159 research outputs found
First measurement of the |t|-dependence of coherent J/Ï photonuclear production
- Author
- Acharya S
- Acosta FT
- Adam J
- Adamova D
- Adler A
- Adolfsson J
- Aggarwal MM
- Agnello M
- Agrawal N
- Ahammed Z
- Ahn SU
- Aiola S
- Akindinov A
- Al-Turany M
- Alam SN
- Albuquerque DSD
- Aleksandrov D
- Alessandro B
- Alfanda HM
- Alfaro Molina R
- 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
- Appelshaeuser H
- Arcelli S
- Arnaldi R
- Arratia M
- Arsene IC
- Arslandok M
- Augustinus A
- Averbeck R
- Azmi MD
- Badala A
- Baek YW
- Bagnasco S
- Bailhache R
- Baillie O Villalobos
- Bala R
- Balbastre G Conesa
- Baldisseri A
- Ball M
- Baral RC
- Barbano AM
- Barbera R
- Barile F
- Barioglio L
- Barnafoeldi GG
- Barnby LS
- Barret V
- Barroso V Chibante
- Bartalini P
- Barth K
- Bartsch E
- Bastid N
- Basu S
- Batigne G
- Batyunya B
- Batzing PC
- Bazo Alba JL
- Bearden IG
- Beck H
- Bedda C
- Behera NK
- Belikov I
- Bellini F
- Bello Martinez H
- 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
- Bolozdynya A
- 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
- Buesching H
- Bufalino S
- Buhler P
- Buncic P
- Busch O
- Bustamante RT Jimenez
- Buthelezi Z
- Butt JB
- Buxton JT
- Cabala J
- Caffarri D
- Caines H
- Caliva A
- Calvo Villar E
- Camacho RS
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- Capon AA
- Carena W
- Carnesecchi F
- Castellanos J Castillo
- Castro AJ
- Casula EAR
- Ceballos Sanchez C
- Chandra S
- Chang B
- Chang W
- Chapeland S
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- Chauvin A
- Cheshkov C
- Cheynis B
- Chinellato DD
- Cho S
- Chochula P
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- Christakoglou P
- Christensen CH
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- Chung SU
- Cicalo C
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- Cosentino MR
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- Crkovska J
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- Da Costa H Pereira
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- del Valle Z Conesa
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- Feofilov G
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- Finogeev D
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- Uysal A Karasu
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- Willems GA
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- Willsher E
- Windelband B
- Witt WE
- Xu R
- Yalcin S
- Yamakawa K
- Yano S
- Yin Z
- Yokoyama H
- Yoo I-K
- Yoon JH
- Yuan S
- 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
- Zhou Y
- Zhou Z
- Zhu H
- Zhu J
- Zhu Y
- Zichichi A
- Zimmermann MB
- Zinovjev G
- Zmeskal J
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2021
- Field of study
The first measurement of the cross section for coherent J/Ï photoproduction as a function of |t|, the square of the momentum transferred between the incoming and outgoing target nucleus, is presented. The data were measured with the ALICE detector in ultra-peripheral PbâPb collisions at a centre-of-mass energy per nucleon pair sNN=5.02TeV with the J/Ï produced in the central rapidity region |y|<0.8, which corresponds to the small Bjorken-x range (0.3â1.4)Ă10â3.
The measured |t|-dependence is not described by computations based only on the Pb nuclear form factor, while the photonuclear cross section is better reproduced by models including shadowing according to the leading-twist approximation, or gluon-saturation effects from the impact-parameter dependent BalitskyâKovchegov equation. These new results are therefore a valid tool to constrain the relevant model parameters and to investigate the transverse gluonic structure at very low Bjorken-x.publishedVersio
Resolving the strange behavior of extraterrestrial potassium in the upper atmosphere
- 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 JL
- 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
- APPELSHAEUSER 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
- BARI D
- 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
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- DA LUZ H
- DA SILVA AC
- DAHMS T
- DAINESE A
- DANI S
- DANISCH MC
- DANU A
- DAS D
- DAS I
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- DASH A
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- DE S
- DEGENHARDT HF
- DEISTING A
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- HARTON A
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- HAYASHI S
- HECKEL ST
- HELLBAER E
- HELSTRUP H
- HERGHELEGIU A
- HERNANDEZ EG
- HERRMANN F
- HETLAND KF
- HILDEN TE
- HILLEMANNS H
- HILLS C
- HIPPOLYTE B
- HOHLWEGER B
- HOORNE JW
- HORAK D
- HORNUNG S
- HOSOKAWA R
- HOTA J
- HRISTOV P
- HUANG C
- HUGHES C
- HUHN P
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- HUSHNUD H
- HUSSAIN N
- HUSSAIN T
- HUTTER D
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- 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
- JENA C
- JERCIC M
- JEVONS O
- JIN M
- JONES PG
- JUSKO A
- KALINAK P
- KALWEIT A
- KANG JH
- KAPLIN V
- KAR S
- KARAVICHEV O
- KARAVICHEVA T
- KARCZMARCZYK P
- KARPECHEV E
- KEBSCHULL U
- KEIDEL R
- KEIJDENER DLD
- KEIL M
- KETZER B
- KHABANOVA Z
- KHAN AM
- KHAN MM
- KHAN S
- KHAN SA
- KHANZADEEV A
- KHARLOV Y
- KHATUN A
- KHUNTIA A
- KIELBOWICZ MM
- KILENG B
- KIM B
- KIM D
- KIM DJ
- KIM EJ
- KIM H
- KIM J
- KIM JS
- KIM M
- KIM S
- KIM T
- KIM T
- KIRSCH S
- KISEL I
- KISELEV S
- KISIEL A
- KLAY JL
- KLEIN C
- KLEIN J
- KLEIN-BOESING C
- KLEWIN S
- KLUGE A
- KNICHEL ML
- KNOSPE AG
- KOBDAJ C
- KOEHLER MK
- KOFARAGO M
- KOLLEGGER T
- KONDRATYEVA N
- KONDRATYUK E
- KONEVSKIKH A
- KONYUSHIKHIN M
- KOVALENKO O
- KOVALENKO V
- KOWALSKI M
- KRALIK I
- KRAVCAKOVA A
- KREIS L
- KRIVDA M
- KRIZEK F
- KRUEGER M
- KRYSHEN E
- KRZEWICKI M
- KUBERA AM
- KUCERA V
- KUHN C
- KUIJER PG
- KUMAR J
- KUMAR L
- KUMAR S
- KUNDU S
- KURASHVILI P
- KUREPIN A
- KUREPIN AB
- KURYAKIN A
- KUSHPIL S
- KVAPIL J
- KWEON MJ
- KWON Y
- LAI YS
- LAKOMOV I
- LANGOY R
- LAPIDUS K
- LARA C
- LARDEUX A
- LARIONOV P
- LAUDI E
- LAVICKA R
- LEA R
- LEARDINI L
- LEE S
- LEEUWEN M
- LEHAS F
- LEHNER S
- LEHRBACH J
- LEMMON RC
- LEVAI P
- LEZAMA EP
- LI X
- LI XL
- LIEN J
- LIETAVA R
- LIM B
- LIMON S
- LINDAL S
- LINDENSTRUTH V
- LINDSAY SW
- LIPPMANN C
- LISA MA
- LITICHEVSKYI V
- LIU A
- LJUNGGREN HM
- LLOPE WJ
- LODATO DF
- LOGINOV V
- LOIZIDES C
- LONCAR P
- LOPEZ X
- LOWE A
- LUETTIG P
- LUHDER JR
- LUNARDON M
- LUPARELLO G
- LUPI M
- MAEVSKAYA A
- MAGER M
- MAHMOOD SM
- MAIRE A
- MAJKA RD
- MAL'KEVICH D
- MALAEV M
- MALIK QW
- MALININA L
- MALZACHER P
- MAMONOV A
- MANKO V
- MANSO F
- MANZARI V
- MAO Y
- MARCHISONE M
- MARCO N
- MARES J
- MARGAGLIOTTI GV
- MARGOTTI A
- MARGUTTI J
- MARIN A
- MARKERT C
- MARQUARD M
- MARTIN NA
- MARTINENGO P
- MARTINEZ H
- MARTINEZ JL
- MARTINEZ MI
- MASCIOCCHI S
- MASERA M
- MASONI A
- MASSACRIER L
- MASSON E
- MASTROSERIO A
- MATHIS AM
- MATUOKA PFT
- MATYJA A
- MAURO A
- MAYER C
- MAZZILLI M
- MAZZONI MA
- MEDDI F
- MELIKYAN Y
- MENCHACA-ROCHA A
- MENINNO E
- MERES M
- MEZA CS
- MHLANGA S
- MIAKE Y
- MICHELETTI L
- MIESKOLAINEN MM
- MIHAYLOV DL
- MIKHAYLOV K
- MISCHKE A
- MISHRA AN
- MISKOWIEC D
- MITRA J
- MITU CM
- MOHAMMADI N
- MOHANTY AP
- MOHANTY B
- MOLINA R
- MONZON I
- MORALES YC
- MORENO LAP
- MORETTO S
- MORREALE A
- MORSCH A
- MUCCIFORA V
- MUDNIC E
- MUEHLHEIM D
- MUENNING K
- MUHURI S
- MUKHERJEE M
- MULLIGAN JD
- MUNHOZ MG
- MUNOZ G
- MUNOZ MIA
- MUNZER RH
- MURAKAMI H
- MURRAY S
- MUSA L
- MUSINSKY J
- MYERS CJ
- MYRCHA JW
- NAIK B
- NAIR R
- NANDI BK
- NANIA R
- NAPPI E
- NARAYAN A
- NARU MU
- NASSIRPOUR AF
- NATTRASS C
- NAVARRO SR
- NAYAK K
- NAYAK R
- NAYAK TK
- NAZARENKO S
- NELLEN L
- NESBO SV
- NESKOVIC G
- NG F
- NICASSIO 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
- OH H
- OHLSON A
- OLENIACZ J
- OLIVEIRA RAN
- 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
- PARKKILA JE
- PARMAR S
- PASQUALE S
- PASSFELD A
- PATHAK SP
- PATRA RN
- PAUL B
- PEDREIRA MM
- PEI H
- PEITZMANN T
- PENG X
- PEREIRA LG
- PERESUNKO D
- PEREZ J
- PESKOV V
- PESTOV Y
- PETRACEK V
- PETROVICI M
- PETTA C
- PEZZI RP
- PIANO S
- PIKNA M
- PILLOT P
- PIMENTEL LODL
- PINAZZA O
- PINSKY L
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- PLANINIC M
- PLIQUETT F
- PLOSKON M
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- PRASAD SK
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- READ KF
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- RIABOV V
- RICHERT T
- RICHTER M
- RIEDLER P
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- RIGGI F
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- ROCCA P
- RODE SP
- ROED K
- ROGALEV R
- ROGOCHAYA E
- ROHR D
- ROHRICH D
- ROKITA PS
- RONCHETTI F
- ROSAS ED
- ROSLON K
- ROSNET P
- ROSSI A
- ROTONDI A
- ROUKOUTAKIS F
- ROY C
- ROY P
- RUEDA OV
- RUI R
- RUMYANTSEV B
- RUSTAMOV A
- RUZZA B
- RYABINKIN E
- RYABOV Y
- RYBICKI A
- SAARINEN S
- SADHU S
- SADOVSKY S
- SAFARIK K
- SAHA SK
- SAHOO B
- SAHOO P
- SAHOO R
- SAHOO S
- SAHU PK
- SAINI J
- SAKAI S
- SALEH MA
- SAMBYAL S
- SAMSONOV V
- SANCHEZ C
- 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 A
- SHARMA M
- SHARMA N
- SHEIKH AI
- SHIGAKI K
- SHIMOMURA M
- SHIRINKIN S
- SHOU Q
- SHTEJER K
- SIBIRIAK Y
- SIDDHANTA S
- SIELEWICZ KM
- SIEMIARCZUK T
- SILVERMYR D
- SIMATOVIC G
- SIMONETTI G
- SINGARAJU R
- SINGH R
- SINGH R
- SINGHAL V
- SINHA T
- SITAR B
- SITTA M
- SKAALI TB
- SLUPECKI M
- SMIRNOV N
- SNELLINGS RJM
- SNELLMAN TW
- SONG J
- SORAMEL F
- SORENSEN S
- SOUZA RD
- 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 A
- TELLO A
- TERREVOLI C
- TEYSSIER B
- THAKUR D
- THAKUR S
- THOMAS D
- THORESEN F
- TIEULENT R
- TIKHONOV A
- TIMMINS AR
- TOIA A
- TOPILSKAYA N
- TOPPI M
- TORRES E
- TORRES SR
- TRIPATHY S
- TROGOLO S
- TROMBETTA G
- TROPP L
- TRUBNIKOV V
- TRZASKA WH
- TRZCINSKI TP
- TRZECIAK BA
- TSUJI T
- TUMKIN A
- TURRISI R
- TVETER TS
- ULLALAND K
- UMAKA EN
- URAS A
- USAI GL
- UTROBICIC A
- UYSAL AK
- VALA M
- VALLE ZC
- VARGA D
- VARGAS A
- VARGYAS M
- VARMA R
- VASILEIOU M
- VASILIEV A
- VAUTHIER A
- VECHERNIN V
- VEEN AM
- VELASQUEZ A
- VERCELLIN E
- VERMUNT L
- VERNET R
- VERTESI R
- VICKOVIC L
- VIINIKAINEN J
- VILAKAZI Z
- VILLAR E
- VINOGRADOV A
- VIRGILI T
- VISLAVICIUS V
- VODOPYANOV A
- VOELKL MA
- VOLOSHIN K
- VOLOSHIN SA
- VOLPE G
- VOROBYEV I
- VOSCEK D
- VRANIC D
- VRLAKOVA J
- VYVRE P
- WAGNER B
- WANG H
- WANG M
- WATANABE Y
- WEBER M
- WEBER SG
- WEGRZYNEK A
- 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
- 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
- ZHOU Y
- ZHOU Z
- ZHU H
- ZHU J
- ZHU Y
- ZICHICHI A
- ZIMMERMANN MB
- ZINOVJEV G
- ZMESKAL J
- ZOU S
- Publication venue
- 'Wiley'
- Publication date
- 01/01/2014
- Field of study
It has been known since the 1960s that the layers of Na and K atoms, which occur between 80 and 105âkm in the Earth's atmosphere as a result of meteoric ablation, exhibit completely different seasonal behavior. In the extratropics Na varies annually, with a pronounced wintertime maximum and summertime minimum. However, K varies semiannually with a small summertime maximum and minima at the equinoxes. This contrasting behavior has never been satisfactorily explained. Here we use a combination of electronic structure and chemical kinetic rate theory to determine two key differences in the chemistries of K and Na. First, the neutralization of K+ ions is only favored at low temperatures during summer. Second, cycling between K and its major neutral reservoir KHCO3 is essentially temperature independent. A whole atmosphere model incorporating this new chemistry, together with a meteor input function, now correctly predicts the seasonal behavior of the K layer
ALICE Collaboration
- Author
- Acharya S
- Acosta FT
- AdamovĂĄ D
- Adolfsson J
- Aggarwal MM
- Aglieri Rinella G
- Agnello M
- Agrawal N
- Ahammed Z
- Ahn SU
- Aiola S
- Akindinov A
- Al-Turany M
- Alam SN
- Albuquerque DSD
- Aleksandrov D
- Alessandro B
- Alfaro Molina R
- 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
- Antinori F
- AntiÄiÄ T
- Antonioli P
- Anwar R
- Apadula N
- Aphecetche L
- AppelshÀuser H
- Arcelli S
- Arnaldi R
- Arnold OW
- Arratia M
- Arsene IC
- Arslandok M
- Augustinus A
- Averbeck R
- Azmi MD
- BadalĂ A
- Baek YW
- Bagnasco S
- Bailhache R
- Bala R
- Baldisseri A
- Ball M
- Baral RC
- Barbano AM
- Barbera R
- Barile F
- Barioglio L
- Barnaföldi GG
- Barnby LS
- Barret V
- Bartalini P
- Barth K
- Bartsch E
- Bastid N
- Basu S
- Batigne G
- Batyunya B
- Batzing PC
- Bazo Alba JL
- Bearden IG
- Beck H
- Bedda C
- Behera NK
- Belikov I
- Bellini F
- Bello Martinez H
- 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
- BielÄĂk J
- BielÄĂkovĂĄ J
- Bilandzic A
- Biro G
- Biswas R
- Biswas S
- Blair JT
- Blau D
- Blume C
- Boca G
- Bock F
- Bogdanov A
- BoldizsĂĄr 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
- Buesching H
- Bufalino S
- Buhler P
- Buncic P
- Busch O
- Buthelezi Z
- Butt JB
- Buxton JT
- Cabala J
- Caffarri D
- Caines H
- Caliva A
- Calvo Villar E
- Camacho RS
- Camerini P
- Capon AA
- Carena F
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- Voloshin SA
- Volpe G
- von Haller B
- Vorobyev I
- Voscek D
- Vranic D
- VrlĂĄkovĂĄ J
- VĂĄzquez Doce O
- VĂ©rtesi R
- Völkl MA
- Wagner B
- Wang H
- Wang M
- Watanabe Y
- Weber M
- Weber SG
- Wegrzynek A
- 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
- Yano S
- Yin Z
- Yokoyama H
- Yoo I-K
- Yoon JH
- Yurchenko V
- Zaccolo V
- Zaman A
- Zampolli C
- Zanoli HJC
- Zardoshti N
- Zarochentsev A
- Zaviyalov N
- Zbroszczyk H
- Zhalov M
- Zhang X
- Zhang Y
- Zhang Z
- Zhao C
- Zherebchevskii V
- Zhigareva N
- Zhou D
- Zhou Y
- Zhou Z
- Zhu H
- Zhu J
- Zhu Y
- Zichichi A
- Zimmermann MB
- Zinovjev G
- Zmeskal J
- Zou S
- ZĂĄvada P
- Ć afaĆĂk K
- Ć efÄĂk M
- Ć umbera M
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/02/2019
- Field of study
J/psi production as a function of charged-particle pseudorapidity density in p-Pb collisions at root s(NN)=5.02 TeV
- Author
- Adamova D
- Aggarwal MM
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad N
- Ahn SU
- Aiola S
- Akindinov A
- Alam SN
- Albuquerque DSD
- Aleksandrov D
- Alessandro B
- Alexandre D
- Alfaro Molina R
- Alici A
- Alkin A
- Alme J
- Alt T
- Altsybeev I
- Alves Garcia Prado C
- An M
- Andrei C
- 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 O Villalobos
- Bala R
- Balbastre G Conesa
- Baldisseri A
- Ball M
- Baral RC
- Barbano AM
- Barbera R
- Barile F
- Barioglio L
- Barnafoldi GG
- Barnby LS
- Barret V
- Barroso V Chibante
- Bartalini P
- Barth K
- Bartke J
- Bartsch E
- Basile M
- Bastid N
- Basu S
- Bathen B
- Batigne G
- Batyunya B
- Batzing PC
- Bearden IG
- Beck H
- Bedda C
- Behera NK
- Belikov I
- Bellini F
- Bello Martinez H
- 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
- Bhati AK
- Bhattacharjee B
- Bhom J
- Bianchi L
- Bianchi N
- Bianchin C
- Bielcik J
- Bielcikova J
- Bilandzic A
- Biro G
- Biswas R
- Biswas S
- Blair JT
- Blanco J Martin
- 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
- Braun-Munzinger P
- Bregant M
- Broker TA
- Browning TA
- Broz M
- Brucken EJ
- Bruna E
- Bruno GE
- Budnikov D
- Buesching H
- Bufalino S
- Buhler P
- Buitron SAI
- Buncic P
- Busch O
- Bustamante RT Jimenez
- Buthelezi Z
- Butt JB
- Buxton JT
- Cabala J
- Caffarri D
- Caines H
- Caliva A
- Calvo Villar E
- Camejo A Batista
- Camerini P
- Capon AA
- Carena F
- Carena W
- Carnesecchi F
- Castellanos J Castillo
- Castro AJ
- Casula EAR
- Ceballos Sanchez C
- Cerello P
- Cervantes I Maldonado
- Chang B
- Chapeland S
- Chartier M
- Charvet JL
- Chattopadhyay S
- Chattopadhyay S
- Chauvin A
- Cherney M
- Cheshkov C
- Cheynis B
- Chinellato DD
- Cho S
- Chochula P
- Choi K
- Chojnacki M
- Choudhury S
- Christakoglou P
- Christensen CH
- Christiansen P
- Chujo T
- Chung SU
- Cicalo C
- Cifarelli L
- Cindolo F
- Cleymans J
- Colamaria F
- Colella D
- Collaboration ALICE
- Collu A
- Colocci M
- Connors ME
- Contreras JG
- Cormier TM
- Cortes Maldonado I
- Cortese P
- Cosentino MR
- Costa F
- Costanza S
- Crkovska J
- Crochet P
- Cuautle E
- Cunqueiro L
- Da Costa H Pereira
- 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 DA Moreira
- De Gruttola D
- De Marco N
- De Oliveira RA Negrao
- De Pasquale S
- De Souza RD
- De S
- Degenhardt HF
- Deisting A
- del Valle Z Conesa
- Deloff A
- Deplano C
- Dhankher P
- Di Bari D
- Di Mauro A
- Di Nezza P
- Di Ruzza B
- Diaz Corchero MA
- Dietel T
- Dillenseger P
- Divia R
- Djuvsland O
- Dobrin A
- Doce O Vazquez
- Doenigus B
- Domenicis Gimenez D
- Dordic O
- Drozhzhova T
- Dubey AK
- Dubla A
- Ducroux L
- Duggal AK
- Dupieux P
- Ehlers RJ
- Elia D
- Endress E
- Engel H
- Epple E
- Erazmus B
- Erhardt F
- Espagnon B
- Esumi S
- Eulisse G
- Eum J
- Evans D
- Evdokimov S
- Fabbietti L
- Faivre J
- Fantoni A
- Fasel M
- Feldkamp L
- Feliciello A
- Feofilov G
- Ferencei J
- Fernandez Tellez A
- Ferreiro EG
- Ferretti A
- Festanti A
- Feuillard VJG
- Figiel J
- Figueredo MAS
- Filchagin S
- Finogeev D
- Fionda FM
- Fiore EM
- 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
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- Yin Z
- Yokoyama H
- Yoo I-K
- Yoon JH
- Yurchenko V
- Zaccolo V
- Zaman A
- Zampolli C
- Zanoli HJC
- Zardoshti N
- Zarochentsev A
- Zavada P
- Zaviyalov N
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- Zhalov M
- Zhang C
- Zhang H
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- Zimmermann MB
- Zimmermann S
- Zinovjev G
- Zmeskal J
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2018
- Field of study
We report measurements of the inclusive J/Ï yield and average transverse momentum as a function of charged-particle pseudorapidity density dNch/dη in pâPb collisions at sNN=5.02TeV with ALICE at the LHC. The observables are normalised to their corresponding averages in non-single diffractive events. An increase of the normalised J/Ï yield with normalised dNch/dη, measured at mid-rapidity, is observed at mid-rapidity and backward rapidity. At forward rapidity, a saturation of the relative yield is observed for high charged-particle multiplicities. The normalised average transverse momentum at forward and backward rapidities increases with multiplicity at low multiplicities and saturates beyond moderate multiplicities. In addition, the forward-to-backward nuclear modification factor ratio is also reported, showing an increasing suppression of J/Ï production at forward rapidity with respect to backward rapidity for increasing charged-particle multiplicity
K*(892)(0) and phi(1020)meson production at high transverse momentum in pp and Pb-Pb collisions at root sNN=2.76 TeV
- Author
- Adam J
- Adamova D
- Aggarwal MM
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn SU
- Aiola S
- Akindinov A
- Alam SN
- Albino R Cruz
- Albuquerque DSD
- Aleksandrov D
- Alessandro B
- Alexandre D
- Alfaro Molina R
- Alici A
- Alkin A
- Alme J
- Alt T
- Altinpinar S
- Altsybeev I
- Alves Garcia Prado C
- An M
- Andrei C
- Andrews HA
- Andronic A
- Anguelov V
- Anson C
- Anticic T
- Antinori F
- Antonioli P
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- Aphecetche L
- Appelshaeuser H
- Arcelli S
- Arnaldi R
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- Azmi MD
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- Baillie O Villalobos
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- Guzman IB
- Haake R
- Hadjidakis C
- Hamagaki H
- Hamar G
- Hamon JC
- Harris JW
- Harton A
- Hatzifotiadou D
- Hayashi S
- Heckel ST
- Hellbar E
- Helstrup H
- Herghelegiu A
- Herrera Corral G
- Herrmann F
- Hess BA
- Hetland KF
- Hillemanns H
- Hippolyte B
- Hladky J
- Horak D
- Hosokawa R
- Hristov P
- Hughes C
- Humanic TJ
- Hussain N
- Hussain T
- Hutter D
- Hwang DS
- Ilkaev R
- Inaba M
- Ippolitov M
- Irfan M
- Isakov V
- Islam MS
- Ivanov M
- Ivanov V
- Izucheev V
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- Jacazio N
- Jacobs PM
- Jadhav MB
- Jadlovska S
- Jadlovsky J
- Jahnke C
- Jakubowska MJ
- Janik MA
- Jayarathna PHSY
- Jena C
- Jena S
- Jercic M
- Jones PG
- Jusko A
- Kalinak P
- Kalweit A
- Kang JH
- Kaplin V
- Kar S
- Karavichev O
- Karavicheva T
- Karayan L
- Karpechev E
- Kebschull U
- Keidel R
- Keijdener DLD
- Keil M
- Ketzer B
- Khan M Mohisin
- Khan P
- Khan SA
- Khanzadeev A
- Kharlov Y
- Khatun A
- Khuntia A
- Kielbowicz MM
- Kileng B
- Kim D
- Kim DJ
- Kim DW
- Kim H
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2017
- Field of study
The production of Kâ(892)0 and Ï(1020) mesons in proton-proton (pp) and lead-lead (Pb-Pb) collisions
at âsNN = 2.76 TeV has been analyzed using a high luminosity data sample accumulated in 2011 with the
ALICE detector at the Large Hadron Collider (LHC). Transverse momentum (pT) spectra have been measured
for Kâ(892)0 and Ï(1020) mesons via their hadronic decay channels for pT up to 20 GeV/c. The measurements
in pp collisions have been compared to model calculations and used to determine the nuclear modification factor
and particle ratios. The Kâ(892)0/K ratio exhibits significant reduction from pp to central Pb-Pb collisions,
consistent with the suppression of the Kâ(892)0 yield at low pT due to rescattering of its decay products in
the hadronic phase. In central Pb-Pb collisions the pT dependent Ï(1020)/Ï and Kâ(892)0/Ï ratios show an
enhancement over pp collisions for pT â 3 GeV/c, consistent with previous observations of strong radial flow.
At high pT, particle ratios in Pb-Pb collisions are similar to those measured in pp collisions. In central Pb-Pb
collisions, the production of Kâ(892)0 and Ï(1020) mesons is suppressed for pT > 8 GeV/c. This suppression is
similar to that of charged pions, kaons, and protons, indicating that the suppression does not depend on particle
mass or flavor in the light quark sector
A(c)(+) Production and Baryon-to-Meson Ratios in pp and p-Pb Collisions at root S-NN=5.02 TeV at the LHC
- Author
- A G Clai
- Acharya S
- Adamova D
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- Adolfsson J
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- Ahmad S
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- Zanoli HJC
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- Zhu Y
- Zichichi A
- Zinovjev G
- Zurlo N
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2021
- Field of study
The prompt production of the charm baryon \u39bc+ and the \u39bc+/D0 production ratios were measured at midrapidity with the ALICE detector in pp and p-Pb collisions at sNN=5.02 TeV. These new measurements show a clear decrease of the \u39bc+/D0 ratio with increasing transverse momentum (pT) in both collision systems in the range 2<12 GeV/c, exhibiting similarities with the light-flavor baryon-to-meson ratios p/\u3c0 and \u39b/KS0. At low pT, predictions that include additional color-reconnection mechanisms beyond the leading-color approximation, assume the existence of additional higher-mass charm-baryon states, or include hadronization via coalescence can describe the data, while predictions driven by charm-quark fragmentation processes measured in e+e- and e-p collisions significantly underestimate the data. The results presented in this Letter provide significant evidence that the established assumption of universality (colliding-system independence) of parton-to-hadron fragmentation is not sufficient to describe charm-baryon production in hadronic collisions at LHC energies
First measurement of jet mass in Pb-Pb and p-Pb collisions at the LHC
- Author
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- Yurchenko V
- Zaccolo V
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- Zanoli HJC
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- Zimmermann S
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- Zmeskal J
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2018
- Field of study
This letter presents the first measurement of jet mass in PbâPb and pâPb collisions at sNN=2.76 TeV and sNN=5.02 TeV, respectively. Both the jet energy and the jet mass are expected to be sensitive to jet quenching in the hot Quantum Chromodynamics (QCD) matter created in nuclear collisions at collider energies. Jets are reconstructed from charged particles using the anti-kT jet algorithm and resolution parameter R=0.4. The jets are measured in the pseudorapidity range |ηjet|<0.5 and in three intervals of transverse momentum between 60 GeV/c and 120 GeV/c. The measurement of the jet mass in central PbâPb collisions is compared to the jet mass as measured in pâPb reference collisions, to vacuum event generators, and to models including jet quenching. It is observed that the jet mass in central PbâPb collisions is consistent within uncertainties with pâPb reference measurements. Furthermore, the measured jet mass in PbâPb collisions is not reproduced by the quenching models considered in this letter and is found to be consistent with PYTHIA expectations within systematic uncertainties
A(c)(+) Production and Baryon-to-Meson Ratios in pp and p-Pb Collisions at root S-NN=5.02 TeV at the LHC
- Author
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- Acharya S
- Adamova D
- Adler A
- Adolfsson J
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn SU
- Akbar Z
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- Alfanda HM
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- Simatovic G
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- Yamakawa K
- Yang S
- Yano S
- Yin Z
- Yokoyama H
- Yoo I-K
- Yoon JH
- Yuan S
- Yuncu A
- Yurchenko V
- Zaccolo V
- Zaman A
- Zampolli C
- Zanoli HJC
- Zardoshti N
- Zarochentsev A
- Zavada P
- Zaviyalov N
- Zbroszczyk H
- Zhalov M
- Zhang S
- Zhang X
- Zhang Y
- Zherebchevskii V
- Zhi Y
- Zhou D
- Zhou Y
- Zhu J
- Zhu Y
- Zichichi A
- Zinovjev G
- Zurlo N
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2021
- Field of study
The prompt production of the charm baryon Î_{c}^{+} and the Î_{c}^{+}/D^{0} production ratios were measured at midrapidity with the ALICE detector in pp and p-Pb collisions at sqrt[s_{NN}]=5.02ââTeV. These new measurements show a clear decrease of the Î_{c}^{+}/D^{0} ratio with increasing transverse momentum (p_{T}) in both collision systems in the range 2<p_{T}<12ââGeV/c, exhibiting similarities with the light-flavor baryon-to-meson ratios p/Ï and Î/K_{S}^{0}. At low p_{T}, predictions that include additional color-reconnection mechanisms beyond the leading-color approximation, assume the existence of additional higher-mass charm-baryon states, or include hadronization via coalescence can describe the data, while predictions driven by charm-quark fragmentation processes measured in e^{+}e^{-} and e^{-}p collisions significantly underestimate the data. The results presented in this Letter provide significant evidence that the established assumption of universality (colliding-system independence) of parton-to-hadron fragmentation is not sufficient to describe charm-baryon production in hadronic collisions at LHC energies
Suppression in Pb-Pb Collisions at the LHC.
- Author
- Acharya S
- AdamovĂĄ D
- Adler A
- Aglieri Rinella G
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad S
- Ahn SU
- Ahuja I
- Akindinov A
- Al-Turany M
- Aleksandrov D
- Alessandro B
- Alfanda HM
- Alfaro Molina R
- Ali B
- ALICE Collaboration
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- Voloshin SA
- Volpe G
- von Haller B
- Vorobyev I
- Vozniuk N
- VrlĂĄkovĂĄ J
- VĂĄzquez Doce O
- VĂ©rtesi R
- Völkl MA
- Wang C
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- Weiglhofer FT
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- Yadav AK
- Yalcin S
- Yamaguchi Y
- Yamakawa K
- Yang S
- Yano S
- Yin Z
- Yoo I-K
- Yoon JH
- 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
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- Zherebchevskii V
- Zhi Y
- Zhou D
- Zhou Y
- Zhu J
- Zhu Y
- Zugravel SC
- Zurlo N
- ZĂĄvada P
- Ć afaĆĂk K
- Ć erkĆĄnytÄ L
- Publication venue
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- Field of study
The production of the Ï(2S) charmonium state was measured with ALICE in Pb-Pb collisions at sqrt[s_{NN}]=5.02ââTeV, in the dimuon decay channel. A significant signal was observed for the first time at LHC energies down to zero transverse momentum, at forward rapidity (2.5<y<4). The measurement of the ratio of the inclusive production cross sections of the Ï(2S) and J/Ï resonances is reported as a function of the centrality of the collisions and of transverse momentum, in the region p_{T}<12ââGeV/c. The results are compared with the corresponding measurements in pp collisions, by forming the double ratio [Ï^{Ï(2S)}/Ï^{J/Ï}]_{Pb-Pb}/[Ï^{Ï(2S)}/Ï^{J/Ï}]_{pp}. It is found that in Pb-Pb collisions the Ï(2S) is suppressed by a factor of âŒ2 with respect to the J/Ï. The Ï(2S) nuclear modification factor R_{AA} was also obtained as a function of both centrality and p_{T}. The results show that the Ï(2S) resonance yield is strongly suppressed in Pb-Pb collisions, by a factor of up to âŒ3 with respect to pp. Comparisons of cross section ratios with previous Super Proton Synchrotron findings by the NA50 experiment and of R_{AA} with higher-p_{T} results at LHC energy are also reported. These results and the corresponding comparisons with calculations of transport and statistical models address questions on the presence and properties of charmonium states in the quark-gluon plasma formed in nuclear collisions at the LHC
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- Acharya S
- Adamova D
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- Adolfsson J
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2020
- Field of study
This paper presents the measurements of ϱ, K±, p and pâ transverse momentum (pTâ) spectra as a function of charged-particle multiplicity density in protonâproton (pp) collisions at sâ = 13 TeV with the ALICE detector at the LHC. Such study allows us to isolate the center-of-mass energy dependence of light-flavour particle production. The measurements reported here cover a pTâ range from 0.1 to 20 GeV/c and are done in the rapidity interval âŁyâŁ<0.5. The pTâ-differential particle ratios exhibit an evolution with multiplicity, similar to that observed in pp collisions at sâ = 7 TeV, which is qualitatively described by some of the hydrodynamical and pQCD-inspired models discussed in this paper. Furthermore, the pTâ-integrated hadron-to-pion yield ratios measured in pp collisions at two different center-of-mass energies are consistent when compared at similar multiplicities. This also extends to strange and multi-strange hadrons, suggesting that, at LHC energies, particle hadrochemistry scales with particle multiplicity the same way under different collision energies and colliding systems
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