17 research outputs found
Challenges in QCD matter physics - The Compressed Baryonic Matter experiment at FAIR
- Author
- Ablyazimov T.
- Abuhoza A.
- Adak R. P.
- Adamczyk M.
- Agarwal K.
- Aggarwal M. M.
- Ahammed Z.
- Ahmad F.
- Ahmad N.
- Ahmad S.
- Akindinov A.
- Akishin P.
- Akishina E.
- Akishina T.
- Akishina V.
- Akram A.
- Al-Turany M.
- Alekseev I.
- Alexandrov E.
- Alexandrov I.
- Amar-Youcef S.
- Andreeva O.
- Andrei C.
- Andronic A.
- Anisimov Yu.
- Anđelić M.
- Appelshäuser H.
- Argintaru D.
- Atkin E.
- Avdeev S.
- Averbeck R.
- Azmi M. D.
- Baban V.
- Bach M.
- Badura E.
- Balog T.
- Balzer M.
- Bao E.
- Baranova N.
- Barczyk T.
- Bartoş D.
- Bashir S.
- Baszczyk M.
- Batenkov O.
- Baublis V.
- Baznat M.
- Becker J.
- Becker K. -H.
- Belogurov S.
- Belyakov D.
- Bendarouach J.
- Berceanu I.
- Bercuci A.
- Berdnikov A.
- Berdnikov Y.
- Berendes R.
- Berezin G.
- Bergmann C.
- Bertini D.
- Bertini O.
- Bezshyyko O.
- Beşliu C.
- Bhaduri P. P.
- Bhasin A.
- Bhati A. K.
- Bhattacharjee B.
- Bhattacharyya A.
- Bhattacharyya T. K.
- Biswas S.
- Blank T.
- Blau D.
- Blinov V.
- Blume C.
- Bocharov Yu.
- Book J.
- Breitner T.
- Brzychczyk J.
- Brüning U.
- Bubak A.
- Bus T.
- Butuzov V.
- Bychkov A.
- Byszuk A.
- Bähr S.
- Büsching H.
- Cai Xu
- Cao Ping
- Caragheorgheopol G.
- Carević I.
- Castillo C. E. Muńoz
- CBM Collaboration
- Chakrabarti A.
- Chattopadhyay S.
- Chaus A.
- Chen Hongfang
- Chen LuYao
- Cheng Jianping
- Chepurnov V.
- Cherif H.
- Chernogorov A.
- Chávez C. García
- Ciobanu M. I.
- Claus G.
- Constantin F.
- Csanád M.
- Cálin M.
- Cătănescu V.
- D'Ascenzo N.
- Das Supriya
- Das Susovan
- de Cuveland J.
- Debnath B.
- Dementiev D.
- Deng Wendi
- Deng Zhi
- Deppe H.
- Deppner I.
- Derenovskaya O.
- Deveaux C. A.
- Deveaux M.
- Dey K.
- Dey M.
- Dillenseger P.
- Dobyrn V.
- Doering D.
- Dong Sheng
- Dorokhov A.
- Dreschmann M.
- Drozd A.
- Dubey A. K.
- Dubnichka S.
- Dubnichkova Z.
- Dutka L.
- Dürr M.
- Dželalija M.
- Elsha V. V.
- Emschermann D.
- Engel H.
- Eremin V.
- Eschke J.
- Eschweiler D.
- Eşanu T.
- Fan Huanhuan
- Fan Xingming
- Farooq M.
- Fateev O.
- Feng Shengqin
- Figuli S. P. D.
- Filozova I.
- Finogeev D.
- Fischer P.
- Flemming H.
- Frankenfeld U.
- Friese V.
- Friske E.
- Fröhlich I.
- Frühauf J.
- Förtsch J.
- Gajda J.
- Galatyuk T.
- Gangopadhyay G.
- Garcia A. M. Marin
- García A. Laso
- Gebelein J.
- Ghosh P.
- Ghosh S. K.
- Gläßel S.
- Goffe M.
- Golinka-Bezshyyko L.
- Golovatyuk V.
- Golovnya S.
- Golovtsov V.
- Golubeva M.
- Golubkov D.
- Gorbunov S.
- Gorokhov S.
- Gottschalk D.
- Gryboś P.
- Grzeszczuk A.
- Guber F.
- Gudima K.
- Gumiński M.
- Gupta A.
- Gusakov Yu.
- Han Dong
- Hartmann H.
- He Shue
- Hehner J.
- Heine N.
- Herghelegiu A.
- Herrmann N.
- Heuser J. M.
- Heß B.
- Himmi A.
- Holzmann R.
- Hu Dongdong
- Huang Guangming
- Huang Xinjie
- Hutter D.
- Höhne C.
- Ierusalimov A.
- Ilgenfritz E. -M.
- Irfan M.
- Ivanischev D.
- Ivanov M.
- Ivanov P.
- Ivanov Valery
- Ivanov Victor
- Ivanov Vladimir
- Ivashkin A.
- Jaaskelainen K.
- Jahan H.
- Jain V.
- Jakovlev V.
- Janson T.
- Jiang Di
- Jipa A.
- Kadenko I.
- Kalinin V.
- Kallunkathariyil J.
- Kampert K. -H.
- Kaptur E.
- Karabowicz R.
- Karavichev O.
- Karavicheva T.
- Karmanov D.
- Karnaukhov V.
- Karpechev E.
- Kasiński K.
- Kasprowicz G.
- Kaur M.
- Kazantsev A.
- Kebschull U.
- Kekelidze G.
- Khan M. M.
- Khan S. A.
- Khanzadeev A.
- Khasanov F.
- Khvorostukhin A.
- Kirakosyan V.
- Kirejczyk M.
- Kiryakov A.
- Kisel I.
- Kisel P.
- Kiselev S.
- Kiss T.
- Kiš M.
- Klaus P.
- Klein-Bösing Ch.
- Kleipa V.
- Klochkov V.
- Kmon P.
- Koch K.
- Kochenda L.
- Koczoń P.
- Koenig W.
- Kohn M.
- Kolb B. W.
- Kolosova A.
- Komkov B.
- Korolev M.
- Korolko I.
- Kotte R.
- Kovalchuk A.
- Kowalski S.
- Koziel M.
- Kozlov G.
- Kozlov V.
- Kramarenko V.
- Kravtsov P.
- Krebs E.
- Kreidl C.
- Kres I.
- Kresan D.
- Kretschmar G.
- Krieger M.
- Kryanev A. V.
- Kryshen E.
- Kuc M.
- Kucewicz W.
- Kucher V.
- Kudin L.
- Kugler A.
- Kumar Ajit
- Kumar Ashwini
- Kumar L.
- Kunkel J.
- Kurepin A.
- Kurepin N.
- Kurilkin A.
- Kurilkin P.
- Kushpil V.
- Kuznetsov S.
- Kyva V.
- Kähler P.
- Kämpfer B.
- Kłeczek R.
- Ladygin V.
- Lara C.
- Larionov P.
- Lavrik E.
- Lazanu I.
- Lebedev A.
- Lebedev S.
- Lebedeva E.
- Lehnert J.
- Lehrbach J.
- Leifels Y.
- Lemke F.
- Li Cheng
- Li Qiyan
- Li Xin
- Li Yuanjing
- Lindenstruth V.
- Linnik B.
- Liu Feng
- Lobanov I.
- Lobanova E.
- Loizeau P. -A.
- Lone S. A.
- Luo Xiaofeng
- Lymanets A.
- Lyu Pengfei
- Löchner S.
- Maevskaya A.
- Mahajan S.
- Mahapatra D. P.
- Mahmoud T.
- Maj P.
- Majka Z.
- Malakhov A.
- Malankin E.
- Malkevich D.
- Malyatina O.
- Malygina H.
- Mandal M. M.
- Mandal S.
- Manko V.
- Manz S.
- Markert J.
- Martínez J. A. Lucio
- Masciocchi S.
- Matulewicz T.
- Meder L.
- Merkin M.
- Mialkovski V.
- Michel J.
- Miftakhov N.
- Mik L.
- Mikhailov K.
- Mikhaylov V.
- Milanović B.
- Militsija V.
- Miskowiec D.
- Momot I.
- Morhardt T.
- Morozov S.
- Mukherjee S.
- Murin Yu.
- Müller W. F. J.
- Müntz C.
- Najman R.
- Nandi C.
- Nandy E.
- Naumann L.
- Nayak T.
- Nedosekin A.
- Negi V. S.
- Niebur W.
- Nikulin V.
- Normanov D.
- Oancea A.
- Oh Kunsu
- Onishchuk Yu.
- Ososkov G.
- Otfinowski P.
- Ovcharenko E.
- Pal S.
- Panasenko I.
- Panda N. R.
- Parzhitskiy S.
- Patel V.
- Pauly C.
- Penschuck M.
- Peshekhonov D.
- Peshekhonov V.
- Petri M.
- Petriş M.
- Petrovici A.
- Petrovici M.
- Petrovskiy A.
- Petráček V.
- Petukhov O.
- Pfeifer D.
- Piasecki K.
- Pieper J.
- Pietraszko J.
- Plotnikov V.
- Plujko V.
- Pluta J.
- Pop A.
- Pospisil V.
- Poźniak K.
- Prakash A.
- Prasad S. K.
- Prokudin M.
- Pshenichnov I.
- Pugach M.
- Pugatch V.
- Płaneta R.
- Querchfeld S.
- Rabtsun S.
- Radulescu L.
- Raha S.
- Rami F.
- Ramírez A. Gómez
- Raniwala R.
- Raniwala S.
- Raportirenko A.
- Rautenberg J.
- Rauza J.
- Ray R.
- Razin S.
- Reichelt P.
- Reinecke S.
- Reinefeld A.
- Reshetin A.
- Ristea C.
- Ristea O.
- Rodriguez A. Rodriguez
- Roether F.
- Romaniuk R.
- Rosado J. Sánchez
- Rost A.
- Rostchin E.
- Rostovtseva I.
- Roy Amitava
- Roy Ankhi
- Rożynek J.
- Ryabov Yu.
- Sadovsky A.
- Sahoo R.
- Sahu P. K.
- Sahu S. K.
- Saini J.
- Samanta S.
- Sambyal S. S.
- Samsonov V.
- Sander O.
- Sarangi S.
- Satława T.
- Sau S.
- Saveliev V.
- Schatral S.
- Schiaua C.
- Schintke F.
- Schmidt C. J.
- Schmidt H. R.
- Schmidt K.
- Scholten J.
- Schweda K.
- Seck F.
- Seddiki S.
- Selyuzhenkov I.
- Semennikov A.
- Senger A.
- Senger P.
- Shabanov A.
- Shabunov A.
- Shao Ming
- Sheremetiev A. D.
- Shi Shusu
- Shumeiko N.
- Shumikhin V.
- Sibiryak I.
- Sikora B.
- Simakov A.
- Simon C.
- Simons C.
- Singaraju R. N.
- Singh A. K.
- Singh B. K.
- Singh C. P.
- Singhal V.
- Singla M.
- Sitzmann P.
- Siwek-Wilczyńska K.
- Skwira-Chalot I.
- Som I.
- Song Guofeng
- Song Jihye
- Sosin Z.
- Soyk D.
- Staszel P.
- Strikhanov M.
- Strohauer S.
- Stroth J.
- Sturm C.
- Sultanov R.
- Sun Yongjie
- Svirida D.
- Svoboda O.
- Szabó A.
- Szczygieł R.
- Talukdar R.
- Tang Zebo
- Tanha M.
- Tarasiuk J.
- Tarassenkova O.
- Teklishyn M.
- Tischler T.
- Tlustý P.
- Toia A.
- Topil'skaya N.
- Tripathy S.
- Träger M.
- Tsakov I.
- Tsyupa Yu.
- Turowiecki A.
- Tuturas N. G.
- Târzilă M. -G.
- Tölyhi T.
- Uhlig F.
- Usenko E.
- Valin I.
- Varga D.
- Vassiliev I.
- Vasylyev O.
- Verbitskaya E.
- Verhoeven W.
- Veshikov A.
- Visinka R.
- Viyogi Y. P.
- Volkov S.
- Volochniuk A.
- Vorobiev A.
- Voronin Aleksey
- Voronin Alexander
- Vovchenko V.
- Vznuzdaev M.
- Wang Dong
- Wang Xi-Wei
- Wang Yaping
- Wang Yi
- Weber M.
- Wendisch C.
- Wessels J. P.
- Wiebusch M.
- Wiechula J.
- Wielanek D.
- Wieloch A.
- Wilms A.
- Winckler N.
- Winter M.
- Wiśniewski K.
- Wolf Gy.
- Won Sanguk
- Wu Ke-Jun
- Wüstenfeld J.
- Xiang Changzhou
- Xu Nu
- Yang Junfeng
- Yang Rongxing
- Yin Zhongbao
- Yoo In-Kwon
- Yuldashev B.
- Yushmanov I.
- Zabołotny W.
- Zaitsev Yu.
- Zamiatin N. I.
- Zanevsky Yu.
- Zhalov M.
- Zhang Yifei
- Zhang Yu
- Zhao Lei
- Zheng Jiajun
- Zheng Sheng
- Zhou Daicui
- Zhou Jing
- Zhu Xianglei
- Zinchenko A.
- Zipper W.
- Zrelov P.
- Zryuev V.
- Zumbruch P.
- Zyzak M.
- Škoda L.
- Żoładź M.
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
Substantial experimental and theoretical efforts worldwide are devoted to
explore the phase diagram of strongly interacting matter. At LHC and top RHIC
energies, QCD matter is studied at very high temperatures and nearly vanishing
net-baryon densities. There is evidence that a Quark-Gluon-Plasma (QGP) was
created at experiments at RHIC and LHC. The transition from the QGP back to the
hadron gas is found to be a smooth cross over. For larger net-baryon densities
and lower temperatures, it is expected that the QCD phase diagram exhibits a
rich structure, such as a first-order phase transition between hadronic and
partonic matter which terminates in a critical point, or exotic phases like
quarkyonic matter. The discovery of these landmarks would be a breakthrough in
our understanding of the strong interaction and is therefore in the focus of
various high-energy heavy-ion research programs. The Compressed Baryonic Matter
(CBM) experiment at FAIR will play a unique role in the exploration of the QCD
phase diagram in the region of high net-baryon densities, because it is
designed to run at unprecedented interaction rates. High-rate operation is the
key prerequisite for high-precision measurements of multi-differential
observables and of rare diagnostic probes which are sensitive to the dense
phase of the nuclear fireball. The goal of the CBM experiment at SIS100
(sqrt(s_NN) = 2.7 - 4.9 GeV) is to discover fundamental properties of QCD
matter: the phase structure at large baryon-chemical potentials (mu_B > 500
MeV), effects of chiral symmetry, and the equation-of-state at high density as
it is expected to occur in the core of neutron stars. In this article, we
review the motivation for and the physics programme of CBM, including
activities before the start of data taking in 2022, in the context of the
worldwide efforts to explore high-density QCD matter.Comment: 15 pages, 11 figures. Published in European Physical Journal
USP25 regulates KEAP1-NRF2 anti-oxidation axis and its inactivation protects acetaminophen-induced liver injury in male mice
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2023
- Field of study
Abstract Nuclear factor erythroid 2-related factor 2 (NRF2) is a transcription factor responsible for mounting an anti-oxidation gene expression program to counter oxidative stress. Under unstressed conditions, Kelch-like ECH-associated protein 1 (KEAP1), an adaptor protein for CUL3 E3 ubiquitin ligase, mediates NRF2 ubiquitination and degradation. We show here that the deubiquitinase USP25 directly binds to KEAP1 and prevents KEAP1’s own ubiquitination and degradation. In the absence of Usp25 or if the DUB is inhibited, KEAP1 is downregulated and NRF2 is stabilized, allowing the cells to respond to oxidative stress more readily. In acetaminophen (APAP) overdose-induced oxidative liver damage in male mice, the inactivation of Usp25, either genetically or pharmacologically, greatly attenuates liver injury and reduces the mortality rates resulted from lethal doses of APAP
Long-range angular correlations of π, K and p in p–Pb collisions at sNN = 5.02 TeV
- Author
- Abelev Betty Bezverkhny
- Adam Jaroslav
- Adamova Dagmar
- Adare Andrew Marshall
- Aggarwal Madan Mohan
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agocs Andras Gabor
- Agostinelli Andrea
- Ahammed Zubayer
- Ahmad Arshad
- Ahmad Nazeer
- Ahmed Ijaz
- Ahn Sang Un
- Ahn Sul-Ah
- Aimo Ilaria
- Aiola Salvatore
- Ajaz Muhammad
- Akindinov Alexander
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alexandre Didier
- Alici Andrea
- Alkin Anton
- Alme Johan
- Alt Torsten
- Altini Valerio
- Altinpinar Sedat
- Altsybeev Igor
- Alves Garcia Prado Caio
- Andrei Cristian
- Andronic Anton
- Anguelov Venelin
- Anielski Jonas
- Anticic Tome
- Antinori Federico
- Antonioli Pietro
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Araujo Silva Figueredo Marcel
- Arbor Nicolas
- Arcelli Silvia
- Armesto Perez Nestor
- Arnaldi Roberta
- Aronsson Tomas
- Arsene Ionut Cristian
- Arslandok Mesut
- Augustinus Andre
- Averbeck Ralf Peter
- Awes Terry
- Aysto Juha Heikki Eskeli
- Azmi Mohd Danish
- Bach Matthias Jakob
- Badala Angela
- Baek Yong Wook
- Bailhache Raphaelle Marie
- Bala Renu
- Baldisseri Alberto
- Baltasar Dos Santos Pedrosa Fernando
- Ban Jaroslav
- Baral Rama Chandra
- Barbera Roberto
- Barile Francesco
- Barnafoldi Gergely Gabor
- Barnby Lee Stuart
- Bartke Jerzy Gustaw
- Basile Maurizio
- Bastid Nicole
- Basu Sumit
- Bathen Bastian
- Batigne Guillaume
- Batyunya Boris
- Batzing Paul Christoph
- Baumann Christoph Heinrich
- Bearden Ian Gardner
- Beck Hans
- Bedda Cristina
- Behera Nirbhay Kumar
- Belikov Iouri
- Bellini Francesca
- Bellwied Rene
- Belmont Moreno Ernesto
- Bencedi Gyula
- Beole Stefania
- Berceanu Ionela
- Bercuci Alexandru
- Berdnikov Yaroslav
- Berenyi Daniel
- Bergognon Anais Annick Erica
- Bertens Redmer Alexander
- Berzano Dario
- Betev Latchezar
- Bhasin Anju
- Bhati Ashok Kumar
- Bhom Jihyun
- Bianchi Livio
- Bianchi Nicola
- Bielcik Jaroslav
- Bielcikova Jana
- Bilandzic Ante
- Bjelogrlic Sandro
- Blanco Fernando
- Blanco Francescorancesco
- Blau Dmitry
- Blume Christoph
- Bock Friederike
- Boettger Stefan
- Bogdanov Alexey
- Boggild Hans
- Bogolyubskiy Mikhail
- Boldizsar Laszlo
- Bombara Marek
- Book Julian Heinz
- Borel Herve
- Borissov Alexander
- Bornschein Joerg
- Botje Michiel
- Botta Elena
- Braidot Ermes
- Braun-Munzinger Peter
- Bregant Marco
- Breitner Timo Gunther
- Broker Theo Alexander
- Browning Tyler Allen
- Broz Michal
- Brun Rene
- Bruna Elena
- Bruno Giuseppe Eugenio
- Budnikov Dmitry
- Buesching Henner
- Bufalino Stefania
- Buncic Predrag
- Busch Oliver
- Buthelezi Edith Zinhle
- Caffarri Davide
- Cai Xu
- Caines Helen Louise
- Caliva Alberto
- Calvo Villar Ernesto
- Camerini Paolo
- Canoa Roman Veronica
- Cara Romeo Giovanni
- Carena Francesco
- Carena Wisla
- Carminati Federico
- Casanova Diaz Amaya Ofelia
- Castillo Castellanos Javier Ernesto
- Casula Ester Anna Rita
- Catanescu Vasile Ioan
- Cavicchioli Costanza
- Ceballos Sanchez Cesar
- Cepila Jan
- Cerello Piergiorgio
- Chang Beomsu
- Chapeland Sylvain
- Charvet Jean-Luc Fernand
- Chattopadhyay Subhasis
- Chattopadhyay Sukalyan
- Cherney Michael Gerard
- Cheshkov Cvetan Valeriev
- Cheynis Brigitte
- Chibante Barroso Vasco Miguel
- Chochula Peter
- Chojnacki Marek
- Choudhury Subikash
- Christakoglou Panagiotis
- Christensen Christian Holm
- Christiansen Peter
- Chujo Tatsuya
- Chung Suh-Urk
- Cicalo Corrado
- Cifarelli Luisa
- Cindolo Federico
- Cleymans Jean Willy Andre
- Colamaria Fabio Filippo
- Colella Domenico
- Collu Alberto
- Colocci Manuel
- Conesa Balbastre Gustavo
- Conesa Del Valle Zaida
- Connors Megan Elizabeth
- Contin Giacomo
- Contreras Nuno Jesus Guillermo
- Cormier Thomas Michael
- Corrales Morales Yasser
- Cortes Maldonado Ismael
- Cortese Pietro
- Cosentino Mauro Rogerio
- Costa Filippo
- Crochet Philippe
- Cruz Albino Rigoberto
- Cuautle Flores Eleazar
- Cunqueiro Mendez Leticia
- D'Erasmo Ginevra
- Dainese Andrea
- Dang Ruina
- Danu Andrea
- Das Debasish
- Das Indranil
- Das Kushal
- Dash Ajay Kumar
- Dash Sadhana
- De Caro Annalisa
- De Cataldo Giacinto
- De Cuveland Jan
- De Falco Alessandro
- De Gruttola Daniele
- De Marco Nora
- De Pasquale Salvatore
- De Rooij Raoul Stefan
- De Sudipan
- Delagrange Hugues
- Deloff Andrzej
- Denes Ervin Sandor
- Deppman Airton
- Di Bari Domenico
- Di Giglio Carmelo
- Di Liberto Sergio
- Di Mauro Antonio
- Di Nezza Pasquale
- Diaz Corchero Miguel Angel
- Dietel Thomas
- Diozcora Vargas Trevino Aurora
- Divia Roberto
- Djuvsland Oeystein
- Dobrigkeit Chinellato David
- Dobrin Alexandru Florin
- Dobrowolski Tadeusz Antoni
- Doenigus Benjamin
- Dordic Olja
- Dubey Anand Kumar
- Dubla Andrea
- Ducroux Laurent
- Dupieux Pascal
- Dutt Mazumder Abhee Kanti
- Elia Domenico
- Emschermann David Philip
- Engel Heiko
- Erazmus Barbara Ewa
- Erdal Hege Austrheim
- Eschweiler Dominic
- Espagnon Bruno
- Estienne Magali Danielle
- Esumi Shinichi
- Evans David
- Evdokimov Sergey
- Eyyubova Gyulnara
- Fabris Daniela
- Faivre Julien
- Falchieri Davide
- Fantoni Alessandra
- Fasel Markus
- Fehlker Dominik
- Feldkamp Linus
- Felea Daniel
- Feliciello Alessandro
- Feofilov Grigory
- Fernandez Tellez Arturo
- Ferretti Alessandro
- Festanti Andrea
- Figiel Jan
- Filchagin Sergey
- Finogeev Dmitry
- Fionda Fiorella
- Fiore Enrichetta Maria
- Floratos Emmanouil
- Floris Michele
- Foertsch Siegfried Valentin
- Foka Panagiota
- Fokin Sergey
- Fragiacomo Enrico
- Francescon Andrea
- Frankenfeld Ulrich Michael
- Fuchs Ulrich
- Furget Christophe
- Fusco Girard Mario
- Gaardhoeje Jens Joergen
- Gagliardi Martino
- Gago Medina Alberto Martin
- Gallio Mauro
- Gameiro Munhoz Marcelo
- Gangadharan Dhevan Raja
- Ganoti Paraskevi
- Garabatos Cuadrado Jose
- Garcia-Solis Edmundo Javier
- Gargiulo Corrado
- Garishvili Irakli
- Gerhard Jochen
- Germain Marie
- Gheata Andrei George
- Gheata Mihaela
- Ghidini Bruno
- Ghosh Premomoy
- Gianotti Paola
- Giubellino Paolo
- Gladysz-Dziadus Ewa
- Glassel Peter
- Gomez Jimenez Ramon
- Gonzalez Ferreiro Elena
- Gonzalez Zamora Pedro
- Gorbunov Sergey
- Gorlich Lidia Maria
- Gotovac Sven
- Graczykowski Lukasz Kamil
- Grajcarek Robert
- Grelli Alessandro
- Grigoras Alina Gabriela
- Grigoras Costin
- Grigoryan Ara
- Grigoryan Smbat
- Grigoryev Vladislav
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- Viesti Giuseppe
- Viinikainen Jussi Samuli
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- Vinogradov Alexander
- Vinogradov Leonid
- Vinogradov Yury
- Virgili Tiziano
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- Vorobyev Ivan
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- Vulpescu Bogdan
- Vyushin Alexey
- Wagner Boris
- Wagner Jan
- Wagner Vladimir
- Wang Mengliang
- Wang Yaping
- Wang Yifei
- Watanabe Daisuke
- Watanabe Kengo
- Weber Michael
- Wessels Johannes Peter
- Westerhoff Uwe
- Wiechula Jens
- Wikne Jon
- Wilde Martin Rudolf
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Williams Crispin
- Windelband Bernd Stefan
- Winn Michael Andreas
- Xiang Changzhou
- Yaldo Chris G
- Yamaguchi Yorito
- Yang Hongyan
- Yang Ping
- Yang Shiming
- Yano Satoshi
- Yasnopolskiy Stanislav
- Yi Jungyu
- Yin Zhongbao
- Yoo In-Kwon
- Yushmanov Igor
- Zaccolo Valentina
- Zach Cenek
- Zampolli Chiara
- Zaporozhets Sergey
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zbroszczyk Hanna Paulina
- Zelnicek Pierre
- Zgura Sorin Ion
- Zhalov Mikhail
- Zhang Fan
- Zhang Haitao
- Zhang Xiaoming
- Zhang Yonghong
- Zhou Daicui
- Zhou Fengchu
- Zhou You
- Zhu Hongsheng
- Zhu Jianhui
- Zhu Jianlin
- Zhu Xiangrong
- Zichichi Antonino
- Zimmermann Alice
- Zimmermann Markus Bernhard
- Zinovjev Gennady
- Zoccarato Yannick Denis
- Zynovyev Mykhaylo
- Zyzak Maksym
- Publication venue
- 'Elsevier BV'
- Publication date
- 11/07/2013
- Field of study
Angular correlations between unidentified charged trigger particles and various species of charged associated particles (unidentified particles, pions, kaons, protons and antiprotons) are measured by the ALICE detector in p-Pb collisions at a nucleon--nucleon centre-of-mass energy of 5.02 TeV in the transverse-momentum range 0.3 < pT < 4 GeV/c. The correlations expressed as associated yield per trigger particle are obtained in the pseudorapidity range |ηlab| < 0.8. Fourier coefficients are extracted from the long-range correlations projected onto the azimuthal angle difference and studied as a function of pT and in intervals of event multiplicity. In high-multiplicity events, the second-order coefficient for protons, v2p, is observed to be smaller than that for pions, v2π, up to about pT = 2 GeV/c. To reduce correlations due to jets, the per-trigger yield measured in low-multiplicity events is subtracted from that in high-multiplicity events. A two-ridge structure is obtained for all particle species. The Fourier decomposition of this structure shows that the second-order coefficients for pions and kaons are similar. The v2p is found to be smaller at low pT and larger at higher pT than v2π, with a crossing occurring at about 2 GeV. This is qualitatively similar to the elliptic-flow pattern observed in heavy-ion collisions. A mass ordering effect at low transverse momenta is consistent with expectations from hydrodynamic model calculations assuming a collectively expanding system.Angular correlations between unidentified charged trigger particles and various species of charged associated particles (unidentified particles, pions, kaons, protons and antiprotons) are measured by the ALICE detector in p-Pb collisions at a nucleon-nucleon centre-of-mass energy of 5.02 TeV in the transverse-momentum range 0.3<pT<4 GeV/c. The correlations expressed as associated yield per trigger particle are obtained in the pseudorapidity range ∣ηlab∣<0.8. Fourier coefficients are extracted from the long-range correlations projected onto the azimuthal angle difference and studied as a function of pT and in intervals of event multiplicity. In high-multiplicity events, the second-order coefficient for protons, v2p, is observed to be smaller than that for pions, v2π, up to about pT=2 GeV/c. To reduce correlations due to jets, the per-trigger yield measured in low-multiplicity events is subtracted from that in high-multiplicity events. A two-ridge structure is obtained for all particle species. The Fourier decomposition of this structure shows that the second-order coefficients for pions and kaons are similar. The v2p is found to be smaller at low pT and larger at higher pT than v2pi, with a crossing occurring at about 2 GeV. This is qualitatively similar to the elliptic-flow pattern observed in heavy-ion collisions. A mass ordering effect at low transverse momenta is consistent with expectations from hydrodynamic model calculations assuming a collectively expanding system.Angular correlations between unidentified charged trigger particles and various species of charged associated particles (unidentified particles, pions, kaons, protons and antiprotons) are measured by the ALICE detector in p–Pb collisions at a nucleon–nucleon centre-of-mass energy of 5.02 TeV in the transverse-momentum range 0.3<pT<4 GeV/c . The correlations expressed as associated yield per trigger particle are obtained in the pseudorapidity range |ηlab|<0.8 . Fourier coefficients are extracted from the long-range correlations projected onto the azimuthal angle difference and studied as a function of pT and in intervals of event multiplicity. In high-multiplicity events, the second-order coefficient for protons, v2p , is observed to be smaller than that for pions, v2π , up to about pT=2 GeV/c . To reduce correlations due to jets, the per-trigger yield measured in low-multiplicity events is subtracted from that in high-multiplicity events. A two-ridge structure is obtained for all particle species. The Fourier decomposition of this structure shows that the second-order coefficients for pions and kaons are similar. The v2p is found to be smaller at low pT and larger at higher pT than v2π , with a crossing occurring at about 2 GeV/c . This is qualitatively similar to the elliptic-flow pattern observed in heavy-ion collisions. A mass ordering effect at low transverse momenta is consistent with expectations from hydrodynamic model calculations assuming a collectively expanding system
Performance of the ALICE Experiment at the CERN LHC
- Author
- Abelev Betty Bezverkhny
- Abramyan Armenuhi
- Adam Jaroslav
- Adamova Dagmar
- Aggarwal Madan Mohan
- Agnello Michelangelo
- Agostinelli Andrea
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Arshad
- Ahmad Nazeer
- Ahmed Ijaz
- Ahn Sang Un
- Ahn Sul-Ah
- Aimo Ilaria
- Aiola Salvatore
- Ajaz Muhammad
- Akindinov Alexander
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alexandre Didier
- Alici Andrea
- Alkin Anton
- Alme Johan
- Alt Torsten
- Altini Valerio
- Altinpinar Sedat
- Altsybeev Igor
- Alves Garcia Prado Caio
- Andrei Cristian
- Andronic Anton
- Anguelov Venelin
- Anielski Jonas
- Anticic Tome
- Antinori Federico
- Antonioli Pietro
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Araujo Silva Figueredo Marcel
- Arbor Nicolas
- Arcelli Silvia
- Armesto Perez Nestor
- Arnaldi Roberta
- Aronsson Tomas
- Arsene Ionut Cristian
- Arslandok Mesut
- Augustinus Andre
- Averbeck Ralf Peter
- Awes Terry
- Azmi Mohd Danish
- Bach Matthias Jakob
- Badala Angela
- Baek Yong Wook
- Bagnasco Stefano
- Bailhache Raphaelle Marie
- Bala Renu
- Baldisseri Alberto
- Baltasar Dos Santos Pedrosa Fernando
- Baral Rama Chandra
- Barbera Roberto
- Barile Francesco
- Barnafoldi Gergely Gabor
- Barnby Lee Stuart
- Bartke Jerzy Gustaw
- Basile Maurizio
- Bastid Nicole
- Basu Sumit
- Bathen Bastian
- Batigne Guillaume
- Batyunya Boris
- Batzing Paul Christoph
- Baumann Christoph Heinrich
- Bearden Ian Gardner
- Beck Hans
- Bedda Cristina
- Behera Nirbhay Kumar
- Belikov Iouri
- Bellini Francesca
- Bellwied Rene
- Belmont Moreno Ernesto
- Bencedi Gyula
- Beole Stefania
- Berceanu Ionela
- Bercuci Alexandru
- Berdnikov Yaroslav
- Berenyi Daniel
- Berger Martin Emanuel
- Bertens Redmer Alexander
- Berzano Dario
- Betev Latchezar
- Bhasin Anju
- Bhati Ashok Kumar
- Bhattacharjee Buddhadeb
- Bhom Jihyun
- Bianchi Livio
- Bianchi Nicola
- Bianchin Chiara
- Bielcik Jaroslav
- Bielcikova Jana
- Bilandzic Ante
- Bjelogrlic Sandro
- Blanco Fernando
- Blau Dmitry
- Blume Christoph
- Bock Friederike
- Boehmer Felix Valentin
- Boettger Stefan
- Bogdanov Alexey
- Boggild Hans
- Bogolyubskiy Mikhail
- Boldizsar Laszlo
- Bombara Marek
- Book Julian Heinz
- Borel Herve
- Borissov Alexander
- Bossu Francesco
- Botje Michiel
- Botta Elena
- Braun-Munzinger Peter
- Bregant Marco
- Breitner Timo Gunther
- Broker Theo Alexander
- Browning Tyler Allen
- Broz Michal
- Bruna Elena
- Bruno Giuseppe Eugenio
- Budnikov Dmitry
- Buesching Henner
- Bufalino Stefania
- Buncic Predrag
- Busch Oliver
- Buthelezi Edith Zinhle
- Caffarri Davide
- Cai Xu
- Caines Helen Louise
- Caliva Alberto
- Calvo Villar Ernesto
- Camerini Paolo
- Canoa Roman Veronica
- Carena Francesco
- Carena Wisla
- Castillo Castellanos Javier Ernesto
- Casula Ester Anna Rita
- Catanescu Vasile Ioan
- Cavicchioli Costanza
- Ceballos Sanchez Cesar
- Cepila Jan
- Cerello Piergiorgio
- Chang Beomsu
- Chapeland Sylvain
- Charvet Jean-Luc Fernand
- Chattopadhyay Subhasis
- Chattopadhyay Sukalyan
- Cherney Michael Gerard
- Cheshkov Cvetan Valeriev
- Cheynis Brigitte
- Chibante Barroso Vasco Miguel
- Chochula Peter
- Chojnacki Marek
- Choudhury Subikash
- Christakoglou Panagiotis
- Christensen Christian Holm
- Christiansen Peter
- Chujo Tatsuya
- Chung Suh-Urk
- Cicalo Corrado
- Cifarelli Luisa
- Cindolo Federico
- Cleymans Jean Willy Andre
- Colamaria Fabio Filippo
- Colella Domenico
- Collu Alberto
- Colocci Manuel
- Conesa Balbastre Gustavo
- Conesa Del Valle Zaida
- Connors Megan Elizabeth
- Contreras Nuno Jesus Guillermo
- Cormier Thomas Michael
- Corrales Morales Yasser
- Cortes Maldonado Ismael
- Cortese Pietro
- Cosentino Mauro Rogerio
- Costa Filippo
- Crochet Philippe
- Cruz Albino Rigoberto
- Cuautle Flores Eleazar
- Cunqueiro Mendez Leticia
- D'Erasmo Ginevra
- Dainese Andrea
- Dang Ruina
- Danu Andrea
- Das Debasish
- Das Indranil
- Das Kushal
- Das Supriya
- Dash Ajay Kumar
- Dash Sadhana
- De Caro Annalisa
- De Cataldo Giacinto
- De Cuveland Jan
- De Falco Alessandro
- De Gruttola Daniele
- De Marco Nora
- De Pasquale Salvatore
- De Rooij Raoul Stefan
- De Sudipan
- Delagrange Hugues
- Deloff Andrzej
- Denes Ervin Sandor
- Di Bari Domenico
- Di Liberto Sergio
- Di Mauro Antonio
- Di Nezza Pasquale
- Diaz Corchero Miguel Angel
- Dietel Thomas
- Diozcora Vargas Trevino Aurora
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- Wang Yifei
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- Wessels Johannes Peter
- Westerhoff Uwe
- Wiechula Jens
- Wikne Jon
- Wilde Martin Rudolf
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Williams Crispin
- Windelband Bernd Stefan
- Winn Michael Andreas
- Xiang Changzhou
- Yaldo Chris G
- Yamaguchi Yorito
- Yang Hongyan
- Yang Ping
- Yang Shiming
- Yano Satoshi
- Yasnopolskiy Stanislav
- Yi Jungyu
- Yin Zhongbao
- Yoo In-Kwon
- Yushmanov Igor
- Zaccolo Valentina
- Zach Cenek
- Zaman Ali
- Zampolli Chiara
- Zaporozhets Sergey
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zbroszczyk Hanna Paulina
- Zgura Sorin Ion
- Zhalov Mikhail
- Zhang Haitao
- Zhang Xiaoming
- Zhang Yonghong
- Zhao Chengxin
- Zhigareva Natalia
- Zhou Daicui
- Zhou Fengchu
- Zhou You
- Zhu Hongsheng
- Zhu Jianhui
- Zhu Xiangrong
- Zichichi Antonino
- Zimmermann Alice
- Zimmermann Markus Bernhard
- Zinovjev Gennady
- Zoccarato Yannick Denis
- Zynovyev Mykhaylo
- Zyzak Maksym
- Publication venue
- 'World Scientific Pub Co Pte Lt'
- Publication date
- 18/02/2014
- Field of study
ALICE is the heavy-ion experiment at the CERN Large Hadron Collider. The experiment continuously took data during the first physics campaign of the machine from fall 2009 until early 2013, using proton and lead-ion beams. In this paper we describe the running environment and the data handling procedures, and discuss the performance of the ALICE detectors and analysis methods for various physics observables.ALICE is the heavy-ion experiment at the CERN Large Hadron Collider. The experiment continuously took data during the first physics campaign of the machine from fall 2009 until early 2013, using proton and lead-ion beams. In this paper we describe the running environment and the data handling procedures, and discuss the performance of the ALICE detectors and analysis methods for various physics observables.ALICE is the heavy-ion experiment at the CERN Large Hadron Collider. The experiment continuously took data during the first physics campaign of the machine from fall 2009 until early 2013, using proton and lead-ion beams. In this paper we describe the running environment and the data handling procedures, and discuss the performance of the ALICE detectors and analysis methods for various physics observables
Measurement of quarkonium production at forward rapidity in pp collisions at s=7 TeV
- Author
- Abelev B.
- Abramyan Armenuhi
- Adam Jaroslav
- Adamova Dagmar
- Aggarwal Madan Mohan
- Agnello Michelangelo
- Agostinelli Andrea
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Arshad
- Ahmad Nazeer
- Ahmed Ijaz
- Ahn Sang Un
- Ahn Sul-Ah
- Aimo Ilaria
- Aiola Salvatore
- Ajaz Muhammad
- Akindinov Alexander
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alexandre Didier
- Alici Andrea
- Alkin Anton
- Alme Johan
- Alt Torsten
- Altini Valerio
- Altinpinar Sedat
- Altsybeev Igor
- Alves Garcia Prado Caio
- Andrei Cristian
- Andronic Anton
- Anguelov Venelin
- Anielski Jonas
- Anticic Tome
- Antinori Federico
- Antonioli Pietro
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Araujo Silva Figueredo Marcel
- Arbor Nicolas
- Arcelli Silvia
- Armesto Perez Nestor
- Arnaldi Roberta
- Aronsson Tomas
- Arsene Ionut Cristian
- Arslandok Mesut
- Augustinus Andre
- Averbeck Ralf Peter
- Awes Terry
- Azmi Mohd Danish
- Bach Matthias Jakob
- Badala Angela
- Baek Yong Wook
- Bagnasco Stefano
- Bailhache Raphaelle Marie
- Bala Renu
- Baldisseri Alberto
- Ball Markus
- Baltasar Dos Santos Pedrosa Fernando
- Baral Rama Chandra
- Barbera Roberto
- Barile Francesco
- Barnafoldi Gergely Gabor
- Barnby Lee Stuart
- Bartke Jerzy Gustaw
- Basile Maurizio
- Bastid Nicole
- Basu Sumit
- Bathen Bastian
- Batigne Guillaume
- Batyunya Boris
- Batzing Paul Christoph
- Baumann Christoph Heinrich
- Bearden Ian Gardner
- Beck Hans
- Bedda Cristina
- Behera Nirbhay Kumar
- Belikov Iouri
- Bellini Francesca
- Bellwied Rene
- Belmont Moreno Ernesto
- Bencedi Gyula
- Beole Stefania
- Berceanu Ionela
- Bercuci Alexandru
- Berdnikov Yaroslav
- Berenyi Daniel
- Berger Martin Emanuel
- Bertens Redmer Alexander
- Berzano Dario
- Betev Latchezar
- Bhasin Anju
- Bhati Ashok Kumar
- Bhattacharjee Buddhadeb
- Bhom Jihyun
- Bianchi Livio
- Bianchi Nicola
- Bianchin Chiara
- Bielcik Jaroslav
- Bielcikova Jana
- Bilandzic Ante
- Bjelogrlic Sandro
- Blanco Fernando
- Blau Dmitry
- Blume Christoph
- Bock Friederike
- Boehmer Felix Valentin
- Boettger Stefan
- Bogdanov Alexey
- Boggild Hans
- Bogolyubskiy Mikhail
- Boldizsar Laszlo
- Bombara Marek
- Book Julian Heinz
- Borel Herve
- Borissov Alexander
- Bossu Francesco
- Botje Michiel
- Botta Elena
- Braun-Munzinger Peter
- Bregant Marco
- Breitner Timo Gunther
- Broker Theo Alexander
- Browning Tyler Allen
- Broz Michal
- Bruna Elena
- Bruno Giuseppe Eugenio
- Budnikov Dmitry
- Buesching Henner
- Bufalino Stefania
- Buncic Predrag
- Busch Oliver
- Buthelezi Edith Zinhle
- Caffarri Davide
- Cai Xu
- Caines Helen Louise
- Caliva Alberto
- Calvo Villar Ernesto
- Camerini Paolo
- Canoa Roman Veronica
- Carena Francesco
- Carena Wisla
- Castillo Castellanos Javier Ernesto
- Casula Ester Anna Rita
- Catanescu Vasile Ioan
- Cavicchioli Costanza
- Ceballos Sanchez Cesar
- Cepila Jan
- Cerello Piergiorgio
- Chang Beomsu
- Chapeland Sylvain
- Charvet Jean-Luc Fernand
- Chattopadhyay Subhasis
- Chattopadhyay Sukalyan
- Cherney Michael Gerard
- Cheshkov Cvetan Valeriev
- Cheynis Brigitte
- Chibante Barroso Vasco Miguel
- Chochula Peter
- Chojnacki Marek
- Choudhury Subikash
- Christakoglou Panagiotis
- Christensen Christian Holm
- Christiansen Peter
- Chujo Tatsuya
- Chung Suh-Urk
- Cicalo Corrado
- Cifarelli Luisa
- Cindolo Federico
- Cleymans Jean Willy Andre
- Colamaria Fabio Filippo
- Colella Domenico
- Collu Alberto
- Colocci Manuel
- Conesa Balbastre Gustavo
- Conesa Del Valle Zaida
- Connors Megan Elizabeth
- Contreras Nuno Jesus Guillermo
- Cormier Thomas Michael
- Corrales Morales Yasser
- Cortes Maldonado Ismael
- Cortese Pietro
- Cosentino Mauro Rogerio
- Costa Filippo
- Crochet Philippe
- Cruz Albino Rigoberto
- Cuautle Flores Eleazar
- Cunqueiro Mendez Leticia
- D'Erasmo Ginevra
- Dainese Andrea
- Dang Ruina
- Danu Andrea
- Das Debasish
- Das Indranil
- Das Kushal
- Das Supriya
- Dash Ajay Kumar
- Dash Sadhana
- De Caro Annalisa
- De Cataldo Giacinto
- De Cuveland Jan
- De Falco Alessandro
- De Gruttola Daniele
- De Marco Nora
- De Pasquale Salvatore
- De Rooij Raoul Stefan
- De Sudipan
- Delagrange Hugues
- Deloff Andrzej
- Denes Ervin Sandor
- Di Bari Domenico
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- Vorobyev Ivan
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- Vulpescu Bogdan
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- Wang Yifei
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- Westerhoff Uwe
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- Wikne Jon
- Wilde Martin Rudolf
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Williams Crispin
- Windelband Bernd Stefan
- Winn Michael Andreas
- Xiang Changzhou
- Yaldo Chris G
- Yamaguchi Yorito
- Yang Hongyan
- Yang Ping
- Yang Shiming
- Yano Satoshi
- Yasnopolskiy Stanislav
- Yi Jungyu
- Yin Zhongbao
- Yoo In-Kwon
- Yushmanov Igor
- Zaccolo Valentina
- Zach Cenek
- Zaman Ali
- Zampolli Chiara
- Zaporozhets Sergey
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zbroszczyk Hanna Paulina
- Zgura Sorin Ion
- Zhalov Mikhail
- Zhang Haitao
- Zhang Xiaoming
- Zhang Yonghong
- Zhao Chengxin
- Zhigareva Natalia
- Zhou Daicui
- Zhou Fengchu
- Zhou You
- Zhu Hongsheng
- Zhu Jianhui
- Zhu Xiangrong
- Zichichi Antonino
- Zimmermann Alice
- Zimmermann Markus Bernhard
- Zinovjev Gennady
- Zoccarato Yannick Denis
- Zynovyev Mykhaylo
- Zyzak Maksym
- Publication venue
- Springer
- Publication date
- 01/01/2014
- Field of study
The inclusive production cross sections at forward rapidity of J/ψ, ψ(2S), Υ(1S) and Υ(2S) are measured in pp collisions at s = 7 TeV with the ALICE detector at the LHC. The analysis is based on a data sample corresponding to an integrated luminosity of 1.35 pb−1. Quarkonia are reconstructed in the dimuon-decay channel and the signal yields are evaluated by fitting the μ+μ− invariant mass distributions. The differential production cross sections are measured as a function of the transverse momentum pT and rapidity y, over the transverse momentum range 0 < pT < 20 GeV/c for J/ψ and 0 < pT < 12 GeV/c for all other resonances and for 2.5 < y < 4. The measured cross sections integrated over pT and y, and assuming unpolarized quarkonia, are: σJ/ψ=6.69 ± 0.04 ± 0.61 μ b, σψ(2S) = 1.13 ± 0.07 ± 0.14 μb, σΥ(1S) = 54.2 ± 5.0 ± 6.7 nb and σΥ(2S)=18.4 ± 3.7 ± 2.2 nb, where the first uncertainty is statistical and the second one is systematic. These cross sections are obtained assuming unpolarized quarkonium production. The results are compared to measurements performed by other LHC experiments and to theoretical models.The inclusive production cross sections at forward rapidity of J/ψ, ψ(2S), Υ(1S) and Υ(2S) are measured in pp collisions at s=7 TeV with the ALICE detector at the LHC. The analysis is based in a data sample corresponding to an integrated luminosity of 1.35 pb−1. Quarkonia are reconstructed in the dimuon-decay channel and the signal yields are evaluated by fitting the μ+μ− invariant mass distributions. The differential production cross sections are measured as a function of the transverse momentum pT and rapidity y, over the ranges 0<pT<20 GeV/c for J/ψ, 0<pT<12 GeV/c for all other resonances and for 2.5<y<4. The measured cross sections integrated over pT and y, and assuming unpolarized quarkonia, are: σJ/ψ=6.69±0.04±0.63 μb, σψ′=1.13±0.07±0.14 μb, σΥ(1S)=54.2±5.0±6.7 nb and σΥ(2S)=18.4±3.7±2.2 nb, where the first uncertainty is statistical and the second one is systematic. The results are compared to measurements performed by other LHC experiments and to theoretical models.The inclusive production cross sections at forward rapidity of J/ψ , ψ(2S) , Υ (1S) and Υ (2S) are measured in pp collisions at s=7 TeV with the ALICE detector at the LHC. The analysis is based on a data sample corresponding to an integrated luminosity of 1.35 pb−1 . Quarkonia are reconstructed in the dimuon-decay channel and the signal yields are evaluated by fitting the μ+μ− invariant mass distributions. The differential production cross sections are measured as a function of the transverse momentum pT and rapidity y , over the ranges 0<pT<20 GeV/c for J/ψ , 0<pT<12 GeV/c for all other resonances and for 2.5<y<4 . The measured cross sections integrated over pT and y , and assuming unpolarized quarkonia, are: σJ/ψ=6.69±0.04±0.63 \upmu b, σψ(2S)=1.13±0.07±0.19 \upmu b, σΥ(1S)=54.2±5.0±6.7 nb and σΥ(2S)=18.4±3.7±2.9 nb, where the first uncertainty is statistical and the second one is systematic. The results are compared to measurements performed by other LHC experiments and to theoretical models
Centrality, rapidity and transverse momentum dependence of J/ψ suppression in Pb-Pb collisions at sNN=2.76 TeV
- Author
- Abelev Betty Bezverkhny
- Adam Jaroslav
- Adamova Dagmar
- Aggarwal Madan Mohan
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agocs Andras Gabor
- Agostinelli Andrea
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Arshad
- Ahmad Nazeer
- Ahmed Ijaz
- Ahn Sang Un
- Ahn Sul-Ah
- Aimo Ilaria
- Aiola Salvatore
- Ajaz Muhammad
- Akindinov Alexander
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alexandre Didier
- Alici Andrea
- Alkin Anton
- Alme Johan
- Alt Torsten
- Altini Valerio
- Altinpinar Sedat
- Altsybeev Igor
- Alves Garcia Prado Caio
- Andrei Cristian
- Andronic Anton
- Anguelov Venelin
- Anielski Jonas
- Anticic Tome
- Antinori Federico
- Antonioli Pietro
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Araujo Silva Figueredo Marcel
- Arbor Nicolas
- Arcelli Silvia
- Armesto Perez Nestor
- Arnaldi Roberta
- Aronsson Tomas
- Arsene Ionut Cristian
- Arslandok Mesut
- Augustinus Andre
- Averbeck Ralf Peter
- Awes Terry
- Azmi Mohd Danish
- Bach Matthias Jakob
- Badala Angela
- Baek Yong Wook
- Bagnasco Stefano
- Bailhache Raphaelle Marie
- Bairathi Vipul
- Bala Renu
- Baldisseri Alberto
- Baltasar Dos Santos Pedrosa Fernando
- Ban Jaroslav
- Baral Rama Chandra
- Barbera Roberto
- Barile Francesco
- Barnafoldi Gergely Gabor
- Barnby Lee Stuart
- Bartke Jerzy Gustaw
- Basile Maurizio
- Bastid Nicole
- Basu Sumit
- Bathen Bastian
- Batigne Guillaume
- Batyunya Boris
- Batzing Paul Christoph
- Baumann Christoph Heinrich
- Bearden Ian Gardner
- Beck Hans
- Bedda Cristina
- Behera Nirbhay Kumar
- Belikov Iouri
- Bellini Francesca
- Bellwied Rene
- Belmont Moreno Ernesto
- Bencedi Gyula
- Beole Stefania
- Berceanu Ionela
- Bercuci Alexandru
- Berdnikov Yaroslav
- Berenyi Daniel
- Berger Martin Emanuel
- Bergognon Anais Annick Erica
- Bertens Redmer Alexander
- Berzano Dario
- Betev Latchezar
- Bhasin Anju
- Bhati Ashok Kumar
- Bhattacharjee Buddhadeb
- Bhom Jihyun
- Bianchi Livio
- Bianchi Nicola
- Bielcik Jaroslav
- Bielcikova Jana
- Bilandzic Ante
- Bjelogrlic Sandro
- Blanco Fernando
- Blau Dmitry
- Blume Christoph
- Bock Friederike
- Boehmer Felix Valentin
- Boettger Stefan
- Bogdanov Alexey
- Boggild Hans
- Bogolyubskiy Mikhail
- Boldizsar Laszlo
- Bombara Marek
- Book Julian Heinz
- Borel Herve
- Borissov Alexander
- Bornschein Joerg
- Bossu Francesco
- Botje Michiel
- Botta Elena
- Braun-Munzinger Peter
- Bregant Marco
- Breitner Timo Gunther
- Broker Theo Alexander
- Browning Tyler Allen
- Broz Michal
- Bruna Elena
- Bruno Giuseppe Eugenio
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- Wang Yifei
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- Wilde Martin Rudolf
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- Wilkinson Jeremy John
- Williams Crispin
- Windelband Bernd Stefan
- Winn Michael Andreas
- Xiang Changzhou
- Yaldo Chris G
- Yamaguchi Yorito
- Yang Hongyan
- Yang Ping
- Yang Shiming
- Yano Satoshi
- Yasnopolskiy Stanislav
- Yi Jungyu
- Yin Zhongbao
- Yoo In-Kwon
- Yushmanov Igor
- Zaccolo Valentina
- Zach Cenek
- Zaman Ali
- Zampolli Chiara
- Zaporozhets Sergey
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zbroszczyk Hanna Paulina
- Zgura Sorin Ion
- Zhalov Mikhail
- Zhang Fan
- Zhang Haitao
- Zhang Xiaoming
- Zhang Yonghong
- Zhao Chengxin
- Zhou Daicui
- Zhou Fengchu
- Zhou You
- Zhu Hongsheng
- Zhu Jianhui
- Zhu Jianlin
- Zhu Xiangrong
- Zichichi Antonino
- Zimmermann Alice
- Zimmermann Markus Bernhard
- Zinovjev Gennady
- Zoccarato Yannick Denis
- Zynovyev Mykhaylo
- Zyzak Maksym
- Publication venue
- 'Elsevier BV'
- Publication date
- 04/11/2013
- Field of study
The inclusive J/ψ nuclear modification factor (RAA) in Pb-Pb collisions at sNN=2.76TeV has been measured by ALICE as a function of centrality in the e+e− decay channel at mid-rapidity |y| < 0.8 and as a function of centrality, transverse momentum and rapidity in the μ+μ− decay channel at forward-rapidity 2.5 < y < 4.The J/ψ yields measured in Pb-Pb are suppressed compared to those in pp collisions scaled by the number of binary collisions.The RAA integrated over a centrality range corresponding to 90% of the inelastic Pb-Pb cross section is 0.72 +- 0.06 (stat.) +- 0.10 (syst.) at mid-rapidity and 0.57 +- 0.01 (stat.) +- 0.09 (syst.) at forward-rapidity. At low transverse momentum, significantly larger values of RAA are measured at forward-rapidity compared to measurements at lower energy.These features suggest that a contribution to the J/ψ yield originates from charm quarks (re)combination in the deconfined partonic medium.The inclusive J/ψ nuclear modification factor ( RAA ) in Pb–Pb collisions at sNN=2.76 TeV has been measured by ALICE as a function of centrality in the e+e− decay channel at mid-rapidity ( |y|<0.8 ) and as a function of centrality, transverse momentum and rapidity in the μ+μ− decay channel at forward-rapidity ( 2.5<y<4 ). The J/ψ yields measured in Pb–Pb are suppressed compared to those in pp collisions scaled by the number of binary collisions. The RAA integrated over a centrality range corresponding to 90% of the inelastic Pb–Pb cross section is 0.72±0.06(stat.)±0.10(syst.) at mid-rapidity and 0.58±0.01(stat.)±0.09(syst.) at forward-rapidity. At low transverse momentum, significantly larger values of RAA are measured at forward-rapidity compared to measurements at lower energy. These features suggest that a contribution to the J/ψ yield originates from charm quark (re)combination in the deconfined partonic medium.The inclusive J/ψ nuclear modification factor RAA in Pb-Pb collisions at sNN=2.76 TeV has been measured by ALICE as a function of centrality in the e+e− decay channel at mid-rapidity ∣y∣<0.8 and as a function of centrality, transverse momentum and rapidity in the μ+μ− decay channel at forward-rapidity 2.5<y<4.The J/ψ yields measured in Pb-Pb are suppressed compared to those in pp collisions scaled by the number of binary collisions. The RAA integrated over a centrality range corresponding to 90% of the inelastic Pb-Pb cross section is 0.72±0.06 (stat.) ±0.10 (syst.) at mid-rapidity and 0.57±0.01 (stat.) ±0.09 (syst.) at forward-rapidity. At low transverse momentum, significantly larger values of RAA are measured at forward-rapidity compared to measurements at lower energy. These features suggest that a contribution to the J/ψ yield originates from charm quarks (re)combination in the deconfined partonic medium
J/ψ production and nuclear effects in p-Pb collisions at SNN = 5.02 TeV
- Author
- Abelev B.
- Adam Jaroslav
- Adamova Dagmar
- Adare Andrew Marshall
- Aggarwal Madan Mohan
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agocs Andras Gabor
- Agostinelli Andrea
- Ahammed Zubayer
- Ahmad Arshad
- Ahmad Nazeer
- Ahmed Ijaz
- Ahn Sang Un
- Ahn Sul-Ah
- Aimo Ilaria
- Aiola Salvatore
- Ajaz Muhammad
- Akindinov Alexander
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alexandre Didier
- Alici Andrea
- Alkin Anton
- Alme Johan
- Alt Torsten
- Altini Valerio
- Altinpinar Sedat
- Altsybeev Igor
- Alves Garcia Prado Caio
- Andrei Cristian
- Andronic Anton
- Anguelov Venelin
- Anielski Jonas
- Anticic Tome
- Antinori Federico
- Antonioli Pietro
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Araujo Silva Figueredo Marcel
- Arbor Nicolas
- Arcelli Silvia
- Armesto Perez Nestor
- Arnaldi Roberta
- Aronsson Tomas
- Arsene Ionut Cristian
- Arslandok Mesut
- Augustinus Andre
- Averbeck Ralf Peter
- Awes Terry
- Azmi Mohd Danish
- Bach Matthias Jakob
- Badala Angela
- Baek Yong Wook
- Bailhache Raphaelle Marie
- Bairathi Vipul
- Bala Renu
- Baldisseri Alberto
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- Westerhoff Uwe
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- Wikne Jon
- Wilde Martin Rudolf
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Williams Crispin
- Windelband Bernd Stefan
- Winn Michael Andreas
- Xiang Changzhou
- Yaldo Chris G
- Yamaguchi Yorito
- Yang Hongyan
- Yang Ping
- Yang Shiming
- Yano Satoshi
- Yasnopolskiy Stanislav
- Yi Jungyu
- Yin Zhongbao
- Yoo In-Kwon
- Yushmanov Igor
- Zaccolo Valentina
- Zach Cenek
- Zampolli Chiara
- Zaporozhets Sergey
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zbroszczyk Hanna Paulina
- Zelnicek Pierre
- Zgura Sorin Ion
- Zhalov Mikhail
- Zhang Fan
- Zhang Haitao
- Zhang Xiaoming
- Zhang Xiaoming
- Zhang Yonghong
- Zhao Chengxin
- Zhou Daicui
- Zhou Fengchu
- Zhou You
- Zhu Hongsheng
- Zhu Jianhui
- Zhu Jianlin
- Zhu Xiangrong
- Zichichi Antonino
- Zimmermann Alice
- Zimmermann Markus Bernhard
- Zinovjev Gennady
- Zoccarato Y.
- Zoccarato Yannick Denis
- Zynovyev M.
- Zynovyev Mykhaylo
- Zyzak M.
- Zyzak Maksym
- Publication venue
- Springer
- Publication date
- 21/08/2013
- Field of study
Inclusive J/ψ production has been studied with the ALICE detector in p-Pb collisions at sNN = 5.02 TeV at the CERN LHC, in the rapidity domains 2.03 < ycms < 3.53 and −4.46 < ycms < −2.96, down to zero transverse momentum. The J/ψ measurement is performed in the Muon Spectrometer through the μ+μ− decay mode. In this Letter, the J/ψ production cross section and the nuclear modification factor RpPb for the rapidities under study are presented. While at forward rapidity a suppression of the J/ψ yield with respect to binary-scaled pp collisions is observed, in the backward region no suppression is present. The ratio of the forward and backward yields is also shown differentially in rapidity and transverse momentum. Theoretical predictions based on nuclear shadowing, as well as on models including, in addition, a contribution from partonic energy loss, are in fair agreement with the experimental results.Inclusive J/ψ production has been studied with the ALICE detector in p-Pb collisions at the nucleon-nucleon center of mass energy sNN = 5.02 TeV at the CERN LHC. The measurement is performed in the center of mass rapidity domains 2.03<ycms<3.53 and −4.46<ycms<−2.96, down to zero transverse momentum, studying the μ+μ− decay mode. In this paper, the J/ψ production cross section and the nuclear modification factor RpPb for the rapidities under study are presented. While at forward rapidity, corresponding to the proton direction, a suppression of the J/ψ yield with respect to binary-scaled pp collisions is observed, in the backward region no suppression is present. The ratio of the forward and backward yields is also measured differentially in rapidity and transverse momentum. Theoretical predictions based on nuclear shadowing, as well as on models including, in addition, a contribution from partonic energy loss, are in fair agreement with the experimental results
Energy Dependence of the Transverse Momentum Distributions of Charged Particles in pp Collisions Measured by ALICE
- Author
- Abelev Betty
- Adam Jaroslav
- Adamova Dagmar
- Adare Andrew Marshall
- Aggarwal Madan
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agocs Andras Gabor
- Agostinelli Andrea
- Ahammed Zubayer
- Ahmad Arshad
- Ahmad Nazeer
- Ahmed Ijaz
- Ahn Sang Un
- Ahn Sul-Ah
- Aimo Ilaria
- Ajaz Muhammad
- Akindinov Alexander
- Aleksandrov Dmitry
- Alessandro Bruno
- Alexandre Didier
- Alici Andrea
- Alkin Anton
- Alme Johan
- Alt Torsten
- Altini Valerio
- Altinpinar Sedat
- Altsybeev Igor
- Andrei Cristian
- Andronic Anton
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- Yi JunGyu
- Yin Zhongbao
- Yoo In-Kwon
- Yoon Jongik
- Yushmanov Igor
- Zaccolo Valentina
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- Zampolli Chiara
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- Zarochentsev Andrey
- Zavada Petr
- Zaviyalov Nikolai
- Zbroszczyk Hanna Paulina
- Zelnicek Pierre
- Zgura Sorin Ion
- Zhalov Mikhail
- Zhang Fan
- Zhang Haitao
- Zhang Xiaoming
- Zhang Yonghong
- Zhou Daicui
- Zhou Fengchu
- Zhou You
- Zhu Hongsheng
- Zhu Jianhui
- Zhu Jianlin
- Zhu Xiangrong
- Zichichi Antonino
- Zimmermann Alice
- Zinovjev Gennady
- Zoccarato Yannick Denis
- Zynovyev Mykhaylo
- Zyzak Maksym
- Publication venue
- Publication date
- 21/06/2013
- Field of study
Differential cross sections of charged particles in inelastic pp collisions as a function of p_T have been measured at s = 0.9, 2.76 and 7 TeV at the LHC. The pT spectra are compared to NLO-pQCD calculations. Though the differential cross section for an individual s cannot be described by NLO-pQCD, the relative increase of cross section with sqrt(s) is in agreement with NLO-pQCD. Based on these measurements and observations, procedures are discussed to construct pp reference spectra at s = 2.76 and 5.02 TeV up to pT = 50 GeV/c as required for the calculation of the nuclear modification factor in nucleus-nucleus and proton-nucleus collisions
Corrigendum to 'Multi-strange baryon production at mid-rapidity in Pb-Pb collisions at sNN = 2.76 TeV' [Phys. Lett. B 728 (2014) 216-227]
- Author
- Abelev Betty Bezverkhny
- Adam Jaroslav
- Adamova Dagmar
- Adare Andrew Marshall
- Aggarwal Madan Mohan
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agocs Andras Gabor
- Agostinelli Andrea
- Ahammed Zubayer
- Ahmad Arshad
- Ahmad Nazeer
- Ahmed Ijaz
- Ahn Sang Un
- Ahn Sul-Ah
- Aimo Ilaria
- Aiola Salvatore
- Ajaz Muhammad
- Akindinov Alexander
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alexandre Didier
- Alici Andrea
- Alkin Anton
- Alme Johan
- Alt Torsten
- Altini Valerio
- Altinpinar Sedat
- Altsybeev Igor
- Alves Garcia Prado Caio
- Andrei Cristian
- Andronic Anton
- Anguelov Venelin
- Anielski Jonas
- Anticic Tome
- Antinori Federico
- Antonioli Pietro
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Araujo Silva Figueredo Marcel
- Arbor Nicolas
- Arcelli Silvia
- Armesto Perez Nestor
- Arnaldi Roberta
- Aronsson Tomas
- Arsene Ionut Cristian
- Arslandok Mesut
- Augustinus Andre
- Averbeck Ralf Peter
- Awes Terry
- Azmi Mohd Danish
- Bach Matthias Jakob
- Badala Angela
- Baek Yong Wook
- Bailhache Raphaelle Marie
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- Baldisseri Alberto
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- Batyunya Boris
- Batzing Paul Christoph
- Baumann Christoph Heinrich
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- Westerhoff Uwe
- Wiechula Jens
- Wikne Jon
- Wilde Martin Rudolf
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Williams Crispin
- Windelband Bernd Stefan
- Winn Michael Andreas
- Xiang Changzhou
- Yaldo Chris G
- Yamaguchi Yorito
- Yang Hongyan
- Yang Ping
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- Yasnopolskiy Stanislav
- Yi Jungyu
- Yin Zhongbao
- Yoo In-Kwon
- Yushmanov Igor
- Zaccolo Valentina
- Zach Cenek
- Zampolli Chiara
- Zaporozhets Sergey
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zbroszczyk Hanna Paulina
- Zelnicek Pierre
- Zgura Sorin Ion
- Zhalov Mikhail
- Zhang Fan
- Zhang Haitao
- Zhang Xiaoming
- Zhang Yonghong
- Zhou Daicui
- Zhou Fengchu
- Zhou You
- Zhu Hongsheng
- Zhu Jianhui
- Zhu Jianlin
- Zhu Xiangrong
- Zichichi Antonino
- Zimmermann Alice
- Zimmermann Markus Bernhard
- Zinovjev Gennady
- Zoccarato Yannick Denis
- Zynovyev Mykhaylo
- Zyzak Maksym
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2014
- Field of study