189 research outputs found
Atletas tenistas adolescentes de alto rendimento: Perfil de consumo e composição corporal
- Author
- Publication venue
- IBPEFEX
- Publication date
- 17/07/2021
- Field of study
Tennis is an intermittent sport, with movements of high intensity and duration. The present study aimed to assess nutritional status focusing on food intake and body composition of high-performance adolescent athletes. Observational, cross-sectional study with a quantitative approach conducted with 9 athletes from a tennis school in Campo Grande-MS, of both sexes, aged between 10 and 15 years. Dietary research of specific food frequency for athletes was used, comparing with the nutritional recommendations of the International Society for Sports Nutrition for energy and macronutrients and the Institute of Medicine for micronutrients. Anthropometric measurements of weight, height, arm and waist circumferences and skinfolds were performed to determine body fat (%) and fat-free mass (kg). Regarding adequacy, we observed 77.8% of energy intake, in relation to the recommendations, mean intake of carbohydrates of 6.9 g/kg/day, 2.0 g /kg/day of protein and 1.9 g/kg/day of lipids. Calcium intake was below recommendation in 100% of cases. Mean intake above the recommendation was found for zinc, vitamin E and C. Adequate body fat was observed in only 33.3% of tennis players. We concluded that the majority of athletes presented inadequate intake of proteins and micronutrients, which may be reflected in their body composition.O tênis é um esporte intermitente, com movimentos de alta intensidade e curta duração. O presente estudo objetivou avaliar o estado nutricional focado no consumo alimentar e composição corporal de atletas adolescentes de alto rendimento. Estudo observacional, transversal, com abordagem quantitativa realizado com 9 atletas de uma escola de tênis de Campo Grande-MS, de ambos os sexos, com idades entre 10 e 15 anos. Utilizou-se inquérito dietético de frequência alimentar especÃfico para atletas, comparando-se com as recomendações nutricionais da International Society of Sports Nutrition de energia e macronutrientes e do Institute of Medicine para micronutrientes. As medidas antropométricas de peso, estatura, circunferências de braço e cintura e dobras cutâneas foram realizadas para a determinação da gordura corporal (%) e da massa livre de gordura (kg). Observou-se consumo energético com 77,8% de adequação em relação as recomendações, carboidratos de 6,9 g/kg/dia, proteÃna de 2,0 g/kg/dia e lipÃdios de 1,9 g/kg/dia. A ingestão de cálcio estava abaixo da recomendação em 100% dos casos. A média de ingestão de zinco, vitamina E e C apresentaram inadequações estando superiores à s recomendações. O percentual de gordura corporal estava adequado em apenas 33,3% dos tenistas. A maioria dos atletas apresentaram ingestão inadequada de proteÃnas e micronutrientes, que pode estar refletindo na composição corporal
Production of He-4 and (4) in Pb-Pb collisions at root(NN)-N-S=2.76 TeV at the LHC
- Author
- Acharya Shreyasi
- Adamova Dagmar
- Adolfsson Jonatan
- Aggarwal Madan Mohan
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahn Sang Un
- Aiola Salvatore
- Akindinov Alexander
- Al-turany Mohammad
- Alam Sk Noor
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfaro Molina Jose Ruben
- Ali Yasir
- ALICE Collaboration
- Alici Andrea
- Alkin Anton
- Alme Johan
- Alt Torsten
- Altenkamper Lucas
- Altsybeev Igor
- Alves Garcia Prado Caio
- Andrei Cristian
- Andreou Dimitra
- Andrews Harry Arthur
- Andronic Anton
- Anguelov Venelin
- Anson Christopher Daniel
- Anticic Tome
- Antinori Federico
- Antonioli Pietro
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Araujo Silva Figueredo Marcel
- Arcelli Silvia
- Arnaldi Roberta
- Arnold Oliver Werner
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- Arslandok Mesut
- Audurier Benjamin
- Augustinus Andre
- Averbeck Ralf Peter
- Azmi Mohd Danish
- Badala Angela
- Baek Yong Wook
- Bagnasco Stefano
- Bailhache Raphaelle Marie
- Bala Renu
- Baldisseri Alberto
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- Yin Zhongbao
- Yokoyama Hiroki
- Yoo In-kwon
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- Zaccolo Valentina
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- Zbroszczyk Hanna Paulina
- Zhalov Mikhail
- Zhang Haitao
- Zhang Xiaoming
- Zhang Yonghong
- Zhang Zuman
- Zhao Chengxin
- Zhigareva Natalia
- Zhou Daicui
- Zhou You
- Zhou Zhuo
- Zhu Hongsheng
- Zhu Jianhui
- Zhu Ya
- Zichichi Antonino
- Zimmermann Markus Bernhard
- Zinovjev Gennady
- Zmeskal Johann
- Zou Shuguang
- Publication venue
- Publication date
- 01/01/2017
- Field of study
Results on the production of He-4 and (4) nuclei in Pb-Pb collisions at root(NN)-N-S = 2.76 TeV in the rapidity range vertical bar y vertical bar <1, using the ALICE detector, are presented in this paper. The rapidity densities corresponding to 0-10% central events are found to be dN/dy4(He) = (0.8 +/- 0.4 (stat) +/- 0.3 (syst)) x 10(-6) and dN/dy4 = (1.1 +/- 0.4 (stat) +/- 0.2 (syst)) x 10(-6), respectively. This is in agreement with the statistical thermal model expectation assuming the same chemical freeze-out temperature (T-chem = 156 MeV) as for light hadrons. The measured ratio of (4)/He-4 is 1.4 +/- 0.8 (stat) +/- 0.5 (syst). (C) 2018 Published by Elsevier B.V.Peer reviewe
Multiplicity dependence of light (anti-)nuclei production in p–Pb collisions at sNN=5.02 TeV
- Author
- Acharya Shreyasi
- Adamova Dagmar
- Adhya Souvik Priyam
- Adler Alexander
- Adolfsson Jonatan
- Aggarwal Madan Mohan
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Akindinov Alexander
- Al-turany Mohammad
- Alam Sk Noor
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Mas'ud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Ali Yasir
- Alici Andrea
- Alkin Anton
- Alme Johan
- Alt Torsten
- Altenkamper Lucas
- Altsybeev Igor
- Anaam Mustafa Naji
- Andrei Cristian
- Andreou Dimitra
- Andrews Harry Arthur
- Andronic Anton
- Angeletti Massimo
- Anguelov Venelin
- Anson Christopher Daniel
- Anticic Tome
- Antinori Federico
- Antonioli Pietro
- Anwar Rafay
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- Aphecetche Laurent Bernard
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- Augustinus Andre
- Averbeck Ralf Peter
- Aziz Sizar
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- Wilkinson Jeremy John
- Willems Guido Alexander
- Willsher Emily Jade
- Windelband Bernd Stefan
- Witt William Edward
- Wu Yitao
- Xu Ran
- Yalcin Kuzu Serpil
- Yamakawa Kosei
- Yang Shiming
- Yano Satoshi
- Yasin Zafar
- Yin Zhongbao
- Yokoyama Hiroki
- Yoo In Kwon
- Yoon Jin Hee
- Yuan Shiming
- Yuncu Alperen
- Yurchenko Volodymyr
- Zaccolo Valentina
- Zaman Ali
- Zampolli Chiara
- Zardoshti Nima
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zbroszczyk Hanna Paulina
- Zhalov Mikhail
- Zhang Xiaoming
- Zhang Zuman
- Zhao Chengxin
- Zherebchevskii Vladimir
- Zhigareva Natalia
- Zhou Daicui
- Zhou You
- Zhou Zhuo
- Zhu Jianhui
- Zhu Ya
- Zichichi Antonino
- Zimmermann Markus Bernhard
- Zinovjev Gennady
- Zurlo Nicola
- Publication venue
- Publication date
- 01/01/2019
- Field of study
The measurement of the deuteron and anti-deuteron production in the rapidity range −1 < y < 0 as a function of transverse momentum and event multiplicity in p–Pb collisions at √sNN = 5.02 TeV is presented. (Anti-)deuterons are identified via their specific energy loss dE/dx and via their time-of- flight. Their production in p–Pb collisions is compared to pp and Pb–Pb collisions and is discussed within the context of thermal and coalescence models. The ratio of integrated yields of deuterons to protons (d/p) shows a significant increase as a function of the charged-particle multiplicity of the event starting from values similar to those observed in pp collisions at low multiplicities and approaching those observed in Pb–Pb collisions at high multiplicities. The mean transverse particle momenta are extracted from the deuteron spectra and the values are similar to those obtained for p and particles. Thus, deuteron spectra do not follow mass ordering. This behaviour is in contrast to the trend observed for non-composite particles in p–Pb collisions. In addition, the production of the rare 3He and 3He nuclei has been studied. The spectrum corresponding to all non-single diffractive p-Pb collisions is obtained in the rapidity window −1 < y < 0 and the pT-integrated yield dN/dy is extracted. It is found that the yields of protons, deuterons, and 3He, normalised by the spin degeneracy factor, follow an exponential decrease with mass number
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- Ηο
- €autier ΤηέορΜΙβ R.
- Publication venue
- 'Walter de Gruyter GmbH'
- Publication date
- 01/01/1943
- Field of study
Measurement of electrons from semileptonic heavy-flavour hadron decays at midrapidity in pp and Pb–Pb collisions at √sNN = 5.02 TeV
- Author
- Acharya Shreyasi
- Adamová Dagmar
- Adhya S.P.
- Adler Alexander
- Adolfsson Jonatan
- Aggarwal Madan Mohan
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Akindinov Alexander
- Al-Turany Mohammad
- Alam Sk Noor
- Albuquerque Danilo Silva de
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Mas’ud
- Alfaro Molina Jose Ruben
- Ali B.
- Ali Y.
- Alici Andrea
- Alkin Anton
- Alme Johan
- Alt Torsten
- Altenkämper Lucas
- Altsybeev Igor
- Anaam M.N.
- Andrei Cristian
- Andreou D.
- Andrews Harry Arthur
- Andronic Anton
- Angeletti M.
- Anguelov Venelin
- Anson Christopher Daniel
- Antinori Federico
- Antičić Tome
- Antonioli Pietro
- Anwar Rafay
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- Aphecetche Laurent Bernard
- Appelshäuser Harald
- Arcelli Silvia
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- Augustinus Andre
- Averbeck Ralf Peter
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- Tropp Lukas
- Trubnikov Victor
- Trzaska Wladyslaw Henryk
- Trzcinski Tomasz Piotr
- Trzeciak Barbara Antonina
- Tsuji Tomoya
- Tumkin Alexandr
- Turrisi Rosario
- Tveter Trine Spedstad
- Ullaland Kjetil
- Umaka Ejiro Naomi
- Uras Antonio
- Usai Gianluca
- Utrobicic Antonija
- Vala Martin
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- Varga Z.
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- Vasiliev Andrey
- Vazquez Rueda Omar
- Vechernin Vladimir
- Veen Annelies Marianne
- Vercellin Ermanno
- Vergara Limón Sergio
- Vermunt L.
- Vernet Renaud
- Vicencio M.G.D.L.C.
- Vicković Linda
- Viinikainen Jussi Samuli
- Vilakazi Zabulon
- Villalobos Baillie Orlando
- Villatoro Tello Abraham
- Vino G.
- Vinogradov Alexander A.
- Virgili Tiziano
- Vislavicius Vytautas
- Vodopyanov Alexander
- Volkel Benedikt
- Voloshin Kirill
- Voloshin Sergei
- Volpe Giacomo
- Vorobyev Ivan
- Voscek Dominik
- Vrláková Janka
- Vyvre Pierre vande
- Vázquez Doce Oton
- Vértesi Róbert
- Völkl Martin Andreas
- Wagner Boris
- Watanabe Yosuke
- Weber Michael
- Weber Steffen Georg
- Wegrzynek Adam Tadeusz
- Weiser Dennis
- Wenzel Sandro Christian
- Wessels Johannes P.
- Widmann E.
- Wiechula Jens
- Wikne Jon
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy
- Willems Guido Alexander
- Willsher Emily Jade
- Windelband Bernd
- Witt William Edward
- Wu Y.
- Xu R.
- Yalcin Serpil
- Yamakawa Kosei
- Yang S.
- Yano Satoshi
- Yin Zhongbao
- Yokoyama Hiroki
- Yoo In-Kwon
- Yoon Jin-Hee
- Yuan S.
- Yurchenko Volodymyr
- Yüncü Alperen
- Zaccolo Valentina
- Zaman Ali
- Zampolli Chiara
- Zanoli Henrique Jose Correia
- Zardoshti Nima
- Zarochentsev Andrey
- Zaviyalov Nikolaj
- Zbroszczyk Hanna Paulina
- Zhalov Mikhail
- Zhang Xiaoming
- Zhang Z.
- Zhao C.
- Zherebchevskii V.
- Zhigareva Natalia
- Zhou Daicui
- Zhou You
- Zhou Zhuo
- Zhu Jianhui
- Zhu Y.
- Zichichi Antonino
- Zimmermann Markus Bernhard
- Zinovjev Gennady M.
- Zurlo Nicola
- Závada Petr
- Šafařík Karel
- Šefčík Michal
- Šuljić Miljenko
- Šumbera Michal
- Publication venue
- 'Elsevier BV'
- Publication date
- 20/03/2020
- Field of study
The differential invariant yield as a function of transverse momentum (pT) of electrons from semileptonic heavy-flavour hadron decays was measured at midrapidity in central (0–10%), semi-central (30–50%) and peripheral (60–80%) lead–lead (Pb–Pb) collisions at √sNN = 5.02 TeV in the pT intervals 0.5–26 GeV/c (0–10% and 30–50%) and 0.5–10 GeV/c (60–80%). The production cross section in proton–proton (pp) collisions at √s = 5.02 TeV was measured as well in 0.5 < pT < 10 GeV/c and it lies close to the upper band of perturbative QCD calculation uncertainties up to pT = 5 GeV/c and close to the mean value for larger pT. The modification of the electron yield with respect to what is expected for an incoherent superposition of nucleon–nucleon collisions is evaluated by measuring the nuclear modification factor RAA. The measurement of the RAA in different centrality classes allows in-medium energy loss of charm and beauty quarks to be investigated. The RAA shows a suppression with respect to unity at intermediate pT, which increases while moving towards more central collisions. Moreover, the measured RAA is sensitive to the modification of the parton distribution functions (PDF) in nuclei, like nuclear shadowing, which causes a suppression of the heavy-quark production at low pT in heavy-ion collisions at LHC
Analysis of the apparent nuclear modification in peripheral Pb–Pb collisions at 5.02 TeV
- Author
- Acharya Shreyasi
- Adamova Dagmar
- Adolfsson Jonatan
- Aggarwal Madan Mohan
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahn Sang Un
- Aiola Salvatore
- Akindinov Alexander
- Al-Turany Mohammad
- Alam Sk Noor
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfaro Molina Jose Ruben
- Ali Yasir
- Alici Andrea
- Alkin Anton
- Alme Johan
- Alt Torsten
- Altenkamper Lucas
- Altsybeev Igor
- Anaam Mustafa Naji
- Andrei Cristian
- Andreou Dimitra
- Andrews Harry Arthur
- Andronic Anton
- Angeletti Massimo
- Anguelov Venelin
- Anson Christopher Daniel
- Anticic Tome
- Antinori Federico
- Antonioli Pietro
- Anwar Rafay
- Apadula Nicole
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Araujo Silva Figueredo Marcel
- Arcelli Silvia
- Arnaldi Roberta
- Arnold Oliver Werner
- Arratia Munoz Miguel Ignacio
- Arsene Ionut Cristian
- Arslandok Mesut
- Arteche Diaz Raul
- Augustinus Andre
- Averbeck Ralf Peter
- Azmi Mohd Danish
- Badala Angela
- Baek Yong Wook
- Bagnasco Stefano
- Bailhache Raphaelle Marie
- Bala Renu
- Baldisseri Alberto
- Ball Markus
- Baral Rama Chandra
- Barbano Anastasia Maria
- Barbera Roberto
- Barile Francesco
- Barioglio Luca
- Barnafoldi Gergely Gabor
- Barnby Lee Stuart
- Bartalini Paolo
- Barth Klaus
- Bartsch Esther
- Bashir Butt Jamila
- Bastid Nicole
- Basu Sumit
- Batigne Guillaume
- Batyunya Boris
- Batzing Paul Christoph
- Bautista Guzman Irais
- Bazo Alba Jose Luis
- Bearden Ian Gardner
- Beck Hans
- Bedda Cristina
- Behera Nirbhay Kumar
- Belikov Iouri
- Bellini Francesca
- Bello Martinez Hector
- Bellwied Rene
- Belyaev Vladimir
- Bencedi Gyula
- Beole Stefania
- Bercuci Alexandru
- Berdnikov Yaroslav
- Berenyi Daniel
- Bertens Redmer Alexander
- Berzano Dario
- Betev Latchezar
- Bhaduri Partha Pratim
- Bhasin Anju
- Bhat Inayat Rasool
- Bhatt Himani
- Bhattacharjee Buddhadeb
- Bhom Jihyun
- Bianchi Antonio
- Bianchi Livio
- Bianchi Nicola
- Bielcik Jaroslav
- Bielcikova Jana
- Bilandzic Ante
- Biro Gabor
- Biswas Rathijit
- Biswas Saikat
- Blair Justin Thomas
- Blau Dmitry
- Blume Christoph
- Boca Gianluigi
- Bock Friederike
- Bogdanov Alexey
- Boldizsar Laszlo
- Bombara Marek
- Bonomi Germano
- Bonora Matthias
- Borel Herve
- Borissov Alexander
- Borri Marcello
- Botta Elena
- Bourjau Christian
- Bratrud Lars
- Braun-Munzinger Peter
- Bregant Marco
- Broker Theo Alexander
- Broz Michal
- Brucken Erik Jens
- Bruna Elena
- Bruno Giuseppe Eugenio
- Budnikov Dmitry
- Buesching Henner
- Bufalino Stefania
- Buhler Paul
- Buncic Predrag
- Busch Oliver
- Buthelezi Edith Zinhle
- Buxton Jesse Thomas
- Cabala Jan
- Cabanillas Noris Juan Carlos
- Caffarri Davide
- Caines Helen Louise
- Caliva Alberto
- Calvo Villar Ernesto
- Camerini Paolo
- Capon Aaron Allan
- Carena Francesco
- Carena Wisla
- Carnesecchi Francesca
- Castillo Castellanos Javier Ernesto
- Castro Andrew John
- Casula Ester Anna Rita
- Ceballos Sanchez Cesar
- Chandra Sinjini
- Chang Beomsu
- Chang Wan
- Chapeland Sylvain
- Chartier Marielle
- Chattopadhyay Subhasis
- Chattopadhyay Sukalyan
- Chauvin Alex
- Cheshkov Cvetan Valeriev
- Cheynis Brigitte
- Chibante Barroso Vasco Miguel
- Cho Soyeon
- Chochula Peter
- Chowdhury Tasnuva
- Christakoglou Panagiotis
- Christensen Christian Holm
- Christiansen Peter
- Chujo Tatsuya
- Chung Suh-Urk
- Cicalo Corrado
- Cifarelli Luisa
- Cindolo Federico
- Cleymans Jean Willy Andre
- Colamaria Fabio Filippo
- Colella Domenico
- Collu Alberto
- Colocci Manuel
- Concas Matteo
- Conesa Balbastre Gustavo
- Conesa del Valle Zaida
- Contreras Nuno Jesus Guillermo
- Cormier Thomas Michael
- Corrales Morales Yasser
- Correa Zanoli Henrique Jose
- Cortese Pietro
- Cosentino Mauro Rogerio
- Costa Filippo
- Costanza Susanna
- Crkovska Jana
- Crochet Philippe
- Cuautle Flores Eleazar
- Cunqueiro Mendez Leticia
- Dahms Torsten
- Dainese Andrea
- Dani Sanskruti
- Danisch Meike Charlotte
- Danu Andrea
- Das Debasish
- Das Indranil
- Das Supriya
- Dash Ajay Kumar
- Dash Sadhana
- de Caro Annalisa
- de Cataldo Giacinto
- de Conti Camila
- de Cuveland Jan
- de Falco Alessandro
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- Watanabe Yosuke
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- Wenzel Sandro Christian
- Wessels Johannes Peter
- Westerhoff Uwe
- Whitehead Andile Mothegi
- Wiechula Jens
- Wikne Jon
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Willems Guido Alexander
- Williams Crispin
- Willsher Emily
- Windelband Bernd Stefan
- Witt William Edward
- Xu Ran
- Yalcin Serpil
- Yamakawa Kosei
- Yano Satoshi
- Yin Zhongbao
- Yokoyama Hiroki
- Yoo In-Kwon
- Yoon Jin Hee
- Yurchenko Volodymyr
- Zaccolo Valentina
- Zaman Ali
- Zampolli Chiara
- Zardoshti Nima
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zbroszczyk Hanna Paulina
- Zhalov Mikhail
- Zhang Xiaoming
- Zhang Yonghong
- Zhang Zuman
- Zhao Chengxin
- Zherebchevskii Vladimir
- Zhigareva Natalia
- Zhou Daicui
- Zhou You
- Zhou Zhuo
- Zhu Hongsheng
- Zhu Jianhui
- Zhu Ya
- Zichichi Antonino
- Zimmermann Markus Bernhard
- Zinovjev Gennady
- Zmeskal Johann
- Zou Shuguang
- Publication venue
- 'Elsevier BV'
- Publication date
- 05/05/2018
- Field of study
International audienceCharged-particle spectra at midrapidity are measured in Pb–Pb collisions at the centre-of-mass energy per nucleon–nucleon pair sNN=5.02 TeV and presented in centrality classes ranging from most central (0–5%) to most peripheral (95–100%) collisions. Possible medium effects are quantified using the nuclear modification factor ( RAA ) by comparing the measured spectra with those from proton–proton collisions, scaled by the number of independent nucleon–nucleon collisions obtained from a Glauber model. At large transverse momenta ( 8<pT<20GeV/c ), the average RAA is found to increase from about 0.15 in 0–5% central to a maximum value of about 0.8 in 75–85% peripheral collisions, beyond which it falls off strongly to below 0.2 for the most peripheral collisions. Furthermore, RAA initially exhibits a positive slope as a function of pT in the 8–20 GeV/c interval, while for collisions beyond the 80% class the slope is negative. To reduce uncertainties related to event selection and normalization, we also provide the ratio of RAA in adjacent centrality intervals. Our results in peripheral collisions are consistent with a PYTHIA-based model without nuclear modification, demonstrating that biases caused by the event selection and collision geometry can lead to the apparent suppression in peripheral collisions. This explains the unintuitive observation that RAA is below unity in peripheral Pb–Pb, but equal to unity in minimum-bias p–Pb collisions despite similar charged-particle multiplicities
Anisotropic flow of identified particles in Pb-Pb collisions at sNN=5.02 TeV
- Author
- Acharya S.
- Adamova Dagmar
- Adolfsson Jonatan
- Aggarwal Madan Mohan
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahn Sang Un
- Aiola Salvatore
- Akindinov Alexander
- Al-turany Mohammad
- Alam Sk Noor
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfaro Molina Jose Ruben
- Ali Yasir
- ALICE Collaboration
- Alici Andrea
- Alkin Anton
- Alme Johan
- Alt Torsten
- Altenkamper Lucas
- Altsybeev Igor
- Anaam Mustafa Naji
- Andrei Cristian
- Andreou Dimitra
- Andrews Harry Arthur
- Andronic Anton
- Angeletti Massimo
- Anguelov Venelin
- Anson Christopher Daniel
- Anticic Tome
- Antinori Federico
- Antonioli Pietro
- Anwar Rafay
- Apadula Nicole
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Araujo Silva Figueredo Marcel
- Arcelli Silvia
- Arnaldi Roberta
- Arnold Oliver Werner
- Arratia Munoz Miguel Ignacio
- Arsene Ionut Cristian
- Arslandok Mesut
- Arteche Diaz Raul
- Audurier Benjamin
- Augustinus Andre
- Averbeck Ralf Peter
- Azmi Mohd Danish
- Badala Angela
- Baek Yong Wook
- Bagnasco Stefano
- Bailhache Raphaelle Marie
- Bala Renu
- Baldisseri Alberto
- Ball Markus
- Baral Rama Chandra
- Barbano Anastasia Maria
- Barbera Roberto
- Barile Francesco
- Barioglio Luca
- Barnafoldi Gergely Gabor
- Barnby Lee Stuart
- Bartalini Paolo
- Barth Klaus
- Bartsch Esther
- Bashir Butt Jamila
- Bastid Nicole
- Basu Sumit
- Batigne Guillaume
- Batyunya Boris
- Batzing Paul Christoph
- Bautista Guzman Irais
- Bazo Alba Jose Luis
- Bearden Ian Gardner
- Beck Hans
- Bedda Cristina
- Behera Nirbhay Kumar
- Belikov Iouri
- Bellini Francesca
- Bello Martinez Hector
- Bellwied Rene
- Belyaev Vladimir
- Bencedi Gyula
- Beole Stefania
- Bercuci Alexandru
- Berdnikov Yaroslav
- Berenyi Daniel
- Bertens Redmer Alexander
- Berzano Dario
- Betev Latchezar
- Bhaduri Partha Pratim
- Bhasin Anju
- Bhat Inayat Rasool
- Bhatt Himani
- Bhattacharjee Buddhadeb
- Bhom Jihyun
- Bianchi Antonio
- Bianchi Livio
- Bianchi Nicola
- Bielcik Jaroslav
- Bielcikova Jana
- Bilandzic Ante
- Biro Gabor
- Biswas Rathijit
- Biswas Saikat
- Blair Justin Thomas
- Blau Dmitry
- Blume Christoph
- Boca Gianluigi
- Bock Friederike
- Bogdanov Alexey
- Boldizsar Laszlo
- Bombara Marek
- Bonomi Germano
- Bonora Matthias
- Borel Herve
- Borissov Alexander
- Borri Marcello
- Botta Elena
- Bourjau Christian
- Bratrud Lars
- Braun-munzinger Peter
- Bregant Marco
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- Willsher Emily
- Windelband Bernd Stefan
- Witt William Edward
- Xu Ran
- Yalcin Serpil
- Yamakawa Kosei
- Yano Satoshi
- Yin Zhongbao
- Yokoyama Hiroki
- Yoo In-kwon
- Yoon Jin Hee
- Yurchenko Volodymyr
- Zaccolo Valentina
- Zaman Ali
- Zampolli Chiara
- Zardoshti Nima
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zbroszczyk Hanna Paulina
- Zhalov Mikhail
- Zhang Xiaoming
- Zhang Yonghong
- Zhang Zuman
- Zhao Chengxin
- Zherebchevskii Vladimir
- Zhigareva Natalia
- Zhou Daicui
- Zhou You
- Zhou Zhuo
- Zhu Hongsheng
- Zhu Jianhui
- Zhu Ya
- Zichichi Antonino
- Zimmermann Markus Bernhard
- Zinovjev Gennady
- Zmeskal Johann
- Zou Shuguang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The elliptic (v2), triangular (v3), and quadrangular (v4) flow coefficients of π±, K±, p+p,Λ+Λ,KS0 , and the ϕ-meson are measured in Pb-Pb collisions at sNN=5.02 TeV. Results obtained with the scalar product method are reported for the rapidity range |y| < 0.5 as a function of transverse momentum, pT, at different collision centrality intervals between 0–70%, including ultra-central (0–1%) collisions for π±, K±, and p+p . For pT < 3 GeV/c, the flow coefficients exhibit a particle mass dependence. At intermediate transverse momenta (3 < pT < 8–10 GeV/c), particles show an approximate grouping according to their type (i.e., mesons and baryons). The ϕ-meson v2, which tests both particle mass dependence and type scaling, follows p+p v2 at low pT and π± v2 at intermediate pT. The evolution of the shape of vn(pT) as a function of centrality and harmonic number n is studied for the various particle species. Flow coefficients of π±, K±, and p+p for pT < 3 GeV/c are compared to iEBE-VISHNU and MUSIC hydrodynamical calculations coupled to a hadronic cascade model (UrQMD). The iEBE-VISHNU calculations describe the results fairly well for pT < 2.5 GeV/c, while MUSIC calculations reproduce the measurements for pT < 1 GeV/c. A comparison to vn coefficients measured in Pb-Pb collisions at sNN=2.76 TeV is also provided
Production of charged pions, kaons, and (anti-)protons in Pb-Pb and inelastic pp collisions at sNN = 5.02 TeV
- Author
- Acharya Shreyasi
- Adamova Dagmar
- Adhya Souvik Priyam
- Adler Alexander
- Adolfsson Jonatan
- Aggarwal Madan Mohan
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Akindinov Alexander
- Al-Turany Mohammad
- Alam Sk Noor
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Mas'Ud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Ali Yasir
- Alici Andrea
- Alkin Anton
- Alme Johan
- Alt Torsten
- Altenkamper Lucas
- Altsybeev Igor
- Anaam Mustafa Naji
- Andrei Cristian
- Andreou Dimitra
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- Anguelov Venelin
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- Matonoha Oliver
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- Mayer Christoph
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- Mazzoni Alessandra Maria
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- Menchaca-Rocha Arturo Alejandro
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- Oskarsson Anders Nils Erik
- Otwinowski Jacek Tomasz
- Oyama Ken
- Ozelin de Lima Pimentel Lais
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- Perez Lezama Edgar
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- Polishchuk Boris
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- Prasad Sidharth Kumar
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- Rakotozafindrabe Andry Malala
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- Rasanen Sami Sakari
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- Read Kenneth Francis
- Redlich Krzysztof
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- Reichelt Patrick Simon
- Reidt Felix
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- Sandoval Andres
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- Seger Janet Elizabeth
- Sekiguchi Yuko
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- Sett Priyanka
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- Shabetai Alexandre
- Shahoyan Ruben
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- Shigaki Kenta
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- Shou Qiye
- Sibiryak Yury
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- Silvermyr David Olle Rickard
- Silvestre Catherine Micaela
- Simatovic Goran
- Simonetti Giuseppe
- Singh Ranbir
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- Sitta Mario
- Skaali Bernhard
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- Snellings Raimond
- Snellman Tomas Wilhelm
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- Song Jihye
- Songmoolnak Arnon
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- Sputowska Iwona Anna
- Spyropoulou-Stassinaki Martha
- Stachel Johanna
- Stan Ionel
- Stankus Paul William
- Steffanic Patrick John
- Stenlund Evert Anders
- Stocco Diego
- Storetvedt Maksim Melnik
- Strmen Peter
- Sugitate Toru
- Suire Christophe Pierre
- Suleymanov Mais Kazim Oglu
- Suljic Miljenko
- Sultanov Rishat
- Sumbera Michal
- Sumowidagdo Suharyo
- Swain Sagarika
- Szabo Alexander
- Szarka Imrich
- Tabassam Uzma
- Taillepied Guillaume
- Takahashi Jun
- Tambave Ganesh Jagannath
- Tang Siyu
- Tarhini Mohamad
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- Tauro Arturo
- Tejeda Munoz Guillermo
- Telesca Adriana
- Terrevoli Cristina
- Thakur Dhananjaya
- Thakur Sanchari
- Thomas Deepa
- Thoresen Freja
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- Timmins Anthony Robert
- Toia Alberica
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- Topilskaya Nataliya
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- Trifiro Antonio
- Tripathy Sushanta
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- Trogolo Stefano
- Trombetta Giuseppe
- Tropp Lukas
- Trubnikov Victor
- Trzaska Wladyslaw Henryk
- Trzcinski Tomasz Piotr
- Trzeciak Barbara Antonina
- Tsuji Tomoya
- Tumkin Alexandr
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- Tveter Trine Spedstad
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- Umaka Ejiro Naomi
- Uras Antonio
- Usai Gianluca
- Utrobicic Antonija
- Vala Martin
- Valle Nicolo'
- Vallero Sara
- van Der Kolk Naomi
- van Doremalen Lennart
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- Vande Vyvre Pierre
- Varga Dezso
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- Varga-Kofarago Monika
- Vargyas Marton
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- Vasileiou Maria
- Vasiliev Andrey
- Vazquez Doce Oton
- Vazquez Rueda Omar
- Vechernin Vladimir
- Veen Annelies Marianne
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- Villalobos Baillie Orlando
- Villatoro Tello Abraham
- Vino Gioacchino
- Vinogradov Alexander
- Virgili Tiziano
- Vislavicius Vytautas
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- Volkel Benedikt
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- Volpe Giacomo
- von Haller Barthelemy
- Vorobyev Ivan
- Voscek Dominik
- Vrlakova Janka
- Wagner Boris
- Weber Michael
- Weber Steffen Georg
- Wegrzynek Adam Tadeusz
- Weiser Dennis Franz
- Wenzel Sandro Christian
- Wessels Johannes Peter
- Wiechula Jens
- Wikne Jon
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Willems Guido Alexander
- Willsher Emily Jade
- Windelband Bernd Stefan
- Witt William Edward
- Wu Yitao
- Xu Ran
- Yalcin Kuzu Serpil
- Yamakawa Kosei
- Yang Shiming
- Yano Satoshi
- Yin Zhongbao
- Yokoyama Hiroki
- Yoo In Kwon
- Yoon Jin Hee
- Yuan Shiming
- Yuncu Alperen
- Yurchenko Volodymyr
- Zaccolo Valentina
- Zaman Ali
- Zampolli Chiara
- Zardoshti Nima
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zbroszczyk Hanna Paulina
- Zhalov Mikhail
- Zhang Xiaoming
- Zhang Zuman
- Zhao Chengxin
- Zherebchevskii Vladimir
- Zhigareva Natalia
- Zhou Daicui
- Zhou You
- Zhou Zhuo
- Zhu Jianhui
- Zhu Ya
- Zichichi Antonino
- Zimmermann Markus Bernhard
- Zinovjev Gennady
- Zurlo Nicola
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 27/09/2019
- Field of study
International audienceMid-rapidity production of π±, K± and (pˉ)p measured by the ALICE experiment at the LHC, in Pb-Pb and inelastic pp collisions at sNN = 5.02 TeV, is presented. The invariant yields are measured over a wide transverse momentum (pT) range from hundreds of MeV/c up to 20 GeV/c. The results in Pb-Pb collisions are presented as a function of the collision centrality, in the range 0−90%. The comparison of the pT-integrated particle ratios, i.e. proton-to-pion (p/π) and kaon-to-pion (K/π) ratios, with similar measurements in Pb-Pb collisions at sNN = 2.76 TeV show no significant energy dependence. Blast-wave fits of the pT spectra indicate that in the most central collisions radial flow is slightly larger at 5.02 TeV with respect to 2.76 TeV. Particle ratios (p/π, K/π) as a function of pT show pronounced maxima at pT ≈ 3 GeV/c in central Pb-Pb collisions. At high pT, particle ratios at 5.02 TeV are similar to those measured in pp collisions at the same energy and in Pb-Pb collisions at sNN = 2.76 TeV. Using the pp reference spectra measured at the same collision energy of 5.02 TeV, the nuclear modification factors for the different particle species are derived. Within uncertainties, the nuclear modification factor is particle species independent for high pT and compatible with measurements at sNN = 2.76 TeV. The results are compared to state-of-the-art model calculations, which are found to describe the observed trends satisfactorily
Multiplicity dependence of (multi-)strange hadron production in proton-proton collisions at s = 13 TeV
- Author
- Acharya Shreyasi
- Adamova Dagmar
- Adhya Souvik Priyam
- Adler Alexander
- Adolfsson Jonatan
- Aggarwal Madan Mohan
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Akindinov Alexander
- Al-turany Mohammad
- Alam Sk Noor
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Mas'ud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Ali Yasir
- ALICE Collaboration
- Alici Andrea
- Alkin Anton
- Alme Johan
- Alt Torsten
- Altenkamper Lucas
- Altsybeev Igor
- Anaam Mustafa Naji
- Andrei Cristian
- Andreou Dimitra
- Andrews Harry Arthur
- Andronic Anton
- Angeletti Massimo
- Anguelov Venelin
- Anson Christopher Daniel
- Anticic Tome
- Antinori Federico
- Antonioli Pietro
- Anwar Rafay
- Apadula Nicole
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Arcelli Silvia
- Arnaldi Roberta
- Arratia Munoz Miguel Ignacio
- Arsene Ionut Cristian
- Arslandok Mesut
- Arteche Diaz Raul
- Augustinus Andre
- Averbeck Ralf Peter
- Aziz Sizar
- Azmi Mohd Danish
- Badala Angela
- Baek Yongwook
- Bagnasco Stefano
- Bai Xiaozhi
- Bailhache Raphaelle Marie
- Bala Renu
- Baldisseri Alberto
- Ball Markus
- Balouza Samah
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- Barbera Roberto
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- Barnafoldi Gergely Gabor
- Barnby Lee Stuart
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- Barth Klaus
- Bartsch Esther
- Baruffaldi Filippo
- Bashir Butt Jamila
- Bastid Nicole
- Basu Sumit
- Batigne Guillaume
- Batyunya Boris
- Batzing Paul Christoph
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- Bautista Guzman Irais
- Bazo Alba Jose Luis
- Bearden Ian Gardner
- Bedda Cristina
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- Szabo Alexander
- Szarka Imrich
- Tabassam Uzma
- Taillepied Guillaume
- Takahashi Jun
- Tambave Ganesh Jagannath
- Tang Siyu
- Tarhini Mohamad
- Tarzila Madalina-gabriela
- Tauro Arturo
- Tejeda Munoz Guillermo
- Telesca Adriana
- Terrevoli Cristina
- Thakur Dhananjaya
- Thakur Sanchari
- Thomas Deepa
- Thoresen Freja
- Tieulent Raphael Noel
- Tikhonov Anatoly
- Timmins Anthony Robert
- Toia Alberica
- Toledo Matuoka Paula Fernanda
- Topilskaya Nataliya
- Toppi Marco
- Torales Acosta Fernando
- Trifiro Antonio
- Tripathy Sushanta
- Tripathy Tulika
- Trogolo Stefano
- Trombetta Giuseppe
- Tropp Lukas
- Trubnikov Victor
- Trzaska Wladyslaw Henryk
- Trzcinski Tomasz Piotr
- Trzeciak Barbara Antonina
- Tsuji Tomoya
- Tumkin Alexandr
- Turrisi Rosario
- Tveter Trine Spedstad
- Ullaland Kjetil
- Umaka Ejiro Naomi
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- Vala Martin
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- Van Leeuwen Marco
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- Varga Dezso
- Varga Zoltan
- Varga-kofarago Monika
- Vargyas Marton
- Varma Raghava
- Vasileiou Maria
- Vasiliev Andrey
- Vazquez Doce Oton
- Vazquez Rueda Omar
- Vechernin Vladimir
- Veen Annelies Marianne
- Vercellin Ermanno
- Vergara Limon Sergio
- Vermunt Lucas Anne
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- Vertesi Robert
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- Viinikainen Jussi Samuli
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- Vino Gioacchino
- Vinogradov Alexander
- Virgili Tiziano
- Vislavicius Vytautas
- Vodopyanov Alexander
- Volkel Benedikt
- Volkl Martin Andreas
- Voloshin Kirill
- Voloshin Sergey
- Volpe Giacomo
- Von Haller Barthelemy
- Vorobyev Ivan
- Voscek Dominik
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- Wagner Boris
- Weber Michael
- Weber Steffen Georg
- Wegrzynek Adam Tadeusz
- Weiser Dennis Franz
- Wenzel Sandro Christian
- Wessels Johannes Peter
- Widmann Eberhard
- Wiechula Jens
- Wikne Jon
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Willems Guido Alexander
- Willsher Emily Jade
- Windelband Bernd Stefan
- Witt William Edward
- Wu Yitao
- Xu Ran
- Yalcin Kuzu Serpil
- Yamakawa Kosei
- Yang Shiming
- Yano Satoshi
- Yin Zhongbao
- Yokoyama Hiroki
- Yoo In Kwon
- Yoon Jin Hee
- Yuan Shiming
- Yuncu Alperen
- Yurchenko Volodymyr
- Zaccolo Valentina
- Zaman Ali
- Zampolli Chiara
- Zardoshti Nima
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zbroszczyk Hanna Paulina
- Zhalov Mikhail
- Zhang Xiaoming
- Zhang Zuman
- Zhao Chengxin
- Zherebchevskii Vladimir
- Zhigareva Natalia
- Zhou Daicui
- Zhou You
- Zhou Zhuo
- Zhu Jianhui
- Zhu Ya
- Zichichi Antonino
- Zimmermann Markus Bernhard
- Zinovjev Gennady
- Zurlo Nicola
- Publication venue
- Springer
- Publication date
- 05/08/2019
- Field of study
The production rates and the transverse momentum distribution of strange hadrons at mid-rapidity (∣y∣<0.5) are measured in proton-proton collisions at s = 13 TeV as a function of the charged particle multiplicity, using the ALICE detector at the LHC. The production rates of KS0, Λ, Ξ, and Ω 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
Measurement of the low-energy antideuteron inelastic cross section
- Author
- Acharya Shreyasi
- Adamova Dagmar
- Adler Alexander
- Adolfsson Jonatan
- Aggarwal Madan Mohan
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Akbar Zaenal
- Akindinov Alexander
- Al-turany Mohammad
- Alam Sk Noor
- Alarcon Do Passo Suaide Alexandre
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Mas'ud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Ali Yasir
- ALICE Collaboration
- Alici Andrea
- Alizadehvandchali Negin
- Alkin Anton
- Alme Johan
- Alt Torsten
- Altenkamper Lucas
- Altsybeev Igor
- Alvarado Garcia Jesus Ricardo
- Anaam Mustafa
- Andrei Cristian
- Andreou Dimitra
- Andronic Anton
- Angeletti Massimo
- Anguelov Venelin
- Anson Christopher Daniel
- Anticic Tome
- Antinori Federico
- Antonioli Pietro
- Apadula Nicole
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Arcelli Silvia
- Arnaldi Roberta
- Arratia Munoz Miguel Ignacio
- Arsene Ionut Cristian
- Arslandok Mesut
- Arteche Diaz Raul
- Augustinus Andre
- Averbeck Ralf Peter
- Aziz Sizar
- Azmi Mohd Danish
- Badala Angela
- Baek Yongwook
- Bagnasco Stefano
- Bai Xiaozhi
- Bailhache Raphaelle Marie
- Bala Renu
- Balbino Alessandro
- Baldisseri Alberto
- Ball Markus
- Balouza Samah
- Banerjee Debjani
- Barbera Roberto
- Barioglio Luca
- Barnafoldi Gergely Gabor
- Barnby Lee Stuart
- Bartalini Paolo
- Bartels Clara
- Barth Klaus
- Bartsch Esther
- Baruffaldi Filippo
- Bashir Butt Jamila
- Bastid Nicole
- Basu Sumit
- Batigne Guillaume
- Batyunya Boris
- Bauri Dibakar
- Bautista Guzman Irais
- Bazo Alba Jose Luis
- Bearden Ian Gardner
- Beattie Caitlin
- Bedda Cristina
- Behera Nirbhay Kumar
- Belikov Iouri
- Bell Hechavarria Ailec
- Bellini Francesca
- Bellwied Rene
- Belyaev Vladimir
- Bencedi Gyula
- Beole Stefania
- Bercuci Alexandru
- Berdnikov Yaroslav
- Berenyi Daniel
- Bertens Redmer Alexander
- Berzano Dario
- Besoiu Mihaela Gabriela
- Betev Latchezar
- Bhasin Anju
- Bhat Inayat Rasool
- Bhat Mohammad Asif
- Bhatt Himani
- Bhattacharjee Buddhadeb
- Bianchi Antonio
- Bianchi Livio
- Bianchi Nicola
- Bielcik Jaroslav
- Bielcikova Jana
- Bilandzic Ante
- Biro Gabor
- Biswas Rathijit
- Biswas Saikat
- Blair Justin Thomas
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- Blume Christoph
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- Bock Friederike
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- Sas Mike Henry Petrus
- Sasikumar Menon Anjaly
- Scapparone Eugenio
- Schambach Johann Joachim
- Scheid Horst Sebastian
- Schiaua Claudiu Cornel
- Schicker Rainer Martin
- Schmah Alexander
- Schmidt Christian Joachim
- Schmidt Hans Rudolf
- Schmidt Marten Ole
- Schmidt Martin
- Schmidt Nicolas
- Schmier Austin Robert
- Schukraft Jurgen
- Schutz Yves Roland
- Schwarz Kilian Eberhard
- Schweda Kai Oliver
- Scioli Gilda
- Scomparin Enrico
- Seger Janet Elizabeth
- Sekiguchi Yuko
- Sekihata Daiki
- Selyuzhenkov Ilya
- Senyukov Serhiy
- Serebryakov Dmitry
- Sevcenco Adrian
- Shabanov Arseniy
- Shabetai Alexandre
- Shahoyan Ruben
- Shaikh Wadut
- Shangaraev Artem
- Sharma Anjali
- Sharma Ankita
- Sharma Himanshu
- Sharma Meenakshi
- Sharma Natasha
- Sharma Sheetal
- Sheibani Oveis
- Shigaki Kenta
- Shirinkin Sergey
- Shou Qiye
- Sibiryak Yury
- Siddhanta Sabyasachi
- Siemiarczuk Teodor
- Silva De Albuquerque Danilo
- Silvermyr David Olle Rickard
- Simatovic Goran
- Simonetti Giuseppe
- Singh Bhawani
- Singh Ranbir
- Singh Randhir
- Singh Ravindra
- Singh Vivek
- Singhal Vikas
- Sitar Branislav
- Sitta Mario
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- Song Jihye
- Songmoolnak Arnon
- Soramel Francesca
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- Soto Camacho Rabi
- Sputowska Iwona Anna
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- Stan Ionel
- Steffanic Patrick John
- Stenlund Evert Anders
- Stiefelmaier Stephan Friedrich
- Stocco Diego
- Storetvedt Maksim Melnik
- Sugitate Toru
- Suire Christophe Pierre
- Suleymanov Mais Kazim Oglu
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- Sultanov Rishat
- Sumbera Michal
- Sumberia Vikash
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- Swain Sagarika
- Szabo Alexander
- Szarka Imrich
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- Taghavi Seyed Farid
- Taillepied Guillaume
- Takahashi Jun
- Tambave Ganesh Jagannath
- Tang Siyu
- Tarhini Mohamad
- Tarzila Madalina-gabriela
- Tauro Arturo
- Tejeda Munoz Guillermo
- Telesca Adriana
- Terlizzi Livia
- Terrevoli Cristina
- Thakur Dhananjaya
- Thakur Sanchari
- Thomas Deepa
- Thoresen Freja
- Tieulent Raphael Noel
- Tikhonov Anatoly
- Timmins Anthony Robert
- Toia Alberica
- Toledo Matuoka Paula Fernanda
- Topilskaya Nataliya
- Toppi Marco
- Torales Acosta Fernando
- Trifiro Antonio
- Tripathy Sushanta
- Tripathy Tulika
- Trogolo Stefano
- Trombetta Giuseppe
- Tropp Lukas
- Trubnikov Victor
- Trzaska Wladyslaw Henryk
- Trzcinski Tomasz Piotr
- Trzeciak Barbara Antonina
- Tumkin Alexandr
- Turrisi Rosario
- Tveter Trine Spedstad
- Ullaland Kjetil
- Umaka Ejiro Naomi
- Uras Antonio
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- Vala Martin
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- Vallero Sara
- Van Der Kolk Naomi
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- Vande Vyvre Pierre
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- Varga Zoltan
- Varga-kofarago Monika
- Vasileiou Maria
- Vasiliev Andrey
- Vazquez Doce Oton
- Vazquez Rueda Omar
- Vechernin Vladimir
- Vercellin Ermanno
- Vergara Limon Sergio
- Vermunt Lucas Anne
- Vernet Renaud
- Vertesi Robert
- Vickovic Linda
- Vilakazi Zabulon
- Villalobos Baillie Orlando
- Vino Gioacchino
- Vinogradov Alexander
- Virgili Tiziano
- Vislavicius Vytautas
- Vodopyanov Alexander
- Volkel Benedikt
- Volkl Martin Andreas
- Voloshin Kirill
- Voloshin Sergey
- Volpe Giacomo
- Von Haller Barthelemy
- Vorobyev Ivan
- Voscek Dominik
- Vrlakova Janka
- Wagner Boris
- Weber Michael
- Weber Steffen Georg
- Wegrzynek Adam Tadeusz
- Wenzel Sandro Christian
- Wessels Johannes Peter
- Wiechula Jens
- Wikne Jon
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Willems Guido Alexander
- Willsher Emily Jade
- Windelband Bernd Stefan
- Winn Michael Andreas
- Witt William Edward
- Wright Josephina Rae
- Wu Yitao
- Xu Ran
- Yalcin Kuzu Serpil
- Yamaguchi Yorito
- Yamakawa Kosei
- Yang Shiming
- Yano Satoshi
- Yin Zhongbao
- Yokoyama Hiroki
- Yoo In Kwon
- Yoon Jin Hee
- Yu Zhi
- Yuan Shiming
- Yuncu Alperen
- Yurchenko Volodymyr
- Zaccolo Valentina
- Zaman Ali
- Zampolli Chiara
- Zardoshti Nima
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zbroszczyk Hanna Paulina
- Zhalov Mikhail
- Zhang Song
- Zhang Xiaoming
- Zhang Zuman
- Zherebchevskii Vladimir
- Zhou Daicui
- Zhou You
- Zhou Zhuo
- Zhu Jianhui
- Zhu Ya
- Zichichi Antonino
- Zinovjev Gennady
- Zurlo Nicola
- Publication venue
- APS
- Publication date
- 01/01/2020
- Field of study
In this Letter, we report the first measurement of the inelastic cross section for antideuteron-nucleus interactions at low particle momenta, covering a range of 0.3 ≤ p < 4 GeV/c. The measurement is carried out using p-Pb collisions at a center-of-mass energy per nucleon–nucleon pair of sNN = 5.02 TeV, recorded with the ALICE detector at the CERN LHC and utilizing the detector material as an absorber for antideuterons and antiprotons. The extracted raw primary antiparticle-to-particle ratios are compared to the results from detailed ALICE simulations based on the geant4 toolkit for the propagation of (anti)particles through the detector material. The analysis of the raw primary (anti)proton spectra serves as a benchmark for this study, since their hadronic interaction cross sections are well constrained experimentally. The first measurement of the inelastic cross section for antideuteron-nucleus interactions averaged over the ALICE detector material with atomic mass numbers ⟨A⟩ = 17.4 and 31.8 is obtained. The measured inelastic cross section points to a possible excess with respect to the Glauber model parametrization used in geant4 in the lowest momentum interval of 0.3 ≤ p < 0.47 GeV/c up to a factor 2.1. This result is relevant for the understanding of antimatter propagation and the contributions to antinuclei production from cosmic ray interactions within the interstellar medium. In addition, the momentum range covered by this measurement is of particular importance to evaluate signal predictions for indirect dark-matter searches
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