PrePrint_References.bib

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	title = {{pdgLive}},
	url = {http://pdglive.lbl.gov/Viewer.action},
	urldate = {2020-04-29},
	file = {pdgLive:/home/romain/Zotero/storage/RQXT8GYS/Viewer.html:text/html},
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@article{collaboration_alice_2008,
	title = {The {ALICE} experiment at the {CERN} {LHC}},
	volume = {3},
	issn = {1748-0221},
	url = {https://doi.org/10.1088/1748-0221/3/08/s08002},
	doi = {10.1088/1748-0221/3/08/S08002},
	abstract = {ALICE (A Large Ion Collider Experiment) is a general-purpose, heavy-ion detector at the CERN LHC which focuses on QCD, the strong-interaction sector of the Standard Model. It is designed to address the physics of strongly interacting matter and the quark-gluon plasma at extreme values of energy density and temperature in nucleus-nucleus collisions. Besides running with Pb ions, the physics programme includes collisions with lighter ions, lower energy running and dedicated proton-nucleus runs. ALICE will also take data with proton beams at the top LHC energy to collect reference data for the heavy-ion programme and to address several QCD topics for which ALICE is complementary to the other LHC detectors. The ALICE detector has been built by a collaboration including currently over 1000 physicists and engineers from 105 Institutes in 30 countries. Its overall dimensions are 16 × 16 × 26 m3 with a total weight of approximately 10 000 t. The experiment consists of 18 different detector systems each with its own specific technology choice and design constraints, driven both by the physics requirements and the experimental conditions expected at LHC. The most stringent design constraint is to cope with the extreme particle multiplicity anticipated in central Pb-Pb collisions. The different subsystems were optimized to provide high-momentum resolution as well as excellent Particle Identification (PID) over a broad range in momentum, up to the highest multiplicities predicted for LHC. This will allow for comprehensive studies of hadrons, electrons, muons, and photons produced in the collision of heavy nuclei. Most detector systems are scheduled to be installed and ready for data taking by mid-2008 when the LHC is scheduled to start operation, with the exception of parts of the Photon Spectrometer (PHOS), Transition Radiation Detector (TRD) and Electro Magnetic Calorimeter (EMCal). These detectors will be completed for the high-luminosity ion run expected in 2010. This paper describes in detail the detector components as installed for the first data taking in the summer of 2008.},
	language = {en},
	number = {08},
	urldate = {2020-05-22},
	journal = {Journal of Instrumentation},
	author = {Collaboration, The ALICE and Aamodt, K. and Quintana, A. Abrahantes and Achenbach, R. and Acounis, S. and Adamová, D. and Adler, C. and Aggarwal, M. and Agnese, F. and Rinella, G. Aglieri and Ahammed, Z. and Ahmad, A. and Ahmad, N. and Ahmad, S. and Akindinov, A. and Akishin, P. and Aleksandrov, D. and Alessandro, B. and Alfaro, R. and Alfarone, G. and Alici, A. and Alme, J. and Alt, T. and Altinpinar, S. and Amend, W. and Andrei, C. and Andres, Y. and Andronic, A. and Anelli, G. and Anfreville, M. and Angelov, V. and Anzo, A. and Anson, C. and Anticić, T. and Antonenko, V. and Antonczyk, D. and Antinori, F. and Antinori, S. and Antonioli, P. and Aphecetche, L. and Appelshäuser, H. and Aprodu, V. and Arba, M. and Arcelli, S. and Argentieri, A. and Armesto, N. and Arnaldi, R. and Arefiev, A. and Arsene, I. and Asryan, A. and Augustinus, A. and Awes, T. C. and Äysto, J. and Azmi, M. Danish and Bablock, S. and Badalà, A. and Badyal, S. 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	month = aug,
	year = {2008},
	note = {Publisher: IOP Publishing},
	pages = {S08002--S08002},
	file = {IOP Full Text PDF:/home/romain/Zotero/storage/3XVU9UBF/Collaboration et al. - 2008 - The ALICE experiment at the CERN LHC.pdf:application/pdf},
}

@misc{silva_de_albuquerque_multi-strange_2019,
	title = {Multi-strange hadrons in {Pb}–{Pb} collisions at the {LHC} with {ALICE}},
	url = {https://cds.cern.ch/record/2690627},
	abstract = {A strongly interacting state of matter known as the Quark-Gluon Plasma (QGP) is formed in the high temperature and high energy density conditions reached in ultra-relativistic heavy-ion collisions, such as the Pb–Pb collisions measured at the Large Hadron Collider (LHC). One of the key measurements for the understanding of the properties of the QGP medium created in these collisions is the production of strange and multi-strange hadrons. ALICE is one of the four major experiments of the LHC and has a detector designed to study identified particle production rates from heavy-ion collisions. The excellent tracking and particle identification capabilities allow the reconstruction of multi-strange baryons (\${\textbackslash}Xi{\textasciicircum}\{-\}\$, \${\textbackslash}bar\{{\textbackslash}Xi\}{\textasciicircum}\{+\}\$,  \${\textbackslash}Omega{\textasciicircum}\{-\}\$ and \${\textbackslash}bar\{{\textbackslash}Omega\}{\textasciicircum}\{+\}\$) via their weak decay channels over a large range in transverse momentum (\$p\_\{{\textbackslash}rm T\}\$).  In this thesis, we study the multi-strange particle production at central rapidity Pb–Pb collisions measured by ALICE at the unprecedented energy of \${\textbackslash}sqrt\{s\_\{NN\}\} = 5.02\$ TeV and \$2.76\$ TeV. The yields are normalized by the corresponding measurement of pion production in the same centrality class in order to study the strangeness enhancement, effect predicted as a probe of the QGP. Comparison of hyperon-to-pion ratio between different systems, such as pp, p–pb and Pb–Pb collisions, shows that production of multi-strange baryons relative to pions follows a continuously increasing trend from low multiplicity pp to central Pb–Pb collisions.},
	language = {fr},
	urldate = {2020-05-30},
	journal = {CERN Document Server},
	author = {Silva De Albuquerque, Danilo},
	month = sep,
	year = {2019},
	note = {Library Catalog: cds.cern.ch
Number: CERN-THESIS-2019-135
University: Campinas State U.},
	file = {Full Text PDF:/home/romain/Zotero/storage/THT27DVK/Silva De Albuquerque - 2019 - Multi-strange hadrons in Pb–Pb collisions at the L.pdf:application/pdf;Snapshot:/home/romain/Zotero/storage/DW5LM9XB/2690627.html:text/html},
}

@article{atlas_collaboration_kshort_2012,
	title = {Kshort and {Lambda} production in pp interactions at sqrt(s) = 0.9 and 7 {TeV} measured with the {ATLAS} detector at the {LHC}},
	volume = {85},
	issn = {1550-7998, 1550-2368},
	url = {http://arxiv.org/abs/1111.1297},
	doi = {10.1103/PhysRevD.85.012001},
	abstract = {The production of Kshort and Lambda hadrons is studied in inelastic pp collisions at sqrt(s) = 0.9 and 7 TeV collected with the ATLAS detector at the LHC using a minimum-bias trigger. The observed distributions of transverse momentum, rapidity, and multiplicity are corrected to hadron level in a model-independent way within well defined phase-space regions. The distribution of the production ratio of Lambdabar to Lambda baryons is also measured. The results are compared with various Monte Carlo simulation models. Although most of these models agree with data to within 15\% in the Kshort distributions, substantial disagreements with data are found in the Lambda distributions of transverse momentum.},
	number = {1},
	urldate = {2020-06-01},
	journal = {Physical Review D},
	author = {ATLAS Collaboration},
	month = jan,
	year = {2012},
	note = {arXiv: 1111.1297},
	keywords = {High Energy Physics - Experiment},
	pages = {012001},
	annote = {Comment: 16 pages plus author list (29 pages total), 24 figures, 2 tables, submitted to Physical Review D},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/K8D4JB8B/ATLAS Collaboration - 2012 - Kshort and Lambda production in pp interactions at.pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/EPDPUUMQ/1111.html:text/html},
}

@article{alice_collaboration_multiplicity_2019,
	title = {Multiplicity dependence of light-flavor hadron production in pp collisions at \${\textbackslash}sqrt\{s\}\$ = 7 {TeV}},
	volume = {99},
	issn = {2469-9985, 2469-9993},
	url = {http://arxiv.org/abs/1807.11321},
	doi = {10.1103/PhysRevC.99.024906},
	abstract = {Comprehensive results on the production of unidentified charged particles, \${\textbackslash}pi{\textasciicircum}\{{\textbackslash}pm\}\$, \${\textbackslash}rm\{K\}{\textasciicircum}\{{\textbackslash}pm\}\$, \${\textbackslash}rm\{K\}{\textasciicircum}\{0\}\_\{S\}\$, \${\textbackslash}rm\{K\}\$*(892)\${\textasciicircum}\{0\}\$, \${\textbackslash}rm\{p\}\$, \${\textbackslash}overline\{{\textbackslash}rm\{p\}\}\$, \${\textbackslash}phi\$(1020), \${\textbackslash}Lambda\$, \${\textbackslash}overline\{{\textbackslash}Lambda\}\$, \${\textbackslash}Xi{\textasciicircum}\{-\}\$, \${\textbackslash}overline\{{\textbackslash}Xi\}{\textasciicircum}\{+\}\$, \${\textbackslash}Omega{\textasciicircum}\{-\}\$ and \${\textbackslash}overline\{{\textbackslash}Omega\}{\textasciicircum}\{+\}\$ hadrons in proton-proton (pp) collisions at \${\textbackslash}sqrt\{s\}\$ = 7 TeV at midrapidity (\${\textbar}y{\textbar} {\textless} 0.5\$) as a function of charged-particle multiplicity density are presented. In order to avoid auto-correlation biases, the actual transverse momentum (\$p\_\{{\textbackslash}rm\{T\}\}\$) spectra of the particles under study and the event activity are measured in different rapidity windows. In the highest multiplicity class, the charged-particle density reaches about 3.5 times the value measured in inelastic collisions. While the yield of protons normalized to pions remains approximately constant as a function of multiplicity, the corresponding ratios of strange hadrons to pions show a significant enhancement that increases with increasing strangeness content. Furthermore, all identified particle to pion ratios are shown to depend solely on charged-particle multiplicity density, regardless of system type and collision energy. The evolution of the spectral shapes with multiplicity and hadron mass shows patterns that are similar to those observed in p-Pb and Pb-Pb collisions at LHC energies. The obtained \$p\_\{{\textbackslash}rm\{T\}\}\$ distributions and yields are compared to expectations from QCD-based pp event generators as well as to predictions from thermal and hydrodynamic models. These comparisons indicate that traces of a collective, equilibrated system are already present in high-multiplicity pp collisions.},
	number = {2},
	urldate = {2021-03-20},
	journal = {Physical Review C},
	author = {ALICE Collaboration},
	month = feb,
	year = {2019},
	note = {arXiv: 1807.11321},
	keywords = {High Energy Physics - Experiment, Nuclear Experiment},
	pages = {024906},
	annote = {Comment: 45 pages, 15 captioned figures, 12 tables, authors from page 40, published, figures at http://alice-publications.web.cern.ch/node/4516},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/5JZCMI48/ALICE Collaboration - 2019 - Multiplicity dependence of light-flavor hadron pro.pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/M8CSSYB3/1807.html:text/html},
}

@article{alice_collaboration_multiplicity_2014,
	title = {Multiplicity {Dependence} of {Pion}, {Kaon}, {Proton} and {Lambda} {Production} in p-{Pb} {Collisions} at \${\textbackslash}sqrt\{s\_\{{\textbackslash}rm {NN}\}\}\$ = 5.02 {TeV}},
	volume = {728},
	issn = {03702693},
	url = {http://arxiv.org/abs/1307.6796},
	doi = {10.1016/j.physletb.2013.11.020},
	abstract = {In this Letter, comprehensive results on \$\{{\textbackslash}rm{\textbackslash}pi\}{\textasciicircum}{\textbackslash}pm\$, K\${\textasciicircum}{\textbackslash}pm\$, K\${\textasciicircum}0\_S\$, p, \${\textbackslash}rm{\textbackslash}bar\{p\}\$, \${\textbackslash}rm {\textbackslash}Lambda\$ and \${\textbackslash}rm {\textbackslash}bar\{{\textbackslash}Lambda\}\$ production at mid-rapidity (\$0 {\textless} y\_\{{\textbackslash}rm cms\} {\textless} 0.5\$) in p-Pb collisions at \${\textbackslash}sqrt\{s\_\{{\textbackslash}rm NN\}\} = 5.02\$ TeV, measured by the ALICE detector at the LHC, are reported. The transverse momentum distributions exhibit a hardening as a function of event multiplicity, which is stronger for heavier particles. This behavior is similar to what has been observed in pp and Pb-Pb collisions at the LHC. The measured \$p\_\{{\textbackslash}rm T\}\$ distributions are compared to results at lower energy and with predictions based on QCD-inspired and hydrodynamic models.},
	urldate = {2021-04-13},
	journal = {Physics Letters B},
	author = {ALICE Collaboration},
	month = jan,
	year = {2014},
	note = {arXiv: 1307.6796},
	keywords = {High Energy Physics - Experiment, Nuclear Experiment},
	pages = {25--38},
	annote = {Comment: 26 pages, 7 captioned figures, 5 tables, authors from page 21, published version, figures at http://aliceinfo.cern.ch/ArtSubmission/node/602},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/62GYELDJ/ALICE Collaboration - 2014 - Multiplicity Dependence of Pion, Kaon, Proton and .pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/DSXH9QS6/1307.html:text/html},
}

@article{alice_collaboration_pensuremath-p_2019,
	title = {\$p{\textbackslash}ensuremath\{-\}p, p{\textbackslash}ensuremath\{-\}{\textbackslash}mathrm\{{\textbackslash}ensuremath\{{\textbackslash}{Lambda}\}\}\$, and \${\textbackslash}mathrm\{{\textbackslash}ensuremath\{{\textbackslash}{Lambda}\}\}{\textbackslash}ensuremath\{-\}{\textbackslash}mathrm\{{\textbackslash}ensuremath\{{\textbackslash}{Lambda}\}\}\$ correlations studied via femtoscopy in \$pp\$ reactions at \${\textbackslash}sqrt\{s\}=7{\textbackslash}phantom\{{\textbackslash}rule\{0.16em\}\{0ex\}\}{\textbackslash}mathrm\{{TeV}\}\$},
	volume = {99},
	url = {https://link.aps.org/doi/10.1103/PhysRevC.99.024001},
	doi = {10.1103/PhysRevC.99.024001},
	abstract = {We report on the first femtoscopic measurement of baryon pairs, such as p−p, p−Λ, and Λ−Λ, measured by ALICE at the Large Hadron Collider (LHC) in proton-proton collisions at √s=7TeV. This study demonstrates the feasibility of such measurements in pp collisions at ultrarelativistic energies. The femtoscopy method is employed to constrain the hyperon-nucleon and hyperon-hyperon interactions, which are still rather poorly understood. A new method to evaluate the influence of residual correlations induced by the decays of resonances and experimental impurities is hereby presented. The p−p, p−Λ, and Λ−Λ correlation functions were fitted simultaneously with the help of a new tool developed specifically for the femtoscopy analysis in small colliding systems: Correlation Analysis Tool using the Schrödinger equation (CATS). Within the assumption that in pp collisions the three particle pairs originate from a common source, its radius is found to be equal to r0=1.125±0.018(stat)+0.058−0.035(syst) fm. The sensitivity of the measured p−Λ correlation is tested against different scattering parameters, which are defined by the interaction among the two particles, but the statistics is not sufficient yet to discriminate among different models. The measurement of the Λ−Λ correlation function constrains the phase space spanned by the effective range and scattering length of the strong interaction. Discrepancies between the measured scattering parameters and the resulting correlation functions at LHC and RHIC energies are discussed in the context of various models.},
	number = {2},
	urldate = {2021-04-19},
	journal = {Physical Review C},
	author = {{ALICE Collaboration} and Acharya, S. and Adamová, D. and Adolfsson, J. and Aggarwal, M. M. and Aglieri Rinella, G. and Agnello, M. and Agrawal, N. and Ahammed, Z. and Ahn, S. U. and Aiola, S. and Akindinov, A. and Al-Turany, M. and Alam, S. N. and Albuquerque, D. S. D. and Aleksandrov, D. and Alessandro, B. and Alfaro Molina, R. and Ali, Y. and Alici, A. and Alkin, A. and Alme, J. and Alt, T. and Altenkamper, L. and Altsybeev, I. and Anaam, M. N. and Andrei, C. and Andreou, D. and Andrews, H. A. and Andronic, A. and Angeletti, M. and Anguelov, V. and Anson, C. and Antičić, T. and Antinori, F. and Antonioli, P. and Anwar, R. and Apadula, N. and Aphecetche, L. and Appelshäuser, H. and Arcelli, S. and Arnaldi, R. and Arnold, O. W. and Arsene, I. C. and Arslandok, M. and Augustinus, A. and Averbeck, R. and Azmi, M. D. and Badalà, A. and Baek, Y. W. and Bagnasco, S. and Bailhache, R. and Bala, R. and Baldisseri, A. and Ball, M. and Baral, R. C. and Barbano, A. M. and Barbera, R. and Barile, F. and Barioglio, L. and Barnaföldi, G. G. and Barnby, L. S. and Barret, V. and Bartalini, P. and Barth, K. and Bartsch, E. and Bastid, N. and Basu, S. and Batigne, G. and Batyunya, B. and Batzing, P. C. and Bazo Alba, J. L. and Bearden, I. G. and Beck, H. and Bedda, C. and Behera, N. K. and Belikov, I. and Bellini, F. and Bello Martinez, H. and Bellwied, R. and Beltran, L. G. E. and Belyaev, V. and Bencedi, G. and Beole, S. and Bercuci, A. and Berdnikov, Y. and Berenyi, D. and Bertens, R. A. and Berzano, D. and Betev, L. and Bhaduri, P. P. and Bhasin, A. and Bhat, I. R. and Bhatt, H. and Bhattacharjee, B. and Bhom, J. and Bianchi, A. and Bianchi, L. and Bianchi, N. and Bielčík, J. and Bielčíková, J. and Bilandzic, A. and Biro, G. and Biswas, R. and Biswas, S. and Blair, J. 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M. and Siemiarczuk, T. and Silvermyr, D. and Simatovic, G. and Simonetti, G. and Singaraju, R. and Singh, R. and Singh, R. and Singhal, V. and Sinha, T. and Sitar, B. and Sitta, M. and Skaali, T. B. and Slupecki, M. and Smirnov, N. and Snellings, R. J. M. and Snellman, T. W. and Sochan, J. and Soncco, C. and Song, J. and Soramel, F. and Sorensen, S. and Sozzi, F. and Sputowska, I. and Stachel, J. and Stan, I. and Stankus, P. and Stenlund, E. and Stocco, D. and Storetvedt, M. M. and Strmen, P. and Suaide, A. A. P. and Sugitate, T. and Suire, C. and Suleymanov, M. and Suljic, M. and Sultanov, R. and Šumbera, M. and Sumowidagdo, S. and Suzuki, K. and Swain, S. and Szabo, A. and Szarka, I. and Tabassam, U. and Takahashi, J. and Tambave, G. J. and Tanaka, N. and Tarhini, M. and Tariq, M. and Tarzila, M. 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C. and Zardoshti, N. and Zarochentsev, A. and Závada, P. and Zaviyalov, N. and Zbroszczyk, H. and Zhalov, M. and Zhang, X. and Zhang, Y. and Zhang, Z. and Zhao, C. and Zherebchevskii, V. and Zhigareva, N. and Zhou, D. and Zhou, Y. and Zhou, Z. and Zhu, H. and Zhu, J. and Zhu, Y. and Zichichi, A. and Zimmermann, M. B. and Zinovjev, G. and Zmeskal, J. and Zou, S.},
	month = feb,
	year = {2019},
	note = {Publisher: American Physical Society},
	pages = {024001},
	file = {Full Text PDF:/home/romain/Zotero/storage/EMSJQ3JT/ALICE Collaboration et al. - 2019 - \$pensuremath - p, pensuremath - mathrm ensurem.pdf:application/pdf;APS Snapshot:/home/romain/Zotero/storage/MM32KUCC/PhysRevC.99.html:text/html},
}

@article{noauthor_improved_2016,
	title = {Improved {Event}-mixing for {Resonance} {Measurements}},
	shorttitle = {Event mixing,{Resonance},phi meson},
	url = {https://lup.lub.lu.se/student-papers/search/publication/8889631},
	abstract = {This report first analyzed the reason for the deviation of the event-mixing method in background estimation for resonance research, and one possible explanation is that the event-mixing method can not reproduce the specific angular distribution of produced particles caused by jet-effects. This assumption was checked by Monte-Carlo simulations with PYTHIA, and a certain method of correction called reweighing was proposed to improve the event-mixing method. The improved event-mixing method was then applied for simulation as well as resonance analysis for experimental data from the ALICE experiment, and the results proved that this reweighing method can improve the performance on resonance signal extraction by reducing the residual background.},
	language = {eng},
	author = {, Mengke, Cai},
	year = {2016},
	note = {Student Paper},
}

@article{alice_collaboration_measurement_2015,
	title = {Measurement of pion, kaon and proton production in proton-proton collisions at \${\textbackslash}sqrt\{s\}=7\$ {TeV}},
	url = {http://arxiv.org/abs/1504.00024},
	doi = {10.1140/epjc/s10052-015-3422-9},
	abstract = {The measurement of primary \${\textbackslash}pi{\textasciicircum}\{{\textbackslash}pm\}\$, K\${\textasciicircum}\{{\textbackslash}pm\}\$, p and \${\textbackslash}overline\{p\}\$ production at mid-rapidity (\${\textbar}y{\textbar} {\textless}\$ 0.5) in proton-proton collisions at \${\textbackslash}sqrt\{s\} = 7\$ TeV performed with ALICE (A Large Ion Collider Experiment) at the Large Hadron Collider (LHC) is reported. Particle identification is performed using the specific ionization energy loss and time-of-flight information, the ring-imaging Cherenkov technique and the kink-topology identification of weak decays of charged kaons. Transverse momentum spectra are measured from 0.1 up to 3 GeV/\$c\$ for pions, from 0.2 up to 6 GeV/\$c\$ for kaons and from 0.3 up to 6 GeV/\$c\$ for protons. The measured spectra and particle ratios are compared with QCD-inspired models, tuned to reproduce also the earlier measurements performed at the LHC. Furthermore, the integrated particle yields and ratios as well as the average transverse momenta are compared with results at lower collision energies.},
	urldate = {2021-04-26},
	journal = {arXiv:1504.00024 [hep-ex, physics:nucl-ex]},
	author = {ALICE Collaboration},
	month = oct,
	year = {2015},
	note = {arXiv: 1504.00024},
	keywords = {High Energy Physics - Experiment, Nuclear Experiment},
	annote = {Comment: 33 pages, 19 captioned figures, 3 tables, authors from page 28, published version, figures at http://aliceinfo.cern.ch/ArtSubmission/node/1562},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/L2LD4LLL/ALICE Collaboration - 2015 - Measurement of pion, kaon and proton production in.pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/46W6JQBT/1504.html:text/html},
}

@article{sjostrand_pythia_2006,
	title = {{PYTHIA} 6.4 {Physics} and {Manual}},
	url = {http://arxiv.org/abs/hep-ph/0603175},
	doi = {10.1088/1126-6708/2006/05/026},
	abstract = {The PYTHIA program can be used to generate high-energy-physics `events', i.e. sets of outgoing particles produced in the interactions between two incoming particles. The objective is to provide as accurate as possible a representation of event properties in a wide range of reactions, within and beyond the Standard Model, with emphasis on those where strong interactions play a role, directly or indirectly, and therefore multihadronic final states are produced. The physics is then not understood well enough to give an exact description; instead the program has to be based on a combination of analytical results and various QCD-based models. This physics input is summarized here, for areas such as hard subprocesses, initial- and final-state parton showers, underlying events and beam remnants, fragmentation and decays, and much more. Furthermore, extensive information is provided on all program elements: subroutines and functions, switches and parameters, and particle and process data. This should allow the user to tailor the generation task to the topics of interest.},
	urldate = {2021-04-26},
	journal = {arXiv:hep-ph/0603175},
	author = {Sjostrand, Torbjorn and Mrenna, Stephen and Skands, Peter},
	month = may,
	year = {2006},
	note = {arXiv: hep-ph/0603175},
	keywords = {High Energy Physics - Phenomenology},
	annote = {Comment: 576 pages, no figures, uses JHEP3.cls. The code and further information may be found on the PYTHIA web page: http://www.thep.lu.se/{\textasciitilde}torbjorn/Pythia.html Changes in version 2: Mistakenly deleted section heading for "Physics Processes" reinserted, affecting section numbering. Minor updates to take into account referee comments and new colour reconnection options},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/MQTXAEVW/Sjostrand et al. - 2006 - PYTHIA 6.4 Physics and Manual.pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/GTHYEKLA/0603175.html:text/html},
}

@misc{noauthor_alice_2017,
	title = {The {ALICE} definition of primary particles},
	url = {https://cds.cern.ch/record/2270008},
	abstract = {In this public note, we specify what we mean by the term ``primary particle''.  The definition is motivated by what is in principle measurable by ALICE and that event generators and other such theoretical considerations must be able to reproduce the same requirements.  To this end, we also provide a Rivet projection to be used in ALICE Rivet analyses.},
	language = {en},
	urldate = {2021-04-26},
	journal = {CERN Document Server},
	month = jun,
	year = {2017},
	note = {Number: ALICE-PUBLIC-2017-005},
	file = {Full Text PDF:/home/romain/Zotero/storage/WU3MBJVI/2017 - The ALICE definition of primary particles.pdf:application/pdf;Snapshot:/home/romain/Zotero/storage/2BXNYTLN/2270008.html:text/html},
}

@article{alice_collaboration_alignment_2017,
	title = {Alignment of the {ALICE} {Inner} {Tracking} {System} with cosmic-ray tracks},
	url = {http://arxiv.org/abs/1001.0502},
	doi = {10.1088/1748-0221/5/03/P03003},
	abstract = {ALICE (A Large Ion Collider Experiment) is the LHC (Large Hadron Collider) experiment devoted to investigating the strongly interacting matter created in nucleus-nucleus collisions at the LHC energies. The ALICE ITS, Inner Tracking System, consists of six cylindrical layers of silicon detectors with three different technologies; in the outward direction: two layers of pixel detectors, two layers each of drift, and strip detectors. The number of parameters to be determined in the spatial alignment of the 2198 sensor modules of the ITS is about 13,000. The target alignment precision is well below 10 micron in some cases (pixels). The sources of alignment information include survey measurements, and the reconstructed tracks from cosmic rays and from proton-proton collisions. The main track-based alignment method uses the Millepede global approach. An iterative local method was developed and used as well. We present the results obtained for the ITS alignment using about 10{\textasciicircum}5 charged tracks from cosmic rays that have been collected during summer 2008, with the ALICE solenoidal magnet switched off.},
	urldate = {2021-04-26},
	journal = {arXiv:1001.0502 [hep-ex, physics:physics]},
	author = {ALICE Collaboration},
	month = sep,
	year = {2017},
	note = {arXiv: 1001.0502},
	keywords = {High Energy Physics - Experiment, Physics - Instrumentation and Detectors},
	annote = {Comment: 37 pages, 15 captioned figures, 1 table, published version, figures at http://aliceinfo.cern.ch/ArtSubmission/node/3907},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/DTW9FH7R/ALICE Collaboration - 2017 - Alignment of the ALICE Inner Tracking System with .pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/I55Q879U/1001.html:text/html},
}

@article{skands_tuning_2014,
	title = {Tuning {PYTHIA} 8.1: the {Monash} 2013 {Tune}},
	shorttitle = {Tuning {PYTHIA} 8.1},
	url = {http://arxiv.org/abs/1404.5630},
	doi = {10.1140/epjc/s10052-014-3024-y},
	abstract = {We present an updated set of parameters for the PYTHIA 8 event generator. We reevaluate the constraints imposed by LEP and SLD on hadronization, in particular with regard to heavy-quark fragmentation and strangeness production. For hadron collisions, we combine the updated fragmentation parameters with a new NNPDF2.3 LO PDF set. We use minimum-bias, Drell-Yan, and underlying-event data from the LHC to constrain the initial-state-radiation and multi-parton-interaction parameters, combined with data from SPS and the Tevatron to constrain the energy scaling. Several distributions show significant improvements with respect to the current defaults, for both ee and pp collisions, though we emphasize that interesting discrepancies remain in particular for strange particles and baryons. The updated parameters are available as an option starting from PYTHIA 8.185, by setting Tune:ee = 7 and Tune:pp = 14.},
	urldate = {2021-04-26},
	journal = {arXiv:1404.5630 [hep-ph]},
	author = {Skands, Peter and Carrazza, Stefano and Rojo, Juan},
	month = apr,
	year = {2014},
	note = {arXiv: 1404.5630},
	keywords = {High Energy Physics - Phenomenology},
	annote = {Comment: 57 pages},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/LXP5FI5M/Skands et al. - 2014 - Tuning PYTHIA 8.1 the Monash 2013 Tune.pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/KUQS37UB/1404.html:text/html},
}

@article{alice_collaboration_k8920_2015,
	title = {K*(892)\${\textasciicircum}\{0\}\$ and \${\textbackslash}{Phi}\$(1020) production in {Pb}-{Pb} collisions at \${\textbackslash}sqrt\{s\_\{{\textbackslash}rm {NN}\}\}\$ = 2.76 {TeV}},
	url = {http://arxiv.org/abs/1404.0495},
	doi = {10.1103/PhysRevC.91.024609},
	abstract = {The yields of the K*(892)\${\textasciicircum}\{0\}\$ and \${\textbackslash}Phi\$(1020) resonances are measured in Pb-Pb collisions at \${\textbackslash}sqrt\{s\_\{{\textbackslash}rm NN\}\}\$ = 2.76 TeV through their hadronic decays using the ALICE detector. The measurements are performed in multiple centrality intervals at mid-rapidity ({\textbar}\$y\${\textbar}{\textless}0.5) in the transverse-momentum ranges 0.3 {\textless} \$p\_\{{\textbackslash}rm T\}\$ {\textless} 5 GeV/\$c\$ for the K*(892)\${\textasciicircum}\{0\}\$ and 0.5 {\textless} \$p\_\{{\textbackslash}rm T\}\$ {\textless} 5 GeV/\$c\$ for the \${\textbackslash}Phi\$(1020). The yields of K*(892)\${\textasciicircum}\{0\}\$ are suppressed in central Pb-Pb collisions with respect to pp and peripheral Pb-Pb collisions (perhaps due to rescattering of its decay products in the hadronic medium), while the longer lived \${\textbackslash}Phi\$(1020) meson is not suppressed. These particles are also used as probes to study the mechanisms of particle production. The shape of the \$p\_\{{\textbackslash}rm T\}\$ distribution of the \${\textbackslash}Phi\$(1020) meson, but not its yield, is reproduced fairly well by hydrodynamic models for central Pb-Pb collisions. In central Pb-Pb collisions at low and intermediate \$p\_\{{\textbackslash}rm T\}\$, the p/\${\textbackslash}Phi\$(1020) ratio is flat in \$p\_\{{\textbackslash}rm T\}\$, while the p/\${\textbackslash}pi\$ and \${\textbackslash}Phi\$(1020)/\${\textbackslash}pi\$ ratios show a pronounced increase and have similar shapes to each other. These results indicate that the shapes of the \$p\_\{{\textbackslash}rm T\}\$ distributions of these particles in central Pb-Pb collisions are determined predominantly by the particle masses and radial flow. Finally, \${\textbackslash}Phi\$(1020) production in Pb-Pb collisions is enhanced, with respect to the yield in pp collisions and the yield of charged pions, by an amount similar to the \${\textbackslash}Lambda\$ and \${\textbackslash}Xi\$.},
	urldate = {2021-04-26},
	journal = {arXiv:1404.0495 [hep-ex, physics:nucl-ex]},
	author = {ALICE Collaboration},
	month = feb,
	year = {2015},
	note = {arXiv: 1404.0495},
	keywords = {High Energy Physics - Experiment, Nuclear Experiment},
	annote = {Comment: 35 pages, 14 captioned figures, 2 tables, authors from page 30, published version, figures at http://aliceinfo.cern.ch/ArtSubmission/node/1153},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/GYRXBQ9J/ALICE Collaboration - 2015 - K(892)\$^ 0 \$ and \$Phi\$(1020) production in Pb-Pb.pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/SK5KCQ6U/1404.html:text/html},
}

@article{alice_collaboration_multiplicity_2019-1,
	title = {Multiplicity dependence of {K}*(892)\${\textasciicircum}\{0\}\$ and \${\textbackslash}phi\$(1020) production in pp collisions at \${\textbackslash}sqrt\{s\}\$ = 13 {TeV}},
	url = {http://arxiv.org/abs/1910.14397},
	abstract = {Measurements of identified hadrons as a function of the charged-particle multiplicity in pp collisions enable a search for the onset of collective effects in small collision systems. With such measurements, it is possible to study the mechanisms that determine the shapes of hadron transverse momentum (\$p\_\{{\textbackslash}rm\{T\}\}\$) spectra, to search for possible modifications of the yields of short-lived hadronic resonances due to scattering effects in the hadron-gas phase, and to investigate different explanations for the multiplicity evolution of strangeness production provided by phenomenological models. In this paper, these topics are addressed through measurements of the \${\textbackslash}rm\{K\}{\textasciicircum}\{*\}(892){\textasciicircum}\{0\}\$ and \${\textbackslash}phi(1020)\$ mesons at midrapidity in pp collisions at \${\textbackslash}sqrt\{s\}\$ = 13 TeV as a function of the charged-particle multiplicity. The results include the \$p\_\{{\textbackslash}rm\{T\}\}\$ spectra, \$p\_\{{\textbackslash}rm\{T\}\}\$-integrated yields, mean transverse momenta, and the ratios of the yields of these resonances to those of longer-lived hadrons. Comparisons with results from other collision systems and energies, as well as predictions from phenomenological models, are also discussed.},
	urldate = {2021-04-28},
	journal = {arXiv:1910.14397 [hep-ex, physics:nucl-ex]},
	author = {ALICE Collaboration},
	month = oct,
	year = {2019},
	note = {arXiv: 1910.14397},
	keywords = {High Energy Physics - Experiment, Nuclear Experiment},
	annote = {Comment: 24 pages, 6 captioned figures, 2 tables, authors from page 19, submitted to PLB, figures at http://alice-publications.web.cern.ch/node/5644},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/B8PYLD59/ALICE Collaboration - 2019 - Multiplicity dependence of K(892)\$^ 0 \$ and \$phi.pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/G29JVAGJ/1910.html:text/html},
}

@article{adam_production_2016,
	title = {Production of {K}\$\${\textasciicircum}\{*\}\$\$(892)\$\${\textasciicircum}\{0\}\$\$and \$\${\textbackslash}phi \$\$(1020) in p–{Pb} collisions at \$\${\textbackslash}sqrt\{s\_\{\{{\textbackslash}text \{{NN}\}\}\}\}\$\$= 5.02 {TeV}},
	volume = {76},
	issn = {1434-6052},
	url = {https://doi.org/10.1140/epjc/s10052-016-4088-7},
	doi = {10.1140/epjc/s10052-016-4088-7},
	abstract = {The production of K\$\${\textasciicircum}\{*\}\$\$(892)\$\${\textasciicircum}\{0\}\$\$and \$\${\textbackslash}phi \$\$(1020) mesons has been measured in p–Pb collisions at \$\${\textbackslash}sqrt\{s\_\{\{{\textbackslash}text \{NN\}\}\}\}\$\$\$\$=\$\$5.02 TeV. K\$\${\textasciicircum}\{*0\}\$\$and \$\${\textbackslash}phi \$\$are reconstructed via their decay into charged hadrons with the ALICE detector in the rapidity range \$\$-0.5 {\textless}y {\textless}0\$\$. The transverse momentum spectra, measured as a function of the multiplicity, have a p\$\$\_\{{\textbackslash}mathrm \{T\}\}\$\$range from 0 to 15 GeV/c for K\$\${\textasciicircum}\{*0\}\$\$and from 0.3 to 21 GeV/c for \$\${\textbackslash}phi \$\$. Integrated yields, mean transverse momenta and particle ratios are reported and compared with results in pp collisions at \$\${\textbackslash}sqrt\{s\}\$\$\$\$=\$\$7 TeV and Pb–Pb collisions at \$\${\textbackslash}sqrt\{s\_\{\{{\textbackslash}text \{NN\}\}\}\}\$\$\$\$=\$\$2.76 TeV. In Pb–Pb and p–Pb collisions, K\$\${\textasciicircum}\{*0\}\$\$and \$\${\textbackslash}phi \$\$probe the hadronic phase of the system and contribute to the study of particle formation mechanisms by comparison with other identified hadrons. For this purpose, the mean transverse momenta and the differential proton-to-\$\${\textbackslash}phi \$\$ ratio are discussed as a function of the multiplicity of the event. The short-lived K\$\${\textasciicircum}\{*0\}\$\$is measured to investigate re-scattering effects, believed to be related to the size of the system and to the lifetime of the hadronic phase.},
	language = {en},
	number = {5},
	urldate = {2021-04-28},
	journal = {The European Physical Journal C},
	author = {Adam, J. and Adamová, D. and Aggarwal, M. M. and Aglieri Rinella, G. and Agnello, M. and Agrawal, N. and Ahammed, Z. and Ahmad, S. and Ahn, S. U. and Aiola, S. and Akindinov, A. and Alam, S. N. and Aleksandrov, D. and Alessandro, B. and Alexandre, D. and Alfaro Molina, R. and Alici, A. and Alkin, A. and Almaraz, J. R. M. and Alme, J. and Alt, T. and Altinpinar, S. and Altsybeev, I. and Alves Garcia Prado, C. and Andrei, C. and Andronic, A. and Anguelov, V. and Antičić, T. and Antinori, F. and Antonioli, P. and Aphecetche, L. and Appelshäuser, H. and Arcelli, S. and Arnaldi, R. and Arnold, O. W. and Arsene, I. C. and Arslandok, M. and Audurier, B. and Augustinus, A. and Averbeck, R. and Azmi, M. D. and Badalà, A. and Baek, Y. W. and Bagnasco, S. and Bailhache, R. and Bala, R. and Balasubramanian, S. and Baldisseri, A. and Baral, R. C. and Barbano, A. M. and Barbera, R. and Barile, F. and Barnaföldi, G. G. and Barnby, L. S. and Barret, V. and Bartalini, P. and Barth, K. and Bartke, J. and Bartsch, E. and Basile, M. and Bastid, N. and Basu, S. and Bathen, B. and Batigne, G. and Batista Camejo, A. and Batyunya, B. and Batzing, P. C. and Bearden, I. G. and Beck, H. and Bedda, C. and Behera, N. K. and Belikov, I. and Bellini, F. and Bello Martinez, H. and Bellwied, R. and Belmont, R. and Belmont-Moreno, E. and Belyaev, V. and Benacek, P. and Bencedi, G. and Beole, S. and Berceanu, I. and Bercuci, A. and Berdnikov, Y. and Berenyi, D. and Bertens, R. A. and Berzano, D. and Betev, L. and Bhasin, A. and Bhat, I. R. and Bhati, A. K. and Bhattacharjee, B. and Bhom, J. and Bianchi, L. and Bianchi, N. and Bianchin, C. and Bielčík, J. and Bielčíková, J. and Bilandzic, A. and Biro, G. and Biswas, R. and Biswas, S. and Bjelogrlic, S. and Blair, J. T. and Blau, D. and Blume, C. and Bock, F. and Bogdanov, A. and Bøggild, H. and Boldizsár, L. and Bombara, M. and Book, J. and Borel, H. and Borissov, A. and Borri, M. and Bossú, F. and Botta, E. and Bourjau, C. and Braun-Munzinger, P. and Bregant, M. and Breitner, T. and Broker, T. A. and Browning, T. A. and Broz, M. and Brucken, E. J. and Bruna, E. and Bruno, G. E. and Budnikov, D. and Buesching, H. and Bufalino, S. and Buncic, P. and Busch, O. and Buthelezi, Z. and Butt, J. B. and Buxton, J. T. and Caffarri, D. and Cai, X. and Caines, H. and Calero Diaz, L. and Caliva, A. and Calvo Villar, E. and Camerini, P. and Carena, F. and Carena, W. and Carnesecchi, F. and Castillo Castellanos, J. and Castro, A. J. and Casula, E. A. R. and Ceballos Sanchez, C. and Cerello, P. and Cerkala, J. and Chang, B. and Chapeland, S. and Chartier, M. and Charvet, J. L. and Chattopadhyay, S. and Chattopadhyay, S. and Chauvin, A. and Chelnokov, V. and Cherney, M. and Cheshkov, C. and Cheynis, B. and Chibante Barroso, V. and Chinellato, D. D. and Cho, S. and Chochula, P. and Choi, K. and Chojnacki, M. and Choudhury, S. and Christakoglou, P. and Christensen, C. H. and Christiansen, P. and Chujo, T. and Chung, S. U. and Cicalo, C. and Cifarelli, L. and Cindolo, F. and Cleymans, J. and Colamaria, F. and Colella, D. and Collu, A. and Colocci, M. and Conesa Balbastre, G. and Conesa del Valle, Z. and Connors, M. E. and Contreras, J. G. and Cormier, T. M. and Corrales Morales, Y. and Cortés Maldonado, I. and Cortese, P. and Cosentino, M. R. and Costa, F. and Crochet, P. and Cruz Albino, R. and Cuautle, E. and Cunqueiro, L. and Dahms, T. and Dainese, A. and Danisch, M. C. and Danu, A. and Das, D. and Das, I. and Das, S. and Dash, A. and Dash, S. and De, S. and De Caro, A. and de Cataldo, G. and de Conti, C. and de Cuveland, J. and De Falco, A. and De Gruttola, D. and De Marco, N. and De Pasquale, S. and Deisting, A. and Deloff, A. and Dénes, E. and Deplano, C. and Dhankher, P. and Di Bari, D. and Di Mauro, A. and Di Nezza, P. and Diaz Corchero, M. A. and Dietel, T. and Dillenseger, P. and Divià, R. and Djuvsland, Ø. and Dobrin, A. and Domenicis Gimenez, D. and Dönigus, B. and Dordic, O. and Drozhzhova, T. and Dubey, A. K. and Dubla, A. and Ducroux, L. and Dupieux, P. and Ehlers, R. J. and Elia, D. and Endress, E. and Engel, H. and Epple, E. and Erazmus, B. and Erdemir, I. and Erhardt, F. and Espagnon, B. and Estienne, M. and Esumi, S. and Eum, J. and Evans, D. and Evdokimov, S. and Eyyubova, G. and Fabbietti, L. and Fabris, D. and Faivre, J. and Fantoni, A. and Fasel, M. and Feldkamp, L. and Feliciello, A. and Feofilov, G. and Ferencei, J. and Fernández Téllez, A. and Ferreiro, E. G. and Ferretti, A. and Festanti, A. and Feuillard, V. J. G. and Figiel, J. and Figueredo, M. A. S. and Filchagin, S. and Finogeev, D. and Fionda, F. M. and Fiore, E. M. and Fleck, M. G. and Floris, M. and Foertsch, S. and Foka, P. and Fokin, S. and Fragiacomo, E. and Francescon, A. and Frankenfeld, U. and Fronze, G. G. and Fuchs, U. and Furget, C. and Furs, A. and Fusco Girard, M. and Gaardhøje, J. J. and Gagliardi, M. and Gago, A. M. and Gallio, M. and Gangadharan, D. R. and Ganoti, P. and Gao, C. and Garabatos, C. and Garcia-Solis, E. and Gargiulo, C. and Gasik, P. and Gauger, E. F. and Germain, M. and Gheata, A. and Gheata, M. and Ghosh, P.},
	month = apr,
	year = {2016},
	pages = {245},
	file = {Springer Full Text PDF:/home/romain/Zotero/storage/KUC9SXPM/Adam et al. - 2016 - Production of K\$\$^ \$\$(892)\$\$^ 0 \$\$and \$\$phi \$\$(.pdf:application/pdf},
}

@misc{noauthor_systematic_nodate,
	title = {Systematic fits of identified particle {pT} spectra with {Lévy}-{Tsallis} and modified {Bylinkin} functions {\textbar} {Public} \& {Analysis} {Notes}},
	url = {https://alice-notes.web.cern.ch/node/786},
	urldate = {2021-04-28},
	file = {Systematic fits of identified particle pT spectra with Lévy-Tsallis and modified Bylinkin functions | Public & Analysis Notes:/home/romain/Zotero/storage/P2BMSIKP/786.html:text/html;2019-12-02-_ANA-786-SystematicFits-WithLevyTsallisModBylinkin-v3-2019-12-02(1).pdf:/home/romain/Documents/Paper/2019-12-02-_ANA-786-SystematicFits-WithLevyTsallisModBylinkin-v3-2019-12-02(1).pdf:application/pdf},
}

@article{maire_levy-tsallis_2019,
	title = {with {Lévy}-{Tsallis} and modified-{Bylinkin} functions},
	language = {en},
	author = {Maire, Antonin},
	year = {2019},
	pages = {91},
}

@article{alice_collaboration_production_2020,
	title = {Production of light-flavor hadrons in pp collisions at \${\textbackslash}sqrt\{s\}\$ = 7 and \${\textbackslash}sqrt\{s\}\$ = 13 {TeV}},
	url = {http://arxiv.org/abs/2005.11120},
	abstract = {The production of \${\textbackslash}pi{\textasciicircum}\{{\textbackslash}pm\}\$, \${\textbackslash}rm\{K\}{\textasciicircum}\{{\textbackslash}pm\}\$, \${\textbackslash}rm\{K\}{\textasciicircum}\{0\}\_\{S\}\$, \${\textbackslash}rm\{K\}*(892){\textasciicircum}\{0\}\$, \${\textbackslash}rm\{p\}\$, \${\textbackslash}phi(1020)\$, \${\textbackslash}Lambda\$, \${\textbackslash}Xi{\textasciicircum}\{-\}\$, \${\textbackslash}Omega{\textasciicircum}\{-\}\$, and their antiparticles was measured in inelastic proton-proton (pp) collisions at a center-of-mass energy of \${\textbackslash}sqrt\{s\}\$ = 13 TeV at midrapidity (\${\textbar}y{\textbar}{\textless}0.5\$) as a function of transverse momentum (\$p\_\{{\textbackslash}rm\{T\}\}\$) using the ALICE detector at the CERN LHC. Furthermore, the single-particle \$p\_\{{\textbackslash}rm\{T\}\}\$ distributions of \${\textbackslash}rm\{K\}{\textasciicircum}\{0\}\_\{S\}\$, \${\textbackslash}Lambda\$, and \${\textbackslash}overline\{{\textbackslash}Lambda\}\$ in inelastic pp collisions at \${\textbackslash}sqrt\{s\}\$ = 7 TeV are reported here for the first time. The \$p\_\{{\textbackslash}rm\{T\}\}\$ distributions are studied at midrapidity within the transverse momentum range \$0{\textbackslash}leq p\_\{{\textbackslash}rm\{T\}\}{\textbackslash}leq20\$ GeV/\$c\$, depending on the particle species. The \$p\_\{{\textbackslash}rm\{T\}\}\$ spectra, integrated yields, and particle yield ratios are discussed as a function of collision energy and compared with measurements at lower \${\textbackslash}sqrt\{s\}\$ and with results from various general-purpose QCD-inspired Monte Carlo models. A hardening of the spectra at high \$p\_\{{\textbackslash}rm\{T\}\}\$ with increasing collision energy is observed, which is similar for all particle species under study. The transverse mass and \$x\_\{{\textbackslash}rm\{T\}\}{\textbackslash}equiv2p\_\{{\textbackslash}rm\{T\}\}/{\textbackslash}sqrt\{s\}\$ scaling properties of hadron production are also studied. As the collision energy increases from \${\textbackslash}sqrt\{s\}\$ = 7 to 13 TeV, the yields of non- and single-strange hadrons normalized to the pion yields remain approximately constant as a function of \${\textbackslash}sqrt\{s\}\$, while ratios for multi-strange hadrons indicate enhancements. The \$p\_\{{\textbackslash}rm\{T\}\}\$-differential cross sections of \${\textbackslash}pi{\textasciicircum}\{{\textbackslash}pm\}\$, \${\textbackslash}rm\{K\}{\textasciicircum}\{{\textbackslash}pm\}\$ and \${\textbackslash}rm\{p\}\$ (\${\textbackslash}overline\{{\textbackslash}rm\{p\}\}\$) are compared with next-to-leading order perturbative QCD calculations, which are found to overestimate the cross sections for \${\textbackslash}pi{\textasciicircum}\{{\textbackslash}pm\}\$ and \${\textbackslash}rm\{p\}\$ (\${\textbackslash}overline\{{\textbackslash}rm\{p\}\}\$) at high \$p\_\{{\textbackslash}rm\{T\}\}\$.},
	urldate = {2021-04-28},
	journal = {arXiv:2005.11120 [hep-ex, physics:nucl-ex]},
	author = {ALICE Collaboration},
	month = may,
	year = {2020},
	note = {arXiv: 2005.11120},
	keywords = {High Energy Physics - Experiment, Nuclear Experiment},
	annote = {Comment: 52 pages, 18 figures, 8 tables, authors from page 47, submitted to EPJC, figures at http://alice-publications.web.cern.ch/node/6218},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/PMX2AFB8/ALICE Collaboration - 2020 - Production of light-flavor hadrons in pp collision.pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/8BZ55THG/2005.html:text/html},
}

@article{alice_collaboration_multiplicity_2020,
	title = {Multiplicity dependence of (multi-)strange hadron production in proton-proton collisions at \${\textbackslash}sqrt\{s\}\$ = 13 {TeV}},
	volume = {80},
	issn = {1434-6044, 1434-6052},
	url = {http://arxiv.org/abs/1908.01861},
	doi = {10.1140/epjc/s10052-020-7673-8},
	abstract = {The production rates and the transverse momentum distribution of strange hadrons at mid-rapidity (\${\textbackslash} {\textbar}y{\textbackslash} {\textbar} {\textless} 0.5\$) are measured in proton-proton collisions at \${\textbackslash}sqrt\{s\}\$ = 13 TeV as a function of the charged particle multiplicity, using the ALICE detector at the LHC. The production rates of \${\textbackslash}rm\{K\}{\textasciicircum}\{0\}\_\{S\}\$, \${\textbackslash}Lambda\$, \${\textbackslash}Xi\$, and \${\textbackslash}Omega\$ increase with the multiplicity faster than what is reported for inclusive charged particles. The increase is found to be more pronounced for hadrons with a larger strangeness content. Possible auto-correlations between the charged particles and the strange hadrons are evaluated by measuring the event-activity with charged particle multiplicity estimators covering different pseudorapidity regions. When comparing to lower energy results, the yields of strange hadrons are found to depend only on the mid-rapidity charged particle multiplicity. Several features of the data are reproduced qualitatively by general purpose QCD Monte Carlo models that take into account the effect of densely-packed QCD strings in high multiplicity collisions. However, none of the tested models reproduce the data quantitatively. This work corroborates and extends the ALICE findings on strangeness production in proton-proton collisions at 7 TeV.},
	number = {2},
	urldate = {2021-04-28},
	journal = {The European Physical Journal C},
	author = {ALICE Collaboration},
	month = feb,
	year = {2020},
	note = {arXiv: 1908.01861},
	keywords = {High Energy Physics - Experiment, Nuclear Experiment},
	pages = {167},
	annote = {Comment: 36 pages, 14 captioned figures, 4 tables, authors from page 31, published version, figures at http://alice-publications.web.cern.ch/node/5464},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/A3K3BQTH/ALICE Collaboration - 2020 - Multiplicity dependence of (multi-)strange hadron .pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/38KGDLW5/1908.html:text/html},
}

@misc{noauthor_going_2021,
	title = {Going with the flow},
	url = {https://cerncourier.com/a/going-with-the-flow/},
	abstract = {The ALICE experiment is making strides towards understanding how charm and beauty quarks flow within cooling droplets of quark–gluon plasma at the LHC, shedding light on the extreme conditions of the early universe.},
	language = {en-GB},
	urldate = {2021-04-30},
	journal = {CERN Courier},
	month = apr,
	year = {2021},
	note = {Section: Strong interactions},
	file = {Snapshot:/home/romain/Zotero/storage/3GXB85WQ/going-with-the-flow.html:text/html},
}

@misc{noauthor_transverse_nodate,
	title = {Transverse momentum spectra of inclusive charged hadrons in pp collisions at √s =13 {TeV} {\textbar} {Public} \& {Analysis} {Notes}},
	url = {https://alice-notes.web.cern.ch/node/415},
	urldate = {2021-05-04},
	file = {Transverse momentum spectra of inclusive charged hadrons in pp collisions at √s =13 TeV | Public & Analysis Notes:/home/romain/Zotero/storage/UIDBE3TW/415.html:text/html;2013-Nov-27-analysis_note-PrimaryParticle.pdf:/home/romain/Documents/Paper/2013-Nov-27-analysis_note-PrimaryParticle.pdf:application/pdf},
}

@article{alice_collaboration_experimental_2021,
	title = {Experimental evidence for an attractive p-\${\textbackslash}phi\$ interaction},
	url = {http://arxiv.org/abs/2105.05578},
	abstract = {This Letter presents the first experimental evidence of the attractive strong interaction between a proton and a \${\textbackslash}phi\$ meson. The result is obtained from two-particle correlations of combined p-\${\textbackslash}phi {\textbackslash}oplus {\textbackslash}overline\{{\textbackslash}rm \{p\}\}\$-\${\textbackslash}phi\$ pairs measured in high-multiplicity pp collisions at \${\textbackslash}sqrt\{s\}{\textasciitilde}={\textasciitilde}13\$ TeV by the ALICE collaboration. The spin-averaged scattering length and effective range of the p-\${\textbackslash}phi\$ interaction are extracted from the fully corrected correlation function employing the Lednick{\textbackslash}'y-Lyuboshits approach. In particular, the imaginary part of the scattering length vanishes within uncertainties, indicating that inelastic processes do not play a prominent role for the p-\${\textbackslash}phi\$ interaction. These data demonstrate that the interaction is dominated by elastic p-\${\textbackslash}phi\$ scattering. Furthermore, an analysis employing phenomenological Gaussian- and Yukawa-type potentials is conducted. Under the assumption of the latter, the N-\${\textbackslash}phi\$ coupling constant is found to be \$g\_\{{\textbackslash}rm\{N\}-{\textbackslash}phi\} = 0.14{\textbackslash}pm 0.03{\textbackslash},({\textbackslash}mathrm\{stat.\}){\textbackslash}pm 0.02{\textbackslash},({\textbackslash}mathrm\{syst.\})\$. This work provides valuable experimental input to accomplish a self-consistent description of the N-\${\textbackslash}phi\$ interaction, which is particularly relevant for the more fundamental studies on partial restoration of chiral symmetry in nuclear medium.},
	urldate = {2021-05-14},
	journal = {arXiv:2105.05578 [hep-ex, physics:nucl-ex]},
	author = {ALICE Collaboration},
	month = may,
	year = {2021},
	note = {arXiv: 2105.05578},
	keywords = {High Energy Physics - Experiment, Nuclear Experiment},
	annote = {Comment: 18 pages, 2 captioned figure, 1 tables, authors from page 12, submitted to PRL, figures at http://alice-publications.web.cern.ch/node/7086},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/33IRTJGF/ALICE Collaboration - 2021 - Experimental evidence for an attractive p-\$phi\$ i.pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/4YF9XSNT/2105.html:text/html},
}

@misc{felix_reidt_alice_2021,
	title = {{ALICE} {Upgrades} - {SQM} 2021},
	url = {https://indico.cern.ch/event/985652/contributions/4298255/attachments/2245839/3808632/SQM2021_ALICE_Upgrades_freidt.pdf},
	language = {En},
	author = {Felix Reidt},
	month = may,
	year = {2021},
	file = {SQM2021_ALICE_Upgrades_freidt.pdf:/home/romain/Documents/Paper/SQM2021_ALICE_Upgrades_freidt.pdf:application/pdf},
}

@article{cms_collaboration_evidence_2015,
	title = {Evidence for collective multi-particle correlations in {pPb} collisions},
	volume = {115},
	issn = {0031-9007, 1079-7114},
	url = {http://arxiv.org/abs/1502.05382},
	doi = {10.1103/PhysRevLett.115.012301},
	abstract = {The second-order azimuthal anisotropy Fourier harmonics, v2, are obtained in pPb and PbPb collisions over a wide pseudorapidity (eta) range based on correlations among six or more charged particles. The pPb data, corresponding to an integrated luminosity of 35 inverse nanobarns, were collected during the 2013 LHC pPb run at a nucleon-nucleon center-of-mass energy of 5.02 TeV by the CMS experiment. A sample of semi-peripheral PbPb collision data at sqrt(s[NN])= 2.76 TeV, corresponding to an integrated luminosity of 2.5 inverse microbarns and covering a similar range of particle multiplicities as the pPb data, is also analyzed for comparison. The six- and eight-particle cumulant and the Lee-Yang zeros methods are used to extract the v2 coefficients, extending previous studies of two- and four-particle correlations. For both the pPb and PbPb systems, the v2 values obtained with correlations among more than four particles are consistent with previously published four-particle results. These data support the interpretation of a collective origin for the previously observed long-range (large Delta[eta]) correlations in both systems. The ratios of v2 values corresponding to correlations including different numbers of particles are compared to theoretical predictions that assume a hydrodynamic behavior of a pPb system dominated by fluctuations in the positions of participant nucleons. These results provide new insights into the multi-particle dynamics of collision systems with a very small overlapping region.},
	number = {1},
	urldate = {2021-06-15},
	journal = {Physical Review Letters},
	author = {CMS Collaboration},
	month = jun,
	year = {2015},
	note = {arXiv: 1502.05382},
	keywords = {High Energy Physics - Experiment, Nuclear Experiment},
	pages = {012301},
	annote = {Comment: Replaced with published version. Added journal reference and DOI},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/4G374GN2/CMS Collaboration - 2015 - Evidence for collective multi-particle correlation.pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/RKG3UGL7/1502.html:text/html},
}

@article{cms_collaboration_observation_2010,
	title = {Observation of {Long}-{Range} {Near}-{Side} {Angular} {Correlations} in {Proton}-{Proton} {Collisions} at the {LHC}},
	volume = {2010},
	issn = {1029-8479},
	url = {http://arxiv.org/abs/1009.4122},
	doi = {10.1007/JHEP09(2010)091},
	abstract = {Results on two-particle angular correlations for charged particles emitted in proton-proton collisions at center-of-mass energies of 0.9, 2.36, and 7 TeV are presented, using data collected with the CMS detector over a broad range of pseudorapidity (eta) and azimuthal angle (phi). Short-range correlations in Delta(eta), which are studied in minimum bias events, are characterized using a simple "independent cluster" parametrization in order to quantify their strength (cluster size) and their extent in eta (cluster decay width). Long-range azimuthal correlations are studied differentially as a function of charged particle multiplicity and particle transverse momentum using a 980 inverse nb data set at 7 TeV. In high multiplicity events, a pronounced structure emerges in the two-dimensional correlation function for particle pairs with intermediate transverse momentum of 1-3 GeV/c, 2.0{\textless} {\textbar}Delta(eta){\textbar} {\textless}4.8 and Delta(phi) near 0. This is the first observation of such a long-range, near-side feature in two-particle correlation functions in pp or p p-bar collisions.},
	number = {9},
	urldate = {2021-06-15},
	journal = {Journal of High Energy Physics},
	author = {CMS Collaboration},
	month = sep,
	year = {2010},
	note = {arXiv: 1009.4122},
	keywords = {High Energy Physics - Experiment},
	pages = {91},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/QYD5WLGS/CMS Collaboration - 2010 - Observation of Long-Range Near-Side Angular Correl.pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/34DKB3SX/1009.html:text/html},
}

@article{alice_collaboration_enhanced_2017,
	title = {Enhanced production of multi-strange hadrons in high-multiplicity proton-proton collisions},
	volume = {13},
	issn = {1745-2473, 1745-2481},
	url = {http://arxiv.org/abs/1606.07424},
	doi = {10.1038/nphys4111},
	abstract = {At sufficiently high temperature and energy density, nuclear matter undergoes a transition to a phase in which quarks and gluons are not confined: the Quark-Gluon Plasma (QGP) [1]. Such an extreme state of strongly-interacting QCD (Quantum Chromo-Dynamics) matter is produced in the laboratory with high-energy collisions of heavy nuclei, where an enhanced production of strange hadrons is observed [2-6]. Strangeness enhancement, originally proposed as a signature of QGP formation in nuclear collisions [7], is more pronounced for multi-strange baryons. Several effects typical of heavy-ion phenomenology have been observed in high-multiplicity proton-proton (pp) collisions [8,9]. Yet, enhanced production of multi-strange particles has not been reported so far. Here we present the first observation of strangeness enhancement in high-multiplicity pp collisions. We find that the integrated yields of strange and multi-strange particles relative to pions increases significantly with the event charged-particle multiplicity. The measurements are in remarkable agreement with p-Pb collision results [10,11] indicating that the phenomenon is related to the final system created in the collision. In high-multiplicity events strangeness production reaches values similar to those observed in Pb-Pb collisions, where a QGP is formed.},
	number = {6},
	urldate = {2021-06-15},
	journal = {Nature Physics},
	author = {ALICE Collaboration},
	month = jun,
	year = {2017},
	note = {arXiv: 1606.07424},
	keywords = {High Energy Physics - Experiment, Nuclear Experiment},
	pages = {535--539},
	annote = {Comment: 18 pages, 4 captioned figures, 1 table, authors from page 13, published version, figures at http://aliceinfo.cern.ch/ArtSubmission/node/2929, Nature Physics 2017},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/MLWQ7S5X/ALICE Collaboration - 2017 - Enhanced production of multi-strange hadrons in hi.pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/5P273MJD/1606.html:text/html},
}

@article{alice_collaboration_pseudorapidity_2020,
	title = {Pseudorapidity distributions of charged particles as a function of mid and forward rapidity mutiplicities in pp collisions at \${\textbackslash}sqrt\{s\}\$ = 5.02, 7 and 13 {TeV}},
	url = {http://arxiv.org/abs/2009.09434},
	abstract = {The multiplicity dependence of the pseudorapidity density of charged particles in proton-proton (pp) collisions at centre-of-mass energies \${\textbackslash}sqrt\{s\}\$ = 5.02, 7 and 13 TeV measured by ALICE is reported. The analysis relies on track segments measured in the midrapidity range (\${\textbar}{\textbackslash}eta{\textbar} {\textless} 1.5\$). Results are presented for inelastic events having at least one charged particle produced in the pseudorapidity interval \${\textbar}{\textbackslash}eta{\textbar}{\textless}1\$ (\${\textbackslash}mathrm\{INEL\}\_\{{\textgreater}0\}\$). The multiplicity dependence of the pseudorapidy density of charged particles is measured with mid and forward rapidity multiplicity estimators, the latter being less affected by autocorrelations. A detailed comparison with predictions from the PYTHIA 8 and EPOS LHC event generators is also presented. Both generators provide a good description of the data.},
	urldate = {2021-07-15},
	journal = {arXiv:2009.09434 [hep-ex, physics:nucl-ex]},
	author = {ALICE Collaboration},
	month = sep,
	year = {2020},
	note = {arXiv: 2009.09434},
	keywords = {High Energy Physics - Experiment, Nuclear Experiment},
	annote = {Comment: 20 pages, 6 captioned figures, 3 tables, authors from page 15, submitted to EPJC, figures at http://alice-publications.web.cern.ch/node/6679"},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/AVYELR6D/ALICE Collaboration - 2020 - Pseudorapidity distributions of charged particles .pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/E4T239SM/2009.html:text/html},
}

@article{adolfsson_studying_2020,
	title = {Studying particle production in small systems through correlation measurements in {ALICE}},
	url = {http://arxiv.org/abs/2005.14675},
	abstract = {In these proceedings, measurements of angular correlations between hadron pairs in pp collisions obtained by the ALICE experiment at the LHC are presented and compared with phenomenological predictions. Correlations between particles carrying the same and opposite quantum numbers are studied to understand the hadron production mechanism, and the difference between same-sign and opposite-sign correlations is used to probe charge-dependent effects in particle production. Correlation measurements dominated by minijet fragmentation agree well with the models, but other results, in particular correlations between baryons and strange hadrons, are not yet understood.},
	urldate = {2021-08-06},
	journal = {arXiv:2005.14675 [hep-ex]},
	author = {Adolfsson, Jonatan},
	month = may,
	year = {2020},
	note = {arXiv: 2005.14675},
	keywords = {High Energy Physics - Experiment},
	annote = {Comment: 7 pages, 5 figures; conference proceedings of Excited QCD 2020, 2-8 February 2020; submitted to Acta Physica Polonica B - Proceedings Supplement},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/AX9PQPBX/Adolfsson - 2020 - Studying particle production in small systems thro.pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/NVFUN3FF/2005.html:text/html},
}

@article{bjorken_highly_1983,
	title = {Highly relativistic nucleus-nucleus collisions: {The} central rapidity region},
	volume = {27},
	shorttitle = {Highly relativistic nucleus-nucleus collisions},
	url = {https://link.aps.org/doi/10.1103/PhysRevD.27.140},
	doi = {10.1103/PhysRevD.27.140},
	abstract = {The space-time evolution of the hadronic matter produced in the central rapidity region in extreme relativistic nucleus-nucleus collisions is described. We find, in agreement with previous studies, that quark-gluon plasma is produced at a temperature ≳200-300 MeV, and that it should survive over a time scale ≳5 fm/c. Our description relies on the existence of a flat central plateau and on the applicability of hydrodynamics.},
	number = {1},
	urldate = {2021-08-18},
	journal = {Physical Review D},
	author = {Bjorken, J. D.},
	month = jan,
	year = {1983},
	note = {Publisher: American Physical Society},
	pages = {140--151},
	file = {Full Text PDF:/home/romain/Zotero/storage/VC53KXR4/Bjorken - 1983 - Highly relativistic nucleus-nucleus collisions Th.pdf:application/pdf;APS Snapshot:/home/romain/Zotero/storage/5H66AKZ9/PhysRevD.27.html:text/html},
}

@article{alice_collaboration_performance_2014,
	title = {Performance of the {ALICE} {Experiment} at the {CERN} {LHC}},
	volume = {29},
	issn = {0217-751X, 1793-656X},
	url = {http://arxiv.org/abs/1402.4476},
	doi = {10.1142/S0217751X14300440},
	abstract = {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.},
	number = {24},
	urldate = {2021-08-19},
	journal = {International Journal of Modern Physics A},
	author = {ALICE Collaboration},
	month = sep,
	year = {2014},
	note = {arXiv: 1402.4476},
	keywords = {High Energy Physics - Experiment, Nuclear Experiment},
	pages = {1430044},
	annote = {Comment: 109 pages, 88 captioned figures, 12 tables, authors from page 104, published version, figures at http://aliceinfo.cern.ch/ArtSubmission/node/716},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/EX2GD3GJ/ALICE Collaboration - 2014 - Performance of the ALICE Experiment at the CERN LH.pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/MUKV3CHH/1402.html:text/html},
}

@article{collaboration_alice_nodate,
	title = {{ALICE} 2016-2017-2018 luminosity determination for pp collisions at \${\textbackslash}sqrt\{s\}\$ = 13 {TeV}},
	abstract = {Luminosity determination in ALICE is based on the measurement of visible cross sections in van der Meer (vdM) scans. In the Run 2 (2015√–2018), the Large Hadron Collider provided proton–proton collisions at a centre-of-mass energy of s = 13 TeV. One vdM scan per year was performed, which allowed for calibration of the ALICE luminometers: the T0 detector with pseudorapidity coverage 4.6 {\textless} η {\textless} 4.9, −3.3 {\textless} η {\textless} −3.0, and the V0 detector with pseudorapidity coverage 2.8 {\textless} η {\textless} 5.1, −3.7 {\textless} η {\textless} −1.7. This document presents the luminosity determination methodology and results for the years 2016, 2017 and 2018.},
	language = {en},
	author = {Collaboration, ALICE},
	pages = {24},
	file = {Collaboration - ALICE 2016-2017-2018 lum√inosity determination for.pdf:/home/romain/Zotero/storage/PBQMQ83M/Collaboration - ALICE 2016-2017-2018 lum√inosity determination for.pdf:application/pdf},
}

@article{collaboration_alice_2006,
	title = {{ALICE}: {Physics} {Performance} {Report}, {Volume} {II}},
	volume = {32},
	issn = {0954-3899},
	shorttitle = {{ALICE}},
	url = {https://doi.org/10.1088/0954-3899/32/10/001},
	doi = {10.1088/0954-3899/32/10/001},
	abstract = {ALICE is a general-purpose heavy-ion experiment designed to study the physics of strongly interacting matter and the quark–gluon plasma in nucleus–nucleus collisions at the LHC. It currently involves more than 900 physicists and senior engineers, from both the nuclear and high-energy physics sectors, from over 90 institutions in about 30 countries. The ALICE detector is designed to cope with the highest particle multiplicities above those anticipated for Pb–Pb collisions (dNch/dy up to 8000) and it will be operational at the start-up of the LHC. In addition to heavy systems, the ALICE Collaboration will study collisions of lower-mass ions, which are a means of varying the energy density, and protons (both pp and pA), which primarily provide reference data for the nucleus–nucleus collisions. In addition, the pp data will allow for a number of genuine pp physics studies. The detailed design of the different detector systems has been laid down in a number of Technical Design Reports issued between mid-1998 and the end of 2004. The experiment is currently under construction and will be ready for data taking with both proton and heavy-ion beams at the start-up of the LHC. Since the comprehensive information on detector and physics performance was last published in the ALICE Technical Proposal in 1996, the detector, as well as simulation, reconstruction and analysis software have undergone significant development. The Physics Performance Report (PPR) provides an updated and comprehensive summary of the performance of the various ALICE subsystems, including updates to the Technical Design Reports, as appropriate. The PPR is divided into two volumes. Volume I, published in 2004 (CERN/LHCC 2003-049, ALICE Collaboration 2004 J. Phys. G: Nucl. Part. Phys. 30 1517–1763), contains in four chapters a short theoretical overview and an extensive reference list concerning the physics topics of interest to ALICE, the experimental conditions at the LHC, a short summary and update of the subsystem designs, and a description of the offline framework and Monte Carlo event generators. The present volume, Volume II, contains the majority of the information relevant to the physics performance in proton–proton, proton–nucleus, and nucleus–nucleus collisions. Following an introductory overview, Chapter 5 describes the combined detector performance and the event reconstruction procedures, based on detailed simulations of the individual subsystems. Chapter 6 describes the analysis and physics reach for a representative sample of physics observables, from global event characteristics to hard processes.},
	language = {en},
	number = {10},
	urldate = {2021-08-22},
	journal = {Journal of Physics G: Nuclear and Particle Physics},
	author = {Collaboration, ALICE and Alessandro, B. and Antinori, F. and Belikov, J. A. and Blume, C. and Dainese, A. and Foka, P. and Giubellino, P. and Hippolyte, B. and Kuhn, C. and Martínez, G. and Monteno, M. and Morsch, A. and Nayak, T. K. and Nystrand, J. and Noriega, M. López and Paić, G. and Pluta, J. and Ramello, L. and Revol, J.-P. and Šafařík, K. and Schukraft, J. and Schutz, Y. and Scomparin, E. and Snellings, R. and Baillie, O. Villalobos and Vercellin, E.},
	month = sep,
	year = {2006},
	note = {Publisher: IOP Publishing},
	pages = {1295--2040},
	file = {IOP Full Text PDF:/home/romain/Zotero/storage/FFEHSC5V/Collaboration et al. - 2006 - ALICE Physics Performance Report, Volume II.pdf:application/pdf},
}

@article{voloshin_two_2005,
	title = {Two particle rapidity, transverse momentum, and azimuthal correlations in relativistic nuclear collisions and transverse radial expansion},
	volume = {749},
	issn = {03759474},
	url = {http://arxiv.org/abs/nucl-th/0410024},
	doi = {10.1016/j.nuclphysa.2004.12.053},
	abstract = {At the very first stage of an ultra-relativistic nucleus-nucleus collision new particles are produced in individual nucleon-nucleon collisions. In the transverse plane, all particles from a single \$NN\$ collision are initially located at the same position. The subsequent transverse radial expansion of the system creates strong position-momentum correlations and leads to characteristic rapidity, transverse momentum, and azimuthal correlations among the produced particles.},
	urldate = {2021-08-25},
	journal = {Nuclear Physics A},
	author = {Voloshin, Sergei A.},
	month = mar,
	year = {2005},
	note = {arXiv: nucl-th/0410024
version: 1},
	keywords = {Nuclear Theory},
	pages = {287--290},
	annote = {Comment: 4 pages. Proceedings of 18th Nuclear Physics Division Conference of the EPS (NPDC18)},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/JADDLIAM/Voloshin - 2005 - Two particle rapidity, transverse momentum, and az.pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/9W4KW5TE/0410024.html:text/html},
}

@article{alice_collaboration_multiplicity_2016,
	title = {Multiplicity and transverse momentum evolution of charge-dependent correlations in pp, p-{Pb}, and {Pb}-{Pb} collisions at the {LHC}},
	volume = {76},
	issn = {1434-6044, 1434-6052},
	url = {http://arxiv.org/abs/1509.07255},
	doi = {10.1140/epjc/s10052-016-3915-1},
	abstract = {We report on two-particle charge-dependent correlations in pp, p-Pb, and Pb-Pb collisions as a function of the pseudorapidity and azimuthal angle difference, \${\textbackslash}mathrm\{{\textbackslash}Delta\}{\textbackslash}eta\$ and \${\textbackslash}mathrm\{{\textbackslash}Delta\}{\textbackslash}varphi\$ respectively. These correlations are studied using the balance function that probes the charge creation time and the development of collectivity in the produced system. The dependence of the balance function on the event multiplicity as well as on the trigger and associated particle transverse momentum (\$p\_\{{\textbackslash}mathrm\{T\}\}\$) in pp, p-Pb, and Pb-Pb collisions at \${\textbackslash}sqrt\{s\_\{{\textbackslash}mathrm\{NN\}\}\} = 7\$, 5.02, and 2.76 TeV, respectively, are presented. In the low transverse momentum region, for \$0.2 {\textless} p\_\{{\textbackslash}mathrm\{T\}\} {\textless} 2.0\$ GeV/\$c\$, the balance function becomes narrower in both \${\textbackslash}mathrm\{{\textbackslash}Delta\}{\textbackslash}eta\$ and \${\textbackslash}mathrm\{{\textbackslash}Delta\}{\textbackslash}varphi\$ directions in all three systems for events with higher multiplicity. The experimental findings favor models that either incorporate some collective behavior (e.g. AMPT) or different mechanisms that lead to effects that resemble collective behavior (e.g. PYTHIA8 with color reconnection). For higher values of transverse momenta the balance function becomes even narrower but exhibits no multiplicity dependence, indicating that the observed narrowing with increasing multiplicity at low \$p\_\{{\textbackslash}mathrm\{T\}\}\$ is a feature of bulk particle production.},
	number = {2},
	urldate = {2021-08-25},
	journal = {The European Physical Journal C},
	author = {ALICE Collaboration},
	month = feb,
	year = {2016},
	note = {arXiv: 1509.07255},
	keywords = {High Energy Physics - Experiment, Nuclear Experiment},
	pages = {86},
	annote = {Comment: 32 pages, 12 captioned figures, 2 tables, authors from page 27, published version, figures at http://aliceinfo.cern.ch/ArtSubmission/node/1869},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/WTAEZZWF/ALICE Collaboration - 2016 - Multiplicity and transverse momentum evolution of .pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/VKD8N5PL/1509.html:text/html},
}

@misc{noauthor_alidpgreconstructeddatatakingperiodspp13tev_nodate,
	title = {{AliDPGReconstructedDataTakingPeriodspp13TeV} {\textless} {ALICE} {\textless} {TWiki}},
	url = {https://twiki.cern.ch/twiki/bin/view/ALICE/AliDPGReconstructedDataTakingPeriodspp13TeV},
	urldate = {2021-08-25},
	file = {AliDPGReconstructedDataTakingPeriodspp13TeV < ALICE < TWiki:/home/romain/Zotero/storage/874S9N6U/AliDPGReconstructedDataTakingPeriodspp13TeV.html:text/html},
}

@article{alice_collaboration_performance_2013,
	title = {Performance of the {ALICE} {VZERO} system},
	volume = {8},
	issn = {1748-0221},
	url = {http://arxiv.org/abs/1306.3130},
	doi = {10.1088/1748-0221/8/10/P10016},
	abstract = {ALICE is an LHC experiment devoted to the study of strongly interacting matter in proton-proton, proton--nucleus and nucleus-nucleus collisions at ultra-relativistic energies. The ALICE VZERO system, made of two scintillator arrays at asymmetric positions, one on each side of the interaction point, plays a central role in ALICE. In addition to its core function as a trigger, the VZERO system is used to monitor LHC beam conditions, to reject beam-induced backgrounds and to measure basic physics quantities such as luminosity, particle multiplicity, centrality and event plane direction in nucleus-nucleus collisions. After describing the VZERO system, this publication presents its performance over more than four years of operation at the LHC.},
	number = {10},
	urldate = {2021-08-26},
	journal = {Journal of Instrumentation},
	author = {ALICE Collaboration},
	month = oct,
	year = {2013},
	note = {arXiv: 1306.3130},
	keywords = {Nuclear Experiment},
	pages = {P10016--P10016},
	annote = {Comment: 20 pages, 10 captioned figures, 1 table, authors from page 15, published version, figures at http://aliceinfo.cern.ch/ArtSubmission/node/595},
	file = {arXiv Fulltext PDF:/home/romain/Zotero/storage/WXBP9BMN/ALICE Collaboration - 2013 - Performance of the ALICE VZERO system.pdf:application/pdf;arXiv.org Snapshot:/home/romain/Zotero/storage/KBP6U3LV/1306.html:text/html},
}