234 research outputs found
‘It used to be brutal, now it’s an art’:changing negotiations of violence and masculinity in British karate
- Author
- A Channon
- A Channon
- A Hochschild
- A Meo
- AM Klein
- B Kidd
- B Pini
- C MacLean
- C MacLean
- C Matthews
- C Mennesson
- C Wang
- D Whitson
- DC Spencer
- DC Spencer
- E Anderson
- E Anderson
- E Dunning
- E McDonagh
- H Noel
- I Wellard
- J Allen-Collinson
- J Hargreaves
- J Laurendeau
- K Woodward
- K Young
- L Wacquant
- M Gard
- M Padfield
- MA Messner
- MJ McNaughton
- MS Kimmel
- N Elias
- P Bourdieu
- R Pringle
- RS Garcia
- RW Connell
- RW Connell
- S Pink
- S Raven
- S Schacht
- SE Hatty
- TJ Curry
- Publication venue
- Publication date
- 20/09/2019
- Field of study
In most western (and indeed eastern) cultures, fighting is seen as an ultimate symbol of masculinity – an embodied display of dominance, control and violence (Bourdieu, 2001). As a space legitimising and praising performances of mimetic violence (Dunning, 1999), combat sports provide an arena where the virtues of dominance and power at the heart of conceptions of orthodox masculinity (Anderson, 2010 ) or hegemonic masculinity (Connell, 2005) can be symbolically presented by men through bodily displays of strength, physical aggression, and the taking and overcoming of pain (Bourdieu, 2001; Messner, 1990; Wacquant, 2004). Yet, over the last twenty years the focus of karate in Britain has been perceived to shift from aggressive acts of 'hitting hard' to developing and displaying controlled, acrobatic and technically precise movements. Drawn from a nine-month ethnography and 7 semi-structured interviews, this chapter explores how British male karate practitioners re/negotiate ideas of masculinity and embodiments of a masculine identity in the context of karate’s changing emphasis on, and practices of, 'violence'. This paper suggests that a 'civilising' shift (Elias and Dunning, 1986) in the competition rules increases in women’s participation in karate with men, and subsequent negotiations of mimetic violence, complicate the use of violence as a symbol of praised masculine identity within British karate . A praised masculine identity is crafted by carefully blending traits conventional deemed feminine such as technical precision, elegance and agility alongside displays of strength and dominance. Such performances challenge conceptions of an orthodox sporting masculinity and notions of hierarchical gender distinction
Detection and quantitation of copy number variation in the voltage-gated sodium channel gene of the mosquito Culex quinquefasciatus
- Author
- A Kliot
- A Zmienko
- AJ Martins
- AM Puinean
- AM Waterhouse
- AO O’Reilly
- BS Assogba
- C Alkan
- C Berticat
- C Mouches
- CM Hindson
- CM Jones
- CS Clarkson
- CS Wilding
- CS Wondji
- D Weetman
- DH Kwon
- DS Buss
- EJ Remnant
- FA Kondrashov
- FA Kondrashov
- H Ranson
- JL Smith
- K Ichimori
- K Tamura
- L Djogbénou
- L Djogbénou
- LB Pinheiro
- LD Kramer
- LS Djogbénou
- M Clement
- M Coleman
- M Long
- M Olsson
- MEO Locke
- MJ Donnelly
- MS Williamson
- N Platt
- P Arensburger
- P Labbé
- P Labbé
- P Labbé
- PV Hickner
- Q Shang
- Q Xu
- T Tomita
- TGE Davies
- TWR Harrop
- V Corbel
- Y Bel
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 13/07/2017
- Field of study
Insecticide resistance is typically associated with alterations to the insecticidal target-site or with gene expression variation at loci involved in insecticide detoxification. In some species copy number variation (CNV) of target site loci (e.g. the Ace-1 target site of carbamate insecticides) or detoxification genes has been implicated in the resistance phenotype. We show that field-collected Ugandan
Culex quinquefasciatus display CNV for the voltage-gated sodium channel gene (Vgsc), target-site of pyrethroid and organochlorine insecticides. In order to develop field-applicable diagnostics for Vgsc
CN, and as a prelude to investigating the possible association of CN with insecticide resistance, three
assays were compared for their accuracy in CN estimation in this species. The gold standard method is
droplet digital PCR (ddPCR), however, the hardware is prohibitively expensive for widespread utility.
Here, ddPCR was compared to quantitative PCR (qPCR) and pyrosequencing. Across all platforms, CNV was detected in ≈10% of mosquitoes, corresponding to three or four copies (per diploid genome).
ddPCR and qPCR-Std-curve yielded similar predictions for Vgsc CN, indicating that the qPCR protocol developed here can be applied as a diagnostic assay, facilitating monitoring of Vgsc CN in wild populations and the elucidation of association between the Vgsc CN and insecticide resistance
Molecular mechanics applied to single-walled carbon nanotubes
- Author
- Agrawal PM
- Antonio Ferreira Ávila
- Belytschko T
- Dresselhaus MS
- Frankland SJV
- Guilherme Silveira Rachid Lacerda
- Hernandez E
- Huang MY
- Iijima S.
- Jin Y
- Kalamkarov AL
- Koloczek J
- Krishnan A
- Li C
- Li C
- Liu WK
- Liu WK
- Lourie O
- Lu J
- Lu JP.
- Lurie S
- Meo M
- Natsuki T
- Odegard GM
- Pantano A
- Popov VN
- Ruoff RS
- Saito R
- Salvetat-Delmont JP
- Sun X
- Tamma KK
- Tserpes KI
- Wang Y
- Xiao JR
- Yakobson BI
- Yu MF
- Zienkiewicz OC
- Ávila AF
- Ávila AF
- Ávila AF
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Asymptotic theory of time-varying social networks with heterogeneous activity and tie allocation
- Author
- A Barrat
- A Clauset
- A Moinet
- A Vázquez
- A-L Barabasi
- B Goncalves
- C Cattuto
- D Centola
- DZ Levin
- F Radicchi
- G Ghoshal
- G Kossinets
- G Laurent
- G Miritello
- H-H Jo
- J Holt-Lunstad
- J Saramäki
- J Saramäki
- J Stehlé
- J Stiller
- J-P Onnela
- JJ Brown
- JL Iribarren
- K Sun
- K-I Goh
- LE Rocha
- Lorenzo Isella
- M Granovetter
- M Karsai
- M Karsai
- M Karsai
- M Morris
- M Starnini
- M Starnini
- M Starnini
- MEJ Newman
- MEJ Newman
- MEJ Newman
- MEJ Newman
- MS Granovetter
- N Friedkin
- N Lin
- N Perra
- P Bourdieu
- P De Meo
- P Holme
- R Pfitzner
- RE Nelson
- RIM Dunbar
- S Boccaletti
- S Fortunato
- S Liu
- S-Y Liu
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 22/09/2015
- Field of study
The dynamic of social networks is driven by the interplay between diverse mechanisms that still challenge our theoretical and modelling efforts. Amongst them, two are known to play a central role in shaping the networks evolution, namely the heterogeneous propensity of individuals to i) be socially active and ii) establish a new social relationships with their alters. Here, we empirically characterise these two mechanisms in seven real networks describing temporal human interactions in three different settings: scientific collaborations, Twitter mentions, and mobile phone calls. We find that the individuals’ social activity and their strategy in choosing ties where to allocate their social interactions can be quantitatively described and encoded in a simple stochastic network modelling framework. The Master Equation of the model can be solved in the asymptotic limit. The analytical solutions provide an explicit description of both the system dynamic and the dynamical scaling laws characterising crucial aspects about the evolution of the networks. The analytical predictions match with accuracy the empirical observations, thus validating the theoretical approach. Our results provide a rigorous dynamical system framework that can be extended to include other processes shaping social dynamics and to generate data driven predictions for the asymptotic behaviour of social networks
The COGs (context, object, and goals) in multisensory processing
- Author
- A Alsius
- A Alsius
- A Alsius
- A Alsius
- A Alsius
- A Amedi
- A Baddeley
- A Finisguerra
- A Fort
- A Jones
- A Klapetek
- A Thelen
- A Thelen
- A Thillay
- A Vatakis
- A Walker-Andrews
- AA Ghazanfar
- AM Cravo
- AO Diaconescu
- AR Powers
- B Baier
- BA Rowland
- BE Stein
- BK Barakat
- BR Sarmiento
- C Cappe
- C Cappe
- C Cappe
- C Chandrasekaran
- C Kayser
- C Lunghi
- C Spence
- C Summerfield
- C Summerfield
- CA Sutherland
- CE Schroeder
- CE Schroeder
- CI Baker
- CJ Mondloch
- CL Folk
- CR Fetsch
- CV Parise
- CV Parise
- D Amso
- D Brang
- D Nardo
- D Sanabria
- D Senkowski
- D Talsma
- D Talsma
- D Talsma
- D Talsma
- DE Astle
- DJ Froyen
- DJ Lewkowicz
- DR Bach
- DS Barth
- E Barenholtz
- E Burg van der
- E Burg van der
- E Orchard-Mills
- E Orchard-Mills
- EM Zion Golumbic
- FC Rind
- G Musacchia
- G Scerif
- H McGurk
- I Holloway
- IC Fiebelkorn
- IC Fiebelkorn
- J Besle
- J Duncan
- J Heron
- J Tuomainen
- J Vroomen
- JJ Stekelenburg
- JT Coull
- JX Maier
- L Iordanescu
- L Naci
- L Spierer
- LH Arnal
- LM Fernández
- M Aller
- M Baart
- M Bar
- M Gori
- M Nardini
- M Nardini
- MA Meredith
- MA Meredith
- MH Giard
- Micah M. Murray
- MM Murray
- MM Murray
- MM Murray
- MS Beauchamp
- N Altieri
- N Atteveldt van
- N Atteveldt van
- N Atteveldt van
- N Bien
- N Ikumi
- N Lavie
- Nienke van Atteveldt
- NM Atteveldt van
- NM Atteveldt van
- O Doehrmann
- O Nahorna
- P Belin
- P Fries
- P Lakatos
- P Niemi
- PA Neil
- Pawel J. Matusz
- PJ Laurienti
- PJ Matusz
- PJ Matusz
- PJ Matusz
- PJ Matusz
- PJ Matusz
- PJ Matusz
- R Cecere
- R Cecere
- R De Meo
- R Desimone
- R Ee van
- R Frost
- R Martuzzi
- RA Stevenson
- RA Stevenson
- RA Stevenson
- RB Welch
- S Dehaene
- S Masterberdino
- S Molholm
- S Molholm
- S Soto-Faraco
- S ten Oever
- S ten Oever
- S Tyll
- S Werner
- S Werner
- S Yuval-Greenberg
- SA Los
- Salvador Soto-Faraco
- Sanne ten Oever
- SJ Luck
- SL Fairhall
- T Raij
- T Raij
- T Rohe
- TD Palmer
- TS Braver
- UR Beierholm
- V Romei
- V Romei
- V Romei
- V Romei
- V Santangelo
- V Santangelo
- V Wassenhove Van
- VA Lamme
- Vincenzo Romei
- W Fujisaki
- W Schiff
- WA Teder-Sälejärvi
- Y Ding
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Our understanding of how perception operates in real-world environments has been substantially advanced by studying both multisensory processes and “top-down” control processes influencing sensory processing via activity from higher-order brain areas, such as attention, memory, and expectations. As the two topics have been traditionally studied separately, the mechanisms orchestrating real-world multisensory processing remain unclear. Past work has revealed that the observer’s goals gate the influence of many multisensory processes on brain and behavioural responses, whereas some other multisensory processes might occur independently of these goals. Consequently, other forms of top-down control beyond goal dependence are necessary to explain the full range of multisensory effects currently reported at the brain and the cognitive level. These forms of control include sensitivity to stimulus context as well as the detection of matches (or lack thereof) between a multisensory stimulus and categorical attributes of naturalistic objects (e.g. tools, animals). In this review we discuss and integrate the existing findings that demonstrate the importance of such goal-, object- and context-based top-down control over multisensory processing. We then put forward a few principles emerging from this literature review with respect to the mechanisms underlying multisensory processing and discuss their possible broader implications
Search for dark matter produced in association with a single top quark or a top quark pair in proton-proton collisions at s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Al-Bataineh A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aleksandrov A
- Alexander J
- Alhusseini M
- Ali MAB Md
- Alimena J
- Allen B
- Almond J
- Alvarez Fernandez A
- Alvarez JD Ruiz
- Alverson G
- Alves FL
- Alves GA
- Alyari M
- Amapane N
- Ambrogi F
- Amendola C
- Amin N
- Amsler C
- Anagnostou G
- Anampa K Hurtado
- Anderson D
- Andrea J
- Andreev V
- Andreev Yu
- Andrews MB
- Androsov K
- Angioni L Pinna
- Antonelli L
- Antropov I
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Apyan A
- Araujo M
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arndt T
- Arneodo M
- Asavapibhop B
- Asawatangtrakuldee C
- Asghar MI
- Asilar E
- Askew A
- Assran Y
- Atakisi IO
- Ather MW
- Attikis A
- Auffray E
- Aushev T
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avila C
- Ayala E
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babaev A
- Babounikau I
- Bacchetta N
- Bachiller I
- Bachtis M
- Backhaus M
- Baden A
- Bagliesi G
- Bahinipati S
- Baidali S
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Ball AH
- Ball F
- Ban Y
- Band R
- Banerjee S
- Banerjee S
- Bani L
- Bansal S
- Barbagli G
- Barberis E
- Bargassa P
- Baringer P
- Barker A
- Barnes VE
- Barney D
- Barnyakov A
- Baron O
- Barone L
- Barria P
- Barrio Luna M
- Bartek R
- Barth C
- Bartok M
- Bartosik N
- Baselga M
- Baskakov A
- Bat A
- Battilana C
- Baty A
- Bauer G
- Bauerdick LAT
- Baur S
- Bayshev I
- Bean A
- Beauceron S
- Beaudette F
- Becerra DA Sanz
- Beernaert K
- Beghin D
- Behera PK
- Behnke O
- Behrens U
- Bein S
- Beirao Da Cruz E Silva C
- Belchior Batista Das Chagas E
- Belforte S
- Bell KW
- Bellan R
- Belloni A
- Belyaev A
- Belyaev A
- Benaglia A
- Benato L
- Bencze G
- Bendavid J
- Benecke A
- Benelli G
- Beni N
- Benitez JF
- Benussi L
- Benvenuti AC
- Beretvas A
- Bergauer T
- Berger P
- Beri SB
- Bernardes CA
- Bernet C
- Berry D
- Berryhill J
- Bertsche D
- Besancon M
- Beschi A
- Betts RR
- Bhandari R
- Bhardwaj A
- Bhardwaj R
- Bharti M
- Bhat MA
- Bhat PC
- Bhatnagar V
- Bhattacharya R
- Bhattacharya S
- Bhattacharya S
- Bhattacharya S
- Bhawandeep U
- Bheesette S
- Bhopatkar V
- Bhowmik D
- Bhowmik S
- Bi R
- Bialkowska H
- Bian JG
- Bianchini L
- Bianco M
- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilin B
- Bilki B
- Bin Anuar AA
- Bisello D
- Bitioukov S
- Blanco J Martin
- Blekman F
- Blinov V
- Blobel V
- Bloch D
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Boccali T
- Bocci A
- Bodek A
- Boimska B
- Boletti A
- Bonacorsi D
- Bondu O
- Boos E
- Boran F
- Boren S
- Borg J
- Borgonovi L
- Bornheim A
- Borras K
- Borrello L
- Bortignon P
- Bose T
- Botta C
- Botta V
- Boudoul G
- Bouhali O
- Bourilkov D
- Bouvier E
- Bowen J
- Bragagnolo A
- Braghieri A
- Braibant-Giacomelli S
- Brainerd C
- Brandstetter J
- Brandt S
- Branson JG
- Bravo C
- Breedon R
- Breeze S
- Brew C
- Brigljevic V
- Brinkerhoff A
- Brivio F
- Brochero Cifuentes JA
- Brochet S
- Brodski M
- Brom J-M
- Brondolin E
- Brooke JJ
- Brown RM
- Brun H
- Bruno G
- Brzhechko D
- Bucci R
- Buccilli A
- Buchanan J
- Buchmuller O
- Bueghly J
- Bundock A
- Bunin P
- Bunkowski K
- Buontempo S
- Burkett K
- Burns D
- Burns D
- Burt K
- Busson P
- Busza W
- Butler JN
- Butler PH
- Butz E
- Bylinkin A
- Bylsma B
- Byszuk A
- Cabrera A
- Cabrillo IJ
- Cadamuro L
- Caillol C
- Cakir A
- Calabria C
- Calderon A
- Cali IA
- Call K
- Calligaris L
- Caminada L
- Campagnari C
- Campanini R
- Campbell A
- Camporesi T
- Candelise V
- Canelli MF
- Canepa A
- Cankocak K
- Capiluppi P
- Cappati A
- Caputo C
- Carlin R
- Carlsmith D
- Carnes A
- Carrera Jarrin E
- Carrillo Montoya CA
- Carrillo Moreno S
- Cartiglia N
- Carvalho W
- Casarsa M
- Caspart R
- Castaldi R
- Castaneda Hernandez A
- Castilla-Valdez H
- Castle J
- Castro A
- Cavallari F
- Cavallo FR
- Cavallo N
- Cavanaugh R
- Ceballos G Gomez
- Cecchi C
- Celik A
- Cenna F
- Cepeda M
- Cerati GB
- Cerci D Sunar
- Cerci S
- Cerminara G
- Cerrada M
- Chabert EC
- Chadeeva M
- Chang P
- Chang P
- Chanon N
- Chao Y
- Chaparro Sierra LF
- Chapon E
- Charaf O
- Charlot C
- Chatterjee K
- Chatterjee RM
- Chatterjee S
- Chauhan S
- Chauhan S
- Chaves J
- Chawla R
- Chazin Quero B
- Checchia P
- Chekhovsky V
- Chen G
- Chen GM
- Chen HS
- Chen KF
- Chen M
- Chen PH
- Chen X
- Chen Y
- Chen Y
- Chen Z
- Chenarani S
- Cheng T
- Cheng Y
- Cherepanov V
- Chernyavskaya N
- Chertok M
- Cheung HWK
- Chhibra SS
- Chierici R
- Chinellato J
- Chlebana F
- Cho S
- Choi S
- Choi Y
- Chou JP
- Choudhary BC
- Choudhury S
- Chowdhury S Roy
- Chu J
- Chudasama R
- Chwalek T
- Ciangottini D
- Cieri D
- Ciocca C
- Ciocci MA
- Cipriani M
- Ciriolo V
- Cirkovic P
- Citron M
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clarida W
- Clement E
- Clerbaux B
- Cockerill DJA
- Cocoros A
- Codispoti G
- Coelho E
- Colafranceschi S
- Colaleo A
- Cole JE
- Colino N
- Collaboration CMS
- Collard C
- Colling D
- Colombo F
- Cometti S
- Connor P
- Contardo D
- Conte E
- Contreras-Campana C
- Conway J
- Conway R
- Cooper SI
- Cooperstein S
- Cornelis T
- Correia Silva G
- Cossutti F
- Costa M
- Coubez X
- Couderc F
- Coughlan JA
- Courbon B
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- Creanza D
- Cremonesi M
- Cristella L
- Csanad M
- Cucciati G
- Cuevas J
- Cuffiani M
- Cumalat JP
- Curry D
- Cussans D
- Cutts D
- Czellar S
- D'Alessandro R
- D'Alfonso M
- d'Enterria D
- D'Hondt J
- Da Costa EM
- Da Rold A
- Da Silveira GG
- Dabrowski A
- Daci N
- Dalchenko M
- Dall'Osso M
- Dallavalle GM
- Damarseckin S
- Damgov J
- Damiani D Dominguez
- Danilov V
- Daponte V
- Das P
- Das S
- Dasgupta A
- Daskalakis G
- Dasu S
- Datta A
- Dauncey P
- David A
- David P
- Davies G
- Davignon O
- de Barbaro P
- De Boer W
- De Bruyn I
- de Cassagnac R Granier
- De Clercq J
- De Cosa A
- de Fatis T Tabarelli
- De Filippis N
- De Guio F
- De Iorio A
- De Jesus Damiao D
- De La Cruz B
- De La Cruz-Burelo E
- De Lentdecker G
- De Lima R Teixeira
- De Mattia M
- de Monchenault G Hamel
- De Oliveira Martins C
- De Oliveira A Carvalho Antunes
- De Palma M
- De Roeck A
- de Troconiz JF
- De Wit A
- De Wolf EA
- Deelen N
- Defranchis MM
- Deiters K
- Dejardin M
- Del Burgo R
- Del Re D
- Del Valle A Escalante
- Delaere C
- Delannoy AG
- Delannoy H
- Delcourt M
- Delgado Peris A
- Delgado A
- Dell'Orso R
- Della Negra M
- Della Porta G Zevi
- Della Ricca G
- Demaria N
- Demina R
- Demiragli Z
- Demiroglu ZS
- Denegri D
- Depasse P
- Derdzinski M
- Dermenev A
- Deroover K
- Dev N
- Devetak D
- Dewanjee RK
- Dey S
- Dhingra N
- Di Crescenzo A
- Di Croce D
- Di Florio A
- Di Francesco A
- Di Guida S
- Di Marco E
- Di Maria R
- Di Mattia A
- Diemoz M
- Dierlamm A
- Dildick S
- Dilsiz K
- Dimitrov A
- Dimova T
- Dinardo ME
- Dissertori G
- Dittmann J
- Dittmar M
- Dittmer S
- Doan TH
- Dobson M
- Dobur D
- Dodd L
- Dolek F
- Dolen J
- Dominguez A
- Donato S
- Donega M
- Dordevic M
- Dorfer C
- Dorigo T
- Dorney B
- Doroba K
- Dosselli U
- Dozen C
- Dragicevic M
- Dremin I
- Dreyer T
- Duarte Campderros J
- Duarte J
- Dube S
- Dubinin M
- Duchardt D
- Dudenas V
- Dudero PR
- Dudko L
- Dugad S
- Duh YT
- Dulemba JL
- Dunser M
- Dupont N
- Duran-Osuna MC
- Durgut S
- Duric S
- Durkin LS
- Dutt S
- Dutta D
- Dutta S
- Dutta V
- Ebrahimi A
- Eckerlin G
- Ecklund KM
- Eerola P
- Ehataht K
- Eichhorn T
- El Mamouni H
- El Morabit K
- Elayavalli R Kunnawalkam
- Elgammal S
- Elliott-Peisert A
- Elmer P
- Elumakhov D
- Elvira VD
- Elwood A
- Eminizer N
- Eno SC
- Epshteyn V
- Erbacher R
- Erdmann M
- Erdmann W
- Erdweg S
- Eren E
- Erice C
- Eroe J
- Errico F
- Ershov A
- Esch T
- Eskut E
- Etesami SM
- Eusebi R
- Evangelou I
- Evans A
- Evdokimov O
- Everaerts P
- Eysermans J
- Fabbri F
- Fabbri F
- Fabozzi F
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search for dark matter produced in association with top quarks in proton-proton collisions at a center-of-mass energy of 13 TeV is presented. The data set used corresponds to an integrated luminosity of 35.9 fb(-1) recorded with the CMS detector at the LHC. Whereas previous searches for neutral scalar or pseudoscalar mediators considered dark matter production in association with a top quark pair only, this analysis also includes production modes with a single top quark. The results are derived from the combination of multiple selection categories that are defined to target either the single top quark or the top quark pair signature. No significant deviations with respect to the standard model predictions are observed. The results are interpreted in the context of a simplified model in which a scalar or pseudoscalar mediator particle couples to a top quark and subsequently decays into dark matter particles. Scalar and pseudoscalar mediator particles with masses below 290 and 300 GeV, respectively, are excluded at 95% confidence level, assuming a dark matter particle mass of 1 GeV and mediator couplings to fermions and dark matter particles equal to unity.Peer reviewe
Search for strongly interacting massive particles generating trackless jets in proton-proton collisions at s = 13 TeV
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- Zorbilmez C
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- Álvarez Fernández A
- Österberg K
- Özçelik Ö
- Široký J
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
A search for dark matter in the form of strongly interacting massive particles (SIMPs) using the CMS detector at the LHC is presented. The SIMPs would be produced in pairs that manifest themselves as pairs of jets without tracks. The energy fraction of jets carried by charged particles is used as a key discriminator to suppress efficiently the large multijet background, and the remaining background is estimated directly from data. The search is performed using proton-proton collision data corresponding to an integrated luminosity of 16.1 fb - 1 , collected with the CMS detector in 2016. No significant excess of events is observed above the expected background. For the simplified dark matter model under consideration, SIMPs with masses up to 100 GeV are excluded and further sensitivity is explored towards higher masses
Measurement of B_{s}^{0} meson production in pp and PbPb collisions at \sqrt{SNN}
- Author
- Aarrestad TK
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- Abbiendi G
- Abbrescia M
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- Abdelalim AA
- Abdullah WATW
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- Yang UK
- Yang YC
- Yates BR
- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
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- Yu D
- Yu GB
- Yu I
- Yu SS
- Yuan L
- Yumiceva F
- Yusli MN
- Zabi A
- Zaganidis N
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zghiche A
- Zhang A
- Zhang F
- Zhang H
- Zhang J
- Zhang S
- Zhang Z
- Zhao J
- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zito G
- Zobec J
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Publication venue
- 'Elsevier BV'
- Publication date
- 10/09/2019
- Field of study
The production cross sections of B_{s}^{0} mesons and charge conjugates are measured in proton-proton (pp) and PbPb collisions via the exclusive decay channel B_{s}^{0}→J/ψϕ→μ^{+}μ^{−}K^{+}K^{−} at a center-of-mass energy of 5.02 TeV per nucleon pair and within the rapidity range |y|<2.4 using the CMS detector at the LHC. The pp measurement is performed as a function of transverse momentum (p_{T}) of the B_{s}^{0} mesons in the range of 7 to 50 GeV/c and is compared to the predictions of perturbative QCD calculations. The B_{s}^{0} production yield in PbPb collisions is measured in two p_{T} intervals, 7 to 15 and 15 to 50 GeV/c, and compared to the yield in pp collisions in the same kinematic region. The nuclear modification factor (R_{AA}) is found to be 1.5±0.6(stat)±0.5(syst) for 7–15 GeV/c, and 0.87±0.30(stat)±0.17(syst) for 15–50 GeV/c, respectively. Within current uncertainties, the B_{s}^{0} results are consistent with models of strangeness enhancement, and suppression by parton energy loss, as observed for the B+ mesons
Measurement of the tt¯ production cross section, the top quark mass, and the strong coupling constant using dilepton events in pp collisions at √s = 13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdullah WATW
- Abdullin S
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- Abercrombie D
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- Xu Q
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- Yang UK
- Yang YC
- Yates BR
- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
- Yu D
- Yu GB
- Yu I
- Yu SS
- Yuan L
- Yumiceva F
- Yusli MN
- Zabi A
- Zaganidis N
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zghiche A
- Zhang A
- Zhang F
- Zhang H
- Zhang J
- Zhang S
- Zhang Z
- Zhao J
- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zobec J
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 29/04/2019
- Field of study
A measurement of the top quark–antiquark pair production cross section σtt¯ in proton–proton collisions at a centre-of-mass energy of 13TeV is presented. The data correspond to an integrated luminosity of 35.9fb−1, recorded by the CMS experiment at the CERN LHC in 2016. Dilepton events (e ± μ ∓, μ+μ−, e+e−) are selected and the cross section is measured from a likelihood fit. For a top quark mass parameter in the simulation of mMCt=172.5GeV the fit yields a measured cross section σtt¯=803±2(stat)±25(syst)±20(lumi)pb, in agreement with the expectation from the standard model calculation at next-to-next-to-leading order. A simultaneous fit of the cross section and the top quark mass parameter in the POWHEG simulation is performed. The measured value of mMCt=172.33±0.14(stat)+0.66−0.72(syst)GeV is in good agreement with previous measurements. The resulting cross section is used, together with the theoretical prediction, to determine the top quark mass and to extract a value of the strong coupling constant with different sets of parton distribution functions
Search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks in proton-proton collisions at root s=13TeV
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- Voutilainen M
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- Vámi TÁ
- Wadud MA
- Wagner SR
- Walczak M
- Wallny R
- Walsh R
- Waltenberger W
- Walter D
- Wamorkar T
- Wang B
- Wang D
- Wang F
- Wang H
- Wang H
- Wang J
- Wang J
- Wang J
- Wang L
- Wang Q
- Wang Q
- Wang S
- Wang S
- Wang TW
- Wang X
- Wang Y
- Wang Y
- Wang Z
- Wang Z
- Waqas M
- Wardle N
- Wassmer M
- Watson IJ
- Wayne M
- Webb SN
- Weber HA
- Weber M
- Wen Y
- Wertz S
- West C
- Wetzel J
- Wezenbeek L
- Whitbeck A
- Wichmann K
- Wickramage N
- Wickramarathna D
- Wiedenbeck S
- Wightman 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
- Wolfe E
- Wong K
- Wong WY
- Wood D
- Woodard A
- Wozniak KA
- Wozniewski S
- Wright D
- Wu Z
- Wuchterl S
- Wulz C-E
- Wuyckens S
- Wyslouch B
- Würthwein F
- Xia F
- Xiao J
- Xiao M
- Xiao R
- Xie S
- Xie W
- Yagil A
- Yalvac M
- Yan F
- Yang UK
- Yang YC
- Yao Y
- Yarar H
- Yates BR
- Yazgan E
- Yetkin EA
- Yi K
- Yohay R
- Yoo HD
- Yoo J
- Yoon I
- You Z
- Yu D
- Yu GB
- Yu I
- Yu SS
- Yuan L
- Yuan S
- Yumiceva F
- Yusli MN
- Yzquierdo AP-C
- Zabi A
- Zacharopoulou A
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli AG
- Zenaiev O
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang S
- Zhang W
- Zhang Y
- Zhang Z
- Zhao J
- Zhizhin I
- Zhokin A
- Zhu DH
- Zhu RY
- Ziemons T
- Zientek M
- Zlebcik R
- Zobec J
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez CR
- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks is performed in proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC. The analyzed data sample corresponds to an integrated luminosity of 35.9 fb(-1). The signal is characterized by a large missing transverse momentum recoiling against a bottom quark-antiquark system that has a large Lorentz boost. The number of events observed in the data is consistent with the standard model background prediction. Results are interpreted in terms of limits both on parameters of the type-2 two-Higgs doublet model extended by an additional light pseudoscalar boson a (2HDM+a) and on parameters of a baryonic Z simplified model. The 2HDM+a model is tested experimentally for the first time. For the baryonic Z model, the presented results constitute the most stringent constraints to date.Peer reviewe
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