249 research outputs found
Effective Rheology of Bubbles Moving in a Capillary Tube
- Author
- Abelev B
- Adam J
- Adamova D
- Adare AM
- Aggarwal MM
- Agocs AG
- Agostinelli A
- Ahammed Z
- Ahmad N
- Ahn SU
- Akindinov A
- Alaniz EC
- Aleksandrov D
- Alessandro B
- Alici A
- Alkin A
- Alme J
- Alt T
- Altini V
- Altinpinar S
- Altsybeev I
- Andrei C
- Andronic A
- Anguelov V
- Anielski J
- Anson C
- Anticic T
- Antinori F
- Antonioli P
- Aphecetche L
- Appelshauser H
- Arbor N
- Arcelli S
- Arend A
- Armesto N
- Arnaldi R
- Aronsson T
- Arsene IC
- Arslandok M
- Asryan A
- Augustinus A
- Averbeck R
- Avina EA
- Awes TC
- Aysto J
- Azmi MD
- Bach M
- Badala A
- Baek YW
- Bailhache R
- Baillie OV
- Bala R
- Balbastre GC
- Baldisseri A
- Baldit A
- Ban J
- Baral RC
- Barbera R
- Bari DD
- Barile F
- Barnafoldi GG
- Barnby LS
- Barret V
- Barros GOVD
- Barroso VC
- Bartke J
- Basile M
- Bastid N
- Bathen B
- Batigne G
- Batyunya B
- Baumann C
- Bearden IG
- Beck H
- Belikov I
- Bellini F
- Bellwied R
- Belmont-Moreno E
- Bencedi G
- Beole S
- Berceanu I
- Bercuci A
- Berdnikov Y
- Berenyi D
- Bergmann C
- Berzano D
- Betev L
- Bhasin A
- Bhati AK
- Bianchi L
- Bianchi N
- Bianchin C
- Bielcik J
- Bielcikova J
- Bjelogrlic S
- Blanco F
- Blanco F
- Blau D
- Blume C
- Boccioli M
- Bock N
- Bogdanov A
- Boggild H
- Bogolyubsky M
- Boldizsar L
- Bombara M
- Book J
- Borel H
- Borissov A
- Bornec YL
- Bose S
- Bossu F
- Botje M
- Bottger S
- Boyer B
- Braidot E
- Braun-Munzinger P
- Bregant M
- Breitner T
- Browning TA
- Broz M
- Brun R
- Bruna E
- Bruno GE
- Budnikov D
- Buesching H
- Bufalino S
- Bugaiev K
- Busch O
- Bustamante RTJ
- Buthelezi Z
- Caffarri D
- Cahuantzi MR
- Cai X
- Caines H
- Camerini P
- Carena F
- Carena W
- Carminati F
- Caro AD
- Castellanos JC
- Castro XS
- Casula EAR
- Cataldo GD
- Catanescu V
- Cavicchioli C
- Cepila J
- Cerello P
- Cervantes IM
- Chang B
- Chapeland S
- Charvet JL
- Chattopadhyay S
- Chattopadhyay S
- Chawla I
- Cherney M
- Cheshkov C
- Cheynis B
- Chiavassa E
- Chinellato DD
- Chochula P
- Chojnacki M
- Christakoglou P
- Christensen CH
- Christiansen P
- Chujo T
- Chung SU
- Cicalo C
- Cifarelli L
- Cindolo F
- Cleymans J
- Coccetti F
- Colamaria F
- Colella D
- Collaboration ALICE
- Constantin P
- Contin G
- Contreras JG
- Corchero MAD
- Cormier TM
- Corral GH
- Cortese P
- Cosentino MR
- Costa F
- Cotallo ME
- Crescio E
- Crochet P
- Cuautle E
- Cunqueiro L
- Cuveland JD
- Dainese A
- Dalsgaard HH
- Danu A
- Das D
- Das I
- Das K
- Dash A
- Dash S
- Davalos AM
- De S
- Delagrange H
- Deloff A
- Demanov V
- Denes E
- Deppman A
- Diaz AC
- Dietel T
- Divia R
- Djuvsland O
- Dobrin A
- Dobrowolski T
- Dominguez I
- Don CKK
- Donigus B
- Dordic O
- Driga O
- Dubey AK
- Ducroux L
- Dupieux P
- Elia D
- Emschermann D
- Engel H
- Erasmo GD
- Erdal HA
- Espagnon B
- Estienne M
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- Evans D
- Eyyubova G
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- Fedunov A
- Fehlker D
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- Feofilov G
- Ferreiro EG
- Ferretti A
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- Figiel J
- Figueredo MAS
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- Filho NC
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- Fionda FM
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- Frankenfeld U
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- Gangadharan DR
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- Gerhard J
- Germain M
- Geuna C
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- Giglio CD
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- Gladysz-Dziadus E
- Glassel P
- Godoy DAMD
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- Gorbunov S
- Goswami A
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- Grabski V
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- Grajcarek R
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- Guber F
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- Guerzoni B
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- Guilbaud M
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- Gupta A
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- Gutbrod H
- Gutierrez CG
- Haaland O
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- Haiduc M
- Haller BV
- Hamagaki H
- Hamar G
- Han BH
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- Hansen A
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- Harris JW
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- Hayrapetyan A
- Heckel ST
- Heide M
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- Hetland KF
- Hicks B
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- Hippolyte B
- Horaguchi T
- Hori Y
- Hristov P
- Hrivnacova I
- Huang M
- Huber S
- Humanic TJ
- Hwang DS
- Ichou R
- Ilkaev R
- Ilkiv I
- Inaba M
- Incani E
- Innocenti GM
- Innocenti PG
- Ippolitov M
- Irfan M
- Ivan C
- Ivanov A
- Ivanov M
- Ivanov V
- Ivanytskyi O
- Jacholkowski A
- Jacobs PM
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- Jang HJ
- Jangal S
- Janik MA
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- Jones PG
- Jung H
- Jusko A
- Kaidalov AB
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- Kolk NVD
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- Kondratiev V
- Kondratyeva N
- Konevskikh A
- Korneev A
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- Kox S
- Kral J
- Kralik I
- Kramer F
- Kraus I
- Krawutschke T
- Krelina M
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- Krizek F
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- Nomokonov P
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- Wilk G
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- Windelband B
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- Yang S
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- Yi J
- Yin Z
- Yokoyama H
- Yoo IK
- Yoon J
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- Zach C
- Zampolli C
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- Zarochentsev A
- Zavada P
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- Zbroszczyk H
- Zelnicek P
- Zetina LM
- Zgura IS
- Zhalov M
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- Zimmermann A
- Zinovjev G
- Zoccarato Y
- Zynovyev M
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 16/03/2012
- Field of study
We calculate the average volumetric flux versus pressure drop of bubbles
moving in a single capillary tube with varying diameter, finding a square-root
relation from mapping the flow equations onto that of a driven overdamped
pendulum. The calculation is based on a derivation of the equation of motion of
a bubble train from considering the capillary forces and the entropy production
associated with the viscous flow. We also calculate the configurational
probability of the positions of the bubbles.Comment: 4 pages, 1 figur
Elucidating the clinical and molecular spectrum of SMARCC2-associated NDD in a cohort of 65 affected individuals
- Author
- Accogli A
- Anyane-Yeboa K
- Baysal Ö
- Bend R
- Beunders G
- Bhola PT
- Bosch E
- Bruno LP
- Campeau PM
- Capra V
- Carter LB
- Close C
- Cogne B
- Cuscó I
- De Marco P
- Dobson A
- Galindo MK
- Garcia EJ
- Goj G
- Graham BH
- Granata S
- Güse E
- Hannibal MC
- Hartwich D
- Holthöfer L
- Hubbard G
- Isidor B
- Jamra RA
- Karimov C
- Kuismin O
- Kurki M
- Marcelis C
- Maroofian R
- Martinez-Agosto JA
- Maystadt I
- McGinnis E
- Mefford HC
- Millan F
- Millichap J
- Morrow MM
- Nibbeling EAR
- Nigro V
- Ognibene M
- Pereira EM
- Pinto AM
- Platzer K
- Popp B
- Prijoles EJ
- Rabani AM
- Rath J
- Reis A
- Renieri A
- Ropers FG
- Salpietro V
- Santen GWE
- Scala M
- Severino M
- Shillington A
- Skinner C
- Stevenson RE
- Thiffault I
- Torella A
- Umair M
- Valenzuela I
- van de Kamp JM
- van der Sluijs PJ
- van Haeringen A
- Vasileiou G
- Wagner M
- Wieczorek D
- Zacher P
- Zweier M
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/11/2023
- Field of study
Purpose: Coffin-Siris and Nicolaides-Baraitser syndromes are recognizable neurodevelopmental disorders caused by germline variants in BAF complex subunits. The SMARCC2 BAFopathy was recently reported. Herein, we present clinical and molecular data on a large cohort. Methods: Clinical symptoms for 41 novel and 24 previously published affected individuals were analyzed using the Human Phenotype Ontology. For genotype-phenotype correlations, molecular data were standardized and grouped into non-truncating and likely gene-disrupting (LGD) variants. Missense variant protein expression and BAF-subunit interactions were examined using 3D protein modeling, co-immunoprecipitation, and proximity-ligation assays. Results: Neurodevelopmental delay with intellectual disability, muscular hypotonia, and behavioral disorders were the major manifestations. Clinical hallmarks of BAFopathies were rare. Clinical presentation differed significantly, with LGD variants being predominantly inherited and associated with mildly reduced or normal cognitive development, whereas non-truncating variants were mostly de novo and presented with severe developmental delay. These distinct manifestations and non-truncating variant clustering in functional domains suggest different pathomechanisms. In vitro testing showed decreased protein expression for N-terminal missense variants similar to LGD. Conclusion: This study improved SMARCC2 variant classification and identified discernible SMARCC2-associated phenotypes for LGD and non-truncating variants, which were distinct from other BAFopathies. The pathomechanism of most non-truncating variants has yet to be investigated
First measurement of the |t|-dependence of coherent J/ψ 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
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- Willems GA
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- Windelband B
- Witt WE
- Xu R
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- Yano S
- Yin Z
- Yokoyama H
- Yoo I-K
- Yoon JH
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- Yurchenko V
- Zaccolo V
- Zaman A
- Zampolli C
- Zanoli HJC
- Zardoshti N
- Zarochentsev A
- Zavada P
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- Zbroszczyk H
- Zhalov M
- Zhang X
- Zhang Y
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- Zhao C
- Zherebchevskii V
- Zhigareva N
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- 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/ψ 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 Pb–Pb collisions at a centre-of-mass energy per nucleon pair sNN=5.02TeV with the J/ψ produced in the central rapidity region |y|<0.8, which corresponds to the small Bjorken-x range (0.3−1.4)×10−3.
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 Balitsky–Kovchegov 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
Global patient outcomes after elective surgery: prospective cohort study in 27 low-, middle- and high-income countries.
- Author
- Ab Majid MA
- Ab Rahman AS
- Ab Rahman R
- Abayasinghe C
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- Abdur-Rahman L
- Abeloos J
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- Zou X
- Zoulamoglou M
- Zsisku L
- Publication venue
- 'Oxford University Press (OUP)'
- Publication date
- 01/01/2016
- Field of study
BACKGROUND: As global initiatives increase patient access to surgical treatments, there remains a need to understand the adverse effects of surgery and define appropriate levels of perioperative care. METHODS: We designed a prospective international 7-day cohort study of outcomes following elective adult inpatient surgery in 27 countries. The primary outcome was in-hospital complications. Secondary outcomes were death following a complication (failure to rescue) and death in hospital. Process measures were admission to critical care immediately after surgery or to treat a complication and duration of hospital stay. A single definition of critical care was used for all countries. RESULTS: A total of 474 hospitals in 19 high-, 7 middle- and 1 low-income country were included in the primary analysis. Data included 44 814 patients with a median hospital stay of 4 (range 2-7) days. A total of 7508 patients (16.8%) developed one or more postoperative complication and 207 died (0.5%). The overall mortality among patients who developed complications was 2.8%. Mortality following complications ranged from 2.4% for pulmonary embolism to 43.9% for cardiac arrest. A total of 4360 (9.7%) patients were admitted to a critical care unit as routine immediately after surgery, of whom 2198 (50.4%) developed a complication, with 105 (2.4%) deaths. A total of 1233 patients (16.4%) were admitted to a critical care unit to treat complications, with 119 (9.7%) deaths. Despite lower baseline risk, outcomes were similar in low- and middle-income compared with high-income countries. CONCLUSIONS: Poor patient outcomes are common after inpatient surgery. Global initiatives to increase access to surgical treatments should also address the need for safe perioperative care. STUDY REGISTRATION: ISRCTN5181700
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
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- CUAUTLE E
- CUNQUEIRO L
- CUVELAND J
- DA LUZ H
- DA SILVA AC
- DAHMS T
- DAINESE A
- DANI S
- DANISCH MC
- DANU A
- DAS D
- DAS I
- DAS S
- DASH A
- DASH S
- DE S
- DEGENHARDT HF
- DEISTING A
- DELOFF A
- DELSANTO S
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- GORBUNOV S
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- HARTON A
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- HAYASHI S
- HECKEL ST
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- 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
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- HUTTER D
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- 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
- PISANO S
- PIYARATHNA DB
- PLANINIC M
- PLIQUETT F
- PLOSKON M
- PLUTA J
- POCHYBOVA S
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- POZDNIAKOV V
- PRASAD SK
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- PUCCIO M
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- RAJPUT S
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- RASANEN SS
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- READ KF
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- REHMAN A
- REICHELT P
- REIDT F
- REN X
- RENFORDT R
- RESHETIN A
- REVOL JP
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- RIABOV V
- RICHERT T
- RICHTER M
- RIEDLER P
- RIEGLER W
- RIGGI F
- RINELLA GA
- RISTEA C
- 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
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- 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 105 km 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
- Adamová 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
- Antičić T
- Antonioli P
- Anwar R
- Apadula N
- Aphecetche L
- Appelshäuser H
- Arcelli S
- Arnaldi R
- Arnold OW
- Arratia M
- Arsene IC
- Arslandok M
- Augustinus A
- Averbeck R
- Azmi MD
- Badalà 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
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- Voloshin K
- Voloshin SA
- Volpe G
- von Haller B
- Vorobyev I
- Voscek D
- Vranic D
- Vrláková J
- Vázquez Doce O
- Vértesi 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
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- Zinovjev G
- Zmeskal J
- Zou S
- Závada P
- Šafařík K
- Šefčík M
- Šumbera M
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/02/2019
- Field of study
Flow Dominance and Factorization of Transverse Momentum Correlations in Pb-Pb Collisions at the LHC
- Author
- Adam J
- Adamova D
- Aggarwal MM
- Agnello M
- Agrawa N
- Ahammed Z
- Ahmad S
- 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
- Altinpinar S
- Altsy-Beev 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
- 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 O Villalobos
- Bala R
- Balbastre G Conesa
- Baldisseri A
- 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
- Blau D
- Blume C
- Bock F
- Bogdanov A
- Boldizsar L
- Bombara M
- Bonora M
- Book J
- Bore H
- Borissov A
- Borri M
- Botta E
- Bourjau C
- Braun-Munzingerm R
- 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
- 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
- Cerkala J
- 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
- Crkovska J
- Crochet P
- Cruz Albino R
- Cuautle E
- Cunqueiro L
- Da Costa H Pereira
- da Luz H Natal
- Da Silva AC Oliveira
- 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
- Doenigus B
- Domenicis Gimenez D
- Dordic O
- Drozhzhova T
- Dubey AK
- Dubla A
- Ducroux L
- Duggal AK
- Dupieux P
- Ehlers RJ
- Elia D
- Elstrup H
- Endress E
- Engel H
- Epple E
- Erazmus B
- Erhardt F
- Espagnon B
- Esumi S
- Eulisse G
- Eum J
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- Yokoyama H
- Yoo I-K
- Yoon JH
- Yurchenko V
- Zaccolo V
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- Zanoli HJC
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- Zimmermann MB
- Zimmermann S
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- Zmeskal J
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2017
- Field of study
We present the first measurement of the two-particle transverse momentum differential correlation function, P2≡ ΔpTΔpT/ pT2, in Pb-Pb collisions at sNN=2.76 TeV. Results for P2 are reported as a function of the relative pseudorapidity (Δη) and azimuthal angle (Δφ) between two particles for different collision centralities. The Δφ dependence is found to be largely independent of Δη for |Δη|≥0.9. In the 5% most central Pb-Pb collisions, the two-particle transverse momentum correlation function exhibits a clear double-hump structure around Δφ=π (i.e., on the away side), which is not observed in number correlations in the same centrality range, and thus provides an indication of the dominance of triangular flow in this collision centrality. Fourier decompositions of P2, studied as a function of the collision centrality, show that correlations at |Δη|≥0.9 can be well reproduced by a flow ansatz based on the notion that measured transverse momentum correlations are strictly determined by the collective motion of the system
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
- Anwar R
- Aphecetche L
- Appelshaeuser H
- Arcelli S
- Arnaldi R
- Arnold OW
- Arsene IC
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- Audurier B
- Augustinus A
- Averbeck R
- Azmi MD
- Badala A
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- Baillie O Villalobos
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- Hippolyte B
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- Yoo I-K
- Yoon JH
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- Zanoli HJC
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2017
- Field of study
The production of K∗(892)0 and φ(1020) mesons in proton-proton (pp) and lead-lead (Pb-Pb) collisions
at √sNN = 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 K∗(892)0 and φ(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 K∗(892)0/K ratio exhibits significant reduction from pp to central Pb-Pb collisions,
consistent with the suppression of the K∗(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 φ(1020)/π and K∗(892)0/π ratios show an
enhancement over pp collisions for pT ≈ 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 K∗(892)0 and φ(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
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
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- Anguelov V
- Anson C
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- Appelshauser H
- Arcelli S
- Arnaldi R
- Arnold OW
- Arsene IC
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- Audurier B
- Augustinus A
- Averbeck R
- Azmi MD
- Badala A
- Baek YW
- Bagnasco S
- Bailhache R
- Baillie O Villalobos
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- Barnafoldi GG
- Barnby LS
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- Barroso V Chibante
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- Behera NK
- Belikov I
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- Beltran LGE
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- Heckel ST
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- Hippolyte B
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- Hohlweger B
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- Humanic TJ
- Hussain N
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- Inaba M
- Ippolitov M
- Irfan M
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- Islam MS
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- Izucheev V
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- Jadhav MB
- Jadlovska S
- Jadlovsky J
- Jaelani S
- 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
- Kim J
- Kim JS
- Kim M
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- Kim S
- Kim T
- Kirsch S
- Kisel I
- Kiselev S
- Kisiel A
- Kiss G
- Klay JL
- Klein C
- Klein J
- Klein-Boesing C
- Klewin S
- Kluge A
- Knichel ML
- Knospe AG
- Kobdaj C
- Kofarago M
- Kollegger T
- Kolojvari A
- Kondratiev V
- Kondratyeva N
- Kondratyuk E
- Konevskikh A
- Kopcik M
- Kour M
- Kouzinopoulos C
- Kovalenko O
- Kovalenko V
- Kowalski M
- Kralik I
- Kravcakova A
- Krivda M
- Krizek F
- Kryshen E
- Krzewicki M
- Kubera AM
- Kucera V
- Kuhn C
- Kuijer PG
- Kumar A
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- Kumar L
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- Kundu S
- Kurashvili P
- Kurepin A
- Kurepin AB
- Kuryakin A
- Kushpil S
- Kweon MJ
- Kwon Y
- La Pointe SL
- La Rocca P
- Lagana Fernandes C
- Lakomov I
- Langoy R
- Lapidus K
- Lara C
- Lardeux A
- Lattuca A
- Laudi E
- Lavicka R
- Lazaridis L
- Lea R
- Leardini L
- Lee S
- Lehas F
- Lehner S
- Lehrbach J
- Lemmon C
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- Yokoyama H
- Yoo I-K
- Yoon JH
- Yurchenko V
- Zaccolo V
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- Zampolli C
- Zanoli HJC
- Zardoshti N
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- Zavada P
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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/ψ yield and average transverse momentum as a function of charged-particle pseudorapidity density dNch/dη in p–Pb 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/ψ 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/ψ production at forward rapidity with respect to backward rapidity for increasing charged-particle multiplicity
First measurement of jet mass in Pb-Pb and p-Pb collisions at the LHC
- Author
- Acharya S
- Adamova D
- Aggarwal MM
- Agnello M
- Agrawal N
- Ahammed Z
- Ahmad N
- Ahn SU
- Aiola S
- Akindinov A
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- Albuquerque DSD
- Aleksandrov D
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- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2018
- Field of study
This letter presents the first measurement of jet mass in Pb–Pb and p–Pb 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 Pb–Pb collisions is compared to the jet mass as measured in p–Pb reference collisions, to vacuum event generators, and to models including jet quenching. It is observed that the jet mass in central Pb–Pb collisions is consistent within uncertainties with p–Pb reference measurements. Furthermore, the measured jet mass in Pb–Pb collisions is not reproduced by the quenching models considered in this letter and is found to be consistent with PYTHIA expectations within systematic uncertainties
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