97 research outputs found
Canine respiratory coronavirus employs caveolin-1-mediated pathway for internalization to HRT-18G cells
- Author
- A Milewska
- A Pratelli
- A Quan
- Aleksandra Milewska
- AM Zaki
- Artur Szczepanski
- B Hernaez
- B Jancekova
- BA Mainou
- BJ Dille
- C Burkard
- C Kooi
- C Liu
- C Liu
- D Dutta
- DM Blau
- E Dietzel
- E Girard
- E Hamme Van
- EJ Bowman
- F Samson
- G Preta
- GA Wudiri
- GM Li
- GR Ares
- H Imhoff
- H Lin
- H Wang
- IC Huang
- IM Mackay
- J Li
- J Schindelin
- J Somsel Rodman
- JA Mitchell
- JK Millet
- JL Wang
- JP Lim
- JR Henley
- Judy A. Mitchell
- K Erles
- K Erles
- K Owczarek
- K Shirato
- K Shirato
- Katarzyna Owczarek
- Krzysztof Pyrc
- KS Choi
- L Kleist von
- L Pelkmans
- LH Wang
- LJ Reed
- M Marsh
- MG Hemida
- MJ Geisow
- MJ Vincent
- O Achour
- O Heikkila
- P Duckert
- P Eifart
- P Oh
- Q Xu
- R Nomura
- S Bertram
- S Bolte
- S Gierer
- S Matsuyama
- SL Priestnall
- TA Hill
- VC Chu
- X Ren
- Y Inoue
- Y Phonphok
- Z Qian
- Z Qinfen
- Zbigniew Baster
- Zenon Rajfur
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
Canine respiratory coronavirus (CRCoV), identified in 2003, is a member of the Coronaviridae family. The virus is a betacoronavirus and a close relative of human coronavirus OC43 and bovine coronavirus. Here, we examined entry of CRCoV into human rectal tumor cells (HRT-18G cell line) by analyzing co-localization of single virus particles with cellular markers in the presence or absence of chemical inhibitors of pathways potentially involved in virus entry. We also targeted these pathways using siRNA. The results show that the virus hijacks caveolin-dependent endocytosis to enter cells via endocytic internalization
Stress-related hormone norepinephrine induces interleukin-6 expression in GES-1 cells
- Author
- Ajuwon KM
- Ben-Eliyahu S
- Ben-Eliyahu S
- Bernabe DG
- Bromberg J
- Chan C
- Costanzo ES
- de Groot RP
- H.B. Gao
- Heikkila K
- Hodge DR
- Jansson C
- Kai H
- Ke Y
- Kiecolt-Glaser JK
- Kishimoto T
- Kondo A
- LeMay LG
- Libermann TA
- Lutgendorf SK
- Lutgendorf SK
- Metz R
- Nilsson MB
- Oh DY
- P. Zhang
- Q. Lin
- R. Yang
- Ray A
- Ray A
- Reiche EM
- Rohrbach S
- Sands WA
- Shaywitz AJ
- Shirakawa F
- Tsujimoto H
- Wang P
- Watabe K
- Xiao W
- Yang EV
- Yang EV
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
A new measurement method for spine reposition sense
- Author
- A Alvemalm
- A Raebold
- A Swinkels
- A Swinkels
- ASN Fu
- BS Hassan
- Cheryl M Petersen
- Chris L Zimmermann
- DC Turk
- DG Altman
- E Kristjannsson
- E-P Takala
- EP Gardner
- Erinn Ewers-Panveno
- EV Evarts
- F Johannsen
- FH Raab
- FS Kaplan
- G Rankin
- GA Koumantakis
- GV Van Herp
- GY Millet
- H Heikkila
- HB Skinner
- HB Skinner
- HS Amonoo-Kuofi
- J Keating
- JA Ashton-Miller
- JA Hides
- JA Hides
- JA Hides
- JE Carpenter
- JK Loudon
- JL Taylor
- JL Taylor
- JM Fritz
- K Newcomer
- KK McCully
- KP Gill
- L Maffey-Ward
- L Sharma
- L Yahia
- LG Portney
- LH Yahia
- M Bjorklund
- M Hagins
- M Revel
- M Revel
- M Truchon
- Mary Ellen Bulow
- MH Sharpe
- MIV Mientjes
- ML Voight
- NN Byl
- PB O'Sullivan
- PB O'Sullivan
- PE Shrout
- PJ Lattanzio
- PW Hodges
- PW Hodges
- PW Hodges
- PW Hodges
- R Marks
- R Marks
- R Marks
- R Preuss
- R Schmidt
- RB Johnston III
- RF McLain
- RF McLain
- RL Smith
- S Brumagne
- S Brumagne
- S Brumagne
- S Brumagne
- S Luoto
- S Luoto
- S Roberts
- S Taimela
- S Taimela
- SH Roy
- SM Lephart
- SSK Lam
- Steven Cope
- SZ George
- T Jakobs
- T Yamashita
- T Yamashita
- TM Parkhurst
- V Leinonen
- V Leinonen
- VB Brooks
- VB Brooks
- WS Marras
- Publication venue
- BioMed Central
- Publication date
- 01/01/2008
- Field of study
Transcriptomic Analysis of the Salivary Glands of an Invasive Whitefly
- Author
- A Cherqui
- A Imai
- A Mortazavi
- A Ratzka
- A Santos
- AL Goldberg
- AM Scrivener
- AM Scrivener
- AP Lourenço
- AS Bowman
- B Berdiales
- B Walz
- C Couldridge
- C Iseli
- CJ Funk
- CL McKenzie
- CM Smith
- DN Byrne
- E Macia
- E Moriones
- ER Mardis
- F Tang
- F Tang
- GP Walker
- H Kato
- I Francischetti
- I Orchard
- IMB Francischetti
- J Hu
- J Kehr
- J Kehr
- J Ramsey
- J Ribeiro
- J Wilhelm
- J Xu
- JBW Wolf
- JC Carolan
- JC Carolan
- JE Serr O
- JIB Bos
- JK Brown
- JL Martinez-Carrillo
- JL McSwain
- JM Baugh
- JM Cicero
- JM Cicero
- JM Li
- John Vontas
- JP Luzio
- Jun-Bo Luan
- Jun-Min Li
- KF Harris
- KT Chung
- L Baumann
- L Garcia-Exposito
- LL Walling
- M Ghanim
- M Ghanim
- M Knoblauch
- M Knoblauch
- M Knoblauch
- M Li
- M Matsumoto
- M Pitino
- Meng Li
- MK Lin
- MM Reis
- N Blow
- N Harmel
- NS Mutti
- O Heikkila
- O Morozova
- PAC 't Hoen
- PJ De Barro
- PW Miles
- R Li
- RD Morin
- RJ Turner
- S Audic
- S Blanc
- S Chen
- S Karim
- S Ray
- S Ueda
- SA Hogenhout
- SC Schuster
- SE Langille
- Shu-Sheng Liu
- SJ Roux
- T Shibasaki
- T Subkhankulova
- T Will
- TA Coudron
- V Medina
- WH Cheng
- WR Cooper
- X Mao
- Xiao-Dong Ye
- Xiao-Wei Wang
- XW Wang
- XW Wang
- Y Yin
- Yun-Lin Su
- YY Zhu
- Z Wang
- Publication venue
- Public Library of Science
- Publication date
- 20/06/2012
- Field of study
<div><h3>Background</h3><p>Some species of the whitefly <em>Bemisia tabaci</em> complex cause tremendous losses to crops worldwide through feeding directly and virus transmission indirectly. The primary salivary glands of whiteflies are critical for their feeding and virus transmission. However, partly due to their tiny size, research on whitefly salivary glands is limited and our knowledge on these glands is scarce.</p> <h3>Methodology/Principal Findings</h3><p>We sequenced the transcriptome of the primary salivary glands of the Mediterranean species of <em>B. tabaci</em> complex using an effective cDNA amplification method in combination with short read sequencing (Illumina). In a single run, we obtained 13,615 unigenes. The quantity of the unigenes obtained from the salivary glands of the whitefly is at least four folds of the salivary gland genes from other plant-sucking insects. To reveal the functions of the primary glands, sequence similarity search and comparisons with the whole transcriptome of the whitefly were performed. The results demonstrated that the genes related to metabolism and transport were significantly enriched in the primary salivary glands. Furthermore, we found that a number of highly expressed genes in the salivary glands might be involved in secretory protein processing, secretion and virus transmission. To identify potential proteins of whitefly saliva, the translated unigenes were put into secretory protein prediction. Finally, 295 genes were predicted to encode secretory proteins and some of them might play important roles in whitefly feeding.</p> <h3>Conclusions/Significance:</h3><p>The combined method of cDNA amplification, Illumina sequencing and <em>de novo</em> assembly is suitable for transcriptomic analysis of tiny organs in insects. Through analysis of the transcriptome, genomic features of the primary salivary glands were dissected and biologically important proteins, especially secreted proteins, were predicted. Our findings provide substantial sequence information for the primary salivary glands of whiteflies and will be the basis for future studies on whitefly-plant interactions and virus transmission.</p> </div
Current opinion on the role of testosterone in the development of prostate cancer: a dynamic model
- Author
- A Darago
- A Discacciati
- A Feustel
- A Feustel
- A Haider
- A Jemal
- A Marczynska
- A Morgentaler
- A Morgentaler
- A Morgentaler
- A Morgentaler
- A Neschadim
- A Netter
- A Nimrod
- AD Berger
- AH Wu
- AK Roy
- AM Nomura
- American Cancer Society
- Amy B. Dailey
- AS Prasad
- AS Prasad
- AS Prasad
- AV Patel
- AW Hsing
- AW Roddam
- B Ettinger
- B Xu
- BA Mohr
- Brandie D. Taylor
- BW Craig
- C Andreini
- C Carson 3rd
- C Chen
- C Couillard
- C Huggins
- C Huggins
- C Wang
- C Wang
- CA Heinlein
- CD Mullins
- CH Bock
- CJ Frederickson
- CJ Frederickson
- CL Hanchette
- D Hofer
- DA Svetec
- DM Kelly
- E Barrett-Connor
- E Giovannucci
- E Wehr
- EA Platz
- EH Allott
- EL Rhoden
- EM John
- ES Orwoll
- FJ Hayes
- FK Habib
- G Karimi
- GB Martin
- GG Schwartz
- GG Schwartz
- GG Schwartz
- GR Schrodt
- HA Feldman
- HA Guess
- HB Carter
- HC Heitkamp
- HJ Litman
- Hui Hu
- HW Baker
- I Cheng
- IG Levy
- J Khoo
- J Lindzey
- JE Fowler Jr
- JF Dorgan
- JK Parsons
- JS Finkelstein
- K McDavid
- K Nimptsch
- KJ Bell
- L Ellis
- LC Costello
- LC Costello
- LD Hayes
- LJ Gooren
- LJ Vatten
- LS Marks
- M Brys
- M Marcelli
- ME Taplin
- MT Schweizer
- N Orsini
- NM Wright
- P Whelan
- PH Gann
- R Gilbert
- R Hartoma
- R Heikkila
- R Ramasamy
- R Ross
- R Sih
- RB Franklin
- RC Travis
- RJ MacInnis
- RL Ferrini
- RR Hajjar
- S Pilz
- S Rohrmann
- S Young-McCaughan
- SA Oliveria
- SJ Winters
- SM Gapstur
- SS Harris
- SS Harris
- T Goel
- T Okamura
- TC Chen
- TK Jensen
- TM Lane
- W Maret
- WC Buschemeyer 3rd
- WJ Kraemer
- WR Miller
- Xiaohui Xu
- Xinguang Chen
- Publication venue
- Springer Nature
- Publication date
- 01/01/2015
- Field of study
Background: Since the landmark study conducted by Huggins and Hodges in 1941, a failure to distinguish between the role of testosterone in prostate cancer development and progression has led to the prevailing opinion that high levels of testosterone increase the risk of prostate cancer. To date, this claim remains unproven.
Presentation of the Hypothesis: We present a novel dynamic mode of the relationship between testosterone and prostate cancer by hypothesizing that the magnitude of age-related declines in testosterone, rather than a static level of testosterone measured at a single point, may trigger and promote the development of prostate cancer.
Testing of the Hypothesis: Although not easily testable currently, prospective cohort studies with population-representative samples and repeated measurements of testosterone or retrospective cohorts with stored blood samples from different ages are warranted in future to test the hypothesis.
Implications of the Hypothesis: Our dynamic model can satisfactorily explain the observed age patterns of prostate cancer incidence, the apparent conflicts in epidemiological findings on testosterone and risk of prostate cancer, racial disparities in prostate cancer incidence, risk factors associated with prostate cancer, and the role of testosterone in prostate cancer progression. Our dynamic model may also have implications for testosterone replacement therapy
Search for the pair production of light top squarks in the e(+/-)mu(-/+) final state in proton-proton 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
- Acosta D
- Acosta G
- 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
- Alexakhin V
- 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 GL 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
- Atay S
- 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
- 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
- Baron O
- Barone L
- Barrera C Oropeza
- 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
- Beck L
- 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
- 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
- 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
- Bolla G
- 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
- Bradmiller-Feld J
- Bragagnolo A
- Braghieri A
- Braibant-Giacomelli S
- Brainerd C
- Brandstetter J
- Brandt S
- Branson JG
- Bravo C
- Breedon R
- Breeze S
- Brew C
- Brianza L
- 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
- 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
- Caputo C
- Carlin R
- Carlsmith D
- Carnes A
- Carrillo Montoya CA
- Cartiglia N
- Carvalho W
- Carver M
- Casarsa M
- Casasso S
- Caspart R
- Castaldi R
- 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 S
- Cerminara G
- Cerrada M
- Chabert EC
- Chang P
- Chang YH
- 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 KY
- Cheng T
- Cheng Y
- Cherepanov V
- Chernyavskaya N
- Chertok M
- Cheung HWK
- Chhibra SS
- Chierici R
- Chinellato J
- Chistov R
- 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
- Corpe L
- Correia Silva G
- Cossutti F
- Costa M
- Costanza F
- 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 Silveira GG
- Dabrowski A
- Daci N
- Dalchenko M
- Dallavalle GM
- Damarseckin S
- Damgov J
- Damiani D Dominguez
- Danilov M
- 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 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 Maria R
- Di Mattia A
- Diemoz M
- Dierlamm A
- Dildick S
- Dilsiz K
- Dimitrov A
- Dimova T
- Dinardo ME
- Dishaw A
- 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
- Dumanoglu I
- Dunser M
- Dupont N
- Duran-Osuna MC
- Durgut S
- Duric S
- Durkin LS
- Dutt S
- Dutta D
- Dutta S
- Dutta V
- 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
- Endres M
- Eno SC
- Epshteyn V
- Erbacher R
- Erdmann M
- Erdmann W
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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 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
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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
Measurement of B_{s}^{0} meson production in pp and PbPb collisions at \sqrt{SNN}
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- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdelalim AA
- Abdullah WATW
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- Abdulsalam A
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- Wu Z
- Wulz C-E
- Wurthwein F
- Wyslouch B
- Xia F
- Xiao M
- Xiao R
- Xie S
- Xie W
- Xu Q
- Yagil A
- Yalvac M
- Yang UK
- Yang YC
- Yates BR
- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
- You C
- 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
- Abdulsalam A
- Abercrombie D
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- Yalvac M
- 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 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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- Zhang F
- Zhang H
- Zhang J
- Zhang S
- Zhang Z
- Zhao J
- Zhokin A
- Zhu DH
- Zhu RY
- Zhukov V
- Zientek M
- Zobec J
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- 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
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