48 research outputs found
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
- Akilli E
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
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- Argyropoulos S
- Arling J-H
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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
Measurements of differential cross-sections in four-lepton events in 13 TeV proton-proton collisions with the ATLAS detector
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- Zemaityte G
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- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
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- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 02/07/2021
- Field of study
Measurements of four-lepton differential and integrated fiducial cross-sections in events with two same-flavour, opposite-charge electron or muon pairs are presented. The data correspond to 139 fb−1 of s√ = 13 TeV proton-proton collisions, collected by the ATLAS detector during Run 2 of the Large Hadron Collider (2015–2018). The final state has contributions from a number of interesting Standard Model processes that dominate in different four-lepton invariant mass regions, including single Z boson production, Higgs boson production and on-shell ZZ production, with a complex mix of interference terms, and possible contributions from physics beyond the Standard Model. The differential cross-sections include the four-lepton invariant mass inclusively, in slices of other kinematic variables, and in different lepton flavour categories. Also measured are dilepton invariant masses, transverse momenta, and angular correlation variables, in four regions of four-lepton invariant mass, each dominated by different processes. The measurements are corrected for detector effects and are compared with state-of-the-art Standard Model calculations, which are found to be consistent with the data. The Z → 4ℓ branching fraction is extracted, giving a value of (4.41 ± 0.30) × 10−6. Constraints on effective field theory parameters and a model based on a spontaneously broken B − L gauge symmetry are also evaluated. Further reinterpretations can be performed with the provided information
Dijet Resonance Search with Weak Supervision Using root S=13 TeV pp Collisions in the ATLAS Detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
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- Aguilar-Saavedra JA
- Ahmad A
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- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Alfonsi A
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- Ali B
- Ali S
- Aliev M
- Alimonti G
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- Boeriu OEV
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Bolz AE
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Booth CD
- Borecka-Bielska HM
- Borgna LS
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Boscherini D
- Bosman M
- Bostanabad MG
- Bouaouda K
- Boudreau J
- Bouhova-Thacker E
- Boumediene D
- Bourdarios CA
- Boutle SK
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- Bozson AJ
- Bracinik J
- Brahimi N
- Brandt G
- Brandt O
- Braren F
- Brau B
- Brau JE
- Brendlinger K
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks WK
- Brost E
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Bruno S
- Bruschi M
- Bruscino N
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
- Buescher V
- Bugge MK
- Bulekov O
- Bullard BA
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Buschmann E
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund OB
- Cabras G
- Cabrera Urban S
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Caltabiano A
- Calvente Lopez S
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camarda S
- Camarero Munoz D
- Camarri P
- Camelia EA
- Camerlingo MT
- Cameron D
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Canesse A
- Cantero J
- Cao T
- Cao Y
- Capriles FGD
- Capua M
- Cardarelli R
- Cardillo F
- Carducci G
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carlson EM
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- Carra S
- Carter JWS
- Carter TM
- Casado MP
- Casha AF
- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Cavaliere V
- Cavallaro E
- Cavasinni V
- Celebi E
- Celli F
- Cerda Alberich L
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chadi Z
- Chakraborty D
- Chan J
- Chan WS
- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chau CC
- Che S
- Chekanov S
- Chekulaev S
- Chelkov GA
- Chen B
- Chen C
- Chen CH
- Chen H
- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen Y
- Chen Y-H
- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
- Cheu E
- Cheung K
- Chevalerias TJA
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu I
- Chiu YH
- Chizhov M
- Choi K
- Chomont AR
- Chouridou S
- Chow YS
- Christopher LD
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Chytka L
- Cieri D
- Ciesla KM
- Cinca D
- Cindro V
- Cioara IA
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubotaru DA
- Ciungu BM
- Clark A
- Clark MR
- Clark PJ
- Clawson SE
- Clement C
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Cohen H
- Coimbra AEC
- Cole B
- Colijn AP
- Collot J
- Conde Muino P
- Connell SH
- Connelly IA
- Constantinescu S
- Conventi F
- Cooper-Sarkar KAM
- Cormier F
- Cormier KJR
- Cornell SD
- Corpe LD
- Corradi M
- Corrado JG
- Correia AMH
- Corrigan EE
- Corriveau F
- Costa MJ
- Costanza F
- Costanzo D
- Cowan G
- Cowley JW
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- Cranmer K
- Crawley SJ
- Creager RA
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Croft V
- Crosetti G
- Cueto A
- Cukierman AR
- Cunningham WR
- Czekierda S
- Czodrowski P
- Czurylo MM
- D'amen G
- D'Amico V
- D'Auria S
- D'Eramo L
- D'onofrio A
- D'Onofrio M
- Da Via C
- Dabrowski W
- Dachs F
- Dado T
- Dahbi S
- Dai T
- Dallapiccola C
- Dam M
- Damazio DO
- Damp J
- Dandoy JR
- Daneri MF
- Dann NS
- Danninger M
- Dao V
- Darbo G
- Dartsi O
- Dattagupta A
- Daubney T
- David C
- Davidek T
- Davis DR
- Dawson I
- de Andrade Filho LM
- De Asmundis R
- De Beurs M
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- De la Torre H
- de Lima DEF
- De Lima RT
- De Maria A
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Salvo A
- De Sanctis U
- De Santis M
- De Santo A
- De Sousa MJDCS
- De K
- Debenedetti C
- Dedovich D
- Deiana AM
- 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
- Demontigny G
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Deterre C
- Dette K
- Deuren M
- Deutsch C
- Devesa MR
- Deviveiros PO
- Di Bello FA
- Di Ciaccio A
- Di Ciaccio L
- Di Clemente WK
- Di Donato C
- Di Girolamo A
- Di Gregorio G
- Di Micco B
- Di Nardo R
- Di Petrillo KF
- Di Sipio R
- Diaconu C
- Dias Do Vale T
- Dias FA
- Diaz LP
- Diaz MA
- Diaz YD
- Dickinson J
- Diehl EB
- Dietrich J
- Dimitrievska A
- Ding W
- Dingfelder J
- Dittus F
- Djama F
- Djobava T
- Djuvsland J
- Do Vale MAB
- Dobre M
- Dodsworth D
- Doglioni C
- Dolejsi J
- Dolezal Z
- Dominguez LP
- Don MMR
- Donadelli M
- Donaldson CP
- Dong B
- Donini J
- Donszelmann TC
- Dopke J
- Doria A
- Dova MT
- Doyle AT
- Drechsler E
- Dreyer E
- Dreyer T
- Drobac AS
- du Pree TA
- Du D
- Duan Y
- Dubinin F
- Dubovsky M
- Dubreuil A
- Duchovni E
- Duckeck G
- Ducu OA
- Duda D
- Dudarev A
- Dudder AC
- Duehrssen M
- Duelsen C
- Duffield EM
- Duflot L
- Dumancic M
- Dumitriu AE
- Duncan AK
- Dunford M
- Duperrin A
- Durglishvili A
- Duschinger D
- Dutta B
- Duvnjak D
- Dyckes G
- Dyndal M
- Dysch S
- Dziedzic BS
- Ecker KM
- Eggleston MG
- Eifert T
- Eigen G
- Einsweiler K
- Ekelof T
- El Jarrari H
- El Kosseifi R
- El Moursli RC
- Ellajosyula V
- Ellert M
- Ellinghaus F
- Elliot AA
- Ellis N
- Elmsheuser J
- Elsing M
- Emeliyanov D
- Emerman A
- Enari Y
- Epland MB
- Erdmann J
- Ereditato A
- Erland PA
- Errenst M
- Escalier M
- Escobar C
- Estrada Pastor O
- Etzion E
- Evans H
- Evans MO
- Ezhilov A
- Fabbri F
- Fabbri L
- Fabiani V
- Facini G
- Faisca Rodrigues Pereira RM
- Fakhrutdinov RM
- Falciano S
- Falke PJ
- Falke S
- Faltova J
- Fang Y
- Fanourakis G
- Fanti M
- Faraj M
- Farbin NA
- Farilla A
- Farina EM
- Farooque T
- Farrington SM
- Farthouat P
- Fassi F
- Fassnacht P
- Fassouliotis D
- Fawcett WJ
- Fayard L
- Fedin OL
- Fedorko W
- Fehr A
- Feickert M
- Feligioni L
- Fell A
- Feng C
- Feng M
- Fenton MJ
- Fenyuk AB
- Ferguson SW
- Ferrando J
- Ferrante A
- Ferrari A
- Ferrari P
- Ferrari R
- Ferrer A
- Ferrere D
- Ferretti C
- Fiedler F
- Filipcic A
- Filthaut F
- Finelli KD
- Fiolhais MCN
- Fiorini L
- Fischer F
- Fisher WC
- Fleck I
- Fleischmann P
- Flick T
- Flierl BM
- Flores L
- Foerster FA
- Follega FM
- Fomin N
- Foo JH
- Forcolin GT
- Formica A
- Forti AC
- Fortin E
- Foti MG
- Fournier D
- Fox H
- Francavilla P
- Francescato S
- Franchini M
- Franchino S
- Francis D
- Franco L
- Franconi L
- Franklin M
- Frattari G
- Fray AN
- Freeman PM
- Freund B
- Freund WS
- Freundlich EM
- Frizzell DC
- Froidevaux D
- Frost JA
- Fujimoto M
- Fukunaga C
- Fullana Torregrosa E
- Fusayasu T
- Fuster J
- Gabrielli A
- Gadatsch S
- Gadow P
- Gagliardi G
- Gagnon LG
- Gajardo CMR
- Galhardo B
- Gallardo GE
- Gallas EJ
- Gallop BJ
- Galster G
- Gama RG
- Gan KK
- Ganguly S
- Gao J
- Gao Y
- Gao YS
- Garcia Navarro JE
- Garcia BRM
- Garcia C
- Garcia RFN
- Garcia-Argos C
- Garcia-Sciveres M
- Gardner RW
- Garelli N
- Gargiulo S
- Garner CA
- Garonne V
- Garrido MDMC
- Gasiorowski SJ
- Gaspar P
- Gaudiello A
- Gaudio G
- Gavrilenko IL
- Gavrilyuk A
- Gay C
- Gaycken G
- Gazis EN
- Geanta AA
- Gee CM
- Gee CNP
- Geisen J
- Geisen M
- Gemme C
- Genest MH
- Geng C
- Gentile S
- George S
- Geralis T
- Gerlach LO
- Gessinger-Befurt P
- Gessner G
- Ghasemi S
- Ghneimat M
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- Giacobbe B
- Giagu S
- Giangiacomi N
- Giannelli MF
- Giannetti P
- Giannini A
- Giannini G
- Gibson SM
- Gignac M
- Gillberg D
- Gilles G
- Gingrich DM
- Giordani MP
- Giraud PF
- Giugliarelli G
- Giugni D
- Giuli F
- Gkaitatzis S
- Gkialas I
- Gkougkousis EL
- Gkountoumis P
- Gladilin LK
- Glasman C
- Glatzer J
- Glaysher PCF
- Glazov A
- Gledhill GR
- Gnesi I
- Goblirsch-Kolb M
- Godin D
- Goldfarb S
- Golling T
- Golubkov D
- Gomes A
- Goncalo R
- Gonella G
- Gonella L
- Gongadze A
- Goni RG
- Gonnella F
- Gonski JL
- Gonzalez de la Hoz S
- Gonzalez Fernandez S
- Gonzalez-Sevilla S
- Gonzalvo Rodriguez GR
- Goossens L
- Gorasia NA
- Gorbounov PA
- Gordon HA
- Gorini B
- Gorini E
- Gorisek A
- Goshaw AT
- Gostkin M
- Gottardo CA
- Gouighri M
- Goussiou AG
- Govender N
- Goy C
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- Grabowska-Bold I
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- Grancagnolo S
- Grandi M
- Gratchev V
- Gravila PM
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- Grillo AA
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- Grout ZJ
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- Guimaraes da Costa JB
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- Gul U
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- Gustavino G
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- Gutschow C
- Guyot C
- Gwenlan C
- Gwilliam CB
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- Hartman NM
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- Hasib A
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- Hawkings RJ
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- Hessey NP
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- Iconomidou-Fayard L
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- Infante CMV
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- Ju X
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- Karyukhin AN
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- Knue A
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- Kondo T
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- Kotwal A
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- Kourkoumelis C
- Kourlitis E
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- Kowalewska AB
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- Laplace S
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- Laudrain A
- Laurier A
- Lavorgna M
- Lawlor SD
- Lazzaroni M
- Le Guirriec E
- Le B
- Lebedev A
- LeBlanc M
- LeCompte T
- Ledroit-Guillon F
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- Leisos A
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- Leitgeb CE
- Leitner R
- Lellouch D
- Leney KJC
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- Zemaityte G
- Zeng JC
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- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu CG
- Zhu H
- Zhu HL
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- Zieminska D
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- Zinonos Z
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- Zivkovic L
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 25/09/2020
- Field of study
This Letter describes a search for narrowly resonant new physics using a machine-learning anomaly
detection procedure that does not rely on signal simulations for developing the analysis selection. Weakly
supervised learning is used to train classifiers directly on data to enhance potential signals. The targeted
topology is dijet events and the features used for machine learning are the masses of the two jets. The
resulting analysis is essentially a three-dimensional search A → BC, for mA ∼ OðTeVÞ, mB; mC ∼
Oð100 GeVÞ and B, C are reconstructed as large-radius jets, without paying a penalty associated with
a large trials factor in the scan of the masses of the two jets. The full run 2 ffiffi
s p ¼ 13 TeV pp collision
dataset of 139 fb−1 recorded by the ATLAS detector at the Large Hadron Collider is used for the search.
There is no significant evidence of a localized excess in the dijet invariant mass spectrum between 1.8 and
8.2 TeV. Cross-section limits for narrow-width A, B, and C particles vary with mA, mB, and mC. For
example, when mA ¼ 3 TeV and mB ≳ 200 GeV, a production cross section between 1 and 5 fb is
excluded at 95% confidence level, depending on mC. For certain masses, these limits are up to 10 times
more sensitive than those obtained by the inclusive dijet search. These results are complementary to the
dedicated searches for the case that B and C are standard model boson
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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- Zhemchugov A
- Zheng Z
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- Zorbas TG
- Zou R
- 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
Search for pair production of third-generation scalar leptoquarks decaying into a top quark and a τ-lepton in pp collisions at s√ = 13 TeV with the ATLAS detector
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- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou M
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 30/06/2021
- Field of study
A search for pair production of third-generation scalar leptoquarks decaying into a top quark and a τ-lepton is presented. The search is based on a dataset of pp collisions at s√ = 13 TeV recorded with the ATLAS detector during Run 2 of the Large Hadron Collider, corresponding to an integrated luminosity of 139 fb−1. Events are selected if they have one light lepton (electron or muon) and at least one hadronically decaying τ -lepton, or at least two light leptons. In addition, two or more jets, at least one of which must be identified as containing b-hadrons, are required. Six final states, defined by the multiplicity and flavour of lepton candidates, are considered in the analysis. Each of them is split into multiple event categories to simultaneously search for the signal and constrain several leading backgrounds. The signal-rich event categories require at least one hadronically decaying τ-lepton candidate and exploit the presence of energetic final-state objects, which is characteristic of signal events. No significant excess above the Standard Model expectation is observed in any of the considered event categories, and 95% CL upper limits are set on the production cross section as a function of the leptoquark mass, for different assumptions about the branching fractions into tτ and bν. Scalar leptoquarks decaying exclusively into tτ are excluded up to masses of 1.43 TeV while, for a branching fraction of 50% into tτ, the lower mass limit is 1.22 TeV
The ATLAS inner detector trigger performance in pp collisions at 13 TeV during LHC Run 2
- Author
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Publication venue
- Publication date
- 01/01/2022
- Field of study
The design and performance of the inner detector trigger for the high level trigger of the ATLAS experiment at the Large Hadron Collider during the 2016-2018 data taking period is discussed. In 2016, 2017, and 2018 the ATLAS detector recorded 35.6 fb(-1), 46.9 fb(-1), and 60.6 fb(-1) respectively of proton-proton collision data at a centre-of-mass energy of 13TeV. In order to deal with the very high interaction multiplicities per bunch crossing expected with the 13TeV collisions the inner detector trigger was redesigned during the long shutdown of the Large Hadron Collider from 2013 until 2015. An overview of these developments is provided and the performance of the tracking in the trigger for the muon, electron, tau and b-jet signatures is discussed. The high performance of the inner detector trigger with these extreme interaction multiplicities demonstrates how the inner detector tracking continues to lie at the heart of the trigger performance and is essential in enabling the ATLAS physics programme
Measurements of differential cross-sections in top-quark pair events with a high transverse momentum top quark and limits on beyond the Standard Model contributions to top-quark pair production with the ATLAS detector at √s = 13 TeV
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- Zhemchugov A
- Zheng Z
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Cross-section measurements of top-quark pair production where the hadronically decaying top quark has transverse momentum greater than 355 GeV and the other top quark decays into ℓνb are presented using 139 fb−1 of data collected by the ATLAS experiment during proton-proton collisions at the LHC. The fiducial cross-section at s = 13 TeV is measured to be σ = 1.267 ± 0.005 ± 0.053 pb, where the uncertainties reflect the limited number of data events and the systematic uncertainties, giving a total uncertainty of 4.2%. The cross-section is measured differentially as a function of variables characterising the tt¯ system and additional radiation in the events. The results are compared with various Monte Carlo generators, including comparisons where the generators are reweighted to match a parton-level calculation at next-to-next-to-leading order. The reweighting improves the agreement between data and theory. The measured distribution of the top-quark transverse momentum is used to search for new physics in the context of the effective field theory framework. No significant deviation from the Standard Model is observed and limits are set on the Wilson coefficients of the dimension-six operators OtG and Otq(8), where the limits on the latter are the most stringent to date. [Figure not available: see fulltext.]
Observation of electroweak production of two jets in association with an isolated photon and missing transverse momentum, and search for a Higgs boson decaying into invisible particles at 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
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- Acharya BS
- Achkar B
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- Adamek L
- Addepalli SV
- Adelman J
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- Affolder AA
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- Agapopoulou C
- Agaras MN
- Agarwala J
- Aggarwal A
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- Alberghi GL
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- Burgard CD
- Burger AM
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- Burton CD
- Burzynski JC
- Busch EL
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Buzykaev AR
- Bylund OB
- Büscher V
- Cabras G
- Caforio D
- Cai H
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- Cakir IT
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- Calace N
- Calafiura P
- Calderini G
- Calfayan P
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- Caloba LP
- Calvet D
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- Camerlingo MT
- Cameron D
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- Camplani A
- Canale V
- Canesse A
- Cantero J
- Cao Y
- Capocasa F
- Capriles FGD
- Capua M
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- Cardillo F
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- Carlson BT
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- Casadei D
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- Casha AF
- Castiglia EG
- Castillo FL
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- Catmore JR
- Cattai A
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- Chen A
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- Chen Y-H
- Cheng CL
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- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu YH
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- Choi K
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- Chou Y
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- Chowdhury T
- Christopher LD
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Ciaccio AD
- Ciaccio LD
- Cieri D
- Ciesla KM
- Cindro V
- Cioară IA
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubotaru DA
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- Clement C
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- Cornell SD
- Corpe LD
- Corradi M
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- Corriveau F
- Costa MJ
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- Cote BM
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- Crescioli F
- Cristinziani M
- Cristoforetti M
- Croft V
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- Cueto A
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- Cukierman AR
- Cunningham WR
- Curcio F
- Czodrowski P
- Czurylo MM
- Da Costa AMMJ
- da Costa JBG
- Da Cruz E Silva CB
- Da Cunha Sargedas De Sousa MJ
- Da Fonseca Pinto JV
- Da Via C
- Daalen TRV
- Dabrowski W
- Dado T
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- Dam M
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- Davis-Purcell B
- Dawson I
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- De Araujo MV
- De Asmundis R
- De Beurs M
- De Carvalho ALM
- De Castro S
- De Groot N
- de Jong P
- de la Hoz SG
- De la Torre H
- De Lima RT
- De Maria A
- De Pedis D
- de Renstrom PAB
- De Sa RCL
- De Salvo A
- De Sanctis U
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- De Souza EEP
- De Vivie De Regie JB
- De K
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- Derendarz D
- Derkaoui JE
- Derue F
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- Deviveiros PO
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- Dimitrievska A
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- Djobava T
- Djuvsland JI
- Dodsworth D
- Doglioni C
- Dolejsi J
- Dolezal Z
- Domenico AD
- Dominguez LP
- Don MMR
- Donadelli M
- Donaldson CP
- Donato CD
- Donell DMM
- Dong B
- Donini J
- Donszelmann TC
- Dopke J
- Doria A
- Dova MT
- Doyle AT
- Drechsler E
- Dreyer E
- Dreyer T
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- Dubreuil A
- Duchovni E
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- Ducu OA
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- Dumitriu AE
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- Dungs S
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- Duperrin A
- Durglishvili A
- Dutta B
- Dyckes GI
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- Dührssen M
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- D’Amico V
- D’Auria S
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- D’onofrio A
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- D’uffizi M
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- Eggleston MG
- Ehrke LF
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- Enari Y
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- Evans G
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- Facini G
- Fadeyev V
- Fakhrutdinov RM
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- Falke PJ
- Falke S
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- Fan Y
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- Farilla A
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- Farooque T
- Farrington SM
- Farthouat P
- Fassi F
- Fassouliotis D
- Fawcett WJ
- Fayard L
- Fedin OL
- Feickert M
- Felice ND
- Feligioni L
- Fell A
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- Fenyuk AB
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- Ferraz VA
- Ferrer JAV
- Ferrere D
- Ferretti C
- Fiedler F
- Filipčič A
- Filthaut F
- Fiolhais MCN
- Fiorini L
- Fischer F
- Fisher WC
- Fitschen T
- Fleck I
- Fleischmann P
- Flick T
- Flierl BM
- Flores L
- Flores M
- Follega FM
- Fomin N
- Foo JH
- Forland BC
- Formica A
- Forti AC
- Fortin E
- Foti MG
- Fountas L
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- Francescato S
- Franchini M
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- Frattari G
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- Freund WS
- Freundlich EM
- Froidevaux D
- Frost JA
- Fu Y
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- Furelos DV
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- Gabrielli A
- Gadow P
- Gagliardi G
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- Gallardo GE
- Gallas EJ
- Gallop BJ
- Galvan IS
- Gama RG
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- Ganguly S
- Gao J
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- García C
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- Gargiulo S
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- Gaspar P
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- Gavrilenko IL
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- Gerlach LO
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- Ghazali YE
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- Gillwald NEK
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- Giordani MP
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- Girolamo AD
- Giugliarelli G
- Giugni D
- Giuli F
- Gkialas I
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- Gonçalo R
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- Gorišek A
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- Gostkin MI
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- Goumarre V
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- Ibragimov I
- Iconomidou-Fayard L
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- Kodys P
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- Konya B
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- Kotwal A
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- Kourkoumelis C
- Kourlitis E
- Kovanda O
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- Lançon E
- Lapertosa A
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- Lari T
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- Latonova V
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- Laudrain A
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- Lawlor SD
- Lawrence Z
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- Lebedev A
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- Leisos A
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- Leitgeb CE
- Leitner R
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- Leonidopoulos C
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- Liberatore M
- Liberti B
- Lie K
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- Lindley RE
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- Lipniacka A
- Liss TM
- Lister A
- Little JD
- Liu B
- Liu BX
- Liu JB
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- Liu X
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- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- 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
- EUROPEAN PHYSICAL JOURNAL C
- Publication date
- 01/01/2022
- Field of study
This paper presents the measurement of the electroweak production of two jets
in association with a Zγ pair with the Z boson decaying into two
neutrinos. It also presents the search for invisible or partially invisible
decays of a Higgs boson with a mass of 125 GeV produced through vector-boson
fusion with a photon in the final state. These results use data from LHC
proton-proton collisions at s = 13 TeV collected with the ATLAS
detector corresponding to an integrated luminosity of 139 fb−1. The event
signature, shared by all benchmark processes considered for measurements and
searches, is characterized by a significant amount of unbalanced transverse
momentum and a photon in the final state, in addition to a pair of forward
jets. For electroweak production of Zγ in association with two jets, the
background-only hypothesis is rejected with an observed (expected) significance
of 5.2 (5.1) standard deviations. The measured fiducial cross-section for this
process is 1.31±0.29 fb. Observed (expected) upper limit of 0.37 (0.34) at
95% confidence level is set on the branching ratio of a 125 GeV Higgs boson to
invisible particles, assuming the Standard Model production cross-section. The
signature is also interpreted in the context of decays of a Higgs boson to a
photon and a dark photon. An observed (expected) 95% CL upper limit on the
branching ratio for this decay is set at 0.018 (0.017), assuming the 125 GeV
Standard Model Higgs boson production cross-section
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at s√=13TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
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- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
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- Affolder AA
- Afik Y
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- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
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- Ahnen JV
- Ai X
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- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
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- Aleksa M
- Aleksandrov IN
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- Zhemchugov A
- Zheng Z
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- Öncel ÖO
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- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/06/2021
- Field of study
Story of Management of a Challenging Case of a Fibrotic Uterine Cavity
- Author
- Publication venue
- 'Jaypee Brothers Medical Publishing'
- Publication date
- Field of study