195 research outputs found
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- 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
- Adachi S
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- Adamek L
- Adelman J
- Adersberger M
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- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Search for heavy neutral Higgs bosons produced in association with b-quarks and decaying into b-quarks at root s=13 TeV with the ATLAS detector
- Author
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- Yildiz HD
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- Zakharchuk N
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- Zanzi D
- Zaripovas DR
- Zeiner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
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- Zhang Z
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- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
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- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- 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
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 13/08/2020
- Field of study
A search for heavy neutral Higgs bosons produced in association with one or two
b
-quarks and decaying to
b
-quark pairs is presented using
27.8
fb
−
1
of
√
s
=
13
TeV
proton-proton collision data recorded by the ATLAS detector at the Large Hadron Collider during 2015 and 2016. No evidence of a signal is found. Upper limits on the heavy neutral Higgs boson production cross section times its branching ratio to
b
¯
b
are set, ranging from 4.0 to 0.6 pb at 95% confidence level over a Higgs boson mass range of 450 to 1400 GeV. Results are interpreted within the two-Higgs-doublet model and the minimal supersymmetric Standard Model
Erratum: Measurement of angular and momentum distributions of charged particles within and around jets in Pb + Pb and pp collisions at √sNN = 5.02 TeV with the ATLAS detector [Phys. Rev. C 100 , 064901 (2019)]
- Author
- Aad G
- Abbott B
- Abbott Dc
- Abed Abud A
- Abeling K
- Abhayasinghe Dk
- Abidi Sh
- Abouzeid Os
- Abraham Nl
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya Bs
- Achkar B
- Adachi S
- Adam Bourdarios C
- 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
- Agheorghiesei C
- Aguilar-Saavedra Ja
- Ahmadov F
- Ahmed Ws
- Ai X
- Aielli G
- Akatsuka S
- Akesson Tpa
- Akilli E
- Akimov Av
- Al Khoury K
- Alberghi Gl
- Albert J
- Alconada Verzini Mj
- Alderweireldt S
- Aleksa M
- Aleksandrov In
- Alexa C
- Alexandre D
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire Sp
- Allaire C
- Allbrooke Bmm
- Allen Bw
- Allport Pp
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri Aa
- Alvarez Estevez M
- Alvarez Piqueras D
- Alviggi Mg
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos Sp
- Amoroso S
- Amrouche Cs
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders Cf
- Anders Jk
- Andreazza A
- Andrei V
- Anelli Cr
- Angelidakis S
- Angerami A
- Anisenkov Av
- Annovi A
- Antel C
- Anthony Mt
- Antonelli M
- Antrim Dja
- Anulli F
- Aoki M
- Aparisi Pozo Ja
- Aperio Bella L
- Arabidze G
- Araque Jp
- Araujo Ferraz V
- Araujo Pereira R
- Arcangeletti C
- Arce Ath
- Arduh Fa
- Arguin J-
- Argyropoulos S
- Arling J-
- Armbruster Aj
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- Arnold H
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- Artamonov A
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- Artz S
- Asai S
- Asbah N
- Asimakopoulou Em
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Atkin Rj
- Atkinson M
- Atlay Nb
- Atmani H
- Augsten K
- Avolio G
- Avramidou R
- Ayoub Mk
- Azoulay Am
- Azuelos G
- Bachacou H
- Bachas K
- Backes M
- Backman F
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey Aj
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- Baines Jt
- Bajic M
- Bakalis C
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- Balli F
- Balunas Wk
- Balz J
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura Aae
- Barak L
- Barbe Wm
- Barberio El
- Barberis D
- Barbero M
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- Barillari T
- Barisits M-
- Barkeloo J
- Barklow T
- Barnea R
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- Barnovska-Blenessy Z
- Baroncelli A
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- Barr Aj
- Barranco Navarro L
- Barreiro Guimaraes Da Costa J
- Barreiro F
- Barsov S
- Bartoldus R
- Bartolini G
- Barton Ae
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- Bates Rl
- Batlamous S
- Batley Jr
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- Battaglia M
- Bauce M
- Bauer F
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- Beacham Jb
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- Bechtle P
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- Becot C
- Beddall A
- Beddall Aj
- Bednyakov Va
- Bedognetti M
- Bee Cp
- Beermann Ta
- Begalli M
- Begel M
- Behera A
- Behr Jk
- Beisiegel F
- Bell As
- Bella G
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev Nl
- Benchekroun D
- Benekos N
- Benhammou Y
- Benjamin Dp
- Benoit M
- Bensinger Jr
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Bergeaas Kuutmann E
- Berger N
- Bergmann B
- Bergsten Lj
- Beringer J
- Berlendis S
- Bernard Nr
- Bernardi G
- Bernius C
- Berry T
- Berta P
- Bertella C
- Bertram Ia
- Bessidskaia Bylund O
- Besson N
- Bethani A
- Bethke S
- Betti A
- Bevan Aj
- Beyer J
- Bhattacharya Ds
- Bhattarai P
- Bi R
- Bianchi Rm
- Biebel O
- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz Nv
- Biglietti M
- Billoud Trv
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Birman M
- Bisanz T
- Biswal Jp
- Biswas D
- Bitadze A
- Bittrich C
- Bjorke K
- Black Km
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Bobbink Gj
- Bobrovnikov Vs
- Bocchetta Ss
- Bocci A
- Boerner D
- Bogavac D
- Bogdanchikov Ag
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Boldyrev As
- Bolz Ae
- Bomben M
- Bona M
- Bonilla Js
- Boonekamp M
- Booth Cd
- Borecka-Bielska Hm
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Boscherini D
- Bosman M
- Bossio Sola Jd
- Bouaouda K
- Boudreau J
- Bouhova-Thacker Ev
- Boumediene D
- 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
- Breaden Madden Wd
- Brendlinger K
- Brenner L
- Brenner R
- Bressler S
- Brickwedde B
- Briglin Dl
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks Wk
- Brost E
- Broughton Jh
- Bruckman De Renstrom Pa
- Bruncko D
- Bruni A
- Bruni G
- Bruni Ls
- Bruno S
- Brunt Bh
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley Ag
- Budagov Ia
- Bugge Mk
- Buhrer F
- Bulekov O
- Burch Tj
- Burdin S
- Burgard Cd
- Burger Am
- Burghgrave B
- Burr Jtp
- Burton Cd
- Burzynski Jc
- Buscher V
- Buschmann E
- Bussey Pj
- Butler Jm
- Buttar Cm
- Butterworth Jm
- Butti P
- Buttinger W
- Buxo Vazquez Cj
- Buzatu A
- Buzykaev Ar
- Cabras G
- Cabrera Urban S
- Caforio D
- Cai H
- Cairo Vmm
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba Lp
- Calvente Lopez S
- Calvet D
- Calvet S
- Calvet Tp
- Calvetti M
- Camacho Toro R
- Camarda S
- Camarero Munoz D
- Camarri P
- Cameron D
- Caminal Armadans R
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Canesse A
- Cano Bret M
- Cantero J
- Cao T
- Cao Y
- Capeans Garrido Mdm
- Capua M
- Cardarelli R
- Cardillo F
- Carducci G
- Carli I
- Carli T
- Carlino G
- Carlson Bt
- Carminati L
- Carney Rmd
- Caron S
- Carquin E
- Carra S
- Carter Jws
- Casado Mp
- Casha Af
- Casper Dw
- Castelijn R
- Castillo Gimenez V
- Castillo Fl
- Castro Nf
- Catinaccio A
- Catmore Jr
- Cattai A
- Caudron J
- Cavaliere V
- Cavallaro E
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
- Ceradini F
- Cerda Alberich L
- Cerny K
- Cerqueira As
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin Sa
- Chadi Z
- Chakraborty D
- Chan Sk
- Chan Ws
- Chan Wy
- Chapman Jd
- Chargeishvili B
- Charlton Dg
- Charman Tp
- Chau Cc
- Che S
- Chekanov S
- Chekulaev Sv
- Chelkov Ga
- Chelstowska Ma
- Chen B
- Chen C
- Chen Ch
- Chen H
- Chen J
- Chen J
- Chen S
- Chen Sj
- Chen X
- Chen Y
- Chen Y-
- Cheng Hc
- Cheng Hj
- Cheplakov A
- Cheremushkina E
- Cherkaoui El Moursli R
- Cheu E
- Cheung K
- Chevalerias Tja
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm As
- Chitan A
- Chiu I
- Chiu Yh
- Chizhov Mv
- Choi K
- Chomont Ar
- Chouridou S
- Chow Ys
- Chu Mc
- Chu X
- Chudoba J
- Chuinard Aj
- 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
- Clement C
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Cohen H
- Coimbra Aec
- Colasurdo L
- Cole B
- Colijn Ap
- Collot J
- Conde Muino P
- Coniavitis E
- Connell Sh
- Connelly Ia
- Constantinescu S
- Conventi F
- Cooper-Sarkar Am
- Cormier F
- Cormier Kjr
- Corpe Ld
- Corradi M
- Corrigan Ee
- Corriveau F
- Cortes-Gonzalez A
- Costa Mj
- Costanza F
- Costanzo D
- Cowan G
- Cowley Jw
- Crane J
- Cranmer K
- Crawley Sj
- Creager Ra
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Croft V
- Crosetti G
- Cueto A
- Cuhadar Donszelmann T
- Cukierman Ar
- Cunningham Wr
- Czekierda S
- Czodrowski P
- D'Amen G
- D'Amico V
- D'Auria S
- D'Eramo L
- D'Onofrio A
- D'Onofrio 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
- Dang Np
- Dann Ns
- Danninger M
- Dao V
- Darbo G
- Dartsi O
- Dattagupta A
- Daubney T
- Davey W
- David C
- Davidek T
- Davis Dr
- Dawson I
- De Asmundis R
- De Beurs M
- De Castro S
- De Cecco S
- De Groot N
- De Jong P
- De La Torre H
- De Maria A
- De Pedis D
- De Salvo A
- De Sanctis U
- De Santis M
- De Santo A
- De Vasconcelos Corga K
- De Vivie De Regie Jb
- De K
- Debenedetti C
- Dedovich Dv
- Deiana Am
- Del Gaudio M
- Del Peso J
- Delabat Diaz Y
- 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
- Denysiuk D
- Derendarz D
- Derkaoui Je
- Derue F
- Dervan P
- Desch K
- Deterre C
- Dette K
- Deutsch C
- Devesa Mr
- Deviveiros Po
- Dewhurst A
- 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
- Di Valentino D
- Diaconu C
- Dias Do Vale T
- Dias Fa
- Diaz Ma
- Dickinson J
- Diehl Eb
- Dietrich J
- Diez Cornell S
- Dimitrievska A
- Ding W
- Dingfelder J
- Dittus F
- Djama F
- Djobava T
- Djuvsland Ji
- Do Vale Mab
- Dobre M
- Dodsworth D
- Doglioni C
- Dolejsi J
- Dolezal Z
- Donadelli M
- Dong B
- Donini J
- Dopke J
- Doria A
- Dova Mt
- Doyle At
- Drechsler E
- Dreyer E
- Dreyer T
- Drobac As
- Du D
- Duan Y
- Dubinin F
- Dubovsky M
- Dubreuil A
- Duchovni E
- Duckeck G
- Ducourthial A
- Ducu Oa
- Duda D
- Dudarev A
- Dudder Ac
- Duffield Em
- Duflot L
- Duhrssen M
- Dulsen C
- Dumancic M
- Dumitriu Ae
- Duncan Ak
- Dunford M
- Duperrin A
- Duran Yildiz H
- Duren M
- Durglishvili A
- Duschinger D
- Dutta B
- Duvnjak D
- Dyckes Gi
- Dyndal M
- Dysch S
- Dziedzic Bs
- Ecker Km
- Edgar Rc
- Eggleston Mg
- Eifert T
- Eigen G
- Einsweiler K
- Ekelof T
- El Jarrari H
- El Kacimi M
- El Kosseifi R
- 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
- Errenst M
- Escalier M
- Escobar C
- Estrada Pastor O
- Etzion E
- Evans H
- 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
- Fang Y
- Fanourakis G
- Fanti M
- Faraj M
- Farbin A
- Farilla A
- Farina Em
- Farooque T
- Farrell S
- Farrington Sm
- Farthouat P
- Fassi F
- Fassnacht P
- Fassouliotis D
- Faucci Giannelli M
- Fawcett Wj
- Fayard L
- Fedin Ol
- Fedorko W
- Feickert M
- Feligioni L
- Fell A
- Feng C
- Feng Ej
- Feng M
- Fenton Mj
- Fenyuk Ab
- Ferrando J
- Ferrante A
- Ferrari A
- Ferrari P
- Ferrari R
- Ferreira De Lima De
- 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
- Fletcher Rrm
- Flick T
- Flierl Bm
- Flores Castillo Lr
- Flores L
- Follega Fm
- Fomin N
- Foo Jh
- Forcolin Gt
- Formica A
- Forster Fa
- Forti Ac
- Foster Ag
- Foti Mg
- Fournier D
- Fox H
- Francavilla P
- Francescato S
- Franchini M
- Franchino S
- Francis D
- Franconi L
- Franklin M
- Fray An
- Freeman Pm
- Freund B
- Freund Ws
- Freundlich Em
- Frizzell Dc
- Froidevaux D
- Frost Ja
- Fukunaga C
- Fullana Torregrosa E
- Fumagalli E
- Fusayasu T
- Fuster J
- Gabrielli A
- Gabrielli A
- Gach Gp
- Gadatsch S
- Gadow P
- Gagliardi G
- Gagnon Lg
- Galea C
- Galhardo B
- Gallardo Ge
- Gallas Ej
- Gallop Bj
- Galster G
- Gamboa Goni R
- Gan Kk
- Ganguly S
- Gao J
- Gao Y
- Gao Ys
- Garcia Navarro Je
- Garcia Pascual Ja
- Garcia C
- Garcia-Argos C
- Garcia-Sciveres M
- Gardner Rw
- Garelli N
- Gargiulo S
- Garonne V
- Gaudiello A
- Gaudio G
- Gavrilenko Il
- Gavrilyuk A
- Gay C
- Gaycken G
- Gazis En
- Geanta Aa
- Gee Cm
- Gee Cnp
- Geisen J
- Geisen M
- Geisler Mp
- Gemme C
- Genest Mh
- Geng C
- Gentile S
- George S
- Geralis T
- Gerlach Lo
- Gessinger-Befurt P
- Gessner G
- Ghasemi Bostanabad M
- Ghasemi S
- Ghosh A
- Ghosh A
- Giacobbe B
- Giagu S
- Giangiacomi N
- Giannetti P
- Giannini A
- Giannini G
- Gibson Sm
- Gignac M
- Gillberg D
- Gilles G
- Gingrich Dm
- Giordani Mp
- Giorgi Fm
- 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
- Goblirsch-Kolb M
- Godin D
- Goldfarb S
- Golling T
- Golubkov D
- Gomes A
- Goncalo R
- Goncalves Gama R
- Gonella G
- Gonella L
- Gongadze A
- Gonnella F
- Gonski Jl
- Gonzalez De La Hoz S
- Gonzalez-Sevilla S
- Gonzalvo Rodriguez Gr
- Goossens L
- Gorbounov Pa
- Gordon Ha
- Gorini B
- Gorini E
- Gorisek A
- Goshaw At
- Gostkin Mi
- Gottardo Ca
- Gouighri M
- Goujdami D
- Goussiou Ag
- Govender N
- Goy C
- Gozani E
- Grabowska-Bold I
- Graham Ec
- Gramling J
- Gramstad E
- Grancagnolo S
- Grandi M
- Gratchev V
- Gravila Pm
- Gravili Fg
- Gray C
- Gray Hm
- Grefe C
- Gregersen K
- Gregor Im
- Grenier P
- Grevtsov K
- Grieco C
- Grieser Na
- Griffiths J
- Grillo Aa
- Grimm K
- Grinstein S
- Grivaz J-
- Groh S
- Gross E
- Grosse-Knetter J
- Grout Zj
- Grud C
- Grummer A
- Guan L
- Guan W
- Guenther J
- Guerguichon A
- Guerrero Rojas Jgr
- Guescini F
- Guest D
- Gugel R
- Guillemin T
- Guindon S
- Gul U
- Guo J
- Guo W
- Guo Y
- Guo Z
- Gupta R
- Gurbuz S
- Gustavino G
- Guth M
- Gutierrez P
- Gutschow C
- Guyot C
- Gwenlan C
- Gwilliam Cb
- Haas A
- Haber C
- Hadavand Hk
- Haddad N
- Hadef A
- Hagebock S
- Haleem M
- Haley J
- Halladjian G
- Hallewell Gd
- Hamacher K
- Hamal P
- Hamano K
- Hamdaoui H
- Hamity Gn
- Han K
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- Han Yf
- Hanagaki K
- Hance M
- Handl Dm
- Haney B
- Hankache R
- Hansen E
- Hansen Jb
- Hansen Jd
- Hansen Mc
- Hansen Ph
- Hanson Ec
- Hara K
- Harenberg T
- Harkusha S
- Harrison Pf
- Hartmann Nm
- Hasegawa Y
- Hasib A
- Hassani S
- Haug S
- Hauser R
- Havener Lb
- Havranek M
- Hawkes Cm
- Hawkings Rj
- Hayden D
- Hayes C
- Hayes Rl
- Hays Cp
- Hays Jm
- Hayward Hs
- Haywood Sj
- He F
- Heath Mp
- Hedberg V
- Heelan L
- Heer S
- Heidegger Kk
- Heidorn Wd
- Heilman J
- Heim S
- Heim T
- Heinemann B
- Heinrich Jj
- Heinrich L
- Heinz C
- Hejbal J
- Helary L
- Held A
- Hellesund S
- Helling Cm
- Hellman S
- Helsens C
- Henderson Rcw
- Heng Y
- Henkelmann S
- Henriques Correia Am
- Herbert Gh
- Herde H
- Herget V
- Hernandez Jimenez Y
- Herr H
- Herrmann Mg
- Herrmann T
- Herten G
- Hertenberger R
- Hervas L
- Herwig Tc
- Hesketh Gg
- Hessey Np
- Higashida A
- Higashino S
- Higon-Rodriguez E
- Hildebrand K
- Hill E
- Hill Jc
- Hill Kk
- Hiller Kh
- Hillier Sj
- Hils M
- Hinchliffe I
- Hinterkeuser F
- Hirose M
- Hirose S
- Hirschbuehl D
- Hiti B
- Hladik O
- Hlaluku Dr
- Hoad X
- Hobbs J
- Hod N
- Hodgkinson Mc
- Hoecker A
- Hoenig F
- Hohn D
- Hohov D
- Holmes Tr
- Holzbock M
- Hommels Lbah
- Honda S
- Hong Tm
- Honig Jc
- Honle A
- Hooberman Bh
- Hopkins Wh
- Horii Y
- Horn P
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- Hou S
- Hoummada A
- Howarth J
- Hoya J
- Hrabovsky M
- Hrdinka J
- Hristova I
- Hrivnac J
- Hryn'Ova T
- Hrynevich A
- Hsu Pj
- Hsu S-
- Hu Q
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- Hu Yf
- Huang Dp
- Huang Y
- Huang Y
- Hubacek Z
- Hubaut F
- Huebner M
- Huegging F
- Huffman Tb
- Huhtinen M
- Hunter Rfh
- Huo P
- Hupe Am
- Huseynov N
- Huston J
- Huth J
- Hyneman R
- Hyrych S
- Iacobucci G
- Iakovidis G
- Ibragimov I
- Iconomidou-Fayard L
- Idrissi Z
- Iengo P
- Ignazzi R
- Igonkina O
- Iguchi R
- Iizawa T
- Ikegami Y
- Ikeno M
- Iliadis D
- Ilic N
- Iltzsche F
- Introzzi G
- Iodice M
- Iordanidou K
- Ippolito V
- Isacson Mf
- Ishino M
- Islam W
- Issever C
- Istin S
- Ito F
- Iturbe Ponce Jm
- Iuppa R
- Ivina A
- Iwasaki H
- Izen Jm
- Izzo V
- Jacka P
- Jackson P
- Jacobs Rm
- Jaeger Bp
- Jain V
- Jakel G
- Jakobi Kb
- Jakobs K
- Jakobsen S
- Jakoubek T
- Jamieson J
- Janas Kw
- Jansky R
- Janssen J
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- Javadov N
- Javurek T
- Javurkova M
- Jeanneau F
- Jeanty L
- Jejelava J
- Jelinskas A
- Jenni P
- Jeong J
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- Jezequel S
- Ji H
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- Jiang H
- Jiang Y
- Jiang Z
- Jiggins S
- Jimenez Morales Fa
- Jimenez Pena J
- Jin S
- Jinaru A
- Jinnouchi O
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- Johansson P
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- Jones Rwl
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- Jones Tj
- Jongmanns J
- Jorge Pm
- Jovicevic J
- Ju X
- Junggeburth Jj
- Juste Rozas A
- Kaczmarska A
- Kado M
- Kagan H
- Kagan M
- Kahra C
- Kaji T
- Kajomovitz E
- Kalderon Cw
- Kaluza A
- Kamenshchikov A
- Kaneda M
- Kanjir L
- Kano Y
- Kantserov Va
- Kanzaki J
- Kaplan Ls
- Kar D
- Karava K
- Kareem Mj
- Karpov Sn
- Karpova Zm
- Kartvelishvili V
- Karyukhin An
- Kashif L
- Kass Rd
- Kastanas A
- Kato C
- Katzy J
- Kawade K
- Kawagoe K
- Kawaguchi T
- Kawamoto T
- Kawamura G
- Kay Ef
- Kazanin Vf
- Keeler R
- Kehoe R
- Keller Js
- Kellermann E
- Kelsey D
- Kempster Jj
- Kendrick J
- Kepka O
- Kersevan Bp
- Kersten S
- Ketabchi Haghighat S
- Khader M
- Khalil-Zada F
- Khandoga M
- Khanov A
- Kharlamov Ag
- Kharlamova T
- Khoda Ee
- Khodinov A
- Khoo Tj
- Khramov E
- Khubua J
- Kido S
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- Kilby Cr
- Kim Yk
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- Kind Om
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- Kirk J
- Kiryunin Ae
- Kishimoto T
- Kisliuk Dp
- Kitali V
- Kivernyk O
- Klapdor-Kleingrothaus T
- Klassen M
- Klein M
- Klein Mh
- Klein U
- Kleinknecht K
- Klimek P
- Klimentov A
- Klingl T
- Klioutchnikova T
- Klitzner Ff
- Kluit P
- Kluth S
- Kneringer E
- Knoops Ebfg
- Knue A
- Kobayashi D
- Kobayashi T
- Kobel M
- Kocian M
- Kodys P
- Koenig Pt
- Koffas T
- Kohler Nm
- Koi T
- Kolb M
- Koletsou I
- Komarek T
- Kondo T
- Kondrashova N
- Koneke K
- Konig Ac
- Kono T
- Konoplich R
- Konstantinides V
- Konstantinidis N
- Konya B
- Kopeliansky R
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- Koren G
- Korn A
- Korolkov I
- Korolkova Ev
- Korotkova N
- Kortner O
- Kortner S
- Kosek T
- Kostyukhin Vv
- Kotsokechagia A
- Kotwal A
- Koulouris A
- Kourkoumeli-Charalampidi A
- Kourkoumelis C
- Kourlitis E
- Kouskoura V
- Kowalewska Ab
- Kowalewski R
- Kozakai C
- Kozanecki W
- Kozhin As
- Kramarenko Va
- Kramberger G
- Krasnopevtsev D
- Krasny Mw
- Krasznahorkay A
- Krauss D
- Kremer Ja
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- Wieseotte N
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- Woods Nl
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- Wosiek Bk
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- Wraight K
- Wu Sl
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- Wyatt Tr
- Wynne Bm
- Xella S
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- Xiao X
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- Xu D
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- Yabsley B
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- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
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- Yamazaki T
- Yamazaki Y
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- Yao W-
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- Yexley Mr
- Yigitbasi E
- Yorita K
- Yoshihara K
- Young C
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- Yu J
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- Yue X
- Yuen Spy
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev Am
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas Dr
- Zeissner Sv
- Zeitnitz C
- Zemaityte G
- Zeng Jc
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang Df
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- 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 M
- Zhou Ms
- 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
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas Tg
- Zou R
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2020
- Field of study
Measurement of the tt¯tt¯ production cross section in pp collisions at √s=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abed Abud A
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Achkar B
- Adam Bourdarios C
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
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- Alberghi GL
- Albert J
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- Angelidakis S
- Angerami A
- Anisenkov AV
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- Araujo Ferraz V
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- de Jong P
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- Denisov SP
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- Zeißner SV
- Zemaityte G
- Zeng JC
- Zenin O
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- Zgubič M
- Zhang B
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- Zhang G
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- Zhao P
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu H
- Zhu HL
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- Zhu Y
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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
Measurement of single top-quark production in association with a W boson in the single-lepton channel at \sqrt{s} = 8\,\text {TeV} with the ATLAS detector
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- Abbott B
- Abbott DC
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- Abhayasinghe DK
- Abidi SH
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- Zakharchuk N
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- Zaripovas DR
- Zeissner S
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- Zemaityte G
- Zeng JC
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- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
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- Zhu C
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- Zhu HL
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- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
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- Zimmermann S
- Zinonos Z
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2021
- Field of study
The production cross-section of a top quark in association with a W boson is measured using proton–proton collisions at \sqrt{s} = 8\,\text {TeV}. The dataset corresponds to an integrated luminosity of 20.2\,\text {fb}^{-1}, and was collected in 2012 by the ATLAS detector at the Large Hadron Collider at CERN. The analysis is performed in the single-lepton channel. Events are selected by requiring one isolated lepton (electron or muon) and at least three jets. A neural network is trained to separate the tW signal from the dominant t{\bar{t}} background. The cross-section is extracted from a binned profile maximum-likelihood fit to a two-dimensional discriminant built from the neural-network output and the invariant mass of the hadronically decaying W boson. The measured cross-section is \sigma _{tW} = 26 \pm 7\,\text {pb}, in good agreement with the Standard Model expectation
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at √=13TeV
- Author
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- Zhemchugov A
- Zheng Z
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- Zieminska D
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- Zimmermann S
- Zinonos Z
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- Zoccoli A
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- Zorbas TG
- Zou R
- Zwalinski L
- 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
Muon reconstruction and identification efficiency in ATLAS using the full Run 2 pp collision data set at \sqrt{s}=13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
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- Acharya BS
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- Zenin O
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zieminska D
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- Zimmermann S
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- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- 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
Performance of the upgraded PreProcessor of the ATLAS Level-1 Calorimeter Trigger
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
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- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- Zwalinski L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2020
- Field of study
The PreProcessor of the ATLAS Level-1 Calorimeter Trigger prepares the analogue trigger signals sent from the ATLAS calorimeters by digitising, synchronising, and calibrating them to reconstruct transverse energy deposits, which are then used in further processing to identify event features. During the first long shutdown of the LHC from 2013 to 2014, the central components of the PreProcessor, the Multichip Modules, were replaced by upgraded versions that feature modern ADC and FPGA technology to ensure optimal performance in the high pile-up environment of LHC Run 2. This paper describes the features of the newMultichip Modules along with the improvements to the signal processing achieved.ANPCyTYerPhI, ArmeniaAustralian Research CouncilBMWFW, AustriaAustrian Science Fund (FWF)Azerbaijan National Academy of Sciences (ANAS)SSTC, BelarusNational Council for Scientific and Technological Development (CNPq)Fundacao de Amparo a Pesquisa do Estado de Sao Paulo (FAPESP)Natural Sciences and Engineering Research Council of CanadaCanada Foundation for InnovationNational Natural Science Foundation of China (NSFC)Departamento Administrativo de Ciencia, Tecnología e Innovación ColcienciasMinistry of Education, Youth & Sports - Czech Republic
Czech Republic GovernmentCzech Republic GovernmentDNRF, DenmarkDanish Natural Science Research CouncilCentre National de la Recherche Scientifique (CNRS)CEA-DRF/IRFU, FranceFederal Ministry of Education & Research (BMBF)Max Planck SocietyGreek Ministry of Development-GSRTRGC and Hong Kong SAR, ChinaIsrael Science FoundationBenoziyo Center, IsraelIstituto Nazionale di Fisica Nucleare (INFN)Ministry of Education, Culture, Sports, Science and Technology, Japan (MEXT)Ministry of Education, Culture, Sports, Science and Technology, Japan (MEXT)
Japan Society for the Promotion of ScienceCNRST, MoroccoRCN, NorwayPortuguese Foundation for Science and TechnologyMNE/IFA, RomaniaMES of RussiaMESTD, SerbiaMSSR, SlovakiaSlovenian Research Agency - SloveniaMIZS, SloveniaSpanish GovernmentSRC, SwedenWallenberg Foundation, SwedenSNSF Geneva, SwitzerlandMinistry of Science and Technology, TaiwanMinistry of Energy & Natural Resources - TurkeyScience & Technology Facilities Council (STFC)United States Department of Energy (DOE)National Science Foundation (NSF)BCKDF, CanadaCANARIE, CanadaCRC, CanadaEuropean Research Council (ERC)European Union (EU)French National Research Agency (ANR)German Research Foundation (DFG)Alexander von Humboldt FoundationGreek NSRF, GreeceBSF-NSF, IsraelGerman-Israeli Foundation for Scientific Research and DevelopmentLa Caixa Banking Foundation, SpainCERCA Programme Generalitat de Catalunya, SpainPROMETEO, SpainGenT Programmes Generalitat Valenciana, SpainGoran Gustafssons Stiftelse, SwedenRoyal Society of LondonLeverhulme TrustNRC, CanadaCERNANID, ChileChinese Academy of SciencesMinistry of Science and Technology, ChinaSRNSFG, GeorgiaHGF, GermanyNetherlands Organization for Scientific Research (NWO)
Netherlands GovernmentMinistry of Science and Higher Education, PolandNCN, PolandNRCKI, Russia FederationJINRDST/NRF, South AfricaSERI, Geneva, SwitzerlandCantons of Bern and Geneva, SwitzerlandCompute Canada, CanadaHorizon 2020Marie Sklodowska-Curie ActionsEuropean Cooperation in Science and Technology (COST)EU-ESF, Greec
Measurements of W+W−+ ≥ 1 jet production cross-sections in pp collisions at s = 13 TeV with the ATLAS detector
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- Zemaityte G
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/06/2021
- Field of study
Fiducial and differential cross-section measurements of W+W− production in
association with at least one hadronic jet are presented. These measurements are sensitive
to the properties of electroweak-boson self-interactions and provide a test of perturbative
quantum chromodynamics and the electroweak theory. The analysis is performed using
proton-proton collision data collected at p
s = 13TeV with the ATLAS experiment, corresponding
to an integrated luminosity of 139 fb−1. Events are selected with exactly one oppositely
charged electron-muon pair and at least one hadronic jet with a transverse momentum
of pT > 30 GeV and a pseudorapidity of |�| < 4.5. After subtracting the background
contributions and correcting for detector effects, the jet-inclusive W+W−+ � 1 jet fiducial
cross-section and W+W−+ jets differential cross-sections with respect to several kinematic
variables are measured. These measurements include leptonic quantities, such as the lepton
transverse momenta and the transverse mass of the W+W− system, as well as jet-related
observables such as the leading jet transverse momentum and the jet multiplicity. Limits on
anomalous triple-gauge-boson couplings are obtained in a phase space where interference
between the Standard Model amplitude and the anomalous amplitude is enhanced
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
- Abud AA
- 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
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmad A
- Ahmadov F
- 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
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alvarez Estevez M
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Andrean SY
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Aparo MA
- Aperio Bella L
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arcangeletti C
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- Arduh FA
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- Asimakopoulou EM
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- Astigarraga MEP
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- Atlay NB
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- Bachacou H
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- Backman F
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- Baines JT
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- Baroncelli A
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- 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
- …