166 research outputs found
Explaining gender differences in non-fatal suicidal behaviour among adolescents: a population-based study
- Author
- A Sourander
- A Spirito
- AC Cameron
- AC Leon
- AE Waldrop
- AL Beautrais
- AL Hills
- AT Beck
- BL Hankin
- C Delmo
- D Shaffer
- DD Hallfors
- DM Fergusson
- DM Fergusson
- DM Fergusson
- E Evans
- EA Thompson
- EK Moscicki
- F Resch
- Franz Resch
- G Portzky
- G Schwarz
- J Kaufman
- JA Bridge
- Jeanette Roos
- JM Cyranowski
- Johann Haffner
- K Hawton
- K Hawton
- K Hawton
- K Hawton
- KS D'Eramo
- M Doepfner
- M Klett
- Martin Klett
- Michael Kaess
- MM Steele
- P Qin
- Peter Parzer
- R Bruffaerts
- R Brunner
- Rainer Steen
- RC Kessler
- Romuald Brunner
- S Bae
- S Schneider
- SS Canetto
- Statistisches Bundesamt
- TM Achenbach
- TM Achenbach
- U Wunderlich
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>While suicide is the second leading cause of death among young people in most industrial countries, non-fatal suicidal behaviour is also a very important public health concern among adolescents. The aim of this study was to investigate gender differences in prevalence and emotional and behavioural correlates of suicidal behaviour in a representative school-based sample of adolescents.</p> <p>Methods</p> <p>A cross-sectional design was used to assess suicidal behaviour and various areas of emotional and behavioural problems by using a self-report booklet including the Youth Self-Report. One hundred sixteen schools in a region of Southern Germany agreed to participate. A representative sample of 5,512 ninth-grade students was studied. Mean age was 14.8 years (SD 0.73); 49.8% were female.</p> <p>Results</p> <p>Serious suicidal thoughts were reported by 19.8% of the female students and 10.8% of the females had ever attempted suicide. In the male group, 9.3% had a history of suicidal thoughts and 4.9% had previously attempted suicide. Internalizing emotional and behavioural problems were shown to be higher in the female group (difference of the group means 4.41) while externalizing emotional and behavioural problems slightly predominated in male students (difference of the group means -0.65). However, the total rate of emotional and behavioural problems was significantly higher in the adolescent female group (difference of the group means 4.98). Using logistic regression models with suicidal thoughts or attempted suicide as dependent variables, the pseudo-R<sup>2</sup> of gender alone was only 2.7% or 2.3%, while it was 30% or 23.2% for emotional and behavioural problems measured by the YSR syndrome scales. By adding gender to the emotional and behavioural problems only an additional 0.3% of information could be explained.</p> <p>Conclusions</p> <p>The findings suggest that gender differences in non-fatal suicidal behaviour among adolescents can to a large extent be explained by the gender differences in emotional and behavioural problems during this age.</p
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
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
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- AbouZeid OS
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- Abramowicz H
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- Zaitsev AM
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- Zanzi D
- Zaripovas DR
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
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- Zgubic M
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- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
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- Zhu CG
- Zhu H
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- 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
- '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
QCD and strongly coupled gauge theories : challenges and perspectives
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- U Aglietti
- U Aglietti
- U Aglietti
- U Aglietti
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- U Gursoy
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- V Baru
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- VA Novikov
- VA Saleev
- VD Toneev
- VF Ezhov
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- W Altmannshofer
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- WT Giele
- WT Giele
- X Feng
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- X Feng
- X Feng
- X Zhao
- X Zhao
- X-D Ji
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- X-D Ji
- X-D Ji
- X-D Ji
- X-F Chen
- X-G He
- X-M Xu
- X-N Wang
- X-N Wang
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- XH Mo
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- Y Akaishi
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- Y He
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- Y Ikeda
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- Y Koma
- Y Li
- Y Liu
- Y Liu
- Y Nambu
- Y Nambu
- Y Sakaki
- Y Zhu
- Y-J Zhang
- Y-J Zhang
- Y-Q Ma
- Y-Q Ma
- Y-Q Ma
- Y-Q Ma
- Y-Q Ma
- Y-T Chien
- Y-Y Bu
- Y-Y Keum
- YA Karpenko
- YA Simonov
- YL Dokshitzer
- YL Dokshitzer
- YM Antipov
- YM Antipov
- YV Kovchegov
- YV Kovchegov
- YV Kovchegov
- YV Stadnick
- YY Keum
- Z Bern
- Z Bern
- Z Bern
- Z Chacko
- Z Fodor
- Z Fodor
- Z Fodor
- Z Fodor
- Z Fodor
- Z Fodor
- Z Fodor
- Z Fodor
- Z Fu
- Z Fu
- Z Komargodski
- Z Komargodski
- Z Ligeti
- Z Ligeti
- Z-B Kang
- Z-B Kang
- Z-B Kang
- Z-G He
- Z-G He
- Z-H Li
- Z-W Lin
- Z-W Lin
- Z. Fodor
- Publication venue
- Publication date
- 01/01/2014
- Field of study
We highlight the progress, current status, and open challenges of QCD-driven physics, in theory and in experiment. We discuss how the strong interaction is intimately connected to a broad sweep of physical problems, in settings ranging from astrophysics and cosmology to strongly coupled, complex systems in particle and condensed-matter physics, as well as to searches for physics beyond the Standard Model. We also discuss how success in describing the strong interaction impacts other fields, and, in turn, how such subjects can impact studies of the strong interaction. In the course of the work we offer a perspective on the many research streams which flow into and out of QCD, as well as a vision for future developments.Peer reviewe
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
- Armstrong A
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- Arnold H
- Arrubarrena Tame Zp
- Artamonov A
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- Artz S
- Asai S
- Asbah N
- Asimakopoulou Em
- Asquith L
- Assahsah J
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- Atlay Nb
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- Barranco Navarro L
- Barreiro Guimaraes Da Costa J
- Barreiro F
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- Bartoldus R
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- Basalaev A
- Bassalat A
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- Becot C
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- Bednyakov Va
- Bedognetti M
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- Begalli M
- Begel M
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- Belotskiy K
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- Benchekroun D
- Benekos N
- Benhammou Y
- Benjamin Dp
- Benoit M
- Bensinger Jr
- Bentvelsen S
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- Bessidskaia Bylund O
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- 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
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- Breaden Madden Wd
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- Britzger D
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- Bruckman De Renstrom Pa
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- Brunt Bh
- Bruschi M
- Bruscino N
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- Bryngemark L
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- 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
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- 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
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- 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
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- Catinaccio A
- Catmore Jr
- Cattai A
- Caudron J
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- Cavallaro E
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
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- Cerda Alberich L
- Cerny K
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- Cerri A
- Cerrito L
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- Charman Tp
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- Chen C
- Chen Ch
- Chen H
- Chen J
- Chen J
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- Chen Sj
- Chen X
- Chen Y
- Chen Y-
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- Cheng Hj
- Cheplakov A
- Cheremushkina E
- Cherkaoui El Moursli R
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- Cheung K
- Chevalerias Tja
- Chevalier L
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- Chiodini G
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- Chitan A
- Chiu I
- Chiu Yh
- Chizhov Mv
- Choi K
- Chomont Ar
- Chouridou S
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- 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
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- 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
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- Delporte C
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- Demarco Da
- Demers S
- Demichev M
- Demontigny G
- Denisov Sp
- Denysiuk D
- Derendarz D
- Derkaoui Je
- Derue F
- Dervan P
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- Dette K
- Deutsch C
- Devesa Mr
- Deviveiros Po
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- Di Bello Fa
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- Diehl Eb
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- Dimitrievska A
- Ding W
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- Djuvsland Ji
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- Dobre M
- Dodsworth D
- Doglioni C
- Dolejsi J
- Dolezal Z
- Donadelli M
- Dong B
- Donini J
- Dopke J
- Doria A
- Dova Mt
- Doyle At
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- Dreyer T
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- Dumitriu Ae
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- Duschinger D
- Dutta B
- Duvnjak D
- Dyckes Gi
- Dyndal M
- Dysch S
- Dziedzic Bs
- Ecker Km
- Edgar Rc
- Eggleston Mg
- Eifert T
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- Einsweiler K
- Ekelof T
- El Jarrari H
- El Kacimi M
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- Ellert M
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- Fakhrutdinov Rm
- Falciano S
- Falke Pj
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- Faltova J
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- Fanourakis G
- Fanti M
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- Farbin A
- Farilla A
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- Farooque T
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- Farrington Sm
- Farthouat P
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- Fawcett Wj
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- Fedin Ol
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- Ferrer A
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- Filthaut F
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- Fiolhais Mcn
- Fiorini L
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- Fisher Wc
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- Fleischmann P
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- Flierl Bm
- Flores Castillo Lr
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- Formica A
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- Foster Ag
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- Franchini M
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- Freundlich Em
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- Froidevaux D
- Frost Ja
- Fukunaga C
- Fullana Torregrosa E
- Fumagalli E
- Fusayasu T
- Fuster J
- Gabrielli A
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- Gach Gp
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- Gkialas I
- Gkougkousis El
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- Gostkin Mi
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- Rodriguez Perez A
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- Rodriguez Vera Am
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- Rusakovich Na
- Russell Hl
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- Sadykov R
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- Sano Y
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- Saraiva Jg
- Sasaki O
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- Scanlon T
- Schaarschmidt J
- Schacht P
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- Schegelsky Va
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- Schoening A
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- Schumm Ba
- Schune P
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- Schwemling P
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- Sciandra A
- Sciolla G
- Scodeggio M
- Scornajenghi M
- Scuri F
- Scutti F
- Scyboz Lm
- Sebastiani Cd
- Seema P
- Seidel Sc
- Seiden A
- Seidlitz Bd
- Seiss T
- Seixas Jm
- Sekhniaidze G
- Sekhon K
- Sekula Sj
- Semprini-Cesari N
- Sen S
- Senkin S
- Serfon C
- Serin L
- Serkin L
- Sessa M
- Severini H
- Sfiligoj T
- Sforza F
- Sfyrla A
- Shabalina E
- Shahinian Jd
- Shaikh Nw
- Shaked Renous D
- Shan Ly
- Shang R
- Shank Jt
- Shapiro M
- Sharma A
- Sharma As
- Shatalov Pb
- Shaw K
- Shaw Sm
- Shcherbakova A
- Shehade M
- Shen Y
- Sherafati N
- Sherman Ad
- Sherwood P
- Shi L
- Shimizu S
- Shimmin Co
- Shimogama Y
- Shimojima M
- Shipsey Ipj
- Shirabe S
- Shiyakova M
- Shlomi J
- Shmeleva A
- Shochet Mj
- Shojaii J
- Shope Dr
- Shrestha S
- Shrif Em
- Shulga E
- Sicho P
- Sickles Am
- Sidebo Pe
- Sideras Haddad E
- Sidiropoulou O
- Sidoti A
- Siegert F
- Sijacki D
- Silva Oliveira Mv
- Silva Mj
- Silverstein Sb
- Simion S
- Simioni E
- Simoniello R
- Simsek S
- Sinervo P
- Sinetckii V
- Sinev Nb
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- Siral I
- Sivoklokov Sy
- Sjolin J
- Skorda E
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- Sliwa K
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- Smart Bh
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- Sobie R
- Soffer A
- Sogaard A
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- Solans Sanchez Ca
- Soldatov Ey
- Soldevila U
- Solodkov Aa
- Soloshenko A
- Solovyanov Ov
- Solovyev V
- Sommer P
- Son H
- Song W
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- Sopczak A
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- Soualah R
- Soukharev Am
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- Strandberg S
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- Tapia Araya S
- Tapprogge S
- Tarek Abouelfadl Mohamed A
- Tarem S
- Tariq K
- Tarna G
- Tartarelli Gf
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- Tayalati Y
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- Teixeira-Dias P
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- Terron J
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- Thais Sj
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- Thiele F
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- Trischuk W
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- Troncon C
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- Turchikhin S
- Turgeman D
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- Vickey Boeriu Oe
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- Vilucchi E
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- Virdee Gs
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- Vivarelli I
- Vogel M
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- Vorobel V
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- Wingerter-Seez I
- Winkels E
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- Wittgen M
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- Wollrath J
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- Wong Vws
- Woods Nl
- Worm Sd
- Wosiek Bk
- Wozniak Kw
- Wraight K
- Wu Sl
- Wu X
- Wu Y
- Wyatt Tr
- Wynne Bm
- Xella S
- Xi Z
- Xia L
- Xiao X
- Xiotidis I
- Xu D
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- Xu W
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- Xu Z
- Yabsley B
- Yacoob S
- Yajima K
- Yallup Dp
- Yamaguchi D
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang Hj
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- Yang X
- Yang Y
- Yao W-
- Yap Yc
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yexley Mr
- Yigitbasi E
- Yorita K
- Yoshihara K
- Young C
- Young Cjs
- Yu J
- Yuan R
- 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 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
- 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
- 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 A
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Aliev M
- 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
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- 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 A
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Arabidze G
- Araque JP
- Araya ST
- Arcangeletti C
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armadans RC
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Artz S
- Asai S
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- 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
- Bailey VR
- Baines JT
- Bajic M
- Bakalis C
- Baker OK
- Bakker PJ
- Balaji S
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barnea R
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barsov S
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Basso MJ
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HC
- Beck HP
- Becker K
- Becker M
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beisiegel F
- Bell AS
- Bella G
- Bella LA
- 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
- Berger N
- Bergmann B
- Bergsten LJ
- Beringer J
- Berlendis S
- Berlingen JM
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Bertella C
- Bertram IA
- 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 N
- Biglietti M
- Billoud TR
- 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
- Boeriu OEV
- 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
- 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
- Broughton JH
- Bruncko D
- Bruni A
- Bruni G
- Bruni LS
- Bruno S
- 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
- 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
- Calandri A
- 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
- Cameron D
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Canesse A
- Cantero J
- Cao T
- Cao Y
- 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
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- Ye S
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- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yuan R
- 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 S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- 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 N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- 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
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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- Abhayasinghe DK
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- Zhemchugov A
- Zheng Z
- Zhong D
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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
Performance of the upgraded PreProcessor of the ATLAS Level-1 Calorimeter Trigger
- Author
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- Zhemchugov A
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- Zimmermann S
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- 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)
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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
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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
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
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- Yexley MR
- Yildiz HD
- Yin P
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- Zanzi D
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- Zeissner SV
- Zeitnitz C
- Zeng JC
- Zenger DT
- Zenin O
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- Zerradi S
- Zerwas D
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- Zhang DF
- Zhang G
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- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhou H
- Zhou N
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- 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
- 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.]
Search for long-lived, massive particles in events with a displaced vertex and a muon with large impact parameter in pp collisions at root s=13 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
- 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 A
- Al Khoury K
- Alberghi GL
- Albert J
- 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 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 A
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Arabidze G
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arcangeletti C
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling JH
- Armadans RC
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
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- Atlay NB
- Atmani H
- Augsten K
- Avolio G
- Avramidou R
- Ayoub MK
- Azoulay AM
- Azuelos G
- B M
- Bachacou H
- Bachas K
- Backes M
- Backman F
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Bailey VR
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- Tosciri C
- Toth J
- Tovey DR
- Traeet A
- Treado CJ
- Trefzger T
- Tresoldi F
- Tricoli A
- Trigger IM
- Trincaz-Duvoid S
- Trischuk DA
- Trischuk W
- Trocme B
- Trofymov A
- Troncon C
- Trovatelli M
- Trovato F
- Truong L
- Trzebinski M
- Trzupek A
- Tsai F
- Tseng JC-L
- Tsiareshka P
- Tsirigotis A
- Tsiskaridze V
- Tskhadadze EG
- Tsopoulou M
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
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- Tulbure TT
- Tuna AN
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- Turgeman D
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- Ueda I
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- Vaidya A
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- Valente M
- Valentinetti S
- Valero A
- Valery L
- Vallance RA
- Vallier A
- Van Daalen TR
- Van Gemmeren P
- Van Vulpen I
- Vanadia M
- Vandelli W
- Vandewall ER
- Vaniachine A
- Vannicola D
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- Vasile ME
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- Vazquez CJB
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- Veloso F
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- Verbytskyi A
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- Yexley MR
- Yigitbasi E
- Yildiz HD
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- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
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- Zhao P
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- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
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- Zhou MS
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- 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
- Zivkovic L
- Zobernig G
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- Zorbas TG
- Zou R
- Zu Theenhausen HM
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- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/08/2020
- Field of study
A search for long-lived particles decaying into hadrons and at least one muon is presented. The analysis selects events that pass a muon or missing-transverse-momentum trigger and contain a displaced muon track and a displaced vertex. The analyzed dataset of proton-proton collisions at
√
s
=
13 TeV
was collected with the ATLAS detector and corresponds to
136
fb
−
1. The search employs dedicated reconstruction techniques that significantly increase the sensitivity to long-lived particle decays that occur in the ATLAS inner detector. Background estimates for Standard Model processes and instrumental effects are extracted from data. The observed event yields are compatible with those expected from background processes. The results are presented as limits at 95% confidence level on model-independent cross sections for processes beyond the Standard Model, and interpreted as exclusion limits in scenarios with pair production of long-lived top squarks that decay via a small
R
-parity-violating coupling into a quark and a muon. Top squarks with masses up to 1.7 TeV are excluded for a lifetime of 0.1 ns, and masses below 1.3 TeV are excluded for lifetimes between 0.01 ns and 30 ns
- …