111 research outputs found
Search for effective Lorentz and CPT violation using ZEUS data
- Author
- Abt I
- Aggarwal R
- Aushev V
- Behnke O
- Bertolin A
- Bloch I
- Brock I
- Brook NH
- Brugnera R
- Bruni A
- Bussey PJ
- Caldwell A
- Catterall CD
- Chwastowski J
- Ciborowski J
- Ciesielski R
- Cooper-Sarkar AM
- Corradi M
- Dementiev RK
- Dusini S
- Ferrando J
- Foster B
- Gallo E
- Gangadharan D
- Garfagnini A
- Geiser A
- Grzelak G
- Gwenlan C
- Hochman D
- Jomhari NZ
- Kadenko I
- Karshon U
- Kaur P
- Klanner R
- Korzhavina IA
- Kovalchuk N
- Kuze M
- Levchenko BB
- Levy A
- Longhin A
- Lorkowski F
- Lunghi E
- Löhr B
- Makarenko I
- Malka J
- Masciocchi S
- Nagano K
- Nam JD
- Onishchuk Y
- Paul E
- Pidhurskyi I
- Polini A
- PrzybycieĆ M
- Quintero A
- Ruspa M
- Schneekloth U
- Schörner-Sadenius T
- Selyuzhenkov I
- Shchedrolosiev M
- Shcheglova LM
- Sherrill N
- Skillicorn IO
- Solano A
- Stanco L
- Stefaniuk N
- Surrow B
- SĆomiĆski W
- Tokushuku K
- Turkot O
- Tymieniecka T
- Verbytskyi A
- Wan Abdullah WAT
- Wichmann K
- Wing M
- Yamada S
- Yamazaki Y
- Zarnecki AF
- Zenaiev O
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/05/2023
- Field of study
Lorentz and CPT symmetry in the quark sector of the Standard Model are studied in the context of an effective field theory using ZEUS e±p data. Symmetry-violating effects can lead to time-dependent oscillations of otherwise time-independent observables, including scattering cross sections. An analysis using five years of inclusive neutral-current deep inelastic scattering events corresponding to an integrated HERA luminosity of 372 pb-1 at s=318 GeV has been performed. No evidence for oscillations in sidereal time has been observed within statistical and systematic uncertainties. Constraints, most for the first time, are placed on 42 coefficients parametrizing dominant CPT-even dimension-four and CPT-odd dimension-five spin-independent modifications to the propagation and interaction of light quarks
AAV Exploits Subcellular Stress Associated with Inflammation, Endoplasmic Reticulum Expansion, and Misfolded Proteins in Models of Cystic Fibrosis
- Author
- AM Douar
- AO Yalkinoglu
- B Akache
- B Groschel
- B Hauck
- B Kantor
- B Kleizen
- BH Qu
- BL Tang
- Boris Kantor
- BP O'Sullivan
- Carla M. P. Ribeiro
- CL Ward
- CM Ribeiro
- CM Ribeiro
- D Duan
- D Duan
- D Wat
- F Buyse
- FK Ferrari
- GM Denning
- H Coe
- HL Su
- HR Pelham
- J Hansen
- J Kartenbeck
- J Rosenecker
- JA Isler
- JA Johnston
- JA Johnston
- Jarrod S. Johnson
- JC Grieger
- JH Lin
- JL Badano
- JM Younger
- JP Bridges
- JR Riordan
- JS Bartlett
- JS Johnson
- JS Johnson
- K Pajusola
- KI Berns
- L Cuschieri
- L Fu
- L Pelkmans
- L Zhang
- L Zhong
- Liqun Zhang
- M Gentzsch
- M Mulvey
- M Schelhaas
- Martina Gentzsch
- MC Lee
- ME Martino
- MJ Lewis
- MK Hadden
- ML Fulcher
- ML Styers
- MS Gelman
- N Gregersen
- N Mizushima
- O Schwartz
- PJ French
- PL Leopold
- PO Seglen
- R Bartoszewski
- R Garcia-Mata
- R. Jude Samulski
- R. Michael Linden
- Raymond J. Pickles
- RP Fabunmi
- S Bernales
- S Kelkar
- S Munro
- S Sanlioglu
- T Wileman
- Tal Kafri
- TJ Sferra
- U Bantel-Schaal
- W Ding
- W Ding
- W Li
- WC Wigley
- X Wang
- X Xiao
- Y Chen
- Y Kawaguchi
- Y Yang
- Z Xu
- Z Yan
- Z Yan
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
Barriers to infection act at multiple levels to prevent viruses, bacteria, and parasites from commandeering host cells for their own purposes. An intriguing hypothesis is that if a cell experiences stress, such as that elicited by inflammation, endoplasmic reticulum (ER) expansion, or misfolded proteins, then subcellular barriers will be less effective at preventing viral infection. Here we have used models of cystic fibrosis (CF) to test whether subcellular stress increases susceptibility to adeno-associated virus (AAV) infection. In human airway epithelium cultured at an air/liquid interface, physiological conditions of subcellular stress and ER expansion were mimicked using supernatant from mucopurulent material derived from CF lungs. Using this inflammatory stimulus to recapitulate stress found in diseased airways, we demonstrated that AAV infection was significantly enhanced. Since over 90% of CF cases are associated with a misfolded variant of Cystic Fibrosis Transmembrane Conductance Regulator (ÎF508-CFTR), we then explored whether the presence of misfolded proteins could independently increase susceptibility to AAV infection. In these models, AAV was an order of magnitude more efficient at transducing cells expressing ÎF508-CFTR than in cells expressing wild-type CFTR. Rescue of misfolded ÎF508-CFTR under low temperature conditions restored viral transduction efficiency to that demonstrated in controls, suggesting effects related to protein misfolding were responsible for increasing susceptibility to infection. By testing other CFTR mutants, G551D, D572N, and 1410X, we have shown this phenomenon is common to other misfolded proteins and not related to loss of CFTR activity. The presence of misfolded proteins did not affect cell surface attachment of virus or influence expression levels from promoter transgene cassettes in plasmid transfection studies, indicating exploitation occurs at the level of virion trafficking or processing. Thus, we surmised that factors enlisted to process misfolded proteins such as ÎF508-CFTR in the secretory pathway also act to restrict viral infection. In line with this hypothesis, we found that AAV trafficked to the microtubule organizing center and localized near Golgi/ER transport proteins. Moreover, AAV infection efficiency could be modulated with siRNA-mediated knockdown of proteins involved in processing ÎF508-CFTR or sorting retrograde cargo from the Golgi and ER (calnexin, KDEL-R, ÎČ-COP, and PSMB3). In summary, our data support a model where AAV exploits a compromised secretory system and, importantly, underscore the gravity with which a stressed subcellular environment, under internal or external insults, can impact infection efficiency
Progress and Research Needs of Plant Biomass Degradation by Basidiomycete Fungi
- Author
- A Dilokpimol
- A Dilokpimol
- A Hatakka
- A Hatakka
- A Hatakka
- A Kapich
- A Kapich
- A Kohler
- A Patyshakuliyeva
- A Thuillier
- A Tolbert
- A VĂĄrnai
- A Wymelenberg Vanden
- A Wymelenberg Vanden
- A Wymelenberg Vanden
- AI Hatakka
- Aitor HernĂĄndez-Ortega
- Annele Hatakka
- AR Mach-Aigner
- B Bissaro
- B CreĆĄnar
- B Dörnte
- B Goodell
- B Wu
- BB Hallac
- BD Lindahl
- C Coulter
- C Hori
- C Hori
- C Hori
- C Liers
- C Liers
- C Pohl
- C-K Wat
- CF Thurston
- CS NĂždvig
- D Feldman
- D Floudas
- D Floudas
- D Klemm
- D Linde
- D Liu
- D Martinez
- D Martinez
- D Salvachua
- D Shallom
- DJ Yelle
- DK Johnson
- E Alazi
- E FernĂĄndez-Fueyo
- E Jurak
- E Kunitake
- E Morin
- E Shelest
- E Shirkavand
- E Sjöström
- E Weterings
- EI Solomon
- EN Tamayo
- FJ Ruiz-Dueñas
- G Brunow
- G Gygli
- GN Presley
- H Doddapaneni
- H Qin
- H Suzuki
- H Wariishi
- HB Dunford
- HP Call
- I Grigoriev
- I Silva Coelho da
- J Gaskell
- J Kuuskeri
- J MacDonald
- J Marui
- J Rytioja
- J Rytioja
- J Zhang
- J Zhang
- JA Buswell
- JD Boeke
- JE Adaskaveg
- JE Kowalczyk
- JF Jong de
- JG Shewale
- JG Zeikus
- JM Alvarez
- K Boominathan
- K Boominathan
- K Hammel
- K Karimi
- K-E Eriksson
- KA Jensen Jr
- KE Hammel
- Kristiina Hildén
- KT Steffen
- KW Sarkanen
- L Akileswaran
- L Munk
- LG Nagy
- LG Nagy
- LTM Pham
- LTM Pham
- LTM Pham
- M Aguilar-Pontes
- M Akhtar
- M Binder
- M Couturier
- M Couturier
- M Hofrichter
- M Hofrichter
- M Hofrichter
- M Hofrichter
- M HĂ€kkinen
- M Ide
- M Kinne
- M MarinoviÄ
- M MarinoviÄ
- M Morel
- M Peng
- M Peng
- M Perez-Boada
- M Schuster
- M Schuster
- MB Linder
- MH Gold
- MH Gold
- MH Gold
- MM Whittaker
- MR Jeffers
- MR MÀkelÀ
- MW Woude Van der
- O Niemenmaa
- P Daly
- P Durairaj
- P Korripally
- P Marowa
- P-A Lallement
- PJ Harris
- Q Liu
- R Bourbonnais
- R Kuhad
- R Liu
- R Riley
- R Sindhu
- RA Blanchette
- RA Blanchette
- RA Ohm
- RA Ohm
- RA Ohm
- RB Todd
- RE Quiroz-Castañeda
- S Andersson
- S Casado LĂłpez
- S Casado LĂłpez
- S Chen
- S El-Gebali
- S Huck
- S Kim
- S Miyauchi
- S Tani
- S Yoav
- S-Y Ding
- SR Decker
- SS Sugano
- T Benocci
- T Kirk
- T Lundell
- T Nakazawa
- T Nakazawa
- T Nakazawa
- T Nakazawa
- T Randall
- T Tsukuda
- Takehito Nakazawa
- TK Hakala
- TK Kirk
- TK Lundell
- TM Mello-de-Sousa
- TM Salame
- V Lombard
- W Hartingsveldt van
- WA Doyle
- Y Ninomiya
- Z Li
- Ă Olson
- Publication venue
- Springer International Publishing
- Publication date
- 01/01/2020
- Field of study
Peer reviewe
Impact of jet-production data on the next-to-next-to-leading-order determination of HERAPDF2.0 parton distributions
- Author
- Abdullah WAT Wan
- Abt I
- Aggarwal R
- Andreev V
- Arratia M
- Aushev V
- Baghdasaryan A
- Baty A
- Begzsuren K
- Behnke O
- Belousov A
- Bertolin A
- Bloch I
- Boudry V
- Brandt G
- Brock I
- Brook NH
- Brugnera R
- Bruni A
- Buniatyan A
- Bussey PJ
- Bystritskaya L
- Caldwell A
- Campbell AJ
- Cantun Avila KB
- Catterall CD
- Cerny K
- Chekelian V
- Chen Z
- Chwastowski J
- Ciborowski J
- Ciesielski R
- Contreras JG
- Cooper-Sarkar AM
- Corradi M
- Currie J
- Cvach J
- Dainton JB
- Daum K
- Dementiev RK
- Deshpande A
- Diaconu C
- Dusini S
- Eckerlin G
- Egli S
- Elsen E
- Favart L
- Fedotov A
- Feltesse J
- Ferrando J
- Fleischer M
- Fomenko A
- Foster B
- Gal C
- Gallo E
- Gangadharan D
- Garfagnini A
- Gayler J
- Gehrmann T
- Gehrmann-De Ridder A
- Geiser A
- Gladilin LK
- Glover EWN
- Goerlich L
- Gogitidze N
- Golubkov Yu A
- Gouzevitch M
- Grab C
- Greenshaw T
- Grindhammer G
- Grzelak G
- Gwenlan C
- Haidt D
- Henderson RCW
- Hladky J
- Hochman D
- Hoffmann D
- Horisberger R
- Hreus T
- Huber F
- Huss A
- Jacobs PM
- Jacquet M
- Janssen T
- Jomhari NZ
- Jung AW
- Jung H
- Kadenko I
- Kapichine M
- Karshon U
- Katzy J
- Kaur P
- Kiesling C
- Klanner R
- Klein M
- Klein U
- Kleinwort C
- Klest HT
- Kogler R
- Korzhavina IA
- Kostka P
- Kovalchuk N
- Kretzschmar J
- Kruecker D
- Kruger K
- Kuze M
- Landon MPJ
- Lange W
- Laycock P
- Lee SH
- Levchenko BB
- Levonian S
- Levy A
- Li W
- Lin J
- Lipka K
- List B
- List J
- Lobodzinski B
- Loehr B
- Lohrmann E
- Long OR
- Longhin A
- Lorkowski F
- Lukina O Yu
- Makarenko I
- Malinovski E
- Malka J
- Martyn H-U
- Masciocchi S
- Maxfield SJ
- Mehta A
- Mendez L Cunqueiro
- Meyer AB
- Meyer J
- Mikocki S
- Mikuni VM
- Mondal MM
- Morgan T
- Morozov A
- Muller K
- Nachman B
- Nagano K
- Nam JD
- Naumann Th
- Newman PR
- Niebuhr C
- Niehues J
- Nowak G
- Olsson JE
- Onishchuk Yu
- Ozerov D
- Park S
- Pascaud C
- Patel GD
- Paul E
- Perez E
- Petrukhin A
- Picuric I
- Pidhurskyi I
- Pires J
- Pitzl D
- Polifka R
- Polini A
- Preins S
- Przybycien M
- Quintero A
- Rabbertz K
- Radescu V
- Raicevic N
- Ravdandorj T
- Reimer P
- Rizvi E
- Robmann P
- Roosen R
- Rostovtsev A
- Rotaru M
- Ruspa M
- Sankey DPC
- Sauter M
- Sauvan E
- Schmitt S
- Schmookler BA
- Schneekloth U
- Schoeffel L
- Schoening A
- Schoerner-Sadenius T
- Sefkow F
- Selyuzhenkov I
- Shchedrolosiev M
- Shcheglova LM
- Shushkevich S
- Skillicorn IO
- Slominski W
- Solano A
- Soloviev Y
- Sopicki P
- South D
- Spaskov V
- Specka A
- Stanco L
- Steder M
- Stefaniuk N
- Stella B
- Straumann U
- Sun C
- Surrow B
- Sutton MR
- Sykora T
- Thompson PD
- Tokushuku K
- Traynor D
- Tseepeldorj B
- Tu Z
- Turkot O
- Tymieniecka T
- Valkarova A
- Vallee C
- Van Mechelen P
- Verbytskyi A
- Wegener D
- Wichmann K
- Wing M
- Wunsch E
- Yamada S
- Yamazaki Y
- Zacek J
- Zarnecki AF
- Zenaiev O
- Zhang J
- Zhang Z
- Zlebcik R
- Zohrabyan H
- Zomer F
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 21/03/2022
- Field of study
The HERAPDF2.0 ensemble of parton distribution functions (PDFs) was introduced in 2015. The final stage is presented, a next-to-next-to-leading-order (NNLO) analysis of the HERA data on inclusive deep inelastic ep scattering together with jet data as published by the H1 and ZEUS collaborations. A perturbative QCD fit, simultaneously of αs(M2Z) and the PDFs, was performed with the result αs(M2Z)=0.1156±0.0011 (exp) +0.0001â0.0002 (model +parameterisation) ±0.0029 (scale). The PDF sets of HERAPDF2.0Jets NNLO were determined with separate fits using two fixed values of αs(M2Z), αs(M2Z)=0.1155 and 0.118, since the latter value was already chosen for the published HERAPDF2.0 NNLO analysis based on HERA inclusive DIS data only. The different sets of PDFs are presented, evaluated and compared. The consistency of the PDFs determined with and without the jet data demonstrates the consistency of HERA inclusive and jet-production cross-section data. The inclusion of the jet data reduced the uncertainty on the gluon PDF. Predictions based on the PDFs of HERAPDF2.0Jets NNLO give an excellent description of the jet-production data used as input
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
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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
- Acosta G
- Adam W
- Adams MR
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- Afanasiev S
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- Ahmad A
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- Alvarez JD Ruiz
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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
- Ć irokĂœ 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
Search for Higgs boson pair production in the gamma gamma b(b)over-bar final state in pp collisions at root 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
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- Acosta JG
- Acosta M Vazquez
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- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search is presented for the production of a pair of Higgs bosons, where one decays into two photons and the other one into a bottom quark-antiquark pair. The analysis is performed using proton-proton collision data at root s = 13 TeV recorded in 2016 by the CMS detector at the LHC, corresponding to an integrated luminosity of 35.9 fb(-1) . The results are in agreement with standard model (SM) predictions. In a search for resonant production, upper limits are set on the cross section for new spin-0 or spin-2 particles. For the SM-like nonresonant production hypothesis, the data exclude a product of cross section and branching fraction larger than 2.0 fb at 95% confidence level (CL), corresponding to about 24 times the SM prediction. Values of the effective Higgs boson self-coupling K X are constrained to be within the range -11 < K-lambda < 17 at 95% CL, assuming all other Higgs boson couplings are at their SM value. The constraints on K-lambda, are the most restrictive to date. (C) 2018 The Author(s). Published by Elsevier B.V.Peer reviewe
Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state with two bquarks and two tau leptons in proton-proton collisions at root s=13 TeV The CMS Collaboration
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- Publication date
- 01/01/2018
- Field of study
A search for an exotic decay of the Higgs boson to a pair of light pseudoscalar bosons is performed for the first time in the final state with two b quarks and two tau leptons. The search is motivated in the context of models of physics beyond the standard model (SM), such as two Higgs doublet models extended with a complex scalar singlet (2HDM + S), which include the next-to-minimal supersymmetric SM (NMSSM). The results are based on a data set of proton-proton collisions corresponding to an integrated luminosity of 35.9 fb(-1), accumulated by the CMS experiment at the LHC in 2016 at a center-of-mass energy of 13 TeV. Masses of the pseudoscalar boson between 15 and 60 GeVare probed, and no excess of events above the SM expectation is observed. Upper limits between 3 and 12% are set on the branching fraction B(h -> aa -> 2 tau 2b) assuming the SM production of the Higgs boson. Upper limits are also set on the branching fraction of the Higgs boson to two light pseudoscalar bosons in different 2HDM + S scenarios. Assuming the SM production cross section for the Higgs boson, the upper limit on this quantity is as low as 20% for a mass of the pseudoscalar of 40 GeV in the NMSSM. (C) 2018 The Author(s). Published by Elsevier B.V.Peer reviewe
Evidence for Top Quark Production in Nucleus-Nucleus Collisions
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- Shopova M
- Shtipliyski A
- Shukla P
- Shvetsov I
- Si W
- Siado JE
- Siddireddy P
- Siikonen H
- Sikdar AK
- Sikler F
- Silva Do Amaral SM
- Silva P
- Silvestris L
- Simone FM
- Simonetto F
- Simonis HJ
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- Singh A
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- Sirois Y
- Siroli GP
- Sirunyan AM
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- Skovpen K
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- Spiezia A
- Spiga D
- Spiridonov A
- Spiropulu M
- Spitzbart D
- Srimanobhas N
- Stadie H
- Stahl Leiton AG
- Stahl A
- Staiano A
- Stakia A
- Stampf V
- Starling E
- Starodumov A
- Steen A
- Steggemann J
- SteinbrĂŒck G
- Stenson K
- Stepennov A
- Stephans GSF
- Stickland D
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- Valencia Palomo L
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- Van Mechelen P
- Van Mulders P
- Van Onsem GP
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- Vander Velde C
- Vanegas Arbelaez N
- Vanlaer P
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- Veelken C
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- Vormwald B
- Vorobiev I
- Vorobyev A
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- Wickramarathna D
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- Xiao M
- Xiao R
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- Ălvarez FernĂĄndez A
- Ăzçelik Ă
- Publication venue
- Publication date
- 01/01/2019
- Field of study
Peer reviewe
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