398 research outputs found
Characterization and Generation of Male Courtship Song in Cotesia congregata (Hymenoptera: Braconidae)
- Author
- A Goriely
- A Michel-Salzat
- A Michelsen
- A Michelsen
- AJ Lentz
- AJ Lentz-Ronning
- AL Joyce
- AL Joyce
- AL Joyce
- AM Wenner
- AT Danci
- C Ellington
- CA Villagra
- CS Henry
- DA Russell
- G Benelli
- G Gordh
- HC Bennet-Clark
- J LaSalle
- J Sivinski
- J Sueur
- Jochen Zeil
- Justin P. Bredlau
- JWS Pringle
- K Dolphin
- K von Frisch
- Karen M. Kester
- KM Kester
- KM Kester
- KM Kester
- KS Bostwick
- MH Dickinson
- MH Dickinson
- Michael L. Fine
- NP Myhrvold
- R Rupprecht
- SA Field
- SB Vinson
- SH Harwood
- T Weis-Fogh
- Timothy M. Cameron
- WF Towne
- Y Bae
- Yasha J. Mohajer
- Publication venue
- VCU Scholars Compass
- Publication date
- 01/01/2013
- Field of study
Background
Male parasitic wasps attract females with a courtship song produced by rapid wing fanning. Songs have been described for several parasitic wasp species; however, beyond association with wing fanning, the mechanism of sound generation has not been examined. We characterized the male courtship song of Cotesia congregata (Hymenoptera: Braconidae) and investigated the biomechanics of sound production. Methods and Principal Findings
Courtship songs were recorded using high-speed videography (2,000 fps) and audio recordings. The song consists of a long duration amplitude-modulated âbuzzâ followed by a series of pulsatile higher amplitude âboings,â each decaying into a terminal buzz followed by a short inter-boing pause while wings are stationary. Boings have higher amplitude and lower frequency than buzz components. The lower frequency of the boing sound is due to greater wing displacement. The power spectrum is a harmonic series dominated by wing repetition rate ~220 Hz, but the sound waveform indicates a higher frequency resonance ~5 kHz. Sound is not generated by the wings contacting each other, the substrate, or the abdomen. The abdomen is elevated during the first several wing cycles of the boing, but its position is unrelated to sound amplitude. Unlike most sounds generated by volume velocity, the boing is generated at the termination of the wing down stroke when displacement is maximal and wing velocity is zero. Calculation indicates a low Reynolds number of ~1000. Conclusions and Significance
Acoustic pressure is proportional to velocity for typical sound sources. Our finding that the boing sound was generated at maximal wing displacement coincident with cessation of wing motion indicates that it is caused by acceleration of the wing tips, consistent with a dipole source. The low Reynolds number requires a high wing flap rate for flight and predisposes wings of small insects for sound production
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at â s = 8 TeV with the ATLAS detector
- Author
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- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yorita K
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- Zhang X
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- Zhang Z
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- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
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- Zhou MS
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- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
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- Zhu Y
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- 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 fbâ1 of â 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
Sequencing of diverse mandarin, pummelo and orange genomes reveals complex history of admixture during citrus domestication
- Author
- A Cornille
- A Garcia-Lor
- Alexandre Lomsadze
- Amparo Herrero-Ortega
- Andrea Zuccolo
- Arnaud Couloux
- BE Pfeil
- Brian Desany
- CD Bustamante
- Chinnappa Kodira
- Chunxian Chen
- Cristian Del Fabbro
- Daniel RamĂłn
- Daniel Rokhsar
- Dominique Brunel
- E Nicolosi
- Federica Cattonaro
- FG Gmitter
- FG Gmitter
- Florent Murat
- Francis Quetier
- Francisco R Tadeo
- François Luro
- Frederick Gmitter
- G Albert Wu
- GA Moore
- GA Tuskan
- GF Liu
- Giuseppe Reforgiato
- HC Barrett
- J Bové
- J Salse
- Jane Grimwood
- Jarrod Chapman
- Javier Terol
- Jeremy Schmutz
- Jerome Salse
- Jerry Jenkins
- JL Trabut
- Juan V Muñoz-Sanz
- Juliana Freitas-AstĂșa
- Julie Poulain
- JuliĂĄn PĂ©rez-PĂ©rez
- JWS Cameron
- Kamel Jabbari
- Karin Fredrikson
- Karine Labadie
- Leandro H Estornell
- LG Samaan
- Luis Navarro
- M Talon
- MA Germana
- Manuel Ruiz
- Manuel Talon
- Marco Aurélio Takita
- Marcos Antonio Machado
- Mark Borodovsky
- MB Hufford
- MG Bausher
- Michele Morgante
- Mikeal Roose
- Mohammed Mohiuddin
- NA Barkley
- NA Johnson
- Olivier Jaillon
- P Aleza
- P Ollitrault
- Pablo Aleza
- Patrick Ollitrault
- Patrick Wincker
- Paul Burns
- PL Morrell
- Q Xu
- RW Scora
- S Myles
- Sara Pinosio
- Simon Prochnik
- Simone Scalabrin
- T Tanaka
- Tim Harkins
- TR Gottwald
- Uffe Hellsten
- Victoria Ibanez
- VM Novelli
- William G Farmerie
- X Huang
- Xavier Perrier
- Y Froelicher
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
Cultivated citrus are selections from, or hybrids of, wild progenitor species whose identities and contributions to citrus domestication remain controversial. Here we sequence and compare citrus genomes-a high-quality reference haploid clementine genome and mandarin, pummelo, sweet-orange and sour-orange genomes-and show that cultivated types derive from two progenitor species. Although cultivated pummelos represent selections from one progenitor species, Citrus maxima, cultivated mandarins are introgressions of C. maxima into the ancestral mandarin species Citrus reticulata. The most widely cultivated citrus, sweet orange, is the offspring of previously admixed individuals, but sour orange is an F1 hybrid of pure C. maxima and C. reticulata parents, thus implying that wild mandarins were part of the early breeding germplasm. A Chinese wild 'mandarin' diverges substantially from C. reticulata, thus suggesting the possibility of other unrecognized wild citrus species. Understanding citrus phylogeny through genome analysis clarifies taxonomic relationships and facilitates sequence-directed genetic improvement. (Résumé d'auteur
Measurement of VH, H â b b ÂŻ production as a function of the vector-boson transverse momentum in 13 TeV pp collisions with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- 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
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Al Khoury K
- Alberghi GL
- Alberich LC
- Albert J
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alfonsi A
- 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
- Alstaty MI
- 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
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Arabidze G
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armadans RC
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Asimakopoulou EM
- Asquith L
- 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
- Baas AE
- Baca MJ
- 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
- Barajas CAC
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- 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
- Barranco Navarro L
- Barreiro F
- Bartoldus R
- Bartolini G
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- Bassalat A
- Bates RL
- Batista SJ
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beau T
- Beauchemin PH
- Bechtle P
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- Beisiegel F
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- Bella G
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- Bellagamba L
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- Belyaev NL
- Benary O
- 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
- Bernard NR
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertram IA
- Besjes GJ
- Besson N
- Bethani A
- Bethke S
- Betti A
- Bevan AJ
- Beyer J
- 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
- Bitadze A
- Bittrich C
- Bjergaard DM
- Black JE
- Black KM
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boeriu OEV
- 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
- Borecka-Bielska HM
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Bortolotto V
- Boscherini D
- Bosman M
- Bostanabad MG
- Bouaouda K
- Boudreau J
- Bouhova-Thacker EV
- 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
- Bratzler U
- Brau B
- Brau JE
- Brendlinger K
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Brickwedde B
- Briglin DL
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- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks T
- Brooks WK
- Brost E
- Broughton JH
- 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
- Buehrer F
- Buescher V
- Bugge MK
- Bulekov O
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burka K
- Burr JTP
- 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 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
- 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 FC
- 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
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Caudron J
- Cavaliere V
- Cavallaro E
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
- Ceradini F
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chafaq A
- Chakraborty D
- Chan SK
- Chan WS
- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Chau CC
- Che S
- Chegwidden A
- 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-H
- Cheng HC
- Cheng HJ
- Cheplakov A
- Cheremushkina E
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- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2019
- Field of study
Cross-sections of associated production of a Higgs boson decaying into bottom-quark pairs and an electroweak gauge boson, W or Z, decaying into leptons are measured as a function of the gauge boson transverse momentum. The measurements are performed in kinematic fiducial volumes defined in the `simplified template cross-section' framework. The results are obtained using 79.8 fb-1 of proton-proton collisions recorded by the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13 TeV. All measurements are found to be in agreement with the Standard Model predictions, and limits are set on the parameters of an effective Lagrangian sensitive to modifications of the Higgs boson couplings to the electroweak gauge bosons
Measurement of the tÂŻtZ and tÂŻtW cross sections in proton-proton collisions at âs=13âTeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
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- Ălvarez Piqueras D
- Ă kesson TPA
- Ć filigoj T
- ĆœeniĆĄ T
- ĆœivkoviÄ L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
A measurement of the associated production of a top-quark pair (tÂŻt) with a vector boson (W, Z) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1ââfbâ1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The tÂŻtZ and tÂŻtW production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are ÏtÂŻtZ=0.95±0.08stat±0.10systâpb and ÏtÂŻtW=0.87±0.13stat±0.14systâpb in agreement with the Standard Model predictions. The measurement of the tÂŻtZ cross section is used to set constraints on effective field theory operators which modify the tÂŻtZ vertex
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
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
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- Yigitbasi E
- Yildiz HD
- Yorita K
- Yoshihara K
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- Yuen SPY
- Zabinski B
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- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- 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 G
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- Zhang J
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- 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 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
âfb
â
1
of
â
s
=
13â
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
ÂŻ
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 âsNN = 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
- Arnaez O
- Arnold H
- Arrubarrena Tame Zp
- Artamonov A
- Artoni G
- 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
- Bailey Vr
- Baines Jt
- Bajic M
- Bakalis C
- Baker Ok
- Bakker Pj
- Bakshi Gupta D
- 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-
- Barkeloo J
- Barklow T
- Barnea R
- Barnes Sl
- Barnett Bm
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- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr Aj
- Barranco Navarro L
- Barreiro Guimaraes Da Costa J
- 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
- 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
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- Elsing M
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- 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
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- Gach Gp
- Gadatsch S
- Gadow P
- Gagliardi G
- Gagnon Lg
- Galea C
- Galhardo B
- Gallardo Ge
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- Gallop Bj
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- Garcia Pascual Ja
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- Gardner Rw
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- Gargiulo S
- Garonne V
- Gaudiello A
- Gaudio G
- Gavrilenko Il
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- Gazis En
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- Gee Cm
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- Geisler Mp
- Gemme C
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- Gentile S
- George S
- Geralis T
- Gerlach Lo
- Gessinger-Befurt P
- Gessner G
- Ghasemi Bostanabad M
- Ghasemi S
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- Giacobbe B
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- Giangiacomi N
- Giannetti P
- Giannini A
- Giannini G
- Gibson Sm
- Gignac M
- Gillberg D
- Gilles G
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- 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
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- Goldfarb S
- Golling T
- Golubkov D
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- Gonzalez De La Hoz S
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- Gonzalvo Rodriguez Gr
- Goossens L
- Gorbounov Pa
- Gordon Ha
- Gorini B
- Gorini E
- Gorisek A
- Goshaw At
- Gostkin Mi
- Gottardo Ca
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- Guyot C
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- Henriques Correia Am
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- Herde H
- Herget V
- Hernandez Jimenez Y
- Herr H
- Herrmann Mg
- Herrmann T
- Herten G
- Hertenberger R
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- Herwig Tc
- Hesketh Gg
- Hessey Np
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- Hoad X
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- Kar D
- Karava K
- Kareem Mj
- Karpov Sn
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- Kartvelishvili V
- Karyukhin An
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- Kass Rd
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- Kato C
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- Khader M
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- Kharlamova T
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- Kitali V
- Kivernyk O
- Klapdor-Kleingrothaus T
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- Knue A
- Kobayashi D
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- Kodys P
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- Komarek T
- Kondo T
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- Korotkova N
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- Kotsokechagia A
- Kotwal A
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- Kourkoumelis C
- Kourlitis E
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- Lampl W
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- Laurier A
- Lavorgna M
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- Lazzaroni M
- Le Guirriec E
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- Leblanc M
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- Ledroit-Guillon F
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- Liberti B
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- Yexley Mr
- Yigitbasi E
- Yorita K
- Yoshihara K
- Young C
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- Yu J
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- 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
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- Zhang G
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- 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
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- 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 ttÂŻttÂŻ production cross section in pp collisions at âs=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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- Affolder AA
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- Agarwala J
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- Alberghi GL
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- Alconada Verzini MJ
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- Aleksa M
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- Anastopoulos C
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- Andrean SY
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- Andrei V
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
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- Antrim DJA
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- Aparisi Pozo JA
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- Araujo Ferraz V
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- Assahsah J
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- Austrup VA
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- Bartoldus R
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- Bogavac D
- Bogdanchikov AG
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- Booth CD
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- Borecka-Bielska HM
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- Briglin DL
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- Brock I
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- Cao Y
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- Carbone A
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- Cardillo F
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- Carlino G
- Carlson BT
- Carlson EM
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- Carney RMD
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- Carter JWS
- Carter TM
- Casadei D
- Casado MP
- Casha AF
- Castiglia EG
- Castillo Garcia L
- Castillo Gimenez V
- Castillo FL
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Cavaliere V
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- Cavasinni V
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- Celli F
- Cerny K
- Cerqueira AS
- Cerri A
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- Chadi Z
- Chakraborty D
- Chala M
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- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chatterjee M
- Chau CC
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chen A
- Chen B
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- Chen CH
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- Cheng CL
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- Cheplakov A
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- Cherkaoui El Moursli R
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
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- Chiodini G
- Chisholm AS
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- Chiu I
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- Christopher LD
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- Chwastowski JJ
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- Ciesla KM
- Cindro V
- CioarÄ IA
- Ciocio A
- Cirotto F
- Citron ZH
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- Clawson SE
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- Conroy EI
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- Cuhadar Donszelmann T
- Cui H
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- Da Cunha Sargedas De Sousa MJ
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- De Beurs M
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- de Jong P
- De la Torre H
- De Maria A
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- Denisov SP
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- Deviveiros PO
- Di Bello FA
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- Di Donato C
- Di Girolamo A
- Di Gregorio G
- Di Luca A
- Di Micco B
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- Didenko M
- Diehl EB
- Dietrich J
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- Ding W
- Dingfelder J
- Dinu I-M
- Dittmeier SJ
- Dittus F
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- Djuvsland JI
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- Zemaityte G
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
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- Zwalinski L
- Ă kesson TPA
- Ăncel ĂO
- ĆœeniĆĄ T
- ĆœivkoviÄ 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 fbâ1 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+17â15 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+7â6 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
- 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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- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
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- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
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- Aguilar-Saavedra JA
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- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
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- Akimov A
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- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
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- Ali B
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- Alison J
- Alkire SP
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- Allen BW
- Allport PP
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- Zhemchugov A
- Zheng Z
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- Zou R
- Zu Theenhausen HM
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- 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 protonâproton 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 â=13TeV
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- Zhemchugov A
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- Zimmermann S
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- Ă kesson TPA
- Ăncel ĂO
- ĆœeniĆĄ T
- ĆœivkoviÄ 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 fbâ1 of sâ=13TeV protonâproton 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+0.38â0.36 , 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
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