81 research outputs found
Combining ability of sugarcane genotypes based on the selection rates of single cross families
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- 'FapUNIFESP (SciELO)'
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Fatores associados à vulnerabilidade de idosos vivendo com HIV/AIDS em Belo Horizonte (MG), Brasil
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- Alencar RA
- Attride-Stirling J
- Ayres JRCM
- Ayres JRCM
- Ayres JRCM
- Barbosa ASM
- Barbosa RM
- Bastos FI
- Bastos FI
- Bertoncini BZ
- Brasileiro M
- Buchalla CM
- Caldas JMP
- Cardoso GP
- Cerqueira MBR
- Cerqueira MBR
- Chepngeno-Langat G
- Cooperman NA
- Costa RG
- Cunha JVQ
- Delor F
- Diniz NMF
- Emlet CA
- Felismino HP
- Fontanella BJB
- Gross JB
- Guimarães CD
- Knauth D
- Laurentino NRS
- Lazzarotto AR
- Levy BR
- Lisboa MES
- Mack K
- Maes CA
- Mann J
- Marília Borborema Rodrigues Cerqueira
- Minayo MCS
- Oliveira ICV
- Oliveira VM
- Olivi M
- Paiva V
- Paiva V
- Parker R
- Parker R
- Patton MQ
- Peters E
- Pottes FA
- Pratt G
- Rezende MCM
- Roberto Nascimento Rodrigues
- Rodrigues NO
- Saldanha AAW
- Sankar A
- Santos NJS
- Silva J
- Turato ER
- Vasconcelos D
- Villela W
- Weiss RS
- Zornitta M
- Publication venue
- 'FapUNIFESP (SciELO)'
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Pré-hipertensão, hipertensão arterial e fatores associados em pacientes odontológicos: estudo transversal na cidade de Santa Maria-RS, Brasil
- Author
- Al-Zahrani MS
- Amer NM
- Barbosa JB
- Bastos-Barbosa RG
- Castro RA
- Chida Y
- Chobanian AV
- Cipullo JP
- Coleman A
- de Gusmão JL
- Espinosa García J
- Fernández-Feijoo J
- Gillespie CD
- Glick M
- Godoy-Matos AF
- Guo F
- Guo X
- Hogan J
- Jardim PCBV
- Jontell M
- Kirkwood BR
- Laurence B
- Lewington S
- Li S
- Little JW
- Morisky DE
- Osterberg L
- Rezende FAC
- Rosário TM
- Silva DAS
- Sipahi I
- Zattar LC
- Zyoud SH
- Publication venue
- 'FapUNIFESP (SciELO)'
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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
- Acharya H
- Acharya S
- Acosta D
- Adam W
- Adamidis K
- Adams E
- Adams MR
- Adams T
- Addesa FM
- Adloff C
- Adzic P
- Aebi D
- Afanasiev S
- Agapitos A
- Agarwal G
- Agram J-L
- Aguilar-Benitez M
- Agyel D
- Ahmad A
- Ahmad M
- Ahmed A
- Aimè C
- Ajmal S
- Akchurin N
- Akgun B
- Akpinar A
- Al Kadhim A
- Albert A
- Albrecht A
- Albrecht S
- Albrow M
- Alcaraz Maestre J
- Alcerro Alcerro LF
- Aldaya Martin M
- Aldá Júnior WL
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Allmond B
- Ally D
- Almond J
- Alpana A
- Alsufyani B
- Alvarez Gonzalez B
- Alves Gallo Pereira M
- Alves GA
- Aly R
- Alyari M
- Amapane N
- Ambrozas M
- Ameen MM
- Amendola C
- Amoroso S
- Amram O
- Amsler C
- An S
- An Y
- Anagnostou G
- Andrea J
- Andreev V
- Andreev Y
- Andrejkovic JW
- Andrews MB
- Androsov K
- Anguiano J
- Antchev G
- Anthony D
- Antonello M
- Apollinari G
- Apparu D
- Appelt E
- Apresyan A
- Araujo M
- Aravind A
- Arcaro D
- Arcidiacono R
- Ardino R
- Argiro S
- Arneodo M
- Aruta C
- Asawatangtrakuldee C
- Asenov P
- Asghar MI
- Asilar E
- Askew A
- Assiouras 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
- Aydilek O
- Azarkin M
- Aziz T
- Azzi P
- Azzurri P
- Baarmand MM
- Babaev A
- Babbar J
- Bacchetta N
- Bachtis M
- Backhaus M
- Baden A
- Baechler J
- Bagliesi G
- Bahinipati S
- Bainbridge R
- Bak G
- Bakas G
- Bakhshiansohi H
- Bakshi AS
- Bala A
- Baldenegro Barrera C
- Ball AH
- Ban Y
- Band R
- Bandyopadhyay H
- Banerjee S
- Banerjee S
- Bansal S
- Baradia S
- Barbagli G
- Barberis E
- Barbosa Trujillo DA
- Bardelli G
- Bargassa P
- Baringer P
- Barman S
- Barnes VE
- Barney D
- Baron O
- Barria P
- Barroso Ferreira Filho M
- Bartek R
- Bartosik N
- Bartók M
- Barzdukas A
- Basnet A
- Bastos D
- Battilana C
- Baty A
- Bauer G
- Bauerdick LAT
- Bautista I
- Baxter S
- Bayatmakou M
- Bean A
- Beauceron S
- Beaudette F
- Becerril Gonzalez H
- Bedoya CF
- Behera PK
- Behera SC
- Behnke O
- Bein S
- Beirão Da Cruz E Silva C
- Belforte S
- Bell KW
- Bellan R
- Belloni A
- Bellora A
- Belvedere A
- Belyaev A
- Belyaev A
- Benaglia A
- Benato L
- Bencze G
- Bendavid J
- Benecke A
- Benelli G
- Benitez JF
- Bennett C
- Benussi L
- Bergauer T
- Beri SB
- Bermúdez Martínez A
- Bernardes CA
- Berry D
- Berryhill J
- Besancon M
- Bestintzanos I
- Bethani A
- Bevilacqua T
- Beyrouthy T
- Bhardwaj A
- Bharthuar S
- Bhat PC
- Bhatnagar V
- Bhattacharya R
- Bhattacharya S
- Bhattacharya S
- Bhattacharya S
- Bhowmik D
- Bhowmik S
- Bhyun JH
- Bialkowska H
- Bianchini L
- Bianco M
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- Biino C
- Bilei GM
- Bilin B
- Bin Anuar AA
- Bin Norjoharuddeen N
- Bisello D
- Black K
- Blanco Fernández S
- Blancon B
- Blekman F
- Blend D
- Blinov V
- Bloch D
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Boccali T
- Bocci A
- Bodek A
- Boimska B
- Boldrini G
- Boletti A
- Bols ES
- Bonacorsi D
- Bonanomi M
- Bonilla J
- Boos E
- Boran F
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- Bornheim A
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- Borshch V
- Bortignon P
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- Botta C
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- Bouchamaoui H
- Boudoul G
- Bouhali O
- Bourilkov D
- Bower N
- Boyaryntsev A
- Bozzo M
- Bragagnolo A
- Braghieri A
- Brainerd C
- Brandao Malbouisson H
- Branson JG
- Breedon R
- Brennan L
- Brew C
- Bright-Thonney S
- Brigljevic V
- Brinkerhoff A
- Brivio F
- Brochero Cifuentes JA
- Brom J-M
- Brommer S
- Brondolin E
- Brooke JJ
- Brown CE
- Brown RM
- Brunner D
- Bruno G
- Bruschini D
- Bryant P
- Bryson M
- Brzhechko D
- Brücken E
- Bubanja I
- Bucci R
- Buchmuller O
- Buchot Perraguin A
- Budkouski D
- Bueghly J
- Bundock A
- Bunichev V
- Bunkowski K
- Buontempo S
- Burkart M
- Burkett K
- Bury F
- Busson P
- Busza W
- Butalla S
- Butler JN
- Butler PH
- Butz E
- Bylsma B
- Bärtschi P
- Cabrera A
- Cabrillo IJ
- Cacchio V
- Cadamuro L
- Cagnotta A
- Caillol C
- Cakir A
- Calandri A
- Calderon De La Barca Sanchez M
- Calderon A
- Cali IA
- Calligaris L
- Calzaferri S
- Camaiani B
- Caminada L
- Campagnari C
- Campana M
- Campanini R
- Campbell A
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- Candelise V
- Canelli MF
- Canepa A
- Cankocak K
- Capiluppi P
- Cappati A
- Caputo C
- Caraway B
- Cardini A
- Cardwell B
- Carlin R
- Carnahan T
- Carnevali F
- Carrera Jarrin E
- Carrigan M
- Carrillo Montoya CA
- Cartiglia N
- Carvalho W
- Casarsa M
- Cassese A
- Castaldi R
- Castaneda Hernandez A
- Castells S
- Castilla-Valdez H
- Castro A
- Cavallari F
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- Chatterjee RM
- Chatterjee S
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- Chatzistavrou T
- Chaudhary G
- Chauhan S
- Chawla R
- Checchia P
- Chekhovsky V
- Chen GM
- Chen HS
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- Chen X
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- Chen Z
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- Chenarani S
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- Cherepanov V
- Chernyavskaya N
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- Chlebana F
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- Christoforou K
- Chudasama R
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- Ciangottini D
- Ciocci MA
- Cipriani M
- Citron M
- Cittolin S
- Ciulli V
- Civinini C
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- Colaleo A
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- Cranshaw DJ
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- Crossman B
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- Dabrowski A
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- Das I
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- Datta A
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- Dauncey P
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- De Bruyn I
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- De Iorio A
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- De Wit A
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- Delgado Peris A
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- Della Negra M
- Della Ricca G
- Demaria N
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- Dharmaratna WGD
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- Dissertori G
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- Dordevic M
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- Dreimanis K
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- Encinas Acosta HA
- Engelke F
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- Erbacher R
- Erdmann M
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- Erice C
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- Escalante Del Valle A
- Escobar Franco R
- Eskut E
- Estevez Banos LI
- Etesami SM
- Eusebi R
- Evangelou I
- Evdokimov O
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- Eysermans J
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- Kasieczka G
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- Kharchilava A
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- Khukhunaishvili A
- Khurana R
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- Yan F
- Yan X
- Yang H
- Yang S
- Yang TJ
- Yang UK
- Yang Y
- Yang YC
- Yao Y
- Yarar H
- Yates BR
- Yazgan E
- Ye Z
- Yi K
- Yi R
- Yigitbasi E
- Yockey H
- Yohay R
- Yoo HD
- Yoo J
- Yoo J
- Yoon I
- You Z
- Yu D
- Yu I
- Yu SS
- Yuan L
- Yuan S
- Yuldashev BS
- Yusuff I
- Zabi A
- Zabolotny W
- Zacharopoulou A
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zaza A
- Zecchinelli AG
- Zehetner P
- Zeinali M
- Zejdl P
- Zeuner WD
- 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 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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- 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
- 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
- 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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Measurement of the Higgs boson production via vector boson fusion and its decay into bottom quarks in proton-proton collisions at s = 13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
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- Yates BR
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- Yigitbasi E
- Yockey H
- Yohay R
- Yoo HD
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- Yu D
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- Yumiceva F
- Yusuff I
- Zabi A
- Zacharopoulou A
- Zaleski S
- Zalewski P
- Zarubin A
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- Zaza A
- Zecchinelli AG
- Zehetner P
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- Zejdl P
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
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- Zhokin A
- Zhu RY
- Ziemons T
- Zilizi G
- Zimermmane Castro Santos A
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- Zisopoulos I
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
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- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Publication venue
- Springer Nature on behalf of SISSA
- Publication date
- 30/01/2024
- Field of study
A preprint version of the article is available at arXiv:2308.01253v2 [hep-ex], https://arxiv.org/abs/2308.01253v2 . 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-22-009 (CMS Public Pages). Report number: CMS-HIG-22-009, CERN-EP-2023-110.A measurement of the Higgs boson (H) production via vector boson fusion (VBF) and its decay into a bottom quark-antiquark pair (bb¯) is presented using proton-proton collision data recorded by the CMS experiment at s√ = 13 TeV and corresponding to an integrated luminosity of 90.8 fb−1. Treating the gluon-gluon fusion process as a background and constraining its rate to the value expected in the standard model (SM) within uncertainties, the signal strength of the VBF process, defined as the ratio of the observed signal rate to that predicted by the SM, is measured to be μqqHHbb¯ = 1.01 +0.55−0.46. The VBF signal is observed with a significance of 2.4 standard deviations relative to the background prediction, while the expected significance is 2.7 standard deviations. Considering inclusive Higgs boson production and decay into bottom quarks, the signal strength is measured to be μincl.Hbb¯ = 0.99 +0.48−0.41, corresponding to an observed (expected) significance of 2.6 (2.9) standard deviations.SCOAP3, STFC; Marie-Curie program and the European Research Council and Horizon 2020 Gran
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- Author
- Aarrestad TK
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- You Z
- Yu D
- Yu I
- Yu SS
- Yuan L
- Yuan S
- Yuldashev BS
- Yusuff I
- Zabi A
- Zabolotny W
- Zacharopoulou A
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zaza A
- Zecchinelli AG
- Zehetner P
- Zeinali M
- Zejdl P
- Zeuner WD
- 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
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Publication venue
- Elsevier
- Publication date
- 02/02/2024
- 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” available online at: https://cms-docdb.cern.ch/cgi-bin/PublicDocDB/RetrieveFile?docid=6032&filename=CMSDataPolicyV1.2.pdf&version=2 .A preprint of this article is available online at arXiv:2311.03261v2 [hep-ex] https://arxiv.org/abs/2311.03261v2 . 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/TOP-22-010 (CMS Public Pages)A search is presented for new Higgs bosons in proton-proton (pp) collision events in which a same-sign top quark pair is produced in association with a jet, via the pp → tH/A → tt¯c and pp → tH/A → tt¯u processes. Here, H and A represent the extra scalar and pseudoscalar boson, respectively, of the second Higgs doublet in the generalized two-Higgs-doublet model (g2HDM). The search is based on pp collision data collected at a center-of-mass energy of 13 TeV with the CMS detector at the LHC, corresponding to an integrated luminosity of 138 fb−1. Final states with a same-sign lepton pair in association with jets and missing transverse momentum are considered. New Higgs bosons in the 200-1000 GeV mass range and new Yukawa couplings between 0.1 and 1.0 are targeted in the search, for scenarios in which either H or A appear alone, or in which they coexist and interfere. No significant excess above the standard model prediction is observed. Exclusion limits are derived in the context of the g2HDM.SCOAP3
Recommended from our members
Measurement of inclusive and differential cross sections for single top quark production in association with a W boson in proton-proton collisions at s = 13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
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- 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
- 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
- Publication venue
- Springer Nature
- Publication date
- 06/11/2022
- Field of study
A preprint version of the article is available at arXiv:2208.00924v2 [hep-ex], https://arxiv.org/abs/2208.00924v2 . 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/TOP-21-010 (CMS Public Pages). Report number: CMS-TOP-21-010, CERN-EP-2022-158.Measurements of the inclusive and normalised differential cross sections are presented for the production of single top quarks in association with a W boson in proton-proton collisions at a centre-of-mass energy of 13 TeV. The data used were recorded with the CMS detector at the LHC during 2016-2018, and correspond to an integrated luminosity of 138 fb^{−1}. Events containing one electron and one muon in the final state are analysed. For the inclusive measurement, a multivariate discriminant, exploiting the kinematic properties of the events is used to separate the signal from the dominant tt¯ background. A cross section of 79.2 ± 0.9 (stat) +7.7−8.0 (syst) ± 1.2 (lumi) pb is obtained, consistent with the predictions of the standard model. For the differential measurements, a fiducial region is defined according to the detector acceptance, and the requirement of exactly one jet coming from the fragmentation of a bottom quark. The resulting distributions are unfolded to particle level and agree with the predictions at next-to-leading order in perturbative quantum chromodynamics.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
- Author
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- 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
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- 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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- Author
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- Aarup Petersen H
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- 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
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Publication venue
- American Physical Society (APS)
- Publication date
- 14/08/2024
- Field of study
A preprint version of this article is available at arXiv:2402.13864v2 [hep-ex], https://arxiv.org/abs/2402.13864 . 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/SMP-22-015 (CMS Public Pages). Report number: CMS-SMP-22-015, CERN-EP-2024-010 .Energy correlators that describe energy-weighted distances between two or three particles in a hadronic jet are measured using an event sample of √ = 13 TeV proton-proton collisions collected by the CMS experiment and corresponding to an integrated luminosity of 36.3 fb^−1. The measured distributions are consistent with the trends in the simulation that reveal two key features of the strong interaction: confinement and asymptotic freedom. By comparing the ratio of the measured three- and two-particle energy correlator distributions with theoretical calculations that resum collinear emissions at approximate next-to-next-to-leading-logarithmic accuracy matched to a next-to-leading-order calculation, the strong coupling is determined at the boson mass: () = 0.1229+0.0040 −0.0050, the most precise () value obtained using jet substructure observables.SCOAP3
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