50 research outputs found
The Effect of Inhalation Anaesthetics on Pulmonary Ventilation and Perfusion
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/1982
- Field of study
Volatile Anästhetika und ihr Effekt auf die Atmung
- Author
- A Berkenbosch
- A Fargas-Babjak
- AK Laws
- C Marshall
- CA Hirshmann
- G Hedenstierna
- GM Wyant
- GR Barer
- HF Don
- J Mathers
- J Vaage
- JF McMurtry
- JF Nunn
- JL Benumof
- JL Benumof
- JLB Marin
- L Bjertnaes
- LJ Bjertnaes
- LJ Bjertnaes
- MK Sykes
- MK Sykes
- PR Saxena
- R Dueck
- R Kaur
- R Lundh
- RF Seed
- RL Knill
- RL Knill
- RN Miller
- S Baehrendtz
- SA Glasser
- V Schulte-Sasse
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/1986
- Field of study
Stability of arterial to end-tidal carbon dioxide gradients during postoperative cardiorespiratory support
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Is hypoxic pulmonary vasoconstriction important during single lung ventilation in the lateral decubitus position?
- Author
- A Tucker
- AB Hill
- AB Lewis
- AB Malik
- AGM Campbell
- AJ Carlson
- Alan Sandler
- BE Marshall
- BE Marshall
- Brian Kavanagh
- C Marshall
- G Simonneau
- GJ Redding
- HE Cohn
- HL Motley
- HM Thomas
- I Johansen
- IF McMurtry
- J Mathers
- JL Benumof
- JL Benumof
- JL Benumof
- JL Benumof
- JL Benumof
- JL Benumof
- JLB Marin
- Jonathan Benumof
- JT Reeves
- KI Fuchs
- LJ Bjertnas
- M D’Oliveira
- M Stahlman
- Mark Friedlander
- MJ Bishop
- MK Sykes
- MK Sykes
- N Konietzko
- NF Voelkel
- PS Colley
- PS Colley
- Timothy Winton
- TS Scanlon
- US Euler von
- WB Conover
- WR Furman
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Effect of one-lung ventilation on oxygen delivery in anesthetized dogs with an open thoracic cavity
- Author
- Alfrey DD
- Benumof JL
- Benumof JL
- Benumof JL
- Benumof JL
- Bishop MJ
- Borst HG
- Campbell MJ
- Colley PS
- De Rycke LM
- Denise Corliss
- Domino KB
- Eric Monnet
- Faunt KK
- Faunt KK
- Flacke JW
- Furman WR
- Garcia F
- Glazier JB
- Hirschl RB
- Inomata S
- James S. Gaynor
- Johnson DH
- Kato M
- Kerr JH
- Landreneau RJ
- Lewis RJ
- Lloyd TC
- M. D. Salman
- MacPhail CM
- Marin JLB
- Miriam Riquelme
- Obara H
- Roos A
- Rustomjee T
- Scanlon TS
- Shimizu T
- Simon T. Kudnig
- Tachibana M
- Walker T
- Wang JYY
- Warrell DA
- West JB
- West JB
- West JB
- West JB.
- Yoshida H
- Publication venue
- 'American Veterinary Medical Association (AVMA)'
- Publication date
- Field of study
J/psi Elliptic Flow in Pb-Pb Collisions at root s(NN)=5.02 TeV
- Author
- Acharya S
- Adamova D
- Adolfsson J
- Aggarwal MM
- Agnello M
- Agrawal N
- Ahammed Z
- Ahn SU
- Aiola S
- Akindinov A
- Al-Turany M
- Alam SN
- Alba JLB
- Albuquerque DSD
- Aleksandrov D
- Alessandro B
- Ali Y
- Alici A
- Alkin A
- Alme J
- Alt T
- Altenkamper L
- Altsybeev I
- Andrei C
- Andreou D
- Andrews HA
- Andronic A
- Anguelov V
- Anson C
- Anticic T
- Antinori F
- Antonioli P
- Anwar R
- Aphecetche L
- Appelshauser H
- Arcelli S
- Arnaldi R
- Arnold OW
- Arsene IC
- Arslandok M
- Audurier B
- Augustinus A
- Averbeck R
- Azmi MD
- Badala A
- Baek YW
- Bagnasco S
- Bailhache R
- Baillie OV
- Bala R
- Balbastre GC
- Baldisseri A
- Ball M
- Baral RC
- Barbano AM
- Barbera R
- Barile F
- Barioglio L
- Barnafoldi GG
- Barnby LS
- Barret V
- Barroso VC
- Bartalini P
- Barth K
- Bartsch E
- Bastid N
- Basu S
- Batigne G
- Batyunya B
- Batzing PC
- Bearden IG
- Beck H
- Bedda C
- Behera NK
- Belikov I
- Bellini F
- Bellwied R
- Beltran LGE
- Belyaev V
- Bencedi G
- Beole S
- Bercuci A
- Berdnikov Y
- Berenyi D
- Bertens RA
- Berzano D
- Betev L
- Bhasin A
- Bhat IR
- Bhattacharjee B
- Bhom J
- Bianchi A
- Bianchi L
- Bianchi N
- Bianchin C
- Bielcik J
- Bielcikova J
- Bilandzic A
- Biro G
- Biswas R
- Biswas S
- Blair JT
- Blau D
- Blume C
- Boca G
- Bock F
- Bogdanov A
- Boldizsar L
- Bombara M
- Bonomi G
- Bonora M
- Book J
- Borel H
- Borissov A
- Borri M
- Botta E
- Bourjau C
- Bratrud L
- Braun-Munzinger P
- Bregant M
- Broker TA
- Broz M
- Brucken EJ
- Bruna E
- Bruno GE
- Budnikov D
- Buesching H
- Bufalino S
- Buhler P
- Buitron SAI
- Buncic P
- Busch O
- Bustamante RTJ
- Buthelezi Z
- Butt JB
- Buxton JT
- Cabala J
- Caffarri D
- Cahuantzi MR
- Caines H
- Caliva A
- Camerini P
- Capon AA
- Carena F
- Carena W
- Carnesecchi F
- Castellanos JC
- Castro AJ
- Casula EAR
- Chandra S
- Chang B
- Chang W
- Chapeland S
- Chartier M
- Chattopadhyay S
- Chauvin A
- Cheshkov C
- Cheynis B
- Chinellato DD
- Cho S
- Chochula P
- Chojnacki M
- Choudhury S
- Chowdhury T
- Christakoglou P
- Christensen CH
- Christiansen P
- Chujo T
- Chung SU
- Cicalo C
- Cifarelli L
- Cindolo F
- Cleymans J
- Colamaria F
- Colella D
- Collu A
- Colocci M
- Concas M
- Contreras JG
- Coral DMG
- Corchero MAD
- Cormier TM
- Corral GH
- Cortese P
- Cosentino MR
- Costa F
- Costanza S
- Crkovska J
- Crochet P
- Cuautle E
- Cunqueiro L
- Da Costa HP
- da Luz HN
- Da Silva ACO
- Dahms T
- Dainese A
- Danisch MC
- Danu A
- Das D
- Das I
- Das S
- Dash A
- Dash S
- De Caro A
- de Cataldo G
- de Conti C
- de Cuveland J
- De Falco A
- De Godoy DAM
- De Gruttola D
- De Marco N
- De Oliveira RAN
- De Pasquale S
- De S
- De Souza RD
- Degenhardt HF
- Deisting A
- del Valle ZC
- Deloff A
- Deplano C
- Dhankher P
- Di Bari D
- Di Mauro A
- Di Nezza P
- Di Ruzza B
- Dietel T
- Dillenseger P
- Ding Y
- Divia R
- Djuvsland O
- Dobrin A
- Doce OV
- Donigus B
- Dordic O
- Doremalen LVR
- Dubey AK
- Dubla A
- Ducati MBG
- Ducroux L
- Dudi S
- Duggal AK
- Dukhishyam M
- Dupieux P
- Ehlers RJ
- Elia D
- Endress E
- Engel H
- Epple E
- Erazmus B
- Erhardt F
- Espagnon B
- Eulisse G
- Eum J
- Evans D
- Evdokimov S
- Fabbietti L
- Faivre J
- Fantoni A
- Fasel M
- Feldkamp L
- Feliciello A
- Feofilov G
- Fernandes CL
- Ferreiro EG
- Ferretti A
- Festanti A
- Feuillard VJG
- Figiel J
- Figueredo MAS
- Filchagin S
- Finogeev D
- Fionda FM
- Floris M
- Foertsch S
- Foka P
- Fokin S
- Fragiacomo E
- Francescon A
- Francisco A
- Frankenfeld U
- Fronze GG
- Fuchs U
- Furget C
- Furs A
- Gaardhoje JJ
- Gagliardi M
- Gago AM
- Gajdosova K
- Gallio M
- Galvan CD
- Ganoti P
- Garabatos C
- Garcia GM
- Garcia-Solis E
- Garg K
- Gargiulo C
- Gasik P
- Gauger EF
- Germain M
- Ghosh J
- Ghosh P
- Ghosh SK
- Gianotti P
- Gimenez DD
- Girard MF
- Giubellino P
- Giubilato P
- Gladysz-Dziadus E
- Glassel P
- Gonzalez AS
- Gonzalez V
- Gonzalez-Zamora P
- Gorbunov S
- Gorlich L
- Gotovac S
- Grabski V
- Graczykowski LK
- Graham KL
- Greiner L
- Grelli A
- Grigoras C
- Grigoriev V
- Grigoryan A
- Grigoryan S
- Gronefeld JM
- Grosa F
- Grosse-Oetringhaus JF
- Grosso R
- Guber F
- Guernane R
- Guerzoni B
- Gulbrandsen K
- Gunji T
- Gupta A
- Gupta R
- Guzman IB
- Haake R
- Hadjidakis C
- Hamagaki H
- Hamar G
- Hamon JC
- Haque MR
- Harris JW
- Harton A
- Hassan H
- Hatzifotiadou D
- Hayashi S
- Heckel ST
- Hellbar E
- Helstrup H
- Herghelegiu A
- Hernandez EG
- Herrmann F
- Hess BA
- Hetland KF
- Hillemanns H
- Hills C
- Hippolyte B
- Hohlweger B
- Horak D
- Hornung S
- Hosokawa R
- Hristov P
- Hughes C
- Humanic TJ
- Hussain N
- Hussain T
- Hutter D
- Hwang DS
- Ilkaev R
- Inaba M
- Ippolitov M
- Islam MS
- Ivanov M
- Ivanov V
- Izucheev V
- Jacak B
- Jacazio N
- Jacobs PM
- Jadhav MB
- Jadlovska S
- Jadlovsky J
- Jaelani S
- Jahnke C
- Jakubowska MJ
- Janik MA
- Jayarathna PHSY
- Jena C
- Jercic M
- Jones PG
- Jusko A
- Kalinak P
- Kalweit A
- Kang JH
- Kaplin V
- Kar S
- Karavichev O
- Karavicheva T
- Karayan L
- Karczmarczyk P
- Karpechev E
- Kebschull U
- Keidel R
- Keijdener DLD
- Keil M
- Ketzer B
- Khabanova Z
- Khan MM
- Khan P
- Khan SA
- Khanzadeev A
- Kharlov Y
- Khatun A
- Khuntia A
- Kielbowicz MM
- Kileng B
- Kim B
- Kim D
- Kim DJ
- Kim H
- Kim J
- Kim JS
- Kim M
- Kim S
- Kim T
- Kirsch S
- Kisel I
- Kiselev S
- Kisiel A
- Kiss G
- Klay JL
- Klein C
- Klein J
- Klein-Bosing C
- Klewin S
- Kluge A
- Knichel ML
- Knospe AG
- Kobdaj C
- Kofarago M
- Kohler MK
- Kollegger T
- Kondratiev V
- Kondratyeva N
- Kondratyuk E
- Konevskikh A
- Konyushikhin M
- Kopcik M
- Kour M
- Kouzinopoulos C
- Kovalenko O
- Kovalenko V
- Kowalski M
- Kralik I
- Kravcakova A
- Kreis L
- Krivda M
- Krizek F
- Kryshen E
- Krzewicki M
- Kubera AM
- Kucera V
- Kuhn C
- Kuijer PG
- Kumar A
- Kumar J
- Kumar L
- Kumar S
- Kundu S
- Kurashvili P
- Kurepin A
- Kurepin AB
- Kuryakin A
- Kushpil S
- Kweon MJ
- Kwon Y
- La Pointe SL
- La Rocca P
- Lai YS
- Lakomov I
- Langoy R
- Lapidus K
- Lara C
- Lardeux A
- Lattuca A
- Laudi E
- Lavicka R
- Lea R
- Leardini L
- Lee S
- Lehas F
- Lehner S
- Lehrbach J
- Lemmon RC
- Leogrande E
- Levai P
- Lezama EP
- Li X
- Lien J
- Lietava R
- Lim B
- Limon SV
- Lindal S
- Lindenstruth V
- Lindsay SW
- Lippmann C
- Lisa MA
- Litichevskyi V
- Llope WJ
- Lodato DF
- Loenne PI
- Loginov V
- Loizides C
- Loncar P
- Lopez X
- Lowe A
- Luettig P
- Luhder JR
- Lunardon M
- Luparello G
- Lupi M
- Lutz TH
- Maevskaya A
- Mager M
- Mahmood SM
- Maire A
- Majka RD
- Mal'Kevich D
- Malaev M
- Maldonado IC
- Malinina L
- Malzacher P
- Mamonov A
- Manko V
- Manso F
- Manzari V
- Mao Y
- Marchisone M
- Mares J
- Margagliotti GV
- Margotti A
- Margutti J
- Marin A
- Markert C
- Marquard M
- Martin NA
- Martinengo P
- Martinez HB
- Martinez JAL
- Martinez MI
- Masciocchi S
- Masera M
- Masoni A
- Masson E
- Mastroserio A
- Mathis AM
- Matuoka PFT
- Matyja A
- Mayer C
- Mazer J
- Mazzilli M
- Mazzoni MA
- Meddi F
- Meethaleveedu GK
- Melikyan Y
- Menchaca-Rocha A
- Meninno E
- Meres M
- Mhlanga S
- Miake Y
- Mieskolainen MM
- Mihaylov DL
- Mikhaylov K
- Mischke A
- Mishra AN
- Miskowiec D
- Mitra J
- Mitu CM
- Mohammadi N
- Mohanty AP
- Mohanty B
- Molina RA
- Montero AJR
- Montes E
- Monzon IL
- Morales YC
- Moreno LAP
- Moretto S
- Morreale A
- Morsch A
- Muccifora V
- Mudnic E
- Muhlheim D
- Muhuri S
- Mukherjee M
- Mulligan JD
- Munhoz MG
- Munning K
- Munoz GT
- Munzer RH
- Murakami H
- Murray S
- Musa L
- Musinsky J
- Myers CJ
- Myrcha JW
- Nag D
- Naik B
- Nair R
- Nandi BK
- Nania R
- Nappi E
- Narayan A
- Naru MU
- Nattrass C
- Navarro SR
- Nayak K
- Nayak R
- Nayak TK
- Nazarenko S
- Nellen L
- Nesbo SV
- Ng F
- Nicassio M
- Niculescu M
- Niedziela J
- Nielsen BS
- Nikolaev S
- Nikulin S
- Nikulin V
- Noferini F
- Nomokonov P
- Nooren G
- Noris JCC
- Norman J
- Nyanin A
- Nystrand J
- Oeschler H
- Ohlson A
- Okubo T
- Olah L
- Oleniacz J
- Oliver MH
- Onderwaater J
- Oppedisano C
- Orava R
- Oravec M
- Oskarsson A
- Otwinowski J
- Oyama K
- Pachmayer Y
- Pacik V
- Pagano D
- Paic G
- Palni P
- Pan J
- Pandey AK
- Panebianco S
- Papikyan V
- Pareek P
- Park J
- Parmar S
- Passfeld A
- Pathak SP
- Patra RN
- Paul B
- Pedreira MM
- Pei H
- Peitzmann T
- Peng X
- Pereira LG
- Peresunko D
- Perez JM
- Peskov V
- Pestov Y
- Petracek V
- Petrov V
- Petrovici M
- Petta C
- Pezzi RP
- Piano S
- Pikna M
- Pillot P
- Pimentel LODL
- Pinazza O
- Pinsky L
- Piyarathna DB
- Planinic M
- Pliquett F
- Ploskon M
- Pluta J
- Pochybova S
- Podesta-Lerma PLM
- Poghosyan MG
- Polichtchouk B
- Poljak N
- Poonsawat W
- Pop A
- Poppenborg H
- Porteboeuf-Houssais S
- Pozdniakov V
- Prado CAG
- Prasad SK
- Preghenella R
- Prino F
- Pruneau CA
- Pshenichnov I
- Puccio M
- Punin V
- Putschke J
- Raha S
- Rajput S
- Rak J
- Rakotozafindrabe A
- Ramello L
- Rami F
- Ramirez AG
- Rana DB
- Raniwala R
- Raniwala S
- Rasanen SS
- Rascanu BT
- Rathee D
- Ratza V
- Ravasenga I
- Read KF
- Redlich K
- Rehman A
- Reichelt P
- Reidt F
- Ren X
- Renfordt R
- Reshetin A
- Reygers K
- Riabov V
- Richert T
- Richter M
- Riedler P
- Riegler W
- Riggi F
- Rinella GA
- Ristea C
- Roed K
- Rogochaya E
- Rohr D
- Rohrich D
- Rokita PS
- Ronchetti F
- Rosas ED
- Rosnet P
- Rossi A
- Rotondi A
- Roukoutakis F
- Roy C
- Roy P
- Rueda OV
- Rui R
- Rumyantsev B
- Rustamov A
- Ryabinkin E
- Ryabov Y
- Rybicki A
- Saarinen S
- Sadhu S
- Sadovsky S
- Safarik K
- Saha SK
- Sahlmuller B
- Sahoo B
- Sahoo P
- Sahoo R
- Sahoo S
- Sahu PK
- Saini J
- Sakai S
- Saleh MA
- Salzwedel J
- Sambyal S
- Samsonov V
- Sanchez CC
- Sandoval A
- Sarkar A
- Sarkar D
- Sarkar N
- Sarma P
- Sas MHP
- Scapparone E
- Scarlassara F
- Schaefer B
- Scheid HS
- Schiaua C
- Schicker R
- Schmidt C
- Schmidt HR
- Schmidt M
- Schmidt MO
- Schmidt NV
- Schukraft J
- Schutz Y
- Schwarz K
- Schweda K
- Scioli G
- Scomparin E
- Sefcik M
- Seger JE
- Sekiguchi Y
- Sekihata D
- Selyuzhenkov I
- Senosi K
- Senyukov S
- Serradilla E
- Sett P
- Sevcenco A
- Shabanov A
- Shabetai A
- Shahoyan R
- Shaikh W
- Shangaraev A
- Sharma A
- Sharma M
- Sharma N
- Sheikh AI
- Shigaki K
- Shirinkin S
- Shou Q
- Shtejer K
- Sibiriak Y
- Siddhanta S
- Sielewicz KM
- Siemiarczuk T
- Silaeva S
- Silvermyr D
- Simatovic G
- Simonetti G
- Singaraju R
- Singh R
- Singhal V
- Sinha T
- Sitar B
- Sitta M
- Skaali TB
- Slupecki M
- Smirnov N
- Snellings RJM
- Snellman TW
- Song J
- Song M
- Soramel F
- Sorensen S
- Sozzi F
- Sputowska I
- Stachel J
- Stan I
- Stankus P
- Stenlund E
- Stocco D
- Storetvedt MM
- Strmen P
- Suaide AAP
- Sugitate T
- Suire C
- Suleymanov M
- Suljic M
- Sultanov R
- Sumbera M
- Sumowidagdo S
- Suzuki K
- Swain S
- Szabo A
- Szarka I
- Tabassam U
- Takahashi J
- Tambave GJ
- Tanaka N
- Tarhini M
- Tariq M
- Tarzila MG
- Tauro A
- Telesca A
- Tellez AF
- Tello AV
- Terasaki K
- Terrevoli C
- Teyssier B
- Thakur D
- Thakur S
- Thomas D
- Thoresen F
- Tieulent R
- Tikhonov A
- Timmins AR
- Toia A
- Toppi M
- Torres EL
- Torres SR
- Tripathy S
- Trogolo S
- Trombetta G
- Tropp L
- Trubnikov V
- Trzaska WH
- Trzeciak BA
- Tsuji T
- Tumkin A
- Turrisi R
- Tveter TS
- Ullaland K
- Umaka EN
- Uras A
- Usai GL
- Utrobicic A
- Uysal AK
- Vala M
- Van Der Maarel J
- Van Hoorne JW
- van Leeuwen M
- Vanat T
- Varga D
- Vargas A
- Vargyas M
- Varma R
- Vasileiou M
- Vasiliev A
- Vauthier A
- Vechernin V
- Veen AM
- Velasquez AO
- Velure A
- Vercellin E
- Vernet R
- Vertesi R
- Vickovic L
- Vigolo S
- Viinikainen J
- Vilakazi Z
- Villar EC
- Vinogradov A
- Vinogradov L
- Virgili T
- Vislavicius V
- Vodopyanov A
- Volkl MA
- Voloshin K
- Voloshin SA
- Volpe G
- von Haller B
- Vorobyev I
- Voscek D
- Vranic D
- Vrlakova J
- Vyvre PV
- Wagner B
- Wang H
- Wang M
- Watanabe D
- Watanabe Y
- Weber M
- Weber SG
- Weiser DF
- Wenzel SC
- Wessels JP
- Westerhoff U
- Whitehead AM
- Wiechula J
- Wikne J
- Wilk G
- Wilkinson J
- Willems GA
- Williams MCS
- Willsher E
- Windelband B
- Witt WE
- Xu R
- Yalcin S
- Yamakawa K
- Yang P
- Yano S
- Yin Z
- Yokoyama H
- Yoo IK
- Yoon JH
- Yun E
- Yurchenko V
- Zaccolo V
- Zaman A
- Zampolli C
- Zanoli HJC
- Zardoshti N
- Zarochentsev A
- Zavada P
- Zaviyalov N
- Zbroszczyk H
- Zhalov M
- Zhang C
- Zhang H
- Zhang X
- Zhang Y
- Zhang Z
- Zhao C
- Zhigareva N
- Zhou D
- Zhou Y
- Zhou Z
- Zhu H
- Zhu J
- Zhu Y
- Zichichi A
- Zimmermann MB
- Zinovjev G
- Zmeskal J
- Zou S
- Publication venue
- Publication date
- 01/01/2017
- Field of study
We report a precise measurement of the J/psi elliptic flow in Pb-Pb collisions at root s(NN) = 5.02 TeV with the ALICE detector at the LHC. The J/psi mesons are reconstructed at midrapidity (|y| < 0.9) in the dielectron decay channel and at forward rapidity (2.5 < y < 4.0) in the dimuon channel, both down to zero transverse momentum. At forward rapidity, the elliptic flow v(2) of the J/psi is studied as a function of the transverse momentum and centrality. A positive v(2) is observed in the transverse momentum range 2<p(T)<8GeV/c in the three centrality classes studied and confirms with higher statistics our earlier results at root s(NN) = 2.76 TeV in semicentral collisions. At midrapidity, the J/psi v(2) is investigated as a function of the transverse momentum in semicentral collisions and found to be in agreement with the measurements at forward rapidity. These results are compared to transport model calculations. The comparison supports the idea that at low p(T) the elliptic flow of the J/psi originates from the thermalization of charm quarks in the deconfined medium but suggests that additional mechanisms might be missing in the models
Production of omega mesons in pp collisions at s=7 TeV
- Author
- Acharya S
- Adamova D
- Adler A
- Adolfsson J
- Aggarwal MM
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn SU
- Akindinov A
- Al-Turany M
- Alam SN
- Alba JLB
- Albuquerque DSD
- Aleksandrov D
- Alessandro B
- Alfanda HM
- Ali B
- Ali Y
- Alici A
- Alkin A
- Alme J
- Alt T
- Altenkamper L
- Altsybeev I
- Anaam MN
- Andrei C
- Andreou D
- Andrews HA
- Andronic A
- Angeletti M
- Anguelov V
- Anson C
- Anticic T
- Antinori F
- Antonioli P
- Anwar R
- Apadula N
- Aphecetche L
- Appelshauser H
- Arcelli S
- Arnaldi R
- Arratia M
- Arsene IC
- Arslandok M
- Augustinus A
- Averbeck R
- Aziz S
- Azmi MD
- Badala A
- Baek YW
- Bagnasco S
- Bai X
- Bailhache R
- Baillie OV
- Bala R
- Balbastre GC
- Baldisseri A
- Ball M
- Balouza S
- Barbera R
- Barioglio L
- Barnafoldi GG
- Barnby LS
- Barret V
- Barroso VC
- Bartalini P
- Barth K
- Bartsch E
- Baruffaldi F
- Bastid N
- Basu S
- Batigne G
- Batyunya B
- Bauri D
- Bearden IG
- Bedda C
- Behera NK
- Belikov I
- Bellini F
- Bellwied R
- Belyaev V
- Bencedi G
- Beole S
- Bercuci A
- Berdnikov Y
- Berenyi D
- Bertens RA
- Berzano D
- Besoiu MG
- Betev L
- Bhasin A
- Bhat IR
- Bhat MA
- Bhatt H
- Bhattacharjee B
- Bianchi A
- Bianchi L
- Bianchi N
- Bielcik J
- Bielcikova J
- Bilandzic A
- Biro G
- Biswas R
- Biswas S
- Blair JT
- Blau D
- Blume C
- Boca G
- Bock F
- Bogdanov A
- Boi S
- Boldizsar L
- Bolozdynya A
- Bombara M
- Bonomi G
- Borel H
- Borissov A
- Bossi H
- Botta E
- Bratrud L
- Braun-Munzinger P
- Bregant M
- Broz M
- Brucken J
- Bruna E
- Bruno GE
- Buckland MD
- Budnikov D
- Buesching H
- Bufalino S
- Bugnon O
- Buhler P
- Buncic P
- Buthelezi Z
- Butt JB
- Buxton JT
- Bysiak SA
- Caffarri D
- Cahuantzi MR
- CALIVà A
- Camacho RS
- Camerini P
- Capon AA
- Carnesecchi F
- Caron R
- Castellanos JC
- Castro AJ
- Casula EAR
- Catalano F
- Chakraborty P
- Chandra S
- Chang W
- Chapeland S
- Chartier M
- Chattopadhyay S
- Chattopadhyay S
- Chauvin A
- Cheshkov C
- Cheynis B
- Chinellato DD
- Cho S
- Chochula P
- Chowdhury T
- Christakoglou P
- Christensen CH
- Christiansen P
- Chujo T
- Cicalo C
- Cifarelli L
- Cindolo F
- Cleymans J
- Colamaria F
- Colella D
- Collu A
- Colocci M
- Concas M
- Contin G
- Contreras JG
- Coral DMG
- Cormier TM
- Corral GH
- Cortese P
- Cosentino MR
- Costa F
- Costanza S
- Crochet P
- Cuautle E
- Cui P
- Cunqueiro L
- Da Costa HP
- Da Silva ACO
- Dabrowski D
- Dahms T
- Dainese A
- Damas FPA
- Danisch MC
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- De Caro A
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- De Falco A
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- Degenhardt HF
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- Ersdal MR
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- Zichichi A
- Zimmermann MB
- Zinovjev G
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2020
- Field of study
The invariant differential cross section of inclusive omega (782) meson production at midrapidity (|y| pi+pi-pi 0 decay channel. The measured omega production cross section is compared to various calculations: PYTHIA 8.2 Monash 2013 describes the data, while PYTHIA 8.2 Tune 4C overestimates the data by about 50%. A recent NLO calculation, which includes a model describing the fragmentation of the whole vector-meson nonet, describes the data within uncertainties below 6 GeV/c, while it overestimates the data by up to 50% for higher pT. The omega/pi 0 ratio is in agreement with previous measurements at lower collision energies and the PYTHIA calculations. In addition, the measurement is compatible with transverse mass scaling within the measured pT range and the ratio is constant with C omega/pi 0=0.67 +/- 0.03(stat) +/- 0.04(sys) above a transverse momentum of 2.5 GeV/c
Non-linear flow modes of identified particles in Pb-Pb collisions at root s(NN)=5.02 TeV with the ALICE detector
- Author
- Acharya S
- Acosta FT
- Adamova D
- Adolfsson J
- Aggarwal MM
- Agnello M
- Agrawal N
- Ahammed Z
- Ahn SU
- Aiola S
- Akindinov A
- Al-Turany M
- Alam SN
- Alba JLB
- Albuquerque DSD
- Aleksandrov D
- Alessandro B
- Ali Y
- Alici A
- Alkin A
- Alme J
- Alt T
- Altenkamper L
- Altsybeev I
- Anaam MN
- Andrei C
- Andreou D
- Andrews HA
- Andronic A
- Angeletti M
- Anguelov V
- Anson C
- Anticic T
- Antinori F
- Antonioli P
- Anwar R
- Apadula N
- Aphecetche L
- Appelshauser H
- Arcelli S
- Arnaldi R
- Arnold OW
- Arratia M
- Arsene IC
- Arslandok M
- Augustinus A
- Averbeck R
- Azmi MD
- Badala A
- Baek YW
- Bagnasco S
- Bailhache R
- Baillie OV
- Bala R
- Balbastre GC
- Baldisseri A
- Ball M
- Baral RC
- Barbano AM
- Barbera R
- Barile F
- Barioglio L
- Barnafoldi GG
- Barnby LS
- Barret V
- Barroso VC
- Bartalini P
- Barth K
- Bartsch E
- Bastid N
- Basu S
- Batigne G
- Batyunya B
- Batzing PC
- Bearden IG
- Beck H
- Bedda C
- Behera NK
- Belikov I
- Bellini F
- Bellwied R
- Beltran LGE
- Belyaev V
- Bencedi G
- Beole S
- Bercuci A
- Berdnikov Y
- Berenyi D
- Bertens RA
- Berzano D
- Betev L
- Bhaduri PP
- Bhasin A
- Bhat IR
- Bhatt H
- Bhattacharjee B
- Bhom J
- Bianchi A
- Bianchi L
- Bianchi N
- Bielcik J
- Bielcikova J
- Bilandzic A
- Biro G
- Biswas R
- Biswas S
- Blair JT
- Blau D
- Blume C
- Boca G
- Bock F
- Bogdanov A
- Boldizsar L
- Bombara M
- Bonomi G
- Bonora M
- Borel H
- Borissov A
- Borri M
- Botta E
- Bourjau C
- Bratrud L
- Braun-Munzinger P
- Bregant M
- Broker TA
- Broz M
- Brucken EJ
- Bruna E
- Bruno GE
- Budnikov D
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- Westerhoff U
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- Wilkinson J
- Willems GA
- Williams MCS
- Willsher E
- Windelband B
- Witt WE
- Xu R
- Yalcin S
- Yamakawa K
- Yano S
- Yin Z
- Yokoyama H
- Yoo IK
- Yoon JH
- Yurchenko V
- Zaccolo V
- Zaman A
- Zampolli C
- Zanoli HJC
- Zardoshti N
- Zarochentsev A
- Zavada P
- Zaviyalov N
- Zbroszczyk H
- Zhalov M
- Zhang X
- Zhang Y
- Zhang Z
- Zhao C
- Zherebchevskii V
- Zhigareva N
- Zhou D
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- Zhou Z
- Zhu H
- Zhu J
- Zhu Y
- Zichichi A
- Zimmermann MB
- Zinovjev G
- Zmeskal J
- Zou S
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2019
- Field of study
The non-linear flow modes, v(4,22), v(5,32) and v(6,33) as a function of transverse momentum (p(T)) have been measured for the first time in Pb-Pb collisions at root s(NN) = 5.02 TeV for identified particles, i.e. charged pions, kaons and (anti-)protons. These observables probe the contribution of the second and third initial anisotropy coefficients to the higher order flow harmonics. Interestingly, all the characteristic features observed in previous p(T)-differential as well as p(T)-integrated measurements (e.g. v(2) and v(3)) for various particle species are present in these measurements, i.e. increase of magnitude with increasing centrality percentile, a mass ordering in the low p(T) region and a particle type grouping in the intermediate p(T) region. The results cover 0-1% (ultra-central collisions), 10-20% (mid-central collisions) and 40-50% (mid-peripheral collisions) centrality intervals and allow to test models that attempt to describe initial conditions and the mode-coupling of different harmonics
Measurements of mixed harmonic cumulants in Pb-Pb collisions at root s(NN)=5.02 TeV
- Author
- Acharya S
- Adamova D
- Adler A
- Adolfsson J
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn SU
- Akbar Z
- Akindinov A
- Al-Turany M
- Alba JLB
- Aleksandrov D
- Alessandro B
- Alfanda HM
- Ali B
- Ali Y
- Alici A
- Alizadehvandchali N
- Alkin A
- Alme J
- Alt T
- Altenkamper L
- Altsybeev I
- Anaam MN
- Andrei C
- Andreou D
- Andronic A
- Anguelov V
- Antinori F
- Antonioli P
- Anuj C
- Apadula N
- Aphecetche L
- Appelshauser H
- Arcelli S
- Arnaldi R
- Arsene IC
- Arslandok M
- Augustinus A
- Averbeck R
- Aziz S
- Azmi MD
- Badala A
- Baek YW
- Bai X
- Bailhache R
- Baillie OV
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- Bala R
- Balbastre GC
- Balbino A
- Baldisseri A
- Ball M
- Banerjee D
- Barbera R
- Barioglio L
- Barlou M
- Barnafoldi GG
- Barnby LS
- Barret V
- Barroso VC
- Bartels C
- Barth K
- Bartsch E
- Baruffaldi F
- Bastid N
- Basu S
- Batigne G
- Batyunya B
- Bauri D
- Bearden IG
- Beattie C
- Belikov I
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- Bellwied R
- Belokurova S
- Belyaev V
- Bencedi G
- Beole S
- Bercuci A
- Berdnikov Y
- Berdnikova A
- Berenyi D
- Bergmann L
- Besoiu MG
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- Braun-Munzinger P
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- Bruno GE
- Buckland MD
- Budnikov D
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- Bufalino S
- Bugnon O
- Buhler P
- Buthelezi Z
- Butt JB
- Bysiak SA
- Caffarri D
- Cahuantzi MR
- Cai M
- CALIVà A
- Camacho JMM
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- Camerini P
- Canedo FDM
- Capon AA
- Carnesecchi F
- Caron R
- Castellanos JC
- Casula EAR
- Catalano F
- Chakraborty P
- Chandra S
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- Chauvin A
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- Chinellato DD
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- Christensen CH
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- Cicalo C
- Cifarelli L
- Cindolo F
- Ciupek MR
- Clai G
- Cleymans J
- Colamaria F
- Colburn JS
- Colella D
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- Corral GH
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- Cosentino MR
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- Costanza S
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- Cuautle E
- Cui P
- Cunqueiro L
- Da Costa HP
- Da Silva ACO
- Dainese A
- Damas FPA
- Danisch MC
- Danu A
- Das I
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- De Caro A
- de Cataldo G
- De Cilladi L
- de Cuveland J
- De Falco A
- De Godoy DAM
- De Gruttola D
- De Marco N
- De Martin C
- De Pasquale S
- De S
- Deb S
- Degenhardt HF
- Deja KR
- del Valle ZC
- Dello Stritto L
- Delsanto S
- Deng W
- Dhankher P
- Di Bari D
- Di Mauro A
- Diaz RA
- Dietel T
- Ding Y
- Divia R
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- Djuvsland O
- Dmitrieva U
- Do J
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- Dudi S
- Dukhishyam M
- Dupieux P
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- Ehlers RJ
- Eikeland VN
- Elia D
- Erazmus B
- Ercolessi F
- Erhardt F
- Erokhin A
- Ersdal MR
- Espagnon B
- Eulisse G
- Evans D
- Evdokimov S
- Fabbietti L
- Faggin M
- Faivre J
- Fan F
- Fantoni A
- Fasel M
- Fecchio P
- Feliciello A
- Feofilov G
- Ferrero A
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- Feuillard VJG
- Figiel J
- Filchagin S
- Finogeev D
- Fionda FM
- Fiorenza G
- Flor F
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- Foertsch S
- Foka P
- Fokin S
- Fragiacomo E
- Fuchs U
- Funicello N
- Furget C
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- Gagliardi M
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- Yin Z
- Yokoyama H
- Yoo IK
- Yoon JH
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- Yuncu A
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- Zaman A
- Zampolli C
- Zanoli HJC
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- Zaviyalov N
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- Zichichi A
- Zinovjev G
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- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2021
- Field of study
Correlations between moments of different flow coefficients are measured in Pb-Pb collisions at root s(NN) = 5.02 TeV recorded with the ALICE detector. These new measurements are based on multiparticle mixed harmonic cumulants calculated using charged particles in the pseudorapidity region vertical bar eta vertical bar < 0.8 with the transverse momentum range 0.2 < p(T) < 5.0 GeV/c. The centrality dependence of correlations between two flow coefficients as well as the correlations between three flow coefficients, both in terms of their second moments, are shown. In addition, a collection of mixed harmonic cumulants involving higher moments of v(2) and v(3) is measured for the first time, where the characteristic signature of negative, positive and negative signs of four-, six- and eight-particle cumulants are observed, respectively. The measurements are compared to the hydrodynamic calculations using iEBE-VISHNU with AMPT and TRENTo initial conditions. It is shown that the measurements carried out using the LHC Run 2 data in 2015 have the precision to explore the details of initial-state fluctuations and probe the nonlinear hydrodynamic response of v(2) and v(3) to their corresponding initial anisotropy coefficients epsilon(2) and epsilon(3). These new studies on correlations between three flow coefficients as well as correlations between higher moments of two different flow coefficients will pave the way to tighten constraints on initial-state models and help to extract precise information on the dynamic evolution of the hot and dense matter created in heavy-ion collisions at the LHC. (C) 2021 The Author. Published by Elsevier B.V
Elliptic flow of identified hadrons in small collisional systems measured with ALICE
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- Acharya S
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- Kalweit A
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- Kaplin V
- Kar S
- Karavichev O
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- Karczmarczyk P
- Karpechev E
- Kebschull U
- Keidel R
- Keijdener DLD
- Keil M
- Ketzer B
- Khabanova Z
- Khan AM
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- Khanzadeev A
- Kharlov Y
- Khatun A
- Khuntia A
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- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2019
- Field of study
Recent observations of long-range multi-particle azimuthal correlations in p-Pb and high multiplicity pp collisions provided new insights into collision dynamics and opened a possibility to study collective effects in these small systems. New measurements of p(T)-differential elliptic flow (v(2)) coefficient for inclusive charged hadrons as well as a variety of identified particle species in p-Pb collisions at root s(NN) = 5.02 TeV are presented. The data was collected by ALICE during the LHC Run 2 data taking. Besides high precision measurements of v(2)(P-T) for pi(+/-), K-+/- and p((p) over bar), the first results for K-s(0), Lambda((Lambda) over bar) and phi are shown. In order to eliminate non-flow contamination, a pseudorapidity separation between correlated particles is applied as well as subtraction of remaining non-flow estimate based on a measurement of minimum-bias pp collisions at root s = 13 TeV. Moreover, the reported characteristic mass ordering and approximate number of constituent quarks (NCQ) and transverse kinetic energy (KET) scaling of v(2) allow to test various theoretical models, constrain the initial conditions, and probe the origin of collective behavior in small collision systems