307 research outputs found
Screening genetic variation for photosynthetic capacity and efficiency in wheat
- Author
- Publication venue
- Publication date
- Field of study
The world population is rising, placing increasing
demands on food production. One way to contribute to food
security is by improving yields of staple crops like wheat. Yield
can be calculated from the product of plant biomass and harvest
index (the ratio of grain yield to above ground biomass). Since
harvest index of wheat has already reached its maximum biological
limit in some environments, attention is now focused on
increasing crop biomass. Efficient interception of
photosynthetically active radiation and effective photosynthetic
sugar production underpin yield, however, little breeding has
been done for photosynthetic performance. Exploiting existing
genetic variation for important photosynthetic traits such as
photosynthetic capacity (Pc) and photosynthetic efficiency (Peff)
will help to improve wheat yield. CO2 assimilation rate, which is
a commonly measured parameter for assessing photosynthetic
performance, is found to vary across wheat genotypes. Two
additionally important parameters are Rubisco activity (Vcmax)
and electron transport rate (J). There is much less information
reported regarding genetic variation of these two latter
parameters because measurements of CO2 response curves with gas
exchange used to derive Vcmax and J are slow and unsuitable for
rapid screening of many genotypes in the field. The two main
objectives of this project were firstly, to find out if there is
genetic variation for these important photosynthetic traits in
wheat, and secondly, to develop a rapid method for screening
photosynthetic and leaf attributes in different wheat genotypes.
To deal with variable leaf temperatures in the field and
accurately estimate Vcmax and J, improved values for the
temperature dependence of several Rubisco kinetic parameters were
needed. These temperature-dependencies were derived from
measurements made under controlled conditions. A method for
rapidly estimating variation in Pc components Vcmax and J and in
other photosynthetic traits was developed based on calibration of
leaf reflectance spectra against photosynthetic parameters
derived using conventional gas exchange, morphological (leaf mass
per unit area, LMA) and chemical (nitrogen and chlorophyll per
unit area) measurements of 76 wheat genotypes screened in several
different environments. When observed data were compared against
predictions from reflectance spectra, correlation coefficients
(R2 values) of 0.62 for Vcmax25, 0.71 (J), 0.89 (LMA) and 0.93
(Narea), were obtained. Reflectance spectra from an additional
458 elite and landrace wheat genotypes were measured to further
assess variation in photosynthetic traits. There were significant
differences between wheat genotypes in Vcmax25 per unit N, which
is a good measure of Peff. Environment presented interaction with
genotypes for Pc and Peff when measurements performed in
glasshouse & field or in Australia & Mexico were compared. In
future, linking genotypic variation for photosynthetic traits to
DNA-based genetic markers will permit even faster selection of
genotypes in breeding. Reflectance spectra should be a good tool
to accelerate identification and selection of wheat genotypes and
detection of important genomic regions for photosynthetic
capacity and efficiency in wheat
Photons to food: genetic improvement of cereal crop photosynthesis
- Publication venue
- 'Oxford University Press (OUP)'
- Publication date
- 28/11/2021
- Field of study
Photosynthesis has become a major trait of interest for cereal yield improvement as breeders appear to have reached the theoretical genetic limit for harvest index, the mass of grain as a proportion of crop biomass. Yield improvements afforded by the adoption of green revolution dwarfing genes to wheat and rice are becoming exhausted, and improvements in biomass and radiation use efficiency are now sought in these crops. Exploring genetic diversity in photosynthesis is now possible using high-throughput techniques, and low-cost genotyping facilitates discovery of the genetic architecture underlying this variation. Photosynthetic traits have been shown to be highly heritable, and significant variation is present for these traits in available germplasm. This offers hope that breeding for improved photosynthesis and radiation use efficiency in cereal crops is tractable and a useful shorter term adjunct to genetic and genome engineering to boost yield potential.the New South Wales Environmental Trust (2016/RD/0006), the Cotton Research
and Development Corporation (CRDC), and the Grains Research and Development Corporation (GRDC
Pulse Root Ideotype for Water Stress in Temperate Cropping System
- Publication venue
- 'MDPI AG'
- Publication date
- 01/04/2021
- Field of study
Pulses are a key component of crop production systems in Southern Australia due to their rotational benefits and potential profit margins. However, cultivation in temperate cropping systems such as that of Southern Australia is limited by low soil water availability and subsoil constraints. This limitation of soil water is compounded by the irregular rainfall, resulting in the absence of plant available water at depth. An increase in the productivity of key pulses and expansion into environments and soil types traditionally considered marginal for their growth will require improved use of the limited soil water and adaptation to sub soil constrains. Roots serve as the interface between soil constraints and the whole plant. Changes in root system architecture (RSA) can be utilised as an adaptive strategy in achieving yield potential under limited rainfall, heterogenous distribution of resources and other soil-based constraints. The existing literature has identified a “‘Steep, Deep and Cheap” root ideotype as a preferred RSA. However, this idiotype is not efficient in a temperate system where plant available water is limited at depth. In addition, this root ideotype and other root architectural studies have focused on cereal crops, which have different structures and growth patterns to pulses due to their monocotyledonous nature and determinant growth habit. The paucity of pulse-specific root architectural studies warrants further investigations into pulse RSA, which should be combined with an examination of the existing variability of known genetic traits so as to develop strategies to alleviate production constraints through either tolerance or avoidance mechanisms. This review proposes a new model of root system architecture of “Wide, Shallow and Fine” roots based on pulse roots in temperate cropping systems. The proposed ideotype has, in addition to other root traits, a root density concentrated in the upper soil layers to capture in-season rainfall before it is lost due to evaporation. The review highlights the potential to achieve this in key pulse crops including chickpea, lentil, faba bean, field pea and lupin. Where possible, comparisons to determinate crops such as cereals have also been made. The review identifies the key root traits that have shown a degree of adaptation via tolerance or avoidance to water stress and documents the current known variability that exists in and amongst pulse crops setting priorities for future research
Mining for allelic gold : finding genetic variation in photosynthetic traits in crops and wild relatives
- Author
- Publication venue
- U.K., Oxford University Press
- Publication date
- 01/01/2022
- Field of study
Improvement of photosynthetic traits in crops to increase yield potential and crop resilience has recently become a major breeding target. Synthetic biology and genetic technologies offer unparalleled opportunities to create new genetics for photosynthetic traits driven by existing fundamental knowledge. However, large ‘gene bank’ collections of germplasm comprising historical collections of crop species and their relatives offer a wealth of opportunities to find novel allelic variation in the key steps of photosynthesis, to identify new mechanisms and to accelerate genetic progress in crop breeding programmes. Here we explore the available genetic resources in food and fibre crops, strategies to selectively target allelic variation in genes underpinning key photosynthetic processes, and deployment of this variation via gene editing in modern elite material
Hyperspectral reflectance as a tool to measure biochemical and physiological traits in wheat
- Author
- Ainsworth
- Amani
- Anthony G Condon
- Babar
- Benedict
- Bernacchi
- Cabrera-Bosquet
- De Kauwe
- Dillen
- Doughty
- Ecarnot
- Farquhar
- Fischer
- Fox
- Galicia
- Gamon
- Gamon
- Garriga
- Geladi
- Gemma Molero
- Gillon
- González-Navarro
- Goward
- Hansen
- Heckmann
- Inada
- John R Evans
- Jones
- Jones
- June
- Lopes
- Matthew P Reynolds
- Mevik
- Mullan
- Munns
- Nguyen
- Parry
- Peñuelas
- Peñuelas
- Peñuelas
- Pimstein
- Pinto
- Rebetzke
- Rebetzke
- Reynolds
- Robert T Furbank
- Serbin
- Serbin
- Shawn P Serbin
- Silva-Pérez
- Singh
- Sirault
- Stinziano
- Tattaris
- Tucker
- UN Department of Economic and Social Affairs
- Viridiana Silva-Perez
- von Caemmerer
- Yang
- Yao
- Yendrek
- Zadoks
- Publication venue
- 'Oxford University Press (OUP)'
- Publication date
- Field of study
K∗(892)± resonance production in Pb−Pb collisions at sNN = 5.02 TeV
- 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
- Fecchio Pietro
- 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
- 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
- Gioachin Giulia
- Giubellino Paolo
- Giubilato Piero
- Glaenzer Aude Marie Camille
- Glassel Peter
- Glimos Ewa
- Goh Daniel Jia Qin
- Gonzalez Sebastian Victor Luis
- 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
- 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
- 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
- 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 Valeriy
- Pradhan Kshitish Kumar
- Prasad Sidharth Kumar
- Prasad Suraj
- Preghenella Roberto
- Prino Francesco
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- Wang Yubiao
- Wegrzynek Adam Tadeusz
- Weiglhofer Felix Thomas
- Wenzel Sandro Christian
- 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
- HAL CCSD
- Publication date
- 07/09/2023
- Field of study
International audienceThe production of K∗(892)± meson resonance is measured at midrapidity (∣y∣8 GeV/c, consistent with measurements for other light-flavored hadrons. The smallest values are observed in most central collisions, indicating larger energy loss of partons traversing the dense medium
Multiplicity and event-scale dependent flow and jet fragmentation in pp collisions at s = 13 TeV and in p−Pb collisions at sNN = 5.02 TeV
- 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
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- 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
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- Bellini Francesca
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- Bhat Mohammad Asif
- Bhattacharjee Buddhadeb
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- Bigot Alexandre Patrick
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- Wang Chunzheng
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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
- HAL CCSD
- Publication date
- 07/09/2023
- Field of study
International audienceLong- and short-range correlations for pairs of charged particles are studied via two-particle angular correlations in pp collisions at s=13 TeV and p−Pb collisions at sNN=5.02 TeV. The correlation functions are measured as a function of relative azimuthal angle Δφ and pseudorapidity separation Δη for pairs of primary charged particles within the pseudorapidity interval ∣η∣<0.9 and the transverse-momentum interval 1<pT<4 GeV/c. Flow coefficients are extracted for the long-range correlations (1.6<∣Δη∣<1.8) in various high-multiplicity event classes using the low-multiplicity template fit method. The method is used to subtract the enhanced yield of away-side jet fragments in high-multiplicity events. These results show decreasing flow signals toward lower multiplicity events. Furthermore, the flow coefficients for events with hard probes, such as jets or leading particles, do not exhibit any significant changes compared to those obtained from high-multiplicity events without any specific event selection criteria. The results are compared with hydrodynamic-model calculations, and it is found that a better understanding of the initial conditions is necessary to describe the results, particularly for low-multiplicity events
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
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- Bhasin Anju
- Bhat Mohammad Asif
- Bhattacharjee Buddhadeb
- Bianchi Livio
- Bianchi Nicola
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- Bielcikova Jana
- Biernat Jacek Bogumil
- Bigot Alexandre Patrick
- Bilandzic Ante
- Biro Gabor
- Biswas Saikat
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- Blair Justin Thomas
- Blau Dmitry
- Blidaru Mihail Bogdan
- Bluhme Nora
- Blume Christoph
- Boca Gianluigi
- Bock Friederike
- Bodova Tea
- Bogdanov Alexey
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- Boldizsar Laszlo
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- 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
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- Danisch Meike Charlotte
- Danu Andrea
- Das Prottay
- Das Prottoy
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- Dash Archita Rani
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- de Caro Annalisa
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- de Cuveland Jan
- de Falco Alessandro
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- de Marco Nora
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- Dobrigkeit Chinellato David
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- Dominguez Rosas Edgar
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- Wang Yubiao
- Wegrzynek Adam Tadeusz
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- Wessels Johannes Peter
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- 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
- 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
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
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- 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
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- Buckland Matthew Daniel
- Budnikov Dmitry
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- Bufalino Stefania
- Buhler Paul Alois
- Burmasov Nazar
- Buthelezi Edith Zinhle
- Bylinkin Aleksandr
- Bysiak Sebastian Adam
- Cai Mengke
- Caines Helen Louise
- Caliva Alberto
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- Camerini Paolo
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- Carnesecchi Francesca
- Caron Robin Albert Andre
- Castillo Castellanos Javier Ernesto
- Catalano Fabio
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- Wegrzynek Adam Tadeusz
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- 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
- HAL CCSD
- Publication date
- 26/10/2023
- Field of study
International audienceResults 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
Skewness and kurtosis of mean transverse momentum fluctuations at the LHC energies
- 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
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- Boldizsar Laszlo
- Bombara Marek
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- Borissov Alexander
- Borquez Carcamo Andres Gerardo
- Bossi Hannah
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- 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
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- 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
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- Dobrigkeit Chinellato David
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- Dominguez Rosas Edgar
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- 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
- HAL CCSD
- Publication date
- 28/08/2023
- Field of study
International audienceThe first measurements of skewness and kurtosis of mean transverse momentum (⟨pT⟩) fluctuations are reported in Pb−Pb collisions at sNN = 5.02 TeV, Xe−Xe collisions at sNN= 5.44 TeV and pp collisions at s=5.02 TeV using the ALICE detector. The measurements are carried out as a function of system size ⟨dNch/dη⟩∣η∣<0.51/3, using charged particles with transverse momentum (pT) and pseudorapidity (η), in the range 0.2<pT<3.0 GeV/c and ∣η∣<0.8, respectively. In Pb−Pb and Xe−Xe collisions, positive skewness is observed in the fluctuations of ⟨pT⟩ for all centralities, which is significantly larger than what would be expected in the scenario of independent particle emission. This positive skewness is considered a crucial consequence of the hydrodynamic evolution of the hot and dense nuclear matter created in heavy-ion collisions. Furthermore, similar observations of positive skewness for minimum bias pp collisions are also reported here. Kurtosis of ⟨pT⟩ fluctuations is found to be in good agreement with the kurtosis of Gaussian distribution, for most central Pb−Pb collisions. Hydrodynamic model calculations with MUSIC using Monte Carlo Glauber initial conditions are able to explain the measurements of both skewness and kurtosis qualitatively from semicentral to central collisions in Pb--Pb system. Color reconnection mechanism in PYTHIA8 model seems to play a pivotal role in capturing the qualitative behavior of the same measurements in pp collisions
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