379 research outputs found
Microfluidic systems for the analysis of the viscoelastic fluid flow phenomena in porous media
- Author
- A Einstein
- A Groisman
- AB Metzner
- CD Meinhart
- CJS Petrie
- CJS Petrie
- D Sinton
- E. van Bokhorst
- EH Wissler
- F. J. Galindo-Rosales
- F. T. Pinho
- GH McKinley
- GM Whitesides
- H Darcy
- HA Stone
- HK Moffatt
- HP Sdougos
- J Soulages
- JC McDonald
- JG Santiago
- JG Savins
- JL Duda
- JRA Pearson
- KC Taylor
- KS Sorbie
- L Campo-Deaño
- L. Campo-Deaño
- LE Rodd
- LE Rodd
- M Rhodes
- M. A. Alves
- M. S. N. Oliveira
- MA Alves
- MJ Blunt
- MSN Oliveira
- MSN Oliveira
- MT Balhoff
- NY Gaitonde
- P Pakdel
- P Pakdel
- P. J. Hamersma
- PC Sousa
- R Holdich
- RG Larson
- RH Christopher
- RJ Marshall
- RP Chhabra
- S Devasenathipathy
- T Sochi
- T Sochi
- VM Entov
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 22/10/2011
- Field of study
In this study, two microfluidic devices are proposed as simplified 1-D microfluidic analogues of a porous medium. The objectives are twofold: firstly to assess the usefulness of the microchannels to mimic the porous medium in a controlled and simplified manner, and secondly to obtain a better insight about the flow characteristics of viscoelastic fluids flowing through a packed bed. For these purposes, flow visualizations and pressure drop measurements are conducted with Newtonian and viscoelastic fluids. The 1-D microfluidic analogues of porous medium consisted of microchannels with a sequence of contractions/ expansions disposed in symmetric and asymmetric arrangements. The real porous medium is in reality, a complex combination of the two arrangements of particles simulated with the microchannels, which can be considered as limiting ideal configurations. The results show that both configurations are able to mimic well the pressure drop variation with flow rate for Newtonian fluids. However, due to the intrinsic differences in the deformation rate profiles associated with each microgeometry, the symmetric configuration is more suitable for studying the flow of viscoelastic fluids at low De values, while the asymmetric configuration provides better results at high De values. In this way, both microgeometries seem to be complementary and could be interesting tools to obtain a better insight about the flow of viscoelastic fluids through a porous medium. Such model systems could be very interesting to use in polymer-flood processes for enhanced oil recovery, for instance, as a tool for selecting the most suitable viscoelastic fluid to be used in a specific formation. The selection of the fluid properties of a detergent for cleaning oil contaminated soil, sand, and in general, any porous material, is another possible application
Microdevices for extensional rheometry of low viscosity elastic liquids : a review
- Author
- A Bazilevsky
- AG Balducci
- AG Banpurkar
- AM Ardekani
- B Berge
- C Pipe
- C Pipe
- CG Hermansky
- CJS Petrie
- CJS Petrie
- CW Macosko
- DR Link
- E Bänsch
- ESG Shaqfeh
- F Mugele
- F. J. Galindo-Rosales
- FR Phelan Jr
- FT Trouton
- G Beni
- GG Fuller
- GH McKinley
- GH McKinley
- GH McKinley
- GI Taylor
- GM Whitesides
- H Münsted
- HA Barnes
- HCH Bandalusena
- HP Babcock
- J Husny
- J Meissner
- J Meissner
- J Remmelgas
- J Soulages
- J Wang
- JA Odell
- JA Pathak
- JE Matta
- JH Song
- JM Maia
- JP Rothstein
- JP Rothstein
- JS Lee
- K Niedzwiedz
- K Niedzwiedz
- K Nijenhuis
- L Campo-Deaño
- L Campo-Deaño
- LE Rodd
- LE Rodd
- LE Rodd
- M Padmanabhan
- M Padmanabhan
- M Roche
- M Sentmanat
- M Tanyeri
- M Tanyeri
- M. A. Alves
- M. S. N. Oliveira
- MA Alves
- MG Pollack
- MK Tan
- MSN Oliveira
- MSN Oliveira
- MSN Oliveira
- MSN Oliveira
- MSN Oliveira
- MSN Oliveira
- MSN Oliveira
- MSN Oliveira
- N Kojic
- N Kumari
- P Becherer
- P Dontula
- P Erni
- P Guillot
- P Guillot
- PC Sousa
- PE Arratia
- PE Arratia
- PK Bhattacharjee
- R Dylla-Spears
- R Sattler
- R Zheng
- RB Bird
- RI Tanner
- RJ Poole
- RR Lagnado
- S Gaudet
- S Ríos
- SD Hudson
- SJ Haward
- SJ Haward
- SJ Haward
- SL Anna
- SL Anna
- SL Anna
- SL Ng
- SS Hsieh
- T Cubaud
- T Funami
- T Schweizer
- T Sridhar
- TM Squires
- TM Squires
- TT Perkins
- W Lee
- WC Nelson
- WW Schultz
- YY Lin
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2013
- Field of study
Extensional flows and the underlying stability/instability mechanisms are of extreme relevance to the efficient operation of inkjet printing, coating processes and drug delivery systems, as well as for the generation of micro droplets. The development of an extensional rheometer to characterize the extensional properties of low viscosity fluids has therefore stimulated great interest of researchers, particularly in the last decade. Microfluidics has proven to be an extraordinary working platform and different configurations of potential extensional microrheometers have been proposed. In this review, we present an overview of several successful designs, together with a critical assessment of their capabilities and limitations
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
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Adam Bourdarios C
- Adamczyk L
- Adamek L
- Addepalli SV
- Addison MJ
- Adelman J
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahuja S
- Ai X
- Aielli G
- Aikot A
- Ait Tamlihat M
- Aitbenchikh B
- Aizenberg I
- Akbiyik M
- Akimov AV
- Akiyama D
- Akolkar NN
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Albouy GL
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi F
- Algren M
- Alhroob M
- Ali B
- Ali HMJ
- Ali S
- Alibocus SW
- Aliev M
- Alimonti G
- Alkakhi W
- Allaire C
- Allbrooke BMM
- Allen JF
- Allendes Flores CA
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alvarez Estevez M
- Alvarez Fernandez A
- Alves Cardoso M
- Alviggi MG
- Aly M
- Amaral Coutinho Y
- Ambler A
- Amelung C
- Amerl M
- Ames CG
- Amidei D
- Amor Dos Santos SP
- Amos KR
- Ananiev V
- Anastopoulos C
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Anulli F
- Aoki M
- Aoki T
- Aparisi Pozo JA
- Aparo MA
- Aperio Bella L
- Appelt C
- Apyan A
- Aranzabal N
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Assamagan K
- Astalos R
- Atashi S
- Atkin RJ
- Atkinson M
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Auriol AD
- Austrup VA
- Avolio G
- Axiotis K
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Bachiu A
- Backman F
- Badea A
- Bagnaia P
- Bahmani M
- Bailey AJ
- Bailey VR
- Baines JT
- Baines L
- Bakalis C
- Baker OK
- Bakos E
- Bakshi Gupta D
- Balakrishnan V
- Balasubramanian R
- Baldin EM
- Balek P
- Ballabene E
- Balli F
- Baltes LM
- Balunas WK
- Balz J
- Banas E
- Bandieramonte M
- Bandyopadhyay A
- Bansal S
- Barak L
- Barakat M
- Barberio EL
- Barberis D
- Barbero M
- Barel MZ
- Barends KN
- Barillari T
- Barisits M-S
- Barklow T
- Baron Moreno DA
- Baron P
- Baroncelli A
- Barone G
- Barr AJ
- Barr JD
- Barranco Navarro L
- Barreiro Guimarães da Costa J
- Barreiro F
- Barron U
- Barros Teixeira MG
- Barsov S
- Bartels F
- Bartoldus R
- Barton AE
- Bartos P
- Basan A
- Baselga M
- Bassalat A
- Basso MJ
- Basson CR
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Battulga D
- Bauce M
- Bauer M
- Bauer P
- Bazzano Hurrell LT
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HP
- Becker K
- Becot C
- Beddall AJ
- Bednyakov VA
- Bee CP
- Beemster LJ
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beirer JF
- Beisiegel F
- Belfkir M
- Bella G
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belyaev NL
- Benchekroun D
- Bendebba F
- Benhammou Y
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Bergeaas Kuutmann E
- Berger N
- Bergmann B
- Beringer J
- Bernardi G
- Bernius C
- Bernlochner FU
- Bernon F
- Berry T
- Berta P
- Berthold A
- Bertram IA
- Bethke S
- Betti A
- Bevan AJ
- Bhamjee M
- Bhatta S
- Bhattacharya DS
- Bhattarai P
- Bhopatkar VS
- Bi R
- Bianchi RM
- Bianco G
- Biebel O
- Bielski R
- Biglietti M
- Billoud TRV
- Bindi M
- Bingul A
- Bini C
- Biondini A
- Birch-sykes CJ
- Bird GA
- Birman M
- Biros M
- Biryukov S
- Bisanz T
- Bisceglie E
- Biswal JP
- Biswas D
- Bitadze A
- Bjørke K
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blumenthal J
- Bobbink GJ
- Bobrovnikov VS
- Boehler M
- Boehm B
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Bomben M
- Bona M
- Boonekamp M
- Booth CD
- Borbély AG
- Bordulev IS
- Borecka-Bielska HM
- Borgna LS
- Borissov G
- Bortoletto D
- Boscherini D
- Bosman M
- Bossio Sola JD
- Bouaouda K
- Bouchhar N
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bouquet R
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- Bracinik J
- Brahimi N
- Brandt G
- Brandt O
- Braren F
- Brau B
- Brau JE
- Brener R
- Brenner L
- Brenner R
- Bressler S
- Britton D
- Britzger D
- Brock I
- Brooijmans G
- Brooks WK
- Brost E
- Brown LM
- Bruce LE
- Bruckler TL
- Bruckman de Renstrom PA
- Bruni A
- Bruni G
- Bruschi M
- Bruscino N
- Brüers B
- Buanes T
- Buat Q
- Buchin D
- Buckley AG
- Bulekov O
- Bullard BA
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burlayenko O
- Burr JTP
- Burton CD
- Burzynski JC
- Busch EL
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Buxo Vazquez CJ
- Buzykaev AR
- Büscher V
- Cabrera Urbán S
- Cadamuro L
- Caforio D
- Cai H
- Cai Y
- Cairo VMM
- Cakir O
- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camacho Toro R
- Camarda S
- Camarero Munoz D
- Camarri P
- Camerlingo MT
- Cameron D
- Camincher C
- Campanelli M
- Camplani A
- Canale V
- Canesse A
- Cantero J
- Cao Y
- Capocasa F
- Capua M
- Carbone A
- Cardarelli R
- Cardenas JCJ
- Cardillo F
- Carli T
- Carlino G
- Carlotto JI
- Carlson BT
- Carlson EM
- Carminati L
- Carnelli A
- Carnesale M
- Caron S
- Carquin E
- Carratta G
- Carrio Argos F
- Carrá S
- Carter JWS
- Carter TM
- Casado MP
- Caspar M
- Castiglia EG
- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
- Castro NF
- Catinaccio A
- Catmore JR
- Cavaliere V
- Cavalli N
- Cavasinni V
- Cekmecelioglu YC
- Celebi E
- Celli F
- Centonze MS
- Cepaitis V
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervato B
- Cervelli A
- Cesarini G
- Cetin SA
- Chadi Z
- Chakraborty D
- Chan J
- Chan WY
- Chapman JD
- Chapon E
- Chargeishvili B
- Charlton DG
- Charman TP
- Chatterjee M
- Chauhan C
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chen A
- Chen B
- Chen B
- Chen H
- Chen H
- Chen J
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- Chen M
- Chen S
- Chen SJ
- Chen X
- Chen X
- Chen Y
- Cheng CL
- Cheng HC
- Cheong S
- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cherkaoui El Moursli R
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiedde N
- Chiodini G
- Chisholm AS
- Chitan A
- Chitishvili M
- Chizhov MV
- Choi K
- Chomont AR
- Chou Y
- Chow EYS
- Chowdhury T
- Chu KL
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Cieri D
- Ciesla KM
- Cindro V
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubotaru DA
- Ciungu BM
- Clark A
- Clark PJ
- Clavijo Columbie JM
- Clawson SE
- Clement C
- Clercx J
- Coadou Y
- Cobal M
- Coccaro A
- Coelho Barrue RF
- Coelho Lopes De Sa R
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- Coimbra AEC
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- Collot J
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- Connell MP
- Connell SH
- Connelly IA
- Conroy EI
- Conventi F
- Cooke HG
- Cooper-Sarkar AM
- Cordeiro Oudot Choi A
- Cormier F
- Corpe LD
- Corradi M
- Corriveau F
- Cortes-Gonzalez A
- Costa MJ
- Costanza F
- Costanzo D
- Cote BM
- Cowan G
- Cranmer K
- Cremonini D
- Crescioli F
- Cristinziani M
- Cristoforetti M
- Croft V
- Crosby JE
- Crosetti G
- Crépé-Renaudin S
- Cueto A
- Cuhadar Donszelmann T
- Cui H
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- Cunningham WR
- Curcio F
- Czodrowski P
- Czurylo MM
- Da Cunha Sargedas De Sousa MJ
- Da Fonseca Pinto JV
- Da Via C
- Dabrowski W
- Dado T
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- Dallapiccola C
- Dam M
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- Dandoy JR
- Daneri MF
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- Das SJ
- David C
- Davidek T
- Davis-Purcell B
- Dawson I
- Day-hall HA
- De Asmundis R
- De Biase N
- De Castro S
- De Groot N
- de Jong P
- De la Torre H
- De Maria A
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- De Santo A
- De Vivie De Regie JB
- De K
- Dedovich DV
- Degens J
- Deiana AM
- Del Corso F
- Del Peso J
- Del Rio F
- Deliot F
- Delitzsch CM
- Della Pietra M
- Della Volpe D
- Dell’Acqua A
- Dell’Asta L
- Delmastro M
- Delsart PA
- Demers S
- Demichev M
- Denisov SP
- Derendarz D
- Derue F
- Dervan P
- Desch K
- Deutsch C
- Di Bello FA
- Di Ciaccio A
- Di Ciaccio L
- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Gregorio G
- Di Luca A
- Di Micco B
- Di Nardo R
- Diaconu C
- Diamantopoulou M
- Dias Do Vale T
- Dias FA
- Diaz Capriles FG
- Diaz MA
- Didenko M
- Diehl EB
- Diehl L
- Diez Pardos C
- Dimitriadi C
- Dimitrievska A
- Dingfelder J
- Dinu I-M
- Dittmeier SJ
- Dittus F
- Djama F
- Djobava T
- Djuvsland JI
- Doglioni C
- Dohnalova A
- Dolejsi J
- Dolezal Z
- Dona KM
- Donadelli M
- Dong B
- Donini J
- Dopke J
- Doria A
- Dos Santos Fernandes N
- Dougan P
- Dova MT
- Doyle AT
- Draguet MA
- Dreyer E
- Drivas-koulouris I
- Drobac AS
- Drozdova M
- du Pree TA
- Du D
- Dubinin F
- Dubovsky M
- Duchovni E
- Duckeck G
- Ducu OA
- Duda D
- Dudarev A
- Duden ER
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- Dumitriu AE
- Dunford M
- Dungs S
- Dunne K
- Duperrin A
- Duran Yildiz H
- Durglishvili A
- Dwyer BL
- Dyckes GI
- Dyndal M
- Dysch S
- Dziedzic BS
- Díez Cornell S
- Dührssen M
- Dülsen C
- Düren M
- D’amen G
- D’Amico V
- D’Auria S
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- D’uffizi M
- Earnshaw ZO
- Eberwein GH
- Eckerova B
- Eggebrecht S
- Egidio Purcino De Souza E
- Ehrke LF
- Eigen G
- Einsweiler K
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- Elmsheuser J
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- Escobar C
- Etzion E
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- Fabbri F
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- Facini G
- Fadeyev V
- Fakhrutdinov RM
- Falciano S
- Falda Ulhoa Coelho LF
- Falke PJ
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- Farilla A
- Farooque T
- Farrington SM
- Fassi F
- Fassouliotis D
- Faucci Giannelli M
- Fawcett WJ
- Fayard L
- Federic P
- Federicova P
- Fedin OL
- Fedotov G
- Feickert M
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- Fellers DE
- Feng C
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- Feng Z
- Fenton MJ
- Fenyuk AB
- Ferencz L
- Ferguson RAM
- Fernandez Luengo SI
- Fernoux MJV
- Ferrando J
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- Ferretti C
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- Filipčič A
- Filmer EK
- Filthaut F
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- Fisher WC
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- Fitzhugh PM
- Fleck I
- Fleischmann P
- Flick T
- Flores Castillo LR
- Flores Sanz De Acedo L
- Flores M
- Follega FM
- Fomin N
- Foo JH
- Forland BC
- Formica A
- Forti AC
- Fortin E
- Fortman AW
- Foti MG
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- Fournier D
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- Francavilla P
- Francescato S
- Franchellucci S
- Franchini M
- Franchino S
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- Franco L
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- Freegard AC
- Freund WS
- Frid YY
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- Fullana Torregrosa E
- Fung KY
- Furtado De Simas Filho E
- Furukawa M
- Fuster J
- Gabrielli A
- Gabrielli A
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- Gagliardi G
- Gagnon LG
- Gallas EJ
- Gallop BJ
- Gan KK
- Ganguly S
- Gao J
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- Garay Walls FM
- Garcia Alonso A
- Garcia Caffaro AG
- Garcia B
- Garcia-Sciveres M
- García Navarro JE
- García C
- Gardner GL
- Gardner RW
- Garelli N
- Garg D
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- Gargan JM
- Garner CA
- Gasiorowski SJ
- Gaspar P
- Gaudio G
- Gautam V
- Gauzzi P
- Gavrilenko IL
- Gavrilyuk A
- Gay C
- Gaycken G
- Gazis EN
- Geanta AA
- Gee CM
- Gemme C
- Genest MH
- Gentile S
- Gentry AD
- George S
- George WF
- Geralis T
- Gessinger-Befurt P
- Geyik ME
- Ghani M
- Ghneimat M
- Ghorbanian K
- Ghosal A
- Ghosh A
- Ghosh A
- Giacobbe B
- Giagu S
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- Giannetti P
- Giannini A
- Gibson SM
- Gignac M
- Gil DT
- Gilbert AK
- Gilbert BJ
- Gillberg D
- Gilles G
- Gillwald NEK
- Ginabat L
- Gingrich DM
- Giordani MP
- Giraud PF
- Giugliarelli G
- Giugni D
- Giuli F
- Gkialas I
- Gladilin LK
- Glasman C
- Gledhill GR
- Glemža G
- Glisic M
- Gnesi I
- Go Y
- Goblirsch-Kolb M
- Gocke B
- Godin D
- Gokturk B
- Goldfarb S
- Golling T
- Gololo MGD
- Golubkov D
- Gombas JP
- Gomes Da Silva G
- Gomes A
- Gomez Delegido AJ
- Gonella G
- Gonella L
- Gongadze A
- Gonnella F
- Gonski JL
- Gonzalez Fernandez S
- Gonzalez Lopez R
- Gonzalez Renteria C
- Gonzalez Rodrigues MV
- Gonzalez Suarez R
- Gonzalez-Sevilla S
- Gonzalvo Rodriguez GR
- González Andana RY
- González de la Hoz S
- Gonçalo R
- Goossens L
- Gorini B
- Gorini E
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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
Search for pair production of squarks or gluinos decaying via sleptons or weak bosons in final states with two same-sign or three leptons with the ATLAS detector
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- Xiang J
- Xiao X
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- Xiong J
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- Yabsley B
- Yacoob S
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- Yamaguchi Y
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- Yue L
- Zaazoua M
- Zabinski B
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- Zakharchuk N
- Zambito S
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- Zang J
- Zanzi D
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- Zeng H
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- Zenger DT
- Zenin O
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- Zerradi S
- Zerwas D
- Zhai M
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- Zhang K
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- Zhang P
- Zhang R
- Zhang S
- Zhang T
- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
- Zhou Y
- Zhu CG
- Zhu J
- Zhu Y
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine NI
- Zinsser J
- 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
- 15/02/2024
- Field of study
A search for pair production of squarks or gluinos decaying via sleptons or weak bosons is reported. The search targets a final state with exactly two leptons with same-sign electric charge or at least three leptons without any charge requirement. The analysed data set corresponds to an integrated luminosity of 139 fb−1 of proton-proton collisions collected at a centre-of-mass energy of 13 TeV with the ATLAS detector at the LHC. Multiple signal regions are defined, targeting several SUSY simplified models yielding the desired final states. A single control region is used to constrain the normalisation of the WZ + jets background. No significant excess of events over the Standard Model expectation is observed. The results are interpreted in the context of several supersymmetric models featuring R-parity conservation or R-parity violation, yielding exclusion limits surpassing those from previous searches. In models considering gluino (squark) pair production, gluino (squark) masses up to 2.2 (1.7) TeV are excluded at 95% confidence level
Muon reconstruction and identification efficiency in ATLAS using the full Run 2 pp collision data set at \sqrt{s}=13 TeV
- Author
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
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- Zhemchugov A
- Zheng Z
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- Zorbas TG
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- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2021
- Field of study
This article documents the muon reconstruction and identification efficiency obtained by the ATLAS experiment for 139 \hbox {fb}^{-1} of pp collision data at \sqrt{s}=13 TeV collected between 2015 and 2018 during Run 2 of the LHC. The increased instantaneous luminosity delivered by the LHC over this period required a reoptimisation of the criteria for the identification of prompt muons. Improved and newly developed algorithms were deployed to preserve high muon identification efficiency with a low misidentification rate and good momentum resolution. The availability of large samples of Z\rightarrow \mu \mu and J/\psi \rightarrow \mu \mu decays, and the minimisation of systematic uncertainties, allows the efficiencies of criteria for muon identification, primary vertex association, and isolation to be measured with an accuracy at the per-mille level in the bulk of the phase space, and up to the percent level in complex kinematic configurations. Excellent performance is achieved over a range of transverse momenta from 3 GeV to several hundred GeV, and across the full muon detector acceptance of |\eta |<2.7
Measurement of the tt¯tt¯ production cross section in pp collisions at √s=13 TeV with the ATLAS detector
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- Zeißner SV
- Zemaityte G
- Zeng JC
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- Zhemchugov A
- Zheng Z
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- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- 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
- 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
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at √=13TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahnen JV
- Ai X
- Aielli G
- Akatsuka S
- Akbiyik M
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- Buschmann E
- Bussey PJ
- Butler JM
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- Butterworth JM
- Buttinger W
- Buzykaev AR
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- Cabras G
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- Calafiura P
- Calderini G
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- Caltabiano A
- Calvet D
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- Camerlingo MT
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- Canesse A
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- Cheu E
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- Chevalier L
- Chevalérias TJA
- Chiarella V
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- Chisholm AS
- Chitan A
- Chiu I
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- Cindro V
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- Ciocio A
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 23/06/2021
- Field of study
The paper presents a measurement of the Standard Model Higgs Boson decaying to b-quark pairs in the vector boson fusion (VBF) production mode. A sample corresponding to 126 fb−1 of s√=13TeV proton–proton collision data, collected with the ATLAS experiment at the Large Hadron Collider, is analyzed utilizing an adversarial neural network for event classification. The signal strength, defined as the ratio of the measured signal yield to that predicted by the Standard Model for VBF Higgs production, is measured to be 0.95+0.38−0.36 , corresponding to an observed (expected) significance of 2.6 (2.8) standard deviations from the background only hypothesis. The results are additionally combined with an analysis of Higgs bosons decaying to b-quarks, produced via VBF in association with a photon
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
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- Aakvaag E
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- Zhemchugov A
- Zheng J
- Zheng K
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- Zhong D
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- Zhukov K
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
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- Zormpa O
- Zou W
- 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
Software Performance of the ATLAS Track Reconstruction for LHC Run 3
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
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- Agullo P Martinez
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- Zhemchugov A
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- Zhulanov V
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 02/04/2024
- Field of study
Charged particle reconstruction in the presence
of many simultaneous proton–proton (pp) collisions in the
LHC is a challenging task for the ATLAS experiment’s reconstruction software due to the combinatorial complexity. This
paper describes the major changes made to adapt the software
to reconstruct high-activity collisions with an average of 50 or
more simultaneous pp interactions per bunch crossing (pileup) promptly using the available computing resources. The
performance of the key components of the track reconstruction chain and its dependence on pile-up are evaluated, and
the improvement achieved compared to the previous software
version is quantified. For events with an average of 60 pp collisions per bunch crossing, the updated track reconstruction
is twice as fast as the previous version, without significant
reduction in reconstruction efficiency and while reducing the
rate of combinatorial fake tracks by more than a factor two
Performance and calibration of quark/gluon-jet taggers using 140 fb⁻¹ of pp collisions at √s=13 TeV with the ATLAS detector
- Author
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- Abbott B
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- Abicht NJ
- Abidi SH
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- Zhemchugov A
- Zheng J
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- Zimine NI
- Zinsser J
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/02/2024
- Field of study
The identification of jets originating from quarks and gluons, often referred to as quark/gluon tagging,
plays an important role in various analyses performed at the Large Hadron Collider, as Standard Model measurements and searches for new particles decaying to quarks often rely on suppressing a large gluon-induced background. This paper describes the measurement of the efficiencies of quark/gluon taggers developed within the ATLAS Collaboration, using √s=13 TeV proton–proton collision data with an integrated luminosity of 140 fb-1 collected by the ATLAS experiment. Two taggers with high performances in rejecting jets from gluon over jets from
quarks are studied: one tagger is based on requirements on the number of inner-detector tracks associated with the
jet, and the other combines several jet substructure observables using a boosted decision tree. A method is established to determine the quark/gluon fraction in data, by using quark/gluon-enriched subsamples defined by the jet
pseudorapidity. Differences in tagging efficiency between data and simulation are provided for jets with transverse
momentum between 500 GeV and 2 TeV and for multiple tagger working points
- …