Abranches de Carvalho Leopoldo
- Acharya Shreyasi
- Adamova Dagmar
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- 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
- 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
- Balbino Alessandro
- Baldisseri Alberto
- Balis Bartosz
- Banerjee Debjani
- Banoo Zarina
- Barbera Roberto
- Barile Francesco
- Barioglio Luca
- Barlou Maria
- Barman Banajit
- Barnafoldi Gergely Gabor
- Barnby Lee Stuart
- 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
- Beole Stefania Maria
- Berdnikov Yaroslav
- Berdnikova Anastasia
- Bergmann Luisa
- Bertran Ferrer Marta
- Besoiu Mihaela Gabriela
- Betev Latchezar
- Bhaduri Partha Pratim
- Bhasin Anju
- Bhat Mohammad Asif
- Bhattacharjee Buddhadeb
- Bianchi Livio
- Bianchi Nicola
- Bielcik Jaroslav
- Bielcikova Jana
- Biernat Jacek Bogumil
- 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
- Bogdanov Alexey
- Boi Stefano
- 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
- Cai Mengke
- Caines Helen Louise
- Caliva Alberto
- Calvo Villar Ernesto
- Camerini Paolo
- Carabas Mihai
- Carnesecchi Francesca
- Caron Robin Albert Andre
- Castillo Castellanos Javier Ernesto
- Catalano Fabio
- Ceballos Sanchez Cesar
- Chakaberia Irakli
- Chakraborty Pritam
- Chandra Sinjini
- Chapeland Sylvain
- Chartier Marielle
- Chattopadhyay Subhasis
- Chattopadhyay Sukalyan
- Cheng Tiantian
- Cheshkov Cvetan Valeriev
- Cheynis Brigitte
- Chibante Barroso Vasco Miguel
- Chizzali Emma Sophia
- Cho Jaeyoon
- Cho Soyeon
- Chochula Peter
- Choudhury Dhrubajyoti
- Christakoglou Panagiotis
- Christensen Christian Holm
- Christiansen Peter
- Chujo Tatsuya
- Ciacco Mario
- Cicalo Corrado
- Cindolo Federico
- 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 Louis
- Cortese Pietro
- Cosentino Mauro Rogerio
- Costa Filippo
- Costanza Susanna
- Cot Corentin
- Crkovska Jana
- Crochet Philippe
- Cruz Torres Reynier
- Cui Pengyao
- Czeslaw Miskowiec Dariusz
- Dainese Andrea
- 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 Moraes Canedo Fabio
- de Pasquale Salvatore
- Deb Rohaan
- del Grande Raffaele
- Dello Stritto Luigi
- Deng Wenjing
- Dhankher Preeti
- Di Bari Domenico
- Di Mauro Antonio
- Diab Batoul
- Dietel Thomas
- Ding Yanchun
- Ditzel Janik
- Divia Roberto
- Dixit Dhruv Utpalkumar
- Djuvsland Oeystein
- Dmitrieva Uliana
- Dobrigkeit Chinellato David
- Dobrin Alexandru Florin
- Dominguez Rosas Edgar
- Donigus Benjamin
- Duarte Galvan Carlos
- Dubinski Jan Michal
- Dubla Andrea
- Dudi Sandeep
- Dupieux Pascal
- Durkac Martin
- 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
- 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
- Fierro Rojas Pablo
- Filova Vendulka
- Finogeev Dmitry
- Fionda Fiorella
- Fiorini da Silva Tiago
- Flatland Erlend
- Flor Fernando Antonio
- Flores Amanda Nicole
- Foertsch Siegfried Valentin
- Fokin Ilya
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- Fragiacomo Enrico
- Frajna Eszter
- Fuchs Ulrich
- Funicello Nicola
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- Furs Artur
- Fusayasu Takahiro
- Gaardhoeje Jens Joergen
- Gagliardi Martino
- Gago Medina Alberto Martin
- Gahlaut Tanu
- Gameiro Munhoz Marcelo
- Gangadharan Dhevan Raja
- Ganoti Paraskevi
- Garabatos Cuadrado Jose Maria
- Garcia Chavez Tonatiuh
- Garcia Guardiano Gabriel
- Garcia-Solis Edmundo Javier
- Gargiulo Corrado
- Gasik Piotr Jan
- Gautam Amrit
- Germain Marie
- Ghimouz Abderrahmane
- Ghosh Chandrasekhar
- Giacalone Marco
- Gioachin Giulia
- Giubellino Paolo
- Giubilato Piero
- Glaenzer Aude Marie Camille
- Glassel Peter
- Glimos Ewa
- Goh Daniel Jia Qin
- Gonzalez Sebastian Victor Luis
- Gordeev Pavel
- Gorgon Marek Boguslaw
- Goswami Kangkan
- Gotovac Sven
- Grabski Varlen
- Graczykowski Lukasz Kamil
- Grecka Ekaterina
- Grelli Alessandro
- Grigoras Costin
- Grigoryan Smbat
- 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
- Gyulai Laszlo
- Hachiya Shimomura Maya
- Hadjidakis Cynthia Marie
- Haider Fakhar Ul
- Haidlova Sara
- Hamagaki Hideki
- Hamdi Abdennacer
- Han Younghoon
- Hanley Brian Gerald
- Hannigan Ryan Patrick
- Hansen Joachim
- Haque Md Rihan
- Harris John William
- Harton Austin Vincent
- Hassan Hadi
- Hatzifotiadou Despina
- Hauer Philip
- Haugland Solheim Emilie
- Havener Laura Brittany
- Heckel Stefan Thomas
- Hellbar Ernst
- Helstrup Haavard
- Hemmer Marvin
- Herman Tomas
- Herrera Corral Gerardo Antonio
- Herrmann Florian
- 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
- Hughes Charles
- Huhn Patrick
- Huhta Laura Maria
- Humanic Thomas
- Hutson Alek
- Hutter Dirk
- Ilkaev Radiy
- Ilyas Hira
- Inaba Motoi
- Innocenti Gian Michele
- Ippolitov Mikhail
- Isakov Artem
- Isidori Tommaso
- Islam Md Samsul
- 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
- Kabus Maja Jadwiga
- Kaewjai Jetnipit
- Kalinak Peter
- Kalteyer Annalena Sophie
- Kalweit Alexander Philipp
- Kaplin Vladimir
- Karasu Uysal Ayben
- Karatovic David
- Karavichev Oleg
- Karavicheva Tatiana
- Karczmarczyk Przemyslaw
- Karpechev Evgeny
- Kebschull Udo Wolfgang
- Keidel Ralf
- Keijdener Darius
- Keil Markus
- Ketzer Bernhard Franz
- Khade Swapnesh Santosh
- Khan Ahsan Mehmood
- Khan Mohammed Mohisin
- Khan Shaista
- Khanzadeev Alexei
- Kharlov Yury
- Khatun Anisa
- Khuntia Arvind
- Kileng Bjarte
- Kim Beomkyu
- Kim Chong
- Kim Dong Jo
- Kim Eun Joo
- Kim Jaehyun
- Kim Jinsook
- Kim Jiyoung
- Kim Junlee
- Kim Minjung
- Kim Se Yong
- Kim Taejun
- Kimura Kento
- 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
- Knospe Anders Garritt
- Kobdaj Chinorat
- Kollegger Thorsten Sven
- Kondratyev Andrey
- Kondratyeva Natalia
- Kondratyuk Evgeny
- Konig Joshua Leon
- Konigstorfer Stephan Alexander
- Konopka Piotr Jan
- Kornakov Van Georgui
- Koryciak Sebastian Dominik
- Kotliarov Artem
- Kovalenko Vladimir
- Kowalski Marek
- Kozhuharov Venelin Valeriev
- Kralik Ivan
- Kravcakova Adela
- Krcal Lubos
- Krivda Marian
- Krizek Filip
- Krizkova Gajdosova Katarina
- Kroesen Martin
- 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
- Kweon Min Jung
- Kwon Youngil
- La Pointe Sarah Louise
- La Rocca Paola
- Lafuente Mazuecos Antonio
- Lakrathok Anantachai
- Lamanna Massimo
- 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 Xiaomei
- 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
- Loncar Petra
- Lopez Torres Ernesto
- Lopez Xavier Bernard
- Lu Pengzhong
- Lugo Fabiola Viridiana
- Luhder Jens Robert
- Lunardon Marcello
- Luparello Grazia
- Ma Yugang
- Mager Magnus
- Maire Antonin
- 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
- 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 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
- Mayer Christoph
- Mazzaschi Francesco
- Mazzilli Marianna
- Mckibben Lofnes Ingrid
- Mdhluli Joyful Elma
- Mejia Camacho Juan Manuel
- Melikyan Yury
- Menchaca-Rocha Arturo Alejandro
- Meninno Elisa
- Meres Michal
- Mesa Perez Guillermo
- Mhlanga Sibaliso
- Miake Yasuo
- Micheletti Luca
- Mihaylov Dimitar Lubomirov
- Mikhaylov Konstantin
- Mishra Aditya Nath
- Modak Abhi
- Mohanty Bedangadas
- Molander Mikael Andreas
- Monira Shirajum
- Mordasini Cindy
- Moreira de Godoy 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
- 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
- Ogino Masanori
- Oh Saehanseul
- Ohlson Alice Elisabeth
- Okorokov Vitaly
- Oleniacz Janusz
- Oliveira da Silva Antonio Carlos
- 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
- Patra Rajendra Nath
- Paul Biswarup
- Paz Jimenez Alom Antonio
- Pei Hua
- Peitzmann Thomas
- Peng Xinye
- Pennisi Michele
- Perciballi Stefania
- Peresunko Dmitry Yurevich
- Peretti Pezzi Rafael
- Pestov Yury
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- 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 Valeriy
- Pradhan Kshitish Kumar
- Prasad Sidharth Kumar
- Prasad Suraj
- Preghenella Roberto
- Prino Francesco
- Pruneau Claude Andre
- Pshenichnov Igor
- Puccio Maximiliano
- Pucillo Sara
- Pugelova Zuzana
- Qiu Shi
- Quaglia Luca
- Ragoni Simone
- Rai Ananya
- Rakotozafindrabe Andry Malala
- Ramello Luciano
- Rami Fouad
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- Wegrzynek Adam Tadeusz
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- Wiechula Jens
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- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Willems Guido Alexander
- Windelband Bernd Stefan
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- Wright Josephina Rae
- Wu Wenya
- Wu Yitao
- Xu Ran
- Yadav Ankur
- Yadav Arun Kumar
- Yalcin Kuzu Serpil
- Yamaguchi Yorito
- Yang Shiming
- Yano Satoshi
- 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 Song
- Zhang Xiaoming
- Zhang Yifei
- Zhang Zhen
- Zhao Mingrui
- Zherebchevskii Vladimir
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Ya
- Zugravel Stefan Cristi
- Zurlo Nicola
- Publication venue
- HAL CCSD
- Publication date
- 07/09/2023
- Field of study
International audienceThe Chiral Magnetic Wave (CMW) phenomenon is essential to provide insights into the strong interaction in QCD, the properties of the quark-gluon plasma, and the topological characteristics of the early universe, offering a deeper understanding of fundamental physics in high-energy collisions. Measurements of the charge-dependent anisotropic flow coefficients are studied in Pb-Pb collisions at center-of-mass energy per nucleon-nucleon collision sNN= 5.02 TeV to probe the CMW. In particular, the slope of the normalized difference in elliptic (v2) and triangular (v3) flow coefficients of positively and negatively charged particles as a function of their event-wise normalized number difference, is reported for inclusive and identified particles. The slope r3Norm is found to be larger than zero and to have a magnitude similar to r2Norm, thus pointing to a large background contribution for these measurements. Furthermore, r2Norm can be described by a blast wave model calculation that incorporates local charge conservation. In addition, using the event shape engineering technique yields a fraction of CMW (fCMW) contribution to this measurement which is compatible with zero. This measurement provides the very first upper limit for fCMW, and in the 10-60% centrality interval it is found to be 26% (38%) at 95% (99.7%) confidence level
Charged-particle production as a function of the relative transverse activity classifier in pp, p−Pb, and Pb−Pb collisions at the LHC
- Author
- Abranches de Carvalho Leopoldo
- Acharya Shreyasi
- Adamova Dagmar
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- 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
- 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
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- von Haller Barthelemy
- Vorobyev Ivan
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- Wang Yubiao
- Wegrzynek Adam Tadeusz
- Weiglhofer Felix Thomas
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- Wilkinson Jeremy John
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- Windelband Bernd Stefan
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- Wright Josephina Rae
- Wu Wenya
- Wu Yitao
- Xu Ran
- Yadav Ankur
- Yadav Arun Kumar
- Yalcin Kuzu Serpil
- 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 Song
- Zhang Xiaoming
- Zhang Yifei
- Zhang Zhen
- Zhao Mingrui
- Zherebchevskii Vladimir
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Ya
- Zugravel Stefan Cristi
- Zurlo Nicola
- Publication venue
- HAL CCSD
- Publication date
- 24/10/2023
- Field of study
International audienceMeasurements of charged-particle production in pp, p−Pb, and Pb−Pb collisions in the toward, away, and transverse regions with the ALICE detector are discussed. These regions are defined event-by-event relative to the azimuthal direction of the charged trigger particle, which is the reconstructed particle with the largest transverse momentum (pTtrig) in the range 8<pTtrig<15 GeV/c. The toward and away regions contain the primary and recoil jets, respectively; both regions are accompanied by the underlying event (UE). In contrast, the transverse region perpendicular to the direction of the trigger particle is dominated by the so-called UE dynamics, and includes also contributions from initial- and final-state radiation. The relative transverse activity classifier, RT=NchT/⟨NchT⟩, is used to group events according to their UE activity, where NchT is the charged-particle multiplicity per event in the transverse region and ⟨NchT⟩ is the mean value over the whole analysed sample. The energy dependence of the RT distributions in pp collisions at s=2.76, 5.02, 7, and 13 TeV is reported, exploring the Koba-Nielsen-Olesen (KNO) scaling properties of the multiplicity distributions. The first measurements of charged-particle pT spectra as a function of RT in the three azimuthal regions in pp, p−Pb, and Pb−Pb collisions at sNN=5.02 TeV are also reported. Data are compared with predictions obtained from the event generators PYTHIA 8 and EPOS LHC. This set of measurements is expected to contribute to the understanding of the origin of collective-like effects in small collision systems (pp and p−Pb)
Light-flavor particle production in high-multiplicity pp collisions at s = 13 TeV as a function of transverse spherocity
- Author
- Abranches De Carvalho Leopoldo
- Acharya Shreyasi
- Adamova Dagmar
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- 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
- 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
- Balbino Alessandro
- Baldisseri Alberto
- Balis Bartosz
- Banerjee Debjani
- Banoo Zarina
- Barbera Roberto
- Barile Francesco
- Barioglio Luca
- Barlou Maria
- Barman Banajit
- Barnafoldi Gergely Gabor
- Barnby Lee Stuart
- 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
- Beole Stefania Maria
- Berdnikov Yaroslav
- Berdnikova Anastasia
- Bergmann Luisa
- Bertran Ferrer Marta
- Besoiu Mihaela Gabriela
- Betev Latchezar
- Bhaduri Partha Pratim
- Bhasin Anju
- Bhat Mohammad Asif
- Bhattacharjee Buddhadeb
- Bianchi Livio
- Bianchi Nicola
- Bielcik Jaroslav
- Bielcikova Jana
- Biernat Jacek Bogumil
- 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
- Bogdanov Alexey
- Boi Stefano
- 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
- Cai Mengke
- Caines Helen Louise
- Caliva Alberto
- Calvo Villar Ernesto
- Camerini Paolo
- Carabas Mihai
- Carnesecchi Francesca
- Caron Robin Albert Andre
- Castillo Castellanos Javier Ernesto
- Catalano Fabio
- Ceballos Sanchez Cesar
- Chakaberia Irakli
- Chakraborty Pritam
- Chandra Sinjini
- Chapeland Sylvain
- Chartier Marielle
- Chattopadhyay Subhasis
- Chattopadhyay Sukalyan
- Cheng Tiantian
- Cheshkov Cvetan Valeriev
- Cheynis Brigitte
- Chibante Barroso Vasco Miguel
- Chizzali Emma Sophia
- Cho Jaeyoon
- Cho Soyeon
- Chochula Peter
- Choudhury Dhrubajyoti
- Christakoglou Panagiotis
- Christensen Christian Holm
- Christiansen Peter
- Chujo Tatsuya
- Ciacco Mario
- Cicalo Corrado
- Cindolo Federico
- Ciupek Michael Rudolf
- Clai Giulia
- Colamaria Fabio Filippo
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- Von Haller Barthelemy
- Vorobyev Ivan
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- Wan Jie
- Wang Chunzheng
- Wang Dongfang
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- Wang Yubiao
- Wegrzynek Adam Tadeusz
- Weiglhofer Felix Thomas
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- Wessels Johannes Peter
- Weyhmiller Sierra Lisa
- Wiechula Jens
- Wikne Jon
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Willems Guido Alexander
- Windelband Bernd Stefan
- Winn Michael Andreas
- Wright Josephina Rae
- Wu Wenya
- Wu Yitao
- Xu Ran
- Yadav Ankur
- Yadav Arun Kumar
- Yalcin Kuzu Serpil
- Yamaguchi Yorito
- Yang Shiming
- Yano Satoshi
- 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 Song
- Zhang Xiaoming
- Zhang Yifei
- Zhang Zhen
- Zhao Mingrui
- Zherebchevskii Vladimir
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Ya
- Zugravel Stefan Cristi
- Zurlo Nicola
- Publication venue
- Publication date
- 26/09/2023
- Field of study
Results on the transverse spherocity dependence of light-flavor particle production (π, K, p, ϕ, K∗0, KS0, Λ, Ξ) at midrapidity in high-multiplicity pp collisions at s = 13 TeV were obtained with the ALICE apparatus. The transverse spherocity estimator (SOpT=1) categorizes events by their azimuthal topology. Utilizing narrow selections on SOpT=1, it is possible to contrast particle production in collisions dominated by many soft initial interactions with that observed in collisions dominated by one or more hard scatterings. Results are reported for two multiplicity estimators covering different pseudorapidity regions. The SOpT=1 estimator is found to effectively constrain the hardness of the events when the midrapidity (∣η∣<0.8) estimator is used. The production rates of strange particles are found to be slightly higher for soft isotropic topologies, and severely suppressed in hard jet-like topologies. These effects are more pronounced for hadrons with larger mass and strangeness content, and observed when the topological selection is done within a narrow multiplicity interval. This demonstrates that an important aspect of the universal scaling of strangeness enhancement with final-state multiplicity is that high-multiplicity collisions are dominated by soft, isotropic processes. On the contrary, strangeness production in events with jet-like processes is significantly reduced. The results presented in this article are compared with several QCD-inspired Monte Carlo event generators. Models that incorporate a two-component phenomenology, either through mechanisms accounting for string density, or thermal production, are able to describe the observed strangeness enhancement as a function of SOpT=1.Results on the transverse spherocity dependence of light-flavor particle production (π, K, p, ϕ, K∗0, KS0, Λ, Ξ) at midrapidity in high-multiplicity pp collisions at s=13 TeV were obtained with the ALICE apparatus. The transverse spherocity estimator (SOpT=1) categorizes events by their azimuthal topology. Utilizing narrow selections on SOpT=1, it is possible to contrast particle production in collisions dominated by many soft initial interactions with that observed in collisions dominated by one or more hard scatterings. Results are reported for two multiplicity estimators covering different pseudorapidity regions. The SOpT=1 estimator is found to effectively constrain the hardness of the events when the midrapidity (∣η∣<0.8) estimator is used. The production rates of strange particles are found to be slightly higher for soft isotropic topologies, and severely suppressed in hard jet-like topologies. These effects are more pronounced for hadrons with larger mass and strangeness content, and observed when the topological selection is done within a narrow multiplicity interval. This demonstrates that an important aspect of the universal scaling of strangeness enhancement with final-state multiplicity is that high-multiplicity collisions are dominated by soft, isotropic processes. On the contrary, strangeness production in events with jet-like processes is significantly reduced. The results presented in this article are compared with several QCD-inspired Monte Carlo event generators. Models that incorporate a two-component phenomenology, either through mechanisms accounting for string density, or thermal production, are able to describe the observed strangeness enhancement as a function of SOpT=1
Common femtoscopic hadron-emission source in pp collisions at the LHC
- Author
- Abranches de Carvalho Leopoldo
- Acharya Shreyasi
- Adamova Dagmar
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- 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
- 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
- Beole Stefania Maria
- Berdnikov Yaroslav
- Berdnikova Anastasia
- Bergmann Luisa
- Bertran Ferrer Marta
- Besoiu Mihaela Gabriela
- Betev Latchezar
- Bhaduri Partha Pratim
- Bhasin Anju
- Bhat Mohammad Asif
- 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
- Boi Stefano
- 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
- Catalano Fabio
- Ceballos Sanchez Cesar
- Chakaberia Irakli
- Chakraborty Pritam
- Chandra Sinjini
- Chapeland Sylvain
- Chartier Marielle
- Chattopadhyay Subhasis
- Chattopadhyay Sukalyan
- Cheng Tiantian
- Cheshkov Cvetan Valeriev
- Cheynis Brigitte
- Chibante Barroso Vasco Miguel
- Chizzali Emma Sophia
- Cho Jaeyoon
- Cho Soyeon
- Chochula Peter
- 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
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- Contin Giacomo
- Contreras Nuno Jesus Guillermo
- Coquet Maurice Louis
- Cortese Pietro
- Cosentino Mauro Rogerio
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- Cot Corentin
- Crkovska Jana
- Crochet Philippe
- Cruz Torres Reynier
- Cui Pengyao
- Czeslaw Miskowiec Dariusz
- Dainese Andrea
- 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
- Dhankher Preeti
- Di Bari Domenico
- Di Mauro Antonio
- Diab Batoul
- Dietel Thomas
- Ding Yanchun
- Ditzel Janik
- Divia Roberto
- Dixit Dhruv Utpalkumar
- Djuvsland Oeystein
- Dmitrieva Uliana
- Dobrigkeit Chinellato David
- Dobrin Alexandru Florin
- Dominguez Rosas Edgar
- Donigus Benjamin
- Duarte Galvan Carlos
- Dubinski Jan Michal
- Dubla Andrea
- Dudi Sandeep
- Dupieux Pascal
- Durkac Martin
- 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
- Fierro Rojas Pablo
- 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
- 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
- Ganoti Paraskevi
- Garabatos Cuadrado Jose Maria
- Garcia Chavez Tonatiuh
- Garcia Guardiano Gabriel
- Garcia-Solis Edmundo Javier
- Gargiulo Corrado
- Gasik Piotr Jan
- Gautam Amrit
- Germain Marie
- Ghimouz Abderrahmane
- Ghosh Chandrasekhar
- Giacalone Marco
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- Tkacik Milan
- Tkacik Tomas
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- Torres Ramos Arianna Grisel
- Trifiro Antonio
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- Trubnikov Victor
- Trzaska Wladyslaw Henryk
- Trzcinski Tomasz Piotr
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- Tveter Trine Spedstad
- Ullaland Kjetil
- Ulukutlu Berkin
- Uras Antonio
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- Vala Martin
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- Valle Nicolo
- van Doremalen Lennart
- van Leeuwen Marco
- van Veen Casper Arie
- van Weelden Roelof Jan Gijs
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- 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
- 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 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
- 05/12/2023
- Field of study
International audienceThe femtoscopic study of pairs of identical pions is particularly suited to investigate the effective source function of particle emission, due to the resulting Bose-Einstein correlation signal. In small collision systems at the LHC, pp in particular, the majority of the pions are produced in resonance decays, which significantly affect the profile and size of the source. In this work, we explicitly model this effect in order to extract the primordial source in pp collisions at s=13 TeV from charged π-π correlations measured by ALICE. We demonstrate that the assumption of a Gaussian primordial source is compatible with the data and that the effective source, resulting from modifications due to resonances, is approximately exponential, as found in previous measurements at the LHC. The universality of hadron emission in pp collisions is further investigated by applying the same methodology to characterize the primordial source of K-p pairs. The size of the primordial source is evaluated as a function of the transverse mass (mT) of the pairs, leading to the observation of a common scaling for both π-π and K-p, suggesting a collective effect. Further, the present results are compatible with the mT scaling of the p-p and p−Λ primordial source measured by ALICE in high multiplicity pp collisions, providing compelling evidence for the presence of a common emission source for all hadrons in small collision systems at the LHC. This will allow the determination of the source function for any hadron--hadron pairs with high precision, granting access to the properties of the possible final-state interaction among pairs of less abundantly produced hadrons, such as strange or charmed particles
Measurement of the production cross section of prompt Ξ0c baryons in p–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
- Averyanov Dmitry
- 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
- Chinu Fabrizio
- Chizzali Emma Sophia
- Cho Jaeyoon
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- Wilhelmi Alexander
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- Xu Ran
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- Yang Shiming
- Yano Satoshi
- Yeats Emma Rose
- Yin Zhongbao
- Yoo In-Kwon
- Yoon Jin Hee
- Yoval Pozos Irandheny
- Yu Hyeonjin
- Yu Zhi
- Yuan Shiming
- Yüncü Alperen
- Zaccolo Valentina
- Zampolli Chiara
- Zanone Federica
- Zardoshti Nima
- Zarochentsev Andrey
- 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
- Závada Petr
- Önnerstad Anna
- Šafařík Karel
- Šerkšnytė Laura
- Šuljić Miljenko
- Țăpuş Nicolae
- Publication venue
- Publication date
- 23/05/2024
- Field of study
The transverse momentum (pT) differential production cross section of the promptly-produced charm-strange baryon Ξ0c (and its charge conjugate Ξ0c¯¯¯¯¯¯) is measured at midrapidity via its hadronic decay into π+Ξ− in p−Pb collisions at a centre-of-mass energy per nucleon−nucleon collision sNN−−−√ = 5.02 TeV with the ALICE detector at the LHC. The Ξ0c nuclear modification factor (RpPb), calculated from the cross sections in pp and p−Pb collisions, is presented and compared with the RpPb of Λ+c baryons. The ratios between the pT-differential production cross section of Ξ0c baryons and those of D0 mesons and Λ+c baryons are also reported and compared with results at forward and backward rapidity from the LHCb Collaboration. The measurements of the production cross section of prompt Ξ0c baryons are compared with a model based on perturbative QCD calculations of charm-quark production cross sections, which includes only cold nuclear matter effects in p−Pb collisions, and underestimates the measurement by a factor of about 50. This discrepancy is reduced when the data is compared with a model in which hadronisation is implemented via quark coalescence. The pT-integrated cross section of prompt Ξ0c-baryon production at midrapidity extrapolated down to pT = 0 is also reported. These measurements offer insights and constraints for theoretical calculations of the hadronisation process. Additionally, they provide inputs for the calculation of the charm production cross section in p−Pb collisions at midrapidity
Measurement of the low-energy antitriton inelastic cross section
- Author
- Abranches De Carvalho Leopoldo
- Acharya Shreyasi
- Adamová Dagmar
- Adler Alexander
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- Akindinov Alexander
- 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
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- Vorobyev Ivan
- Vozniuk Nikita
- Vrlakova Janka
- Vyvre Pierre vande
- Vértesi Róbert
- Völkel Benedikt
- Völkl Martin Andreas
- Wan Jie
- Wang Chunzheng
- Wang Dongfang
- Wang Yuanzhe
- Wang Yubiao
- Weelden Roelof Jan Gijs van
- Wegrzynek Adami Tadeusz
- Weiglhofer Felix Thomas
- Wenzel Sandro Christian
- Wessels Johannes P.
- Weyhmiller Sierra Lisa
- Wiechula Jens
- Wikne Jon
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Willems Guido Alexander
- Windelband Bernd
- Winn Michael
- Wright Josephina Rae
- Wu Wenya
- Wu Yitao
- Xu Ran
- Yadav Ankur
- Yadav Arun Kumar
- Yalcin Kuzu Serpil
- Yamaguchi Yorito
- Yang Shiming
- Yano Satoshi
- Yin Zhongbao
- Yoo In-Kwon
- Yoon Jin Hee
- Yoval Pozos Irandheny
- Yu Hyeonjin
- Yu Zhi
- Yuan Shiming
- Yüncü Alperen
- Zaccolo Valentina
- Zampolli Chiara
- Zanone Federica
- Zardoshti Nima
- Zarochentsev Andrey
- Zavyalov Nikolay
- Zhalov Mikhail
- Zhang Biao
- Zhang Chi
- Zhang Liuyao
- Zhang Song
- Zhang Xiaoming
- Zhang Yifei
- Zhang Zhen
- Zhao Mingrui
- Zherebchevskii Vladimir
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Ya
- Zugravel Stefan Cristi
- Zurlo Nicola
- Závada Petr
- Önnerstad Anna
- Šafařík Karel
- Šerkšnytė Laura
- Šuljić Miljenko
- Țăpuş Nicolae
- Publication venue
- Publication date
- 07/07/2023
- Field of study
In this Letter, the first measurement of the inelastic cross section for antitriton−nucleus interactions is reported, covering the momentum range of 0.8≤p<2.4 GeV/c. The measurement is carried out using data recorded with the ALICE detector in pp and Pb−Pb collisions at a centre-of-mass energy per nucleon of 13 TeV and 5.02 TeV, respectively. The detector material serves as an absorber for antitriton nuclei. The raw yield of (anti)triton nuclei measured with the ALICE apparatus is compared to the results from detailed ALICE simulations based on the GEANT4 toolkit for the propagation of (anti)particles through matter, allowing one to quantify the inelastic interaction probability in the detector material. This analysis complements the measurement of the inelastic cross section of antinuclei up to A=3 carried out by the ALICE Collaboration, and demonstrates the feasibility of the study of the isospin dependence of inelastic interaction cross section with the analysis techniques presented in this Letter
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