116 research outputs found
Neural entrainment and sensorimotor synchronization to the beat in children with developmental dyslexia: An EEG study
- Publication venue
- Frontiers in Neuroscience
- Publication date
- 01/01/2017
- Field of study
Tapping in time to a metronome beat (hereafter beat synchronization) shows considerable variability in child populations, and individual differences in beat synchronization are reliably related to reading development. Children with developmental dyslexia show impairments in beat synchronization. These impairments may reflect deficiencies in auditory perception of the beat which in turn affect auditory-motor mapping, or may reflect an independent motor deficit. Here we used a new methodology in EEG based on measuring beat-related steady-state evoked potentials (SS-EPs, Nozaradan et al., 2015) in an attempt to disentangle neural sensory and motor contributions to behavioural beat synchronization in children with dyslexia. Children tapped with both their left and right hands to every second beat of a metronome pulse delivered at 2.4 Hz, or listened passively to the beat. Analyses of preferred phase in EEG showed that the children with dyslexia had a significantly different preferred phase compared to control children in all conditions. Regarding SS-EPs, the groups differed significantly for the passive Auditory listening condition at 2.4Hz, and showed a trend towards a difference in the Right hand tapping condition at 3.6 Hz (sensorimotor integration measure). The data suggest that neural rhythmic entrainment is atypical in children with dyslexia for both an auditory beat and during sensorimotor coupling (tapping). The data are relevant to a growing literature suggesting that rhythm-based interventions may help language processing in children with developmental disorders of language learning.Medical Research Counci
Statistical inference and the replication crisis
- Author
- A Eklund
- A Gelman
- A Gelman
- AOJ Cramer
- BD Haig
- BM Hill
- C Babbage
- D Lakens
- D Lakens
- D SzĹącs
- D SzĹącs
- D SzĹącs
- D Trafimow
- DA Dyk van
- Deborah G. Mayo
- DG Mayo
- DG Mayo
- DG Mayo
- DJ Bem
- DJ Bem
- DJ Benjamin
- DM Kaplan
- DV Lindley
- DVM Bishop
- DĂŠnes SzĹącs
- E Yong
- E-J Wagenmakers
- E-J Wagenmakers
- EC Yu
- EJ Masicampo
- G Gandenberger
- H Jeffreys
- H Pashler
- HV Roberts
- J Cohen
- J Neyman
- J Neyman
- JC Winter de
- JJ Ware
- JN Rouder
- JN Rouder
- JO Berger
- JO Berger
- JP Simmons
- JPA Ioannidis
- KF Phillips
- KS Button
- Lincoln J. Colling
- LJ Colling
- LJ Colling
- LK John
- MA GarcĂa-PĂŠrez
- Open Science Collaboration
- R Nuzzo
- RA Fisher
- RD Morey
- RD Morey
- RL Wasserstein
- RS Nickerson
- S Steegen
- U Simonsohn
- W Edwards
- W Stroebe
- Z Dienes
- Z Dienes
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The replication crisis has prompted many to call for statistical reform within the psychological sciences. Here we examine issues within Frequentist statistics that may have led to the replication crisis, and we examine the alternativeâBayesian statisticsâthat many have suggested as a replacement. The Frequentist approach and the Bayesian approach offer radically different perspectives on evidence and inference with the Frequentist approach prioritising error control and the Bayesian approach offering a formal method for quantifying the relative strength of evidence for hypotheses. We suggest that rather than mere statistical reform, what is needed is a better understanding of the different modes of statistical inference and a better understanding of how statistical inference relates to scientific inference
X-ray emission from the Sombrero galaxy: discrete sources
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahmed I
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alexander J
- Aliev T
- Allfrey P
- Almeida N
- Alver B
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Aranyi A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Asaadi J
- Asghar MI
- Askew A
- Ata M
- Atac M
- Atramentov O
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avery P
- Avetisyan A
- Awad A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baesso P
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Bakken JA
- Balazs M
- Ball AH
- Ball G
- Ballin J
- Ban Y
- Bandurin D
- Banerjee S
- Banerjee S
- Bansal S
- Banzuzi K
- Barbagli G
- Barberis E
- Barbone L
- Barge D
- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
- Barone L
- Barrett M
- Bartalini P
- Barth C
- Basegmez S
- Basso L
- Battilana C
- Baty C
- Bauer G
- Bauer J
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bazterra VE
- Bean A
- Beauceron S
- Beaudette F
- Beaupere N
- Bedjidian M
- Bedoya CF
- Behrenhoff W
- Behrens U
- Belforte S
- Beliy N
- Bell AJ
- Bell KW
- Bell P
- Bellan P
- Bellan R
- Bellinger JN
- Belotelov I
- Belyaev A
- Benaglia A
- Bencze G
- Bendavid J
- Bender W
- Benedetti D
- Benelli G
- Beni N
- Benucci L
- Benussi L
- Benvenuti AC
- Beretvas A
- Bergauer T
- Bergholz M
- Beri SB
- Bernardini J
- Bernet C
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- Berry E
- Berryhill J
- Bertl W
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- Besson A
- Betchart B
- Betts RR
- Beuselinck R
- Bhat PC
- Bhatnagar V
- Bhattacharya S
- Bhattacharya S
- Bhatti A
- Bialas W
- Bian JG
- Bianchini L
- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilinskas MJ
- Bilki B
- Bilmis S
- Biselli A
- Bisello D
- Bitioukov S
- Blekman F
- Bloch D
- Bloch I
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Blyweert S
- Bobrovskyi S
- Boccali T
- Bocci A
- Bochenek J
- Bodek A
- Bodin D
- Boeriu O
- Boldizsar L
- Bolla G
- Bolognesi S
- Bolton T
- Bonacorsi D
- Bonato A
- Bondar N
- Bondu O
- Bontenackels M
- Boos E
- Borcherding F
- Borgia MA
- Bornheim A
- Borras K
- Borrello L
- Bortignon P
- Bortoletto D
- Bose S
- Bose T
- Bostock F
- Botta C
- Boucerneur M
- Boudoul G
- Boulahouache C
- Boumediene D
- Bourilkov D
- Boutle S
- Braibant-Giacomelli S
- Branca A
- Branson JG
- Breedon R
- Breuker H
- Brew C
- Brigliadori L
- Brigljevic V
- Broccolo G
- Brom JM
- Brona G
- Brooke JJ
- Broutin C
- Brown RM
- Brownson E
- Brun H
- Bruno G
- Bryer AG
- Buchmuller O
- Buege V
- Buehler M
- Bunin P
- Bunkowski K
- Bunn J
- Buontempo S
- Burelo ED
- Burkett K
- Busson P
- Busza W
- Butler JN
- Butler PH
- Butt J
- Butz E
- Bylsma B
- Caballero IG
- Cabrera A
- Cabrillo IJ
- Caebergs T
- Cakir A
- Calabria C
- Calderon A
- Cali IA
- Callner J
- Calvo E
- Camanzi B
- Caminada L
- Campagnari C
- Campbell A
- Campderros JD
- Camporesi T
- Cankocak K
- Cano E
- Capiluppi P
- Caponeri B
- Cappello G
- Cardaci M
- Carlin R
- Carlsmith D
- Carroll R
- Cartiglia N
- Carvalho W
- Castaldi R
- Castello R
- Castro A
- Castro E
- Caudron J
- Cavallari F
- Cavallo FR
- Cavanaugh R
- Ceard L
- Ceballos GG
- Cebra D
- Cepeda M
- Cerati GB
- Cerci S
- Cerizza G
- Cerminara G
- Cerny K
- Ceron C
- Cerrada M
- Chabert EC
- Chadwick M
- Chakaberia I
- Chan M
- Chang P
- Chang S
- Chang YH
- Chang YH
- Chang YW
- Chanon N
- Chao Y
- Charaf O
- Charlot C
- Chasco M
- Chatterjee A
- Chauhan S
- Checchia P
- Chen GM
- Chen HS
- Chen J
- Chen KF
- Chen KH
- Chen M
- Chen WT
- Chen Y
- Chen Z
- Cheng TL
- Chertok M
- Chetluru V
- Cheung HWK
- Chierici R
- Chiochia V
- Chiorboli M
- Chlebana F
- Choi M
- Choi S
- Choi Y
- Choi YK
- Chou JP
- Choudhary BC
- Choudhury RK
- Choudhury S
- Christiansen T
- Chuang SH
- Chung J
- Chung YS
- Chwalek T
- Ciesielski R
- Cifuentes JAB
- Cihangir S
- Cimmino A
- Cirino G
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clarida W
- Clement E
- Clerbaux B
- Cline D
- CMS Collaboration
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
- Cole P
- Colino N
- Collard C
- Colling D
- Conetti S
- Contardo D
- Conte E
- Conte E
- Conway J
- Cooper SI
- Cortabitarte RV
- Cossutti F
- Costa M
- Costa S
- Costantini S
- Coughlan JA
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- Creanza D
- Cremaldi LM
- Cripps N
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cuplov V
- Cure B
- Cushman P
- Cussans D
- Cutajar M
- Cutts D
- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
- D'Hondt J
- Da Costa EM
- Da Silva WLP
- Dahmes B
- Dahms T
- Dallavalle GM
- Damgov J
- Damiao DD
- Dammann D
- Danielson T
- Darmenov N
- Das S
- Daskalakis G
- Dasu S
- Daubie E
- David A
- Davids M
- Davies G
- De Araujo FTD
- de Barbaro P
- De Benedetti A
- De Boer W
- de Cassagnac RG
- De Cosa A
- de Fatis TT
- De Filippis N
- De Gruttola M
- De Guio F
- De Jeneret JD
- De La Cruz B
- De Lentdecker G
- De Mattia M
- de Monchenault GH
- De Palma M
- De Roeck A
- De Souza SF
- de Troconiz JF
- De Visscher S
- De Wolf EA
- Debreczeni G
- Deisher A
- Deiters K
- Dejardin M
- del Arbol PMR
- Del Re D
- Delaere C
- Deliomeroglu M
- Dell'Orso R
- Della Negra M
- Della Ricca G
- Demaria N
- Demarteau M
- Demin P
- Demina R
- Demir D
- Demir Z
- Demortier L
- Denegri D
- Deniz M
- Depasse P
- Dero V
- Devroede O
- Dhingra N
- Di Giovanni GP
- Di Guida S
- Di Marco E
- Di Matteo L
- Diamond B
- Dias FA
- Dias MAF
- Diemoz M
- Dierlamm A
- Dimitrov A
- Dimitrov L
- Dinardo ME
- Dirkes G
- Dissertori G
- Dittmar M
- Djordjevic M
- Do Amaral SMS
- Dobrzynski L
- Dobur D
- Doesburg R
- Dolen J
- Dominguez A
- Dominik W
- Dorigo T
- Dorney B
- Doroba K
- Dosselli U
- Dozen C
- Draeger J
- Dragicevic M
- Dragoiu C
- Drell BR
- Dremin I
- Drouhin F
- Drozdetskiy A
- Dubinin M
- Duda M
- Dudero PR
- Dudko L
- Dugad S
- Duggan D
- Dumanoglu I
- Duric S
- Duris J
- Durkin LS
- Duru F
- Dusinberre E
- Dutta D
- Dutta S
- Dutta V
- Dyulendarova M
- Dzelalija M
- Eads M
- Eartly DP
- Eckerlin G
- Ecklund KM
- Eckstein D
- Edelhoff M
- Edelmaier CJ
- Eerola P
- Efron J
- Eggert N
- El Mamouni H
- Elliott-Peisert A
- Ellison J
- Elmer P
- Elvira VD
- Enderle H
- Engh D
- Eno SC
- Epshteyn V
- Erbacher R
- Erdmann M
- Erdmann W
- Erhan S
- Ero J
- Ershov A
- Esen S
- Eshaq Y
- Eskew C
- Eskut E
- Etesami SM
- Eugster J
- Eusebi R
- Evangelou I
- Evans D
- Everaerts P
- Everett A
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- Fabbricatore P
- Fabbro B
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- Fabozzi F
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- Fasanella D
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- Fehling D
- Feindt M
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- Ferapontov A
- Ferencek D
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- Fields LJ
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- Fisk I
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- Flix J
- Florez C
- Flossdorf A
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- Flucke G
- Flugge G
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- Fontaine JC
- Ford WT
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- Fouz MC
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- Francis B
- Frangenheim J
- Franzoni G
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- Freeman J
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- Garcia-Solis EJ
- Garfinkel AF
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- Gauthier L
- Gavrilov V
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- Gentit FX
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- Gerber CE
- Gershtein Y
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- Kortelainen MJ
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- Kravchenko I
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- Wood JS
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- Wrochna G
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- Wulz CE
- Wurthwein F
- Wyslouch B
- Xiao H
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- Xu M
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- Yetkin T
- Yi K
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- Yilmaz Y
- Yohay R
- Yoo HD
- Yoon AS
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- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
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- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zorbilmez C
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2010
- Field of study
We present a study of discrete X-ray sources in and around the
bulge-dominated, massive Sa galaxy, Sombrero (M104), based on new and archival
Chandra observations with a total exposure of ~200 ks. With a detection limit
of L_X = 1E37 erg/s and a field of view covering a galactocentric radius of ~30
kpc (11.5 arcminute), 383 sources are detected. Cross-correlation with Spitler
et al.'s catalogue of Sombrero globular clusters (GCs) identified from HST/ACS
observations reveals 41 X-rays sources in GCs, presumably low-mass X-ray
binaries (LMXBs). We quantify the differential luminosity functions (LFs) for
both the detected GC and field LMXBs, whose power-low indices (~1.1 for the
GC-LF and ~1.6 for field-LF) are consistent with previous studies for
elliptical galaxies. With precise sky positions of the GCs without a detected
X-ray source, we further quantify, through a fluctuation analysis, the GC LF at
fainter luminosities down to 1E35 erg/s. The derived index rules out a
faint-end slope flatter than 1.1 at a 2 sigma significance, contrary to recent
findings in several elliptical galaxies and the bulge of M31. On the other
hand, the 2-6 keV unresolved emission places a tight constraint on the field
LF, implying a flattened index of ~1.0 below 1E37 erg/s. We also detect 101
sources in the halo of Sombrero. The presence of these sources cannot be
interpreted as galactic LMXBs whose spatial distribution empirically follows
the starlight. Their number is also higher than the expected number of cosmic
AGNs (52+/-11 [1 sigma]) whose surface density is constrained by deep X-ray
surveys. We suggest that either the cosmic X-ray background is unusually high
in the direction of Sombrero, or a distinct population of X-ray sources is
present in the halo of Sombrero.Comment: 11 figures, 5 tables, ApJ in pres
Search for dijet resonances in 7 TeV pp collisions at CMS
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdel-Basit A
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahmed I
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alexander J
- Aliev T
- Allfrey P
- Almeida N
- Alver B
- Alverson G
- Alves GA
- Amapane N
- Ambroglini F
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Antonelli L
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Aranyi A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Asaadi J
- Asghar MI
- Askew A
- Assran Y
- Ata M
- Atac M
- Atramentov O
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- Zoeller MH
- Zorbilmez C
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2010
- Field of study
This is the Pre-print version of the Article. The official published version of the paper can be accessed from the link below - Copyright @ 2010 APSA search for narrow resonances in the dijet mass spectrum is performed using data corresponding to an integrated luminosity of 2.9ââpb-1 collected by the CMS experiment at the Large Hadron Collider. Upper limits at the 95% confidence level are presented on the product of the resonance cross section, branching fraction into dijets, and acceptance, separately for decays into quark-quark, quark-gluon, or gluon-gluon pairs. The data exclude new particles predicted in the following models at the 95% confidence level: string resonances, with mass less than 2.50 TeV, excited quarks, with mass less than 1.58 TeV, and axigluons, colorons, and E6 diquarks, in specific mass intervals. This extends previously published limits on these models.This work is supported by FMSR (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MES (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES (Croatia); RPF (Cyprus); Academy of Sciences and NICPB (Estonia); Academy of Finland, ME, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); NRF and WCU (Korea); LAS (Lithuania); CINVESTAV, CONACYT, SEP, and UASLP-FAI (Mexico); PAEC (Pakistan); SCSR (Poland); FCT (Portugal); JINR (Armenia, Belarus, Georgia, Ukraine, Uzbekistan); MST and MAE (Russia); MSTD (Serbia); MICINN and CPAN (Spain); Swiss Funding Agencies (Switzerland); NSC (Taipei); TUBITAK and TAEK (Turkey); STFC (United Kingdom); DOE and NSF (USA)
Transverse-momentum and pseudorapidity distributions of charged hadrons in pp collisions at âs=7 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Actis O
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- Yi K
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- Yumiceva F
- Yun JC
- Zabi A
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- Zakaria M
- Zalewski P
- Zanetti M
- Zang SL
- Zarubin A
- Zatzerklyaniy A
- Zeidler C
- Zeinali M
- Zeise M
- Zennamo J
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zinonos Z
- Zito G
- Zoeller MH
- Zorbilmez C
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2010
- Field of study
This is the pre-print version of the Published Article which can be accessed from the link below.Charged-hadron transverse-momentum and pseudorapidity distributions in proton-proton collisions at âs=7ââTeV are measured with the inner tracking system of the CMS detector at the LHC. The charged-hadron yield is obtained by counting the number of reconstructed hits, hit pairs, and fully reconstructed charged-particle tracks. The combination of the three methods gives a charged-particle multiplicity per unit of pseudorapidity dNch/dΡ||Ρ|<0.5=5.78Âą0.01(stat)Âą0.23(syst) for non-single-diffractive events, higher than predicted by commonly used models. The relative increase in charged-particle multiplicity from âs=0.9 to 7 TeV is [66.1Âą1.0(stat)Âą4.2(syst)]%. The mean transverse momentum is measured to be 0.545Âą0.005(stat)Âą0.015(syst)ââGeV/c. The results are compared with similar measurements at lower energies
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
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- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
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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 the pair production of light top squarks in the e(+/-)mu(-/+) final state in proton-proton collisions at root s=13 TeV
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- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search for the production of a pair of top squarks at the LHC is presented. This search targets a region of parameter space where the kinematics of top squark pair production and top quark pair production are very similar, because of the mass difference between the top squark and the neutralino being close to the top quark mass. The search is performed with 35.9 fb(-1) of proton-proton collisions at a centre-of-mass energy of root s = 13 TeV, collected by the CMS detector in 2016, using events containing one electron-muon pair with opposite charge. The search is based on a precise estimate of the top quark pair background, and the use of the M-T2 variable, which combines the transverse mass of each lepton and the missing transverse momentum. No excess of events is found over the standard model predictions. Exclusion limits are placed at 95% confidence level on the production of top squarks up to masses of 208 GeV for models with a mass difference between the top squark and the lightest neutralino close to that of the top quark.Peer reviewe
Search for strongly interacting massive particles generating trackless jets in proton-proton collisions at s = 13 TeV
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- Ălvarez FernĂĄndez A
- Ăsterberg K
- Ăzçelik Ă
- Ĺ irokĂ˝ 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
Dijet azimuthal decorrelations in pp collisions at âs = 7TeV
- Author
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- Abbiendi G
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- Abdullin S
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- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yan M
- Yang F
- Yang M
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang L
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zorbilmez C
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- American Physical Society
- Publication date
- 01/01/2011
- Field of study
This is the pre-print version of the Published Article which can be accessed from the link below.Measurements of dijet azimuthal decorrelations in pp collisions at âs=7ââTeV using the CMS detector at the CERN LHC are presented. The analysis is based on an inclusive dijet event sample corresponding to an integrated luminosity of 2.9ââpb-1. The results are compared to predictions from perturbative QCD calculations and various Monte Carlo event generators. The dijet azimuthal distributions are found to be sensitive to initial-state gluon radiation
Search for supersymmetry in pp collisions at 7 TeV in events with jets and missing transverse energy
- Author
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- Abbiendi G
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- Abdullin S
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- Yilmaz Y
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- Zalewski P
- Zanetti M
- Zang J
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- Zeinali M
- Zeise M
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- Zheng Y
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- Zhukov V
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- Ziebarth EB
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- Zuranski A
- Publication venue
- Elsevier
- Publication date
- 01/01/2011
- Field of study
This is the Pre-print version of the Article. The official published version of the paper can be accessed from the link below - Copyright @ 2011 ElsevierA search for supersymmetry with R-parity conservation in proton-proton collisions at a centre-of-mass energy of 7 TeV is presented. The data correspond to an integrated luminosity of 35 inverse picobarns collected by the CMS experiment at the LHC. The search is performed in events with jets and significant missing transverse energy, characteristic of the decays of heavy, pair-produced squarks and gluinos. The primary background, from standard model multijet production, is reduced by several orders of magnitude to a negligible level by the application of a set of robust kinematic requirements. With this selection, the data are consistent with the standard model backgrounds, namely t t-bar, W + jet and Z + jet production, which are estimated from data control samples. Limits are set on the parameters of the constrained minimal supersymmetric extension of the standard model. These limits extend those set previously by experiments at the Tevatron and LEP colliders.This work is supported by FMSR (Austria); FNRS and FWO (Belgium); CNPq, CAPES, FAPERJ, and FAPESP (Brazil); MES (Bulgaria); CERN; CAS, MoST, and NSFC (China); COLCIENCIAS (Colombia); MSES (Croatia); RPF (Cyprus); Academy of Sciences and NICPB (Estonia); Academy of Finland, ME, and HIP (Finland); CEA and CNRS/IN2P3 (France); BMBF, DFG, and HGF (Germany); GSRT (Greece); OTKA and NKTH (Hungary); DAE and DST (India); IPM (Iran); SFI (Ireland); INFN (Italy); NRF and WCU (Korea); LAS (Lithuania); CINVESTAV, CONACYT,
SEP, and UASLP-FAI (Mexico); PAEC (Pakistan); SCSR (Poland); FCT (Portugal); JINR (Armenia, Belarus, Georgia, Ukraine, Uzbekistan); MST and MAE (Russia); MSTD (Serbia); MICINN and CPAN (Spain); Swiss Funding Agencies (Switzerland); NSC (Taipei); TUBITAK and TAEK (Turkey); STFC (United Kingdom); DOE and NSF (USA)
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