222 research outputs found
Genetic Affinities within a Large Global Collection of Pathogenic Leptospira: Implications for Strain Identification and Molecular Epidemiology
- Author
- AB Ibarz Pavon
- Ahmed Ahmed
- AJ Drummond
- AJ Drummond
- AJ McBride
- AL Nascimento
- AR Bharti
- B Victoria
- C Gravekamp
- DJ Brenner
- E Kmety
- EL Gouveia
- ER Segura
- GM Cerqueira
- HJ Bandelt
- J Thaipadungpanit
- Kishore Nalam
- Leonardo A. Sechi
- M Picardeau
- MA Matthias
- MC Enright
- MC Maiden
- MC Maiden
- Mumtaz Baig
- N Ahmed
- N Ahmed
- N Ahmed
- Niyaz Ahmed
- P Perolat
- P Vijayachari
- P Vijayachari
- Paolo Francalacci
- PN Levett
- PN Levett
- PN Levett
- Ramy K. Aziz
- RK Aziz
- Rudy A. Hartskeerl
- S Kumar
- SB Faine
- SM Devi
- Sundru Manjulata Devi
- Z Majed
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2010
- Field of study
Leptospirosis is an important zoonosis with widespread human health implications. The non-availability of accurate identification methods for the individualization of different Leptospira for outbreak investigations poses bountiful problems in the disease control arena. We harnessed fluorescent amplified fragment length polymorphism analysis (FAFLP) for Leptospira and investigated its utility in establishing genetic relationships among 271 isolates in the context of species level assignments of our global collection of isolates and strains obtained from a diverse array of hosts. In addition, this method was compared to an in-house multilocus sequence typing (MLST) method based on polymorphisms in three housekeeping genes, the rrs locus and two envelope proteins. Phylogenetic relationships were deduced based on bifurcating Neighbor-joining trees as well as median joining network analyses integrating both the FAFLP data and MLST based haplotypes. The phylogenetic relationships were also reproduced through Bayesian analysis of the multilocus sequence polymorphisms. We found FAFLP to be an important method for outbreak investigation and for clustering of isolates based on their geographical descent rather than by genome species types. The FAFLP method was, however, not able to convey much taxonomical utility sufficient to replace the highly tedious serotyping procedures in vogue. MLST, on the other hand, was found to be highly robust and efficient in identifying ancestral relationships and segregating the outbreak associated strains or otherwise according to their genome species status and, therefore, could unambiguously be applied for investigating phylogenetics of Leptospira in the context of taxonomy as well as gene flow. For instance, MLST was more efficient, as compared to FAFLP method, in clustering strains from the Andaman island of India, with their counterparts from mainland India and Sri Lanka, implying that such strains share genetic relationships and that leptospiral strains might be frequently circulating between the islands and the mainland
Isothiocyanate NB7M causes selective cytotoxicity, pro-apoptotic signalling and cell-cycle regression in ovarian cancer cells
- Author
- A Kip
- A P Singh
- AB Gladden
- AC Bharti
- APM Heintz
- B Stillman
- BP Zhou
- CC Conaway
- CH Page
- D Xiao
- D Xiao
- DR Hanahan
- E Lamberth
- F Demarchi
- FJ Oliver
- FR Greten
- G Malich
- G Pearson
- GI Shapiro
- GS Salvesen
- I Ott
- J Ahmed-Choudhury
- J Bodo
- J Pines
- JH Albrecht
- K Inoki
- K K Kim
- KE Crosier
- KM Nicholson
- KS Satyan
- KY Fang
- L Brard
- L Brard
- LH Hartwell
- M Serova
- MJ Piccart
- MM Leitao Jr
- MS Satoh
- N Vorsa
- NA Thornberry
- PX Petit
- R K Singh
- RH Kolm
- RK Singh
- RK Singh
- S Kalkunte
- S Lee
- S Mazumder
- S Shishodia
- SJ Jackson
- SV Singh
- SW Blain
- T S Lange
- TS Lange
- TS Lange
- WC Earnshaw
- WP McGuire
- WP McGuire
- Y Liao
- Publication venue
- Nature Publishing Group
- Publication date
- Field of study
The present report identifies indole-3-ethyl isothiocyanate NB7M as a potent cytotoxic agent with selective activity against cell lines derived from various tumour types. Ovarian cancer cell lines showed sensitivity to NB7M (60–70% cytotoxicity at 2.5 μM), in contrast to control cells (TCL-1 and HTR-8; IC50 ∼15 μM). In a screen performed by the National Cancer Institute (NCI) (NCI60 cancer cell-line assay) NB7M (NSC746077) reduced growth up to 100% with an IC50 between 0.1 and 10 μM depending on the cell line studied. Using SKOV-3 ovarian cancer cells as a model, mechanisms of cytotoxicity were analysed. NB7M caused hallmarks of apoptosis such as PARP-1 deactivation, chromatin condensation, DNA nicks, activation of caspases-9, -8, -3, loss of mitochondrial transmembrane depolarisation potential and upregulation of pro-apoptotic mitogen activated protein kinases (p38, SAP/JNK). NB7M downregulated phosphorylation of prosurvival kinases (PI-3K, AKT, IKKα), transcription factor NF-κB, and expression of DNA-Pk and AXL receptor tyrosine kinase. Subcytotoxic doses of NB7M inhibited DNA synthesis, caused G1-phase cell-cycle arrest and upregulated p27 expression. The present report suggests that NB7M is a selective cytotoxic agent in vitro for cell lines derived from ovarian and certain other tumours. In addition, NB7M acts as a growth/cell-cycle-suppressing agent and may be developed as a potential therapeutic drug to treat ovarian cancer
Mouse mammary tumors display Stat3 activation dependent on leukemia inhibitory factor signaling
- Author
- A Badache
- A Gattelli
- A Gattelli
- AC Bharti
- AM Bamberger
- Ana Quaglino
- BP Haines
- C Lu
- C Lutticken
- C Schere-Levy
- Carolina Schere-Levy
- DP Gearing
- DP Gearing
- DP Gearing
- EA Kritikou
- Edith C Kordon
- H Boeuf
- H Kodama
- H Yu
- J Bromberg
- JA Hutt
- JE Darnell Jr
- JG Cheng
- JI Park
- K Dhingra
- KG Danielson
- KS Selander
- L Li
- L Puricelli
- L Puricelli
- L Zhao
- L Zhao
- LB Mora
- Leonardo Romorini
- M Berishaj
- M Dolled-Filhart
- M Li
- M Minami
- MM Bradford
- P Kellokumpu-Lehtinen
- PY Desprez
- R Buettner
- R Catlett-Falcone
- R Garcia
- R Lopez-Marure
- R Raz
- RD Catalano
- RK Ball
- Roberto P Meiss
- RS Chapman
- S Jenab
- T Taga
- V Buggiano
- VM Golubovskaya
- WM Burke
- X Ling
- Z Estrov
- Publication venue
- BioMed Central
- Publication date
- 01/01/2007
- Field of study
Introduction: It has been demonstrated that leukemia inhibitory factor (LIF) induces epithelium apoptosis through Stat3 activation during mouse mammary gland involution. In contrast, it has been shown that this transcription factor is commonly activated in breast cancer cells, although what causes this effect remains unknown. Here we have tested the hypothesis that locally produced LIF can be responsible for Stat3 activation in mouse mammary tumors. Methods: The studies were performed in different tumorigenic and non-tumorigenic mammary cells. The expression of LIF and LIF receptor was tested by RT-PCR analysis. In tumors, LIF and Stat3 proteins were analyzed by immunohistochemistry, whereas Stat3 and extracellular signal-regulated kinase (ERK)1/2 expression and phosphorylation were studied by Western blot analysis. A LIF-specific blocking antibody was used to determine whether this cytokine was responsible for Stat3 phosphorylation induced by conditioned medium. Specific pharmacological inhibitors (PD98059 and Stat3ip) that affect ERK1/2 and Stat3 activation were used to study their involvement in LIF-induced effects. To analyze cell survival, assays with crystal violet were performed. Results: High levels of LIF expression and activated Stat3 were found in mammary tumors growing in vivo and in their primary cultures. We found a single mouse mammary tumor cell line, LM3, that showed low levels of activated Stat3. Incidentally, these cells also showed very little expression of LIF receptor. This suggested that autocrine/paracrine LIF would be responsible for Stat3 activation in mouse mammary tumors. This hypothesis was confirmed by the ability of conditioned medium of mammary tumor primary cultures to induce Stat3 phosphorylation, activity that was prevented by pretreatment with LIF-blocking antibody. Besides, we found that LIF increased tumor cell viability. Interestingly, blocking Stat3 activation enhanced this effect in mammary tumor cells. Conclusion: LIF is overexpressed in mouse mammary tumors, where it acts as the main Stat3 activator. Interestingly, the positive LIF effect on tumor cell viability is not dependent on Stat3 activation, which inhibits tumor cell survival as it does in normal mammary epithelium. © 2007 Quaglino et al.; licensee BioMed Central Ltd.Fil:Quaglino, A. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina.Fil:Schere-Levy, C. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina.Fil:Romorini, L. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina.Fil:Kordon, E.C. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales; Argentina
Apoptosis, autophagy, necroptosis, and cancer metastasis
- Author
- A Calon
- A Degterev
- A Grosse-Wilde
- A Hübner
- A Jansson
- A Nagasaka
- AC Bharti
- AM Choi
- AM Stark
- AZ Kalea
- B Liu
- BD Hedley
- BN Singh
- C Bellodi
- C Buchheit
- C Fung
- C Gong
- C-H Heldin
- C-W Jang
- CD Simpson
- CE Horak
- CL Chaffer
- CM Kenific
- D Ofengeim
- D-W Zhang
- DF Quail
- DG DeNardo
- DJ Burgess
- DN Dhanasekaran
- DX Nguyen
- E Carrasco-García
- E Powell
- F Azab
- F Basit
- F Gonzalvez
- FK-M Chan
- G Chen
- G Huang
- G Lee
- G Mariño
- G Melino
- GN Naumov
- H Huang
- H Liu
- H Liu
- H Valderrama-Carvajal
- H Yang
- H Zhu
- H-M Shen
- H-Y Chen
- I Hashimoto
- I Tachibana
- I Verbrugge
- IL Ch’en
- IP Nezis
- J Bollrath
- J Debnath
- J Folkman
- J Long
- J Lu
- J Pinkas
- J Thorburn
- J Thorburn
- J Yan
- JE Talmadge
- JL Townson
- JN Dynek
- JR Cerhan
- JS Mattick
- JV Lu
- JY Guo
- K Degenhardt
- K Kessenbrock
- K Takeda
- K Yuan
- KC Wang
- KH Vousden
- KJ Luzzi
- L Apetoh
- L Bai
- L Holmgren
- L Jing
- L K-h
- L Sun
- LA Dempsey
- LB Owen-Schaub
- LM Weiner
- M Adorno
- M Lakshman
- M Schmitz
- M Zörnig
- MA O’Donnell
- MC Guadamillas
- MM Young
- MS Shin
- MS Sosa
- N Isobe
- N Li
- N Mitsiades
- N Mizushima
- N Pasupuleti
- N Umetani
- NE Joo
- NM Fofaria
- O Berezovskaya
- P Boya
- P Clarke
- P Liu
- P Vandenabeele
- Qiang Yu
- R Koomägi
- R Lock
- R Ojha
- R Perlman
- R Wong
- RK Amaravadi
- RT Lima
- S Douma
- S Feng
- S Fulda
- S He
- S Jouan-Lanhouet
- S Mehrotra
- S Pallavi
- S Rao
- S Saiki
- S Schwitalla
- S Vanharanta
- SA Eccles
- SS Martin
- T Sun
- T Teitz
- T Toshima
- TM Morgan
- W Han
- W Pattje
- X Hu
- X Hu
- X Liu
- XP Tong
- Y Cho
- Y Drabsch
- Y Gottfried
- Y Kawano
- Y Lin
- Y Wu
- Y Xuan
- Y Zhao
- Y-F Peng
- Yongbin Chen
- Yongqing Xu
- Z Cai
- Z Fu
- Z Lu
- Z Wang
- Zhenyi Su
- Zuozhang Yang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Elastic and anelastic relaxation behaviour of perovskite multiferroics I: PbZr0.53Ti0.47O3 (PZT)–PbFe0.5Nb0.5O3 (PFN)
- Author
- A Bouzid
- A Falqui
- A Fundora
- A Kumar
- A Kumar
- A Kumar
- A Levstik
- A Marbeuf
- A Migliori
- A Prasatkhetragarn
- A. J. F. Heap
- A. Kumar
- AA Bokov
- AA Bokov
- AA Spivakov
- AF Devonshire
- AG Souza Filho
- AK Singh
- AP Roberts
- AP Roberts
- B Dkhil
- B Fang
- B Fang
- B Fang
- B Fraygola
- B Jaffe
- B Noheda
- B Noheda
- B Noheda
- B Noheda
- B Noheda
- B-J Fang
- BP Blazhievskii
- C Bharti
- C Stock
- C-S Tu
- C. Salazar Mejia
- CJ Howard
- CR Pike
- CR Pike
- D Bochenek
- D Heslop
- D Pandey
- D Pandey
- D Vanderbilt
- D. A. Sanchez
- DA Sanchez
- DA Sanchez
- DA Sanchez
- DD Viehland
- DI Woodward
- DL Corker
- DL Corker
- DM Evans
- DM Evans
- DM Evans
- DM Hatch
- E Dul’kin
- E Pytte
- E Pytte
- EA Mikhaleva
- EI Sitalo
- EKH Salje
- EKH Salje
- EM Bourim
- EV Lovkova
- F Cordero
- F Cordero
- F Cordero
- F Cordero
- GA Rossetti
- GA Rossetti
- GA Rossetti
- GF Nataf
- GM Rotaru
- H Fujishita
- H Thomas
- H Yokota
- H. Shinohara
- HM Rietveld
- I Franke
- I Mayergoyz
- I. Lascu
- IA Kornev
- IH Brunskill
- IP Raevski
- IP Raevski
- IP Raevski
- IP Raevskii
- J Rodriguez-Carvajal
- J Schiemer
- J. A. Schiemer
- J. F. Scott
- JD Axe
- JF Scott
- JM Pérez-Mato
- KH Ehses
- L Yu
- M Correa
- M. A. Carpenter
- MA Carpenter
- MA Carpenter
- MA Carpenter
- MA Carpenter
- MA Carpenter
- MA Carpenter
- MA Carpenter
- MA Carpenter
- MA Carpenter
- MA Carpenter
- MA Carpenter
- MD Glinchuk
- MD Glinchuk
- N Kumar
- N Lampis
- N Zhang
- N Zhang
- N. Ortega
- O Aktas
- O Raymond
- O Raymond
- P Amonpattaratkit
- R Blinc
- R Clarke
- R Egli
- R Havlicek
- R Ranjan
- R Zachariasz
- R. J. Harrison
- R. Nagaratnam
- R. S. Katiyar
- RD Shannon
- REA McKnight
- REA McKnight
- REA McKnight
- RJ Harrison
- RK Mishra
- RM Piticescu
- RO Kuzian
- RO Kuzian
- RS Solanki
- RS Solanki
- RS Solanki
- RW Whatmore
- RW Whatmore
- RW Whatmore
- S Chillal
- S Matteppanavar
- S Matteppanavar
- S. E. Dutton
- SA Ivanov
- SB Majumder
- SK Mishra
- SK Mishra
- SP Singh
- SP Singh
- T Yoshida
- TH Kim
- UT Höchli
- V Bonny
- VAA Bokov
- VS Postnikov
- VV Eremkin
- VV Laguta
- VV Laguta
- VVSS Sai Sunder
- W Kleemann
- W Schranz
- W. Schnelle
- X Meng
- XS Gao
- Z Zhang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Measurement of B_{s}^{0} meson production in pp and PbPb collisions at \sqrt{SNN}
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdelalim AA
- Abdullah WATW
- 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
- 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 MABM
- Alimena J
- Allen B
- Almond J
- Alvarez Fernandez A
- Alvarez JDR
- Alverson G
- Alves FL
- Alves GA
- Alyari M
- Amapane N
- Ambrogi F
- Amendola C
- Amin N
- Amsler C
- Anagnostou G
- Anampa KH
- Anderson D
- Andrea J
- Andreev V
- Andreev Y
- Andrews MB
- Androsov K
- Angioni GLP
- Antonelli L
- Antropov I
- Antunes De Oliveira AC
- 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 M
- Asilar E
- Askew A
- 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
- Ball AH
- Ball F
- Ban Y
- Band R
- 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 DAS
- 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
- 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
- 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 JM
- 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
- Bunichev V
- Bunin P
- Bunkowski K
- Buontempo S
- Burkett K
- 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 GG
- Cecchi C
- Celik A
- Cenna F
- Cepeda M
- Cerati GB
- Cerci S
- Cerminara G
- Cerrada M
- Chabert EC
- Chadeeva M
- Chang P
- Chanon N
- Chao Y
- Chaparro Sierra LF
- Chapon E
- Charaf O
- Charlot C
- Chatterjee K
- Chatterjee RM
- Chatterjee 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 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 SR
- 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
- Collard C
- Colling D
- Colombo F
- Cometti S
- Connor P
- Contardo D
- Conte E
- Contreras-Campana C
- Conway J
- Conway R
- Cooper S
- Cooperstein S
- Cornelis T
- Correa Martins M
- 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 DD
- 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 RG
- De Clercq J
- De Cosa A
- de Fatis TT
- 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 RT
- De Mattia M
- de Monchenault GH
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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
Constraints on anomalous HVV couplings from the production of Higgs bosons decaying to τ lepton pairs
- Author
- Aarrestad TK
- Abbaneo D
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- Abdullah WATW
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- Yohay R
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- Yoo J
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- Yumiceva F
- Yusli MN
- Zabi A
- Zaganidis N
- Zahid S
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- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
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- Zeinali M
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- 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
- AMER PHYSICAL SOC
- Publication date
- 04/12/2019
- Field of study
A study is presented of anomalous HVV interactions of the Higgs boson, including its CP properties. The study uses Higgs boson candidates produced mainly in vector boson fusion and gluon fusion that subsequently decay to a pair of τ leptons. The data were recorded by the CMS experiment at the LHC in 2016 at a center-of-mass energy of 13 TeV and correspond to an integrated luminosity of 35.9 fb−1. A matrix element technique is employed for the analysis of anomalous interactions. The results are combined with those from the H→4ℓ decay channel presented earlier, yielding the most stringent constraints on anomalous Higgs boson couplings to electroweak vector bosons expressed as effective cross section fractions and phases: the CP-violating parameter fa3cos(ϕa3)=(0.00±0.27)×10−3 and the CP-conserving parameters fa2cos(ϕa2)=(0.08+1.04−0.21)×10−3, fΛ1cos(ϕΛ1)=(0.00+0.53−0.09)×10−3, and fZγΛ1cos(ϕZγΛ1)=(0.0+1.1−1.3)×10−3. The current dataset does not allow for precise constraints on CP properties in the gluon fusion process. The results are consistent with standard model expectations
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
- Abu Zeid S
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- Xiao M
- Xiao R
- Xie S
- Xie W
- Xu Q
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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 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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- 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
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
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- Abu Zeid S
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- 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
- 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
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