277 research outputs found
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
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- Adelman J
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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
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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- Yao W-M
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- Yin P
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- Yue L
- Zaazoua M
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- Zaid E
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- Zakharchuk N
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- Zamora Saa JA
- Zang J
- Zanzi D
- Zaplatilek O
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- Zeng H
- Zeng JC
- Zenger DT
- Zenin O
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- Zerwas D
- Zhai M
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- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao T
- Zhao Y
- Zhao Z
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
- Zhou Y
- Zhou Y
- Zhu CG
- Zhu J
- Zhu Y
- Zhu Y
- Zhuang X
- Zhukov K
- 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 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
Corrigendum to "Search for flavour-changing neutral-current couplings between the top quark and the photon with the ATLAS detector at √s=13 TeV" (Physics Letters B, 842 (2023), 137379)
- Author
- Aad G
- Abbott B
- Abbott Dc
- Abed Abud A
- Abeling K
- Abidi Sh
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman Ac
- Acharya Bs
- Achkar B
- Adam Bourdarios C
- Adam L
- Adamczyk L
- Adamek L
- Addepalli Sv
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder Aa
- Afik Y
- Agaras Mn
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra Ja
- Ahmad A
- Ahmadov F
- Ahmed Ws
- Ai X
- Aielli G
- Aizenberg I
- Akbiyik M
- Akimov Av
- Al Khoury K
- Alberghi Gl
- Albert J
- Albicocco P
- Alconada Verzini Mj
- Alderweireldt S
- Aleksa M
- Aleksandrov In
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke Bmm
- Allport Pp
- Aloisio A
- Alonso F
- Alpigiani C
- Alunno Camelia E
- Alvarez Estevez M
- Alviggi Mg
- Amaral Coutinho Y
- Ambler A
- Amelung C
- Ames Cg
- Amidei D
- Amor Dos Santos Sp
- Amoroso S
- Amos Kr
- Amrouche Cs
- Ananiev V
- Anastopoulos C
- Andari N
- Andeen T
- Anders Jk
- Andrean Sy
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov Av
- Annovi A
- Antel C
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- Antipov E
- Antonelli M
- Antrim Dja
- Anulli F
- Aoki M
- Aparisi Pozo Ja
- Aparo Ma
- Aperio Bella L
- Appelt C
- Aranzabal N
- Araujo Ferraz V
- Arcangeletti C
- Arce Ath
- Arena E
- Arguin J
- Argyropoulos S
- Arling J-
- Armbruster Aj
- Arnaez O
- Arnold H
- Arrubarrena Tame Zp
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah Na
- Asimakopoulou Em
- Assahsah J
- Assamagan K
- Astalos R
- Atkin Rj
- Atkinson M
- Atlay Nb
- Atmani H
- Atmasiddha Pa
- Augsten K
- Auricchio S
- Auriol Ad
- Austrup Va
- Avner G
- Avolio G
- Axiotis K
- Ayoub Mk
- Azuelos G
- Åkesson Tpa
- Babal D
- Bachacou H
- Bachas K
- Bachiu A
- Backman F
- Badea A
- Bagnaia P
- Bahmani M
- Bailey Aj
- Bailey Vr
- Baines Jt
- Bakalis C
- Baker Ok
- Bakker Pj
- Bakos E
- Bakshi Gupta D
- Balaji S
- 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
- Barberio El
- Barberis D
- Barbero M
- Barbour G
- Barends Kn
- Barillari T
- Barisits M
- Barkeloo J
- Barklow T
- Barnett Rm
- Baron Moreno Da
- Baron P
- Baroncelli A
- Barone G
- Barr Aj
- Barranco Navarro L
- Barreiro Guimarães da Costa J
- Barreiro F
- Barron U
- Barsov S
- Bartels F
- Bartoldus R
- Barton Ae
- Bartos P
- Basalaev A
- Basan A
- Baselga M
- Bashta I
- Bassalat A
- Basso Mj
- Basson Cr
- Bates Rl
- Batlamous S
- Batley Jr
- Batool B
- Battaglia M
- Bauce M
- Bauer P
- Bayirli A
- 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
- Beirao Da Cruz E Silva C
- Beirer Jf
- Beisiegel F
- Belfkir M
- Bella G
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev Nl
- Benchekroun D
- Benhammou Y
- Benjamin Dp
- Benoit M
- Bensinger Jr
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Bergeaas Kuutmann E
- Berger N
- Bergmann B
- Beringer J
- Berlendis S
- Bernardi G
- Bernius C
- Bernlochner Fu
- Berry T
- Berta P
- Berthold A
- Bertram Ia
- Bessidskaia Bylund O
- Bethke S
- Betti A
- Bevan Aj
- Bhatta S
- Bhattacharya Ds
- Bhattarai P
- Bhopatkar Vs
- Bi R
- Bi R
- Bianchi Rm
- Biebel O
- Bielski R
- Biesuz Nv
- Biglietti M
- Billoud Trv
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Biondini A
- Birch-sykes Cj
- Bird Ga
- Birman M
- Bisanz T
- Biswas D
- Bitadze A
- Bjørke K
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blumenthal J
- Bobbink Gj
- Bobrovnikov Vs
- Boehler M
- Bogavac D
- Bogdanchikov Ag
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Bomben M
- Bona M
- Boonekamp M
- Booth Cd
- Borbély Ag
- Borecka-Bielska Hm
- Borgna Ls
- Borissov G
- Bortoletto D
- Boscherini D
- Bosman M
- Bossio Sola Jd
- Bouaouda K
- 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
- Breaden Madden Wd
- Brendlinger K
- Brener R
- Brenner L
- Brenner R
- Bressler S
- Brickwedde B
- Britton D
- Britzger D
- Brock I
- Brooijmans G
- Brooks Wk
- Brost E
- Bruckman de Renstrom Pa
- Bruncko D
- Bruni A
- Bruni G
- Bruschi M
- Bruscino N
- Brüers B
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley Ag
- Budagov Ia
- Bugge Mk
- Bulekov O
- Bullard Ba
- Burdin S
- Burgard Cd
- Burger Am
- Burghgrave B
- 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
- Cabras G
- Cabrera Urbán S
- 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
- Cano Bret M
- Cantero J
- Cao Y
- Capocasa F
- Capua M
- Carbone A
- Cardarelli R
- Cardenas Jcj
- Cardillo F
- Carli T
- Carlino G
- Carlson Bt
- Carlson Em
- Carminati L
- Carnesale M
- Caron S
- Carquin E
- Carratta G
- Carrá S
- Carter Jws
- Carter Tm
- Casado Mp
- Casha Af
- Castiglia Eg
- Castillo Garcia L
- Castillo Gimenez V
- Castillo Fl
- Castro Nf
- Catinaccio A
- Catmore Jr
- Cavaliere V
- Cavalli N
- Cavasinni V
- Celebi E
- Celli F
- Centonze Ms
- Cerny K
- Cerqueira As
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin Sa
- Chadi Z
- Chakraborty D
- Chala M
- Chan J
- Chan Ws
- Chan Wy
- Chapman Jd
- Chargeishvili B
- Charlton Dg
- Charman Tp
- Chatterjee M
- Chekanov S
- Chekulaev Sv
- Chelkov Ga
- Chen A
- Chen B
- Chen B
- Chen C
- Chen H
- Chen H
- Chen J
- Chen J
- Chen S
- Chen Sj
- Chen X
- Chen X
- Chen Y
- Cheng Cl
- Cheng Hc
- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cherkaoui El Moursli R
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm As
- Chitan A
- Chiu Yh
- Chizhov Mv
- Choi K
- Chomont Ar
- Chou Y
- Chow Eys
- Chowdhury T
- Christopher Ld
- 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
- Clissa L
- Coadou Y
- Cobal M
- Coccaro A
- Coelho Barrue Rf
- Coelho Lopes De Sa R
- Coelli S
- Cohen H
- Coimbra Aec
- Cole B
- Collot J
- Conde Muiño P
- Connell Sh
- Connelly Ia
- Conroy Ei
- Conventi F
- Cooke Hg
- Cooper-Sarkar Am
- Cormier F
- Corpe Ld
- Corradi M
- Corrigan Ee
- Corriveau F
- Cortes-Gonzalez A
- Costa Mj
- Costanza F
- Costanzo D
- Cote Bm
- Cowan G
- Cowley Jw
- Cranmer K
- Crescioli F
- Crépé-Renaudin S
- Cristinziani M
- Cristoforetti M
- Croft V
- Crosetti G
- Cueto A
- Cuhadar Donszelmann T
- Cui H
- Cui Z
- Cukierman Ar
- Cunningham Wr
- Curcio F
- Czodrowski P
- Czurylo Mm
- D'Amen G
- D'Amico V
- D'Auria S
- D'Eramo L
- D'Onofrio A
- D'Onofrio M
- D'Uffizi M
- Da Cunha Sargedas De Sousa Mj
- Da Fonseca Pinto Jv
- Da Via C
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dallapiccola C
- Dam M
- Damp J
- Dandoy Jr
- Daneri Mf
- Danninger M
- Dao V
- Darbo G
- Darmora S
- Das Sj
- Dattagupta A
- David C
- Davidek T
- Davis Dr
- Davis-Purcell B
- Dawson I
- De Asmundis R
- De Beurs M
- De Castro S
- De Groot N
- de Jong P
- De la Torre H
- De Maria A
- De Salvo A
- De Sanctis U
- De Santis M
- 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
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- Della Volpe D
- Delmastro M
- Delsart Pa
- Demers S
- Demichev M
- Denisov Sp
- Derendarz D
- Derue F
- Dervan P
- Desch K
- Dette K
- Deutsch C
- Deviveiros Po
- 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
- Dias Do Vale T
- Dias Fa
- Diaz Capriles Fg
- Diaz Ma
- Didenko M
- Diehl Eb
- Diehl L
- Diez Pardos C
- Dimitriadi C
- Dimitrievska A
- Ding W
- Dingfelder J
- Dinu I
- Dittmeier Sj
- Dittus F
- Díez Cornell S
- Djama F
- Djobava T
- Djuvsland Ji
- Dodsworth D
- Doglioni C
- Dolejsi J
- Dolezal Z
- Donadelli M
- Dong B
- Donini J
- Dopke J
- Doria A
- Dova Mt
- Doyle At
- Draguet Ma
- Drechsler E
- Dreyer E
- Drivas-koulouris I
- Drobac As
- du Pree Ta
- Du D
- Dubinin F
- Dubovsky M
- Duchovni E
- Duckeck G
- Ducu Oa
- Duda D
- Dudarev A
- Duflot L
- Dumitriu Ae
- Dunford M
- Dungs S
- Dunne K
- Duperrin A
- Duran Yildiz H
- Durglishvili A
- Dührssen M
- Dülsen C
- Düren M
- Dwyer Bl
- Dyckes Gi
- Dyndal M
- Dysch S
- Dziedzic Bs
- Eckerova B
- Eggleston Mg
- Egidio Purcino De Souza E
- Ehrke Lf
- Eigen G
- Einsweiler K
- Ekelof T
- Ekman Pa
- El Ghazali Y
- El Jarrari H
- El Moussaouy A
- Ellajosyula V
- Ellert M
- Ellinghaus F
- Elliot Aa
- Ellis N
- Elmsheuser J
- Elsing M
- Emeliyanov D
- Emerman A
- Enari Y
- Ene I
- Epari S
- Erdmann J
- Ereditato A
- Erland Pa
- Errenst M
- Escalier M
- Escobar C
- Etzion E
- Evans G
- Evans H
- Evans Mo
- Ezhilov A
- Ezzarqtouni S
- Fabbri F
- Fabbri L
- Facini G
- Fadeyev V
- Fakhrutdinov Rm
- Falciano S
- Falke Pj
- Falke S
- Faltova J
- Fan Y
- Fang Y
- Fanourakis G
- Fanti M
- Faraj M
- Farbin A
- Farilla A
- Farooque T
- Farrington Sm
- Fassi F
- Fassouliotis D
- Faucci Giannelli M
- Fawcett Wj
- Fayard L
- Fedin Ol
- Fedotov G
- Feickert M
- Feligioni L
- Fell A
- Fellers De
- Feng C
- Feng M
- Fenton Mj
- Fenyuk Ab
- Ferencz L
- Ferguson Sw
- Ferrando J
- Ferrari A
- Ferrari P
- Ferrari R
- Ferrere D
- Ferretti C
- Fiedler F
- Filipčič A
- Filmer Ek
- Filthaut F
- Fiolhais Mcn
- Fiorini L
- Fischer F
- Fisher Wc
- Fitschen T
- Fleck I
- Fleischmann P
- Flick T
- Flores Castillo Lr
- Flores L
- Flores M
- Follega Fm
- Fomin N
- Foo Jh
- Forland Bc
- Formica A
- Forti Ac
- Fortin E
- Fortman Aw
- Foti Mg
- Fountas L
- Fournier D
- Fox H
- Francavilla P
- Francescato S
- Franchini M
- Franchino S
- Francis D
- Franco L
- Franconi L
- Franklin M
- Frattari G
- Freegard Ac
- Freeman Pm
- Freund Ws
- Fritzsche N
- Froch A
- Froidevaux D
- Frost Ja
- Fu Y
- Fujimoto M
- Fullana Torregrosa E
- Fuster J
- Gabrielli A
- Gabrielli A
- Gadow P
- Gagliardi G
- Gagnon Lg
- Gallardo Ge
- Gallas Ej
- Gallop Bj
- Gamboa Goni R
- Gan Kk
- Ganguly S
- Gao J
- Gao Y
- Garay Walls Fm
- Garcia B
- Garcia-Sciveres M
- García Navarro Je
- García Pascual Ja
- García C
- Gardner Rw
- Garg D
- Garg Rb
- Gargiulo S
- Garner Ca
- Garonne V
- Gasiorowski Sj
- Gaspar P
- Gaudio G
- Gauzzi P
- Gavrilenko Il
- Gavrilyuk A
- Gay C
- Gaycken G
- Gazis En
- Geanta Aa
- Gee Cm
- Geisen J
- Geisen M
- Gemme C
- Genest Mh
- Gentile S
- George S
- George Wf
- Geralis T
- Gerlach Lo
- Gessinger-Befurt P
- Ghasemi Bostanabad M
- Ghneimat M
- Ghosal A
- Ghosh A
- Ghosh A
- Giacobbe B
- Giagu S
- Giangiacomi N
- 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
- Glisic M
- Gnesi I
- Go Y
- Goblirsch-Kolb M
- Gocke B
- Godin D
- Goldfarb S
- Golling T
- Gololo Mgd
- Golubkov D
- Gombas Jp
- Gomes A
- Gomez Delegido Aj
- Goncalves Gama R
- Gonçalo R
- Gonella G
- Gonella L
- Gongadze A
- Gonnella F
- Gonski Jl
- Gonzalez Fernandez S
- Gonzalez Lopez R
- Gonzalez Renteria C
- Gonzalez Suarez R
- Gonzalez-Sevilla S
- Gonzalvo Rodriguez Gr
- González Andana Ry
- González de la Hoz S
- Goossens L
- Gorasia Na
- Gorbounov Pa
- Gorini B
- Gorini E
- Gorišek A
- Goshaw At
- Gostkin Mi
- Gottardo Ca
- Gouighri M
- Goumarre V
- Goussiou Ag
- Govender N
- Goy C
- Grabowska-Bold I
- Graham K
- Gramstad E
- Grancagnolo S
- Grandi M
- Gratchev V
- Gravila Pm
- Gravili Fg
- Gray Hm
- Greco M
- Grefe C
- Gregor Im
- Grenier P
- Grieco C
- Grillo Aa
- Grimm K
- Grinstein S
- Grivaz J-
- Gross E
- Grosse-Knetter J
- Grud C
- Grummer A
- Grundy Jc
- Guan L
- Guan W
- Gubbels C
- Guerrero Rojas Jgr
- Guerrieri G
- Guescini F
- Gugel R
- Guhit Jam
- Guida A
- Guillemin T
- Guilloton E
- Guindon S
- Guo F
- Guo J
- Guo L
- Guo Y
- Gupta R
- Gurbuz S
- Gustavino G
- Guth M
- Gutierrez Zagazeta Lf
- Gutierrez P
- Gutschow C
- Guyot C
- Gwenlan C
- Gwilliam Cb
- Haaland Es
- Haas A
- Habedank M
- Haber C
- Hadavand Hk
- Hadef A
- Hadzic S
- Haleem M
- Haley J
- Hall Jj
- Hallewell Gd
- Halser L
- Hamano K
- Hamdaoui H
- Hamer M
- Hamity Gn
- Han J
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- Hance M
- Hangal Da
- Hank Md
- Hankache R
- Hansen Jb
- Hansen Jd
- Hansen Ph
- Hara K
- Harada D
- Harenberg T
- Harkusha S
- Harris Yt
- Harrison Pf
- Hartman Nm
- Hartmann Nm
- Hasegawa Y
- Hasib A
- Haug S
- Hauser R
- Havranek M
- Hawkes Cm
- Hawkings Rj
- Hayashida S
- Hayden D
- Hayes C
- Hayes Rl
- Hays Cp
- Hays Jm
- Hayward Hs
- He F
- He Y
- He Y
- Heath Mp
- Hedberg V
- Heggelund Al
- Hehir Nd
- Heidegger C
- Heidegger Kk
- Heidorn Wd
- Heilman J
- Heim S
- Heim T
- Heinemann B
- Heinlein Jg
- Heinrich Jj
- Heinrich L
- Hejbal J
- Helary L
- Held A
- Hellesund S
- Helling Cm
- Hellman S
- Helsens C
- Henderson Rcw
- Henkelmann L
- Henriques Correia Am
- Herde H
- Hernández Jiménez Y
- Herr H
- Herrmann Mg
- Herrmann T
- Herten G
- Hertenberger R
- Hervas L
- Hessey Np
- Hibi H
- Higón-Rodriguez E
- Hillier Sj
- Hinchliffe I
- Hinterkeuser F
- Hirose M
- Hirose S
- Hirschbuehl D
- Hiti B
- Hobbs J
- Hobincu R
- Hod N
- Hodgkinson Mc
- Hodkinson Bh
- Hoecker A
- Hofer J
- Hohn D
- Holm T
- Holzbock M
- Hommels Lbah
- Honan Bp
- Hong J
- Hong Tm
- Hong Y
- Honig Jc
- Hooberman Bh
- Hopkins Wh
- Horii Y
- Hou S
- Howarth J
- Hoya J
- Hönle A
- Hrabovsky M
- Hryn'Ova T
- Hrynevich A
- Hsu Pj
- Hsu S-
- Hu Q
- Hu Yf
- Huang Dp
- Huang S
- Huang X
- Huang Y
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- Huang Z
- Hubacek Z
- Huebner M
- Huegging F
- Huffman Tb
- Huhtinen M
- Huiberts Sk
- Hulsken R
- Huseynov N
- Huston J
- Huth J
- Hyneman R
- Hyrych S
- Iacobucci G
- Iakovidis G
- Ibragimov I
- Iconomidou-Fayard L
- Iengo P
- Iguchi R
- Iizawa T
- Ikegami Y
- Ilg A
- Ilic N
- Imam H
- Ingebretsen Carlson T
- Introzzi G
- Iodice M
- Ippolito V
- Ishino M
- Islam W
- Issever C
- Istin S
- Ito H
- Iturbe Ponce Jm
- Iuppa R
- Ivina A
- Izen Jm
- Izzo V
- Jacka P
- Jackson P
- Jacobs Rm
- Jaeger Bp
- Jagfeld Cs
- Jakobs K
- Jakoubek T
- Jamieson J
- Janas Kw
- Jarlskog G
- Jaspan Ae
- Javurkova M
- Javůrek T
- Jäkel G
- Jeanneau F
- Jeanty L
- Jejelava J
- Jenni P
- Jessiman Ce
- Jézéquel S
- Jia J
- Jia X
- Jia X
- Jia Z
- Jiang Y
- Jiggins S
- Jimenez Pena J
- Jin S
- Jinaru A
- Jinnouchi O
- Jivan H
- Johansson P
- Johns Ka
- Johnson Ca
- Jones Dm
- Jones E
- Jones Rwl
- Jones Tj
- Jovicevic J
- Ju X
- Junggeburth Jj
- Juste Rozas A
- Kabana S
- Kaczmarska A
- Kado M
- Kagan H
- Kagan M
- Kahn A
- Kahn A
- Kahra C
- Kaji T
- Kajomovitz E
- Kakati N
- Kalderon Cw
- Kamenshchikov A
- Kang Nj
- Kano Y
- Kar D
- Karava K
- Kareem Mj
- Karentzos E
- Karkanias I
- Karpov Sn
- Karpova Zm
- Kartvelishvili V
- Karyukhin An
- Kasimi E
- Kato C
- Katzy J
- Kaur S
- Kawade K
- Kawagoe K
- Kawaguchi T
- Kawamoto T
- Kawamura G
- Kay Ef
- Kaya Fi
- Kazakos S
- Kazanin Vf
- Ke Y
- Keaveney Jm
- Keeler R
- Kehris Gv
- Keller Js
- Kelly As
- Kelsey D
- Kempster Jj
- Kendrick J
- Kennedy Ke
- Kepka O
- Kerridge Bp
- Kersten S
- Kerševan Bp
- Keszeghova L
- Ketabchi Haghighat S
- Khandoga M
- Khanov A
- Kharlamov Ag
- Kharlamova T
- Khoda Ee
- Khoo Tj
- Khoriauli G
- Khubua J
- Khwaira Yar
- Kiehn M
- Kilgallon A
- Kim E
- Kim Yk
- Kimura N
- Kirchhoff A
- Kirchmeier D
- Kirfel C
- Kirk J
- Kiryunin Ae
- Kishimoto T
- Kisliuk Dp
- Kitsaki C
- Kivernyk O
- Klassen M
- Klein C
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- Klein Mh
- Klein U
- Klimek P
- Klimentov A
- Klimpel F
- Klingl T
- Klioutchnikova T
- Klitzner Ff
- Kluit P
- Kluth S
- Kneringer E
- Knight Tm
- Knue A
- Kobayashi D
- Kobayashi R
- Kocian M
- Kodama T
- Kodyš P
- Koeck Dm
- Koenig Pt
- Koffas T
- Kolb M
- Koletsou I
- Komarek T
- Kong Axy
- Kono T
- Konstantinidis N
- Konya B
- Kopeliansky R
- Koperny S
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- Korolkov I
- Korotkova N
- Kortman B
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- Kostecka Wh
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- Kotsokechagia A
- Kotwal A
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- Kourkoumeli-Charalampidi A
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- Publication venue
- ELSEVIER
- Publication date
- 01/01/2023
- Field of study
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
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
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- Aielli G
- Aizenberg I
- Akbiyik M
- Akesson TPA
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
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- Alves FLL
- Alviggi MG
- Ambler A
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- Amelung C
- Amidei D
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- Amos KR
- Amrouche CS
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- Anastopoulos C
- Andana RYG
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- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
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- Antonelli M
- Antrim DJA
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- Aoki M
- Aparo MA
- Appelt C
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- Araya ST
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- Armbruster AJ
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- Zhemchugov A
- Zheng Z
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- Zieminska D
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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.]
Determination of the parton distribution functions of the proton using diverse ATLAS data from pp collisions at √s = 7, 8 and 13 TeV
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- Zambito S
- Zanzi D
- Zaplatilek O
- Zeitnitz C
- Zeißner SV
- Zeng JC
- Zenger DT
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang X
- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- 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 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
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
This paper presents an analysis at next-to-next-to-leading order in the theory of quantum chromodynamics for the determination of a new set of proton parton distribution functions using diverse measurements in pp collisions at \sqrt{s} = 7, 8 and 13 TeV, performed by the ATLAS experiment at the Large Hadron Collider, together with deep inelastic scattering data from ep collisions at the HERA collider. The ATLAS data sets considered are differential cross-section measurements of inclusive W^{±} and Z/gamma^{*} boson production, W^{±} and Z boson production in association with jets, t\bar{t} production, inclusive jet production and direct photon production. In the analysis, particular attention is paid to the correlation of systematic uncertainties within and between the various ATLAS data sets and to the impact of model, theoretical and parameterisation uncertainties. The resulting set of parton distribution functions is called ATLASpdf21
Modelling and computational improvements to the simulation of single vector-boson plus jet processes for the ATLAS experiment
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
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- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Achkar B
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- Alberghi GL
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- Zhemchugov A
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- Zimmermann S
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- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
This paper presents updated Monte Carlo configurations used to model the production of single electroweak vector bosons (W, Z/gamma*) in association with jets in proton-proton collisions for the ATLAS experiment at the Large Hadron Collider. Improvements pertaining to the electroweak input scheme, parton-shower splitting kernels and scale-setting scheme are shown for multi-jet merged configurations accurate to next-to-leading order in the strong and electroweak couplings. The computational resources required for these set-ups are assessed, and approximations are introduced resulting in a factor three reduction of the per-event CPU time without affecting the physics modelling performance. Continuous statistical enhancement techniques are introduced by ATLAS in order to populate low cross-section regions of phase space and are shown to match or exceed the generated effective luminosity. This, together with the lower per-event CPU time, results in a 50% reduction in the required computing resources compared to a legacy set-up previously used by the ATLAS collaboration. The set-ups described in this paper will be used for future ATLAS analyses and lay the foundation for the next generation of Monte Carlo predictions for single vector-boson plus jets production
Search for dark photons in rare Z boson decays with the ATLAS detector
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- Yamaguchi Y
- Yamashita E
- Yamauchi H
- Yamazaki T
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- Yao W-M
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- Yeo BK
- Yexley MR
- Yildiz H Duran
- Yin P
- Yorita K
- Younas S
- Young C
- Young CJS
- Yu Y
- Yuan M
- Yuan R
- Yue L
- Zaazoua M
- Zabinski B
- Zaid E
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zamora Saa JA
- Zang J
- Zanzi D
- Zaplatilek O
- Zeitnitz C
- Zeng H
- Zeng JC
- Zenger DT
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhai M
- Zhang B
- Zhang DF
- Zhang J
- Zhang J
- Zhang K
- Zhang L
- 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
- American Physical Society
- Publication date
- 01/01/2023
- Field of study
A search for events with a dark photon produced in association with a dark Higgs boson via rare decays of the standard model
Z
boson is presented, using
139
fb
−
1
of
√
s
=
13
TeV
proton-proton collision data recorded by the ATLAS detector at the Large Hadron Collider. The dark boson decays into a pair of dark photons, and at least two of the three dark photons must each decay into a pair of electrons or muons, resulting in at least two same-flavor opposite-charge lepton pairs in the final state. The data are found to be consistent with the background prediction, and upper limits are set on the dark photon’s coupling to the dark Higgs boson times the kinetic mixing between the standard model photon and the dark photon,
α
D
ϵ
2
, in the dark photon mass range of [5, 40] GeV except for the
Υ
mass window [8.8, 11.1] GeV. This search explores new parameter space not previously excluded by other experiments
Combined measurement of the Higgs boson mass from the H → γγ and H → ZZ∗ → 4ℓ decay channels with the ATLAS detector using √s = 7, 8, and 13 TeV pp collision data
- Author
- Aad G
- Abbott B
- Abeling K
- Abicht NJ
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adam Bourdarios C
- Adamczyk 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
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- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
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- Zhu Y
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- 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
- American Physical Society
- Publication date
- 01/01/2023
- Field of study
A measurement of the mass of the Higgs boson combining the
H
→
Z
Z
∗
→
4
ℓ
and
H
→
γ
γ
decay channels is presented. The result is based on
140
fb
−
1
of proton-proton collision data collected by the ATLAS detector during LHC run 2 at a center-of-mass energy of 13 TeV combined with the run 1 ATLAS mass measurement, performed at center-of-mass energies of 7 and 8 TeV, yielding a Higgs boson mass of
125.11
±
0.09
(
stat
)
±
0.06
(
syst
)
=
125.11
±
0.11
GeV
. This corresponds to a 0.09% precision achieved on this fundamental parameter of the Standard Model of particle physics
Direct constraint on the Higgs–charm coupling from a search for Higgs boson decays into charm quarks with the ATLAS detector
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- Ottino GJ
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- Ouellette J
- Ould-Saada F
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- Owen RE
- O’Keefe MW
- O’Neil DC
- O’neill AP
- O’Shea V
- Pardos CD
- Pascual JAG
- Paz IL
- Pena JJ
- Pietra MD
- Pino SAO
- Ponce JMI
- Pozo JAA
- Pree TAD
- Pretel JAF
- Ramos JM
- Renteria CG
- Rodriguez GRG
- Rojas JGRG
- Romero LM
- Rosende SJN
- Rozas AJ
- Sanchez FJM
- Santos SPAD
- Seabra LFO
- Sola JDB
- Solis AL
- Suarez PM
- Suarez RG
- Tame ZPA
- Toro RC
- Torregrosa EF
- Urbán SC
- Vazquez CJB
- Verzini MJA
- Volpe DD
- Walls FMG
- Yildiz HD
- Zagazeta LFG
- Åkesson TPA
- Öncel ÖO
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/08/2022
- Field of study
A search for the Higgs boson decaying into a pair of charm quarks is presented. The analysis uses proton–proton collisions to target the production of a Higgs boson in association with a leptonically decaying W or Z boson. The dataset delivered by the LHC at a centre-of-mass energy of and recorded by the ATLAS detector corresponds to an integrated luminosity of 139 fb−1. Flavour-tagging algorithms are used to identify jets originating from the hadronisation of charm quarks. The analysis method is validated with the simultaneous measurement of WW, WZ and ZZ production, with observed (expected) significances of 2.6 (2.2) standard deviations above the background-only prediction for the (W/Z)Z(→cc¯) process and 3.8 (4.6) standard deviations for the (W/Z)W(→cq) process. The (W/Z)H(→cc¯) search yields an observed (expected) upper limit of 26 (31) times the predicted Standard Model cross-section times branching fraction for a Higgs boson with a mass of , corresponding to an observed (expected) constraint on the charm Yukawa coupling modifier |κc|<8.5 (12.4), at the 95% confidence level. A combination with the ATLAS (W/Z)H,H→bb¯ analysis is performed, allowing the ratio κc/κb to be constrained to less than 4.5 at the 95% confidence level, smaller than the ratio of the b- and c-quark masses, and therefore determines the Higgs-charm coupling to be weaker than the Higgs-bottom coupling at the 95% confidence level
Search for neutral long-lived particles in pp collisions at s√ = 13 TeV that decay into displaced hadronic jets in the ATLAS calorimeter
- Author
- Aad G
- Abbott B
- Abbott DC
- Abed Abud A
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Achkar B
- Adam Bourdarios C
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Aizenberg I
- Akbiyik M
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
A search for decays of pair-produced neutral long-lived particles (LLPs) is presented using 139 fb−1 of proton-proton collision data collected by the ATLAS detector at the LHC in 2015–2018 at a centre-of-mass energy of 13 TeV. Dedicated techniques were developed for the reconstruction of displaced jets produced by LLPs decaying hadronically in the ATLAS hadronic calorimeter. Two search regions are defined for different LLP kinematic regimes. The observed numbers of events are consistent with the expected background, and limits for several benchmark signals are determined. For a SM Higgs boson with a mass of 125 GeV, branching ratios above 10% are excluded at 95% confidence level for values of c times LLP mean proper lifetime in the range between 20 mm and 10 m depending on the model. Upper limits are also set on the cross-section times branching ratio for scalars with a mass of 60 GeV and for masses between 200 GeV and 1 TeV
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