9 research outputs found
Magneto-Thermo-Structural Analysis of Power Transformers under Inrush and Short Circuit Conditions
- Author
- Publication venue
- 'MDPI AG'
- Publication date
- 03/06/2021
- Field of study
The main equipment responsible for connection and transmission of electric power from generating centers to consumers are power transformers. This type of equipment is subject to various types of faults that can affect its components, in some cases also compromising its operation and, consequently, the electric power supply. Thus, in this paper, electromagnetic, thermal, and structural analysis of power transformers was carried out with the objective of providing the operator with information on the ideal moment for performing predictive maintenance, avoiding unplanned shutdowns. For this, computational simulations were performed using the finite element method (FEM) and, from that, the different transformer operation ways, nominal currents, inrush current, and short-circuit current were analyzed. In this perspective, analyses of the effects that thermal expansion, axial forces, and radial forces exerted were carried out, contributing to possible defects in this type of equipment. As a study object, simulations were carried out on a 50 MVA single-phase transformer. It is important to emphasize that the simulations were validated with real data of measurements and with results presented in the current literature
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
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- Bhati Ashok Kumar
- Bhattacharjee Buddhadeb
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- 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
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
- 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
- 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
- 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
- Bossu Francesco
- Botje Michiel
- Botta Elena
- 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
- 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
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- Cortese Pietro
- Cosentino Mauro Rogerio
- Costa Filippo
- Crochet Philippe
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- Cuautle Flores Eleazar
- Cunqueiro Mendez Leticia
- D'Erasmo Ginevra
- Dainese Andrea
- Dang Ruina
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- Das Debasish
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- 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
- Divia Roberto
- Djuvsland Oeystein
- Dobrigkeit Chinellato David
- Dobrin Alexandru Florin
- Dobrowolski Tadeusz Antoni
- Doenigus Benjamin
- Domenicis Gimenez Diogenes
- 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
- Ferencei Jozef
- Fernandez Tellez Arturo
- Ferretti Alessandro
- Festanti Andrea
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- Finogeev Dmitry
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- Floratos Emmanouil
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- Foertsch Siegfried Valentin
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- Francescon Andrea
- Frankenfeld Ulrich Michael
- Fuchs Ulrich
- Furget Christophe
- Fusco Girard Mario
- Gaardhoeje Jens Joergen
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- Gallio Mauro
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- Gangadharan Dhevan Raja
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- Ghosh Premomoy
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- Gladysz-Dziadus Ewa
- Glassel Peter
- Gomez Jimenez Ramon
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- Gonzalez Zamora Pedro
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- Grajcarek Robert
- Grelli Alessandro
- Grigoras Alina Gabriela
- Grigoras Costin
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- Grosse-Oetringhaus Jan Fiete
- Grossiord Jean-Yves
- Grosso Raffaele
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- Gulbrandsen Kristjan Herlache
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- Haaland Oystein Senneset
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- Haiduc Maria
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- Hanratty Luke David
- Hansen Alexander
- Harris John William
- Hartmann Helvi
- Harton Austin Vincent
- Hatzifotiadou Despina
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- Heckel Stefan Thomas
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- Helstrup Haavard
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- 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
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
- Bairathi Vipul
- Bala Renu
- Baldisseri Alberto
- Baltasar Dos Santos Pedrosa Fernando
- Ban Jaroslav
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- 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
- Behera Nirbhay Kumar
- Belikov Iouri
- Bellini Francesca
- Bellwied Rene
- Belmont Moreno Ernesto
- Bencedi Gyula
- Beole Stefania
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- Bercuci Alexandru
- Berdnikov Yaroslav
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- Bergognon Anais Annick Erica
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- Boldizsar Laszlo
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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 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
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
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- Bhom Jihyun
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- Bilandzic Ante
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- 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
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- Broker Theo Alexander
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- 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 v2p​i, 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
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
- 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
- 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
- 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
- Divia Roberto
- Djuvsland Oeystein
- Dobrigkeit Chinellato David
- Dobrin Alexandru Florin
- Dobrowolski Tadeusz Antoni
- Doenigus Benjamin
- Domenicis Gimenez Diogenes
- Dordic Olja
- Dorheim Sverre
- Dubey Anand Kumar
- Dubla Andrea
- Ducroux Laurent
- Dupieux Pascal
- Dutt Mazumder Abhee Kanti
- Elia Domenico
- 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
- Ferencei Jozef
- 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
- Ghosh Sanjay Kumar
- 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
- Grion Nevio
- Grosse-Oetringhaus Jan Fiete
- Grossiord Jean-Yves
- Grosso Raffaele
- Grynyov Borys
- Guber Fedor
- Guernane Rachid
- Guerzoni Barbara
- Guilbaud Maxime Rene Joseph
- Gulbrandsen Kristjan Herlache
- Gulkanyan Hrant
- Gunji Taku
- Gupta Anik
- Gupta Ramni
- Haake Rudiger
- Haaland Oystein Senneset
- Hadjidakis Cynthia Marie
- Haiduc Maria
- Hamagaki Hideki
- Hamar Gergoe
- Hanratty Luke David
- Hansen Alexander
- Harris John William
- Hartmann Helvi
- Harton Austin Vincent
- Hatzifotiadou Despina
- Hayashi Shinichi
- Hayrapetyan Arsen
- Heckel Stefan Thomas
- Heide Markus Ansgar
- Helstrup Haavard
- Herghelegiu Andrei Ionut
- Herrera Corral Gerardo Antonio
- Hess Benjamin Andreas
- Hetland Kristin Fanebust
- Hicks Bernard Richard
- Hippolyte Boris
- Hladky Jan
- Hristov Peter Zahariev
- Huang Meidana
- Humanic Thomas
- Hutter Dirk
- Hwang Dae Sung
- Ianigro Jean-Christophe
- Ilkaev Radiy
- Ilkiv Iryna
- Inaba Motoi
- Incani Elisa
- Innocenti Gian Michele
- Ionita Costin
- Ippolitov Mikhail
- Irfan Muhammad
- Ivanov Marian
- Ivanov Vladimir
- Ivanytskyi Oleksii
- Jacholkowski Adam Wlodzimierz
- Jacobs Peter Martin
- Jahnke Cristiane
- Jang Haeng Jin
- Janik Malgorzata Anna
- Jena Satyajit
- Jimenez Bustamante Raul Tonatiuh
- Jones Peter Graham
- Jung Hyungtaik
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- Kalcher Sebastian
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- Kalweit Alexander Philipp
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- Kluge Alexander
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- Knospe Anders Garritt
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- Kollegger Thorsten
- Kolozhvari Anatoly
- Kondratev Valerii
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- Konevskikh Artem
- Kovalenko Vladimir
- Kowalski Marek
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- Kral Jiri
- Kralik Ivan
- Kramer Frederick
- Kravcakova Adela
- Krelina Michal
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- Krivda Marian
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- Krzewicki Mikolaj
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- Kweon Min Jung
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- Lardeux Antoine Xavier
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- Legrand Iosif
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- Lu Xianguo
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- Lunardon Marcello
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- Symons Timothy
- Szanto De Toledo Alejandro
- Szarka Imrich
- Szczepankiewicz Adam
- Szymanski Maciej Pawel
- Takahashi Jun
- Tangaro Marco-Antonio
- Tapia Takaki Daniel Jesus
- Tarantola Peloni Attilio
- Tarazona Martinez Alfonso
- Tauro Arturo
- Tejeda Munoz Guillermo
- Telesca Adriana
- Ter-Minasyan Astkhik
- Terrevoli Cristina
- Thaeder Jochen Mathias
- Thomas Deepa
- Tieulent Raphael Noel
- Timmins Anthony Robert
- Toia Alberica
- Torii Hisayuki
- Trubnikov Victor
- Trzaska Wladyslaw Henryk
- Tsuji Tomoya
- Tumkin Alexandr
- Turrisi Rosario
- Tveter Trine Spedstad
- Ulery Jason Glyndwr
- Ullaland Kjetil
- Ulrich Jochen
- Uras Antonio
- Usai Gianluca
- Vajzer Michal
- Vala Martin
- Valencia Palomo Lizardo
- Vallero Sara
- Van Hoorne Jacobus Willem
- Van Leeuwen Marco
- Vande Vyvre Pierre
- Vannucci Luigi
- Vargas Trevino Aurora Diozcora
- Varma Raghava
- Vasileiou Maria
- Vasiliev Andrey
- Vechernin Vladimir
- Veldhoen Misha
- Venaruzzo Massimo
- Vercellin Ermanno
- Vergara Limon Sergio
- Vernet Renaud
- Verweij Marta
- Vickovic Linda
- Viesti Giuseppe
- Viinikainen Jussi Samuli
- Vilakazi Zabulon
- Villalobos Baillie Orlando
- Vinogradov Alexander
- Vinogradov Leonid
- Vinogradov Yury
- Virgili Tiziano
- Viyogi Yogendra
- Vodopyanov Alexander
- Volkl Martin Andreas
- Voloshin Kirill
- Voloshin Sergey
- Volpe Giacomo
- Von Haller Barthelemy
- Vorobyev Ivan
- Vranic Danilo
- Vrlakova Janka
- Vulpescu Bogdan
- Vyushin Alexey
- Wagner Boris
- Wagner Jan
- Wagner Vladimir
- Wang Mengliang
- Wang Yifei
- Watanabe Daisuke
- 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
- 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
Two- and three-pion quantum statistics correlations in Pb-Pb collisions at sNN​​= 2.76 TeV at the CERN Large Hadron Collider
- 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
- 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
- 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
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- Connors Megan Elizabeth
- Contin Giacomo
- Contreras Nuno Jesus Guillermo
- Cormier Thomas Michael
- Corrales Morales Yasser
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- Das Debasish
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- Dash Sadhana
- De Caro Annalisa
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- De Falco Alessandro
- De Gruttola Daniele
- De Marco Nora
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- De Rooij Raoul Stefan
- De Sudipan
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- Denes Ervin Sandor
- Di Bari Domenico
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- Diaz Corchero Miguel Angel
- Dietel Thomas
- Divia Roberto
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- Dorheim Sverre
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- Dubla Andrea
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- Dupieux Pascal
- Dutt Mazumder Abhee Kanti
- Elia Domenico
- 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
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- Feliciello Alessandro
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- Ferencei Jozef
- Fernandez Tellez Arturo
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- Festanti Andrea
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- Filchagin Sergey
- Finogeev Dmitry
- Fionda Fiorella
- Fiore Enrichetta Maria
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- 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
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- 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
- Ghosh Sanjay Kumar
- 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
- Grion Nevio
- Grosse-Oetringhaus Jan Fiete
- Grossiord Jean-Yves
- Grosso Raffaele
- Grynyov Borys
- Guber Fedor
- Guernane Rachid
- Guerzoni Barbara
- Guilbaud Maxime Rene Joseph
- Gulbrandsen Kristjan Herlache
- Gulkanyan Hrant
- Gunji Taku
- Gupta Anik
- Gupta Ramni
- Haake Rudiger
- Haaland Oystein Senneset
- Hadjidakis Cynthia Marie
- Haiduc Maria
- Hamagaki Hideki
- Hamar Gergoe
- Hanratty Luke David
- Hansen Alexander
- Harris John William
- Hartmann Helvi
- Harton Austin Vincent
- Hatzifotiadou Despina
- Hayashi Shinichi
- Hayrapetyan Arsen
- Heckel Stefan Thomas
- Heide Markus Ansgar
- Helstrup Haavard
- Herghelegiu Andrei Ionut
- Herrera Corral Gerardo Antonio
- Hess Benjamin Andreas
- Hetland Kristin Fanebust
- Hicks Bernard Richard
- Hippolyte Boris
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- Huang Meidana
- Humanic Thomas
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- Ianigro Jean-Christophe
- Ilkaev Radiy
- Ilkiv Iryna
- Inaba Motoi
- Incani Elisa
- Innocenti Gian Michele
- Ionita Costin
- Ippolitov Mikhail
- Irfan Muhammad
- Ivanov Marian
- Ivanov Vladimir
- Ivanytskyi Oleksii
- Jacholkowski Adam Wlodzimierz
- Jacobs Peter Martin
- Jahnke Cristiane
- Jang Haeng Jin
- Janik Malgorzata Anna
- Jena Satyajit
- Jimenez Bustamante Raul Tonatiuh
- Jones Peter Graham
- Jung Hyungtaik
- Jusko Anton
- Kalcher Sebastian
- Kalinak Peter
- Kalweit Alexander Philipp
- Kamin Jason Adrian
- Kang Ju Hwan
- Kaplin Vladimir
- Kar Somnath
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- Karavichev Oleg
- Karavicheva Tatiana
- Karpechev Evgeny
- Kebschull Udo Wolfgang
- Keidel Ralf
- Ketzer Bernhard Franz
- Khan Kamal
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- Khanzadeev Alexei
- Kharlov Yury
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- Kiss Gabor
- Klay Jennifer Lynn
- Klein Jochen
- Klein-Boesing Christian
- Kluge Alexander
- Knichel Michael Linus
- Knospe Anders Garritt
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- Kohler Markus Konrad
- Kollegger Thorsten
- Kolozhvari Anatoly
- Kondratev Valerii
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- Kovalenko Vladimir
- Kowalski Marek
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- Lakomov Igor
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- Read Kenneth Francis
- Real Jean-Sebastien
- Redlich Krzysztof
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- Rehman Attiq Ur
- Reichelt Patrick Simon
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- Renfordt Rainer Arno Ernst
- Reolon Anna Rita
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- Schmidt Christian Joachim
- Schmidt Hans Rudolf
- Schuchmann Simone
- Schukraft Jurgen
- Schulc Martin
- Schuster Tim Robin
- Schutz Yves Roland
- Schwarz Kilian Eberhard
- Schweda Kai Oliver
- Scioli Gilda
- Scomparin Enrico
- Scott Patrick Aaron
- Scott Rebecca Michelle
- Segato Gianfranco
- Seger Janet Elizabeth
- Selyuzhenkov Ilya
- Seo Jeewon
- Serradilla Rodriguez Eulogio
- Sevcenco Adrian
- Shabetai Alexandre
- Shabratova Galina
- Shahoyan Ruben
- Shangaraev Artem
- Sharma Natasha
- Sharma Rohni
- Sharma Satish
- Shigaki Kenta
- Shtejer Diaz Katherin
- Sibiryak Yury
- Siddhanta Sabyasachi
- Siemiarczuk Teodor
- Silvermyr David Olle Rickard
- Silvestre Catherine Micaela
- Simatovic Goran
- Singaraju Rama Narayana
- Singh Ranbir
- Singha Subhash
- Singhal Vikas
- Sinha Bikash
- Sitar Branislav
- Sitta Mario
- Skaali Bernhard
- Skjerdal Kyrre
- Smakal Radek
- Smirnov Nikolai
- Snellings Raimond
- Soegaard Carsten
- Soltz Ron Ariel
- Song Jihye
- Song Myunggeun
- Soramel Francesca
- Sorensen Soren Pontoppidan
- Spacek Michal
- Sputowska Iwona Anna
- Spyropoulou-Stassinaki Martha
- Srivastava Brijesh Kumar
- Stachel Johanna
- Stan Ionel
- Stefanek Grzegorz
- Steinpreis Matthew Donald
- Stenlund Evert Anders
- Steyn Gideon Francois
- Stiller Johannes Hendrik
- Stocco Diego
- Stolpovskiy Mikhail
- Strmen Peter
- Subieta Vasquez Martin Alfonso
- Sugitate Toru
- Suire Christophe Pierre
- Suleymanov Mais Kazim Oglu
- Sultanov Rishat
- Sumbera Michal
- Susa Tatjana
- Symons Timothy
- Szanto De Toledo Alejandro
- Szarka Imrich
- Szczepankiewicz Adam
- Szymanski Maciej Pawel
- Takahashi Jun
- Tangaro Marco-Antonio
- Tapia Takaki Daniel Jesus
- Tarantola Peloni Attilio
- Tarazona Martinez Alfonso
- Tauro Arturo
- Tejeda Munoz Guillermo
- Telesca Adriana
- Ter-Minasyan Astkhik
- Terrevoli Cristina
- Thaeder Jochen Mathias
- Thomas Deepa
- Tieulent Raphael Noel
- Timmins Anthony Robert
- Toia Alberica
- Torii Hisayuki
- Trubnikov Victor
- Trzaska Wladyslaw Henryk
- Tsuji Tomoya
- Tumkin Alexandr
- Turrisi Rosario
- Tveter Trine Spedstad
- Ulery Jason Glyndwr
- Ullaland Kjetil
- Ulrich Jochen
- Uras Antonio
- Usai Gianluca
- Vajzer Michal
- Vala Martin
- Valencia Palomo Lizardo
- Vallero Sara
- Van Hoorne Jacobus Willem
- Van Leeuwen Marco
- Vande Vyvre Pierre
- Vannucci Luigi
- Vargas Trevino Aurora Diozcora
- Varma Raghava
- Vasileiou Maria
- Vasiliev Andrey
- Vechernin Vladimir
- Veldhoen Misha
- Venaruzzo Massimo
- Vercellin Ermanno
- Vergara Limon Sergio
- Vernet Renaud
- Verweij Marta
- Vickovic Linda
- Viesti Giuseppe
- Viinikainen Jussi Samuli
- Vilakazi Zabulon
- Villalobos Baillie Orlando
- Vinogradov Alexander
- Vinogradov Leonid
- Vinogradov Yury
- Virgili Tiziano
- Viyogi Yogendra
- Vodopyanov Alexander
- Volkl Martin Andreas
- Voloshin Kirill
- Voloshin Sergey
- Volpe Giacomo
- Von Haller Barthelemy
- Vorobyev Ivan
- Vranic Danilo
- Vrlakova Janka
- Vulpescu Bogdan
- Vyushin Alexey
- Wagner Boris
- Wagner Jan
- Wagner Vladimir
- Wang Mengliang
- Wang Yifei
- Watanabe Daisuke
- 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
- 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
- 'American Physical Society (APS)'
- Publication date
- 21/10/2013
- Field of study
Correlations induced by quantum statistics are sensitive to the spatio-temporal extent as well as dynamics of particle emitting sources in heavy-ion collisions. In addition, such correlations can be used to search for the presence of a coherent component of pion production. Two and three-pion correlations of same and mixed-charge are measured at low relative momentum to estimate the coherent fraction of charged pions in Pb-Pb collisions at sNN​​= 2.76 TeV at the LHC with ALICE. The genuine three-pion quantum statistics correlation is found to be suppressed relative to the two-pion correlation based on the assumption of fully chaotic pion emission.The suppression is observed to decrease with triplet momentum. The observed suppression at low triplet momentum may correspond to a coherent fraction in charged pion emission of 22% +- 12%.Correlations induced by quantum statistics are sensitive to the spatio-temporal extent as well as dynamics of particle emitting sources in heavy-ion collisions. In addition, such correlations can be used to search for the presence of a coherent component of pion production. Two and three-pion correlations of same and mixed-charge are measured at low relative momentum to estimate the coherent fraction of charged pions in Pb-Pb collisions at sNN​​=2.76 TeV at the LHC with ALICE. The genuine three-pion quantum statistics correlation is found to be suppressed relative to the two-pion correlation based on the assumption of fully chaotic pion emission. The suppression is observed to decrease with triplet momentum. The observed suppression at low triplet momentum may correspond to a coherent fraction in charged pion emission of 23% ± 8%.Correlations induced by quantum statistics are sensitive to the spatiotemporal extent as well as dynamics of particle-emitting sources in heavy-ion collisions. In addition, such correlations can be used to search for the presence of a coherent component of pion production. Two- and three-pion correlations of same and mixed charge are measured at low relative momentum to estimate the coherent fraction of charged pions in Pb-Pb collisions at sNN=2.76 TeV at the CERN Large Hadron Collider with ALICE. The genuine three-pion quantum statistics correlation is found to be suppressed relative to the two-pion correlation based on the assumption of fully chaotic pion emission. The suppression is observed to decrease with triplet momentum. The observed suppression at low triplet momentum may correspond to a coherent fraction in charged-pion emission of 23%±8%.</p