Jet fragmentation transverse momentum measurements from di-hadron correlations in s = 7 $$ \sqrt{\mathrm{s}}=7 $$ TeV pp and s N N = 5.02 $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$ TeV p–Pb collisions
2019
- Shreyasi Acharya
- Fernando Torales Acosta
- Dagmar Adamová
- Souvik Priyam Adhya
- Alexander Adler
- Jonatan Adolfsson
- Madan Mohan Aggarwal
- G. Aglieri Rinella
- Michelangelo Agnello
- Zubayer Ahammed
- S. Ahmad
- Sang Un Ahn
- Salvatore Aiola
- Alexander Akindinov
- Mohammed Al-Turany
- Sk Noor Alam
- Dsd Albuquerque
- Dimitry Aleksandrov
- B. Alessandro
- Haidar Mas'ud Alfanda
- R Alfaro-Molina
- Yasir Ali
- Andrea Alici
- Anton Alkin
- Johan Alme
- Torsten Alt
- Lucas Altenkamper
- Igor Altsybeev
- Mustafa Naji Anaam
- Cristian Andrei
- Dimitra Andreou
- Harry Arthur Andrews
- Anton Andronic
- Massimo Angeletti
- Venelin Anguelov
- Christopher Daniel Anson
- Tome Anticic
- F. Antinori
- Pietro Antonioli
- Rafay Anwar
- Nicole Apadula
- Laurent Bernard Aphecetche
- H. Appelshäuser
- Silvia Arcelli
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- Mesut Arslandok
- Andre Augustinus
- Ralf Peter Averbeck
- Mohd Danish Azmi
- A. Badalá
- Yong Wook Baek
- Yong Wook Baek
- Stefano Bagnasco
- Raphaelle Marie Bailhache
- Renu Bala
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- Markus Ball
- Rama Chandra Baral
- Roberto Barbera
- Luca Barioglio
- G. G. Barnaföldi
- Lee Stuart Barnby
- Valerie Ramillien Barret
- Paolo Bartalini
- Klaus Barth
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- N. Bastid
- Sumit Basu
- Guillaume Batigne
- Boris Batyunya
- Paul Christoph Batzing
- Dibakar Bauri
- J.L. Bazo Alba
- I. G. Bearden
- Hans Beck
- Cristina Bedda
- Nirbhay Kumar Behera
- Iouri Belikov
- Francesca Bellini
- H. Bello Martinez
- Rene Bellwied
- Lucina Gabriela Espinoza Beltran
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- D. Berenyi
- Redmer Alexander Bertens
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- Anju Bhasin
- Inayat Rasool Bhat
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- C. Blume
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- Laszlo Boldizsar
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- M Bombara
- Germano Bonomi
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- Alexander Borissov
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- Rabi Soto Camacho
- Paolo Camerini
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- Ester Anna Rita Casula
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- Megan Elizabeth Connors
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- Benedikt Volkel
- Martin Andreas Volkl
- Kirill Voloshin
- S. A. Voloshin
- G. Volpe
- B. von Haller
- Ivan Vorobyev
- Dominik Voscek
- Janka Vrlakova
- Boris Wagner
- Mengliang Wang
- Yosuke Watanabe
- M Weber
- Steffen Georg Weber
- Adam Wegrzynek
- Dennis Franz Weiser
- Sandro Christian Wenzel
- J.P. Wessels
- Uwe Westerhoff
- Andile Mothegi Whitehead
- Eberhard Widmann
- Jens Wiechula
- Jon Wikne
- Grzegorz Andrzej Wilk
- Jeremy John Wilkinson
- Guido Alexander Willems
- Emily Willsher
- Bernd Stefan Windelband
- William Edward Witt
- Yitao Wu
- Rong Xu
- Serpil Yalcin
- Kosei Yamakawa
- Satoshi Yano
- Z. Yin
- Hiroki Yokoyama
- Hiroki Yokoyama
- I. K. Yoo
- Jin Hee Yoon
- Shiming Yuan
- Volodymyr Yurchenko
- Valentina Zaccolo
- Ali Zaman
- Chiara Zampolli
- H. J. C. Zanoli
- Nima Zardoshti
- Nima Zardoshti
- Andrey Zarochentsev
- Petr Závada
- N. Zaviyalov
- Hanna Paulina Zbroszczyk
- Mikhail Zhalov
- Xueyao Zhang
- Yinhong Zhang
- Z. H. Zhang
- Z. H. Zhang
- Chengxin Zhao
- Vladimir Zherebchevskii
- Natalia Zhigareva
- Dai-Mei Zhou
- You Zhou
- Zhuo Zhou
- Hongsheng Zhu
- J. Zhu
- Ya Zhu
- Antonino Zichichi
- Markus Bernhard Zimmermann
- Gennady Zinovjev
- Nicola Zurlo
The transverse structure of jets was studied via jet fragmentation transverse momentum (jT) distributions, obtained using two-particle correlations in proton-proton and proton-lead collisions, measured with the ALICE experiment at the LHC. The highest transverse momentum particle in each event is used as the trigger particle and the region 3 < pTt < 15GeV/c is explored in this study. The measured distributions show a clear narrow Gaussian component and a wide non-Gaussian one. Based on Pythia simulations, the narrow component can be related to non-perturbative hadronization and the wide component to quantum chromodynamical splitting. The width of the narrow component shows a weak dependence on the transverse momentum of the trigger particle, in agreement with the expectation of universality of the hadronization process. On the other hand, the width of the wide component shows a rising trend suggesting increased branching for higher transverse momentum. The results obtained in pp collisions at $$ \sqrt{s}=7 $$
TeV and in p–Pb collisions at $$ \sqrt{s_{\mathrm{NN}}}=5.02 $$
TeV are compatible within uncertainties and hence no significant cold nuclear matter effects are observed. The results are compared to previous measurements from CCOR and PHENIX as well as to Pythia 8 and Herwig 7 simulations.
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