921 research outputs found
Combined parameter and model reduction of cardiovascular problems by means of active subspaces and POD-Galerkin methods
- Author
- A Caiazzo
- A Logg
- A Manzoni
- A Morris
- A Pinkus
- AL Marsden
- CK Zarins
- D Forti
- D González
- Elías Cueto
- F Ballarin
- F Ballarin
- F Ballarin
- F Ballarin
- F Chinesta
- G Berkooz
- G Rozza
- GE Box
- Giovanni Stabile
- I Dryden
- J Kaipio
- Jean Duchon
- JL Devore
- JL Jefferson
- K Carlberg
- K McLeod
- M Barrault
- M Morris
- MD Buhmann
- MD Gunzburger
- N Metropolis
- P Chen
- P Chen
- P Frey
- Paul Constantine
- PG Constantine
- PG Constantine
- R Guibert
- RD Cook
- S Ravindran
- SA Brown
- T Lassila
- V Agoshkov
- V Agoshkov
- Vicky Y. Wang
- X Hu
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
In this chapter we introduce a combined parameter and model reduction methodology and present its application to the efficient numerical estimation of a pressure drop in a set of deformed carotids. The aim is to simulate a wide range of possible occlusions after the bifurcation of the carotid. A parametric description of the admissible deformations, based on radial basis functions interpolation, is introduced. Since the parameter space may be very large, the first step in the combined reduction technique is to look for active subspaces in order to reduce the parameter space dimension. Then, we rely on model order reduction methods over the lower dimensional parameter subspace, based on a POD-Galerkin approach, to further reduce the required computational effort and enhance computational efficiency
2 nd Brazilian Consensus on Chagas Disease, 2015
- Author
- Abad-Franch F
- Abad-Franch F
- Abad-Franch F
- Abad-Franch F
- Abad-Franch F
- Abílio Augusto Fragata Filho
- Acquatella H
- Akhavan D
- Alberto Novaes Ramos Jr.
- Alejandro Luquetti
- Alejandro Marcel Hasslocher-Moreno
- Alessandra Viana Cardoso
- Almeida EA
- Almeida EA
- Almeida EA
- Almeida EA
- Almeida-Filho OC
- Altclas J
- Altclas JD
- Alves RM
- Ana Maria Jansen
- Ana Yecê das Neves Pinto
- Andrade AL
- Andrade SG
- Andréa Silvestre de Sousa
- Angheben A
- Anis Rassi
- Anis Rassi Jr.
- Antonio Walter Ferreira
- Antônio Carlos Silveira
- Barcán L
- Baroldi G
- Barreto ML
- Bern C
- Bern C
- Bern C
- Bern C
- Bern C
- Bestetti RB
- Bestetti RB
- Bestetti RB
- Bitto C
- Bocchi EA
- Bocchi EA
- Bocchi EA
- Brener Z
- Brener Z
- Britto CC
- Brutus L
- Brücher BL
- Bua J
- Buekens P
- Camargo ME
- Camargo ME
- Camargo ME
- Camargo ME
- Campos SV
- Cançado JR
- Carlier Y
- Carlier Y
- CarlierI Y
- Carrasco HA
- Carvalho VB
- Castro AM
- Castro CN
- Castro I
- Cerisola JA
- Cerisola JA
- Chagas C
- Chiale PA
- Chiari E
- Chiari E
- Chiari E
- Chippaux JP
- Constança Felícia De Paoli de Carvalho Britto
- Cordova E
- Coura JR
- Coura JR
- Coura JR
- Coura JR
- Coura JR
- Coura JR
- Coura JR
- Cunha GP
- D'Albuquerque LA
- Dalmo Correia
- Davila DF
- Dayse Elisabeth Campos
- De Rissio AM
- Del Castilho M
- Dias E
- Dias JC
- Dias JC
- Dias JC
- Dias JC
- Dias JCP
- Dias JCP
- Dias JCP
- Dias JCP
- Dias JCP
- Dias JCP
- Dias JCP
- Dias JCP
- Dias JCP
- Dias JP
- Divina Seila de Oliveira Marques
- Drumond JAG
- Duhamel B
- Egler Chiari
- Eliane Dias Gontijo
- Eliane Furtado Moreira
- Eliane Lages Silva
- Eros Antonio de Almeida
- Fabbro DL
- Fabiane Scalabrini Pinto
- Ferguson MK
- Fernando Abad-Franch
- Ferreira AW
- Ferreira HO
- Ferreira HO
- Ferreira MS
- Fonseca FM
- Fragata Filho AA
- França LCM
- Freilij H
- Freitas H
- Freitas VL
- Gallerano RH
- Garcia S
- Garzon SA
- Gebrekristos HT
- Glaucia Manzan Queiroz Andrade
- Gontijo ED
- González-Tomé MI
- Guariento ME
- Heller E
- Herwaldt BL
- Higuchi ML
- Higuchi ML
- Higuchi ML
- Hijar G
- Hotez PJ
- Hotez PJ
- Howard EJ
- Ianni BM
- Inoue H
- Joffre Marcondes de Rezende
- José Antonio Marin-Neto
- José Renan da Cunha Melo
- José Rodrigues Coura
- João Carlos Pinto Dias
- Junqueira AC
- Jörg ME
- Júnior Rassi A
- Lana M
- Leeuwenburgh I
- Lima-Costa MF
- Livramento JA
- Lopes ER
- Lorosa ES
- Lugones HS
- Luquetti AO
- Luquetti AO
- Luquetti AO
- Luquetti AO
- Lúcia Maria da Cunha Galvão
- Macêdo VO
- Macêdo VO
- Mady C
- Maegawa FA
- Maguire JH
- Mahoney RT
- Mallimaci MC
- Maria Aparecida Shikanai-Yasuda
- Marin-Neto JA
- Marin-Neto JA
- Marin-Neto JA
- Marin-Neto JA
- Marin-Neto JA
- Martes ACB
- Martinelli Filho M
- Martins-Melo FR
- Martins-Melo FR
- Martins-Melo FR
- Martins-Melo FR
- Martins-Melo FR
- Martins-Melo FR
- Martins-Melo FR
- Mayara Maia Lima
- Medeiros MB
- Meier-Ruge WA
- Mendes EV
- Messenger LA
- Molina I
- Moncayo A
- Montera MW
- Moraes-Souza H
- Morais BB
- Morillo CA
- Mougabure-Cueto G
- Nishioka SA
- Nisida IV
- Norman FF
- Noya BA
- Noêmia Barbosa Carvalho
- Nóbrega AA
- Nóbrega AA
- Oliveira Júnior W
- Oliveira Júnior W
- Oliveira RB
- Ostermayer AL
- Ozaki Y
- Padilla-Torres SD
- Parada H
- Pasricha PJ
- Passos ADC
- Pazin-Filho A
- Pereira Barretto AC
- Perez-Ramirez L
- Pessoa GCA
- Pessoa GCA
- Pinazo MJ
- Pinotti HW
- Pinto AY
- Pinto AY
- Pinto AYN
- Pinto AYN
- Pinto AYN
- Portela-Lindoso AAB
- Porto CC
- Prata A
- Prata A
- Prata A
- Prata A
- Pérez-Ayala A
- Pérez-Molina JA
- Rafaella Albuquerque e Silva
- Ramos G
- Ramos Júnior AN
- Ramos Júnior AN
- Ramos Júnior AN
- Rassi A
- Rassi A
- Rassi Jr A
- Rassi Júnior A
- Rassi Júnior A
- Rassi Júnior A
- Rassi Júnior A
- Rassi Júnior A
- Reis-Neto JA
- Renato Vieira Alves
- Requena-Méndez A
- Rezende JM
- Riarte A
- Ribeiro dos Santos R
- Roberti RR
- Rocha A
- Rocha MOC
- Rodriguez-Salas LA
- Romaña C
- Roque AL
- Roque AL
- Rosália Morais Torres
- Roux E
- Roux E
- Russomando G
- Salas NA
- Salvatella R
- Samuel J
- Sangenis LH
- Santo AH
- Santos CB
- Sartori AM
- Scanavacca M
- Scapellato PG
- Schijman AG
- Schmunis GA
- Sebastião Aldo da Silva Valente
- Sergio Salles Xavier
- Shaw J
- Shikanai-Yasuda MA
- Shikanai-Yasuda MA
- Shikanai-Yasuda MA
- Silva CP
- Silvana Eloi Santos
- Silveira AC
- Silveira AC
- Silveira AC
- Silveira C
- Silveira JF
- Simone Monzani Vivaldini
- Simões MV
- Sosa Estani S
- Sosa-Estani S
- Sousa AA
- Sousa AS
- Souza DSM
- Spiess AE
- Spina-França A
- Stavropoulos SN
- Strasen J
- Suelene Mamede Oliveira
- Swanstrom LL
- Sánchez-Camargo CL
- Torrico F
- Valença-Barbosa C
- Ventura-Garcia L
- Vera da Costa Valente
- Veruska Maia da Costa
- Victora CG
- Victora CG
- Villela E
- Vinhaes MC
- Viotti R
- Viotti R
- Viotti RJ
- Voller A
- Wendell S
- Wilson de Oliveira Jr.
- Xavier SC
- Xavier SC
- Xavier SS
- Xavier SS
- Yun O
- Zicker F
- Zimerman LI
- Zingales B
- Zingales B
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- 01/01/2016
- Field of study
Abstract Chagas disease is a neglected chronic condition with a high burden of morbidity and mortality. It has considerable psychological, social, and economic impacts. The disease represents a significant public health issue in Brazil, with different regional patterns. This document presents the evidence that resulted in the Brazilian Consensus on Chagas Disease. The objective was to review and standardize strategies for diagnosis, treatment, prevention, and control of Chagas disease in the country, based on the available scientific evidence. The consensus is based on the articulation and strategic contribution of renowned Brazilian experts with knowledge and experience on various aspects of the disease. It is the result of a close collaboration between the Brazilian Society of Tropical Medicine and the Ministry of Health. It is hoped that this document will strengthen the development of integrated actions against Chagas disease in the country, focusing on epidemiology, management, comprehensive care (including families and communities), communication, information, education, and research
Combined measurement of differential and total cross sections in the H → γγ and the H → ZZ* → 4ℓ decay channels at s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- Abouzeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Gonzalez B
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aperio Bella L
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Atkin RJ
- Atkinson M
- Atlas Collaboration
- Atlay NB
- Augsten K
- Avolio G
- Avramidou R
- Axen B
- Ayoub MK
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Baines JT
- Bajic M
- Bakalis C
- Baker OK
- Bakker PJ
- Bakshi Gupta D
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barlow N
- Barnea R
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro Guimarães Da Costa J
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batlamous S
- Batley JR
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beattie MD
- Beau T
- Beauchemin PH
- Bechtle P
- Beck HC
- Beck HP
- Becker K
- Becker M
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Bell AS
- Bella G
- Bellagamba L
- Bellerive A
- Bellomo M
- Bellos P
- Belotskiy K
- Belyaev NL
- Benary O
- Benchekroun D
- Bender M
- Benekos N
- Benhammou Y
- Benhar Noccioli E
- Benitez J
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Bergeaas Kuutmann E
- Berger N
- Bergsten LJ
- Beringer J
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- Bernardi G
- Bernius C
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- Berta P
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- Bessidskaia Bylund O
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- Betti A
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- Cao T
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- Capeans Garrido MDM
- Caprini I
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- Capua M
- Carbone RM
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- Cardillo FC
- Carli I
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- Carlino G
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- Casadei D
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- Casha AF
- Casolino M
- Casper DW
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- Castillo Gimenez V
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- Ceradini F
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- Chafaq A
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- Chapman JD
- Charlton DG
- Chau CC
- Chavez Barajas CA
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- Chegwidden A
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- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
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- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cherkaoui El Moursli R
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
- Chiu YH
- Chizhov MV
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- Chouridou S
- Chow YS
- Christodoulou V
- Chu MC
- Chudoba J
- Chuinard AJ
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- Cinca D
- Cindro V
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- Citron ZH
- Citterio M
- Clark A
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- Clark PJ
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- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Coimbra AEC
- Colasurdo L
- Cole B
- Colijn AP
- Collot J
- Conde Muiño P
- Coniavitis E
- Connell SH
- Connelly IA
- Constantinescu S
- Conventi F
- Cooper-Sarkar AM
- Cormier F
- Cormier KJR
- Corradi M
- Corrigan EE
- Corriveau F
- Cortes-Gonzalez A
- Costa MJ
- Costanzo D
- Cottin G
- Cowan G
- Cox BE
- Crane J
- Cranmer K
- Crawley SJ
- Creager RA
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- Crescioli F
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- Crosetti G
- Crépé-Renaudin S
- Cueto A
- Cuhadar Donszelmann T
- Cukierman AR
- Curatolo M
- Czekierda S
- Czodrowski P
- Cúth J
- D'Amen G
- D'Auria S
- D'Eramo L
- D'Onofrio A
- D'Onofrio M
- Da Cunha Sargedas De Sousa MJ
- Da Via C
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dallaire F
- Dallapiccola C
- Dam M
- Damp J
- Dandoy JR
- Daneri MF
- Dang NP
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- Danninger M
- Dao V
- Darbo G
- Darmora S
- Dartsi O
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- Davey W
- David C
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- Davis DR
- Dawe E
- Dawson I
- De Asmundis R
- De Benedetti A
- De Castro S
- De Cecco S
- De Groot N
- De Jong P
- De La Torre H
- De Lorenzi F
- De Maria A
- De Pedis D
- De Salvo A
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- De Vasconcelos Corga K
- De Vivie De Regie JB
- De K
- Debenedetti C
- Dedovich DV
- Dehghanian N
- Del Gaudio M
- Del Peso J
- Delgove D
- Deliot F
- Delitzsch CM
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- Della Volpe D
- Delmastro M
- Delporte C
- Delsart PA
- Demarco DA
- Demers S
- Demichev M
- Denisov SP
- Denysiuk D
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Deterre C
- Dette K
- Devesa MR
- Deviveiros PO
- Dewhurst A
- Dhaliwal S
- Di Bello FA
- Di Ciaccio A
- Di Ciaccio L
- Di Clemente WK
- Di Donato C
- Di Girolamo A
- Di Micco B
- Di Nardo R
- Di Petrillo KF
- Di Simone A
- Di Sipio R
- Di Valentino D
- Diaconu C
- Diamond M
- Dias Do Vale T
- Dias FA
- Diaz MA
- Dickinson J
- Diehl EB
- Dietrich J
- Dimitrievska A
- Dingfelder J
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- Djama F
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- Djuvsland JI
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- Dobre M
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- Doglioni C
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- Dolezal Z
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- Doria A
- Dova MT
- Doyle AT
- Drechsler E
- Dreyer E
- Dreyer T
- Dris M
- Du Y
- Duarte-Campderros J
- Dubinin F
- Dubovsky M
- Dubreuil A
- Duchovni E
- Duckeck G
- Ducourthial A
- Ducu OA
- Duda D
- Dudarev A
- Dudder AC
- Duffield EM
- Duflot L
- Dumancic M
- Dumitriu AE
- Duncan AK
- Dunford M
- Duperrin A
- Duran Yildiz H
- Durglishvili A
- Duschinger D
- Dutta B
- Duvnjak D
- Dyndal M
- Dysch S
- Dziedzic BS
- Díez Cornell S
- Dührssen M
- Dülsen C
- Düren M
- Eckardt C
- Ecker KM
- Edgar RC
- Eifert T
- Eigen G
- Einsweiler K
- Ekelof T
- El Kacimi M
- El Kosseifi R
- Ellajosyula V
- Ellert M
- Ellinghaus F
- Elliot AA
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- Yusuff I
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- Zakharchuk N
- Zalieckas J
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeitnitz C
- Zeißner SV
- Zemaityte G
- Zeng JC
- Zeng Q
- Zenin O
- Zerwas D
- Zgubič M
- Zhang D
- Zhang DF
- Zhang F
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- Zhang L
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- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- Elsevier
- Publication date
- 01/01/2018
- Field of study
A combined measurement of differential and inclusive total cross sections of Higgs boson production is performed using 36.1 fb−1 of 13 TeV proton–proton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured H→γγ and H→ZZ*(→4ℓ event yields, which are combined taking into account detector efficiencies, resolution, acceptances and branching fractions. The total Higgs boson production cross section is measured to be 57.0−5.9 +6.0 (stat.) −3.3 +4.0 (syst.) pb, in agreement with the Standard Model prediction. Differential cross-section measurements are presented for the Higgs boson transverse momentum distribution, Higgs boson rapidity, number of jets produced together with the Higgs boson, and the transverse momentum of the leading jet. The results from the two decay channels are found to be compatible, and their combination agrees with the Standard Model predictions
Search for supersymmetry in events with four or more leptons in √s =13 TeV pp collisions with ATLAS
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Afik Y
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt SC
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Gonzalez B
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Anjos N
- Annovi A
- Antel C
- Antonelli M
- Antonov A
- Antrim DJ
- Anulli F
- Aoki M
- Aperio Bella L
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J
- Argyropoulos S
- Arik M
- Armbruster AJ
- Armitage LJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asquith L
- Assamagan K
- Astalos R
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
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- Ayoub MK
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Baines JT
- Bajic M
- Baker OK
- Bakker PJ
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barak L
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M
- Barkeloo JT
- Barklow T
- Barlow N
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro F
- Barreiro Guimarães da Costa J
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batley JR
- Battaglia M
- Bauce M
- Bauer F
- Bawa HS
- Beacham JB
- Beattie MD
- Beau T
- Beauchemin PH
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- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beermann TA
- Begalli M
- Begel M
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- Zinser M
- Ziolkowski M
- Zobernig G
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- zur Nedden M
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- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
Results from a search for supersymmetry in events with four or more charged leptons (electrons, muons and taus) are presented. The analysis uses a data sample corresponding to 36.1 fb −1 of proton-proton collisions delivered by the Large Hadron Collider at s √ =13 TeV and recorded by the ATLAS detector. Four-lepton signal regions with up to two hadronically decaying taus are designed to target a range of supersymmetric scenarios that can be either enriched in or depleted of events involving the production and decay of a Z boson. Data yields are consistent with Standard Model expectations and results are used to set upper limits on the event yields from processes beyond the Standard Model. Exclusion limits are set at the 95% confidence level in simplified models of General Gauge Mediated supersymmetry, where higgsino masses are excluded up to 295 GeV. In R -parity-violating simplified models with decays of the lightest supersymmetric particle to charged leptons, lower limits of 1.46 TeV, 1.06 TeV, and 2.25 TeV are placed on wino, slepton and gluino masses, respectively
Measurement of the t¯tZ and t¯tW cross sections in proton-proton collisions at √s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
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- Abbott DC
- Abdinov O
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- Abhayasinghe DK
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zibell A
- Zieminska D
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- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
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- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
A measurement of the associated production of a top-quark pair (t¯t) with a vector boson (W, Z) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1 fb−1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The t¯tZ and t¯tW production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are σt¯tZ=0.95±0.08stat±0.10syst pb and σt¯tW=0.87±0.13stat±0.14syst pb in agreement with the Standard Model predictions. The measurement of the t¯tZ cross section is used to set constraints on effective field theory operators which modify the t¯tZ vertex
Measurement of the tt¯tt¯ production cross section in pp collisions at √s=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abed Abud A
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Achkar B
- Adam Bourdarios C
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
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- Agaras MN
- Agarwala J
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- Aguilar-Saavedra JA
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- Ahmed WS
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- Aielli G
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- Alberghi GL
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- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
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- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
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- Anders JK
- Andrean SY
- Andreazza A
- Andrei V
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
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- Aparo MA
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- Booth CD
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- Boscherini D
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- Bouhova-Thacker EV
- Boumediene D
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- Breaden Madden WD
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- Zenin O
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- Zerwas D
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- Zhang DF
- Zhang G
- Zhang J
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- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 16/11/2021
- Field of study
A measurement of four-top-quark production using proton-proton collision data at a centre-of-mass energy of 13 TeV collected by the ATLAS detector at the Large Hadron Collider corresponding to an integrated luminosity of 139 fb−1 is presented. Events are selected if they contain a single lepton (electron or muon) or an opposite-sign lepton pair, in association with multiple jets. The events are categorised according to the number of jets and how likely these are to contain b-hadrons. A multivariate technique is then used to discriminate between signal and background events. The measured four-top-quark production cross section is found to be 26+17−15 fb, with a corresponding observed (expected) significance of 1.9 (1.0) standard deviations over the background-only hypothesis. The result is combined with the previous measurement performed by the ATLAS Collaboration in the multilepton final state. The combined four-top-quark production cross section is measured to be 24+7−6 fb, with a corresponding observed (expected) signal significance of 4.7 (2.6) standard deviations over the background-only predictions. It is consistent within 2.0 standard deviations with the Standard Model expectation of 12.0 ± 2.4 fb
Measurement and interpretation of same-sign W boson pair production in association with two jets in pp collisions at s = 13 TeV with the ATLAS detector
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- Zhemchugov A
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- Zhulanov V
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 01/04/2024
- Field of study
This paper presents the measurement of fducial and diferential cross sections for both the inclusive and electroweak production of a same-sign W-boson pair in association with two jets (W±W±jj) using 139 fb−1 of proton-proton collision data recorded at a centre-of-mass energy of √s = 13 TeV by the ATLAS detector at the Large Hadron Collider. The analysis is performed by selecting two same-charge leptons, electron or muon, and at least two jets with large invariant mass and a large rapidity diference. The measured fducial cross sections for electroweak and inclusive W±W±jj production are 2.92 ± 0.22 (stat.) ± 0.19 (syst.)fb and 3.38±0.22 (stat.)±0.19 (syst.)fb, respectively, in agreement with Standard Model predictions. The measurements are used to constrain anomalous quartic gauge couplings by extracting 95% confdence level intervals on dimension-8 operators. A search for doubly charged Higgs bosons H±± that are produced in vector-boson fusion processes and decay into a same-sign W boson pair is performed. The largest deviation from the Standard Model occurs for an H±± mass near 450 GeV, with a global signifcance of 2.5 standard deviations
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Search for Dark Matter Produced in Association with a Higgs Boson Decaying to bb[over ¯] Using 36 fb^{-1} of pp Collisions at sqrt[s]=13 TeV with the ATLAS Detector.
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- Zinser M
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zou R
- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Ženiš T
- Živković L
- Publication venue
- Phys Rev Lett
- Publication date
- 03/11/2017
- Field of study
Several extensions of the standard model predict associated production of dark-matter particles with a Higgs boson. Such processes are searched for in final states with missing transverse momentum and a Higgs boson decaying to a bb[over ¯] pair with the ATLAS detector using 36.1 fb^{-1} of pp collisions at a center-of-mass energy of 13 TeV at the LHC. The observed data are in agreement with the standard model predictions and limits are placed on the associated production of dark-matter particles and a Higgs boson
Combination of searches for heavy spin-1 resonances using 139 fb−1 of proton-proton collision data at s = 13 TeV with the ATLAS detector
- Author
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- Aakvaag E
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 19/04/2024
- Field of study
A combination of searches for new heavy spin-1 resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons or quarks, is presented. The data sample used corresponds to 139 fb−1 of proton-proton collisions at
= 13 TeV collected during 2015–2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb,
, and tb) or third-generation leptons (τν and ττ) are included in this kind of combination for the first time. A simplified model predicting a spin-1 heavy vector-boson triplet is used. Cross-section limits are set at the 95% confidence level and are compared with predictions for the benchmark model. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The complementarity of the various analyses increases the sensitivity to new physics, and the resulting constraints are stronger than those from any individual analysis considered. The data exclude a heavy vector-boson triplet with mass below 5.8 TeV in a weakly coupled scenario, below 4.4 TeV in a strongly coupled scenario, and up to 1.5 TeV in the case of production via vector-boson fusion
Measurements of W+W−+ ≥ 1 jet production cross-sections in pp collisions at s = 13 TeV with the ATLAS detector
- Author
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- Zemaityte G
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- Zhemchugov A
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- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
- Zoch K
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/06/2021
- Field of study
Fiducial and differential cross-section measurements of W+W− production in
association with at least one hadronic jet are presented. These measurements are sensitive
to the properties of electroweak-boson self-interactions and provide a test of perturbative
quantum chromodynamics and the electroweak theory. The analysis is performed using
proton-proton collision data collected at p
s = 13TeV with the ATLAS experiment, corresponding
to an integrated luminosity of 139 fb−1. Events are selected with exactly one oppositely
charged electron-muon pair and at least one hadronic jet with a transverse momentum
of pT > 30 GeV and a pseudorapidity of |�| < 4.5. After subtracting the background
contributions and correcting for detector effects, the jet-inclusive W+W−+ � 1 jet fiducial
cross-section and W+W−+ jets differential cross-sections with respect to several kinematic
variables are measured. These measurements include leptonic quantities, such as the lepton
transverse momenta and the transverse mass of the W+W− system, as well as jet-related
observables such as the leading jet transverse momentum and the jet multiplicity. Limits on
anomalous triple-gauge-boson couplings are obtained in a phase space where interference
between the Standard Model amplitude and the anomalous amplitude is enhanced
- …