292 research outputs found
Pay Satisfaction, Job Satisfaction and Turnover Intent
- Publication venue
- 'Consortium Erudit'
- Publication date
- 01/01/2010
- Field of study
The purpose of this paper was to examine the relationships among pay satisfaction, job satisfaction, and turnover. While there is a fairly large body of literature on pay satisfaction/dissatisfaction-turnover relationship, there are reasons to expect different outcomes in occupations – such as social work and nursing – where job satisfaction, versus pay, may be of equal, if not greater importance. Essentially, it may be argued that in these sectors, workers are driven more by job satisfaction rather than their paychecks. Yet, there is little empirical research on this issue; thus, a primary purpose of this study is to address this research need. This study will add to the recent research that has focused on key human resources management and industrial relations issues related to the nursing profession in Canada. Furthermore, many studies use a unidimensional measure of pay satisfaction even though the literature suggests that there are better measures. Using a four-dimensional instrument in this study, we improve on past practices.Using a sample of 200 nurses in a unionized hospital in Ontario to test our hypotheses, we found support for both (viz., 1. The four pay dimensions will affect turnover intent differently; and 2. Job satisfaction will add incrementally to the explained variance in the pay satisfaction-turnover relationship). The findings support the contention that nurses may be more motivated by their jobs, versus their pay. The findings may be good news for organizations that want to better manage labour costs. There are different ways for hospitals to improve their workplace environment in order to increase satisfaction with intrinsic job factors and reduce turnover.Cet article examine la relation entre la satisfaction à l’égard de la rémunération, la satisfaction au travail et le roulement de la main-d’oeuvre. Alors qu’il existe un corpus plutôt vaste de littérature sur la satisfaction/insatisfaction à l’égard de la rémunération, il y a des raisons de penser que les résultats pourraient différés pour certaines professions, comme dans le cas du travail social et celui des soins infirmiers, où la satisfaction au travail comparativement à celle à l’égard de la rémunération peut être d’importance égale ou même supérieure. Essentiellement on peut argumenter que dans ces secteurs, les travailleurs et travailleuses sont davantage motivés par la satisfaction au travail que par leur chèque de paie. Pourtant il y a peu de recherche empirique sur ce sujet. Un premier objectif de l’étude est de combler en partie du moins ce manque. Elle ajoutera ainsi aux études récentes qui mettent l’accent sur la gestion des ressources humaines clés dans les organisations et les problèmes de relations industrielles liées à la profession des soins infirmiers au Canada. Plusieurs études utilisent une mesure unidimensionnelle de la satisfaction à l’égard de la rémunération alors que la littérature suggère que de meilleures mesures pourraient être utilisées. Aussi en proposant une mesure à quatre dimensions, nous croyons pouvoir améliorer les pratiques passées de recherche dans ce domaine.À partir d’un échantillon de 200 infirmiers et infirmières d’un hôpital torontois nous obtenons des résultats empiriques qui tendent à appuyer nos deux hypothèses, à savoir : 1) que chacune des quatre dimensions de la rémunération exerce un effet différent sur l’intention de quitter, et 2) que la satisfaction au travail constitue un facteur additionnel dans l’explication de la variance dans la relation satisfaction à l’égard de la rémunération-roulement (intention de quitter). Cela constitue un appui à l’argument que les infirmiers et les infirmières sont sans doute davantage motivés par les conditions d’exercice de leur travail que par leur rémunération. De tels résultats peuvent être une bonne nouvelle pour les organisations désireuses de mieux gérer leurs coûts de main-d’oeuvre puisqu’il y a différentes façons pour les hôpitaux d’améliorer l’environnement de travail dans le but d’accroître la satisfaction à l’égard des caractéristiques intrinsèques du travail et ainsi réduire le roulement du personnel.El propósito de este documento es de examinar las relaciones entre satisfacción del salario, satisfacción del empleo y cambio de empleo. Mientras existe una impresionante cantidad de literatura sobre la relación satisfacción/insatisfacción del salario y cambio de empleo, hay razones para esperar diferentes resultados en las ocupaciones tales como trabajo social y enfermería – donde la satisfacción del empleo, versus salario, puede ser de igual sino de mayor importancia. Esencialmente, puede argumentarse que en estos sectores, los trabajadores son más interesados por la satisfacción del empleo que por sus cheques de pago. Además, hay pocos estudios empíricos sobre esta problemática; así, un primer propósito de este estudio de responder a esta necesidad de investigación. Este estudio se añade a la reciente investigación que ha focalizado las problemáticas claves de gestión de recursos humanos y de relaciones industriales respecto a la profesión de enfermería en Canadá. Más aún, muchos estudios utilizan una medida unidimensional de la satisfacción del salario aunque la literatura sugiere que hay mejores medidas. Usando un instrumento de cuatro dimensiones en este estudio, se mejora las prácticas pasadas.Se utiliza una muestra de 200 enfermeras en un hospital sindicalizado de Ontario para evaluar nuestras hipótesis siendo éstas validadas: 1. Las cuatro dimensiones de pago van afectar la intención de cambio de empleo de manera diferente; 2. La satisfacción del empleo aumenta la contribución para explicar la varianza en la relación satisfacción salarial – cambio de empleo. Estos resultados confirman el punto de vista que las enfermeras pueden estar más motivadas por sus empleo, versus sus salarios. Los resultados pueden ser buenas noticias para las organizaciones que quieren administrar mejor los costos del trabajo. Hay diferentes maneras en los hospitales de mejorar el ambiente en el lugar de trabajo de manera a aumentar la satisfacción con los factores intrínsecos del empleo y reducir así el cambio de empleo
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
- Arsene Ionut Cristian
- 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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- Publication venue
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- 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
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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
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- 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
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- Zbroszczyk Hanna Paulina
- Zhalov Mikhail
- Zhang Xiaoming
- Zhang Zuman
- Zhao Chengxin
- Zherebchevskii Vladimir
- Zhigareva Natalia
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- 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
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
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- 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
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- Borel Herve
- Borissov Alexander
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- Westerhoff Uwe
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- 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
- Broker Theo Alexander
- Broz Michal
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- Capon Aaron Allan
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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
Jet fragmentation transverse momentum distributions in pp and p-Pb collisions at s, sNN = 5.02 TeV
- Author
- Acharya Shreyasi
- Adamova Dagmar
- Adler Alexander
- Adolfsson Jonatan
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Akbar Zaenal
- Akindinov Alexander
- Al-turany Mohammad
- 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
- Anguelov Venelin
- 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
- Bai Xiaozhi
- Bailhache Raphaelle Marie
- Bala Renu
- Balbino Alessandro
- Baldisseri Alberto
- Ball Markus
- Banerjee Debjani
- Barbera Roberto
- Barioglio Luca
- Barlou Maria
- Barnafoldi Gergely Gabor
- Barnby Lee Stuart
- 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
- Belikov Iouri
- Bell Hechavarria A. D. C.
- Bellini Francesca
- Bellwied Rene
- Belokurova Svetlana
- Belyaev Vladimir
- Bencedi Gyula
- Beole Stefania
- Bercuci Alexandru
- Berdnikov Yaroslav
- Berdnikova Anastasia
- Berenyi Daniel
- Bergmann Luisa
- Besoiu Mihaela Gabriela
- Betev Latchezar
- Bhaduri Partha Pratim
- Bhasin Anju
- Bhat Inayat Rasool
- Bhat Mohammad Asif
- Bhattacharjee Buddhadeb
- Bhattacharya Purba
- Bianchi Antonio
- Bianchi Livio
- Bianchi Nicola
- Bielcik Jaroslav
- Bielcikova Jana
- Bilandzic Ante
- Biro Gabor
- Biswas Saikat
- Blair Justin Thomas
- Blau Dmitry
- Blidaru Mihail Bogdan
- Blume Christoph
- Boca Gianluigi
- Bock Friederike
- Bogdanov Alexey
- Boi Stefano
- Bok Jeongsu
- Boldizsar Laszlo
- Bolozdynya Alexander
- Bombara Marek
- Bonomi Germano
- Borel Herve
- Borissov Alexander
- Bossi Hannah
- Botta Elena
- Bratrud Lars
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- 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 Yifei
- Zherebchevskii Vladimir
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Ya
- Zichichi Antonino
- Zinovjev Gennady
- Zurlo Nicola
- Publication venue
- SISSA
- Publication date
- 10/11/2020
- Field of study
Jet fragmentation transverse momentum (jT) distributions are measured in proton-proton (pp) and proton-lead (p-Pb) collisions at sNN = 5.02 TeV with the ALICE experiment at the LHC. Jets are reconstructed with the ALICE tracking detectors and electromagnetic calorimeter using the anti-kT algorithm with resolution parameter R = 0.4 in the pseudorapidity range |η| < 0.25. The jT values are calculated for charged particles inside a fixed cone with a radius R = 0.4 around the reconstructed jet axis. The measured jT distributions are compared with a variety of parton-shower models. Herwig and Pythia 8 based models describe the data well for the higher jT region, while they underestimate the lower jT region. The jT distributions are further characterised by fitting them with a function composed of an inverse gamma function for higher jT values (called the “wide component”), related to the perturbative component of the fragmentation process, and with a Gaussian for lower jT values (called the “narrow component”), predominantly connected to the hadronisation process. The width of the Gaussian has only a weak dependence on jet transverse momentum, while that of the inverse gamma function increases with increasing jet transverse momentum. For the narrow component, the measured trends are successfully described by all models except for Herwig. For the wide component, Herwig and PYTHIA 8 based models slightly underestimate the data for the higher jet transverse momentum region. These measurements set constraints on models of jet fragmentation and hadronisation
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
- 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
- Baral Rama Chandra
- Barbera Roberto
- Barioglio Luca
- Barnafoldi Gergely Gabor
- Barnby Lee Stuart
- Bartalini Paolo
- Barth Klaus
- Bartsch Esther
- Baruffaldi Filippo
- Bashir Butt Jamila
- Bastid Nicole
- Basu Sumit
- Batigne Guillaume
- Batyunya Boris
- Batzing Paul Christoph
- Bauri Dibakar
- Bautista Guzman Irais
- Bazo Alba Jose Luis
- Bearden Ian Gardner
- Bedda Cristina
- Behera Nirbhay Kumar
- Belikov Iouri
- Bell Hechavarria Ailec de La
- 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
- Blau Dmitry
- Blume Christoph
- Boca Gianluigi
- Bock Friederike
- Bogdanov Alexey
- Boldizsar Laszlo
- Bolozdynya Alexander
- Bombara Marek
- Bonomi Germano
- Borel Herve
- Borissov Alexander
- Borri Marcello
- Bossi Hannah
- Botta Elena
- Bratrud Lars
- Braun-Munzinger Peter
- Bregant Marco
- Broker Theo Alexander
- Broz Michal
- Brucken Jens Erik
- Bruna Elena
- Bruno Giuseppe Eugenio
- Buckland Matthew Daniel
- Budnikov Dmitry
- Buesching Henner
- Bufalino Stefania
- Bugnon Ophelie
- Buhler Paul Alois
- Buncic Predrag
- Buthelezi Edith Zinhle
- Buxton Jesse Thomas
- Bysiak Sebastian Adam
- Caffarri Davide
- Caliva Alberto
- Calvo Villar Ernesto
- Camerini Paolo
- Capon Aaron Allan
- Carnesecchi Francesca
- Caron Robin Albert Andre
- Castillo Castellanos Javier Ernesto
- Castro Andrew John
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- Chang Wan
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- Chattopadhyay Sukalyan
- Chauvin Alex Henri Jean
- Cheshkov Cvetan Valeriev
- Cheynis Brigitte
- Chibante Barroso Vasco Miguel
- Cho Soyeon
- Chochula Peter
- Chowdhury Tasnuva
- Christakoglou Panagiotis
- Christensen Christian Holm
- Christiansen Peter
- Chujo Tatsuya
- Cicalo Corrado
- Cifarelli Luisa
- Cindolo Federico
- Cleymans Jean Willy Andre
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- Colella Domenico
- Collu Alberto
- Colocci Manuel
- Concas Matteo
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- von Haller Barthelemy
- Vorobyev Ivan
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- 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
Measurements of the groomed and ungroomed jet angularities in pp collisions at s = 5.02 TeV
- Author
- Acharya Shreyasi
- Adamova Dagmar
- Adler Alexander
- Aglieri Rinella Gianluca
- Agnello Michelangelo
- Agrawal Neelima
- Ahammed Zubayer
- Ahmad Shakeel
- Ahn Sang Un
- Ahuja Ishaan
- 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
- Antinori Federico
- Antonioli Pietro
- Apadula Nicole
- Aphecetche Laurent Bernard
- Appelshaeuser Harald
- Arcelli Silvia
- Arnaldi Roberta
- Arsene Ionut Cristian
- Arslandok Mesut
- Arteche Diaz Raul
- Augustinus Andre
- Averbeck Ralf Peter
- Aziz Sizar
- Azmi Mohd Danish
- Badala Angela
- Baek Yongwook
- Bai Xiaozhi
- Bailhache Raphaelle Marie
- Bailung Yoshini
- Bala Renu
- Balbino Alessandro
- Baldisseri Alberto
- Balis Bartosz
- Ball Markus
- Banerjee Debjani
- Barbera Roberto
- Barioglio Luca
- Barlou Maria
- Barnafoldi Gergely Gabor
- Barnby Lee Stuart
- Bartels Clara
- Barth Klaus
- Bartsch Esther
- Baruffaldi Filippo
- Bashir Butt Jamila
- Bastid Nicole
- Basu Sumit
- Batigne Guillaume
- Batyunya Boris
- Bauri Dibakar
- Bazo Alba Jose Luis
- Bearden Ian Gardner
- Beattie Caitlin
- Belikov Iouri
- Bell Hechavarria A. D. C.
- Bellini Francesca
- Bellwied Rene
- Belokurova Svetlana
- Belyaev Vladimir
- Bencedi Gyula
- Beole Stefania
- Bercuci Alexandru
- Berdnikov Yaroslav
- Berdnikova Anastasia
- Bergmann Luisa
- Besoiu Mihaela Gabriela
- Betev Latchezar
- Bhaduri Partha Pratim
- Bhasin Anju
- Bhat Inayat Rasool
- Bhat Mohammad Asif
- Bhattacharjee Buddhadeb
- Bhattacharya Purba
- Bianchi Livio
- Bianchi Nicola
- Bielcik Jaroslav
- Bielcikova Jana
- Biernat Jacek
- Bilandzic Ante
- Biro Gabor
- Biswas Saikat
- Blair Justin Thomas
- Blau Dmitry
- Blidaru Mihail Bogdan
- Blume Christoph
- Boca Gianluigi
- Bock Friederike
- Bogdanov Alexey
- Boi Stefano
- Bok Jeongsu
- Boldizsar Laszlo
- Bolozdynya Alexander
- Bombara Marek
- Bond Peter Matthew
- Bonomi Germano
- Borel Herve
- Borissov Alexander
- Bossi Hannah
- Botta Elena
- Bratrud Lars
- Braun-munzinger Peter
- Bregant Marco
- Broz Michal
- Bruno Giuseppe Eugenio
- Buckland Matthew Daniel
- Budnikov Dmitry
- Buesching Henner
- Bufalino Stefania
- Bugnon Ophelie
- Buhler Paul Alois
- Buthelezi Edith Zinhle
- Bysiak Sebastian Adam
- Cai Mengke
- Caines Helen Louise
- Caliva Alberto
- Calvo Villar Ernesto
- Camerini Paolo
- Carnesecchi Francesca
- Caron Robin Albert Andre
- Castillo Castellanos Javier Ernesto
- Casula Ester Anna Rita
- Catalano Fabio
- Ceballos Sanchez Cesar
- Chakraborty Pritam
- Chandra Anuj
- Chandra Sinjini
- Chapeland Sylvain
- Chartier Marielle
- Chattopadhyay Subhasis
- Chattopadhyay Sukalyan
- Chauvin Alex Henri Jean
- Cheng Tiantian
- Cheshkov Cvetan Valeriev
- Cheynis Brigitte
- Chibante Barroso Vasco Miguel
- Cho Soyeon
- Chochula Peter
- Christakoglou Panagiotis
- Christensen Christian Holm
- Christiansen Peter
- Chujo Tatsuya
- Cicalo Corrado
- Cifarelli Luisa
- Cindolo Federico
- Ciupek Michael Rudolf
- Clai Giulia
- Cleymans Jean Willy Andre
- Colamaria Fabio Filippo
- Colburn Jonathan Samuel
- Colella Domenico
- Collu Alberto
- Colocci Manuel
- Concas Matteo
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- Divia Roberto
- Dixit Dhruv Utpalkumar
- Djuvsland Oeystein
- Dmitrieva Uliana
- Do Jaehyeon
- Dobrigkeit Chinellato David
- Dobrin Alexandru Florin
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- Storetvedt Maksim Melnik
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- Vasileiou Maria
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- Vertesi Robert
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- Villalobos Baillie Orlando
- Vino Gioacchino
- Vinogradov Alexander
- Virgili Tiziano
- Vislavicius Vytautas
- Vodopyanov Alexander
- Voelkel Benedikt
- Volkl Martin Andreas
- Voloshin Kirill
- Voloshin Sergey
- Volpe Giacomo
- Von Haller Barthelemy
- Vorobyev Ivan
- Voscek Dominik
- Vozniuk Nikita
- Vrlakova Janka
- Wagner Boris
- Wang Chunzheng
- Wang Dongfang
- Weber Michael
- Wegrzynek Adam Tadeusz
- Wenzel Sandro Christian
- Wessels Johannes Peter
- Wiechula Jens
- Wikne Jon
- Wilk Grzegorz Andrzej
- Wilkinson Jeremy John
- Willems Guido Alexander
- Windelband Bernd Stefan
- Winn Michael Andreas
- Witt William Edward
- Wright Josephina Rae
- Wu Wenya
- Wu Yitao
- Xu Ran
- Yadav Arun Kumar
- 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
- Zaccolo Valentina
- Zaman Ali
- Zampolli Chiara
- Zardoshti Nima
- Zarochentsev Andrey
- Zavada Petr
- Zavyalov Nikolay
- Zhalov Mikhail
- Zhang Biao
- Zhang Song
- Zhang Xiaoming
- Zhang Yifei
- Zherebchevskii Vladimir
- Zhigareva Natalia
- Zhou Daicui
- Zhou You
- Zhu Jianhui
- Zhu Ya
- Zichichi Antonino
- Zinovjev Gennady
- Zurlo Nicola
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 16/07/2021
- Field of study
International audienceThe jet angularities are a class of jet substructure observables which characterize the angular and momentum distribution of particles within jets. These observables are sensitive to momentum scales ranging from perturbative hard scatterings to nonperturbative fragmentation into final-state hadrons. We report measurements of several groomed and ungroomed jet angularities in pp collisions at s = 5.02 TeV with the ALICE detector. Jets are reconstructed using charged particle tracks at midrapidity (|η| < 0.9). The anti-kT algorithm is used with jet resolution parameters R = 0.2 and R = 0.4 for several transverse momentum {p}_{\mathrm{T}}^{\mathrm{ch}} ^{jet} intervals in the 20–100 GeV/c range. Using the jet grooming algorithm Soft Drop, the sensitivity to softer, wide-angle processes, as well as the underlying event, can be reduced in a way which is well-controlled in theoretical calculations. We report the ungroomed jet angularities, λα, and groomed jet angularities, λα,g, to investigate the interplay between perturbative and nonperturbative effects at low jet momenta. Various angular exponent parameters α = 1, 1.5, 2, and 3 are used to systematically vary the sensitivity of the observable to collinear and soft radiation. Results are compared to analytical predictions at next-to-leading-logarithmic accuracy, which provide a generally good description of the data in the perturbative regime but exhibit discrepancies in the nonperturbative regime. Moreover, these measurements serve as a baseline for future ones in heavy-ion collisions by providing new insight into the interplay between perturbative and nonperturbative effects in the angular and momentum substructure of jets. They supply crucial guidance on the selection of jet resolution parameter, jet transverse momentum, and angular scaling variable for jet quenching studies.[graphic not available: see fulltext
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