67 research outputs found
First measurement of Ωc0 production in pp collisions at s=13 TeV
- Author
- Acharya S.
- Adamová D.
- Adler A.
- Aglieri Rinella G.
- Agnello M.
- Agrawal N.
- Ahammed Z.
- Ahmad S.
- Ahn S.U.
- Ahuja I.
- Akindinov A.
- Al-Turany M.
- Aleksandrov D.
- Alessandro B.
- Alfanda H.M.
- Alfaro Molina R.
- Ali B.
- Ali Y.
- Alici A.
- Alizadehvandchali N.
- Alkin A.
- Alme J.
- Alocco G.
- Alt T.
- Altsybeev I.
- Anaam M.N.
- Andrei C.
- Andronic A.
- Anguelov V.
- Antinori F.
- Antonioli P.
- Anuj C.
- Apadula N.
- Aphecetche L.
- Appelshäuser H.
- Arata C.
- Arcelli S.
- Arnaldi R.
- Arsene I.C.
- Arslandok M.
- Augustinus A.
- Averbeck R.
- Aziz S.
- Azmi M.D.
- Badalà A.
- Baek Y.W.
- Bai X.
- Bailhache R.
- Bailung Y.
- Bala R.
- Balbino A.
- Baldisseri A.
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- Banerjee D.
- Banoo Z.
- Barbera R.
- Barioglio L.
- Barlou M.
- Barnaföldi G.G.
- Barnby L.S.
- Barret V.
- Barreto L.
- Bartels C.
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- Belyaev V.
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- Wegrzynek A.
- Weiglhofer F.T.
- Wenzel S.C.
- Wessels J.P.
- Weyhmiller S.L.
- Wiechula J.
- Wikne J.
- Wilk G.
- Wilkinson J.
- Willems G.A.
- Windelband B.
- Winn M.
- Wright J.R.
- Wu W.
- Wu Y.
- Xu R.
- Yadav A.
- Yadav A.K.
- Yalcin S.
- Yamaguchi Y.
- Yamakawa K.
- Yang S.
- Yano S.
- Yin Z.
- Yoo I.-K.
- Yoon J.H.
- Yuan S.
- Yuncu A.
- Zaccolo V.
- Zampolli C.
- Zanoli H.J.C.
- Zanone F.
- Zardoshti N.
- Zarochentsev A.
- Zaviyalov N.
- Zhalov M.
- Zhang B.
- Zhang S.
- Zhang X.
- Zhang Y.
- Zhang Z.
- Zhao M.
- Zherebchevskii V.
- Zhi Y.
- Zhigareva N.
- Zhou D.
- Zhou Y.
- Zhu J.
- Zhu Y.
- Zinovjev G.
- Zurlo N.
- Závada P.
- Šafařík K.
- Šerkšnytė L.
- Publication venue
- Elsevier BV
- Publication date
- 10/11/2023
- Field of study
The inclusive production of the charm–strange baryon 0 c is measured for the first time via its hadronic √ decay into −π+ at midrapidity (|y| <0.5) in proton–proton (pp) collisions at the centre-of-mass energy s =13 TeV with the ALICE detector at the LHC. The transverse momentum (pT) differential cross section multiplied by the branching ratio is presented in the interval 2 < pT < 12 GeV/c. The pT dependence of the 0 c-baryon production relative to the prompt D0-meson and to the prompt 0 c-baryon production is compared to various models that take different hadronisation mechanisms into consideration. In the measured pT interval, the ratio of the pT-integrated cross sections of 0 c and prompt + c baryons multiplied by the −π+ branching ratio is found to be larger by a factor of about 20 with a significance of about 4σ when compared to e+e− collisions
Elliptic flow of charged particles at midrapidity relative to the spectator plane in Pb–Pb and Xe–Xe collisions
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- Tieulent R.
- Tikhonov A.
- Timmins A.R.
- Tkacik M.
- Tkacik T.
- Toia A.
- Topilskaya N.
- Toppi M.
- Torales-Acosta F.
- Tork T.
- Torres Ramos A.G.
- Trifiró A.
- Triolo A.S.
- Tripathy S.
- Tripathy T.
- Trogolo S.
- Trubnikov V.
- Trzaska W.H.
- Trzcinski T.P.
- Turrisi R.
- Tveter T.S.
- Ullaland K.
- Ulukutlu B.
- Uras A.
- Urioni M.
- Usai G.L.
- Vala M.
- Valle N.
- Vallero S.
- van Doremalen L.V.R.
- van Leeuwen M.
- van Veen C.A.
- van Weelden R.J.G.
- Vande Vyvre P.
- Varga D.
- Varga Z.
- Varga-Kofarago M.
- Vasileiou M.
- Vasiliev A.
- Vazquez Rueda O.
- Vechernin V.
- Vercellin E.
- Vergara Limón S.
- Vermunt L.
- Verweij M.
- Vickovic L.
- Vilakazi Z.
- Villalobos Baillie O.
- Vino G.
- Vinogradov A.
- Virgili T.
- Vislavicius V.
- Vodopyanov A.
- Volkel B.
- Voloshin K.
- Voloshin S.A.
- Volpe G.
- von Haller B.
- Vorobyev I.
- Vozniuk N.
- Vrláková J.
- Vázquez Doce O.
- Vértesi R.
- Völkl M.A.
- Wagner B.
- Wang C.
- Wang D.
- Weber M.
- Wegrzynek A.
- Weiglhofer F.T.
- Wenzel S.C.
- Wessels J.P.
- Weyhmiller S.L.
- Wiechula J.
- Wikne J.
- Wilk G.
- Wilkinson J.
- Willems G.A.
- Windelband B.
- Winn M.
- Wright J.R.
- Wu W.
- Wu Y.
- Xu R.
- Yadav A.K.
- Yalcin S.
- Yamaguchi Y.
- Yamakawa K.
- Yang S.
- Yano S.
- Yin Z.
- Yoo I.-K.
- Yoon J.H.
- Yuan S.
- Yuncu A.
- Zaccolo V.
- Zampolli C.
- Zanoli H.J.C.
- Zanone F.
- Zardoshti N.
- Zarochentsev A.
- Zaviyalov N.
- Zhalov M.
- Zhang B.
- Zhang S.
- Zhang X.
- Zhang Y.
- Zhao M.
- Zherebchevskii V.
- Zhi Y.
- Zhigareva N.
- Zhou D.
- Zhou Y.
- Zhu J.
- Zhu Y.
- Zinovjev G.
- Zurlo N.
- Závada P.
- Šafařík K.
- Šerkšnytė L.
- Publication venue
- Elsevier BV
- Publication date
- 10/11/2023
- Field of study
Measurements of the elliptic flow coefficient relative to the collision plane defined by the spectator neutrons v2{ SP} in collisions of Pb ions at center-of-mass energy per nucleon–nucleon pair √ 2.76 TeV and Xe ions at √ sNN = sNN =5.44 TeV are reported. The results are presented for charged particles produced at midrapidity as a function of centrality and transverse momentum for the 5–70% and 0.2–6 GeV/c ranges, respectively. The ratio between v2{ SP} and the elliptic flow coefficient relative to the participant plane v2{4}, estimated using four-particle correlations, deviates by up to 20% from unity depending on centrality. This observation differs strongly from the magnitude of the corresponding eccentricity ratios predicted by the TRENTo and the elliptic power models of initial state fluctuations that are tuned to describe the participant plane anisotropies. The differences can be interpreted as a decorrelation of the neutron spectator plane and the reaction plane because of fragmentation of the remnants from the colliding nuclei, which points to an incompleteness of current models describing the initial state fluctuations. A significant transverse momentum dependence of the ratio v2{ SP}/v2{4} is observed in all but the most central collisions, which may help to understand whether momentum anisotropies at low and intermediate transverse momentum have a common origin in initial state f luctuations. The ratios of v2{ SP} and v2{4} to the corresponding initial state eccentricities for Xe–Xe and Pb–Pb collisions at similar initial entropy density show a difference of (7.0 ±0.9)%with an additional variation of +1.8% when including RHIC data in the TRENTo parameter extraction. These observations provide new experimental constraints for viscous effects in the hydrodynamic modeling of the expanding quark–gluon plasma produced in heavy-ion collisions at the LHC
Evaluation of a standardised assay for the measurement of antibodies to double-stranded (native) DNA.
- Author
- Publication venue
- 'BMJ'
- Publication date
- Field of study
The Impact of Investment Readiness on Investor Commitment and Market Accessibility in SMEs
- Author
- Aernoudt R.
- Aernoudt R.
- Aernoudt R.
- Anderson J.C.
- Armstrong S.J.
- Atkin R.
- Atkins M.H.
- Blatt R.
- Blomstermo A.
- Bygrave W.D.
- Bygrave W.D.
- Carriere S.R.
- Chang C.K.N.
- Christensen J. L.
- Christensen J. L.
- Churchill G.A.
- Commission European
- Coveney P.
- de Chernatony L.
- DTI (Department of Trade and Industry)
- EBAN
- Erikson K.
- G Lipper.
- Haines G.H.
- Heydebreck P.
- Howorth C.A.
- Johnstone H.
- Joreskog K.
- Kelly P.
- Keuschnigg C.
- Knyphausen-Aufsess D.
- Lange J.
- Lerner J.
- Lumme A.
- Lumpkin G.T.
- Mason C. M.
- Mason C.M.
- Mason C.M.
- Mason C.M.
- Mason C.M.
- Mason C.M.
- Mattson S.
- McGlue D.
- McGrath R.G.
- Paul S.
- Preston S.L.
- Reynolds P.D.
- Riding A.L.
- Saetre A.S.
- San Jose A.
- Schmid F.
- Sjogren H.
- Sorheim R.
- Tucker J.
- van Osnabrugge M.
- van Osnabrugge M.
- Wetzel W. E.
- Yu J.
- Publication venue
- 'Informa UK Limited'
- Publication date
- Field of study
Aggressive behavior: Genetic and physiological mechanisms
- Author
- A. Buettner
- A. Caspi
- A. Caspi
- A. Holmes
- A. Raab
- A. Takahashi
- A.C. Edwards
- A.D. Stewart
- A.H. Veenema
- A.H. Veenema
- A.L. Pritchard
- A.L. Pritchard
- A.L. Scott
- A.S. Book
- A.T. Leshner
- A.V. Azaryan
- A.V. Goloshchapov
- A.V. Kulikov
- A.V. Val’dman
- B.E. Eleftheriou
- B.S. Abrahams
- C. Mucignat-Caretta
- C. Packer
- C.D. Nichols
- C.H. Southwick
- C.H. Southwick
- D. Auboeuf
- D. Craig
- D. Craig
- D.A. Smagin
- D.C. Blanchard
- D.F. Avgustinovich
- D.K. Belyaev
- D.K. Kim
- D.L. Aylor
- D.L. Murphy
- E.B. Barratt
- E.L. Kinnally
- E.M. Nikulina
- F. Assal
- F. Saudou
- F.W. Albert
- G. Nedic
- G. Parruti
- G.A. Churchill
- G.A. Oortmerssen Van
- G.M. Karere
- H. Wong
- H.C. Dow
- H.G. Brunner
- I. Roy Le
- I.C.G. Weaver
- I.W. Craig
- I.Z. Pliusnina
- I.Z. Plyusnina
- I.Z. Plyusnina
- J. Archer
- J. Archer
- J. Charpentier
- J. Haller
- J. Haller
- J. Kim-Cohen
- J. Lazary
- J. Sallinen
- J. Scholtens
- J.A. Crespo
- J.A. Gogos
- J.D. Gatewood
- J.F. Goldsmith
- J.J. Hudziak
- J.K. Pinsonneault
- J.P. Scott
- J.P. Scott
- J.S. Rao
- K. Lorenz
- K. Malki
- K.A. Miczek
- K.A. Miczek
- K.A. Nolan
- K.A. Pavlov
- K.A. Young
- K.E. Moyer
- K.M.J. Lagerspetz
- K.M.J. Lagerspetz
- L. Lewejohann
- L.A. Fairbanks
- L.V. Devoino
- L.V. Krushinskii
- M. Kotler
- M. Sarchiopone
- M. Wilson
- M.D. Marino
- M.E. Hahn
- M.E. May
- M.K. Selmanoff
- M.L. Filipenko
- M.L. Filipenko
- M.L. Filipenko
- M.L. Filipenko
- M.L. Filipenko
- M.T. Yeh
- M.V. Tenditnik
- N. Chattopadhyay
- N. Provencal
- N. Weder
- N.K. Popova
- N.K. Popova
- N.K. Sandnabba
- N.N. i Kudryavtseva
- N.N. Kudryavtseva
- N.N. Kudryavtseva
- N.N. Kudryavtseva
- N.N. Kudryavtseva
- N.N. Kudryavtseva
- N.N. Kudryavtseva
- N.N. Kudryavtseva
- N.P. Bondar
- O. Cases
- O.T. Eldakar
- P. Hollingworth
- P. Lindenfors
- P. Saetre
- P.F. Brain
- P.F. Brain
- P.F. Ferrari
- P.J. Drent
- P.L. Roubertoux
- P.O. McGowan
- P.V. Guillot
- Q. LaPlant
- R. Bell
- R. Chu
- R. Spangler
- R. Tirindelli
- R.A. Baron
- R.A. Hind
- R.A. Sweet
- R.B. Cairns
- R.D. Ciaranello
- R.D. Strous
- R.F. Benus
- R.G. Beilharz
- R.J. Nelson
- R.J. Nelson
- R.J. Nelson
- R.N. Walsh
- R.R.H. Anholt
- S. Chiavegatto
- S. Hohmann
- S. Kessler
- S. Parmigiani
- S. Tosato
- S.B. Manuck
- S.C. Gammie
- S.C. Gammie
- S.C. Maxson
- S.E. Young
- S.J. Tsai
- T.E. Moffitt
- T.J.H. Chen
- T.K. Newman
- U.A. Boyarskikh
- V.P. Poshivalov
- W.F. Mathes
- W.M. Flier van der
- X. Gonda
- Y. Annen
- Y. Isogai
- Y.Y. Huang
- Publication venue
- 'Pleiades Publishing Ltd'
- Publication date
- Field of study
First measurement of <math><msubsup><mi mathvariant="normal">Λ</mi><mrow><mi>c</mi></mrow><mo>+</mo></msubsup></math> production down to <math><mrow><msub><mi>p</mi><mi>T</mi></msub><mo>=</mo><mn>0</mn></mrow></math> in <math><mrow><mi>p</mi><mi>p</mi></mrow></math> and <math><mi>p</mi></math>-Pb collisions at <math><mrow><msqrt><msub><mi>s</mi><mrow><mi>N</mi><mi>N</mi></mrow></msub></msqrt><mo>=</mo><mn>5.02</mn></mrow></math> TeV
- Author
- Acharya S
- Adamová D
- Adler A
- Aglieri Rinella G
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn S.U
- Ahuja I
- Akindinov A
- Al-Turany M
- Aleksandrov D
- Alessandro B
- Alfanda H.M
- Alfaro Molina R
- Ali B
- Alici A
- Alizadehvandchali N
- Alkin A
- Alme J
- Alocco G
- Alt T
- Altsybeev I
- Anaam M.N
- Andrei C
- Andronic A
- Anguelov V
- Antinori F
- Antonioli P
- Apadula N
- Aphecetche L
- Appelshäuser H
- Arata C
- Arcelli S
- Aresti M
- Arnaldi R
- Arneiro J.G.M.C.A
- Arsene I.C
- Arslandok M
- Augustinus A
- Averbeck R
- Azmi M.D
- Badalà A
- Bae J
- Baek Y.W
- Bai X
- Bailhache R
- Bailung Y
- Balbino A
- Baldisseri A
- Balis B
- Banerjee D
- Banoo Z
- Barbera R
- Barile F
- Barioglio L
- Barlou M
- Barnaföldi G.G
- Barnby L.S
- Barret V
- Barreto L
- Bartels C
- Barth K
- Bartsch E
- Bastid N
- Basu S
- Batigne G
- Battistini D
- Batyunya B
- Bauri D
- Bazo Alba J.L
- Bearden I.G
- Beattie C
- Becht P
- Behera D
- Belikov I
- Bell Hechavarria A.D.C
- Bellini F
- Bellwied R
- Belokurova S
- Belyaev V
- Bencedi G
- Beole S
- Bercuci A
- Berdnikov Y
- Berdnikova A
- Bergmann L
- Besoiu M.G
- Betev L
- Bhaduri P.P
- Bhasin A
- Bhat M.A
- Bhattacharjee B
- Bianchi L
- Bianchi N
- Bielčík J
- Bielčíková J
- Biernat J
- Bigot A.P
- Bilandzic A
- Biro G
- Biswas S
- Bize N
- Blair J.T
- Blau D
- Blidaru M.B
- Bluhme N
- Blume C
- Boca G
- Bock F
- Bodova T
- Bogdanov A
- Boi S
- Bok J
- Boldizsár L
- Bolozdynya A
- Bombara M
- Bond P.M
- Bonomi G
- Borel H
- Borissov A
- Borquez Carcamo A.G
- Bossi H
- Botta E
- Bouziani Y.E.M
- Bratrud L
- Braun-Munzinger P
- Bregant M
- Broz M
- Bruno G.E
- Buckland M.D
- Budnikov D
- Buesching H
- Bufalino S
- Bugnon O
- Buhler P
- Buthelezi Z
- Bysiak S.A
- Cai M
- Caines H
- Caliva A
- Calvo Villar E
- Camacho J.M.M
- Camerini P
- Canedo F.D.M
- Carabas M
- Carballo A.A
- Carnesecchi F
- Caron R
- Carvalho L.A.D
- Castillo Castellanos J
- Catalano F
- Ceballos Sanchez C
- Chakaberia I
- Chakraborty P
- Chandra S
- Chapeland S
- Chartier M
- Chattopadhyay S
- Chattopadhyay S
- Chavez T.G
- Cheng T
- Cheshkov C
- Cheynis B
- Chibante Barroso V
- Chinellato D.D
- Chizzali E.S
- Cho J
- Cho S
- Chochula P
- Christakoglou P
- Christensen C.H
- Christiansen P
- Chujo T
- Ciacco M
- Cicalo C
- Cindolo F
- Ciupek M.R
- Clai G
- Colamaria F
- Colburn J.S
- Colella D
- Colocci M
- Concas M
- Conesa Balbastre G
- Conesa del Valle Z
- Contin G
- Contreras J.G
- Coquet M.L
- Cormier T.M
- Cortese P
- Cosentino M.R
- Costa F
- Costanza S
- Cot C
- Crkovská J
- Crochet P
- Cruz-Torres R
- Cuautle E
- Cui P
- Dainese A
- Danisch M.C
- Danu A
- Das P
- Das P
- Das S
- Dash A.R
- Dash S
- de Caro A
- de Cataldo G
- de Cuveland J
- de Falco A
- de Gruttola D
- de Marco N
- de Martin C
- de Pasquale S
- Deb S
- Debski R.J
- Deja K.R
- del Grande R
- Dello Stritto L
- Deng W
- Dhankher P
- Di Bari D
- Di Mauro A
- Diaz R.A
- Dietel T
- Ding Y
- Divià R
- Dixit D.U
- Djuvsland Ø
- Dmitrieva U
- Dobrin A
- Dubinski J.M
- Dubla A
- Dudi S
- Dupieux P
- Durkac M
- Dzalaiova N
- Dönigus B
- Eder T.M
- Ehlers R.J
- Eikeland V.N
- Eisenhut F
- Elia D
- Erazmus B
- Ercolessi F
- Erhardt F
- Ersdal M.R
- Espagnon B
- Eulisse G
- Evans D
- Evdokimov S
- Fabbietti L
- Faggin M
- Faivre J
- Fan F
- Fan W
- Fantoni A
- Fasel M
- Fecchio P
- Feliciello A
- Feofilov G
- Fernández Téllez A
- Ferrandi L
- Ferrer M.B
- Ferrero A
- Ferrero C
- Ferretti A
- Feuillard V.J.G
- Filova V
- Finogeev D
- Fionda F.M
- Flor F
- Flores A.N
- Foertsch S
- Fokin I
- Fokin S
- Fragiacomo E
- Frajna E
- Fuchs U
- Funicello N
- Furget C
- Furs A
- Fusayasu T
- Gaardhøje J.J
- Gagliardi M
- Gago A.M
- Galvan C.D
- Gangadharan D.R
- Ganoti P
- Garabatos C
- Garcia J.R.A
- Garcia-Solis E
- Garg K
- Gargiulo C
- Garner K
- Gasik P
- Gautam A
- Gay Ducati M.B
- Germain M
- Ghimouz A
- Ghosh C
- Giacalone M
- Giubellino P
- Giubilato P
- Glaenzer A.M.C
- Glimos E
- Glässel P
- Goh D.J.Q
- Gonzalez V
- González-Trueba L.H
- Gorgon M
- Gotovac S
- Grabski V
- Graczykowski L.K
- Grecka E
- Grelli A
- Grigoras C
- Grigoriev V
- Grigoryan S
- Grosa F
- Gross-Bolting S.J
- Grosse-Oetringhaus J.F
- Grosso R
- Grund D
- Guardiano G.G
- Guernane R
- Guilbaud M
- Gulbrandsen K
- Gundem T
- Gunji T
- Guo W
- Gupta A
- Gupta R
- Guzman S.P
- Gyulai L
- Habib M.K
- Hadjidakis C
- Haider F.U
- Hamagaki H
- Hamdi A
- Hamid M
- Han Y
- Hannigan R
- Haque M.R
- Harris J.W
- Harton A
- Hassan H
- Hatzifotiadou D
- Hauer P
- Havener L.B
- Heckel S.T
- Hellbär E
- Helstrup H
- Hemmer M
- Herman T
- Herrera Corral G
- Herrmann F
- Herrmann S
- Hetland K.F
- Heybeck B
- Hillemanns H
- Hills C
- Hippolyte B
- Hoffmann F.W
- Hofman B
- Hohlweger B
- Hong G.H
- Horst M
- Horzyk A
- Hosokawa R
- Hou Y
- Hristov P
- Hughes C
- Huhn P
- Huhta L.M
- Hulse C.V
- Humanic T.J
- Hutson A
- Hutter D
- Iddon J.P
- Ilkaev R
- Ilyas H
- Inaba M
- Innocenti G.M
- Ippolitov M
- Isakov A
- Isidori T
- Islam M.S
- Ivanov M
- Ivanov M
- Ivanov V
- Jablonski M
- Jacak B
- Jacazio N
- Jacobs P.M
- Jadlovska S
- Jadlovsky J
- Jaelani S
- Jaffe L
- Jahnke C
- Jakubowska M.J
- Janik M.A
- Janson T
- Jercic M
- Jia S
- Jimenez A.A.P
- Jonas F
- Jowett J.M
- Jung J
- Jung M
- Junique A
- Jusko A
- Kabus M.J
- Kaewjai J
- Kalinak P
- Kalteyer A.S
- Kalweit A
- Kaplin V
- Karasu Uysal A
- Karatovic D
- Karavichev O
- Karavicheva T
- Karczmarczyk P
- Karpechev E
- Kebschull U
- Keidel R
- Keijdener D.L.D
- Keil M
- Ketzer B
- Khan A.M
- Khan S
- Khanzadeev A
- Kharlov Y
- Khatun A
- Khuntia A
- Kidson M.B
- Kileng B
- Kim B
- Kim C
- Kim D.J
- Kim E.J
- Kim J
- Kim J
- Kim J.S
- Kim M
- Kim S
- Kim T
- Kimura K
- Kirsch S
- Kisel I
- Kiselev S
- Kisiel A
- Kitowski J.P
- Klay J.L
- Klein J
- Klein S
- Klein-Bösing C
- Kleiner M
- Klemenz T
- Kluge A
- Knospe A.G
- Kobdaj C
- Kollegger T
- Kondratyev A
- Kondratyeva N
- Kondratyuk E
- Konig J
- Konigstorfer S.A
- Konopka P.J
- Kornakov G
- Koryciak S.D
- Kotliarov A
- Kovalenko V
- Kowalski M
- Kozhuharov V
- Kravčáková A
- Kreis L
- Krivda M
- Krizek F
- Krizkova Gajdosova K
- Kroesen M
- Krupova D.M
- Kryshen E
- Králik I
- Krüger M
- Kuhn C
- Kuijer P.G
- Kumaoka T
- Kumar D
- Kumar L
- Kumar N
- Kumar S
- Kundu S
- Kurashvili P
- Kurepin A
- Kurepin A.B
- Kuryakin A
- Kushpil S
- Kučera V
- Kvapil J
- Kweon M.J
- Kwon J.Y
- Kwon Y
- La Pointe S.L
- La Rocca P
- Lai Y.S
- Lakrathok A
- Lamanna M
- Langoy R
- Larionov P
- Laudi E
- Lautner L
- Lavicka R
- Lazareva T
- Lea R
- Lee H
- Legras G
- Lehrbach J
- Lemmon R.C
- Lesch M.M
- Lesser E.D
- Lettrich M
- León Monzón I
- Li X
- Li X.L
- Lien J
- Lietava R
- Likmeta I
- Lim B
- Lim S.H
- Lindenstruth V
- Lindner A
- Lippmann C
- Liu A
- Liu D.H
- Liu J
- Lofnes I.M
- Loizides C
- Lokos S
- Lomker J
- Loncar P
- Lopez J.A
- Lopez X
- Lu P
- Luhder J.R
- Lunardon M
- Luparello G
- Lévai P
- López Torres E
- Ma Y.G
- Maevskaya A
- Mager M
- Mahmoud T
- Maire A
- Makariev M.V
- Mal'Kevich D
- Malaev M
- Malfattore G
- Malik N.M
- Malik Q.W
- Malik S.K
- Malinina L
- Mallick D
- Mallick N
- Mandaglio G
- Manko V
- Manso F
- Manzari V
- Mao Y
- Margagliotti G.V
- Margotti A
- Markert C
- Martinengo P
- Martinez J.L
- Martínez García G
- Martínez M.I
- Marín A
- Masciocchi S
- Masera M
- Masoni A
- Massacrier L
- Mastroserio A
- Matonoha O
- Matuoka P.F.T
- Matyja A
- Mayer C
- Mazuecos A.L
- Mazzaschi F
- Mazzilli M
- Mdhluli J.E
- Mechler A.F
- Melikyan Y
- Menchaca-Rocha A
- Meninno E
- Menon A.S
- Meres M
- Mhlanga S
- Miake Y
- Micheletti L
- Migliorin L.C
- Mihaylov D.L
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- Wenzel S.C
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- Weyhmiller S.L
- Wiechula J
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- Wilkinson J
- Willems G.A
- Windelband B
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- Wright J.R
- Wu W
- Wu Y
- Xu R
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- Yadav A.K
- Yalcin S
- Yamaguchi Y
- Yang S
- Yano S
- Yin Z
- Yoo I.-K
- Yoon J.H
- Yuan S
- Yuncu A
- Zaccolo V
- Zampolli C
- Zanone F
- Zardoshti N
- Zarochentsev A
- Zaviyalov N
- Zhalov M
- Zhang B
- Zhang L
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao M
- Zherebchevskii V
- Zhi Y
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- Zugravel S.C
- Zurlo N
- Závada P
- Šafařík K
- Šerkšnytė L
- Publication venue
- HAL CCSD
- Publication date
- 01/01/2023
- Field of study
International audienceThe production of prompt Λc+ baryons has been measured at midrapidity in the transverse momentum interval 0<pT<1 GeV/c for the first time, in pp and p–Pb collisions at a center-of-mass energy per nucleon-nucleon collision sNN=5.02TeV. The measurement was performed in the decay channel Λc+→pKS0 by applying new decay reconstruction techniques using a Kalman-Filter vertexing algorithm and adopting a machine-learning approach for the candidate selection. The pT-integrated Λc+ production cross sections in both collision systems were determined and used along with the measured yields in Pb–Pb collisions to compute the pT-integrated nuclear modification factors RpPb and RAA of Λc+ baryons, which are compared to model calculations that consider nuclear modification of the parton distribution functions. The Λc+/D0 baryon-to-meson yield ratio is reported for pp and p–Pb collisions. Comparisons with models that include modified hadronization processes are presented, and the implications of the results on the understanding of charm hadronization in hadronic collisions are discussed. A significant (3.7σ) modification of the mean transverse momentum of Λc+ baryons is seen in p–Pb collisions with respect to pp collisions, while the pT-integrated Λc+/D0 yield ratio was found to be consistent between the two collision systems within the uncertainties
Accessing the strong interaction between Λ baryons and charged kaons with the femtoscopy technique at the LHC
- Author
- A. Adler
- A. Akindinov
- A. Alici
- A. Alkin
- A. Andronic
- A. Augustinus
- A. Badalà
- A. Balbino
- A. Baldisseri
- A. Bercuci
- A. Berdnikova
- A. Bhasin
- A. Bilandzic
- A. Bogdanov
- A. Borissov
- A. Bylinkin
- A. Caliva
- A. Dainese
- A. Danu
- A. De Caro
- A. De Falco
- A. Di Mauro
- A. Dobrin
- A. Dubla
- A. Fantoni
- A. Feliciello
- A. Fernández Téllez
- A. Ferrero
- A. Ferretti
- A. Furs
- A. Gautam
- A. Ghimouz
- A. Grelli
- A. Gupta
- A. Hamdi
- A. Harton
- A. Horzyk
- A. Hutson
- A. Isakov
- A. Junique
- A. Jusko
- A. Kalweit
- A. Karasu Uysal
- A. Khanzadeev
- A. Khatun
- A. Khuntia
- A. Kisiel
- A. Kluge
- A. Kondratyev
- A. Kotliarov
- A. Kravčáková
- A. Kurepin
- A. Kuryakin
- A. Lakrathok
- A. Lindner
- A. Liu
- A. Maire
- A. Margotti
- A. Marín
- A. Masoni
- A. Mastroserio
- A. Matyja
- A. Menchaca-Rocha
- A. Modak
- A. Morsch
- A. Mulliri
- A. Nath
- A. Neagu
- A. Negru
- A. Nyanin
- A. Ohlson
- A. Onnerstad
- A. Ortiz Velasquez
- A. Palasciano
- A. Pop
- A. Rakotozafindrabe
- A. Rehman
- A. Riabov
- A. Rosano
- A. Rossi
- A. Roy
- A. Rustamov
- A. Rybicki
- A. Schmah
- A. Schröter
- A. Sevcenco
- A. Shabetai
- A. Shangaraev
- A. Sharma
- A. Shatat
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- A. Tauro
- A. Telesca
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- A. Trifiró
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- X. Zhang
- X.L. Li
- Y. Bailung
- Y. Berdnikov
- Y. Ding
- Y. Han
- Y. Hou
- Y. Kamiya
- Y. Kharlov
- Y. Kwon
- Y. Mao
- Y. Melikyan
- Y. Miake
- Y. Pachmayer
- Y. Patley
- Y. Pestov
- Y. Ryabov
- Y. Sekiguchi
- Y. Sibiriak
- Y. Wang
- Y. Wang
- Y. Wu
- Y. Yamaguchi
- Y. Zhang
- Y. Zhi
- Y. Zhou
- Y. Zhu
- Y.E.M. Bouziani
- Y.G. Ma
- Y.W. Baek
- Z. Ahammed
- Z. Banoo
- Z. Buthelezi
- Z. Conesa del Valle
- Z. Moravcova
- Z. Pugelova
- Z. Rescakova
- Z. Tang
- Z. Varga
- Z. Vilakazi
- Z. Yin
- Z. Zhang
- Ø. Djuvsland
- Publication venue
- Elsevier
- Publication date
- 01/10/2023
- Field of study
The interaction between Λ baryons and kaons/antikaons is a crucial ingredient for the strangeness S=0 and S=−2 sector of the meson–baryon interaction at low energies. In particular, the ΛK‾ might help in understanding the origin of states such as the Ξ(1620), whose nature and properties are still under debate. Experimental data on Λ–K and Λ–K‾ systems are scarce, leading to large uncertainties and tension between the available theoretical predictions constrained by such data. In this Letter we present the measurements of Λ–K⊕+Λ‾–K− and Λ–K⊕−Λ‾–K+ correlations obtained in the high-multiplicity triggered data sample in pp collisions at s=13 TeV recorded by ALICE at the LHC. The correlation function for both pairs is modeled using the Lednický–Lyuboshits analytical formula and the corresponding scattering parameters are extracted. The Λ–K⊕−Λ‾–K+ correlations show the presence of several structures at relative momenta k⁎ above 200 MeV/c, compatible with the Ω baryon, the Ξ(1690), and Ξ(1820) resonances decaying into Λ–K− pairs. The low k⁎ region in the Λ–K⊕−Λ‾–K+ also exhibits the presence of the Ξ(1620) state, expected to strongly couple to the measured pair. The presented data allow to access the ΛK+ and ΛK− strong interaction with an unprecedented precision and deliver the first experimental observation of the Ξ(1620) decaying into ΛK−
Production of pions, kaons, and protons as a function of the relative transverse activity classifier in pp collisions at s = 13 TeV
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2023
- Field of study
International audienceThe production of π±, K±, and (p)p is measured in pp collisions at s = 13 TeV in different topological regions of the events. Particle transverse momentum (pT) spectra are measured in the “toward”, “transverse”, and “away” angular regions defined with respect to the direction of the leading particle in the event. While the toward and away regions contain the fragmentation products of the near-side and away-side jets, respectively, the transverse region is dominated by particles from the Underlying Event (UE). The relative transverse activity classifier, RT = NT/〈NT〉, is used to group events according to their UE activity, where NT is the measured charged-particle multiplicity per event in the transverse region and 〈NT〉 is the mean value over all the analysed events. The first measurements of identified particle pT spectra as a function of RT in the three topological regions are reported. It is found that the yield of high transverse momentum particles relative to the RT-integrated measurement decreases with increasing RT in both the toward and the away regions, indicating that the softer UE dominates particle production as RT increases and validating that RT can be used to control the magnitude of the UE. Conversely, the spectral shapes in the transverse region harden significantly with increasing RT. This hardening follows a mass ordering, being more significant for heavier particles. Finally, it is observed that the pT-differential particle ratios \left(\textrm{p}+\overline{\textrm{p}}\right)/\left({\uppi}^{+}+{\uppi}^{-}\right) and (K+ + K−)/(π+ + π−) in the low UE limit (RT → 0) approach expectations from Monte Carlo generators such as PYTHIA 8 with Monash 2013 tune and EPOS LHC, where the jet-fragmentation models have been tuned to reproduce e+e− results.[graphic not available: see fulltext
Anisotropic flow and flow fluctuations of identified hadrons in Pb–Pb collisions at sNN = 5.02 TeV
- Author
- Acharya S
- Adamová D
- Adler A
- Aglieri Rinella G
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn S.U
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- Yin Z
- Yoo I.K
- Yoon J.H
- Yuan S
- Yuncu A
- Zaccolo V
- Zampolli C
- Zanoli H.J. C
- Zanone F
- Zardoshti N
- Zarochentsev A
- Zaviyalov N
- Zhalov M
- Zhang B
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao M
- Zherebchevskii V
- Zhi Y
- Zhigareva N
- Zhou D
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- Zhu J
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- Zinovjev G
- Zurlo N
- Závada P
- Šafařík K
- Šerkšnytė L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2023
- Field of study
International audienceThe first measurements of elliptic flow of π±, K±, p+p, KS0, Λ+Λ, ϕ, Ξ−+Ξ+, and Ω−+Ω+ using multiparticle cumulants in Pb–Pb collisions at sNN = 5.02 TeV are resented. Results obtained with two- (v2{2}) and four-particle cumulants (v2{4}) are shown as a function of transverse momentum, pT, for various collision centrality intervals. Combining the data for both v2{2} and v2{4} also allows us to report the first measurements of the mean elliptic flow, elliptic flow fluctuations, and relative elliptic flow fluctuations for various hadron species. These observables probe the event-by-event eccentricity fluctuations in the initial state and the contributions from the dynamic evolution of the expanding quark–gluon plasma. The characteristic features observed in previous pT-differential anisotropic flow measurements for identified hadrons with two-particle correlations, namely the mass ordering at low pT and the approximate scaling with the number of constituent quarks at intermediate pT, are similarly present in the four-particle correlations and the combinations of v2{2} and v2{4}. In addition, a particle species dependence of flow fluctuations is observed that could indicate a significant contribution from final state hadronic interactions. The comparison between experimental measurements and CoLBT model calculations, which combine the various physics processes of hydrodynamics, quark coalescence, and jet fragmentation, illustrates their importance over a wide pT range.[graphic not available: see fulltext
Pseudorapidity densities of charged particles with transverse momentum thresholds in pp collisions at <math display="inline"><mrow><msqrt><mrow><mi>s</mi></mrow></msqrt><mo>=</mo><mn>5.02</mn></mrow></math> and 13 TeV
- Author
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- Adamová D
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- Wu W
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- Yalcin S
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- Yoon J.H
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- Yuncu A
- Zaccolo V
- Zampolli C
- Zanone F
- Zardoshti N
- Zarochentsev A
- Zaviyalov N
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- Zherebchevskii V
- Zhi Y
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- Zugravel S.C
- Zurlo N
- Závada P
- Šafařík K
- Šerkšnytė L
- Publication venue
- HAL CCSD
- Publication date
- 01/01/2023
- Field of study
International audienceThe pseudorapidity density of charged particles with minimum transverse momentum (pT) thresholds of 0.15, 0.5, 1, and 2 GeV/c is measured in pp collisions at the center of mass energies of s=5.02 and 13 TeV with the ALICE detector. The study is carried out for inelastic collisions with at least one primary charged particle having a pseudorapidity (η) within ±0.8 and pT larger than the corresponding threshold. In addition, measurements without pT-thresholds are performed for inelastic and nonsingle-diffractive events as well as for inelastic events with at least one charged particle having |η|<1 in pp collisions at s=5.02 TeV for the first time at the LHC. These measurements are compared to the pythia 6, pythia 8, and epos-lhc models. In general, the models describe the η dependence of particle production well. However, discrepancies are observed for the highest transverse momentum threshold (pT>2 GeV/c), highlighting the importance of such measurements for tuning event generators. The new measurements agree within uncertainties with results from the ATLAS and CMS experiments obtained at s=13 TeV
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