94 research outputs found
Host status of progenies of yellow passion fruit to Meloidogyne incognita race 2
- Author
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Systematic meta-analyses and field synopsis of genetic association studies of violence and aggression
- Author
- A Caspi
- A Caspi
- A Fresan
- A Johansson
- A Reif
- A Taylor
- CB Begg
- CJ Ferguson
- CJ Ferguson
- D A Collier
- D Moher
- DA Anderson
- DM Dick
- DR Miles
- E Baca-Garcia
- E Vassos
- E Verona
- EE Eichler
- EG Krug
- EL Kinnally
- FK Kavvoura
- G Frazzetto
- IW Craig
- J Evans
- J McGuire
- J Volavka
- JH Beitchman
- JP Higgins
- JP Higgins
- JP Ioannidis
- JP Ioannidis
- JP Ioannidis
- JP Ioannidis
- K Thorlund
- KM Beaver
- KW Nilsson
- LJ Siever
- M Egger
- M Fava
- M Goodman
- MH de Moor
- N Perroud
- N Weder
- NC Allen
- P Macaskill
- PM Visscher
- R DerSimonian
- RD Oades
- RJ Davidson
- RJ Nelson
- RL Sjoberg
- RM Harbord
- S Fazel
- S Hohmann
- S Wagner
- S Zammit
- SJ Morse
- SR Kay
- TE Moffitt
- W Bernet
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 02/04/2013
- Field of study
A large number of candidate gene studies for aggression and violence have been conducted. Successful identification of associations between genetic markers and aggression would contribute to understanding the neurobiology of antisocial behavior and potentially provide useful tools for risk prediction and therapeutic targets for high-risk groups of patients and offenders. We systematically reviewed the literature and assessed the evidence on genetic association studies of aggression and related outcomes in order to provide a field synopsis. We searched PubMed and Huge Navigator databases and sought additional data through reviewing reference lists and correspondence with investigators. Genetic association studies were included if outcome data on aggression or violent behavior either as a binary outcome or as a quantitative trait were provided. From 1331 potentially relevant investigations, 185 studies constituting 277 independent associations on 31 genes fulfilled the predetermined selection criteria. Data from variants investigated in three or more samples were combined in meta-analyses and potential sources of heterogeneity were investigated using subgroup analyses. In the primary analyses, which used relaxed inclusion criteria, we found no association between any polymorphism analyzed and aggression at the 5% level of significance. Subgroup analyses, including by severity of outcome, age group, characteristics of the sample and ethnicity, did not demonstrate any consistent findings. Current evidence does not support the use of such genes to predict dangerousness or as markers for therapeutic interventions
Facial-muscle weakness, speech disorders and dysphagia are common in patients with classic infantile Pompe disease treated with enzyme therapy
- Author
- A Amalfitano
- A Chakrapani
- A. J. J. Reuser
- A. T. van der Ploeg
- AG Bijvoet
- AT Ploeg Van der
- B. J. Ebbink
- C. I. van Capelle
- C. M. van Gelder
- CI Capelle Van
- CW Muller
- DJ Begley
- EF Rudnick
- EL Mancall
- FL Darley
- FL Darley
- H Hout Van den
- H Kobayashi
- H. H. W. de Gier
- HM Hout Van den
- I Sakurai
- I. F. M. de Coo
- I. Moor-van Nugteren
- J. M. P. van den Hout
- JC Pompe
- JF Hoh
- JJ Martin
- JJ Sciote
- JM Hout Van den
- L Klinge
- L Klinge
- M Nicolino
- M. M. Hakkesteegt
- MR Drost
- N Raben
- NW Slingerland
- P Gambetti
- P. A. van Doorn
- PS Kishnani
- PS Kishnani
- PS Kishnani
- PS Kishnani
- R Hirschhorn
- RD Kent
- SE Langmore
- SE Langmore
- V Dubowitz
- Publication venue
- Springer Netherlands
- Publication date
- 01/01/2011
- Field of study
Classic infantile Pompe disease is an inherited generalized glycogen storage disorder caused by deficiency of lysosomal acid α-glucosidase. If left untreated, patients die before one year of age. Although enzyme-replacement therapy (ERT) has significantly prolonged lifespan, it has also revealed new aspects of the disease. For up to 11 years, we investigated the frequency and consequences of facial-muscle weakness, speech disorders and dysphagia in long-term survivors. Sequential photographs were used to determine the timing and severity of facial-muscle weakness. Using standardized articulation tests and fibreoptic endoscopic evaluation of swallowing, we investigated speech and swallowing function in a subset of patients. This study included 11 patients with classic infantile Pompe disease. Median age at the start of ERT was 2.4 months (range 0.1-8.3 months), and median age at the end of the study was 4.3 years (range 7.7 months −12.2 years). All patients developed facial-muscle weakness before the age of 15 months. Speech was studied in four patients. Articulation was disordered, with hypernasal resonance and reduced speech intelligibility in all four. Swallowing function was studied in six patients, the most important findings being ineffective swallowing with residues of food (5/6), penetration or aspiration (3/6), and reduced pharyngeal and/or laryngeal sensibility (2/6). We conclude that facial-muscle weakness, speech disorders and dysphagia are common in long-term survivors receiving ERT for classic infantile Pompe disease. To improve speech and reduce the risk for aspiration, early treatment by a speech therapist and regular swallowing assessments are recommended
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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
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
- 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
- Agram J-L
- Aguilar-Benitez M
- Agyel D
- Ahmad A
- Ahmad M
- Ahmed A
- Aimè C
- Akchurin N
- Akgun B
- Akpinar A
- Al-Mashad MA
- 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
- Almond J
- Alpana A
- 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
- Andreev V
- Andreev Y
- Andrejkovic JW
- Andrews MB
- Androsov K
- Anguiano J
- Antchev G
- Anthony D
- Antonello M
- Antunovic Z
- Apollinari G
- Apparu D
- Appelt E
- Apresyan A
- Araujo M
- Arcaro D
- Arcidiacono R
- Argiro S
- Arneodo M
- Aruta C
- Asawatangtrakuldee C
- Asenov P
- Asghar MI
- Asilar E
- Askew A
- Asmuss P
- 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
- Bagaturia I
- Bagliesi G
- Bahinipati S
- Baillon P
- Bainbridge R
- Bakas G
- Bakhshiansohi H
- Bakshi AS
- 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
- Bargassa P
- Baringer P
- Barman S
- Barnes VE
- Barney D
- Baron O
- Barria P
- Barroso Ferreira Filho M
- Barroso AV
- Bartek R
- Bartosik N
- Bartók M
- Bastos D
- Battilana C
- Baty A
- Bauer G
- Bauerdick LAT
- Baxter S
- Bayatmakou M
- Bean A
- Beauceron S
- Beaudette F
- Becerril Gonzalez H
- Bechtel J
- Bedoya CF
- Behera PK
- Behera SC
- Behnke O
- Bein S
- Belforte S
- Bell KW
- Bellan R
- Belloni A
- Bellora A
- Belyaev A
- Belyaev A
- Benaglia A
- Benato L
- Bencze G
- Bendavid J
- Benecke A
- Benelli G
- Beni N
- Benitez JF
- Benussi L
- Bergauer T
- Berger P
- Beri SB
- Bermúdez Martínez A
- Bernardes CA
- Bernet C
- Berry D
- Berryhill J
- Bertacchi V
- Besancon M
- Bestintzanos I
- Bethani A
- Beyrouthy T
- Bhal E
- 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
- Bianco S
- Biasotto M
- Biino C
- Bilei GM
- Bilin B
- Bin Anuar AA
- Bin Norjoharuddeen N
- Bisello D
- Black K
- Blancon B
- Blekman F
- 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
- Bonomally S
- Boos E
- Boran F
- Borg J
- Borgonovi L
- Bornheim A
- Borras K
- 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
- Branson JG
- Breedon R
- Breeze S
- Brew C
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- Brigliadori L
- Brigljevic V
- Brinkerhoff A
- Brivio F
- Brochero Cifuentes JA
- Brom J-M
- Brommer S
- Brondolin E
- Brooke JJ
- Brown CE
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- Brunner D
- Bruno G
- Bruschini D
- Bryant P
- Bryson M
- Brzhechko D
- Brücken E
- Bubanja I
- Bucci R
- Buccilli A
- Buchmuller O
- Buchot Perraguin A
- Budkouski D
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- Bundock A
- Bunichev V
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- Buontempo S
- Burgo RD
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- Calderon De La Barca Sanchez M
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- Calzaferri S
- Camaiani B
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- Candelise V
- Canelli MF
- Canepa A
- Cankocak K
- Capiluppi P
- Cappati A
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- Carvalho Antunes De Oliveira A
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- Casarsa M
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- Cassese A
- Castaldi R
- Castaneda Hernandez A
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- Castilla-Valdez H
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- Cepaitis V
- Cepeda M
- Cerati GB
- Cerci S
- Cerminara G
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- Cerri O
- Cetorelli F
- Chabert EC
- Chahal GS
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- Charlot C
- Chatagnon P
- Chatterjee RM
- Chatterjee S
- Chatzistavrou T
- Chaudhary G
- Chauhan S
- Chawla R
- Checchia P
- Chekhovsky V
- Chen C
- Chen GM
- Chen HS
- Chen KF
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- Chen Z
- Chenarani S
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- Cherepanov V
- Chernyavskaya N
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- Cheung HWK
- Chhibra SS
- Chiarito B
- Chinellato J
- Chistov R
- Chitroda BK
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- Chou JP
- Choudhary BC
- Choudhury S
- Christoforou K
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- Ciangottini D
- Ciocci MA
- Cipriani M
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- Cittolin S
- Ciulli V
- Civinini C
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- Covarelli R
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- Creanza D
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- Cremonesi M
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- de Monchenault GH
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- De Palma M
- De Roeck A
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- De Souza SF
- de Trocóniz JF
- De Wit A
- Decaro M
- Defranchis MM
- Deile M
- Dejardin M
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- Delaere C
- Delannoy AG
- Delcourt M
- Delgado Peris A
- Delgado A
- Della Negra M
- Della Ricca G
- Dell’Orso R
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- Demina R
- Demiragli Z
- Demiroglu ZS
- Denegri D
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- Dermenev A
- Dewanjee RK
- Dezoort G
- Dharmaratna WGD
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- Diamantopoulou M
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- Didukh L
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- Diotalevi T
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- Donegà M
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- Dubinin M
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- Dugad S
- Dulemba JL
- Dumanoglu I
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- Duric S
- Durkin LS
- Dutta I
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- Dziwok C
- Dünser M
- D’Alessandro R
- D’Alfonso M
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- d’Enterria D
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- Ecklund KM
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- Elkafrawy T
- Elliott-Peisert A
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- Elmetenawee W
- Elvira VD
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- Encinas Acosta HA
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- Epshteyn V
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- Erdmann M
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- Erice C
- Errico F
- Escalante Del Valle A
- Eskut E
- Estevez Banos LI
- Etesami SM
- Eusebi R
- Evangelou I
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- Evdokimov O
- Everaerts P
- Eysermans J
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- Fernandez M
- Fernández Del Val D
- Fernández Manteca PJ
- Ferri F
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- Field RD
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- Fiorina D
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- Gutiérrez GR
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- Hadjiiska R
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- Hauser J
- Havukainen J
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- Heikkilä JK
- Heindl M
- Heintz U
- Heller R
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- Heredia-De La Cruz I
- Hernandez JM
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- Higginbotham S
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- Hinzmann A
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- Horzela M
- Hos I
- Hou W-S
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- Huang T
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- Husemann U
- Hussain PS
- Huwiler M
- Iaselli G
- Iashvili I
- Iaydjiev P
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- Ignatenko M
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- Incandela J
- Ince M
- Ingram Q
- Innocente V
- Iorio AOM
- Iqbal MA
- Isidori T
- Isik C
- Isildak B
- Ivanchenko V
- Ivanov A
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- Ivanov Y
- Ivone F
- Jabeen S
- Jabusch HR
- Jafari A
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- James T
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- Jaroslawski D
- Jarrin EC
- Jarry P
- Javaid T
- Jayananda MK
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- Jeon S
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- Jiang CH
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- 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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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
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- Yumiceva F
- Yusuff I
- Zabi A
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- Zoi I
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- Zotto P
- Zotz A
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- 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
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- 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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Evidence for tWZ production in proton-proton collisions at √s=13 TeV in multilepton final states
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- Zalewski P
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- Zehetner P
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- Ziemons T
- Zilizi G
- Zimermmane Castro Santos A
- Zipper N
- Zisopoulos I
- Zoi I
- Zolkapli Z
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- Zorbilmez C
- Zotto P
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- Zou R
- Zucchetta A
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- 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
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
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- 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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Search for new Higgs bosons via same-sign top quark pair production in association with a jet in proton-proton collisions at √s = 13 TeV
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- Vourliotis E
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- Vámi TÁ
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- Walkingshaw Pass K
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- Wyslouch B
- Würthwein F
- Xiang Y
- Xiao J
- Xiao M
- Xie S
- Xie W
- Yagil A
- Yalvac M
- Yan F
- Yan X
- Yanes E
- 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
- 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
Search for Higgs boson decays to a Z boson and a photon in proton-proton collisions at s = 13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
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- 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
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- Watson IJ
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- Webb SN
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- Wei K
- Wen Y
- Wertz S
- West C
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- Whitbeck A
- White R
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- Wichmann K
- Wickramage N
- Wickramarathna DDC
- Wiedenbeck S
- Wieland S
- Wiens L
- Wightman A
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- 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
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- Wuchterl S
- Wulz C-E
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- 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
- Zahid S
- 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
- 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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