24 research outputs found
Measurements of differential cross-sections in top-quark pair events with a high transverse momentum top quark and limits on beyond the Standard Model contributions to top-quark pair production with the ATLAS detector at √s = 13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
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- Aielli G
- Aizenberg I
- Akbiyik M
- Akesson TPA
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
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- Alfonsi A
- Alfonsi F
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- Ali B
- Ali S
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- Alimonti G
- Allaire C
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- Allport PP
- Aloisio A
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- Alviggi MG
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- Amelung C
- Amidei D
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- Amos KR
- Amrouche CS
- Ananiev V
- Anastopoulos C
- Andana RYG
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- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
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- Anthony MT
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- Aoki M
- Aparo MA
- Appelt C
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- Arcangeletti C
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- Arena E
- Arguin JF
- Argyropoulos S
- Arling JH
- Armbruster AJ
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Asimakopoulou EM
- Assahsah J
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- Zhemchugov A
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Cross-section measurements of top-quark pair production where the hadronically decaying top quark has transverse momentum greater than 355 GeV and the other top quark decays into ℓνb are presented using 139 fb−1 of data collected by the ATLAS experiment during proton-proton collisions at the LHC. The fiducial cross-section at s = 13 TeV is measured to be σ = 1.267 ± 0.005 ± 0.053 pb, where the uncertainties reflect the limited number of data events and the systematic uncertainties, giving a total uncertainty of 4.2%. The cross-section is measured differentially as a function of variables characterising the tt¯ system and additional radiation in the events. The results are compared with various Monte Carlo generators, including comparisons where the generators are reweighted to match a parton-level calculation at next-to-next-to-leading order. The reweighting improves the agreement between data and theory. The measured distribution of the top-quark transverse momentum is used to search for new physics in the context of the effective field theory framework. No significant deviation from the Standard Model is observed and limits are set on the Wilson coefficients of the dimension-six operators OtG and Otq(8), where the limits on the latter are the most stringent to date. [Figure not available: see fulltext.]
Observation of electroweak production of two jets in association with an isolated photon and missing transverse momentum, and search for a Higgs boson decaying into invisible particles at 13 TeV with the ATLAS detector
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- Zagazeta LFG
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- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeitnitz C
- Zeißner SV
- Zeng JC
- Zenger DT
- Zenin O
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- Zerradi S
- Zerwas D
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- Zhang G
- Zhang J
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- Zhang L
- Zhang M
- Zhang R
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- Zhang X
- Zhang X
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- EUROPEAN PHYSICAL JOURNAL C
- Publication date
- 01/01/2022
- Field of study
This paper presents the measurement of the electroweak production of two jets
in association with a Zγ pair with the Z boson decaying into two
neutrinos. It also presents the search for invisible or partially invisible
decays of a Higgs boson with a mass of 125 GeV produced through vector-boson
fusion with a photon in the final state. These results use data from LHC
proton-proton collisions at s = 13 TeV collected with the ATLAS
detector corresponding to an integrated luminosity of 139 fb−1. The event
signature, shared by all benchmark processes considered for measurements and
searches, is characterized by a significant amount of unbalanced transverse
momentum and a photon in the final state, in addition to a pair of forward
jets. For electroweak production of Zγ in association with two jets, the
background-only hypothesis is rejected with an observed (expected) significance
of 5.2 (5.1) standard deviations. The measured fiducial cross-section for this
process is 1.31±0.29 fb. Observed (expected) upper limit of 0.37 (0.34) at
95% confidence level is set on the branching ratio of a 125 GeV Higgs boson to
invisible particles, assuming the Standard Model production cross-section. The
signature is also interpreted in the context of decays of a Higgs boson to a
photon and a dark photon. An observed (expected) 95% CL upper limit on the
branching ratio for this decay is set at 0.018 (0.017), assuming the 125 GeV
Standard Model Higgs boson production cross-section
The role of immunity and neuroinflammation in genetic predisposition and pathogenesis of Alzheimer's disease
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- Wildsmith KR Holley M, Savage JC, et al.
- Wyss-Coray T Loike JD, Brionne TC, et al.
- Xiao M Hu G
- Xiao Q Gil SC, Yan P, et al.
- Xu Z Yoshida T, Wu L, et al.
- Yamanaka M Ishikawa T, Griep A, et al.
- Yoshiyama Y Higuchi M, Zhang B, et al.
- Yuyama K Sun H, Mitsutake S, et al.
- Zhang J Ke KF, Liu Z, et al.
- Zhao L Lin S, Bales KR, et al.
- Zota V Nemirovsky A, Baron R, et al.
- Zuccolo J Bau J, Childs SJ, et al.
- Publication venue
- 'American Institute of Mathematical Sciences (AIMS)'
- Publication date
- 01/01/2015
- Field of study
AtlFast3: The Next Generation of Fast Simulation in ATLAS
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahnen JV
- Ai X
- Aielli G
- Aizenberg I
- Akatsuka S
- Akbiyik M
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amos KR
- Amrouche CS
- Ananiev V
- Anastopoulos C
- Andana RYG
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparo MA
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Austrup VA
- Avner G
- Avolio G
- Ayoub MK
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Bachiu A
- Backman F
- Badea A
- Bagnaia P
- Bahilo JJL
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
- Bakos E
- Balaji S
- Balasubramanian R
- Baldin EM
- Balek P
- Ballabene E
- Balli F
- Baltes LM
- Balunas WK
- Balz J
- Banas E
- Bandieramonte M
- Bandyopadhyay A
- Bansal S
- Barak L
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barends KN
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barnett BM
- Barnett RM
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barron U
- Barrue RFC
- Barsov S
- Bartels F
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Baselga M
- Bashta I
- Bassalat A
- Basso MJ
- Basson CR
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Bauce M
- Bauer F
- Bauer P
- Bawa HS
- Bayirli A
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HP
- Becker K
- Becot C
- Beddall AJ
- Bednyakov VA
- Bee CP
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beirer JF
- Beisiegel F
- Belfkir M
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bello FAD
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev NL
- Benchekroun D
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Bergmann B
- Bergsten LJ
- Beringer J
- Berlendis S
- Berlingen JM
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Berthold A
- Bertram IA
- Bethke S
- Betti A
- Bevan AJ
- Bhatta S
- Bhattacharya DS
- Bhattarai P
- Bhopatkar VS
- Bi R
- Bianchi RM
- Biebel O
- Bielski R
- Biesuz NV
- Biglietti M
- Billoud TRV
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Biondini A
- Birch-sykes CJ
- Bird GA
- Birman M
- Bisanz T
- Biswal JP
- Biswas D
- Bitadze A
- Bittrich C
- Bjørke K
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blumenthal J
- Bobbink GJ
- Bobrovnikov VS
- Boehler M
- Boeriu OEV
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bolanos GR
- Bold T
- Bomben M
- Bona M
- Boonekamp M
- Booth CD
- Borbély AG
- Borecka-Bielska HM
- Borgna LS
- Borissov G
- Bortoletto D
- Bosca SR
- Boscherini D
- Bosman M
- Bostanabad MG
- Bouaouda K
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bouquet R
- Bourdarios CA
- 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
- Brener R
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks WK
- Brost E
- Bruncko D
- Bruni A
- Bruni G
- Bruschi M
- Bruscino N
- Bryngemark L
- Brüers B
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Bugge MK
- Bulekov O
- Bullard BA
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Busch EL
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Buzykaev AR
- Bylund OB
- Büscher V
- Cabras G
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camarda S
- Camarri P
- Camelia EA
- Camerlingo MT
- Cameron D
- Camincher C
- Campanelli M
- Camplani A
- Canale V
- Canesse A
- Cantero J
- Cao Y
- Capocasa F
- Capriles FGD
- Capua M
- Carbone A
- Cardarelli R
- Cardenas JCJ
- Cardillo F
- Carducci G
- Carli T
- Carlino G
- Carlson BT
- Carlson EM
- Carlson TI
- Carminati L
- Carnesale M
- Carney RMD
- Caron S
- Carquin E
- Carratta G
- Carrá S
- Carter JWS
- Carter TM
- Casadei D
- Casado MP
- Casha AF
- Castiglia EG
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Cavaliere V
- Cavalli N
- Cavasinni V
- Celebi E
- Celli F
- Centonze MS
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chadi Z
- Chakraborty D
- Chala M
- Chan J
- Chan WS
- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chatterjee M
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chen A
- Chen B
- Chen B
- Chen C
- Chen CH
- Chen H
- Chen H
- Chen J
- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen X
- Chen Y
- Chen Y-H
- Cheng CL
- Cheng HC
- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu YH
- Chizhov MV
- Choi K
- Chomont AR
- Chou Y
- Chow YS
- Chowdhury T
- Christopher LD
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Ciaccio AD
- Ciaccio LD
- Cieri D
- Ciesla KM
- Cindro V
- Cioară IA
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubotaru DA
- Ciungu BM
- Clark A
- Clark PJ
- Clawson SE
- Clement C
- Clissa L
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Codina EP
- Coelli S
- Cohen H
- Coimbra AEC
- Cole B
- Collot J
- Columbie JMC
- Connell SH
- Connelly IA
- Conroy EI
- Conventi F
- Cooke HG
- Cooper-Sarkar AM
- Cormier F
- Cornell SD
- Corpe LD
- Corradi M
- Correia AMH
- Corrigan EE
- Corriveau F
- Costa MJ
- Costanza F
- Costanzo D
- Cote BM
- Coutinho YA
- Cowan G
- Cowley JW
- Cranmer K
- Crescioli F
- Cristinziani M
- Cristoforetti M
- Croft V
- Crosetti G
- Crépé-Renaudin S
- Cueto A
- Cui H
- Cukierman AR
- Cunningham WR
- Curcio F
- Czodrowski P
- Czurylo MM
- Da Costa AMMJ
- da Costa JBG
- Da Cruz E Silva CB
- Da Cunha Sargedas De Sousa MJ
- Da Fonseca Pinto JV
- Da Via C
- Daalen TRV
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dallapiccola C
- Dam M
- Damazio DO
- Damp J
- Dandoy JR
- Daneri MF
- Danninger M
- Dao V
- Darbo G
- Darmora S
- Dattagupta A
- David C
- Davidek T
- Davis DR
- Davis-Purcell B
- Dawson I
- de Andrade Filho LM
- De Araujo MV
- De Asmundis R
- De Beurs M
- De Carvalho ALM
- De Castro S
- De Groot N
- de Jong P
- de la Hoz SG
- De la Torre H
- De Lima RT
- De Maria A
- De Pedis D
- de Renstrom PAB
- De Sa RCL
- De Salvo A
- De Sanctis U
- De Santis M
- De Santo A
- De Souza EEP
- De Vivie De Regie JB
- De K
- Dedovich DV
- Degens J
- Deiana AM
- Deliot F
- Delitzsch CM
- Dell’Acqua A
- Dell’Asta L
- Delmastro M
- Delsart PA
- Demers S
- Demichev M
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Dette K
- Deutsch C
- Deviveiros PO
- Diaconu C
- Dias FA
- Diaz LP
- Diaz MA
- Diaz YD
- Dickinson J
- Didenko M
- Diehl EB
- Dietrich J
- Dimitrievska A
- Ding W
- Dingfelder J
- Dinu I-M
- Dittmeier SJ
- Dittus F
- Djama F
- Djobava T
- Djuvsland JI
- Dodsworth D
- Doglioni C
- Dolejsi J
- Dolezal Z
- Domenico AD
- Dominguez LP
- Don MMR
- Donadelli M
- Donaldson CP
- Donato CD
- Donell DMM
- Dong B
- Donini J
- Donszelmann TC
- Dopke J
- Doria A
- Dova MT
- Doyle AT
- Drechsler E
- Dreyer E
- Dreyer T
- Drobac AS
- Du D
- Dubinin F
- Dubovsky M
- Dubreuil A
- Duchovni E
- Duckeck G
- Ducu OA
- Duda D
- Dudarev A
- Duflot L
- Dumitriu AE
- Dunford M
- Dungs S
- Dunne K
- Duperrin A
- Durglishvili A
- Dutta B
- Dyckes GI
- Dyndal M
- Dysch S
- Dziedzic BS
- Dührssen M
- Dülsen C
- Düren M
- D’amen G
- D’Amico V
- D’Auria S
- D’Eramo L
- D’onofrio A
- D’Onofrio M
- D’uffizi M
- Eckerova B
- Eggleston MG
- Ehrke LF
- Eifert T
- Eigen G
- Einsweiler K
- Ekelof T
- Ellajosyula V
- Ellert M
- Ellinghaus F
- Elliot AA
- Ellis N
- Elmsheuser J
- Elsing M
- Emeliyanov D
- Emerman A
- Enari Y
- Erdmann J
- Ereditato A
- Erland PA
- Errenst M
- Escalier M
- Escobar C
- Estabragh MR
- Estevez MA
- Etzion E
- Evans G
- Evans H
- Evans MO
- Ezhilov A
- Fabbri F
- Fabbri L
- Facini G
- Fadeyev V
- Fakhrutdinov RM
- Falciano S
- Falke PJ
- Falke S
- Faltova J
- Fan Y
- Fang Y
- Fanourakis G
- Fanti M
- Faraj M
- Farbin A
- Farilla A
- Farina EM
- Farooque T
- Farrington SM
- Farthouat P
- Fassi F
- Fassouliotis D
- Fawcett WJ
- Fayard L
- Fedin OL
- Feickert M
- Feligioni L
- Fell A
- Feng C
- Feng M
- Fenton MJ
- Fenyuk AB
- Ferguson SW
- Fernandez SG
- Ferrando J
- Ferrari A
- Ferrari P
- Ferrari R
- Ferraz VA
- Ferrer JAV
- Ferrere D
- Ferretti C
- Fiacco D
- Fiedler F
- Filipčič A
- Filthaut F
- Fiolhais MCN
- Fiorini L
- Fischer F
- Fisher WC
- Fitschen T
- Fleck I
- Fleischmann P
- Flick T
- Flierl BM
- Flores L
- Flores M
- Follega FM
- Fomin N
- Foo JH
- Forland BC
- Formica A
- Forti AC
- Fortin E
- Foti MG
- Fountas L
- Fournier D
- Fox H
- Francavilla P
- Francescato S
- Franchini M
- Franchino S
- Francis D
- Franco L
- Franconi L
- Franklin M
- Frattari G
- Freegard AC
- Freeman PM
- Freund WS
- Freundlich EM
- Froidevaux D
- Frost JA
- Fu Y
- Fujimoto M
- Furelos DV
- Fuster J
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- Gabrielli A
- Gabrielli A
- Gadow P
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- Gajardo CMR
- Gallardo GE
- Gallas EJ
- Gallop BJ
- Galvan IS
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- Ganguly S
- Gao J
- Gao Y
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- Garcia LC
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- Gargiulo S
- Garner CA
- Garonne V
- Garzon GOY
- Gasiorowski SJ
- Gaspar P
- Gaudio G
- Gauzzi P
- Gavrilenko IL
- Gavrilyuk A
- Gay C
- Gaycken G
- Gazis EN
- Geanta AA
- Gee CM
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- Geisen J
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- Genest MH
- Gentile S
- George S
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- Gessinger-Befurt P
- Ghazali YE
- Ghosh A
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- Giacobbe B
- Giagu S
- Giangiacomi N
- Giannelli MF
- Giannetti P
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- Gilbert BJ
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- Gilles G
- Gillwald NEK
- Gimenez VC
- Gingrich DM
- Ginn CM
- Giordani MP
- Giovinazzo S
- Giraud PF
- Girolamo AD
- Giugliarelli G
- Giugni D
- Giuli F
- Gkialas I
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- Glasman C
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- Goni RG
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- Gorbounov PA
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- Gorišek A
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- Gostkin MI
- Gottardo CA
- Gouighri M
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- Grud C
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- Grundy JC
- Guan L
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- Gubbels C
- Gudnadottir OS
- Guenther J
- Guescini F
- Guest D
- Gugel R
- Guida A
- Guillemin T
- Guindon S
- Guo J
- Guo L
- Guo Y
- Gupta DB
- Gupta R
- Gurbuz S
- Gustavino G
- Guth M
- Gutierrez P
- Gutschow C
- Guyot C
- Gwenlan C
- Gwilliam CB
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- Haas A
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- Hartman NM
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- Hawkings RJ
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- Heggelund AL
- Hehir ND
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- Herr H
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- Herrmann T
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- Hinchliffe I
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- Hiti B
- Hladik O
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- Hommels LBAH
- Honan BP
- Hong J
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- Hooberman BH
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- Horii Y
- Horyn LA
- Hou S
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- Hrabovsky M
- Hrynevich A
- Hryn’ova T
- Hsu PJ
- Hsu S-C
- Hu Q
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- Hu YF
- Huang DP
- Huang X
- Huang Y
- Huang Y
- Hubacek Z
- Hubaut F
- Huebner M
- Huegging F
- Huffman TB
- Huhtinen M
- Huiberts SK
- Hulsken R
- Huseynov N
- Huston J
- Huth J
- Hyneman R
- Hyrych S
- Hönle A
- Iacobucci G
- Iakovidis G
- Ibanez AP
- Ibragimov I
- Iconomidou-Fayard L
- Iengo P
- Iglesias JAS
- Iguchi R
- Iizawa T
- Ikegami Y
- Ilg A
- Ilic N
- Imam H
- Introzzi G
- Iodice M
- Ippolito V
- Ishino M
- Islam W
- Issever C
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- Iuppa R
- Ivina A
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- Izzo V
- Jacka P
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- Jamieson J
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- Jarrari HE
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- Jeanneau F
- Jeanty L
- Jejelava J
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- Jiggins S
- Jiménez YH
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- Jinaru A
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Computing and Software for Big Science
- Publication date
- 01/01/2022
- Field of study
Funder: Open access funding provided by CERN (European Organization for Nuclear Research.The ATLAS experiment at the Large Hadron Collider has a broad physics
programme ranging from precision measurements to direct searches for new
particles and new interactions, requiring ever larger and ever more accurate
datasets of simulated Monte Carlo events. Detector simulation with GEANT4 is
accurate but requires significant CPU resources. Over the past decade, ATLAS
has developed and utilized tools that replace the most CPU-intensive component
of the simulation -- the calorimeter shower simulation -- with faster
simulation methods. Here, AtlFast3, the next generation of high-accuracy fast
simulation in ATLAS is introduced. AtlFast3 combines parameterized approaches
with machine-learning techniques and is deployed to meet current and future
computing challenges and simulation needs of the ATLAS experiment. With highly
accurate performance and a new ability to model substructure within jets,
AtlFast3 is designed to be used to simulate large numbers of events for a wide
range of physics processes
Measurement of the energy asymmetry in t(t)over-barj production at 13 TeV with the ATLAS experiment and interpretation in the SMEFT framework
- Author
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- Abbott B
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- Abhayasinghe DK
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- Filthaut F
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- Zenger DT
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- EUROPEAN PHYSICAL JOURNAL C
- Publication date
- 01/01/2022
- Field of study
A measurement of the energy asymmetry in jet-associated top-quark pair
production is presented using 139 fb−1 of data collected by the
ATLAS detector at the Large Hadron Collider during pp collisions at
s=13 TeV. The observable measures the different probability of top and
antitop quarks to have the higher energy as a function of the jet scattering
angle with respect to the beam axis. The energy asymmetry is measured in the
semileptonic ttˉ decay channel, and the hadronically decaying top quark
must have transverse momentum above 350 GeV. The results are corrected for
detector effects to particle level in three bins of the scattering angle of the
associated jet. The measurement agrees with the SM prediction at
next-to-leading-order accuracy in quantum chromodynamics in all three bins. In
the bin with the largest expected asymmetry, where the jet is emitted
perpendicular to the beam, the energy asymmetry is measured to be
−0.043±0.020, in agreement with the SM prediction of −0.037±0.003.
Interpreting this result in the framework of the Standard Model effective field
theory (SMEFT), it is shown that the energy asymmetry is sensitive to the
top-quark chirality in four-quark operators and is therefore a valuable new
observable in global SMEFT fits
Measurement of the energy response of the ATLAS calorimeter to charged pions from W±→τ±(→π±ντ)ντ events in Run 2 data
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahnen JV
- Ai X
- Aielli G
- Aizenberg I
- Akatsuka S
- Akbiyik M
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Andana RYG
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparo MA
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
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- Arnold H
- Artoni G
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- Asbah NA
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Austrup VA
- Avner G
- Avolio G
- Ayoub MK
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Bachiu A
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- Badea A
- Bagnaia P
- Bahilo JJL
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- Bailey AJ
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- Baines JT
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- Baker OK
- Bakker PJ
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- Baldin EM
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- Baroncelli A
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- Barreiro F
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- Barrue RFC
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- Busch EL
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- Butterworth JM
- Buttinger W
- Buzykaev AR
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- Cindro V
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- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
The energy response of the ATLAS calorimeter is measured for single charged pions with transverse momentum in the range 10<pT<300 GeV. The measurement is performed using 139 fb−1 of LHC proton–proton collision data at s√=13 TeV taken in Run 2 by the ATLAS detector. Charged pions originating from τ-lepton decays are used to provide a sample of high-pT isolated particles, where the composition is known, to test an energy regime that has not previously been probed by in situ single-particle measurements. The calorimeter response to single-pions is observed to be overestimated by ∼2% across a large part of the pT spectrum in the central region and underestimated by ∼4% in the endcaps in the ATLAS simulation. The uncertainties in the measurements are ≲1% for 15<pT<185 GeV in the central region. To investigate the source of the discrepancies, the width of the distribution of the ratio of calorimeter energy to track momentum, the energies per layer and response in the hadronic calorimeter are also compared between data and simulation
Search for resonant pair production of Higgs bosons in the b(b)over-barb(b)over-bar final state using pp collisions at root s=13 TeV with the ATLAS detector
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- Publication venue
- Publication date
- 01/01/2022
- Field of study
A search for resonant Higgs boson pair production in the b (b) over barb (b) over bar final state is presented. The analysis uses 126 fb(-1)- 139 fb(-1) of pp collision data at root s = 13 TeV collected with the ATLAS detector at the Large Hadron Collider. The analysis is divided into two channels, targeting Higgs boson decays which are reconstructed as pairs of small-radius jets or as individual large-radius jets. Spin-0 and spin2 benchmark signal models are considered, both of which correspond to resonant HH production via gluon-gluon fusion. The data are consistent with Standard Model predictions. Upper limits are set on the production cross section times branching ratio to Higgs boson pairs of a new resonance in the mass range from 251 GeV to 5 TeV
Determination of the parton distribution functions of the proton using diverse ATLAS data from pp collisions at root s=7, 8 and 13 TeV
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
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- Publication venue
- Publication date
- 01/01/2022
- Field of study
This paper presents an analysis at next-to-next-to-leading order in the theory of quantum chromodynamics for the determination of a new set of proton parton distribution functions using diverse measurements in pp collisions at root s = 7, 8 and 13 TeV, performed by the ATLAS experiment at the Large Hadron Collider, together with deep inelastic scattering data from ep collisions at the HERA collider. The ATLAS data sets considered are differential cross-section measurements of inclusive W-+/- and Z/gamma* boson production, W-+/- and Z boson production in association with jets, t (t) over bar production, inclusive jet production and direct photon production. In the analysis, particular attention is paid to the correlation of systematic uncertainties within and between the various ATLAS data sets and to the impact of model, theoretical and parameterisation uncertainties. The resulting set of parton distribution functions is called ATLASpdf21
Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahuja S
- Ai X
- Aielli G
- Aizenberg I
- Akbiyik M
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Amelung C
- Ames CG
- Amidei D
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- Blumenthal J
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- Burgard CD
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- Busch EL
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- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Buzykaev AR
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- Cabras G
- Caforio D
- Cai H
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- Cairo VMM
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- Calafiura P
- Calderini G
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- Caloba LP
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- Camerlingo MT
- Cameron D
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- Camplani A
- Canale V
- Canesse A
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- Cao Y
- Capocasa F
- Capriles FGD
- Capua M
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- Cardarelli R
- Cardenas JCJ
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- Carlino G
- Carlson BT
- Carlson EM
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- Castillo FL
- Castillo LRF
- Castro NF
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- Catmore JR
- Cavaliere V
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- Cherepanova E
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- Chiu YH
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- Chwastowski JJ
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- Ciesla KM
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- Ciocio A
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- Corpe LD
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- Cortes-Gonzalez A
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- Da Costa AMMJ
- da Costa JBG
- Da Cruz E Silva CB
- Da Fonseca Pinto JV
- Da Silva GG
- Da Via C
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- De Maria A
- de Renstrom PAB
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- De K
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- Deviveiros PO
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- Do Vale TD
- Dodsworth D
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- Drechsler E
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- Fleck I
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- Yamaguchi N
- Yamaguchi Y
- Yamauchi H
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- Yao W-M
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- Yexley MR
- Yildiz HD
- Yin P
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- Yuan M
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- Yue L
- Yue X
- Zaazoua M
- Zabinski B
- Zagazeta LFG
- Zaid E
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zang J
- Zanzi D
- Zaplatilek O
- Zeitnitz C
- Zeißner SV
- Zeng JC
- Zenger DT
- Zenin O
- Zenz S
- Zerradi S
- Zerwas D
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang P
- Zhang R
- Zhang S
- Zhang T
- Zhang X
- Zhang X
- Zhang Z
- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/05/2023
- Field of study
Observation of electroweak production of two jets in association with an isolated photon and missing transverse momentum, and search for a Higgs boson decaying into invisible particles at 13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahnen JV
- Ai X
- Aielli G
- Aizenberg I
- Akatsuka S
- Akbiyik M
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amrouche CS
- Anastopoulos C
- Andana RYG
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparo MA
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin J
- Argyropoulos S
- Arling J
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Austrup VA
- Avner G
- Avolio G
- Ayoub MK
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Bachiu A
- Backman F
- Badea A
- Bagnaia P
- Bahilo JJL
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
- Bakos E
- Balaji S
- Balasubramanian R
- Baldin EM
- Balek P
- Ballabene E
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandieramonte M
- Bandyopadhyay A
- Bansal S
- Barak L
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barends KN
- Barillari T
- Barisits M
- Barkeloo J
- Barklow T
- Barnett BM
- Barnett RM
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barron U
- Barrue RFC
- Barsov S
- Bartels F
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Baselga M
- Bashta I
- Bassalat A
- Basso MJ
- Basson CR
- Bates RL
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- Batley JR
- Batool B
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- Bawa HS
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- Bellerive A
- Bello FAD
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- Beloborodov K
- Belotskiy K
- Belyaev NL
- Benchekroun D
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- Benjamin DP
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- Bhopatkar VS
- Bi R
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- Bingul A
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- Biondini A
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- Burton CD
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- Butterworth JM
- Buttinger W
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- Caforio D
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- Cakir IT
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- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvet D
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- Calvet TP
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- Camarda S
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- Camelia EA
- Camerlingo MT
- Cameron D
- Camincher C
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- Cardillo F
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- Carlson BT
- Carlson EM
- Carlson TI
- Carminati L
- Carnesale M
- Carney RMD
- Caron S
- Carquin E
- Carratta G
- Carrá S
- Carter JWS
- Carter TM
- Casadei D
- Casado MP
- Casha AF
- Castiglia EG
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Cavaliere V
- Cavalli N
- Cavasinni V
- Celebi E
- Celli F
- Centonze MS
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chadi Z
- Chakraborty D
- Chala M
- Chan J
- Chan WS
- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chatterjee M
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chen A
- Chen B
- Chen C
- Chen CH
- Chen H
- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen Y
- Cheng CL
- Cheng HC
- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu YH
- Chizhov MV
- Choi K
- Chomont AR
- Chou Y
- Chow YS
- Chowdhury T
- Christopher LD
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Ciaccio AD
- Ciaccio LD
- Cieri D
- Ciesla KM
- Cindro V
- Cioară IA
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubotaru DA
- Ciungu BM
- Clark A
- Clark PJ
- Clawson SE
- Clement C
- Clissa L
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Codina EP
- Coelli S
- Cohen H
- Coimbra AEC
- Cole B
- Collot J
- Columbie JMC
- Connell SH
- Connelly IA
- Conroy EI
- Conventi F
- Cooke HG
- Cooper-Sarkar AM
- Cormier F
- Cornell SD
- Corpe LD
- Corradi M
- Correia AMH
- Corrigan EE
- Corriveau F
- Costa MJ
- Costanza F
- Costanzo D
- Cote BM
- Coutinho YA
- Cowan G
- Cowley JW
- Cranmer K
- Crescioli F
- Cristinziani M
- Cristoforetti M
- Croft V
- Crosetti G
- Crépé-Renaudin S
- Cueto A
- Cui H
- Cukierman AR
- Cunningham WR
- Curcio F
- Czodrowski P
- Czurylo MM
- Da Costa AMMJ
- da Costa JBG
- Da Cruz E Silva CB
- Da Cunha Sargedas De Sousa MJ
- Da Fonseca Pinto JV
- Da Via C
- Daalen TRV
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dallapiccola C
- Dam M
- Damazio DO
- Damp J
- Dandoy JR
- Daneri MF
- Danninger M
- Dao V
- Darbo G
- Darmora S
- Dattagupta A
- David C
- Davidek T
- Davis DR
- Davis-Purcell B
- Dawson I
- de Andrade Filho LM
- De Araujo MV
- De Asmundis R
- De Beurs M
- De Carvalho ALM
- De Castro S
- De Groot N
- de Jong P
- De K
- de la Hoz SG
- De la Torre H
- De Lima RT
- De Maria A
- De Pedis D
- de Renstrom PAB
- De Sa RCL
- De Salvo A
- De Sanctis U
- De Santis M
- De Santo A
- De Souza EEP
- De Vivie De Regie JB
- Dedovich DV
- Degens J
- Deiana AM
- Deliot F
- Delitzsch CM
- Dell’Acqua A
- Dell’Asta L
- Delmastro M
- Delsart PA
- Demers S
- Demichev M
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Dette K
- Deutsch C
- Deviveiros PO
- Diaconu C
- Dias FA
- Diaz LP
- Diaz MA
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- Dickinson J
- Didenko M
- Diehl EB
- Dietrich J
- Dimitrievska A
- Ding W
- Dingfelder J
- Dinu I
- Dittmeier SJ
- Dittus F
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- Djuvsland JI
- Dodsworth D
- Doglioni C
- Dolejsi J
- Dolezal Z
- Domenico AD
- Dominguez LP
- Don MMR
- Donadelli M
- Donaldson CP
- Donato CD
- Donell DMM
- Dong B
- Donini J
- Donszelmann TC
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- Dova MT
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- Drechsler E
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- Drobac AS
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- Dubreuil A
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- Dziedzic BS
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- Eggleston MG
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- Farina EM
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- Fenyuk AB
- Ferguson SW
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- Filthaut F
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- Fleck I
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- Rennie AG
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- Rimoldi M
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- Rinnagel MP
- Ripellino G
- Riu I
- Rivadeneira P
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- Rusakovich NA
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- Ryzhov A
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- Salzburger A
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- Sander CO
- Sanderswood IG
- Sandesara JA
- Sandhoff M
- Sandoval C
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- Sapronov A
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- Scanlon T
- Schaarschmidt J
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- Schioppa EJ
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- Schleicher KE
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- Schmitt C
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- Schoeffel L
- Schoening A
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- Schroeder F
- Schroeder TV
- Schultz-Coulon H
- Schumacher M
- Schumm BA
- Schune P
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- Schwarz TA
- Schwemling P
- Schwienhorst R
- Schäfer U
- Sciandra A
- Sciolla G
- Scuri F
- Scutti F
- Seabra LFO
- Sebastian VS
- Sebastiani CD
- Sedlaczek K
- Seema P
- Seidel SC
- Seiden A
- Seidlitz BD
- Seiss T
- Seitz C
- Seixas JM
- Sekhniaidze G
- Sekula SJ
- Selem LP
- Semprini-Cesari N
- Sen S
- Serfon C
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- Serkin L
- Sessa M
- Severini H
- Sevova S
- Sforza F
- Sfyrla A
- Shabalina E
- Shaheen R
- Shahinian JD
- Shaikh NW
- Shan LY
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- Sharma A
- Sharma AS
- Sharma S
- Shatalov PB
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- Shi L
- Shimmin CO
- Shimogama Y
- Shinner JD
- Shipsey IPJ
- Shirabe S
- Shiyakova M
- Shlomi J
- Shochet MJ
- Shojaii J
- Shope DR
- Shrestha S
- Shrif EM
- Shroff MJ
- Shulga E
- Sicho P
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- Siegert F
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- Silverstein SB
- Simion S
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- Sinetckii V
- Singh S
- Sinha S
- Sioli M
- Siral I
- Sivoklokov S
- Sjölin J
- Skaf A
- Skorda E
- Skubic P
- Slawinska M
- Sliwa K
- Smakhtin V
- Smart BH
- Smiesko J
- Smirnov S
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smith EA
- Smith HA
- Smizanska M
- Smolek K
- Smykiewicz A
- Snesarev AA
- Snoek HL
- Snyder S
- Sobie R
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- Sohns F
- Sola JDB
- Soldatov E
- Soldevila U
- Solis AL
- Solodkov AA
- Solomon S
- Soloshenko A
- Solovyanov OV
- Solovyev V
- Sommer P
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- Sonay A
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- Sopczak A
- Sopio AL
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- Sottocornola S
- Soualah R
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- Spalla M
- Spangenberg M
- Spanò F
- Sperlich D
- Spieker TM
- Spigo G
- Spina M
- Spiteri DP
- Spousta M
- Stabile A
- Stamas BL
- Stamen R
- Stamenkovic M
- Stampekis A
- Standke M
- Stanecka E
- Stanislaus B
- Stanitzki MM
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- Stapf B
- Starchenko EA
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- Starko DM
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- Starovoitov P
- Staszewski R
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- Steinberg P
- Steinhebel AL
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- Straessner A
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- Strandberg S
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- Strebler T
- Strizenec P
- Strom DM
- Strom LR
- Stroud SV
- Stroynowski R
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- Ströhmer R
- Stucci SA
- Stugu B
- Stupak J
- Styles NA
- Stärz S
- Su D
- Su S
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- Su X
- Suarez RG
- Sugizaki K
- Sulin VV
- Sullivan MJ
- Sultan DMS
- Sultansoy S
- Sumida T
- Sun S
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- Suster CJE
- Sutton MR
- Svatos M
- Swiatlowski M
- Swirski T
- Sykora I
- Sykora M
- Sykora T
- Sánchez J
- Ta D
- Tackmann K
- Taffard A
- Tafirout R
- Taibah RHM
- Takashima R
- Takeda K
- Takeshita T
- Takeva EP
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- Talby M
- Talyshev AA
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- Tamir NM
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- Tanaka J
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- Tayalati Y
- Taylor GN
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- Tehrani FS
- Teixeira-Dias P
- Teoh JJ
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- Terron J
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- Testa M
- Teuscher RJ
- Themistokleous N
- Theveneaux-Pelzer T
- Thielmann O
- Thomas DW
- Thomas JP
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- Thompson PD
- Thomson E
- Thorpe EJ
- Tian Y
- Tikhomirov VO
- Tikhonov Y
- Timoshenko S
- Tipton P
- Tisserant S
- Tlou SH
- Tnourji A
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- Todt S
- Toerne EV
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- Trofymov A
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- Tsiskaridze V
- Tskhadadze EG
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- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsur O
- Tsybychev D
- Tu Y
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- Tudorache V
- Tuna AN
- Turchikhin S
- Turner RJ
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- Tuts PM
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- Tzovara E
- Uchida K
- Ukegawa F
- Unal G
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- Unel G
- Ungaro FC
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- Urban J
- Urbán SC
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- Ushioda R
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- Uysal Z
- Vacek V
- Vachon B
- Vadla KOH
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- Vale MABD
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- Valero A
- Vallance RA
- Vallier A
- Valéry L
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- Vandewall ER
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- Vari R
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- Varvell KE
- Vasile ME
- Vaslin L
- Vasquez GA
- Vazeille F
- Vazquez CJB
- Vazquez JGP
- Veatch J
- Vecchio V
- Veen MJ
- Veliscek I
- Veloce LM
- Veloso F
- Veneziano S
- Ventura A
- Vera AMR
- Verbytskyi A
- Verducci M
- Vergara JCR
- Vergis C
- Verkerke W
- Vermeulen AT
- Vermeulen JC
- Vernieri C
- Verschuuren PJ
- Verzini MJA
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- Vgenopoulos A
- Vickey T
- Viehhauser GHA
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- Villa M
- Villhauer EM
- Vilucchi E
- Vincter MG
- Virdee GS
- Vishwakarma A
- Vittori C
- Vivarelli I
- Vladimirov V
- Voevodina E
- Vogel M
- Vokac P
- Volpe DD
- Vorobel V
- Vorobev K
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- Vossebeld JH
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- Vranjes N
- Vrba V
- Vreeswijk M
- Vu NK
- Vuillermet R
- Vujinovic OV
- Vukotic I
- Vulpen IV
- Wada S
- Wagner C
- Wagner W
- Wahdan S
- Wahlberg H
- Wakasa R
- Wakida M
- Walbrecht VM
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- Walker SD
- Walkowiak W
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- Wang AM
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- Wanotayaroj C
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- Weingarten J
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- White MJ
- Whiteson D
- Wickremasinghe L
- Wiedenmann W
- Wiel C
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs LAM
- Wilbern DJ
- Wilkens HG
- Wilkins LJ
- Williams DM
- Williams HH
- Williams S
- Willocq S
- Windischhofer PJ
- Wingerter-Seez I
- Winklmeier F
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
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- Wolter MW
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- Wongel AF
- Worm SD
- Wosiek BK
- Woźniak KW
- Wraight K
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- Wu SL
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- Wuerzinger J
- Wyatt TR
- Wynne BM
- Wölker R
- Xella S
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- Xiang J
- Xiao X
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- Xie X
- Xiotidis I
- Xu D
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- Xu W
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- Yabsley B
- Yacoob S
- Yamaguchi N
- Yamaguchi Y
- Yamatani M
- Yamauchi H
- Yamazaki T
- Yamazaki Y
- Yan J
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- Yan Z
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- Yang Z
- Yao W
- Yap YC
- Ye H
- Ye J
- Ye S
- Yeletskikh I
- Yexley MR
- Yildiz HD
- Yin P
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zagazeta LFG
- Zaid E
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zeitnitz C
- Zeißner SV
- Zeng JC
- Zenger DT
- Zenin O
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- Zerradi S
- Zerwas D
- Zhang B
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- Zhang G
- Zhang J
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- Zhang X
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- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
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- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
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- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Publication date
- 01/01/2022
- Field of study