142 research outputs found
Evidence of exposure to SARS-CoV-2 in cats and dogs from households in Italy
- Author
- Publication venue
- 'Cold Spring Harbor Laboratory'
- Publication date
- 01/01/2020
- Field of study
AbstractSARS-CoV-2 originated in animals and is now easily transmitted between people. Sporadic detection of natural cases in animals alongside successful experimental infections of pets, such as cats, ferrets and dogs, raises questions about the susceptibility of animals under natural conditions of pet ownership. Here we report a large-scale study to assess SARS-CoV-2 infection in 817 companion animals living in northern Italy, sampled at a time of frequent human infection. No animals tested PCR positive. However, 3.4% of dogs and 3.9% of cats had measurable SARS-CoV-2 neutralizing antibody titers, with dogs from COVID-19 positive households being significantly more likely to test positive than those from COVID-19 negative households. Understanding risk factors associated with this and their potential to infect other species requires urgent investigation.One Sentence SummarySARS-CoV-2 antibodies in pets from Italy.</jats:sec
Relaxing learned constraints through cathodal tDCS on the left dorsolateral prefrontal cortex
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 28/04/2017
- Field of study
We solve problems by applying previously learned rules. The dorsolateral prefrontal cortex (DLPFC) plays a pivotal role in automating this process of rule induction. Despite its usual efficiency, this process fails when we encounter new problems in which past experience leads to a mental rut. Learned rules could therefore act as constraints which need to be removed in order to change the problem representation for producing the solution. We investigated the possibility of suppressing the DLPFC by transcranial direct current stimulation (tDCS) to facilitate such representational change. Participants solved matchstick arithmetic problems before and after receiving cathodal, anodal or sham tDCS to the left DLPFC. Participants who received cathodal tDCS were more likely to solve the problems that require the maximal relaxation of previously learned constraints than the participants who received anodal or sham tDCS. We conclude that cathodal tDCS over the left DLPFC might facilitate the relaxation of learned constraints, leading to a successful representational change
High Visual Working Memory Capacity in Trait Social Anxiety
- Author
- Andreas Keil
- AP Pacheco-Unguetti
- ARA Conway
- CD Spielberger
- D Gimmig
- D Soto
- DM Clark
- DM Stout
- E Awh
- E Awh
- E Leigh
- EA Holmes
- EK Vogel
- EK Vogel
- F McNab
- GA Alvarez
- H Pashler
- H Shimizu
- I Okajima
- I Régner
- J Moriya
- J Moriya
- J Moriya
- J Stöeber
- J Stöeber
- JJ Todd
- JL Birk
- Jun Moriya
- K Fukuda
- K Fukuda
- K Mogg
- L Visu-Petra
- M Gamer
- MG Machizawa
- ML Turner
- MM Chun
- MR Leary
- MS DeCaro
- MW Eysenck
- N Amir
- N Cowan
- N Derakshan
- N Lavie
- N Lavie
- N Sadeh
- O Robinson
- PJ Olesen
- R Pishyar
- RM Rapee
- RW Engle
- S Hayes
- S Sasagawa
- SJ Bishop
- SJ Bishop
- SJ Luck
- SL Beilock
- SL Beilock
- SM Jaeggi
- T Klingberg
- T Schmader
- W Zhang
- Y Xu
- Yoshinori Sugiura
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2012
- Field of study
Working memory capacity is one of the most important cognitive functions influencing individual traits, such as attentional control, fluid intelligence, and also psychopathological traits. Previous research suggests that anxiety is associated with impaired cognitive function, and studies have shown low verbal working memory capacity in individuals with high trait anxiety. However, the relationship between trait anxiety and visual working memory capacity is still unclear. Considering that people allocate visual attention more widely to detect danger under threat, visual working memory capacity might be higher in anxious people. In the present study, we show that visual working memory capacity increases as trait social anxiety increases by using a change detection task. When the demand to inhibit distractors increased, however, high visual working memory capacity diminished in individuals with social anxiety, and instead, impaired filtering of distractors was predicted by trait social anxiety. State anxiety was not correlated with visual working memory capacity. These results indicate that socially anxious people could potentially hold a large amount of information in working memory. However, because of an impaired cognitive function, they could not inhibit goal-irrelevant distractors and their performance decreased under highly demanding conditions
Incubation and interactivity in insight problem solving
- Author
- A Chuderski
- A Toon
- A Weller
- AS Patrick
- C Baber
- C González-Vallejo
- D Kirsh
- D Kirsh
- DA Norman
- DE Rumelhart
- E Fioratou
- E Fioratou
- E Hutchins
- E Segal
- F Vallée-Tourangeau
- F Vallée-Tourangeau
- F Vallée-Tourangeau
- Frédéric Vallée-Tourangeau
- G Knoblich
- G Vallée-Tourangeau
- G Vallée-Tourangeau
- G Wallas
- Gaëlle Vallée-Tourangeau
- HL Roediger
- JN MacGregor
- KJ Gilhooly
- L Malafouris
- MH Aschraft
- MS DeCaro
- Niyat Henok
- R Ellis
- RW Weisberg
- S Ohlsson
- SV Steffensen
- T Ingold
- UN Sio
- Y Chu
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 26/02/2018
- Field of study
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
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdelalim AA
- Abdullin S
- Abercrombie D
- Abreu A
- Acharya H
- Acosta D
- Adam W
- Adamidis K
- Adams E
- Adams MR
- Adams T
- Addesa FM
- Adloff C
- Adzic P
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmed A
- Ahuja S
- Aime' C
- Akchurin N
- Akgun B
- Akpinar A
- Albergo S
- Albert A
- Albrecht S
- Albrow M
- Alcaraz Maestre J
- Aldaya Martin M
- Aldá Júnior WL
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Almond J
- Alpana K
- Alvarez Gonzalez B
- Alverson G
- Alves Gallo Pereira M
- Alves GA
- Aly R
- Alyari M
- Amapane N
- Ambrozas M
- Amendola C
- Amin N
- Amram O
- Amsler C
- An S
- An Y
- Anagnostou G
- Andrea J
- Andreassi G
- Andreev V
- Andreev Y
- Andrejkovic JW
- Andrews MB
- Androsov K
- Anguiano J
- Antchev G
- Anthony D
- Antunovic Z
- Apollinari G
- Apparu D
- Appelt E
- Apresyan A
- Apyan A
- Araujo M
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arneodo M
- Aruta C
- Asavapibhop B
- Asawatangtrakuldee C
- Asenov P
- Asghar MI
- Asilar E
- Askew A
- Asmuss P
- Atakisi IO
- Attikis A
- Auffray E
- Aushev T
- Auzinger G
- Avati V
- Avery P
- Avila C
- Awais A
- Awan MIM
- Ayala E
- Ayala G
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzurri P
- Baarmand MM
- Babaev A
- Bacchetta N
- Bachiller I
- Bachtis M
- Backhaus M
- Baden A
- Baechler J
- Bagliesi G
- Bahinipati S
- Baillon P
- Bainbridge R
- Bakas G
- Bakhshiansohi H
- Bakshi AS
- Baldenegro Barrera C
- Ban Y
- Band R
- Bandyopadhyay H
- Banerjee S
- Banerjee S
- Bansal S
- Barbagli G
- Barberis E
- Bargassa P
- Baringer P
- Barnes VE
- Barney D
- Baron O
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- Barrio Luna M
- Barroso Ferreira Filho M
- Bartek R
- Bartosik N
- Bartók M
- Bastos D
- Battilana C
- Baty A
- Bauer G
- Bauerdick LAT
- Baxter S
- Bayatmakou M
- Bayshev I
- Bean A
- Beauceron S
- Beaudette F
- Becerril Gonzalez H
- Bechtel J
- Bedoya CF
- Beghin D
- Behera PK
- Behera SC
- Behnke O
- Bein S
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- Bell KW
- Bellan R
- Belloni A
- Bellora A
- Belyaev A
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- Benaglia A
- Benato L
- Bencze G
- Bendavid J
- Benecke A
- Benelli G
- Benitez JF
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- Berenguer Antequera J
- Bergauer T
- Berger P
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- Bermúdez Martínez A
- Bernardes CA
- Bernet C
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- Bertacchi V
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- Bestintzanos I
- Bethani A
- Beyrouthy T
- Bhal E
- Bhardwaj A
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- Bhattacharya R
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- Bhowmik D
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- Bhyun JH
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- Bialkowska H
- Bianchini L
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- Bilin B
- Bin Anuar AA
- Bin Norjoharuddeen N
- Bisello D
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- Blekman F
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- Blumenfeld B
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- Bocci A
- Bodek A
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- Boldrini G
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- Bonacorsi D
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- Bonomally S
- Boos E
- Boran F
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- Bornheim A
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- Borshch V
- Bortignon P
- Bose T
- Bossini E
- Botta C
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- Boudoul G
- Bouhali O
- Bourgatte G
- Bourilkov D
- Bozzo M
- Bragagnolo A
- Braghieri A
- Brainerd C
- Brandao Malbouisson H
- Brandt S
- Branson JG
- Breedon R
- Breeze S
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- Brinkerhoff A
- Brivio F
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- Cakir A
- Calandri A
- Calderon De La Barca Sanchez M
- Calderon A
- Cali IA
- Calligaris L
- Calzaferri S
- Camen C
- Caminada L
- Campagnari C
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- Candelise V
- Canelli MF
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- Capeans Garrido M
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- Carvalho Antunes De Oliveira A
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- Casarsa M
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- Castaldi R
- Castaneda Hernandez A
- Castilla-Valdez H
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- Cepeda M
- Cerati GB
- Cerci S
- Cerminara G
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- Cetorelli F
- Chabert EC
- Chadeeva M
- Chahal GS
- Chang P
- Chanon N
- Chao Y
- Chapon E
- Charlot C
- Chatterjee RM
- Chatterjee S
- Chaudhary G
- Chauhan S
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- Chawla R
- Checchia P
- Chekhovsky V
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- Chen GM
- Chen HS
- Chen KF
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- Chen PH
- Chen X
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- Chenarani S
- Cheng C
- Cheng T
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- Cherepanov V
- Chernyavskaya N
- Chertok M
- Cheung HWK
- Chhibra SS
- Chiarito B
- Chinellato J
- Chlebana F
- Cho S
- Choi J
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- Choi S
- Chou JP
- Choudhary BC
- Choudhury S
- Christoforou K
- Chudasama R
- Chwalek T
- Ciangottini D
- Ciocci MA
- Cipriani M
- Citron M
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clement E
- Clerbaux B
- CMS Collaboration
- Cockerill DJA
- Colaleo A
- Coldham K
- Cole JE
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- Collard C
- Colling D
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- Cometti S
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- Consuegra Rodríguez S
- Contardo D
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- Cranshaw DJ
- Creanza D
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- Cutts D
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- D'Hondt J
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- Dabrowski A
- Dalchenko M
- Dallavalle GM
- Damarseckin S
- Damgov J
- Danilov V
- Darej D
- Darwish MR
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- Dewanjee RK
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- Donegà M
- Donertas IS
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- Droll A
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- Ebrahimi A
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- Fallavollita F
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- Herwig TC
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- Iaydjiev P
- Iemmi F
- Ignatenko M
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- Incandela J
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- Iorio AOM
- Iqbal MA
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- Ivanov Y
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- Jayananda MK
- Jayatilaka B
- Jeitler M
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- Jeon S
- Jessop C
- Jha V
- Jin W
- Jindariani S
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- Johnson KF
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- Jomhari NZ
- Jones M
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- Joshi BM
- Joshi U
- Joyce M
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- Kaestli HC
- Kailasapathy B
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- Yao Y
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- Yi K
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- Yohay R
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- Yuan S
- Yuldashev BS
- 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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- 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
Observation of triple J/ψ meson production in proton-proton collisions
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullah WATW
- Abdullin S
- Abercrombie D
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- Yohay R
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- Yumiceva F
- Yusli MN
- Yzquierdo AP-C
- Zabi A
- Zacharopoulou A
- Zahid S
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
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- Zecchinelli AG
- Zeid SA
- Zeinali M
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang W
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- Zhang Y
- Zhang Y
- Zhang Z
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- Zhizhin I
- Zhokin A
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- Zhu RY
- Ziemons T
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zotz A
- Zou D
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- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez CR
- Özçelik Ö
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 19/01/2023
- Field of study
Data availability:
Tabulated results are provided in the HEPData record for this analysis71. 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.Code availability:
The CMS core software is publically available at https://github.com/cms-sw/cmssw.Copyright . Protons consist of three valence quarks, two up-quarks and one down-quark, held together by gluons and a sea of quark-antiquark pairs. Collectively, quarks and gluons are referred to as partons. In a proton-proton collision, typically only one parton of each proton undergoes a hard scattering – referred to as single-parton scattering – leaving the remainder of each proton only slightly disturbed. Here, we report the study of double- and triple-parton scatterings through the simultaneous production of three J/ψ mesons, which consist of a charm quark-antiquark pair, in proton-proton collisions recorded with the CMS experiment at the Large Hadron Collider. We observed this process – reconstructed through the decays of J/ψ mesons into pairs of oppositely charged muons – with a statistical significance above five standard deviations. We measured the inclusive fiducial cross-section to be 272+141−104(stat)±17(syst)fb, and compared it to theoretical expectations for triple-J/ψ meson production in single-, double- and triple-parton scattering scenarios. Assuming factorization of multiple hard-scattering probabilities in terms of single-parton scattering cross-sections, double- and triple-parton scattering are the dominant contributions for the measured process.SCOAP3.Change history:
27 February 2023A Correction to this paper has been published: https://doi.org/10.1038/s41567-023-01992-
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
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- 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
Recommended from our members
Search for new heavy resonances decaying to WW, WZ, ZZ, WH, or ZH boson pairs in the all-jets final state in proton-proton collisions at s = 13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
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- Wissing C
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- Yockey H
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- Yusuff I
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- Zalewski P
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- Zecchinelli AG
- Zeuner WD
- Zghiche A
- Zhang F
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- Zhizhin I
- Zhokin A
- Zhu RY
- Ziemons T
- Zimermmane Castro Santos A
- Zipper N
- Zisopoulos I
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zotto P
- Zotz A
- Zou R
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez Fernández A
- Özçelik Ö
- Publication venue
- Elsevier
- Publication date
- 26/02/2023
- Field of study
A preprint version of this article is available at arXiv:2210.00043v2 [hep-ex], https://arxiv.org/abs/2210.00043v2 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables, including additional supplementary figures, can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/B2G-20-009 (CMS Public Pages). Report number: CMS-B2G-20-009, CERN-EP-2022-152.Data availability: see: https://cms-results.web.cern.ch/cms-results/public-results/publications/B2G-20-009 .A search for new heavy resonances decaying to WW, WZ, ZZ, WH, or ZH boson pairs in the all-jets final state is presented. The analysis is based on proton-proton collision data recorded by the CMS detector in 2016-2018 at a centre-of-mass energy of 13 TeV at the CERN LHC, corresponding to an integrated luminosity of 138 fb^{-1}. The search is sensitive to resonances with masses between 1.3 and 6 TeV, decaying to bosons that are highly Lorentz-boosted such that each of the bosons forms a single large-radius jet. Machine learning techniques are employed to identify such jets. No significant excess over the estimated standard model background is observed. A maximum local significance of 3.6 standard deviations, corresponding to a global significance of 2.3 standard deviations, is observed at masses of 2.1 and 2.9 TeV. In a heavy vector triplet model, spin-1 Z' and W' resonances with masses below 4.8 TeV are excluded at the 95% confidence level (CL). These limits are the most stringent to date. In a bulk graviton model, spin-2 gravitons and spin-0 radions with masses below 1.4 and 2.7 TeV, respectively, are excluded at 95% CL. Production of heavy resonances through vector boson fusion is constrained with upper cross section limits at 95% CL as low as 0.1 fb.SCOAP3
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Search for Higgs boson decays to a Z boson and a photon in proton-proton collisions at s = 13 TeV
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- Aarup Petersen H
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- Yao Y
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- Ye Z
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- Yohay R
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- Yumiceva F
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- Zacharopoulou A
- Zahid S
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- Zalewski P
- Zanetti M
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- 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
- Springer Nature on behalf of SISSA
- Publication date
- 01/08/2022
- Field of study
A preprint version of the article is available at arXiv:2204.12945v2 [hep-ex], https://arxiv.org/abs/2204.12945v2 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables can be found at https://cms-results.web.cern.ch/cms-results/public-results/publications/HIG-19-014 (CMS Public Pages). Report number: CMS-HIG-19-014, CERN-EP-2022-019.Results are presented from a search for the Higgs boson decay H → Zγ, where Z → ℓ+ℓ− with ℓ = e or μ. The search is performed using a sample of proton-proton (pp) collision data at a center-of-mass energy of 13 TeV, recorded by the CMS experiment at the LHC, corresponding to an integrated luminosity of 138 fb^{−1}. Events are assigned to mutually exclusive categories, which exploit differences in both event topology and kinematics of distinct Higgs production mechanisms to enhance signal sensitivity. The signal strength μ, defined as the product of the cross section and the branching fraction [σ(pp → H)B(H → Zγ)] relative to the standard model prediction, is extracted from a simultaneous fit to the ℓ+ℓ−γ invariant mass distributions in all categories and is found to be μ = 2.4 ± 0.9 for a Higgs boson mass of 125.38 GeV. The statistical significance of the observed excess of events is 2.7 standard deviations. This measurement corresponds to σ(pp → H)B(H → Zγ) = 0.21 ± 0.08 pb. The observed (expected) upper limit at 95% confidence level on μ is 4.1 (1.8). The ratio of branching fractions B(H → Zγ)/B(H → γγ) is measured to be 1.5 +0.7−0.6, which agrees with the standard model prediction of 0.69 ± 0.04 at the 1.5 standard deviation level.SCOAP3
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Measurements of the Higgs boson production cross section and couplings in the W boson pair decay channel in proton-proton collisions at s = 13 TeV
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- Whitbeck A
- White R
- 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 M
- 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 Y
- Yang YC
- Yao Y
- Yarar H
- Yates BR
- Yazgan E
- Ye Z
- Yi K
- Yigitbasi E
- Yockey H
- Yohay R
- Yoo HD
- Yoo J
- Yoo J
- Yoon I
- You Z
- Yu D
- Yu I
- Yu PR
- Yu SS
- Yuan L
- Yuan S
- Yuldashev BS
- Yumiceva F
- Yusuff I
- Zabi A
- Zacharopoulou A
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli AG
- Zeid SA
- Zeinali M
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang W
- Zhang Y
- Zhang Y
- Zhao J
- Zhizhin I
- Zhokin A
- Zhu RY
- Ziemons T
- Zimermmane Castro Santos A
- Zipper N
- Zisopoulos I
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zotto P
- Zotz A
- Zou R
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez Fernández A
- Özçelik Ö
- Publication venue
- Springer Nature on behalf of SISSA
- Publication date
- 09/10/2022
- Field of study
A preprint version of the article is available at arXiv:2206.09466v2 [hep-ex], https://arxiv.org/abs/2206.09466v2 . Comments: Replaced with the published version. Added the journal reference and the DOI. All the figures and tables can be found at httpS://cms-results.web.cern.ch/cms-results/public-results/publications/HIG-20-013 (CMS Public Pages). Report number: CMS-HIG-20-013, CERN-EP-2022-120.Production cross sections of the standard model Higgs boson decaying to a pair of W bosons are measured in proton-proton collisions at a center-of-mass energy of 13 TeV. The analysis targets Higgs bosons produced via gluon fusion, vector boson fusion, and in association with a W or Z boson. Candidate events are required to have at least two charged leptons and moderate missing transverse momentum, targeting events with at least one leptonically decaying W boson originating from the Higgs boson. Results are presented in the form of inclusive and differential cross sections in the simplified template cross section framework, as well as couplings of the Higgs boson to vector bosons and fermions. The data set collected by the CMS detector during 2016-2018 is used, corresponding to an integrated luminosity of 138 fb^−1. The signal strength modifier μ, defined as the ratio of the observed production rate in a given decay channel to the standard model expectation, is measured to be μ = 0.95 +0.10−0.09. All results are found to be compatible with the standard model within the uncertainties.SCOAP3
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