170 research outputs found
Transcriptomics and methylomics of CD4-positive T cells in arsenic-exposed women
- Author
- A Cardenas
- A Fragale
- A Rahman
- AE Jaffe
- AM Deaton
- AS Andrew
- B Hernandez-Castro
- BC Jackson
- C Cambiaggi
- CH Tseng
- CM Schlebusch
- CM Schlebusch
- CY McLean
- D Ferrario
- D Rojas
- DC Koestler
- DL Boone
- F Harari
- F Krueger
- Francesco Marabita
- Francesco Vezzi
- G Concha
- GA Soto-Pena
- IARC
- Joel Gruselius
- JR Pilsner
- K Broberg
- K Heyninck
- K Li
- KA Bailey
- KA Ramsey
- Karin Broberg
- Karin Engström
- KC Nadeau
- KD Hansen
- LH Boise
- M Argos
- M Lohoff
- M Miyamoto
- M Salgado-Bustamante
- M Vahter
- Marie Vahter
- Max Käller
- MC Wang
- ML Kile
- MT Zhao
- Nicola Prezza
- NL Dangleben
- P Intarasunanont
- Philip Ewels
- R Biswas
- R Raqib
- S Ahmed
- S Ahmed
- S Ahmed
- S Chuvpilo
- SE Moore
- SF Farzan
- T Dorn
- TK Wojdacz
- Tomasz K. Wojdacz
- VM Dixit
- W Ding
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Immune cell subsets and their gene expression profiles from human PBMC isolated by Vacutainer Cell Preparation Tube (CPT™) and standard density gradient
- Author
- A Boyum
- A Posevitz-Fejfar
- A Schroeder
- AL Rasmussen
- AM Newman
- AR Abbas
- AR Whitney
- C Nilsson
- C Palmer
- C Pelegri
- Christopher Burgess
- Christopher P. Corkum
- CR Bolen
- Danielle P. Ings
- DJ Tollerud
- E Arico
- EC Baechler
- GA Soto-Pena
- JD Herazo-Maya
- JE Kang
- JJ Bouwman
- JJ Eady
- JJ Ruitenberg
- JM Zimmerer
- JP Cobb
- K Murphy
- KA Reimann
- KC McKenna
- KR Tamul
- KR Tamul
- L Mole
- LE Peterson
- M Ehrhardt
- M Eikmans
- M Holodniy
- M Ishimura
- M Shi
- MJ Baine
- N Komatsu
- NI Rallon
- O Alter
- P Autissier
- P Elliott
- P Schlenke
- PA Bryant
- PJ McLaren
- R Edgar
- R Masud
- RJ Feezor
- S Debey
- S Fleige
- S Hashimoto
- S Shin
- S Sidharthan
- S Srivastava
- SS Shen-Orr
- Sylwia Karwowska
- T Gong
- T Huang
- TA Fava
- TF Meehan
- TJ Vries de
- TNQ Pham
- TNQ Pham
- Tomasz I. Michalak
- V Copois
- W Qiao
- Werner Kroll
- Y Jing
- Y Sasaki
- Y Tan
- YA Grigoryev
- YL Miao
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Scintillation light detection in the 6-m drift-length ProtoDUNE Dual Phase liquid argon TPC
- Author
- Abi B
- Abud A Abed
- Acciarri R
- Acero MA
- Adames MR
- Adamov G
- Adamowski M
- Adams D
- Adinolfi M
- Aduszkiewicz A
- Aguilar J
- Ahmad Z
- Ahmed J
- Aimard B
- Ali-Mohammadzadeh B
- Alion T
- Allison K
- Alonso MJ Rodriguez
- AlRashed M
- Alt C
- Alton A
- Alvarez R
- Alzas P Barham
- Amedo P
- Anderson J
- Andreopoulos C
- Andreotti M
- Andrews M
- Andrianala F
- Andringa S
- Anfimov N
- Ankowski A
- Antoniassi M
- Antonova M
- Antoshkin A
- Antusch S
- Aranda-Fernandez A
- Arellano L
- Arnold LO
- Arroyave MA
- Asaadi J
- Asquith L
- Aurisano A
- Aushev V
- Autiero D
- Ayala Lara V
- Ayala-Torres M
- Azfar F
- Back A
- Back H
- Back JJ
- Backhouse C
- Bagaturia I
- Bagby L
- Balashov N
- Balasubramanian S
- Baldi P
- Baller B
- Bambah B
- Barao F
- Barenboim G
- Barker G
- Barkhouse W
- Barnes C
- Barr G
- Barranco Monarca J
- Barros A
- Barros N
- Barrow JL
- Basharina-Freshville A
- Bashyal A
- Basque V
- Batchelor C
- Battat JBR
- Battisti F
- Bay F
- Bazetto MCQ
- Bazo Alba JLL
- Beacom JF
- Bechetoille E
- Behera B
- Beigbeder C
- Bellantoni L
- Bellettini G
- Bellini V
- Beltramello O
- Benekos N
- Berger J
- Berkman S
- Bernardini P
- Berner RM
- Bersani A
- Bertolucci S
- Betancourt M
- Betancur Rodriguez A
- Bevan A
- Bezawada Y
- Bezerra TJC
- Bhardwaj A
- Bhatnagar V
- Bhattacharjee M
- Bhattarai D
- Bhuller S
- Bhuyan B
- Biagi S
- Bian J
- Biassoni M
- Biery K
- Bilki B
- Bishai M
- Bitadze A
- Blake A
- Blaszczyk F
- Blazey GC
- Blucher E
- Boissevain J
- Bolognesi S
- Bolton T
- Bomben L
- Bonesini M
- Bongrand M
- Bonilla-Diaz C
- Bonini F
- Booth A
- Boran F
- Bordoni S
- Borkum A
- Bostan N
- Bour P
- Bourgeois C
- Boyden D
- Bracinik J
- Braga D
- Brailsford D
- Branca A
- Brandt A
- Bremer J
- Breton D
- Brew C
- Brice SJ
- Brizzolari C
- Bromberg C
- Brooke J
- Bross A
- Brunetti G
- Brunetti M
- Buchanan N
- Budd H
- Butorov I
- Cagnoli I
- Cai T
- Caicedo DA Martinez
- Caiulo D
- Calabrese R
- Calafiura P
- Calcutt J
- Calin M
- Calvez S
- Calvo E
- Caminata A
- Campanelli M
- Caratelli D
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- Carceller JC
- Carini G
- Carlus B
- Carneiro MF
- Carniti P
- Carranza H
- Carroll T
- Castano Forero JF
- Castillo A
- Castromonte C
- Catano-Mur E
- Cattadori C
- Cavalier F
- Cavallaro G
- Cavanna F
- Centro S
- Cerati G
- Cervelli A
- Cervera Villanueva A
- Chalifour M
- Chappell A
- Chardonnet E
- Charitonidis N
- Chatterjee A
- Chattopadhyay S
- Chavarry Neyra MSS
- Chen H
- Chen M
- Chen Y
- Chen Z
- Chen-Wishart Z
- Cheon Y
- Cherdack D
- Chi C
- Childress S
- Chirco R
- Chiriacescu A
- Chisnall G
- Cho K
- Choate S
- Chokheli D
- Chong PS
- Christensen A
- Christian D
- Christodoulou G
- Chukanov A
- Chung M
- Church E
- Cicero V
- Clarke P
- Cline G
- Coan TE
- Cocco AG
- Coelho JAB
- Colton N
- Conley E
- Conley R
- Conrad J
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- Copello S
- Cova P
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- Crespo-Anadon J
- Crisler M
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- Cross R
- Cudd A
- Cuesta C
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- Cussans D
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- DaMotta H
- das Chagas E Batista
- David C
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- Davies GS
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- De Bonis I
- De Gouvea A
- De Holanda PC
- De Icaza Astiz IL
- De Jong P
- De Lurgio P
- De Mello Neto JRT
- De Roeck A
- De Romeri V
- De Souza G
- de Souza H Vieira
- De K
- De S
- Debbins P
- Decowski MP
- Deisting A
- Delbart A
- Delepine D
- Delgado M
- Delgado MA Ramirez
- Dell'Acqua A
- Delmonte N
- DeMuth DM
- Dennis S
- Densham C
- Deptuch GW
- Devi R
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- Di Domizio S
- Di Giulio L
- Di Noto L
- Dias M
- Diaz F
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- Ding P
- Dirkx G
- Distefano C
- Diurba R
- Diwan M
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- Doering D
- Dolan S
- Dolinski M
- Domine L
- Donon Y
- Douglas D
- Douillet D
- Dragone A
- Drake G
- Drielsma F
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- Duchesneau D
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- Duyang H
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- Dwyer D
- Dyshkant A
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- Edmunds D
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- Emery S
- Englezos P
- Ereditato A
- Erjavec T
- Escobar C
- Eurin G
- Evans JJ
- Ewart E
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- Fahey K
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- Fani' M
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- Farzan Y
- Fedoseev D
- Felix J
- Feng Y
- Fernandez Menendez P
- Fernandez Morales M
- Fernandez-Martinez E
- Ferraro F
- Fields L
- Filip P
- Filthaut F
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- Fischer V
- Fitzpatrick RS
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- Zaki R
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- Zani A
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- Zeller GP
- Zennamo J
- Zeug K
- Zhang C
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- Zhao M
- Zhivun E
- Zhu G
- Zimmerman ED
- Zucchelli S
- Zuklin J
- Zutshi V
- Zwaska R
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 16/07/2022
- Field of study
DUNE is a dual-site experiment for long-baseline neutrino oscillation studies, neutrino astrophysics and nucleon decay searches. ProtoDUNE Dual Phase (DP) is a 6 × 6 × 6 m 3 liquid argon time-projection-chamber (LArTPC) that recorded cosmic-muon data at the CERN Neutrino Platform in 2019-2020 as a prototype of the DUNE Far Detector. Charged particles propagating through the LArTPC produce ionization and scintillation light. The scintillation light signal in these detectors can provide the trigger for non-beam events. In addition, it adds precise timing capabilities and improves the calorimetry measurements. In ProtoDUNE-DP, scintillation and electroluminescence light produced by cosmic muons in the LArTPC is collected by photomultiplier tubes placed up to 7 m away from the ionizing track. In this paper, the ProtoDUNE-DP photon detection system performance is evaluated with a particular focus on the different wavelength shifters, such as PEN and TPB, and the use of Xe-doped LAr, considering its future use in giant LArTPCs. The scintillation light production and propagation processes are analyzed and a comparison of simulation to data is performed, improving understanding of the liquid argon properties
Combination of searches for heavy spin-1 resonances using 139 fb−1 of proton-proton collision data at s = 13 TeV with the ATLAS detector
- Author
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- Aakvaag E
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- Abicht NJ
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- Zhemchugov A
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- Zimine NI
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- Springer Nature
- Publication date
- 19/04/2024
- Field of study
A combination of searches for new heavy spin-1 resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons or quarks, is presented. The data sample used corresponds to 139 fb−1 of proton-proton collisions at
= 13 TeV collected during 2015–2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb,
, and tb) or third-generation leptons (τν and ττ) are included in this kind of combination for the first time. A simplified model predicting a spin-1 heavy vector-boson triplet is used. Cross-section limits are set at the 95% confidence level and are compared with predictions for the benchmark model. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The complementarity of the various analyses increases the sensitivity to new physics, and the resulting constraints are stronger than those from any individual analysis considered. The data exclude a heavy vector-boson triplet with mass below 5.8 TeV in a weakly coupled scenario, below 4.4 TeV in a strongly coupled scenario, and up to 1.5 TeV in the case of production via vector-boson fusion
Measurement of the inclusive and differential Higgs boson production cross sections in the decay mode to a pair of τ Leptons in pp collisions at sqrt[s]=13 TeV
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- Aarrestad TK
- Aarup Petersen H
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- Yi K
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- Yohay R
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- Yumiceva F
- Yusli MN
- Zabi A
- Zacharopoulou A
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli AG
- Zeinali M
- Zeuner WD
- Zghiche A
- Zhang F
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- Zhang L
- Zhang W
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- Zhang Z
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- Zhizhin I
- Zhokin A
- Zhu DH
- Zhu RY
- Ziemons T
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zotz A
- Zou D
- Zou R
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez Fernández A
- Özçelik Ö
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2022
- Field of study
Measurements of the inclusive and differential fiducial cross sections of the Higgs boson are presented, using the τ lepton decay channel. The differential cross sections are measured as functions of the Higgs boson transverse momentum, jet multiplicity, and transverse momentum of the leading jet in the event, if any. The analysis is performed using proton-proton collision data collected with the CMS detector at the LHC at a center-of-mass energy of 13 TeV and corresponding to an integrated luminosity of 138 fb^{-1}. These are the first differential measurements of the Higgs boson cross section in the final state of two τ leptons. In final states with a large jet multiplicity or with a Lorentz-boosted Higgs boson, these measurements constitute a significant improvement over measurements performed in other final states
Separation of track- and shower-like energy deposits in ProtoDUNE-SP using a convolutional neural network
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- Publication venue
- Publication date
- 01/01/2022
- Field of study
Liquid argon time projection chamber detector technology provides high spatial and calorimetric resolutions on the charged particles traversing liquid argon. As a result, the technology has been used in a number of recent neutrino experiments, and is the technology of choice for the Deep Underground Neutrino Experiment (DUNE). In order to perform high precision measurements of neutrinos in the detector, final state particles need to be effectively identified, and their energy accurately reconstructed. This article proposes an algorithm based on a convolutional neural network to perform the classification of energy deposits and reconstructed particles as track-like or arising from electromagnetic cascades. Results from testing the algorithm on data from ProtoDUNE-SP, a prototype of the DUNE far detector, are presented. The network identifies track- and shower-like particles, as well as Michel electrons, with high efficiency. The performance of the algorithm is consistent between data and simulation
Separation of track- and shower-like energy deposits in ProtoDUNE-SP using a convolutional neural network
- Author
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Liquid argon time projection chamber detector technology provides high spatial and calorimetric resolutions on the charged particles traversing liquid argon. As a result, the technology has been used in a number of recent neutrino experiments, and is the technology of choice for the Deep Underground Neutrino Experiment (DUNE). In order to perform high precision measurements of neutrinos in the detector, final state particles need to be effectively identified, and their energy accurately reconstructed. This article proposes an algorithm based on a convolutional neural network to perform the classification of energy deposits and reconstructed particles as track-like or arising from electromagnetic cascades. Results from testing the algorithm on experimental data from ProtoDUNE-SP, a prototype of the DUNE far detector, are presented. The network identifies track- and shower-like particles, as well as Michel electrons, with high efficiency. The performance of the algorithm is consistent between experimental data and simulation
Combined measurement of the Higgs boson mass from the H → γγ and H → ZZ∗ → 4ℓ decay channels with the ATLAS detector using √s = 7, 8, and 13 TeV pp collision data
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- Zhang B
- Zhang DF
- Zhang J
- Zhang J
- Zhang K
- Zhang L
- Zhang P
- Zhang R
- Zhang S
- Zhang S
- Zhang T
- Zhang X
- Zhang X
- Zhang Y
- Zhang Y
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao H
- Zhao P
- Zhao T
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng J
- Zheng K
- Zheng X
- Zheng Z
- Zhong D
- Zhou B
- Zhou H
- Zhou N
- Zhou Y
- Zhu CG
- Zhu J
- Zhu Y
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zimine NI
- Zinsser J
- Ziolkowski M
- Zoccoli A
- Zoch K
- Zorbas TG
- Zormpa O
- Zou W
- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2023
- Field of study
A measurement of the mass of the Higgs boson combining the
H
→
Z
Z
∗
→
4
ℓ
and
H
→
γ
γ
decay channels is presented. The result is based on
140
fb
−
1
of proton-proton collision data collected by the ATLAS detector during LHC run 2 at a center-of-mass energy of 13 TeV combined with the run 1 ATLAS mass measurement, performed at center-of-mass energies of 7 and 8 TeV, yielding a Higgs boson mass of
125.11
±
0.09
(
stat
)
±
0.06
(
syst
)
=
125.11
±
0.11
GeV
. This corresponds to a 0.09% precision achieved on this fundamental parameter of the Standard Model of particle physics
Recommended from our members
Evidence for tWZ production in proton-proton collisions at √s=13 TeV in multilepton final states
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbott S
- Abbrescia M
- Abdullin S
- Abreu A
- Abu Zeid S
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- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang W
- Zhang Y
- Zhang Y
- Zhizhin I
- Zhokin A
- Zhou C
- Zhu RY
- Ziemons T
- Zilizi G
- Zimermmane Castro Santos A
- Zipper N
- Zisopoulos I
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zotz A
- Zou R
- Zucchetta A
- Zuo X
- Zuolo D
- Zygala L
- Publication venue
- Elsevier BV
- Publication date
- 21/06/2024
- Field of study
Data availability - https://www.sciencedirect.com/science/article/pii/S0370269324003733?via%3Dihub#dav0001 [Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS data preservation, re-use and open access policy (https://cms-docdb.cern.ch/cgi-bin/PublicDocDB/RetrieveFile?docid=6032&filename=CMSDataPolicyV1.2.pdf&version=2)]The first evidence for the standard model production of a top quark in association with a W boson and a Z boson is reported. The measurement is performed in multilepton final states, where the Z boson is reconstructed via its decays to electron or muon pairs. At least one W boson, associated or from top quark decay, decays leptonically, too. The analysed data were recorded by the CMS experiment at the CERN LHC in 2016–2018 in proton-proton collisions at √s=13 TeV, and correspond to an integrated luminosity of 138 fb−1. The measured cross section is 354±54(stat)±95(syst) fb, and corresponds to a statistical significance of 3.4 standard deviations.SCOAP
Recommended from our members
Search for electroweak production of charginos and neutralinos at s = 13 TeV in final states containing hadronic decays of WW, WZ, or WH and missing transverse momentum
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
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- Landsberg G
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- Matveev V
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- Palencia Cortezon E
- Palichik V
- Palit P
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- Panagiotou A
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- Pandolfi F
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- Paolucci P
- Papadimitriou V
- Papadopoulos I
- Papakrivopoulos I
- Papavergou I
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- Perez Lara CE
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- Perovic V
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- Petkov P
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- Piccolo D
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- Pinolini BS
- Piparo D
- Piperov S
- Pisano M
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- Pitters FM
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- Polatoz A
- Pompili A
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- Postiau N
- Potenza R
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- Pugliese G
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- Puljak I
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- Rappoccio S
- Raspereza A
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- Rathjens D
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- Ratti SP
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- Raymond DM
- Razis PA
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- Reales Gutiérrez G
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- Redjimi R
- Redondo I
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- Regnery B
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- Reichmann M
- Reid ID
- Reid M
- Reimers A
- Reinsvold Hall A
- Reis T
- Reissel C
- Reitenspiess T
- Reithler H
- Rejeb Sfar H
- Rembser J
- Rendón C
- Revering M
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- Ribeiro Lopes B
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- Rodríguez Bouza V
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- Roy A
- Roy D
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- Royon C
- Ruchti R
- Rudrabhatla S
- Ruini D
- Ruiz Alvarez JD
- Ruiz-Jimeno A
- Rumerio P
- Rusack R
- Rusinov V
- Ruspa M
- Ryd A
- Rykaczewski H
- Ryu MS
- Rádl AJ
- Röwert N
- Rübenach J
- Safonov A
- Saggio A
- Sagir S
- Saha G
- Saha P
- Sahasransu AR
- Sahin MÖ
- Sahu B
- Saibel A
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- Sakulin H
- Salazar Ibarguen HA
- Salerno R
- Salfeld-Nebgen J
- Saltzberg D
- Salur S
- Salvatico R
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- Schmitz E
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- Schnepf M
- Schnetzer S
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- Schroeder N
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- Schuler SC
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- Schwandt J
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- Schweiger K
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- Schütze P
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- Sekmen S
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- Setti F
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- Sguazzoni G
- Shafiei N
- Shah A
- Shah MA
- Shalaev V
- Shang V
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- Sharma A
- Sharma A
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- Shoaib M
- Shopova M
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- Shulha S
- Shvetsov I
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- Siado JE
- Siddireddy P
- Siikonen H
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- Silvestris L
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- Slabospitskii S
- Smirnov I
- Smirnov V
- Smith C
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- Smith VJ
- Smith WH
- Snigirev A
- Snoeys W
- Snow GR
- Snyder C
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- Solano A
- Soldi D
- Somalwar S
- Song D
- Sonnadara DUJ
- Sonneveld J
- Sordini V
- Sorrentino G
- Sosa Ricardo RE
- Sosnov D
- Soto Rodríguez A
- Spagnolo P
- Spanier S
- Sperka D
- Sphicas P
- Spiegel L
- Spiga D
- Spiropulu M
- Spitzbart D
- Srimanobhas N
- Stadie H
- Stafford D
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- Staiano A
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- Susa T
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- Sánchez Hernández A
- Sánchez Navas S
- Sözbilir Ü
- Tabarelli de Fatis T
- Tabb W
- Tadel M
- Takahashi Y
- Tali B
- Taliercio A
- Tamulaitis G
- Tani L
- Tannenwald B
- Tao J
- Tapper A
- Tarabini A
- Tatar K
- Taus R
- Tavernier S
- Tavolaro VR
- Taylor D
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- Teague D
- Tedeschi T
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- Tekten S
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- Teodorescu L
- Terkulov A
- Teroerde M
- Terrill W
- Teryaev O
- Tews A
- Teyssier D
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- Thiel M
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- Thomas L
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- Tiras E
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- Titov M
- Tiwari PC
- Tkaczyk S
- Tok UG
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- Tomalin IR
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- Tonjes MB
- Tonon N
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- Tornago M
- Toropin A
- Torres Da Silva De Araujo F
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- Tosi M
- Tosi S
- Touquet G
- Townsend A
- Tramontano R
- Tran NV
- Tran TT
- Trapote A
- Treille D
- Trembath-Reichert S
- Trevisani N
- Tricomi A
- Trocino D
- Trocsanyi ZL
- Tropea P
- Tsamalaidze Z
- Tsatsos A
- Tsipolitis G
- Tsirou A
- Tully C
- Tumasyan A
- Tuo S
- Tuominen E
- Tuominiemi J
- Turini N
- Turkcapar S
- Tuuva T
- Tuve C
- Tytgat M
- Tziaferi E
- Uchida K
- Ujvari B
- Ulmer KA
- Ulrich R
- Uniyal R
- Uplegger L
- Urda Gómez L
- Uribe Estrada C
- Usai E
- Uvarov L
- Uzunian A
- Vaandering EW
- Vagnerini A
- Vai I
- Valencia Palomo L
- Valsecchi D
- Valuev V
- Van De Klundert M
- Van Der Linden J
- Van Doninck W
- Van Hove P
- Van Mechelen P
- Van Onsem GP
- Van Putte S
- Van Remortel N
- Vanden Bemden M
- Vander Donckt M
- Vander Velde C
- Vanlaer P
- Vannerom D
- Varela J
- Varelas N
- Vargas Hernandez AM
- Vats D
- Vazquez Valencia F
- Vazzoler F
- Veckalns V
- Veelken C
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- Vellidis K
- Venditti R
- Venturi A
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- Veres GI
- Vermassen B
- Verwilligen P
- Veszpremi V
- Vetens W
- Viazlo O
- Vico Villalba C
- Vigilante L
- Viinikainen J
- Vila I
- Vilela Pereira A
- Viliani L
- Virdee T
- Virdi AK
- Viret S
- Vischia P
- Vitulo P
- Vizan Garcia JM
- Vlasov E
- Vlimant JR
- Vojinovic M
- Volkov S
- Volobouev I
- Von Cube RF
- Vorobyev A
- Vourliotis E
- Voutilainen M
- Voytishin N
- Vámi TÁ
- Wadud MA
- Wagner SR
- Walkingshaw Pass K
- Wallny R
- Walsh R
- Waltenberger W
- Walter D
- Wamorkar T
- Wanczyk J
- Wang B
- Wang C
- Wang D
- Wang F
- Wang H
- Wang J
- Wang J
- Wang J
- Wang L
- Wang Q
- Wang Q
- Wang S
- Wang X
- Wang Y
- Wang Z
- Wang Z
- Waqas M
- Wardle N
- Warner Z
- Wassmer M
- Watson IJ
- Wayne M
- Webb SN
- Weber HA
- Weber M
- Wei K
- Wen Y
- Wertz S
- West C
- Wezenbeek L
- Whitbeck A
- White R
- White S
- Wichmann K
- Wickramage N
- Wickramarathna DDC
- Wiedenbeck S
- Wieland S
- Wiens L
- Wightman A
- Williams A
- Williams J
- Williams T
- Willmott C
- Wilson G
- Wilson J
- Wimpenny S
- Winer BL
- Winterbottom D
- Wisecarver A
- Wissing C
- Wittich P
- Wolf R
- Wong K
- Wong WY
- Wood D
- Wozniak KA
- Wozniewski S
- Wright D
- Wu HY
- Wu Z
- Wuchterl S
- Wulz C-E
- Wunsch S
- Wyslouch B
- Würthwein F
- Xiang Y
- Xiao J
- Xiao M
- Xiao R
- Xie S
- Xie W
- Yagil A
- Yalvac M
- Yan F
- Yan X
- Yang H
- Yang S
- Yang S
- Yang UK
- Yang YC
- Yao Y
- Yarar H
- Yates BR
- Yazgan E
- Ye Z
- Yetkin EA
- Yi K
- Yigitbasi E
- Yohay R
- Yoo HD
- Yoo J
- Yoon I
- You Z
- Yu D
- Yu GB
- Yu I
- Yu PR
- Yu SS
- Yuan L
- Yuan S
- Yuldashev BS
- Yumiceva F
- Zabi A
- Zacharopoulou A
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli AG
- Zeinali M
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang W
- Zhang Y
- Zhang Y
- Zhang Y
- Zhang Z
- Zhao J
- Zhizhin I
- Zhokin A
- Zhu RY
- Ziemons T
- Zipper N
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zotz A
- Zou D
- Zou R
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez Fernández A
- Özçelik Ö
- Publication venue
- Elsevier
- Publication date
- 15/09/2022
- Field of study
Data availability:
Release and preservation of data used by the CMS Collaboration as the basis for publications is guided by the CMS policy as stated in “CMS data preservation, re-use and open access policy”.A preprint version of this article is archived at: arXiv:2205.09597v2 [hep-ex], https://arxiv.org/abs/2205.09597v2 . Comments: Replaced with the published version. Added the journal reference. All the figures and tables, including additional supplementary figures and tables, can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/SUS-21-002 (CMS Public Pages). Report number: CMS-SUS-21-002, CERN-EP-2022-031This Letter presents a search for direct production of charginos and neutralinos via electroweak interactions. The results are based on data from proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC, corresponding to an integrated luminosity of 137 fb^{-1}. The search considers final states with large missing transverse momentum and pairs of hadronically decaying bosons WW, WZ, and WH, where H is the Higgs boson. These bosons are identified using novel algorithms. No significant excess of events is observed relative to the expectations from the standard model. Limits at the 95% confidence level are placed on the cross section for production of mass-degenerate wino-like supersymmetric particles χ~±1 and χ~02, and mass-degenerate higgsino-like supersymmetric particles χ~±1, χ~02, and χ~03. In the limit of a nearly-massless lightest supersymmetric particle χ~01, wino-like particles with masses up to 870 and 960 GeV are excluded in the cases of χ~02 → Zχ~01 and χ~02 → Hχ~01, respectively, and higgsino-like particles are excluded between 300 and 650 GeV.SCOAP3
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