-
Notifications
You must be signed in to change notification settings - Fork 0
/
PrePrint_References.bib
executable file
·574 lines (537 loc) · 106 KB
/
PrePrint_References.bib
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19
20
21
22
23
24
25
26
27
28
29
30
31
32
33
34
35
36
37
38
39
40
41
42
43
44
45
46
47
48
49
50
51
52
53
54
55
56
57
58
59
60
61
62
63
64
65
66
67
68
69
70
71
72
73
74
75
76
77
78
79
80
81
82
83
84
85
86
87
88
89
90
91
92
93
94
95
96
97
98
99
100
101
102
103
104
105
106
107
108
109
110
111
112
113
114
115
116
117
118
119
120
121
122
123
124
125
126
127
128
129
130
131
132
133
134
135
136
137
138
139
140
141
142
143
144
145
146
147
148
149
150
151
152
153
154
155
156
157
158
159
160
161
162
163
164
165
166
167
168
169
170
171
172
173
174
175
176
177
178
179
180
181
182
183
184
185
186
187
188
189
190
191
192
193
194
195
196
197
198
199
200
201
202
203
204
205
206
207
208
209
210
211
212
213
214
215
216
217
218
219
220
221
222
223
224
225
226
227
228
229
230
231
232
233
234
235
236
237
238
239
240
241
242
243
244
245
246
247
248
249
250
251
252
253
254
255
256
257
258
259
260
261
262
263
264
265
266
267
268
269
270
271
272
273
274
275
276
277
278
279
280
281
282
283
284
285
286
287
288
289
290
291
292
293
294
295
296
297
298
299
300
301
302
303
304
305
306
307
308
309
310
311
312
313
314
315
316
317
318
319
320
321
322
323
324
325
326
327
328
329
330
331
332
333
334
335
336
337
338
339
340
341
342
343
344
345
346
347
348
349
350
351
352
353
354
355
356
357
358
359
360
361
362
363
364
365
366
367
368
369
370
371
372
373
374
375
376
377
378
379
380
381
382
383
384
385
386
387
388
389
390
391
392
393
394
395
396
397
398
399
400
401
402
403
404
405
406
407
408
409
410
411
412
413
414
415
416
417
418
419
420
421
422
423
424
425
426
427
428
429
430
431
432
433
434
435
436
437
438
439
440
441
442
443
444
445
446
447
448
449
450
451
452
453
454
455
456
457
458
459
460
461
462
463
464
465
466
467
468
469
470
471
472
473
474
475
476
477
478
479
480
481
482
483
484
485
486
487
488
489
490
491
492
493
494
495
496
497
498
499
500
501
502
503
504
505
506
507
508
509
510
511
512
513
514
515
516
517
518
519
520
521
522
523
524
525
526
527
528
529
530
531
532
533
534
535
536
537
538
539
540
541
542
543
544
545
546
547
548
549
550
551
552
553
554
555
556
557
558
559
560
561
562
563
564
565
566
567
568
569
570
571
572
573
574
@misc{noauthor_pdglive_nodate,
title = {{pdgLive}},
url = {http://pdglive.lbl.gov/Viewer.action},
urldate = {2020-04-29},
file = {pdgLive:/home/romain/Zotero/storage/RQXT8GYS/Viewer.html:text/html},
}
@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. K. and Baechler, J. and Bagnasco, S. and Bailhache, R. and Bala, R. and Baldisseri, A. and Baldit, A. and Bán, J. and Barbera, R. and Barberis, P.-L. and Barbet, J. M. and Barnäfoldi, G. and Barret, V. and Bartke, J. and Bartos, D. and Basile, M. and Basmanov, V. and Bastid, N. and Batigne, G. and Batyunya, B. and Baudot, J. and Baumann, C. and Bearden, I. and Becker, B. and Belikov, J. and Bellwied, R. and Belmont-Moreno, E. and Belogianni, A. and Belyaev, S. and Benato, A. and Beney, J. L. and Benhabib, L. and Benotto, F. and Beolé, S. and Berceanu, I. and Bercuci, A. and Berdermann, E. and Berdnikov, Y. and Bernard, C. and Berny, R. and Berst, J. D. and Bertelsen, H. and Betev, L. and Bhasin, A. and Baskar, P. and Bhati, A. and Bianchi, N. and Bielčik, J. and Bielčiková, J. and Bimbot, L. and Blanchard, G. and Blanco, F. and Blanco, F. and Blau, D. and Blume, C. and Blyth, S. and Boccioli, M. and Bogdanov, A. and Bøggild, H. and Bogolyubsky, M. and Boldizsár, L. and Bombara, M. and Bombonati, C. and Bondila, M. and Bonnet, D. and Bonvicini, V. and Borel, H. and Borotto, F. and Borshchov, V. and Bortoli, Y. and Borysov, O. and Bose, S. and Bosisio, L. and Botje, M. and Böttger, S. and Bourdaud, G. and Bourrion, O. and Bouvier, S. and Braem, A. and Braun, M. and Braun-Munzinger, P. and Bravina, L. and Bregant, M. and Bruckner, G. and Brun, R. and Bruna, E. and Brunasso, O. and Bruno, G. E. and Bucher, D. and Budilov, V. and Budnikov, D. and Buesching, H. and Buncic, P. and Burns, M. and Burachas, S. and Busch, O. and Bushop, J. and Cai, X. and Caines, H. and Calaon, F. and Caldogno, M. and Cali, I. and Camerini, P. and Campagnolo, R. and Campbell, M. and Cao, X. and Capitani, G. P. and Romeo, G. Cara and Cardenas-Montes, M. and Carduner, H. and Carena, F. and Carena, W. and Cariola, P. and Carminati, F. and Casado, J. and Diaz, A. Casanova and Caselle, M. and Castellanos, J. Castillo and Castor, J. and Catanescu, V. and Cattaruzza, E. and Cavazza, D. and Cerello, P. and Ceresa, S. and Černý, V. and Chambert, V. and Chapeland, S. and Charpy, A. and Charrier, D. and Chartoire, M. and Charvet, J. L. and Chattopadhyay, S. and Chattopadhyay, S. and Chepurnov, V. and Chernenko, S. and Cherney, M. and Cheshkov, C. and Cheynis, B. and Chochula, P. and Chiavassa, E. and Barroso, V. Chibante and Choi, J. and Christakoglou, P. and Christiansen, P. and Christensen, C. and Chykalov, O. A. and Cicalo, C. and Cifarelli-Strolin, L. and Ciobanu, M. and Cindolo, F. and Cirstoiu, C. and Clausse, O. and Cleymans, J. and Cobanoglu, O. and Coffin, J.-P. and Coli, S. and Colla, A. and Colledani, C. and Combaret, C. and Combet, M. and Comets, M. and Balbastre, G. Conesa and Valle, Z. Conesa del and Contin, G. and Contreras, J. and Cormier, T. and Corsi, F. and Cortese, P. and Costa, F. and Crescio, E. and Crochet, P. and Cuautle, E. and Cussonneau, J. and Dahlinger, M. and Dainese, A. and Dalsgaard, H. H. and Daniel, L. and Das, I. and Das, T. and Dash, A. and Silva, R. Da and Davenport, M. and Daues, H. and Caro, A. De and Cataldo, G. de and Cuveland, J. De and Falco, A. De and Gaspari, M. de and Girolamo, P. de and Groot, J. de and Gruttola, D. De and Haas, A. De and Marco, N. De and Pasquale, S. De and Remigis, P. De and Vaux, D. de and Decock, G. and Delagrange, H. and Franco, M. Del and Dellacasa, G. and Dell{\textbackslash}textquotesingleOlio, C. and Dell{\textbackslash}textquotesingleOlio, D. and Deloff, A. and Demanov, V. and Dénes, E. and D{\textbackslash}textquotesingleErasmo, G. and Derkach, D. and Devaux, A. and Bari, D. Di and Bartelomen, A. Di and Giglio, C. Di and Liberto, S. Di and Mauro, A. Di and Nezza, P. Di and Dialinas, M. and Diaz, L. and Valdes, R. Díaz and Dietel, T. and Dima, R. and Ding, H. and Dinca, C. and Divià, R. and Dobretsov, V. and Dobrin, A. and Doenigus, B. and Dobrowolski, T. and Domínguez, I. and Dorn, M. and Drouet, S. and Dubey, A. E. and Ducroux, L. and Dumitrache, F. and Dumonteil, E. and Dupieux, P. and Duta, V. and Majumdar, A. Dutta and Majumdar, M. Dutta and Dyhre, Th and Efimov, L. and Efremov, A. and Elia, D. and Emschermann, D. and Engster, C. and Enokizono, A. and Espagnon, B. and Estienne, M. and Evangelista, A. and Evans, D. and Evrard, S. and Fabjan, C. W. and Fabris, D. and Faivre, J. and Falchieri, D. and Fantoni, A. and Farano, R. and Fearick, R. and Fedorov, O. and Fekete, V. and Felea, D. and Feofilov, G. and Téllez, A. Férnandez and Ferretti, A. and Fichera, F. and Filchagin, S. and Filoni, E. and Finck, C. and Fini, R. and Fiore, E. M. and Flierl, D. and Floris, M. and Fodor, Z. and Foka, Y. and Fokin, S. and Force, P. and Formenti, F. and Fragiacomo, E. and Fragkiadakis, M. and Fraissard, D. and Franco, A. and Franco, M. and Frankenfeld, U. and Fratino, U. and Fresneau, S. and Frolov, A. and Fuchs, U. and Fujita, J. and Furget, C. and Furini, M. and Girard, M. Fusco and Gaardhøje, J.-J. and Gabrielli, A. and Gadrat, S. and Gagliardi, M. and Gago, A. and Gaido, L. and Torreira, A. Gallas and Gallio, M. and Gandolfi, E. and Ganoti, P. and Ganti, M. and Garabatos, J. and Lopez, A. Garcia and Garizzo, L. and Gaudichet, L. and Gemme, R. and Germain, M. and Gheata, A. and Gheata, M. and Ghidini, B. and Ghosh, P. and Giolu, G. and Giraudo, G. and Giubellino, P. and Glasow, R. and Glässel, P. and Ferreiro, E. G. and Gutierrez, C. Gonzalez and Gonzales-Trueba, L. H. and Gorbunov, S. and Gorbunov, Y. and Gos, H. and Gosset, J. and Gotovac, S. and Gottschlag, H. and Gottschalk, D. and Grabski, V. and Grassi, T. and Gray, H. and Grebenyuk, O. and Grebieszkow, K. and Gregory, C. and Grigoras, C. and Grion, N. and Grigoriev, V. and Grigoryan, A. and Grigoryan, C. and Grigoryan, S. and Grishuk, Y. and Gros, P. and Grosse-Oetringhaus, J. and Grossiord, J.-Y. and Grosso, R. and Grynyov, B. and Guarnaccia, C. and Guber, F. and Guerin, F. and Guernane, R. and Guerzoni, M. and Guichard, A. and Guida, M. and Guilloux, G. and Gulkanyan, H. and Gulbrandsen, K. and Gunji, T. and Gupta, A. and Gupta, V. and Gustafsson, H.-A. and Gutbrod, H. and Hadjidakis, C. and Haiduc, M. and Hamar, G. and Hamagaki, H. and Hamblen, J. and Hansen, J. C. and Hardy, P. and Hatzifotiadou, D. and Harris, J. W. and Hartig, M. and Harutyunyan, A. and Hayrapetyan, A. and Hasch, D. and Hasegan, D. and Hehner, J. and Heine, N. and Heinz, M. and Helstrup, H. and Herghelegiu, A. and Herlant, S. and Corral, G. Herrera and Herrmann, N. and Hetland, K. and Hille, P. and Hinke, H. and Hippolyte, B. and Hoch, M. and Hoebbel, H. and Hoedlmoser, H. and Horaguchi, T. and Horner, M. and Hristov, P. and Hřivnáčová, I. and Hu, S. and Guo, C. Hu and Humanic, T. and Hurtado, A. and Hwang, D. S. and Ianigro, J. C. and Idzik, M. and Igolkin, S. and Ilkaev, R. and Ilkiv, I. and Imhoff, M. and Innocenti, P. G. and Ionescu, E. and Ippolitov, M. and Irfan, M. and Insa, C. and Inuzuka, M. and Ivan, C. and Ivanov, A. and Ivanov, M. and Ivanov, V. and Jacobs, P. and Jacholkowski, A. and Jančurová, L. and Janik, R. and Jasper, M. and Jena, C. and Jirden, L. and Johnson, D. P. and Jones, G. T. and Jorgensen, C. and Jouve, F. and Jovanović, P. and Junique, A. and Jusko, A. and Jung, H. and Jung, W. and Kadija, K. and Kamal, A. and Kamermans, R. and Kapusta, S. and Kaidalov, A. and Kakoyan, V. and Kalcher, S. and Kang, E. and Kapitan, J. and Kaplin, V. and Karadzhev, K. and Karavichev, O. and Karavicheva, T. and Karpechev, E. and Karpio, K. and Kazantsev, A. and Kebschull, U. and Keidel, R. and Khan, M. Mohsin and Khanzadeev, A. and Kharlov, Y. and Kikola, D. and Kileng, B. and Kim, D. and Kim, D. S. and Kim, D. W. and Kim, H. N. and Kim, J. S. and Kim, S. and Kinson, J. B. and Kiprich, S. K. and Kisel, I. and Kiselev, S. and Kisiel, A. and Kiss, T. and Kiworra, V. and Klay, J. and Bösing, C. Klein and Kliemant, M. and Klimov, A. and Klovning, A. and Kluge, A. and Kluit, R. and Kniege, S. and Kolevatov, R. and Kollegger, T. and Kolojvari, A. and Kondratiev, V. and Kornas, E. and Koshurnikov, E. and Kotov, I. and Kour, R. and Kowalski, M. and Kox, S. and Kozlov, K. and Králik, I. and Kramer, F. and Kraus, I. and Kravčáková, A. and Krawutschke, T. and Krivda, M. and Kryshen, E. and Kucheriaev, Y. and Kugler, A. and Kuhn, C. and Kuijer, P. and Kumar, L. and Kumar, N. and Kumpumaeki, P. and Kurepin, A. and Kurepin, A. N. and Kushpil, S. and Kushpil, V. and Kutovsky, M. and Kvaerno, H. and Kweon, M. and Labbé, J.-C. and Lackner, F. and Guevara, P. Ladron de and Lafage, V. and Rocca, P. La and Lamont, M. and Lara, C. and Larsen, D. T. and Laurenti, G. and Lazzeroni, C. and Bornec, Y. Le and Bris, N. Le and Gailliard, C. Le and Lebedev, V. and Lecoq, J. and Lee, K. S. and Lee, S. C. and Lefévre, F. and Legrand, I. and Lehmann, T. and Leistam, L. and Lenoir, P. and Lenti, V. and Leon, H. and Monzon, I. Leon and Lévai, P. and Li, Q. and Li, X. and Librizzi, F. and Lietava, R. and Lindegaard, N. and Lindenstruth, V. and Lippmann, C. and Lisa, M. and Listratenko, O. M. and Littel, F. and Liu, Y. and Lo, J. and Lobanov, V. and Loginov, V. and Noriega, M. López and López-Ramírez, R. and Torres, E. López and Lorenzo, P. M. and Løvhøiden, G. and Lu, S. and Ludolphs, W. and Lunardon, M. and Luquin, L. and Lusso, S. and Lutz, J.-R. and Luvisetto, M. and Lyapin, V. and Maevskaya, A. and Magureanu, C. and Mahajan, A. and Majahan, S. and Mahmoud, T. and Mairani, A. and Mahapatra, D. and Makarov, A. and Makhlyueva, I. and Malek, M. and Malkiewicz, T. and Mal{\textbackslash}textquotesingleKevich, D. and Malzacher, P. and Mamonov, A. and Manea, C. and Mangotra, L. K. and Maniero, D. and Manko, V. and Manso, F. and Manzari, V. and Mao, Y. and Marcel, A. and Marchini, S. and Mareš, J. and Margagliotti, G. V. and Margotti, A. and Marin, A. and Marin, J.-C. and Marras, D. and Martinengo, P. and Martínez, M. I. and Martinez-Davalos, A. and Garcia, G. Martínez and Martini, S. and Chiesa, A. Marzari and Marzocca, C. and Masciocchi, S. and Masera, M. and Masetti, M. and Maslov, N. I. and Masoni, A. and Massera, F. and Mast, M. and Mastroserio, A. and Matthews, Z. L. and Mayer, B. and Mazza, G. and Mazzaro, M. D. and Mazzoni, A. and Meddi, F. and Meleshko, E. and Menchaca-Rocha, A. and Meneghini, S. and Meoni, M. and Perez, J. Mercado and Mereu, P. and Meunier, O. and Miake, Y. and Michalon, A. and Michinelli, R. and Miftakhov, N. and Mignone, M. and Mikhailov, K. and Milosevic, J. and Minaev, Y. and Minafra, F. and Mischke, A. and Miśkowiec, D. and Mitsyn, V. and Mitu, C. and Mohanty, B. and Moisa, D. and Molnar, L. and Mondal, M. and Mondal, N. and Zetina, L. Montaño and Monteno, M. and Morando, M. and Morel, M. and Moretto, S. and Morhardt, Th and Morsch, A. and Moukhanova, T. and Mucchi, M. and Muccifora, V. and Mudnic, E. and Müller, H. and Müller, W. and Munoz, J. and Mura, D. and Musa, L. and Muraz, J. F. and Musso, A. and Nania, R. and Nandi, B. and Nappi, E. and Navach, F. and Navin, S. and Nayak, T. and Nazarenko, S. and Nazarov, G. and Nellen, L. and Nendaz, F. and Nianine, A. and Nicassio, M. and Nielsen, B. S. and Nikolaev, S. and Nikolic, V. and Nikulin, S. and Nikulin, V. and Nilsen, B. and Nitti, M. and Noferini, F. and Nomokonov, P. and Nooren, G. and Noto, F. and Nouais, D. and Nyiri, A. and Nystrand, J. and Odyniec, G. and Oeschler, H. and Oinonen, M. and Oldenburg, M. and Oleks, I. and Olsen, E. K. and Onuchin, V. and Oppedisano, C. and Orsini, F. and Ortiz-Velázquez, A. and Oskamp, C. and Oskarsson, A. and Osmic, F. and Österman, L. and Otterlund, I. and Ovrebekk, G. and Oyama, K. and Pachr, M. and Pagano, P. and Paić, G. and Pajares, C. and Pal, S. and Pal, S. and Pálla, G. and Palmeri, A. and Pancaldi, G. and Panse, R. and Pantaleo, A. and Pappalardo, G. S. and Pastirčák, B. and Pastore, C. and Patarakin, O. and Paticchio, V. and Patimo, G. and Pavlinov, A. and Pawlak, T. and Peitzmann, T. and Pénichot, Y. and Pepato, A. and Pereira, H. and Peresunko, D. and Perez, C. and Griffo, J. Perez and Perini, D. and Perrino, D. and Peryt, W. and Pesci, A. and Peskov, V. and Pestov, Y. and Peters, A. J. and Petráček, V. and Petridis, A. and Petris, M. and Petrov, V. and Petrov, V. and Petrovici, M. and Peyré, J. and Piano, S. and Piccotti, A. and Pichot, P. and Piemonte, C. and Pikna, M. and Pilastrini, R. and Pillot, P. and Pinazza, O. and Pini, B. and Pinsky, L. and Morais, V. Pinto and Pismennaya, V. and Piuz, F. and Platt, R. and Ploskon, M. and Plumeri, S. and Pluta, J. and Pocheptsov, T. and Podesta, P. and Poggio, F. and Poghosyan, M. and Poghosyan, T. and Polák, K. and Polichtchouk, B. and Polozov, P. and Polyakov, V. and Pommeresch, B. and Pompei, F. and Pop, A. and Popescu, S. and Posa, F. and Pospíšil, V. and Potukuchi, B. and Pouthas, J. and Prasad, S. and Preghenella, R. and Prino, F. and Prodan, L. and Prono, G. and Protsenko, M. A. and Pruneau, C. A. and Przybyla, A. and Pshenichnov, I. and Puddu, G. and Pujahari, P. and Pulvirenti, A. and Punin, A. and Punin, V. and Putschke, J. and Quartieri, J. and Quercigh, E. and Rachevskaya, I. and Rachevski, A. and Rademakers, A. and Radomski, S. and Radu, A. and Rak, J. and Ramello, L. and Raniwala, R. and Raniwala, S. and Rasmussen, O. B. and Rasson, J. and Razin, V. and Read, K. and Real, J. and Redlich, K. and Reichling, C. and Renard, C. and Renault, G. and Renfordt, R. and Reolon, A. R. and Reshetin, A. and Revol, J.-P. and Reygers, K. and Ricaud, H. and Riccati, L. and Ricci, R. A. and Richter, M. and Riedler, P. and Rigalleau, L. M. and Riggi, F. and Riegler, W. and Rindel, E. and Riso, J. and Rivetti, A. and Rizzi, M. and Rizzi, V. and Cahuantzi, M. Rodriguez and Røed, K. and Röhrich, D. and Román-López, S. and Romanato, M. and Romita, R. and Ronchetti, F. and Rosinsky, P. and Rosnet, P. and Rossegger, S. and Rossi, A. and Rostchin, V. and Rotondo, F. and Roukoutakis, F. and Rousseau, S. and Roy, C. and Roy, D. and Roy, P. and Royer, L. and Rubin, G. and Rubio, A. and Rui, R. and Rusanov, I. and Russo, G. and Ruuskanen, V. and Ryabinkin, E. and Rybicki, A. and Sadovsky, S. and Šafařík, K. and Sahoo, R. and Saini, J. and Saiz, P. and Salur, S. and Sambyal, S. and Samsonov, V. and Šándor, L. and Sandoval, A. and Sann, H. and Santiard, J.-C. and Santo, R. and Santoro, R. and Sargsyan, G. and Saturnini, P. and Scapparone, E. and Scarlassara, F. and Schackert, B. and Schiaua, C. and Schicker, R. and Schioler, T. and Schippers, J. D. and Schmidt, C. and Schmidt, H. and Schneider, R. and Schossmaier, K. and Schukraft, J. and Schutz, Y. and Schwarz, K. and Schweda, K. and Schyns, E. and Scioli, G. and Scomparin, E. and Snow, H. and Sedykh, S. and Segato, G. and Sellitto, S. and Semeria, F. and Senyukov, S. and Seppänen, H. and Serci, S. and Serkin, L. and Serra, S. and Sesselmann, T. and Sevcenco, A. and Sgura, I. and Shabratova, G. and Shahoyan, R. and Sharkov, E. and Sharma, S. and Shigaki, K. and Shileev, K. and Shukla, P. and Shurygin, A. and Shurygina, M. and Sibiriak, Y. and Siddi, E. and Siemiarczuk, T. and Sigward, M. H. and Silenzi, A. and Silvermyr, D. and Silvestri, R. and Simili, E. and Simion, V. and Simon, R. and Simonetti, L. and Singaraju, R. and Singhal, V. and Sinha, B. and Sinha, T. and Siska, M. and Sitár, B. and Sitta, M. and Skaali, B. and Skowronski, P. and Slodkowski, M. and Smirnov, N. and Smykov, L. and Snellings, R. and Snoeys, W. and Soegaard, C. and Soerensen, J. and Sokolov, O. and Soldatov, A. and Soloviev, A. and Soltveit, H. and Soltz, R. and Sommer, W. and Soos, C. and Soramel, F. and Sorensen, S. and Soyk, D. and Spyropoulou-Stassinaki, M. and Stachel, J. and Staley, F. and Stan, I. and Stavinskiy, A. and Steckert, J. and Stefanini, G. and Stefanek, G. and Steinbeck, T. and Stelzer, H. and Stenlund, E. and Stocco, D. and Stockmeier, M. and Stoicea, G. and Stolpovsky, P. and Strmeň, P. and Stutzmann, J. S. and Su, G. and Sugitate, T. and Šumbera, M. and Suire, C. and Susa, T. and Kumar, K. Sushil and Swoboda, D. and Symons, J. and Szarka, I. and Szostak, A. and Szuba, M. and Szymanski, P. and Tadel, M. and Tagridis, C. and Tan, L. and Takaki, D. Tapia and Taureg, H. and Tauro, A. and Tavlet, M. and Munoz, G. Tejeda and Thäder, J. and Tieulent, R. and Timmer, P. and Tolyhy, T. and Topilskaya, N. and Matos, C. Torcato de and Torii, H. and Toscano, L. and Tosello, F. and Tournaire, A. and Traczyk, T. and Tröger, G. and Tromeur, W. and Truesdale, D. and Trzaska, W. and Tsiledakis, G. and Tsilis, E. and Tsvetkov, A. and Turcato, M. and Turrisi, R. and Tuveri, M. and Tveter, T. and Tydesjo, H. and Tykarski, L. and Tywoniuk, K. and Ugolini, E. and Ullaland, K. and Urbán, J. and Urciuoli, G. M. and Usai, G. L. and Usseglio, M. and Vacchi, A. and Vala, M. and Valiev, F. and Vyvre, P. Vande and Brink, A. Van Den and Eijndhoven, N. Van and Kolk, N. Van Der and Leeuwen, M. van and Vannucci, L. and Vanzetto, S. and Vanuxem, J.-P. and Vargas, M. A. and Varma, R. and Vascotto, A. and Vasiliev, A. and Vassiliou, M. and Vasta, P. and Vechernin, V. and Venaruzzo, M. and Vercellin, E. and Vergara, S. and Verhoeven, W. and Veronese, F. and Vetlitskiy, I. and Vernet, R. and Victorov, V. and Vidak, L. and Viesti, G. and Vikhlyantsev, O. and Vilakazi, Z. and Baillie, O. Villalobos and Vinogradov, A. and Vinogradov, L. and Vinogradov, Y. and Virgili, T. and Viyogi, Y. and Vodopianov, A. and Volpe, G. and Vranic, D. and Vrláková, J. and Vulpescu, B. and Wabnitz, C. and Wagner, V. and Wallet, L. and Wan, R. and Wang, Y. and Wang, Y. and Wheadon, R. and Weis, R. and Wen, Q. and Wessels, J. and Westergaard, J. and Wiechula, J. and Wiesenaecker, A. and Wikne, J. and Wilk, A. and Wilk, G. and Williams, C. and Willis, N. and Windelband, B. and Witt, R. and Woehri, H. and Wyllie, K. and Xu, C. and Yang, C. and Yang, H. and Yermia, F. and Yin, Z. and Yin, Z. and Ky, B. Yun and Yushmanov, I. and Yuting, B. and Zabrodin, E. and Zagato, S. and Zagreev, B. and Zaharia, P. and Zalite, A. and Zampa, G. and Zampolli, C. and Zanevskiy, Y. and Zarochentsev, A. and Zaudtke, O. and Závada, P. and Zbroszczyk, H. and Zepeda, A. and Zeter, V. and Zgura, I. and Zhalov, M. and Zhou, D. and Zhou, S. and Zhu, G. and Zichichi, A. and Zinchenko, A. and Zinovjev, G. and Zoccarato, Y. and Zubarev, A. and Zucchini, A. and Zuffa, M.},
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. T. and Blau, D. and Blume, C. and Boca, G. and Bock, F. and Bogdanov, A. and Boldizsár, L. and Bombara, M. and Bonomi, G. and Bonora, M. and Borel, H. and Borissov, A. and Borri, M. and Botta, E. and Bourjau, C. and Bratrud, L. and Braun-Munzinger, P. and Bregant, M. and Broker, 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 Buhler, P. and Buncic, P. and Busch, O. and Buthelezi, Z. and Butt, J. B. and Buxton, J. T. and Cabala, J. and Caffarri, D. and Caines, H. and Caliva, A. and Calvo Villar, E. and Camacho, R. S. and Camerini, P. and Capon, A. A. 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 Chandra, S. and Chang, B. and Chang, W. and Chapeland, S. and Chartier, M. and Chattopadhyay, S. and Chattopadhyay, S. and Chauvin, A. and Cheshkov, C. and Cheynis, B. and Chibante Barroso, V. and Chinellato, D. D. and Cho, S. and Chochula, P. and Chowdhury, T. 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 Concas, M. and Conesa Balbastre, G. and Conesa del Valle, Z. and Contreras, J. G. and Cormier, T. M. and Corrales Morales, Y. and Cortese, P. and Cosentino, M. R. and Costa, F. and Costanza, S. and Crkovská, J. and Crochet, P. and Cuautle, E. and Cunqueiro, L. and Dahms, T. and Dainese, A. and Damas, F. P. A. and Dani, S. 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 De Souza, R. D. and Degenhardt, H. F. and Deisting, A. and Deloff, A. and Delsanto, S. and Deplano, C. and Dhankher, P. and Di Bari, D. and Di Mauro, A. and Di Ruzza, B. and Diaz, R. A. and Dietel, T. and Dillenseger, P. and Ding, Y. and Divià, R. and Djuvsland, Ø. and Dobrin, A. and Domenicis Gimenez, D. and Dönigus, B. and Dordic, O. and Doremalen, L. V. R. and Dubey, A. K. and Dubla, A. and Ducroux, L. and Dudi, S. and Duggal, A. K. and Dukhishyam, M. and Dupieux, P. and Ehlers, R. J. and Elia, D. and Endress, E. and Engel, H. and Epple, E. and Erazmus, B. and Erhardt, F. and Ersdal, M. R. and Espagnon, B. and Eulisse, G. and Eum, J. and Evans, D. and Evdokimov, S. and Fabbietti, L. and Faggin, M. and Faivre, J. and Fantoni, A. and Fasel, M. and Feldkamp, L. and Feliciello, A. and Feofilov, G. and Fernández Téllez, A. 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 Fiorenza, G. and Flor, F. and Floris, M. and Foertsch, S. and Foka, P. and Fokin, S. and Fragiacomo, E. and Francescon, A. and Francisco, 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 Gajdosova, K. and Gallio, M. and Galvan, C. D. and Ganoti, P. and Garabatos, C. and Garcia-Solis, E. and Garg, K. and Gargiulo, C. and Gasik, P. and Gauger, E. F. and Gay Ducati, M. B. and Germain, M. and Ghosh, J. and Ghosh, P. and Ghosh, S. K. and Gianotti, P. and Giubellino, P. and Giubilato, P. and Glässel, P. and Goméz Coral, D. M. and Gomez Ramirez, A. and Gonzalez, V. and González-Zamora, P. and Gorbunov, S. and Görlich, L. and Gotovac, S. and Grabski, V. and Graczykowski, L. K. and Graham, K. L. and Greiner, L. and Grelli, A. and Grigoras, C. and Grigoriev, V. and Grigoryan, A. and Grigoryan, S. and Gronefeld, J. M. and Grosa, F. and Grosse-Oetringhaus, J. F. and Grosso, R. and Guernane, R. and Guerzoni, B. and Guittiere, M. and Gulbrandsen, K. and Gunji, T. and Gupta, A. and Gupta, R. and Guzman, I. B. and Haake, R. and Habib, M. K. and Hadjidakis, C. and Hamagaki, H. and Hamar, G. and Hamid, M. and Hamon, J. C. and Hannigan, R. and Haque, M. R. and Harlenderova, A. and Harris, J. W. and Harton, A. and Hassan, H. and Hatzifotiadou, D. and Hayashi, S. and Heckel, S. T. and Hellbär, E. and Helstrup, H. and Herghelegiu, A. and Hernandez, E. G. and Herrera Corral, G. and Herrmann, F. and Hetland, K. F. and Hilden, T. E. and Hillemanns, H. and Hills, C. and Hippolyte, B. and Hohlweger, B. and Horak, D. and Hornung, S. and Hosokawa, R. and Hota, J. and Hristov, P. and Huang, C. and Hughes, C. and Huhn, P. and Humanic, T. J. and Hushnud, H. and Hussain, N. and Hussain, T. and Hutter, D. and Hwang, D. S. and Iddon, J. P. and Iga Buitron, S. A. and Ilkaev, R. and Inaba, M. and Ippolitov, M. and Islam, M. S. and Ivanov, M. and Ivanov, V. and Izucheev, V. and Jacak, B. and Jacazio, N. and Jacobs, P. M. and Jadhav, M. B. and Jadlovska, S. and Jadlovsky, J. and Jaelani, S. and Jahnke, C. and Jakubowska, M. J. and Janik, M. A. and Jena, C. and Jercic, M. and Jevons, O. and Jimenez Bustamante, R. T. and Jin, M. and Jones, P. G. and Jusko, A. and Kalinak, P. and Kalweit, A. and Kang, J. H. and Kaplin, V. and Kar, S. and Karasu Uysal, A. and Karavichev, O. and Karavicheva, T. and Karczmarczyk, P. and Karpechev, E. and Kebschull, U. and Keidel, R. and Keijdener, D. L. D. and Keil, M. and Ketzer, B. and Khabanova, Z. and Khan, A. M. and Khan, S. and Khan, S. A. and Khanzadeev, A. and Kharlov, Y. and Khatun, A. and Khuntia, A. and Kielbowicz, M. M. and Kileng, B. and Kim, B. and Kim, D. and Kim, D. J. and Kim, E. J. and Kim, H. and Kim, J. S. and Kim, J. and Kim, M. and Kim, S. and Kim, T. and Kim, T. and Kirsch, S. and Kisel, I. and Kiselev, S. and Kisiel, A. and Klay, J. L. and Klein, C. and Klein, J. and Klein-Bösing, C. and Klewin, S. and Kluge, A. and Knichel, M. L. and Knospe, A. G. and Kobdaj, C. and Kofarago, M. and Köhler, M. K. and Kollegger, T. and Kondratyeva, N. and Kondratyuk, E. and Konevskikh, A. and Konopka, P. J. and Konyushikhin, M. and Koska, L. and Kovalenko, O. and Kovalenko, V. and Kowalski, M. and Králik, I. and Kravčáková, A. and Kreis, L. and Krivda, M. and Krizek, F. and Krüger, M. and Kryshen, E. and Krzewicki, M. and Kubera, A. M. and Kučera, V. and Kuhn, C. and Kuijer, P. G. and Kumar, J. and Kumar, L. and Kumar, S. and Kundu, S. and Kurashvili, P. and Kurepin, A. and Kurepin, A. B. and Kuryakin, A. and Kushpil, S. and Kvapil, J. and Kweon, M. J. and Kwon, Y. and La Pointe, S. L. and La Rocca, P. and Lai, Y. S. and Lakomov, I. and Langoy, R. and Lapidus, K. and Lardeux, A. and Larionov, P. and Laudi, E. and Lavicka, R. and Lea, R. and Leardini, L. and Lee, S. and Lehas, F. and Lehner, S. and Lehrbach, J. and Lemmon, R. C. and León Monzón, I. and Lévai, P. and Li, X. and Li, X. L. and Lien, J. and Lietava, R. and Lim, B. and Lindal, S. and Lindenstruth, V. and Lindsay, S. W. and Lippmann, C. and Lisa, M. A. and Litichevskyi, V. and Liu, A. and Ljunggren, H. M. and Llope, W. J. and Lodato, D. F. and Loginov, V. and Loizides, C. and Loncar, P. and Lopez, X. and López Torres, E. and Lowe, A. and Luettig, P. and Luhder, J. R. and Lunardon, M. and Luparello, G. and Lupi, M. and Maevskaya, A. and Mager, M. and Mahmood, S. M. and Maire, A. and Majka, R. D. and Malaev, M. and Malik, Q. W. and Malinina, L. and Mal'Kevich, D. and Malzacher, P. and Mamonov, A. and Manko, V. and Manso, F. and Manzari, V. and Mao, Y. and Marchisone, M. and Mareš, J. and Margagliotti, G. V. and Margotti, A. and Margutti, J. and Marín, A. and Markert, C. and Marquard, M. and Martin, N. A. and Martinengo, P. and Martinez, J. L. and Martínez, M. I. and Martínez García, G. and Martinez Pedreira, M. and Masciocchi, S. and Masera, M. and Masoni, A. and Massacrier, L. and Masson, E. and Mastroserio, A. and Mathis, A. M. and Matuoka, P. F. T. and Matyja, A. and Mayer, C. and Mazzilli, M. and Mazzoni, M. A. and Meddi, F. and Melikyan, Y. and Menchaca-Rocha, A. and Meninno, E. and Mercado Pérez, J. and Meres, M. and Mhlanga, S. and Miake, Y. and Micheletti, L. and Mieskolainen, M. M. and Mihaylov, D. L. and Mikhaylov, K. and Mischke, A. and Mishra, A. N. and Miśkowiec, D. and Mitra, J. and Mitu, C. M. and Mohammadi, N. and Mohanty, A. P. and Mohanty, B. and Mohisin Khan, M. and Moreira De Godoy, D. A. and Moreno, L. A. P. and Moretto, S. and Morreale, A. and Morsch, A. and Mrnjavac, T. and Muccifora, V. and Mudnic, E. and Mühlheim, D. and Muhuri, S. and Mukherjee, M. and Mulligan, J. D. and Munhoz, M. G. and Münning, K. and Munoz, M. I. A. and Munzer, R. H. and Murakami, H. and Murray, S. and Musa, L. and Musinsky, J. and Myers, C. J. and Myrcha, J. W. and Naik, B. and Nair, R. and Nandi, B. K. and Nania, R. and Nappi, E. and Narayan, A. and Naru, M. U. and Nassirpour, A. F. and Natal da Luz, H. and Nattrass, C. and Navarro, S. R. and Nayak, K. and Nayak, R. and Nayak, T. K. and Nazarenko, S. and Negrao De Oliveira, R. A. and Nellen, L. and Nesbo, S. V. and Neskovic, G. and Ng, F. and Nicassio, M. and Niedziela, J. and Nielsen, B. S. and Nikolaev, S. and Nikulin, S. and Nikulin, V. and Noferini, F. and Nomokonov, P. and Nooren, G. and Noris, J. C. C. and Norman, J. and Nyanin, A. and Nystrand, J. and Oh, H. and Ohlson, A. and Oleniacz, J. and Oliveira Da Silva, A. C. and Oliver, M. H. and Onderwaater, J. and Oppedisano, C. and Orava, R. and Oravec, M. and Ortiz Velasquez, A. and Oskarsson, A. and Otwinowski, J. and Oyama, K. and Pachmayer, Y. and Pacik, V. and Pagano, D. and Paić, G. and Palni, P. and Pan, J. and Pandey, A. K. and Panebianco, S. and Papikyan, V. and Pareek, P. and Park, J. and Parkkila, J. E. and Parmar, S. and Passfeld, A. and Pathak, S. P. and Patra, R. N. and Paul, B. and Pei, H. and Peitzmann, T. and Peng, X. and Pereira, L. G. and Pereira Da Costa, H. and Peresunko, D. and Perez Lezama, E. and Peskov, V. and Pestov, Y. and Petráček, V. and Petrovici, M. and Petta, C. and Pezzi, R. P. and Piano, S. and Pikna, M. and Pillot, P. and Pimentel, L. O. D. L. and Pinazza, O. and Pinsky, L. and Pisano, S. and Piyarathna, D. B. and Płoskoń, M. and Planinic, M. and Pliquett, F. and Pluta, J. and Pochybova, S. and Podesta-Lerma, P. L. M. and Poghosyan, M. G. and Polichtchouk, B. and Poljak, N. and Poonsawat, W. and Pop, A. and Poppenborg, H. and Porteboeuf-Houssais, S. and Pozdniakov, V. and Prasad, S. K. and Preghenella, R. and Prino, F. and Pruneau, C. A. and Pshenichnov, I. and Puccio, M. and Punin, V. and Putschke, J. and Raha, S. and Rajput, S. and Rak, J. and Rakotozafindrabe, A. and Ramello, L. and Rami, F. and Raniwala, R. and Raniwala, S. and Räsänen, S. S. and Rascanu, B. T. and Rath, R. and Ratza, V. and Ravasenga, I. and Read, K. F. and Redlich, K. and Rehman, A. and Reichelt, P. and Reidt, F. and Ren, X. and Renfordt, R. and Reshetin, A. and Revol, J.-P. and Reygers, K. and Riabov, V. and Richert, T. and Richter, M. and Riedler, P. and Riegler, W. and Riggi, F. and Ristea, C. and Rode, S. P. and Rodríguez Cahuantzi, M. and Røed, K. and Rogalev, R. and Rogochaya, E. and Rohr, D. and Röhrich, D. and Rokita, P. S. and Ronchetti, F. and Rosas, E. D. and Roslon, K. and Rosnet, P. and Rossi, A. and Rotondi, A. and Roukoutakis, F. and Roy, C. and Roy, P. and Rueda, O. V. and Rui, R. and Rumyantsev, B. and Rustamov, A. and Ryabinkin, E. and Ryabov, Y. and Rybicki, A. and Saarinen, S. and Sadhu, S. and Sadovsky, S. and Šafařík, K. and Saha, S. K. and Sahoo, B. and Sahoo, P. and Sahoo, R. and Sahoo, S. and Sahu, P. K. and Saini, J. and Sakai, S. and Saleh, M. A. and Sambyal, S. and Samsonov, V. and Sandoval, A. and Sarkar, A. and Sarkar, D. and Sarkar, N. and Sarma, P. and Sas, M. H. P. and Scapparone, E. and Scarlassara, F. and Schaefer, B. and Scheid, H. S. and Schiaua, C. and Schicker, R. and Schmidt, C. and Schmidt, H. R. and Schmidt, M. O. and Schmidt, M. and Schmidt, N. V. and Schukraft, J. and Schutz, Y. and Schwarz, K. and Schweda, K. and Scioli, G. and Scomparin, E. and Šefčík, M. and Seger, J. E. and Sekiguchi, Y. and Sekihata, D. and Selyuzhenkov, I. and Senyukov, S. and Serradilla, E. and Sett, P. and Sevcenco, A. and Shabanov, A. and Shabetai, A. and Shahoyan, R. and Shaikh, W. and Shangaraev, A. and Sharma, A. and Sharma, A. and Sharma, M. and Sharma, N. and Sheikh, A. I. and Shigaki, K. and Shimomura, M. and Shirinkin, S. and Shou, Q. and Shtejer, K. and Sibiriak, Y. and Siddhanta, S. and Sielewicz, K. 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. G. and Tauro, A. and Tejeda Muñoz, G. and Telesca, A. and Terrevoli, C. and Teyssier, B. and Thakur, D. and Thakur, S. and Thomas, D. and Thoresen, F. and Tieulent, R. and Tikhonov, A. and Timmins, A. R. and Toia, A. and Topilskaya, N. and Toppi, M. and Torales-Acosta, F. and Torres, S. R. and Tripathy, S. and Trogolo, S. and Trombetta, G. and Tropp, L. and Trubnikov, V. and Trzaska, W. H. and Trzcinski, T. P. and Trzeciak, B. A. and Tsuji, T. and Tumkin, A. and Turrisi, R. and Tveter, T. S. and Ullaland, K. and Umaka, E. N. and Uras, A. and Usai, G. L. and Utrobicic, A. and Vala, M. and Van Hoorne, J. W. and van Leeuwen, M. and Vande Vyvre, P. and Varga, D. and Vargas, A. and Vargyas, M. and Varma, R. and Vasileiou, M. and Vasiliev, A. and Vauthier, A. and Vázquez Doce, O. and Vechernin, V. and Veen, A. M. and Vercellin, E. and Vergara Limón, S. and Vermunt, L. and Vernet, R. and Vértesi, R. and Vickovic, L. and Viinikainen, J. and Vilakazi, Z. and Villalobos Baillie, O. and Villatoro Tello, A. and Vinogradov, A. and Virgili, T. and Vislavicius, V. and Vodopyanov, A. and Völkl, M. A. and Voloshin, K. and Voloshin, S. A. and Volpe, G. and von Haller, B. and Vorobyev, I. and Voscek, D. and Vranic, D. and Vrláková, J. and Wagner, B. and Wang, H. and Wang, M. and Watanabe, Y. and Weber, M. and Weber, S. G. and Wegrzynek, A. and Weiser, D. F. and Wenzel, S. C. and Wessels, J. P. and Westerhoff, U. and Whitehead, A. M. and Wiechula, J. and Wikne, J. and Wilk, G. and Wilkinson, J. and Willems, G. A. and Williams, M. C. S. and Willsher, E. and Windelband, B. and Witt, W. E. and Xu, R. and Yalcin, S. and Yamakawa, K. and Yano, S. and Yin, Z. and Yokoyama, H. and Yoo, I.-K. and Yoon, J. H. and Yurchenko, V. and Zaccolo, V. and Zaman, A. and Zampolli, C. and Zanoli, H. J. 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},
}