227 research outputs found
Direct photon elliptic flow in Pb-Pb collisions at root s(NN)=2.76 TeV
- Author
- A
- A
- A
- A
- A
- A
- A
- A. Gomez and Gonzalez
- A. J
- A. Karasu and Karavichev
- Acosta F. T
- Adamova D
- Adolfsson J
- Aggarwal M. M
- Agrawal N
- Ahammed Z
- Ahn S. U
- Aiola S
- Akindinov A
- Al-Turany M
- Alam S. N
- Albuquerque D. S. D
- Aleksandrov D
- Alessandro B
- Alfaro Molina R
- Ali Y
- ALICE Collaboration
- Alici A
- Alkin A
- Alme J
- Alt T
- Altenkamper L
- Altsybeev
- Andrei C
- Andreou D
- Andrews H. A
- Andronic A
- Angeletti M
- Anguelov
- Anticic T
- Antinori F
- Antonioli P
- Anwar R
- Apadula N
- Aphecetche L
- Appelshaeuser H
- Arcelli S
- Arnaldi R
- Arnold O. W
- Arratia M
- Arsene I. C
- Arslandok M
- Augustinus A
- Averbeck R
- Azmi M. D
- B
- Badala A
- Baek Y. W
- Bagnasco S
- Bailhache R
- Baillie
- Bala R
- Balbastre
- Baldisseri A
- Ball M
- Baral R. C
- Barbano A. M
- Barbera R
- Barile F
- Barioglio L
- Barnafoldi G. G
- Barnby L. S
- Barret
- Barroso
- Barth K
- Bartsch E
- Bastid N
- Basu S
- Batigne G
- Batyunya B
- Batzing P. C
- Bazo Alba J. L
- Bearden I. G
- Beck H
- Bedda C
- Behera N. K
- Belikov
- Bello Martinez H
- Bellwied R
- Beltran L. G. E
- Belyaev
- Beole S
- Bercuci A
- Berdnikov Y
- Berenyi D
- Bertens R. A
- Berzano D
- Betev L
- Bhaduri P. P
- Bhasin A
- Bhat I. R
- Bhatt H
- Bhattacharjee B
- Bhom J
- Bianchi A
- Bianchi L
- Bianchi N
- Bielcik J
- Bielcikova J
- Bilandzic A
- Biro G
- Biswas R
- Biswas S
- Blair J. T
- Blau D
- Blume C
- Boca G
- Bock F
- Bogdanov A
- Boldizsar L
- Bombara M
- Bonomi G
- Bonora M
- Borel H
- Borissov A
- Borri M
- Botta E
- Bourjau C
- Bratrud L
- Braun-Munzinger P
- Bregant M
- Broker T. A
- Broz M
- Brucken E. J
- Bruna E
- Bruno G. E
- Budnikov D
- Buesching H
- Bufalino S
- Buhler P
- Buncic P
- Busch O
- Bustamante
- Buthelezi Z
- Butt J. B
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- Caffarri D
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- Carnesecchi F
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- Chattopadhyay S
- Chauvin A
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- Chochula P
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- Christensen C. H
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- De Falco A
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- Domenicis Gimenez D
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- Guernane R
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- Gupta A
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- Guzman I. B
- H. Pereira and Peresunko
- Haake R
- Habib M. K
- Hadjidakis C
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- Hannigan R
- Haque M. R
- Harlenderova A
- Harris J. W
- Harton A
- Hassan H
- Hatzifotiadou D
- Hauer P
- Hayashi S
- Heckel S. T
- Hellbaer E
- Helstrup H
- Herghelegiu A
- Hernandez E. G
- Herrera Corral G
- Herrmann F
- Hetland K. F
- Hilden T. E
- Hillemanns H
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- Horak D
- Hornung S
- Hosokawa R
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- Hughes C
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- Humanic T. J
- Hushnud H
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- Hussain T
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- Hwang D. S
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- Iddon J. P
- Iga Buitron S. A
- Ilkaev R
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- Jakubowska M. J
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- Kalweit A
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- Mike and Acharya
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- Utrobicic A
- Uysal
- V
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- V and Anson
- V and Bartalini
- V and Bencedi
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- V and Sinha
- V and Trzaska
- V and Zaccolo
- V and Zaman
- V and Zhigareva
- V. Chibante and Chinellato
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- Xu R
- Y
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- Yalcin S
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- Yano S
- Yin Z
- Yokoyama H
- Yoo
- Yurchenko
- Z. Conesa and Contreras
- Zampolli C
- Zanoli H. J. C
- Zardoshti N
- Zarochentsev A
- Zavada P
- Zaviyalov N
- Zbroszczyk H
- Zhalov M
- Zhang X
- Zhang Y
- Zhang Z
- Zhao C
- Zherebchevskii
- Zhou D
- Zhou Y
- Zhou Z
- Zhu H
- Zhu J
- Zhu Y
- Zichichi A
- Zimmermann M. B
- Zinovjev G
- Zmeskal J
- Zou S
- Publication venue
- Publication date
- 01/01/2018
- Field of study
The elliptic flow of inclusive and direct photons was measured at mid-rapidity in two centrality classes 0-20% and 20-40% in Pb-Pb collisions at root s(NN) = 2.76 TeV by ALICE. Photons were detected with the highly segmented electromagnetic calorimeter PHOS and via conversions in the detector material with the e(broken vertical bar)e pairs reconstructed in the central tracking system. The results of the two methods were combined and the direct-photon elliptic flow was extracted in the transverse momentum range 0.9 < p(T) < 6.2 GeV/c. A comparison to RHIC data shows a similar magnitude of the measured direct-photon elliptic flow. Hydrodynamic and transport model calculations are systematically lower than the data, but are found to be compatible. (C) 2018 The Author. Published by Elsevier B.V.Peer reviewe
Higher moment fluctuations of identified particle distributions from ALICE
- Author
- Behera
- Nirbhay Kumar and Acharya
- S
- Acosta F. T
- Adamova D
- Adolfsson J
- Aggarwal M. M
- Rinella
- G. Aglieri and Agnello
- M
- Agrawal N
- Ahammed Z
- Ahn S. U
- Aiola S
- Akindinov A
- Al-Turany M
- Alam S. N
- Albuquerque D. S. D
- Aleksandrov D
- Alessandro B
- Alfaro Molina R
- Ali Y
- Alici A
- Alkin A
- Alme J
- Alt T
- Altenkamper L
- Altsybeev
- I and Anaam
- M. N
- Andrei C
- Andreou D
- Andrews H. A
- Andronic A
- Angeletti M
- Anguelov
- V and Anson
- C
- Anticic T
- Antinori F
- Antonioli P
- Anwar R
- Apadula N
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- Yamakawa K
- Yano S
- Yin Z
- Yokoyama H
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- I-K and Yoon
- J. H
- Yurchenko
- V and Zaccolo
- V and Zaman
- A
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- Zanoli H. J. C
- Zardoshti N
- Zarochentsev A
- Zavada P
- Zaviyalov N
- Zbroszczyk H
- Zhalov M
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- Zinovjev G
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- Zou S
- Alice Collaboration
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2012
- Field of study
Cumulants of conserved charges fluctuations are regarded as a potential tool
to study the criticality in the QCD phase diagram and to determine the
freeze-out parameters in a model-independent way. At LHC energies, the
measurements of the ratio of the net-baryon (net-proton) cumulants can be used
to test the lattice QCD predictions. In this work, we present the first
measurements of cumulants of the net-proton number distributions up to 4th
order in Pb--Pb collisions at sNN = 2.76 and 5.02 TeV as a
function of collision centrality. We compare our cumulant ratios results with
the STAR experiment net-proton results measured in the first phase of the Beam
Energy Scan program at RHIC. The results can be used to obtain the chemical
freeze-out parameters at LHC.Comment: 4 pages, 3 figures, Proceedings of XXVIIth International Conference
on Ultrarelativistic Nucleus-Nucleus Collisions (Quark Matter 2018
Spin alignment measurements using vector mesons with ALICE detector at the LHC
- Author
- A
- A
- A
- A
- A
- A
- A
- A. Gomez and Gonzalez
- A. J
- A. Karasu and Karavichev
- Acosta F. T
- Adamova D
- Adolfsson J
- Aggarwal M. M
- Agrawal N
- Ahammed Z
- Ahn S. U
- Aiola S
- Akindinov A
- Al-Turany M
- Alam S. N
- Albuquerque D. S. D
- Aleksandrov D
- Alessandro B
- Alfaro Molina R
- Ali Y
- Alice Collaboration
- Alici A
- Alkin A
- Alme J
- Alt T
- Altenkamper L
- Altsybeev
- Andrei C
- Andreou D
- Andrews H. A
- Andronic A
- Angeletti M
- Anguelov
- Anticic T
- Antinori F
- Antonioli P
- Anwar R
- Apadula N
- Aphecetche L
- Appelshaeuser H
- Arcelli S
- Arnaldi R
- Arnold O. W
- Arratia M
- Arsene I. C
- Arslandok M
- Augustinus A
- Averbeck R
- Azmi M. D
- B
- Badala A
- Baek Y. W
- Bagnasco S
- Bailhache R
- Baillie
- Bala R
- Balbastre
- Baldisseri A
- Ball M
- Baral R. C
- Barbano A. M
- Barbera R
- Barile F
- Barioglio L
- Barnafoldi G. G
- Barnby L. S
- Barret
- Barroso
- Barth K
- Bartsch E
- Bastid N
- Basu S
- Batigne G
- Batyunya B
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- Witt W. E
- Xu R
- Y
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- Yalcin S
- Yamakawa K
- Yano S
- Yin Z
- Yokoyama H
- Yoo
- Yurchenko
- Z. Conesa and Contreras
- Zampolli C
- Zanoli H. J. C
- Zardoshti N
- Zarochentsev A
- Zavada P
- Zaviyalov N
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- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2019
- Field of study
We present new measurements related to spin alignment of K*(0) vector
mesons at mid-rapidity for Pb-Pb collisions at root s(NN) = 2.76 and
5.02 TeV. The spin alignment measurements are carried out with respect
to production plane and 2nd order event plane. At low p(T) the spin
density matrix element rho(00) for K*(0) is found to have values
slightly below 1/3, while it is consistent with 1/3, i.e. no spin
alignment, at high p(T). Similar values of rho(00) are observed with
respect to both production plane and event plane. Within statistical and
systematic uncertainties, rho(00) values are also found to be
independent of root s(NN). rho(00) also shows centrality dependence with
maximum deviation from 1/3 for mid-central collisions with respect to
both the kinematic planes. The measurements for K*(0) in pp collisions
at root s = 13 TeV and for K-s(0) (a spin 0 hadron) in 20-40\% central
Pb-Pb collisions at root s(NN) = 2.76 TeV are consistent with no spin
alignment
Muon physics at forward rapidity with the ALICE detector upgrade
- Author
- A
- A
- A
- A
- A
- A
- A
- A. Gomez and Gonzalez
- A. J
- A. Karasu and Karavichev
- Acosta F. T
- Adamova D
- Adolfsson J
- Aggarwal M. M
- Agrawal N
- Ahammed Z
- Ahn S. U
- Aiola S
- Akindinov A
- Al-Turany M
- Alam S. N
- Albuquerque D. S. D
- Aleksandrov D
- Alessandro B
- Alfaro Molina R
- Ali Y
- Alice Collaboration
- Alici A
- Alkin A
- Alme J
- Alt T
- Altenkamper L
- Altsybeev
- Andrei C
- Andreou D
- Andrews H. A
- Andronic A
- Angeletti M
- Anguelov
- Anticic T
- Antinori F
- Antonioli P
- Anwar R
- Apadula N
- Aphecetche L
- Appelshaeuser H
- Arcelli S
- Arnaldi R
- Arnold O. W
- Arratia M
- Arsene I. C
- Arslandok M
- Augustinus A
- Averbeck R
- Azmi M. D
- B
- Badala A
- Baek Y. W
- Bagnasco S
- Bailhache R
- Baillie
- Bala R
- Balbastre
- Baldisseri A
- Ball M
- Baral R. C
- Barbano A. M
- Barbera R
- Barile F
- Barioglio L
- Barnafoldi G. G
- Barnby L. S
- Barret
- Barroso
- Barth K
- Bartsch E
- Bastid N
- Basu S
- Batigne G
- Batyunya B
- Batzing P. C
- Bazo Alba J. L
- Bearden I. G
- Beck H
- Bedda C
- Behera N. K
- Belikov
- Bello Martinez H
- Bellwied R
- Beltran L. G. E
- Belyaev
- Beole S
- Bercuci A
- Berdnikov Y
- Berenyi D
- Bertens R. A
- Berzano D
- Betev L
- Bhaduri P. P
- Bhasin A
- Bhat I. R
- Bhatt H
- Bhattacharjee B
- Bhom J
- Bianchi A
- Bianchi L
- Bianchi N
- Bielcik J
- Bielcikova J
- Bilandzic A
- Biro G
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- Usai G. L
- Utrobicic A
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- V and Anson
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- V and Gonzalez-Zamora
- V and Graczykowski
- V and Grigoryan
- V and Izucheev
- V and Jacak
- V and Kar
- V and Kowalski
- V and Kuhn
- V and Lindsay
- V and Liu
- V and Loizides
- V and Manso
- V and Mao
- V and Mudnic
- V and Noferini
- V and Pagano
- V and Pareek
- V and Pestov
- V and Petrovici
- V and Prasad
- V and Putschke
- V and Ravasenga
- V and Richert
- V and Sandoval
- V and Sinha
- V and Trzaska
- V and Zaccolo
- V and Zaman
- V and Zhigareva
- V
- V
- V
- V
- V
- V. Chibante and Chinellato
- Vala M
- van Doremalen L. V. R
- Van Hoorne J. W
- van Leeuwen M
- Vande Vyvre P
- Varga D
- Vargas A
- Vargyas M
- Varma R
- Vasileiou M
- Vasiliev A
- Vauthier A
- Veen A. M
- Vercellin E
- Vergara Limon S
- Vermunt L
- Vernet R
- Vertesi R
- Vickovic L
- Viinikainen J
- Vilakazi Z
- Vinogradov A
- Virgili T
- Vislavicius V
- Vodopyanov A
- Volkl M. A
- Voloshin K
- Voloshin S. A
- Volpe G
- von Haller B
- Vorobyev
- Vranic D
- Vrlakova J
- W. H
- Wagner B
- Wang H
- Wang M
- Watanabe Y
- Weber M
- Weber S. G
- Wegrzynek A
- Weiser D. F
- Wenzel S. C
- Wessels J. P
- Westerhoff U
- Whitehead A. M
- Wiechula J
- Wikne J
- Wilk G
- Wilkinson J
- Willems G. A
- Williams M. C. S
- Willsher E
- Windelband B
- Witt W. E
- Xu R
- Y
- Y
- Y. Corrales and Cortese
- Yalcin S
- Yamakawa K
- Yano S
- Yin Z
- Yokoyama H
- Yoo
- Yurchenko
- Z. Conesa and Contreras
- Zampolli C
- Zanoli H. J. C
- Zardoshti N
- Zarochentsev A
- Zavada P
- Zaviyalov N
- Zbroszczyk H
- Zhalov M
- Zhang X
- Zhang Y
- Zhang Z
- Zhao C
- Zherebchevskii
- Zhou D
- Zhou Y
- Zhou Z
- Zhu H
- Zhu J
- Zhu Y
- Zichichi A
- Zimmermann M. B
- Zinovjev G
- Zmeskal J
- Zou S
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2019
- Field of study
ALICE is the experiment specifically designed to study the Quark-Gluon
Plasma (QGP) in heavy-ion collisions at the CERN LHC. The ALICE detector
will be upgraded during the Long Shutdown 2, planned for 2019-2020, in
order to cope with the maximum interaction rate of 50 kHz of Pb-Pb
collisions foreseen for Runs 3 and 4. The ambitious programme of
high-precision measurements, expected for muon physics after 2020,
requires an upgrade of the front-end and readout electronics of the
existing Muon Spectrometer. This concerns the Cathode Pad Chambers (CPC)
used for tracking and the Resistive Plate Chambers (RPC) used for
triggering and for muon identification. The Muon Forward Tracker (MFT),
an internal tracker added in front of the front absorber of the existing
Muon Spectrometer, is also part of the ALICE detector upgrade programme.
It is based on an assembly of circular planes made of Monolithic Active
Pixel Sensors (MAPS), covering the pseudorapidity range 2.5 < eta < 3.6.
The MFT will improve present measurements and enable new ones. A
selection of results from physics performance studies will be presented,
together with an overview of the technical aspects of the upgrade
project
Measuring (KSK +/-)-K-0 interactions using pp collisions at root s=7 TeV
- Author
- A
- A
- A
- A
- A
- A
- A
- A. Gomez and Gonzalez
- A. J
- A. Karasu and Karavichev
- Acharya S
- Acosta F. T
- Adamova D
- Adler A
- Adolfsson J
- Aggarwal M. M
- Agrawal N
- Ahammed Z
- Ahn S. U
- Aiola S
- Akindinov A
- Al-Turany M
- Alam S. N
- Albuquerque D. S. D
- Aleksandrov D
- Alessandro B
- Alfanda H. M
- ALICE Collaboration
- Alici A
- Alkin A
- Alme J
- Alt T
- Altenkamper L
- Altsybeev
- Andrei C
- Andreou D
- Andrews H. A
- Andronic A
- Angeletti M
- Anguelov
- Anticic T
- Antinori F
- Antonioli P
- Anwar R
- Apadula N
- Aphecetche L
- Appelshaeuser H
- Arcelli S
- Arnaldi R
- Arratia M
- Arsene I. C
- Arslandok M
- Augustinus A
- Averbeck R
- Azmi M. D
- B
- Badala A
- Baek Y. W
- Bagnasco S
- Bailhache R
- Baillie
- Bala R
- Balbastre
- Baldisseri A
- Ball M
- Baral R. C
- Barbano A. M
- Barbera R
- Barile F
- Barioglio L
- Barnafoldi G. G
- Barnby L. S
- Barret
- Barroso
- Barth K
- Bartsch E
- Bastid N
- Basu S
- Batigne G
- Batyunya B
- Batzing P. C
- Bazo Alba J. L
- Bearden I. G
- Beck H
- Bedda C
- Behera N. K
- Belikov
- Bello Martinez H
- Bellwied R
- Beltran L. G. E
- Belyaev
- Beole S
- Bercuci A
- Berdnikov Y
- Berenyi D
- Bertens R. A
- Berzano D
- Betev L
- Bhaduri P. P
- Bhasin A
- Bhat I. R
- Bhatt H
- Bhattacharjee B
- Bhom J
- Bianchi A
- Bianchi L
- Bianchi N
- Bielcik J
- Bielcikova J
- Bilandzic A
- Biro G
- Biswas R
- Biswas S
- Blair J. T
- Blau D
- Blume C
- Boca G
- Bock F
- Bogdanov A
- Boldizsar L
- Bolozdynya A
- Bombara M
- Bonomi G
- Bonora M
- Borel H
- Borissov A
- Borri M
- Botta E
- Bourjau C
- Bratrud L
- Braun-Munzinger P
- Bregant M
- Broker T. A
- Broz M
- Brucken E. J
- Bruna E
- Bruno G. E
- Budnikov D
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- Publication venue
- Publication date
- 27/08/2018
- Field of study
We present the first measurements of femtoscopic correlations between the K-S(0) and K-+/- particles in pp collisions at root s = 7 TeV measured by the ALICE experiment. The observed femtoscopic correlations are consistent with final-state interactions proceeding solely via the a(0)(980) resonance. The extracted kaon source radius and correlation strength parameters for (KSK-)-K-0 are found to be equal within the experimental uncertainties to those for (KSK+)-K-0. Results of the present study are compared with those from identical-kaon femtoscopic studies also performed with pp collisions at root s = 7 TeV by ALICE and with a (KSK +/-)-K-0 measurement in Pb-Pb collisions at root s(NN) = 2.76 TeV. Combined with the Pb-Pb results, our pp analysis is found to be compatible with the interpretation of the a (980) having a tetraquark structure instead of that of a diquark. (C) 2018 Published by Elsevier B.V.Peer reviewe
Light (anti-)nuclei production and elliptic flow at the LHC with ALICE
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- A
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- A
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- A. Gomez and Gonzalez
- A. J
- A. Karasu and Karavichev
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- Altsybeev
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- Buxton J. T
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- Calvo Villar E
- Camacho R. S
- Camerini P
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- Carena W
- Carnesecchi F
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- Ceballos Sanchez C
- Chandra S
- Chang B
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- Chapeland S
- Chartier M
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- Chauvin A
- Cheshkov C
- Cheynis B
- Cho S
- Chochula P
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- V and Izucheev
- V and Jacak
- V and Kar
- V and Kowalski
- V and Kuhn
- V and Lindsay
- V and Liu
- V and Loizides
- V and Manso
- V and Mao
- V and Mudnic
- V and Noferini
- V and Pagano
- V and Pareek
- V and Pestov
- V and Petrovici
- V and Prasad
- V and Putschke
- V and Ravasenga
- V and Richert
- V and Sandoval
- V and Sinha
- V and Trzaska
- V and Zaccolo
- V and Zaman
- V and Zhigareva
- V
- V
- V
- V
- V
- V. Chibante and Chinellato
- Vala M
- van Doremalen L. V. R
- Van Hoorne J. W
- van Leeuwen M
- Vande Vyvre P
- Varga D
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- Vargyas M
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- Voloshin K
- Voloshin S. A
- Volpe G
- von Haller B
- Vorobyev
- Vranic D
- Vrlakova J
- W. H
- Wagner B
- Wang H
- Wang M
- Watanabe Y
- Weber M
- Weber S. G
- Wegrzynek A
- Weiser D. F
- Wenzel S. C
- Wessels J. P
- Westerhoff U
- Whitehead A. M
- Wiechula J
- Wikne J
- Wilk G
- Wilkinson J
- Willems G. A
- Williams M. C. S
- Willsher E
- Windelband B
- Witt W. E
- Xu R
- Y
- Y
- Y. Corrales and Cortese
- Yalcin S
- Yamakawa K
- Yano S
- Yin Z
- Yokoyama H
- Yoo
- Yurchenko
- Z. Conesa and Contreras
- Zampolli C
- Zanoli H. J. C
- Zardoshti N
- Zarochentsev A
- Zavada P
- Zaviyalov N
- Zbroszczyk H
- Zhalov M
- Zhang X
- Zhang Y
- Zhang Z
- Zhao C
- Zherebchevskii
- Zhou D
- Zhou Y
- Zhou Z
- Zhu H
- Zhu J
- Zhu Y
- Zichichi A
- Zimmermann M. B
- Zinovjev G
- Zmeskal J
- Zou S
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2019
- Field of study
Results on the production of stable light nuclei, including deuterons,
He-3, He-4 and the corresponding anti-nuclei, in Pb-Pb collisions at
root s(NN) = 2.76 TeV and root s(NN) = 5.02 TeV are presented and
compared with theoretical predictions and with the results in small
systems to provide insight into the production mechanisms of
(anti-)nuclei at colliders.
The experimental results are presented giving a critical view of their
comparison to the expectations from coalescence and hydrodynamic models
that aim at describing both the p(T)-spectra and the elliptic flow
Open heavy-flavour production and elliptic flow in p-Pb collisions at the LHC with ALICE
- Author
- A
- A
- A
- A
- A
- A
- A
- A. Gomez and Gonzalez
- A. J
- A. Karasu and Karavichev
- Acharya S
- Acosta F. T
- Adamova D
- Adolfsson J
- Aggarwal M. M
- Agrawal N
- Ahammed Z
- Ahn S. U
- Aiola S
- Akindinov A
- Al-Turany M
- Alam S. N
- Albuquerque D. S. D
- Aleksandrov D
- Alessandro B
- Alfaro Molina R
- Ali Y
- Alice Collaboration
- Alici A
- Alkin A
- Alme J
- Alt T
- Altenkamper L
- Altsybeev
- Andrei C
- Andreou D
- Andrews H. A
- Andronic A
- Angeletti M
- Anguelov
- Anticic T
- Antinori F
- Antonioli P
- Anwar R
- Apadula N
- Aphecetche L
- Appelshaeuser H
- Arcelli S
- Arnaldi R
- Arnold O. W
- Arratia M
- Arsene I. C
- Arslandok M
- Augustinus A
- Averbeck R
- Azmi M. D
- B
- Badala A
- Baek Y. W
- Bagnasco S
- Bailhache R
- Baillie
- Bala R
- Balbastre
- Baldisseri A
- Ball M
- Baral R. C
- Barbano A. M
- Barbera R
- Barile F
- Barioglio L
- Barnafoldi G. G
- Barnby L. S
- Barret
- Barroso
- Barth K
- Bartsch E
- Bastid N
- Basu S
- Batigne G
- Batyunya B
- Batzing P. C
- Bazo Alba J. L
- Bearden I. G
- Beck H
- Bedda C
- Behera N. K
- Belikov
- Bello Martinez H
- Bellwied R
- Beltran L. G. E
- Belyaev
- Beole S
- Bercuci A
- Berdnikov Y
- Berenyi D
- Bertens R. A
- Berzano D
- Betev L
- Bhaduri P. P
- Bhasin A
- Bhat I. R
- Bhatt H
- Bhattacharjee B
- Bhom J
- Bianchi A
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- Bielcikova J
- Bilandzic A
- Biro G
- Biswas R
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- Blair J. T
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- Borissov A
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- Botta E
- Bourjau C
- Bratrud L
- Braun-Munzinger P
- Bregant M
- Broker T. A
- Broz M
- Brucken E. J
- Bruna E
- Bruno G. E
- Budnikov D
- Buesching H
- Bufalino S
- Buhler P
- Buncic P
- Busch O
- Bustamante
- Buthelezi Z
- Butt J. B
- Buxton J. T
- C
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- Caffarri D
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- Caliva A
- Calvo Villar E
- Camacho R. S
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- Capon A. A
- Carena F
- Carena W
- Carnesecchi F
- Castellanos
- Casula E. A. R
- Ceballos Sanchez C
- Chandra S
- Chang B
- Chang W
- Chapeland S
- Chartier M
- Chattopadhyay S
- Chauvin A
- Cheshkov C
- Cheynis B
- Cho S
- Chochula P
- Chowdhury T
- Christakoglou P
- Christensen C. H
- Christiansen P
- Chujo T
- Chung S. U
- Cicalo C
- Cifarelli L
- Cindolo F
- Cleymans J
- Colamaria F
- Colella D
- Collu A
- Colocci M
- Concas M
- Cormier T. M
- Cosentino M. R
- Costa F
- Costanza S
- Crkovska J
- Crochet P
- Cuautle E
- Cunqueiro L
- D
- D
- D
- D D.
- D. A. Moreira and Moreno
- Da Costa
- Dahms T
- Dainese A
- Damas F. P. A
- Dani S
- Danisch M. C
- Danu A
- Das
- Das D
- Dash A
- Dash S
- De Caro A
- de Cataldo G
- de Conti C
- de Cuveland J
- De Falco A
- De Gruttola D
- De Marco N
- De Pasquale S
- De Souza R. D
- De Oliveira
- De S
- Degenhardt H. F
- Deisting A
- Deloff A
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- V and Jacak
- V and Kar
- V and Kowalski
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- V and Lindsay
- V and Liu
- V and Loizides
- V and Manso
- V and Mao
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- V and Noferini
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- V and Zaman
- V and Zhigareva
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- V
- V. Chibante and Chinellato
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- Vranic D
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- W. H
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- Wang H
- Wang M
- Watanabe Y
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- Weber S. G
- Wegrzynek A
- Weiser D. F
- Wenzel S. C
- Wessels J. P
- Westerhoff U
- Whitehead A. M
- Wiechula J
- Wikne J
- Wilk G
- Wilkinson J
- Willems G. A
- Williams M. C. S
- Willsher E
- Windelband B
- Witt W. E
- Xu R
- Y
- Y
- Y. Corrales and Cortese
- Yalcin S
- Yamakawa K
- Yano S
- Yin Z
- Yokoyama H
- Yoo
- Yurchenko
- Z. Conesa and Contreras
- Zampolli C
- Zanoli H. J. C
- Zanoli Henrique J. C
- Zardoshti N
- Zarochentsev A
- Zavada P
- Zaviyalov N
- Zbroszczyk H
- Zhalov M
- Zhang X
- Zhang Y
- Zhang Z
- Zhao C
- Zherebchevskii
- Zhou D
- Zhou Y
- Zhou Z
- Zhu H
- Zhu J
- Zhu Y
- Zichichi A
- Zimmermann M. B
- Zinovjev G
- Zmeskal J
- Zou S
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2019
- Field of study
Measurements of open heavy flavour production in p-A collisions allow
the investigation of Cold Nuclear Matter effects. In addition, they are
an important tool for a complementary investigation of the long-range
correlations found in small systems in the light flavour sector. In this
work, production measurements of D mesons at mid-rapidity in p-Pb
collisions at root S-NN = 5.02 TeV are reported. Production yields are
also reported for the heavy-flavour hadron decay electrons at central
rapidity at root(SNN) = 5.02 and 8.16 TeV. The elliptic flow (nu(2)) of
heavy-flavour hadron decay electrons in high multiplicity p-Pb
collisions at root(SNN) = 5.02 TeV is found to be positive with a
significance larger than 5 sigma
Upsilon suppression at forward rapidity in Pb-Pb collisions at root s(NN)=5.02 TeV
- Author
- A
- A
- A
- A
- A
- A
- A
- A. Gomez and Gonzalez
- A. J
- A. Karasu and Karavichev
- Acharya S
- Acosta F. T
- Adamova D
- Adolfsson J
- Aggarwal M. M
- Agrawal N
- Ahammed Z
- Ahn S. U
- Aiola S
- Akindinov A
- Al-Turany M
- Alam S. N
- Albuquerque D. S. D
- Aleksandrov D
- Alessandro B
- ALICE Collaboration
- Alici A
- Alkin A
- Alme J
- Alt T
- Altenkamper L
- Altsybeev
- Andrei C
- Andreou D
- Andrews H. A
- Andronic A
- Angeletti M
- Anguelov
- Anticic T
- Antinori F
- Antonioli P
- Anwar R
- Apadula N
- Aphecetche L
- Appelshaeuser H
- Arcelli S
- Arnaldi R
- Arnold O. W
- Arsene I. C
- Arslandok M
- Audurier B
- Augustinus A
- Averbeck R
- Azmi M. D
- B
- Badala A
- Baek Y. W
- Bagnasco S
- Bailhache R
- Baillie
- Bala R
- Balbastre
- Baldisseri A
- Ball M
- Baral R. C
- Barbano A. M
- Barbera R
- Barile F
- Barioglio L
- Barnafoldi G. G
- Barnby L. S
- Barret
- Barroso
- Barth K
- Bartsch E
- Bastid N
- Basu S
- Batigne G
- Batyunya B
- Batzing P. C
- Bazo Alba J. L
- Bearden I. G
- Beck H
- Bedda C
- Behera N. K
- Belikov
- Bello Martinez H
- Bellwied R
- Beltran L. G. E
- Belyaev
- Beole S
- Bercuci A
- Berdnikov Y
- Berenyi D
- Bertens R. A
- Berzano D
- Betev L
- Bhaduri P. P
- Bhasin A
- Bhat I. R
- Bhatt H
- Bhattacharjee B
- Bhom J
- Bianchi A
- Bianchi L
- Bianchi N
- Bielcik J
- Bielcikova J
- Bilandzic A
- Biro G
- Biswas R
- Biswas S
- Blair J. T
- Blau D
- Blume C
- Boca G
- Bock F
- Bogdanov A
- Boldizsar L
- Bombara M
- Bonomi G
- Bonora M
- Borel H
- Borissov A
- Borri M
- Botta E
- Bourjau C
- Bratrud L
- Braun-Munzinger P
- Bregant M
- Broker T. A
- Broz M
- Brucken E. J
- Bruna E
- Bruno G. E
- Budnikov D
- Buesching H
- Bufalino S
- Buhler P
- Buncic P
- Busch O
- Bustamante
- Buthelezi Z
- Butt J. B
- Buxton J. T
- C
- C
- C
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- Cabala J
- Caffarri D
- Caines H
- Caliva A
- Calvo Villar E
- Camacho R. S
- Camerini P
- Capon A. A
- Carena W
- Carnesecchi F
- Castellanos
- Casula E. A. R
- Ceballos Sanchez C
- Chandra S
- Chang B
- Chang W
- Chapeland S
- Chartier M
- Chattopadhyay S
- Chauvin A
- Cheshkov C
- Cheynis B
- Cho S
- Chochula P
- Chowdhury T
- Christakoglou P
- Christensen C. H
- Christiansen P
- Chujo T
- Chung S. U
- Cicalo C
- Cifarelli L
- Cindolo F
- Cleymans J
- Colamaria F
- Colella D
- Collu A
- Colocci M
- Concas M
- Cormier T. M
- Cosentino M. R
- Costa F
- Costanza S
- Crkovska J
- Crochet P
- Cuautle E
- Cunqueiro L
- D
- D
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- D. D
- da Luz
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- de Cuveland J
- De Falco A
- De Gruttola D
- De Marco N
- De Oliveira
- De Pasquale S
- De Souza R. D
- De S
- Degenhardt H. F
- Deisting A
- Deloff A
- Delsanto S
- Deplano C
- Dhankher P
- Di Bari D
- Di Mauro A
- Di Ruzza B
- Diaz R. A
- Dietel T
- Dillenseger P
- Ding Y
- Divia R
- Djuvsland O
- Dobrin A
- Doce
- Doenigus B
- Domenicis Gimenez D
- Dordic O
- Doremalen L. V. R
- Dubey A. K
- Dubla A
- Ducroux L
- Dudi S
- Duggal A. K
- Dukhishyam M
- Dupieux P
- E
- E. Perez and Peskov
- Ehlers R. J
- Elia D
- Endress E
- Engel H
- Epple E
- Erazmus B
- Erhardt F
- Erokhin A
- Ersdal M. R
- Espagnon B
- Eulisse G
- Eum J
- Evans D
- Evdokimov S
- F
- F
- F
- Fabbietti L
- Faggin M
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- Publication venue
- Elsevier BV
- Publication date
- 01/01/2018
- Field of study
Inclusive Υ(1S) and Υ(2S) production have been measured in Pb–Pb collisions at the centre-of-mass energy per nucleon–nucleon pair √sNN = 5.02 TeV, using the ALICE detector at the CERN LHC. The Υ mesons are reconstructed in the centre-of-mass rapidity interval 2.5 < y < 4 and in the transverse-momentum range pT < 15 GeV/c, via their decays to muon pairs. In this Letter, we present results on the inclusive Υ(1S) nuclear modification factor RAA as a function of collision centrality, transverse momentum and rapidity. The Υ(1S) and Υ(2S) RAA, integrated over the centrality range 0–90%, are 0.37± 0.02(stat) ± 0.03(syst) and 0.10 ± 0.04(stat) ± 0.02(syst), respectively, leading to a ratio RΥ(2S)/RΥ(1S) of 0.28±0.12(stat)±0.06(syst). The observed Υ(1S) suppression increases with the centrality of the collision and no significant variation is observed as a function of transverse momentum and rapidity
Inclusive quarkonium production at forward rapidity in pp collisions at root s=8 TeV
- Publication venue
- Publication date
- 01/01/2016
- Field of study
We report on the inclusive production cross sections of J/psi, psi(2S),
gamma(1S), gamma(2S) and gamma(3S), measured at forward rapidity with
the ALICE detector in pp collisions at a center-of-mass energy root s =
8 TeV. The analysis is based on data collected at the LHC and
corresponds to an integrated luminosity of 1.23 pb(-1). Quarkonia are
reconstructed in the dimuon-decay channel. The differential production
cross sections are measured as a function of the transverse momentum
p(T) and rapidity y, over the p(T) ranges 0 < p(T) < 20 GeV/c for J/psi,
0 < p(T) < 12 GeV/c for all other resonances, and for 2.5 < y < 4. The
cross sections, integrated over p(T) and y, and assuming unpolarized
quarkonia, are sigma(J/psi) = 8.98 +/- 0.04 +/- 0.82 mu b,
sigma(psi(2S)) = 1.23 +/- 0.08 +/- 0.22 mu b, sigma(gamma(1S)) = 71 +/-
6 +/- 7 nb, sigma(gamma(2S)) = 26 +/- 5 +/- 4 nb and sigma(gamma(3S)) =
9 +/- 4 +/- 1 nb, where the first uncertainty is statistical and the
second one is systematic. These values agree, within at most 1.4 sigma,
with measurements performed by the LHCb collaboration in the same
rapidity range
Measurement of transverse energy at midrapidity in Pb-Pb collisions at root s(NN)=2.76 TeV
- Publication venue
- Publication date
- 01/01/2016
- Field of study
We report the transverse energy (ET) measured with ALICE at midrapidity
in Pb-Pb collisions at root s(NN) = 2.76 TeV as a function of
centrality. The transverse energy was measured using identified
single-particle tracks. The measurement was cross checked using the
electromagnetic calorimeters and the transverse momentum distributions
of identified particles previously reported by ALICE. The results are
compared to theoretical models as well as to results from other
experiments. The mean ET per unit pseudorapidity (eta), < dE(T)/d eta >,
in 0%-5% central collisions is 1737 +/- 6(stat.) +/- 97(sys.) GeV. We
find a similar centrality dependence of the shape of < dE(T)/d eta > as
a function of the number of participating nucleons to that seen at lower
energies. The growth in < dE(T)/d eta > at the LHC energies exceeds
extrapolations of low-energy data. We observe a nearly linear scaling of
< dE(T)/d eta > with the number of quark participants. With the
canonical assumption of a 1 fm/c formation time, we estimate that the
energy density in 0%-5% central Pb-Pb collisions at root s(NN) = 2.76
TeV is 12.3 +/- 1.0 GeV/fm(3) and that the energy density at the most
central 80 fm(2) of the collision is at least 21.5 +/- 1.7 GeV/fm(3).
This is roughly 2.3 times that observed in 0%-5% central Au-Au
collisions at root s(NN) = 200 GeV
- …