57 research outputs found
Conservation of Mediterranean oak woodlands: understorey dynamics under different shrub management
- Author
- A Bonet
- A Troumbis
- AB Carvalhosa
- AE Magurran
- AV PĂ©rez Latorre
- B Ramos Solano
- C Hoff
- C PapiĂł
- C Quilchano
- C Raunkjaer
- CA Thanos
- Carla Pinto-Cruz
- CĂĄtia Canteiro
- F Pulido
- FJ Pulido
- G Moreno
- G Scarascia-Mugnozza
- GE Overbeck
- IM PĂ©rez-Ramos
- J Blondel
- J Maroco
- JA Franco
- JA Franco
- JE Keeley
- JM Cable
- JM GĂ©hu
- L Calvo
- L Croitoru
- L Trabaud
- Luiz Gazarini
- M Martin Bolaños
- M. Paula SimÔes
- MD EspĂrito-Santo
- ME Figueroa
- MP Eichhorn
- MP SimÔes
- MP SimÔes
- N MontĂšs
- P Garcia-Fayos
- R Joffre
- R TĂĄrrega
- S Lavorel
- T Pinto-Correia
- T Plieninger
- T Plieninger
- T Plieninger
- TA White
- TE Fulbright
- V Andreu
- WH Schlesinger
- Ă TavĆanoÄlu
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 05/02/2011
- Field of study
The effect of experimental disturbances
on the dynamics of a shrub community was studied
on a âMontadoâ ecosystem, in southern Portugal. The
evolution of the community physiognomy, composition
and diversity were monitored after shrub clearing
followed by biomass removal, deposition on soil
surface and incorporation with the soil, over a 9-year
period. Maximum shrub density was recorded in the
first year after the disturbances, excepting in mulched
plots which showed the greatest number of individuals
1 year later. The increment of shrub leaf biomass
was very fast in the first 3 years, whereas wood
production was slower but occurred along the whole
study period. At the end of the study, leaf and wood
biomass was still significantly lower than in the predisturbance
situation. The variation pattern of leaf
area index was similar to that of leaf biomass. The
evolution of total plant cover and diversity was
similar across treatments. The highest species richness
and diversity were recorded 2 years after
cutting, decreasing afterwards with the increasing
dominance of shrubs. Thus it seems likely that,
although a 9 year period is too short for these
communities to reach steady equilibrium, they are
very resistant and resilient to disturbances, as regeneration
was fast and vegetation dynamics was not
influenced by differences among treatments. We can
conclude that shrub clearing promotes biodiversity
and the time of permanence of shrub patches depends
on the particular goal we want to achieve
Conservation of Mediterranean oak woodlands: understorey dynamics under different shrub management
- Author
- CĂĄtia Canteiro
- Carla Pinto-Cruz
- M. Paula SimÔes
- Luiz Gazarini
- V Andreu
- J Blondel
- A Bonet
- JM Cable
- L Calvo
- AB Carvalhosa
- L Croitoru
- MP Eichhorn
- MD EspĂrito-Santo
- ME Figueroa
- JA Franco
- JA Franco
- TE Fulbright
- P Garcia-Fayos
- JM GĂ©hu
- C Hoff
- R Joffre
- JE Keeley
- S Lavorel
- AE Magurran
- J Maroco
- M Martin Bolaños
- N MontĂšs
- G Moreno
- GE Overbeck
- C PapiĂł
- AV PĂ©rez Latorre
- IM PĂ©rez-Ramos
- T Pinto-Correia
- T Plieninger
- T Plieninger
- T Plieninger
- F Pulido
- FJ Pulido
- C Quilchano
- B Ramos Solano
- C Raunkjaer
- G Scarascia-Mugnozza
- WH Schlesinger
- MP SimÔes
- MP SimÔes
- R TĂĄrrega
- Ă TavĆanoÄlu
- CA Thanos
- L Trabaud
- A Troumbis
- TA White
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 05/02/2011
- Field of study
The effect of experimental disturbances
on the dynamics of a shrub community was studied
on a âMontadoâ ecosystem, in southern Portugal. The
evolution of the community physiognomy, composition
and diversity were monitored after shrub clearing
followed by biomass removal, deposition on soil
surface and incorporation with the soil, over a 9-year
period. Maximum shrub density was recorded in the
first year after the disturbances, excepting in mulched
plots which showed the greatest number of individuals
1 year later. The increment of shrub leaf biomass
was very fast in the first 3 years, whereas wood
production was slower but occurred along the whole
study period. At the end of the study, leaf and wood
biomass was still significantly lower than in the predisturbance
situation. The variation pattern of leaf
area index was similar to that of leaf biomass. The
evolution of total plant cover and diversity was
similar across treatments. The highest species richness
and diversity were recorded 2 years after
cutting, decreasing afterwards with the increasing
dominance of shrubs. Thus it seems likely that,
although a 9 year period is too short for these
communities to reach steady equilibrium, they are
very resistant and resilient to disturbances, as regeneration
was fast and vegetation dynamics was not
influenced by differences among treatments. We can
conclude that shrub clearing promotes biodiversity
and the time of permanence of shrub patches depends
on the particular goal we want to achieve
Conservation of Mediterranean oak woodlands: understorey dynamics under different shrub management
- Author
- A Bonet
- A Troumbis
- AB Carvalhosa
- AE Magurran
- AV PĂ©rez Latorre
- B Ramos Solano
- C Hoff
- C PapiĂł
- C Quilchano
- C Raunkjaer
- CA Thanos
- Carla Pinto-Cruz
- CĂĄtia Canteiro
- F Pulido
- FJ Pulido
- G Moreno
- G Scarascia-Mugnozza
- GE Overbeck
- IM PĂ©rez-Ramos
- J Blondel
- J Maroco
- JA Franco
- JA Franco
- JE Keeley
- JM Cable
- JM GĂ©hu
- L Calvo
- L Croitoru
- L Trabaud
- Luiz Gazarini
- M Martin Bolaños
- M. Paula SimÔes
- MD EspĂrito-Santo
- ME Figueroa
- MP Eichhorn
- MP SimÔes
- MP SimÔes
- N MontĂšs
- P Garcia-Fayos
- R Joffre
- R TĂĄrrega
- S Lavorel
- T Pinto-Correia
- T Plieninger
- T Plieninger
- T Plieninger
- TA White
- TE Fulbright
- V Andreu
- WH Schlesinger
- Ă TavĆanoÄlu
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Worldwide comparison of survival from childhood leukaemia for 1995â2009, by subtype, age, and sex (CONCORD-2): a population-based study of individual data for 89â828 children from 198 registries in 53 countries
- Author
- Ab Manan A
- Abdel-Rahman M
- Adamcik J
- Agius D
- Aitken J
- Al Khater Ahm
- Al-Eid H
- Aleinikova Ov
- Allemani C
- Allemani Claudia
- Almar E
- Almon L
- Alonso R
- Alverson J
- Antunes L
- Ardanaz Ee
- Arias-Ortiz Ne
- Arveux P
- Asquez Ra
- Autelitano M
- Azevedo e Silva G
- Bah E
- Baili P
- Baker D
- Bannon F
- Bara S
- Barrios E
- Bastos J
- Bates J
- Bayakly Ar
- Bayo S
- Bella F
- Bento Mj
- Berrino F
- Bertrand C
- Bidaurrazaga J
- Bielska-Lasota M
- Black Rj
- Blaszczyk J
- Bolick Sw
- Bonaventure A
- Bonaventure Audrey
- Borchers R
- Bordoni A
- Bouchardy C
- Bouvier Am
- Bouvier V
- Bouzbid S
- Bradshaw D
- Bravo Le
- Bray F
- Brenner H
- Brewster Dh
- Brockhouse Jt
- Brown H
- Budroni M
- Bulliard Jl
- Busco S
- Calabrano Gh
- Caldarella A
- Calleja N
- Camey B
- Candela G
- Capocaccia R
- Carballo Quintero B
- Carreira H
- Carreira Helena
- Castaing M
- Cesaraccio R
- Chalker E
- Charlton Me
- Chen Jg
- Chen Js
- Chen Wq
- Cheng Lp
- Cheteri MB Keitheri
- Chiang Cj
- Chimedsuren O
- Chiolero A
- Chirlaque Md
- Cirilli C
- Clarke Ca
- Clavel J
- Clavel Jacqueline
- Coldman Aj
- Coleman Michel P
- Coleman Mp
- Colonna M
- Comber H
- Contiero P
- Contrino Ml
- Copeland Ge
- Cornet E
- Cowppli-Bony A
- Coza D
- Cremone L
- Cromartie B
- Cueva P
- Curado Mp
- Currow D
- Cusimano R
- Daniel C
- Daoprasert K
- Daoulas M
- De Angelis R
- de Oliveira E Lobo
- de Oliveira Jc
- De Souza Pcf
- Deapen D
- Degré D
- Dehler Si
- Dei Tos Ap
- Del Pino K
- Demers S
- Demetriou Av
- Devigili E
- Dewar Rad
- Di Carlo V
- Di Felice E
- Didkowska Ja
- Dimitrova N
- Diumenjo Mc
- Dong J
- Dyzmann-Sroka A
- DĂaz GarcĂa Jm
- Eberle A
- Edwards Bk
- Eisemann N
- El Mistiri Mm
- El Mistiri Mm
- Emrich K
- Engholm G
- Erb C
- Eser S
- Espinola Sb
- Espinoza Jr
- Ess Sm
- EstĂšve J
- Fabowale Null
- Faivre J
- Falcini F
- Fanetti Ac
- Farley S
- Farrugia H
- Federico M
- FernĂĄndez-Delgado R
- Ferretti S
- Finan P
- Fita R
- Fitzpatrick D
- Forjaz G
- Fournier E
- Frick H
- Fulton Jp
- Fusco M
- Galaz Jc
- Galceran J
- GalĂĄn Yh
- Ganry O
- Garcilazo Da
- Gatta G
- Gatta Gemma
- Gavin A
- Ge Hm
- Geater Sl
- Gentilini Ma
- George Jt
- Gershman St
- Giacciani Pl
- Giacomin A
- Giles Gg
- Giljahn L
- Glaser Sl
- Gola G
- GonzĂĄlez Ms
- Gradalska-Lampart M
- Green Ma
- Green Md
- Grosclaude P
- Gu Xp
- Guizard Av
- Guo Gp
- GĂłzdz S
- Hackl M
- Hamdi-Chérif M
- Hannah H
- Harewood R
- Harewood Rhea
- Harrelson Dg
- Hattori M
- Henau K
- Hendrix J
- Herget K
- Hernandez By
- Herrera Vm
- Herrmann C
- Herrmann Da
- Holleczek B
- Hood M
- Hosain Gm
- Hsieh Mc
- Huang B
- Huang Qh
- Huang Sq
- Hudson Ag
- Hurley Dm
- Huws Dw
- Ibañez Sg
- Innos K
- Ito H
- Jaidane L
- Janes Ta
- Jaramillo L
- Jayalekshmi Pa
- Johnson Cj
- Jozwik D
- Jung Kw
- Jurado Dm
- JĂ©gu J
- Kahn Ar
- Kaizaki Y
- Kajueter H
- Kanemura S
- Kataki Ac
- Katalinic A
- Katayama K
- Keinan-Boker L
- Kepska K
- Key C
- Khan S
- Kieschke J
- Knowlton Rc
- Koike T
- Konzelmann I
- Krishnatreya M
- Kuehni Ce
- Kuehni Claudia E
- Kumar E
- Kumar V
- Kumcher I
- Kwiatkowska K
- La Rosa F
- Lai Ms
- Lalany A
- Lambe M
- Lanza Mf
- Laporte C
- LapĂŽtre-Ledoux B
- Larrañaga N
- LarĂžnningen S
- Laspada Wd
- Latorre Mrdo
- Launoy G
- Laura Ea
- Le Guyader-Peyrou S
- Lemons D
- Leung G
- Lewis C
- Li Ql
- Li W
- Liepina E
- Lillini R
- Lima Ca
- Liu K
- Liu L
- Louchini R
- Lynch Cf
- Macintyre M
- Mackinnon Ja
- Malila N
- Malle B
- Mang Wk
- Manraj Ss
- Marcos Ai
- Marcos-Gragera R
- Marcos-Gragera Rafael
- Marrett L
- Martin J
- MartĂnez-Reyes F
- Maspero S
- Maspoli-Conconi M
- Mateos A
- Matsuda T
- Matthes Kl
- Matz M
- Maule Mm
- Maurina A
- Mayer-da-Silva A
- Maynadié M
- Mazzoleni G
- Mazzucco W
- Mcclure C
- Mccrate Fr
- Melo Cd
- Mezyk R
- Michiara M
- Miranda A
- Miyashiro I
- Mokni M
- Molina E
- Molinié F
- Monnereau A
- Montel L
- Montserrat M Ramos
- Moreno F
- Moreno-Iribas Cc
- Mounier M
- Moya Ja
- Mueller L
- Murphy Mfg
- Murphy Michael F G
- MĂ€gi M
- MĂžller B
- MĂŒhlböck H
- Nakagawa H
- Nandakumar A
- Narimatsu H
- Navarro C
- Nennecke A
- Newman L
- Ngan Kc
- Nikiforuk C
- NikĆĄiÄ M
- Nimri O
- Nishri De
- Nogueira Lm
- Noonan G
- Nortje Sh
- O'Brien Dk
- Oberaigner W
- Ogunbiyi Oj
- Oki I
- Pannozzo F
- Pascucci C
- Pate A
- Pathy N Bhoo
- Patil M
- Pavlou P
- Pawlish Ks
- Peake M
- Peris-Bonet R
- Peris-Bonet Rafael
- Phillips C
- Piffer S
- Piñeros M
- Piñeros Marion
- Pongnikorn D
- Primic-Ćœakelj M
- PĂ©rez-Meza Ml
- Quinto R
- QuirĂłs Jr
- Rachet B
- Radziszewska Au
- Rao C
- Rashbass J
- Rees Jr
- Rego Ra
- Ricci P
- Richards J
- Robb Ki
- Rogers Db
- Rosso S
- Rousseau Dl
- Rubertone Jj
- Ruta M
- Ryan S
- Rycroft R
- Sacchetto L
- Sacerdote C
- Safaei Diba C
- Sant M
- Sant Milena
- Sanz N
- Sapkota Sd
- Sassi F
- Scandiuzzi C
- Schindler M
- Schubert Ss
- Schwartz Ag
- Schwartz Sm
- Schymura Mj
- Scott C
- Scuderi T
- Sebastian P
- SeppÀ K
- Serraino D
- Sewpaul-Sungkur R
- Sgargi P
- Shack L
- Shen X
- Shen Y
- Shibata A
- Siesling S
- Silva Ma
- Silverman Bg
- Sirri E
- Slack Sj
- Smailyte G
- Soeberg Mj
- Somdyala Nim
- Song Gh
- Spika D
- Spika Devon
- Spitale A
- Sriplung H
- Stabenow R
- Stare J
- Stefan Daniela C
- Stefan Dc
- Stephens R
- Stephenson L
- Stern K
- Stiller Ca
- Stiller Charles A
- Stokes Bc
- Storm H
- Stracci F
- Stroup A
- Stuart-Panko H
- Sugiyama H
- Sundseth H
- Sureda P Franch
- Sutera A
- Suwanrungruang K
- Suzanna E
- Swaminathan R
- Swaminathan R
- Sweeney C
- SĂĄnchez Mj
- Tagliabue G
- Tanaka Lf
- Tang Jg
- Threlfall T
- Tisano F
- Todescu Ai
- Torres P
- Torres-CintrĂłn Cr
- Tortolero-Luna G
- Trojanowski M
- Troussard X
- TryggvadĂłttir L
- Trétarre B
- Tucker Tc
- Tumino R
- Turner D
- Tuvshingerel S
- Uribe Cj
- Usala M
- Usel M
- Utada M
- Valerianova Z
- Valkov My
- Van Eycken L
- Vargas S
- Velten M
- Veneziano Cla
- Veneziano Db
- Venn A
- Vercelli M
- Verma Y
- Vicentini M
- Vigneau F
- Vilardell Gil Ml
- Visser O
- Vitale Mf
- Vitarelli S
- Vriends Ka
- Walsh Pm
- Wang J
- Wang N
- Wang S
- Ward Kc
- Warther B
- Wei K
- Weir Hk
- West D
- White C
- Whiteside Ma
- Wiangnon S
- Wiggins C
- Williamson Ll
- Wohler B
- Wojciechowska U
- Won Yj
- Woods Rr
- Woronoff As
- Wright S
- Wu Xc
- Yakut Ci
- Yang L
- Yang Xp
- Yoshii M
- You H
- YĂ©pez Jg
- YĂ©pez Mc
- Zaidi Z
- Zanetti R
- Zborovskaya Aa
- Zeissig Sr
- Zeng H
- Zhang B
- Zhang Jh
- Zhang P
- Zhao Dl
- Zhu Fd
- Zorzi M
- Zucchetto A
- ZvolskĂœ M
- ĂlafsdĂłttir Ej
- Ć ekerija M
- Ćœagar T
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2017
- Field of study
Background Global inequalities in access to health care are reflected in differences in cancer survival. The CONCORD programme was designed to assess worldwide differences and trends in population-based cancer survival. In this population-based study, we aimed to estimate survival inequalities globally for several subtypes of childhood leukaemia.
Methods Cancer registries participating in CONCORD were asked to submit tumour registrations for all children aged 0-14 years who were diagnosed with leukaemia between Jan 1, 1995, and Dec 31, 2009, and followed up until Dec 31, 2009. Haematological malignancies were defined by morphology codes in the International Classification of Diseases for Oncology, third revision. We excluded data from registries from which the data were judged to be less reliable, or included only lymphomas, and data from countries in which data for fewer than ten children were available for analysis. We also excluded records because of a missing date of birth, diagnosis, or last known vital status. We estimated 5-year net survival (ie, the probability of surviving at least 5 years after diagnosis, after controlling for deaths from other causes [background mortality]) for children by calendar period of diagnosis (1995-99, 2000-04, and 2005-09), sex, and age at diagnosis (< 1, 1-4, 5-9, and 10-14 years, inclusive) using appropriate life tables. We estimated age-standardised net survival for international comparison of survival trends for precursor-cell acute lymphoblastic leukaemia (ALL) and acute myeloid leukaemia (AML).
Findings We analysed data from 89 828 children from 198 registries in 53 countries. During 1995-99, 5-year agestandardised net survival for all lymphoid leukaemias combined ranged from 10.6% (95% CI 3.1-18.2) in the Chinese registries to 86.8% (81.6-92.0) in Austria. International differences in 5-year survival for childhood leukaemia were still large as recently as 2005-09, when age-standardised survival for lymphoid leukaemias ranged from 52.4% (95% CI 42.8-61.9) in Cali, Colombia, to 91.6% (89.5-93.6) in the German registries, and for AML ranged from 33.3% (18.9-47.7) in Bulgaria to 78.2% (72.0-84.3) in German registries. Survival from precursor-cell ALL was very close to that of all lymphoid leukaemias combined, with similar variation. In most countries, survival from AML improved more than survival from ALL between 2000-04 and 2005-09. Survival for each type of leukaemia varied markedly with age: survival was highest for children aged 1-4 and 5-9 years, and lowest for infants (younger than 1 year). There was no systematic difference in survival between boys and girls.
Interpretation Global inequalities in survival from childhood leukaemia have narrowed with time but remain very wide for both ALL and AML. These results provide useful information for health policy makers on the effectiveness of health-care systems and for cancer policy makers to reduce inequalities in childhood survival
A922 Sequential measurement of 1 hour creatinine clearance (1-CRCL) in critically ill patients at risk of acute kidney injury (AKI)
- Author
- Abbott TE
- Abdallah RI
- Abdel-Aal IR
- Abdelmonem SA
- Abdo WF
- Abellan AN
- AbellĂĄn AN
- AbellĂĄn AN
- AbellĂĄn AN
- Abrams ST
- Ackerley C
- Acuña M
- Adda M
- Adhikari NK
- Adriano G
- Adrie C
- Affatato R
- Affatato R
- Afonso-Rivero D
- Agarossi A
- Agarwal LK
- Ageeva T
- Agrawal R
- Aguayo-DeHoyos E
- Aguilar AL
- Aguilar-Alonso E
- Aguilar-Alonso E
- Aguilar-Alonso E
- Aguirregabyria M
- Ahmadnia E
- Ahn C
- Ahn JY
- Ahn JY
- Ahn MY
- Ahn MY
- Aitken LM
- Akalaev R
- Akbarzadeh A
- Akcan-Arikan A
- Akhlagh SH
- Akhtar N
- AKI Research Group
- Akiduki N
- Akin S
- Akizuki N
- Akkoc T
- Ala-Kokko T
- Alanio A
- Albaiceta GM
- Albaladejo P
- Alberto F
- Albuisson E
- Alcala MA
- AlcĂĄzar L
- Aldabo-Pallas T
- Aldana NN
- Aldecoa C
- AlegrĂa L
- Alejandro R
- Alejo GC
- Alejos RM
- Alexandrova E
- Algarte R
- Algarte R
- Algieri I
- Algora-Weber A
- Alhamdi Y
- Aliaga FA
- Aliberti S
- Alkan A
- Almudena PM
- Almudevar PM
- Almudevar PM
- Almudévar PM
- Altıntas ND
- Alvarez J
- Alves SC
- Alzola LM
- Amargianitakis V
- Amaro R
- Amato MB
- Ambler M
- Amerongen MP
- Amininejad T
- Amor LL
- Amorim V
- Anand RK
- Andersen LW
- Andersson S
- Andoh K
- Andrade AH
- Andrade AH
- Andrade AH
- Andrade G
- Andreis DT
- Andreis DT
- Annane D
- Antonelli M
- Antoniadou A
- Antonio C
- Antonucci E
- AntĂłn DG
- Anzueto A
- Appiani F
- Aquevedo A
- Aragon C
- Araujo NJ
- Araujo VF
- ARIAM registry of adult cardiac surgery
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- Arias CC
- Arias N
- Arias-Verdu MD
- Arias-Verdu MD
- Arias-Verdu MD
- Armaganidis A
- Arora MK
- Arora N
- Arrigo M
- Arslantas MK
- Artiguenave M
- Aslanian P
- Aspide R
- Asyralyyeva G
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- Ataman S
- Atchade E
- Atchade E
- Atchasiri S
- Athapattu P
- Atkins G
- Aublanc M
- Aublanc M
- Augustin P
- Augustin P
- Auquier P
- Avilés-Jurado FX
- Avramidis V
- Ayala LY
- Aydin M
- Azevedo JC
- Azevedo JR
- Aznar GP
- Babalis D
- Babini G
- Bachli EB
- Bader A
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- Baidya DK
- Baikova VN
- Bakker J
- BalcĂĄzar LC
- BalcĂĄzar LC
- Baldassarri R
- Baldwin CE
- Balik M
- Ball I
- Ballin A
- Balsera B
- Banderas-Bravo ME
- Banderas-Bravo ME
- Bandert A
- Bangstad IL
- Baptista N
- Baquero JD
- Barbadillo S
- Barberet G
- Barberet G
- Barberet G
- Barbier J
- Barcenilla F
- Barea-Mendoza JA
- Barinas OD
- Baron AV
- Barrachina LG
- Barral M
- Basile-Filho A
- Bassi GL
- Bates D
- Battistini M
- Bauer M
- Bauer PR
- Baumstarck K
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- Bawin M
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- Bañeras J
- Beane A
- Beduneau G
- Beduneau G
- Beduneau G
- Beeharry SD
- Beerepoot M
- Begzjav T
- Beishuizen A
- Bell C
- Belletti A
- Bellissimo-Rodrigues F
- Belloli A
- Bellomo R
- Bellver BQ
- Belmonte R
- Ben-Hamouda N
- Bendel S
- Bendel S
- Benyamina M
- Beretta S
- Berg R
- Bergantino B
- Berghmans J
- Bernal FF
- Berric A
- Berrutti D
- Berthelsen RE
- Bertini P
- Bertini P
- Berto MB
- Besevli SG
- Bestle MH
- Bettex D
- Bettex DA
- Beunders R
- Bhasin D
- Bhattal MK
- Bhide S
- Bianchi I
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- Bianzina S
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- Bishop J
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- FINNRESUSCI Study Group
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- IPREA Study Group
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- Japan Septic Disseminated Intravascular Coagulation (JSEPTIC DIC) study group
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- JSEPTIC (Japanese Society of Education for Physicians and Trainees in Intensive Care) Clinical Trial Group
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- MartĂn-Loeches I
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- Mercat A
- Mercat A
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- Merino-Vega D
- Messenger D
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- Midwinter MJ
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- Miguelena PR
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- Olaechea P
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- Picoita F
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- Shinotsuka CR
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- Stamm J
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- Suchomel P
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- Tomas E
- Tomas E
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- WIND study group
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- Young A
- Yu KM
- Yumoto T
- Yuzawa J
- Yuzawa J
- Zabaletta WJ
- Zabini D
- Zahorec M
- Zaien I
- Zakynthinos S
- Zanello M
- Zani D
- Zarantonello F
- Zayas B
- Zepeda EM
- Zeroual N
- Zerva L
- Zhang J
- Zhou JC
- Zhou JC
- Zhou JX
- Zhovnir V
- Zibandah N
- Zijlstra F
- Zimmerman J
- Zogheib E
- Zogheib E
- Zogheib E
- Zullino V
- Zwaag J
- ZĂœkovĂĄ I
- Ălvarez JT
- Ălvarez-Lerma F
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Meeting abstrac
Recommended from our members
Measurement of inclusive and differential cross sections for single top quark production in association with a W boson in proton-proton collisions at sâ = 13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdullin S
- Abercrombie D
- Abreu A
- Abu Zeid S
- Acharya H
- Acosta D
- Adam W
- Adamidis K
- Adams E
- Adams MR
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- Addesa FM
- Adloff C
- Adzic P
- Afanasiev S
- Agapitos A
- Agarwal G
- Agram J-L
- Aguilar-Benitez M
- Agyel D
- Ahmad A
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- AimĂš C
- Akchurin N
- Akgun B
- Akpinar A
- Albert A
- Albrecht A
- Albrecht S
- Albrow M
- Alcaraz Maestre J
- Alcerro Alcerro LF
- Aldaya Martin M
- AldĂĄ JĂșnior WL
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Allmond B
- Almond J
- Alpana A
- Alvarez Gonzalez B
- Alverson G
- Alves Gallo Pereira M
- Alves GA
- Aly R
- Alyari M
- Amapane N
- Ambrozas M
- Amendola C
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- Amram O
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- Apresyan A
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- Arcaro D
- Arcidiacono R
- Argiro S
- Arneodo M
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- Asenov P
- Asghar MI
- Asilar E
- Askew A
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- Assiouras P
- Assran Y
- Atakisi IO
- Attikis A
- Auffray E
- Aushev T
- Auzinger G
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- Zuolo D
- Zygala L
- Ălvarez FernĂĄndez A
- Publication venue
- Springer Nature
- Publication date
- 06/11/2022
- Field of study
A preprint version of the article is available at arXiv:2208.00924v2 [hep-ex], https://arxiv.org/abs/2208.00924v2 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables, including additional supplementary figures, can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/TOP-21-010 (CMS Public Pages). Report number: CMS-TOP-21-010, CERN-EP-2022-158.Measurements of the inclusive and normalised differential cross sections are presented for the production of single top quarks in association with a W boson in proton-proton collisions at a centre-of-mass energy of 13 TeV. The data used were recorded with the CMS detector at the LHC during 2016-2018, and correspond to an integrated luminosity of 138 fb^{â1}. Events containing one electron and one muon in the final state are analysed. For the inclusive measurement, a multivariate discriminant, exploiting the kinematic properties of the events is used to separate the signal from the dominant ttÂŻ background. A cross section of 79.2 ± 0.9 (stat) +7.7â8.0 (syst) ± 1.2 (lumi) pb is obtained, consistent with the predictions of the standard model. For the differential measurements, a fiducial region is defined according to the detector acceptance, and the requirement of exactly one jet coming from the fragmentation of a bottom quark. The resulting distributions are unfolded to particle level and agree with the predictions at next-to-leading order in perturbative quantum chromodynamics.SCOAP3
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Measurement of the Higgs boson production via vector boson fusion and its decay into bottom quarks in proton-proton collisions at sâ = 13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
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- Laha A
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- Papageorgakis C
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- Papavergou I
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- Piparo D
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- Polikarpov S
- Pompili A
- Pooth O
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- Postiau N
- Potenza R
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- Redondo Ferrero DD
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- Regnery B
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- Reichmann M
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- Reinsvold Hall A
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- Reitenspiess T
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- Roy Chowdhury S
- Roy D
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- Rudrabhatla S
- Ruini D
- Ruiz Alvarez JD
- Rumerio P
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- Ryu MS
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- Sadangi P
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- Saggio A
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- Saha NR
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- Sahasransu AR
- Sahin MĂ
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- Sert H
- Setti F
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- Sgaravatto M
- Sguazzoni G
- Shalaev V
- Shang V
- Sharma A
- Sharma A
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- Shchelina K
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- Smirnov V
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- Solano A
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- Sonnadara DUJ
- Sorrentino G
- Sosa Ricardo RE
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- Spiegel L
- Spiga D
- Spiropulu M
- Spitzbart D
- Sreelatha Pramod LP
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- Strautnieks NR
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- Strologas J
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- SĂĄnchez HernĂĄndez A
- SĂĄnchez Navas S
- Sözbilir Ă
- Tabarelli de Fatis T
- Tabb W
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- Takahashi Y
- Tali B
- Taliercio A
- Tamulaitis G
- Tani L
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- Tapper A
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- Tedeschi T
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- Teroerde M
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- Teryaev O
- Tews A
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- Tiras E
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- Tkaczyk S
- Tlisova I
- Tok UG
- Tomalin IR
- Toms M
- Tonelli G
- Tonjes MB
- Tornago M
- Toropin A
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- Tosi M
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- Townsend A
- Tramontano R
- Tran NV
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- Tricomi A
- Triossi A
- Trocino D
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- Tsoi HF
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- Ujvari B
- Ulmer KA
- Ulrich R
- Umoret G
- Uniyal R
- Uplegger L
- Urda GĂłmez L
- Uribe Estrada C
- Usai E
- Uslan E
- Uttley GP
- Uvarov L
- Uzunian A
- Vaandering EW
- Vage LH
- Vagnerini A
- Vai I
- Valencia Palomo L
- Valsecchi D
- Valuev V
- Van Den Bossche N
- van der Linden J
- Van Hove P
- Van Mechelen P
- Van Onsem GP
- Van Putte S
- Vanden Bemden M
- Vander Donckt M
- Vander Velde C
- Vanlaer P
- Vannerom D
- Varela J
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- Vargas Hernandez AM
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- Vazzoler F
- Veckalns V
- Veelken C
- Velasco M
- Velkovska J
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- Ventura Barroso A
- Ventura S
- Venturi A
- Verdier P
- Verdini PG
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- Vernazza E
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- Veszpremi V
- Vetens W
- Viazlo O
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- Viinikainen J
- Vila I
- Vilela Pereira A
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- Virdee T
- Virdi AK
- Vischia P
- Vitulo P
- Vizan Garcia JM
- Vlasov E
- Vlimant JR
- Vojinovic M
- Volobouev I
- Von Cube RF
- Vora J
- Vorobyev A
- Vourliotis E
- Voutilainen M
- Voytishin N
- VĂĄmi TĂ
- Wachirapusitanand V
- Wadud MA
- Wagner SR
- Walkingshaw Pass K
- Wallny R
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- Walter D
- Wanczyk J
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- Wang C
- Wang D
- Wang F
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- Wang J
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- Wang Q
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- Wang X
- Wang Z
- Warden A
- Wardle N
- Wassmer M
- Watson IJ
- Wayne M
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- Wei W
- Wen Y
- Wertz S
- West C
- Wezenbeek L
- Whitbeck A
- White R
- Wichmann K
- Wickramage N
- Wickramarathna DDC
- Wiedenbeck S
- Wieland S
- Wiens L
- Wightman A
- Williams A
- Williams T
- Willmott C
- Wilson G
- Wilson J
- Wimpenny S
- Winer BL
- Winterbottom D
- Wissing C
- Wittich P
- Wolf M
- Wolf R
- Wong K
- Wong WY
- Wood D
- Wozniak KA
- Wright D
- Wu HY
- Wuchterl S
- Wulansatiti M
- Wulz C-E
- Wunsch S
- Wyslouch B
- WĂŒrthwein F
- Xiang Y
- Xiao J
- Xiao M
- Xie S
- Xie W
- Yagil A
- Yalvac M
- Yan F
- Yan X
- Yang H
- Yang S
- Yang S
- Yang TJ
- Yang UK
- Yang Y
- Yang YC
- Yao Y
- Yarar H
- Yates BR
- Yazgan E
- Ye Z
- Yi K
- Yigitbasi E
- Yockey H
- Yohay R
- Yoo HD
- Yoo J
- Yoo J
- Yoon I
- You Z
- Yu D
- Yu I
- Yu SS
- Yuan L
- Yuan S
- Yuldashev BS
- Yumiceva F
- Yusuff I
- Zabi A
- Zacharopoulou A
- Zaleski S
- Zalewski P
- Zarubin A
- Zarucki M
- Zaza A
- Zecchinelli AG
- Zehetner P
- Zeinali M
- Zejdl P
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang W
- Zhang Y
- Zhang Y
- Zhizhin I
- Zhokin A
- Zhu RY
- Ziemons T
- Zilizi G
- Zimermmane Castro Santos A
- Zipper N
- Zisopoulos I
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zotz A
- Zou R
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Publication venue
- Springer Nature on behalf of SISSA
- Publication date
- 30/01/2024
- Field of study
A preprint version of the article is available at arXiv:2308.01253v2 [hep-ex], https://arxiv.org/abs/2308.01253v2 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/HIG-22-009 (CMS Public Pages). Report number: CMS-HIG-22-009, CERN-EP-2023-110.A measurement of the Higgs boson (H) production via vector boson fusion (VBF) and its decay into a bottom quark-antiquark pair (bbÂŻ) is presented using proton-proton collision data recorded by the CMS experiment at sâ = 13 TeV and corresponding to an integrated luminosity of 90.8 fbâ1. Treating the gluon-gluon fusion process as a background and constraining its rate to the value expected in the standard model (SM) within uncertainties, the signal strength of the VBF process, defined as the ratio of the observed signal rate to that predicted by the SM, is measured to be ÎŒqqHHbbÂŻ = 1.01 +0.55â0.46. The VBF signal is observed with a significance of 2.4 standard deviations relative to the background prediction, while the expected significance is 2.7 standard deviations. Considering inclusive Higgs boson production and decay into bottom quarks, the signal strength is measured to be ÎŒincl.HbbÂŻ = 0.99 +0.48â0.41, corresponding to an observed (expected) significance of 2.6 (2.9) standard deviations.SCOAP3, STFC; Marie-Curie program and the European Research Council and Horizon 2020 Gran
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Higher-order moments of the elliptic flow distribution in PbPb collisions at âsNN = 5.02 TeV
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- Ziemons T
- Zimermmane Castro Santos A
- Zipper N
- Zisopoulos I
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zotto P
- Zotz A
- Zou R
- Zucchetta A
- Zuo X
- Zuolo D
- Zygala L
- Ălvarez FernĂĄndez A
- Publication venue
- Springer Nature on behalf of SISSA
- Publication date
- 15/02/2024
- Field of study
A preprint version of the article is available at arXiv:2311.11370v2 [nucl-ex], https://arxiv.org/abs/2311.11370 .
Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/HIN-21-010 (CMS Public Pages).The hydrodynamic flow-like behavior of charged hadrons in high-energy lead-lead collisions is studied through multiparticle correlations. The elliptic anisotropy values based on different orders of multiparticle cumulants, v2{2k}, are measured up to the tenth order (k = 5) as functions of the collision centrality at a nucleon-nucleon center-of-mass energy of âsNN = 5.02 TeV. The data were recorded by the CMS experiment at the LHC and correspond to an integrated luminosity of 0.607 nbâ1. A hierarchy is observed between the coefficients, with v2{2}>v2{4}âłv2{6}âłv2{8}âłv2{10}. Based on these results, centrality-dependent moments for the fluctuation-driven event-by-event v2 distribution are determined, including the skewness, kurtosis and, for the first time, superskewness. Assuming a hydrodynamic expansion of the produced medium, these moments directly probe the initial-state geometry in high-energy nucleus-nucleus collisions.SCOAP3
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- Author
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- Aarup Petersen H
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- Zygala L
- Publication venue
- Springer Nature on behalf of SISSA
- Publication date
- 13/12/2023
- Field of study
A preprint version of the article is available at arXiv:2305.07998v2 [hep-ex], https://arxiv.org/abs/2305.07998v2 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/EXO-20-012 (CMS Public Pages). Report number: CMS-EXO-20-012, CERN-EP-2023-064.A search for resonances in events with the Îł+jet final state has been performed using proton-proton collision data collected at âs = 13 TeV by the CMS experiment at the LHC. The total data analyzed correspond to an integrated luminosity of 138 fbâ1. Models of excited quarks and quantum black holes are considered. Using a wide-jet reconstruction for the candidate jet, the Îł+jet invariant mass spectrum measured in data is examined for the presence of resonances over the standard model continuum background. The background is estimated by fitting the mass distribution with a functional form. The data exhibit no statistically significant deviations from the expected standard model background. Exclusion limits at 95% confidence level on the resonance mass and other parameters are set. Excited light-flavor quarks (excited bottom quarks) are excluded up to a mass of 6.0 (3.8) TeV. Quantum black hole production is excluded for masses up to 7.5 (5.2) TeV in the Arkani-Hamed-Dimopoulos-Dvali (Randall-Sundrum) model. These lower mass bounds are the most stringent to date among those obtained in the Îł+jet final state.SCOAP3
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Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at âs = 13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
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- Zisopoulos I
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zotz A
- Zou R
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Publication venue
- Elsevier
- Publication date
- 02/02/2024
- Field of study
Data availability:
Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS policy as stated in âCMS data preservation, re-use and open access policyâ available online at: https://cms-docdb.cern.ch/cgi-bin/PublicDocDB/RetrieveFile?docid=6032&filename=CMSDataPolicyV1.2.pdf&version=2 .A preprint of this article is available online at arXiv:2311.03261v2 [hep-ex] https://arxiv.org/abs/2311.03261v2 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/TOP-22-010 (CMS Public Pages)A search is presented for new Higgs bosons in proton-proton (pp) collision events in which a same-sign top quark pair is produced in association with a jet, via the pp â tH/A â ttÂŻc and pp â tH/A â ttÂŻu processes. Here, H and A represent the extra scalar and pseudoscalar boson, respectively, of the second Higgs doublet in the generalized two-Higgs-doublet model (g2HDM). The search is based on pp collision data collected at a center-of-mass energy of 13 TeV with the CMS detector at the LHC, corresponding to an integrated luminosity of 138 fbâ1. Final states with a same-sign lepton pair in association with jets and missing transverse momentum are considered. New Higgs bosons in the 200-1000 GeV mass range and new Yukawa couplings between 0.1 and 1.0 are targeted in the search, for scenarios in which either H or A appear alone, or in which they coexist and interfere. No significant excess above the standard model prediction is observed. Exclusion limits are derived in the context of the g2HDM.SCOAP3
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