114 research outputs found
Measurement of prompt J/psi and beauty hadron production cross sections at mid-rapidity in pp collisions at root s=7 TeV
- Author
- ABELEV B
- ADAM J
- ADAMOVA D
- ADARE AM
- AGGARWAL M
- AGOCS AC
- AGOSTINELLI A
- AHAMMED Z
- AHMAD A
- AHMAD N
- AHN SA
- AHN SU
- AKINDINOV A
- ALANIZ EC
- ALEKSANDROV D
- ALESSANDRO B
- ALICI A
- ALKIN A
- ALME J
- ALT T
- ALTINI V
- ALTINPINAR S
- ALTSYBEEV I
- ANDREI C
- ANDRONIC A
- ANGUELOV V
- ANIELSKI J
- ANSON CD
- ANTICIC T
- ANTINORI F
- ANTONIOLI P
- APHECETCHE LB
- APPELSHAUSER H
- ARBOR N
- ARCELLI S
- AREND A
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- ARNALDI R
- ARONSSON TR
- ARSENE IC
- ARSLANDOK M
- ASRYAN A
- AUGUSTINUS A
- AVERBECK RP
- AVINA EJA
- AWES T
- AYSTO JH
- AZMI MD
- BACH MJ
- BADALA A
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- BOCK N
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- BOGDANOV A
- BOGGILD H
- BOGOLYUBSKY M
- BOLDIZSAR L
- BOMBARA M
- BOOK J
- BOREL H
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- YIN ZB
- YOO IK
- YOON J
- YU WL
- YUAN XB
- YUSHMANOV I
- ZACH C
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- ZAPOROZHETS S
- ZAROCHENTSEV A
- ZAVADA P
- ZAVIYALOV N
- ZBROSZCZYK HP
- ZELNICEK P
- ZETINA LMM
- ZGURA SI
- ZHALOV M
- ZHANG HT
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- ZHOU Y
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- ZYNOVYEV M
- ZYZAKBZ M
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2012
- Field of study
The ALICE experiment at the LHC has studied J/psi production at mid-rapidity in pp collisions at root s = 7 TeV through its electron pair decay on a data sample corresponding to an integrated luminosity L-int = 5.6 nb(-1). The fraction of J/psi from the decay of long-lived beauty hadrons was determined for J/psi candidates with transverse momentum p(t) > 1,3 GeV/c and rapidity vertical bar y vertical bar 1.3 GeV/c, vertical bar y vertical bar 1.3 GeV/c and vertical bar y vertical bar 1.3 GeV/c, vertical bar y vertical bar < 0.9) = 1.46 +/- 0.38 (stat.)(-0.32)(+0.26) (syst.) mu b. The results are compared to QCD model predictions. The shape of the p(t) and y distributions of b-quarks predicted by perturbative QCD model calculations are used to extrapolate the measured cross section to derive the b (b) over bar pair total cross section and d sigma/dy at mid-rapidity
Underlying Event measurements in pp collisions at root s=0.9 and 7 TeV with the ALICE experiment at the LHC
- Author
- ABELEV B
- ADAMOVA D
- ADARE AM
- AGGARWAL M
- AGOCS AG
- AGOSTINELLI A
- AHAMMED Z
- AHMAD A
- AHMAD N
- AHN SU
- AKINDINOV A
- ALANIZ EC
- ALEKSANDROV D
- ALESSANDRO B
- ALICI A
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- URCIUOLI GM
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- UYSAL AK
- VAJZER M
- VALA M
- VALLERO S
- VAN DER KOLK N
- VAN LEEUWEN M
- VANNUCCI L
- VARGAS AD
- VARGAS HL
- VARMA R
- VASILEIOU M
- VASILIEV A
- VASQUEZ MAS
- VECHERNIN V
- VELASQUEZ AO
- VELDHOEN M
- VENARUZZO M
- VERCELLIN E
- VERGARA S
- VERNEKOHL DC
- VERNET R
- VERWEIJ M
- VICKOVIC L
- VIESTI G
- VIKHLYANTSEV O
- VILAKAZI Z
- VILLAR EC
- VINOGRADOV A
- VINOGRADOV L
- VINOGRADOV Y
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- VIYOGI Y
- VODOPIANOV A
- VOLOSHIN K
- VOLOSHIN S
- VOLPE G
- VON HALLER B
- VRANIC D
- VREBEKK G
- VRLAKOVA J
- VULPESCU B
- VYUSHIN A
- VYVRE PV
- WAGNER B
- WAGNER V
- WAN RZ
- WANG D
- WANG ML
- WANG YF
- WANG YP
- WATANABE K
- WESSELS J
- WESTERHOFF U
- WIECHULA J
- WIKNE J
- WILDE MR
- WILK A
- WILK GA
- WILLIAMS C
- WINDELBAND BS
- YANG HY
- YANG SM
- YANO S
- YASNOPOLSKY S
- YI J
- YIN ZB
- YOKOYAMA H
- YOO IK
- YOON J
- YU WL
- YUAN XB
- YUSHMANOV I
- ZACH C
- ZAMPOLLI C
- ZAPOROZHETS S
- ZAROCHENTSEV A
- ZAVADA P
- ZAVIYALOV N
- ZBROSZCZYK HP
- ZELNICEK P
- ZETINA LMM
- ZGURA SI
- ZHALOV M
- ZHANG XM
- ZHOU DC
- ZHOU FC
- ZHOU Y
- ZHU XR
- ZICHICHI A
- ZIMMERMANN A
- ZINOVJEV G
- ZOCCARATO YD
- ZYNOVYEV M
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2012
- Field of study
We present measurements of Underlying Event observables in pp collisions at root s = 0 : 9 and 7 TeV. The analysis is performed as a function of the highest charged-particle transverse momentum p(T),L-T in the event. Different regions are defined with respect to the azimuthal direction of the leading (highest transverse momentum) track: Toward, Transverse and Away. The Toward and Away regions collect the fragmentation products of the hardest partonic interaction. The Transverse region is expected to be most sensitive to the Underlying Event activity. The study is performed with charged particles above three different p(T) thresholds: 0.15, 0.5 and 1.0 GeV/c. In the Transverse region we observe an increase in the multiplicity of a factor 2-3 between the lower and higher collision energies, depending on the track p(T) threshold considered. Data are compared to PYTHIA 6.4, PYTHIA 8.1 and PHOJET. On average, all models considered underestimate the multiplicity and summed p(T) in the Transverse region by about 10-30%
Underlying Event measurements in pp collisions at root s=0.9 and 7 TeV with the ALICE experiment at the LHC
- Author
- Abelev B
- Adamova D
- Adare AM
- Aggarwal M
- Agocs AG
- Agostinelli A
- Ahammed Z
- Ahmad A
- Ahmad N
- Ahn SU
- Akindinov A
- Alaniz EC
- Aleksandrov D
- Alessandro B
- Alici A
- Alkin A
- Alt T
- Altini V
- Altinpinar S
- Altsybeev I
- Andrei C
- Andronic A
- Anguelov V
- Anson CD
- Anticic T
- Antinori F
- Antonioli P
- Aphecetche LB
- Appelshauser H
- Arbor N
- Arcelli S
- Arend A
- Armesto N
- Arnaldi R
- Aronsson TR
- Arsene IC
- Arslandok M
- Asryan A
- Augustinus A
- Averbeck RP
- Avina EJA
- Awes T
- Aysto JH
- Azmi MD
- Bach MJ
- Badala A
- Baek YW
- Bailhache RM
- Baillie OV
- Bala R
- Balbastre GC
- Baldisseri A
- Baldit A
- Ban J
- Baral RC
- Barbera R
- Barile F
- Barnafoldi GG
- Barnby LS
- Barret V
- Barroso VMC
- Bartke JG
- Basile M
- Bastid N
- Bathen B
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- Beck H
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- Cavicchioli C
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- Chang B
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- Chiavassa E
- Chinellato D
- Chochula P
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- Chung SU
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- Coccetti F
- Coffin JPM
- Colamaria F
- Colella D
- Constantin P
- Contin G
- Contreras JG
- Cormier TM
- Corral GAH
- Cortese P
- Cosentino MR
- Costa F
- Cotallo ME
- Crescio E
- Crochet P
- Cuautle E
- Cunqueiro L
- D'Erasmo G
- Dainese A
- Dalsgaard HH
- Danu A
- Das D
- Das I
- Das K
- Dash AK
- Dash S
- Davalos AM
- de Barros G
- De Caro A
- de Cataldo G
- de Cuveland J
- De Falco A
- De Godoy DAM
- De Gruttola D
- de Guevara PL
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- De Oliveira EP
- De Pasquale S
- de Rooij RS
- De S
- de Toledo AS
- del Valle ZC
- Delagrange H
- Deloff A
- Demanov V
- Denes E
- Deppman A
- Di Bari D
- Di Giglio C
- Di Liberto S
- Di Mauro A
- Di Nezza P
- Diaz AOC
- Dietel T
- Divia R
- Djuvsland O
- Dobrin AF
- Dobrowolski TA
- Dominguez I
- Don CKK
- Donigus B
- Dordic O
- Driga O
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- Ducroux L
- Dupieux P
- Elia D
- Emschermann DP
- Engel H
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- Estienne MD
- Esumi S
- Evans D
- Eyyubova G
- Fabris D
- Faivre J
- Falchieri D
- Fantoni A
- Fasel M
- Fearick RW
- Fedunov A
- Fehlker D
- Feldkamp L
- Felea D
- Feofilov G
- Ferreiro EG
- Ferretti A
- Ferretti R
- Ferroli RB
- Figiel J
- Figueredo M
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- Vulpescu B
- Vyushin A
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- Wang YP
- Watanabe K
- Wessels J
- Westerhoff U
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- Wikne J
- Wilde MR
- Wilk A
- Wilk GA
- Williams C
- Windelband BS
- Yang HY
- Yang SM
- Yano S
- Yasnopolsky S
- Yi J
- Yin ZB
- Yokoyama H
- Yoo IK
- Yoon J
- Yu WL
- Yuan XB
- Yushmanov I
- Zach C
- Zampolli C
- Zaporozhets S
- Zarochentsev A
- Zavada P
- Zaviyalov N
- Zbroszczyk HP
- Zelnicek P
- Zetina LMM
- Zgura SI
- Zhalov M
- Zhang XM
- Zhou DC
- Zhou FC
- Zhou Y
- Zhu XR
- Zichichi A
- Zimmermann A
- Zinovjev G
- Zoccarato YD
- Zynovyev M
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
We present measurements of Underlying Event observables in pp collisions at root s = 0 : 9 and 7 TeV. The analysis is performed as a function of the highest charged-particle transverse momentum p(T),L-T in the event. Different regions are defined with respect to the azimuthal direction of the leading (highest transverse momentum) track: Toward, Transverse and Away. The Toward and Away regions collect the fragmentation products of the hardest partonic interaction. The Transverse region is expected to be most sensitive to the Underlying Event activity. The study is performed with charged particles above three different p(T) thresholds: 0.15, 0.5 and 1.0 GeV/c. In the Transverse region we observe an increase in the multiplicity of a factor 2-3 between the lower and higher collision energies, depending on the track p(T) threshold considered. Data are compared to PYTHIA 6.4, PYTHIA 8.1 and PHOJET. On average, all models considered underestimate the multiplicity and summed p(T) in the Transverse region by about 10-30%
Underlying Event measurements in pp collisions at root s=0.9 and 7 TeV with the ALICE experiment at the LHC
- Author
- Abelev B
- Adamova D
- Adare AM
- Aggarwal M
- Agocs AG
- Agostinelli A
- Ahammed Z
- Ahmad A
- Ahmad N
- Ahn SU
- Akindinov A
- Alaniz EC
- Aleksandrov D
- Alessandro B
- Alici A
- Alkin A
- Alt T
- Altini V
- Altinpinar S
- Altsybeev I
- Andrei C
- Andronic A
- Anguelov V
- Anson CD
- Anticic T
- Antinori F
- Antonioli P
- Aphecetche LB
- Appelshauser H
- Arbor N
- Arcelli S
- Arend A
- Armesto N
- Arnaldi R
- Aronsson TR
- Arsene IC
- Arslandok M
- Asryan A
- Augustinus A
- Averbeck RP
- Avina EJA
- Awes T
- Aysto JH
- Azmi MD
- Bach MJ
- Badala A
- Baek YW
- Bailhache RM
- Baillie OV
- Bala R
- Balbastre GC
- Baldisseri A
- Baldit A
- Ban J
- Baral RC
- Barbera R
- Barile F
- Barnafoldi GG
- Barnby LS
- Barret V
- Barroso VMC
- Bartke JG
- Basile M
- Bastid N
- Bathen B
- Batigne G
- Batyunya B
- Baumann CH
- Bearden IG
- Beck H
- Belikov I
- Bellini F
- Bellwied R
- Belmont Moreno E
- Beole S
- Berceanu I
- Bercuci A
- Berdnikov Y
- Berenyi D
- Bergmann C
- Berzano D
- Betev L
- Bhasin A
- Bhati AK
- Bianchi L
- Bianchi N
- Bianchin C
- Bielcik J
- Bielcikova J
- Bilandzic A
- Blanco F
- Blanco F
- Blau D
- Blume C
- Boccioli M
- Bock N
- Bogdanov A
- Boggild H
- Bogolyubsky M
- Boldizsar L
- Bombara M
- Book J
- Borel H
- Borissov A
- Bortolin C
- Bose SN
- Bossu F
- Botje M
- Bottger S
- Boyer BA
- Braun Munzinger P
- Bregant M
- Breitner TG
- Broz M
- Brun R
- Bruna E
- Bruno GE
- Budnikov D
- Buesching H
- Bufalino S
- Bugaiev K
- Busch O
- Bustamante RTJ
- Buthelezi EZ
- Caffarri D
- Cahuantzi MR
- Cai X
- Caines HL
- Camerini P
- Carena F
- Carena W
- Carlin NC
- Carminati F
- Caselle M
- Castellanos JEC
- Castro XS
- Casula EAR
- Catanescu V
- Cavicchioli C
- Cepila J
- Cerello P
- Cervantes IAM
- Chang B
- Chapeland S
- Charvet JLF
- Chattopadhyay S
- Chattopadhyay S
- Cherney MG
- Cheshkov C
- Cheynis B
- Chiavassa E
- Chinellato D
- Chochula P
- Chojnacki M
- Christakoglou P
- Christensen CH
- Christiansen P
- Chujo T
- Chung SU
- Cicalo C
- Cifarelli L
- Cindolo F
- Cleymans JWA
- Coccetti F
- Coffin JPM
- Colamaria F
- Colella D
- Constantin P
- Contin G
- Contreras JG
- Cormier TM
- Corral GAH
- Cortese P
- Cosentino MR
- Costa F
- Cotallo ME
- Crescio E
- Crochet P
- Cuautle E
- Cunqueiro L
- D'Erasmo G
- Dainese A
- Dalsgaard HH
- Danu A
- Das D
- Das I
- Das K
- Dash AK
- Dash S
- Davalos AM
- de Barros G
- De Caro A
- de Cataldo G
- de Cuveland J
- DE FALCO ALESSANDRO
- De Godoy DAM
- De Gruttola D
- de Guevara PL
- De Marco N
- De Oliveira EP
- De Pasquale S
- de Rooij RS
- De S
- de Toledo AS
- del Valle ZC
- Delagrange H
- Deloff A
- Demanov V
- Denes E
- Deppman A
- Di Bari D
- Di Giglio C
- Di Liberto S
- Di Mauro A
- Di Nezza P
- Diaz AOC
- Dietel T
- Divia R
- Djuvsland O
- Dobrin AF
- Dobrowolski TA
- Dominguez I
- Don CKK
- Donigus B
- Dordic O
- Driga O
- Dubey AK
- Ducroux L
- Dupieux P
- Elia D
- Emschermann DP
- Engel H
- Erdal HA
- Espagnon B
- Estienne MD
- Esumi S
- Evans D
- Eyyubova G
- Fabris D
- Faivre J
- Falchieri D
- Fantoni A
- Fasel M
- Fearick RW
- Fedunov A
- Fehlker D
- Feldkamp L
- Felea D
- Feofilov G
- Ferreiro EG
- Ferretti A
- Ferretti R
- Ferroli RB
- Figiel J
- Figueredo M
- Filchagin S
- Fini RA
- Finogeev D
- FIONDA FIORELLA MARIA CELESTE
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- Zimmermann A
- Zinovjev G
- Zoccarato YD
- Zynovyev M.
- Publication venue
- Publication date
- 01/01/2012
- Field of study
We present measurements of Underlying Event observables in pp collisions at root s = 0 : 9 and 7 TeV. The analysis is performed as a function of the highest charged-particle transverse momentum p(T),L-T in the event. Different regions are defined with respect to the azimuthal direction of the leading (highest transverse momentum) track: Toward, Transverse and Away. The Toward and Away regions collect the fragmentation products of the hardest partonic interaction. The Transverse region is expected to be most sensitive to the Underlying Event activity. The study is performed with charged particles above three different p(T) thresholds: 0.15, 0.5 and 1.0 GeV/c. In the Transverse region we observe an increase in the multiplicity of a factor 2-3 between the lower and higher collision energies, depending on the track p(T) threshold considered. Data are compared to PYTHIA 6.4, PYTHIA 8.1 and PHOJET. On average, all models considered underestimate the multiplicity and summed p(T) in the Transverse region by about 10-30%
Investigating charm production and fragmentation via azimuthal correlations of prompt D mesons with charged particles in pp collisions at s=13 TeV
- Author
- Acharya Shreyasi
- Adamova Dagmar
- Adler Alexander
- Adolfsson Jonatan
- 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
- 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
- Bylinkin Aleksandr
- 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
- Conesa Balbastre Gustavo
- Conesa Del Valle Zaida
- Contin Giacomo
- Contreras Nuno Jesus Guillermo
- Coquet Maurice Louis
- Cormier Thomas Michael
- Correia Zanoli Henrique Jose
- Cortese Pietro
- Cosentino Mauro Rogerio
- Costa Filippo
- Costanza Susanna
- Crochet Philippe
- Cruz Torres Reynier
- Cuautle Flores Eleazar
- Cui Pengyao
- Cunqueiro Mendez Leticia
- Dainese Andrea
- Danisch Meike Charlotte
- Danu Andrea
- Das Indranil
- Das Prottay
- Das Prottoy
- Das Supriya
- Dash Sadhana
- De Caro Annalisa
- De Cataldo Giacinto
- De Cilladi Lorenzo
- De Cuveland Jan
- De Falco Alessandro
- De Gruttola Daniele
- De Leone Gay Maria Beatriz
- De Marco Nora
- De Martin Chiara
- De Moraes Canedo Fabio
- De Pasquale Salvatore
- De Sudipan
- Deb Suman
- Deja Kamil Rafal
- Dello Stritto Luigi
- Demmich Katharina
- Deng Wenjing
- Dhankher Preeti
- Di Bari Domenico
- Di Mauro Antonio
- Dietel Thomas
- Ding Yanchun
- Divia Roberto
- Dixit Dhruv Utpalkumar
- Djuvsland Oeystein
- Dmitrieva Uliana
- Do Jaehyeon
- Dobrigkeit Chinellato David
- Dobrin Alexandru Florin
- Dominguez Rosas Edgar
- Donigus Benjamin
- Dordic Olja
- Duarte Galvan Carlos
- Dubey Anand Kumar
- Dubla Andrea
- Dudi Sandeep
- Dupieux Pascal
- Dzalaiova Natalia
- Eder Tabea Maria
- Ehlers Iii Raymond James
- Eikeland Viljar Nilsen
- Eisenhut Florian
- Elia Domenico
- Erazmus Barbara Ewa
- Ercolessi Francesca
- Erhardt Filip
- Erokhin Andrey
- Ersdal Magnus Rentsch
- Espagnon Bruno
- Eulisse Giulio
- Evans David
- Evdokimov Sergey
- Fabbietti Laura
- Faggin Mattia
- Faivre Julien
- Fan Feng
- Fantoni Alessandra
- Fasel Markus
- Fecchio Pietro
- Feliciello Alessandro
- Feofilov Grigorii
- Fernandez Tellez Arturo
- Ferrero Andrea
- Ferretti Alessandro
- Feuillard Victor Jose Gaston
- Fierro Rojas Pablo
- Figiel Jan
- Filchagin Sergey
- Finogeev Dmitry
- Fionda Fiorella
- Fiorenza Gabriele
- Fiorini Da Silva Tiago
- Flor Fernando Antonio
- Flores Amanda Nicole
- Foertsch Siegfried Valentin
- Foka Panagiota
- Fokin Sergey
- Fragiacomo Enrico
- Frajna Eszter
- Franz Degenhardt Hermann
- Fuchs Ulrich
- Funicello Nicola
- Furget Christophe
- Furs Artur
- Gaardhoeje Jens Joergen
- Gagliardi Martino
- Gago Medina Alberto Martin
- Gal Arthur Willem Jean
- Gameiro Munhoz Marcelo
- Ganoti Paraskevi
- Garabatos Cuadrado Jose Maria
- Garcia Chavez Tonatiuh
- Garcia Guardiano Gabriel
- Garcia-solis Edmundo Javier
- Garg Kunal
- Gargiulo Corrado
- Garibli Aydan
- Garner K.
- Gasik Piotr Jan
- Gauger Erin Frances
- Gautam Amrit
- Gay Ducati M. B.
- Germain Marie
- Ghosh Premomoy
- Ghosh Sanjay Kumar
- Giacalone Marco
- Gianotti Paola
- Giubellino Paolo
- Giubilato Piero
- Glaenzer Aude Marie Camille
- Glassel Peter
- Goh Daniel Jia Qin
- Gonzalez Hernandez Emma
- Gonzalez Trueba Laura Helena
- Gonzalez Victor
- Gorbunov Sergey
- Gorgon Marek Boguslaw
- Gorlich Lidia Maria
- Gotovac Sven
- Grabski Varlen
- Graczykowski Lukasz Kamil
- Greiner Leo Clifford
- Grelli Alessandro
- Grigoras Costin
- Grigoryan Smbat
- Grigoryev Vladislav
- Gromada Alena
- Grosa Fabrizio
- Grosse-oetringhaus Jan Fiete
- Grosso Raffaele
- Guernane Rachid
- Guilbaud Maxime Rene Joseph
- Gulbrandsen Kristjan Herlache
- Gunji Taku
- Guo Wenda
- Gupta Anik
- Gupta Ramni
- Gyulai Laszlo
- Habib Michael Karim
- Hachiya Shimomura Maya
- Hadjidakis Cynthia Marie
- Halimoglu Gokhan
- Hamagaki Hideki
- Hamar Gergoe
- Hamid Mohammed
- Hannigan Ryan Patrick
- Haque Md Rihan
- Harlenderova A.
- Harris John William
- Harton Austin Vincent
- Hasenbichler Jan Anton
- Hassan Hadi
- Hatzifotiadou Despina
- Hauer Philip
- Havener Laura Brittany
- Heckel Stefan Thomas
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- Varga Zoltan
- Varga-kofarago Monika
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- Vasiliev Andrey
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- Voloshin Sergey
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- Von Haller Barthelemy
- Vorobyev Ivan
- Voscek Dominik
- Vozniuk Nikita
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- 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
- 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
- 10/09/2021
- Field of study
International audienceAngular correlations of heavy-flavour and charged particles in high-energy proton–proton collisions are sensitive to the production mechanisms of heavy quarks and to their fragmentation as well as hadronisation processes. The measurement of the azimuthal-correlation function of prompt D mesons with charged particles in proton–proton collisions at a centre-of-mass energy of s=13 TeV with the ALICE detector is reported, considering D0, D+, and D∗+ mesons in the transverse-momentum interval 30.3 GeV/c and pseudorapidity ∣η∣<0.8. This measurement has an improved precision and provides an extended transverse-momentum coverage compared to previous ALICE measurements at lower energies. The study is also performed as a function of the charged-particle multiplicity, showing no modifications of the correlation function with multiplicity within uncertainties. The properties and the transverse-momentum evolution of the near- and away-side correlation peaks are studied and compared with predictions from various Monte Carlo event generators. Among those considered, PYTHIA8 and POWHEG+PYTHIA8 provide the best description of the measured observables. The obtained results can provide guidance on tuning the generators
Hypertriton production in p–Pb collisions at √sNN = 5.02 TeV
- Author
- Acharya Shreyasi
- Adamová 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
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Mas’ud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Ali Yasir
- Alici Andrea
- Alizadehvandchali Negin
- Alkin Anton
- Alme Johan
- Alt Torsten
- Altenkämper Lucas
- Altsybeev Igor
- Alvarado Garcia Jesús Ricardo
- Anaam Mustafa Naji
- 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
- Badalà Angela
- Baek Yong Wook
- Bai Xiaozhi
- Bailhache Raphaëlle
- Bailung Yoshini
- Bala Renu
- Balbino Alessandro
- Baldisseri Alberto
- Balis Bartosz
- Ball Markus
- Banerjee Debjani
- Barbera Roberto
- Barioglio Luca
- Barlou Maria
- Barnaföldi Gergely Gábor
- 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 José Luis
- Bearden Ian Gardner
- Beattie Caitlin
- Belikov Iouri
- Bell Hechavarria Ailec de la Caridad
- Bellini Francesca
- Bellwied Rene
- Belokurova Svetlana
- Belyaev Vladimir
- Bencédi Gyula
- Beolè 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
- Bielčík Jaroslav
- Bielčíková Jana
- Biernat Jacek
- Bilandzic Ante
- Biro Gabor
- Biswas Saikat
- Blair Justin Thomas
- Blau Dmitry S.
- Blidaru Mihail-Bogdan
- Blume Christoph
- Boca Gianluigi
- Bock Friederike
- Bogdanov Alexey A.
- Boi Stefano
- Bok Jeongsu
- Boldizsar Laszlo
- Bolozdynya Alexander I.
- 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
- Bufalino Stefania
- Bugnon Ophélie
- Buthelezi Edith Zinhle
- Bysiak Sebastian Adam
- Bühler Paul
- Büsching Henner
- Cai Mengke
- Caines Helen Louise
- Caliva Alberto
- Calvo Villar Ernesto
- Camerini Paolo
- Canedo Fabio de Moraes Canedo
- 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
- Chinellato David Dobrigkeit
- Cho Soyeon
- Chochula Peter
- Christakoglou Panagiotis
- Christensen Christian Holm
- Christiansen Peter L.
- Chujo Tatsuya
- Cicalò 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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- Contin Giacomo
- Contreras Nuno Jesus Guillermo
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- Cunqueiro Mendez Leticia
- Cuveland Jan de
- Czeslaw Miskowiec Dariusz
- Dainese Andrea
- Danisch Meike Charlotte
- Danu Andrea
- Das Indranil
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- Das Prottoy
- Das Supriya
- Dash Sadhana
- De Caro Annalisa
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- De Falco Alessandro
- De Gruttola Daniele
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- De Martin Chiara
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- Demmich Katharina
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- Divià Roberto
- Dixit Dhruv Utpalkumar
- Djuvsland Øystein
- Dmitrieva Uliana
- Do Jaehyeon
- Dobrin Alexandru Florin
- Dominguez Rosas Edgar
- Donigus Benjamin
- Dordic Olja
- Doremalen Lennart Vincent Rogier van
- Duarte Galvan Carlos
- Dubey Anand Kumar
- Dubla Andrea
- Ducati Maria Beatriz de Leone Gay
- Ducati Maria Beatriz de Leone Gay
- Dudi Sandeep
- Dupieux Pascal
- Dzalaiova Natalia
- Eder Tabea Maria
- Ehlers Raymond James, III
- Eikeland Viljar Nilsen
- Eisenhut Florian
- Elia Domenico
- Erazmus Barbara Ewa
- Ercolessi Francesca
- Erhardt Filip
- Erokhin Andrey
- Ersdal Magnus Rentsch
- Espagnon Bruno
- Eulisse Giulio
- Evans David
- Evdokimov Sergey
- Fabbietti Laura
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- Wilkinson Jeremy John
- Willems Guido Alexander
- Windelband Bernd
- Winn Michael
- Witt William Edward
- Wright Josephina Rae
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- 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
- Yüncü Alperen
- Zaccolo Valentina
- Zampolli Chiara
- Zardoshti Nima
- Zarochentsev Andrey
- 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 M.
- Zurlo Nicola
- Závada Petr
- Önnerstad Anna
- Šafařík Karel
- Šerkšnytė Laura
- Šuljić Miljenko
- Šumbera Michal
- Publication venue
- Publication date
- 22/07/2021
- Field of study
The study of nuclei and antinuclei production has proven to be a powerful tool to investigate the formation mechanism of loosely bound states in high-energy hadronic collisions. The first measurement of the production of 3ΛH in p-Pb collisions at sNN−−−√ = 5.02 TeV is presented in this Letter. Its production yield measured in the rapidity interval −1<y<0 for the 40% highest multiplicity p-Pb collisions is dN/dy=[6.3±1.8(stat.)±1.2(syst.)]×10−7. The measurement is compared with the expectations of statistical hadronisation and coalescence models, which describe the nucleosynthesis in hadronic collisions. These two models predict very different yields of the hypertriton in charged particle multiplicity environments relevant to small collision systems such as p-Pb and therefore the measurement of dN/dy is crucial to distinguish between them. The precision of this measurement leads to the exclusion with a significance larger than 6.9σ of some configurations of the statistical hadronization model, thus constraining the theory behind the production of loosely bound states at hadron colliders
Measurements of the groomed and ungroomed jet angularities in pp collisions at √s = 5.02 TeV
- Author
- Acharya Shreyasi
- Adamová 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
- Aleksandrov Dmitry
- Alessandro Bruno
- Alfanda Haidar Mas’ud
- Alfaro Molina Jose Ruben
- Ali Bushra
- Ali Yasir
- Alici Andrea
- Alizadehvandchali Negin
- Alkin Anton
- Alme Johan
- Alt Torsten
- Altenkämper Lucas
- Altsybeev Igor
- Alvarado Garcia Jesús Ricardo
- Anaam Mustafa Naji
- Andrei Cristian
- Andreou Dimitra
- Andronic Anton
- Angeletti Massimo
- Anguelov Venelin
- Antinori Federico
- Antonioli Pietro
- Apadula Nicole
- Aphecetche Laurent Bernard
- Appelshäuser Harald
- Arcelli Silvia
- Arnaldi Roberta
- Arsene Ionut Cristian
- Arslandok Mesut
- Arteche Diaz Raul
- Augustinus Andre
- Averbeck Ralf Peter
- Aziz Sizar
- Azmi Mohd Danish
- Badalà Angela
- Baek Yong Wook
- Bai Xiaozhi
- Bailhache Raphaëlle
- Bailung Yoshini
- Bala Renu
- Balbino Alessandro
- Baldisseri Alberto
- Balis Bartosz
- Ball Markus
- Banerjee Debjani
- Barbera Roberto
- Barioglio Luca
- Barlou Maria
- Barnaföldi Gergely Gábor
- 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 José Luis
- Bearden Ian Gardner
- Beattie Caitlin
- Belikov Iouri
- Bell Hechavarria Ailec de la Caridad
- Bellini Francesca
- Bellwied Rene
- Belokurova Svetlana
- Belyaev Vladimir
- Bencédi Gyula
- Beolè 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
- Bielčík Jaroslav
- Bielčíková Jana
- Biernat Jacek
- Bilandzic Ante
- Biro Gabor
- Biswas Saikat
- Blair Justin Thomas
- Blau Dmitry S.
- Blidaru Mihail-Bogdan
- Blume Christoph
- Boca Gianluigi
- Bock Friederike
- Bogdanov Alexey A.
- Boi Stefano
- Bok Jeongsu
- Boldizsar Laszlo
- Bolozdynya Alexander I.
- 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
- Bufalino Stefania
- Bugnon Ophélie
- Buthelezi Edith Zinhle
- Bysiak Sebastian Adam
- Bühler Paul
- Büsching Henner
- Cai Mengke
- Caines Helen Louise
- Caliva Alberto
- Calvo Villar Ernesto
- Camerini Paolo
- Canedo Fabio de Moraes Canedo
- Carnesecchi Francesca
- Caron Robin Albert Andre
- Castillo Castellanos Javier Ernesto
- Casula Ester Anna Rita
- Catalano Fabio
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- Wang Dongfang
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- Weelden Roelof Jan Gijs van
- Wegrzynek Adam Tadeusz
- Wenzel Sandro Christian
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- Wiechula Jens
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- Wilkinson Jeremy John
- Willems Guido Alexander
- Windelband Bernd
- Winn Michael
- Witt William Edward
- Wright Josephina Rae
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- 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
- Yüncü Alperen
- Zaccolo Valentina
- Zaman Ali
- Zampolli Chiara
- Zardoshti Nima
- Zarochentsev Andrey
- 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 M.
- Zurlo Nicola
- Závada Petr
- Önnerstad Anna
- Šafařík Karel
- Šerkšnytė Laura
- Šuljić Miljenko
- Šumbera Michal
- Publication venue
- Publication date
- 23/07/2021
- Field of study
The 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 pch jetT 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
Measurement of K∗(892)± production in inelastic pp collisions at the LHC
- Author
- Acharya Shreyasi
- Adamova Dagmar
- Adler Alexander
- Adolfsson Jonatan
- 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
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- Winn Michael Andreas
- Witt William Edward
- Wright Josephina Rae
- Wu Wenya
- 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
- 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
- 'Elsevier BV'
- Publication date
- 12/05/2021
- Field of study
International audienceThe first results on K⁎(892)± resonance production in inelastic pp collisions at LHC energies of s=5.02, 8, and 13 TeV are presented. The K⁎(892)± has been reconstructed via its hadronic decay channel K⁎(892)→±KS0+π± with the ALICE detector. Measurements of transverse momentum distributions, pT-integrated yields, and mean transverse momenta for charged K⁎(892) are found to be consistent with previous ALICE measurements for neutral K⁎(892) within uncertainties. For pT>1 GeV/c the K⁎(892)± transverse momentum spectra become harder with increasing centre-of-mass energy from 5.02 to 13 TeV, similar to what previously observed for charged kaons and pions. For pT<1 GeV/c the K⁎(892)± yield does not evolve significantly and the abundance of K⁎(892)± relative to K is rather independent of the collision energy. The transverse momentum spectra, measured for K⁎(892)± at midrapidity in the interval 0 <pT<15 GeV/c, are not well described by predictions of different versions of PYTHIA 6, PYTHIA 8 and EPOS-LHC event generators. These generators reproduce the measured pT-integrated K⁎±/K ratios and describe well the momentum dependence for pT<2 GeV/c
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
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- Tersimonov Georgy
- Thakur Sanchari
- Thomas Deepa
- Tieulent Raphael Noel
- Tikhonov Anatoly
- Timmins Anthony Robert
- Tkacik Milan
- Toia Alberica
- Toledo Matuoka Paula Fernanda
- Topilskaya Nataliya
- Toppi Marco
- Torales Acosta Fernando
- Torres Ramos Arianna Grisel
- 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
- Usai Gianluca
- Vala Martin
- Valle Nicolo'
- Vallero Sara
- Van Der Kolk Naomi
- Van Doremalen Lennart
- Van Leeuwen Marco
- Vande Vyvre Pierre
- Varga Dezso
- 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
- Vertesi Robert
- Verweij Marta
- 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
- 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 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
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
- Conesa Balbastre Gustavo
- Conesa Del Valle Zaida
- Contin Giacomo
- Contreras Nuno Jesus Guillermo
- Coquet Maurice Louis
- Cormier Thomas Michael
- Correia Zanoli Henrique Jose
- Cortese Pietro
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- Costanza Susanna
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- Czeslaw Miskowiec Dariusz
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- Das Indranil
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- De Cuveland Jan
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- Djuvsland Oeystein
- Dmitrieva Uliana
- Do Jaehyeon
- Dobrigkeit Chinellato David
- Dobrin Alexandru Florin
- Dominguez Rosas Edgar
- Donigus Benjamin
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- Duarte Galvan Carlos
- Dubey Anand Kumar
- Dubla Andrea
- Dudi Sandeep
- Dupieux Pascal
- Dzalaiova Natalia
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- Ehlers Iii Raymond James
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- Espagnon Bruno
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- Evans David
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- Furget Christophe
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- Gago Medina Alberto Martin
- Gal Arthur Willem Jean
- Gameiro Munhoz Marcelo
- Ganoti Paraskevi
- Garabatos Cuadrado Jose Maria
- Garcia Chavez Tonatiuh
- Garcia Guardiano Gabriel
- Garcia-solis Edmundo Javier
- Garg Kunal
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- Garibli Aydan
- Garner K.
- Gasik Piotr Jan
- Gauger Erin Frances
- Gautam Amrit
- Gay Ducati M. B.
- Germain Marie
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- Ghosh Sanjay Kumar
- Giacalone Marco
- Gianotti Paola
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- Glaenzer Aude Marie Camille
- Glassel Peter
- Goh Daniel Jia Qin
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- Gonzalez Trueba Laura Helena
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- Gorbunov Sergey
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- Gorlich Lidia Maria
- Gotovac Sven
- Grabski Varlen
- Graczykowski Lukasz Kamil
- Greiner Leo Clifford
- Grelli Alessandro
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- Grigoryev Vladislav
- Groettvik Ola Slettevoll
- Gromada Alena
- Grosa Fabrizio
- Grosse-oetringhaus Jan Fiete
- Grosso Raffaele
- Guernane Rachid
- Guilbaud Maxime Rene Joseph
- Gulbrandsen Kristjan Herlache
- Gunji Taku
- Guo Wenda
- Gupta Anik
- Gupta Ramni
- Gyulai Laszlo
- Habib Michael Karim
- Hachiya Shimomura Maya
- Hadjidakis Cynthia Marie
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- Hamagaki Hideki
- Hamar Gergoe
- Hamid Mohammed
- Hannigan Ryan Patrick
- Haque Md Rihan
- Harlenderova A.
- Harris John William
- Harton Austin Vincent
- Hasenbichler Jan Anton
- Hassan Hadi
- Hatzifotiadou Despina
- Hauer Philip
- Havener Laura Brittany
- Hayashi Shinichi
- Heckel Stefan Thomas
- Hellbar Ernst
- Helstrup Haavard
- Herman Tomas
- Herrera Corral Gerardo Antonio
- Herrmann Florian
- Hetland Kristin Fanebust
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- Ilkaev Radiy
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- Janson Thomas
- Jercic Marko
- Jevons Oliver Thomas
- Jonas Florian
- Jones Peter Graham
- Jowett John
- Jung Jerome
- Jung Michael
- Junique Antoine Jean-simon
- Jusko Anton
- Kaewjai Jetnipit
- Kalinak Peter
- Kalweit Alexander Philipp
- Kaplin Vladimir
- Kar Somnath
- Karasu Uysal Ayben
- Karatovic David
- Karavichev Oleg
- Karavicheva Tatiana
- Karczmarczyk Przemyslaw
- Karpechev Evgeny
- Kazantsev Andrey
- Kebschull Udo Wolfgang
- Keidel Ralf
- Keijdener D. L. D.
- Keil Markus
- Ketzer Bernhard Franz
- Khabanova Zhanna
- Khan Ahsan Mehmood
- Khan Mohammed Mohisin
- Khan Shaista
- Khanzadeev Alexei
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- Khatun Anisa
- Khuntia Arvind
- Kileng Bjarte
- Kim Beomkyu
- Kim Chong
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- Kim Jaehyun
- Kim Jinsook
- Kim Jiyoung
- Kim Jungeol
- Kim Junlee
- Kim Minjung
- Kim Se Yong
- Kim Taejun
- Kirsch Stefan
- Kisel Ivan
- Kiselev Sergey
- Kisiel Adam Ryszard
- Kitowski Jacek Pawel
- Klay Jennifer Lynn
- Klein Jochen
- Klein Spencer Robert
- Klein-boesing Christian
- Kleiner Matthias
- Klemenz Thomas
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- Knospe Anders Garritt
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- Kollegger Thorsten Sven
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- Kroesen Martin
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- Read Kenneth Francis
- Redelbach Andreas Ralph
- Redlich Krzysztof
- Rehman Attiq Ur
- Reichelt Patrick Simon
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- Renfordt Rainer Arno Ernst
- Rescakova Z.
- Reygers Klaus Johannes
- Riabov Andrei
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- Richert Tuva Ora Herenui
- Richter Matthias Rudolph
- Riegler Werner
- Riggi Francesco
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- Roeed Ketil
- Roehrich Dieter
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- Samsonov Vladimir
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- Sarkar Nachiketa
- Sarma Pranjal
- Sas Mike Henry Petrus
- Sasikumar Menon Anjaly
- 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
- Schotter Romain
- 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
- Seo Jin Joo
- Serebryakov Dmitry
- Serksnyte Laura
- Sevcenco Adrian
- Shaba Tebogo Joyce
- Shabanov Arseniy
- Shabetai Alexandre
- Shahoyan Ruben
- Shaikh Wadut
- Shangaraev Artem
- Sharma Anjali
- Sharma Himanshu
- Sharma Meenakshi
- Sharma Natasha
- Sharma Sheetal
- Sharma Upasana
- Sheibani Oveis
- Shigaki Kenta
- Shirinkin Sergey
- Shou Qiye
- Sibiryak Yury
- Siddhanta Sabyasachi
- Siemiarczuk Teodor
- Silvermyr David Olle Rickard
- Simonetti Giuseppe
- Singh Bhawani
- Singh Ranbir
- Singh Randhir
- Singh Ravindra
- Singh Vivek
- Singhal Vikas
- Sitar Branislav
- Sitta Mario
- Skaali Bernhard
- Skorodumovs Georgijs
- Slupecki Maciej
- Smirnov Nikolai
- Snellings Raimond
- Soncco Meza Carlos
- Song Jihye
- Songmoolnak Arnon
- Soramel Francesca
- Sorensen Soren Pontoppidan
- Soto Camacho Rabi
- Sputowska Iwona Anna
- Stachel Johanna
- Stan Ionel
- Steffanic Patrick John
- Stiefelmaier Stephan Friedrich
- Stocco Diego
- Storehaug Ida
- Storetvedt Maksim Melnik
- Sugitate Toru
- Suire Christophe Pierre
- Sukhanov Mikhail
- Suljic Miljenko
- Sultanov Rishat
- Sumbera Michal
- Sumberia Vikash
- Sumowidagdo Suharyo
- Swain Sagarika
- Szabo Alexander
- Szarka Imrich
- Tabassam Uzma
- Taghavi Seyed Farid
- Taillepied Guillaume
- Takahashi Jun
- Tambave Ganesh Jagannath
- Tang Siyu
- Tang Zebo
- Tarhini Mohamad
- Tarzila Madalina-gabriela
- Tauro Arturo
- Tejeda Munoz Guillermo
- Telesca Adriana
- Terlizzi Livia
- Terrevoli Cristina
- Tersimonov Georgy
- Thakur Sanchari
- Thomas Deepa
- Tieulent Raphael Noel
- Tikhonov Anatoly
- Timmins Anthony Robert
- Tkacik Milan
- Toia Alberica
- Toledo Matuoka Paula Fernanda
- Topilskaya Nataliya
- Toppi Marco
- Torales Acosta Fernando
- Tork Theraa
- Torres Ramos Arianna Grisel
- Trifiro Antonio
- Tripathy Sushanta
- Tripathy Tulika
- Trogolo Stefano
- Trombetta Giuseppe
- Trubnikov Victor
- Trzaska Wladyslaw Henryk
- Trzcinski Tomasz Piotr
- Trzeciak Barbara Antonina
- Tumkin Alexandr
- Turrisi Rosario
- Tveter Trine Spedstad
- Ullaland Kjetil
- Uras Antonio
- Urioni Marta
- Usai Gianluca
- Vala Martin
- Valle Nicolo'
- Vallero Sara
- Van Der Kolk Naomi
- Van Doremalen Lennart
- Van Leeuwen Marco
- Van Weelden Roelof Jan Gijs
- Vande Vyvre Pierre
- Varga Dezso
- Varga Zoltan
- Varga-kofarago Monika
- Vargas Trevino Aurora Diozcora
- Vasileiou Maria
- Vasiliev Andrey
- Vazquez Doce Oton
- Vazquez Rueda Omar
- Vechernin Vladimir
- Vercellin Ermanno
- Vergara Limon Sergio
- Vermunt Lucas Anne
- Vertesi Robert
- Verweij Marta
- Vickovic Linda
- Vilakazi Zabulon
- 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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