190 research outputs found
Valproate, thalidomide and ethyl alcohol alter the migration of HTR-8/SVneo cells
- Author
- A Giese
- A Toivanen
- AC Chang
- AE Sutherland
- AL Moreira
- B Ahluwalia
- BS Shastry
- C Chakraborty
- C Chakraborty
- C Damsky
- C Irl
- C Pilo
- CH Damsky
- CH Graham
- CP Sibley
- CW Spraul
- DG McCarver
- DJ Barker
- DN Bailey
- E Klaffky
- EW Carney
- F Moya
- F Ushigome
- G Bignami
- G Bug
- G Szabo
- G Xu
- GC Douglas
- IA Shibley Jr
- J Botting
- J Komorowski
- J Luo
- JA Irving
- JC Cross
- JD Aplin
- JD Aplin
- JJ Stachecki
- JR Spurzem
- K Miyazaki
- K Uhl
- KS Amankwah
- KS Khera
- KS Khera
- LC Fuller
- M Adachi
- M Marin-Padilla
- M Turan Akay
- M Zygmunt
- M Zygmunt
- MM Knupfer
- MR Nasca
- MR Shen
- MW Miller
- N Oki
- N Utoguchi
- PI Karl
- PS Walmod
- Q Yang
- R Alsdorf
- R Padmanabhan
- RB Shireman
- RC Bates
- RJ Hendrickson
- SM Mooney
- SP Wu
- T McKinnon
- T Murai
- TD Burrows
- Ujjwal K Rout
- UK Rout
- W Chen
- Y Hao
- Publication venue
- BioMed Central
- Publication date
- 01/01/2006
- Field of study
BACKGROUND: Valproate, thalidomide and alcohol (ethanol) exposure during the first trimester of pregnancy is known to cause several developmental disorders. All these teratogens are known to pass the placental barrier and interfere directly with the normal development of the fetus. However, these teratogens also alter the formation and function of the placenta itself which may in turn affect the proper nourishment and development of the fetus. Optimum development of the placenta requires adequate invasion of trophoblast into the maternal uterine tissues. Changes in the migratory behavior of trophoblast by maternal exposure to these teratogens during placentogenesis may therefore alter the structure and function of the placenta. METHODS: In the present study, the effects of sodium valproate, thalidomide and alcohol on the migration of human first trimester trophoblast cell line (HTR-8/SVneo) were examined in vitro. Cells were cultured in the wells of 48-well culture plates as mono or multilayers. Circular patches of cells were removed from the center of the wells by suction, and the migration of cells into the wound was studied using microscopy. Effects of low and high concentrations of valproate, thalidomide and alcohol were examined on the healing of wounds and on the migration rate of cells by determining the wound areas at 0, 3, 6, 12, 24 and 48 h. Effects of drugs and alcohol on the proliferation and the expression levels of integrin subunits beta1 and alpha5 in cells were examined. RESULTS: The migration rates of trophoblast differed between wounds created in mono and multilayers of cells. Exposure to teratogens altered the migration of trophoblast into mono and multilayer wounds. The effects of valproate, thalidomide and alcohol on the proliferation of cells during the rapid migratory phase were mild. Drug exposure caused significant changes in the expression levels of beta1 and alpha5 integrin subunits. CONCLUSION: Results suggest that exposure to valproate, thalidomide or alcohol during the first trimester of pregnancy may change the ultrastructure of the placenta by altering the migration of trophoblast cells and this effect may be mediated by drug- or alcohol-induced changes in the expression levels of beta1 and alpha5 integrin subunits
An interactome-centered protein discovery approach reveals novel components involved in mitosome function and homeostasis in giardia lamblia
- Author
- Samuel Rout
- Jon Paulin Zumthor
- Elisabeth M. Schraner
- Carmen Faso
- Adrian B. Hehl
- Krishan Kumar
- MW Gray
- SB Hedges
- D Yang
- GJ Olsen
- AM Viale
- A Karnkowska
- MF Bauer
- RE Jensen
- CM Koehler
- A Matouschek
- H Prokisch
- J Reinders
- A Sickmann
- N Pfanner
- T Gabaldon
- A Cerkasovová
- DG Lindmark
- Z Mai
- M Muller
- J Tovar
- AM Shiflett
- SM Adl
- A Regoes
- J Tovar
- CE Riordan
- MD Katinka
- J Jerlstrom-Hultqvist
- MS Abrahamsen
- G Leon-Avila
- G Turner
- M van der Giezen
- P Dolezal
- PL Jedelsky
- R Lill
- EA Craig
- R Lill
- J Ankarklev
- HG Morrison
- SR Davis-Hayman
- SE Boucher
- M Abodeely
- S Stefanic
- AV Goldberg
- F Mi-ichi
- L Putignani
- SJ Sanderson
- AD Tsaousis
- PB Wampfler
- E Martincova
- MJ Dagley
- AB Hehl
- L Morf
- J Zumthor
- C Konrad
- JA Vizcaino
- V Gaechter
- DC Chan
- H Chen
- E Martincova
- CG England
- GW Morgan
- AL Chanez
- Y Wexler-Cohen
- N Rajala
- EV Elias
- S Sonda
- HG Elmendorf
- S Isenmann
- JG Duman
- S Bandyopadhyay
- G Manning
- E Martincova
- M Eilers
- F Mi-Ichi
- J Dudek
- F Xu
- AI de Kroon
- E Zinser
- P Kumar
- Y Tamura
- K Yamano
- T Tatsuta
- JG Wideman
- A Rigotti
- J Zhao
- AM van der Bliek
- K Okamoto
- K Elgass
- M Marti
- AG McArthur
- E Smirnova
- SY Miyagishima
- K Nishida
- R Pan
- H Otera
- H Lee
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/01/1995
- Field of study
Protozoan parasites of the genus Giardia are highly prevalent globally, and infect a wide range of vertebrate hosts including humans, with proliferation and pathology restricted to the small intestine. This narrow ecological specialization entailed extensive structural and functional adaptations during host-parasite co-evolution. An example is the streamlined mitosomal proteome with iron-sulphur protein maturation as the only biochemical pathway clearly associated with this organelle. Here, we applied techniques in microscopy and protein biochemistry to investigate the mitosomal membrane proteome in association to mitosome homeostasis. Live cell imaging revealed a highly immobilized array of 30–40 physically distinct mitosome organelles in trophozoites. We provide direct evidence for the single giardial dynamin-related protein as a contributor to mitosomal morphogenesis and homeostasis. To overcome inherent limitations that have hitherto severely hampered the characterization of these unique organelles we applied a novel interaction-based proteome discovery strategy using forward and reverse protein co-immunoprecipitation. This allowed generation of organelle proteome data strictly in a protein-protein interaction context. We built an initial Tom40-centered outer membrane interactome by co-immunoprecipitation experiments, identifying small GTPases, factors with dual mitosome and endoplasmic reticulum (ER) distribution, as well as novel matrix proteins. Through iterative expansion of this protein-protein interaction network, we were able to i) significantly extend this interaction-based mitosomal proteome to include other membrane-associated proteins with possible roles in mitosome morphogenesis and connection to other subcellular compartments, and ii) identify novel matrix proteins which may shed light on mitosome-associated metabolic functions other than Fe-S cluster biogenesis. Functional analysis also revealed conceptual conservation of protein translocation despite the massive divergence and reduction of protein import machinery in Giardia mitosomes
Motives for early retirement of self-employed GPs in the Netherlands: a comparison of two time periods
- Author
- A Luce
- A Manzoni
- A Maynard
- A Scott
- A Spickard Jr
- AACM Maes
- AB Bakker
- AD Misra-Hebert
- B Rechel
- B Rechel
- B Sibbald
- B Sibbald
- BE Landon
- BS Bloom
- C Masseria
- Commissie Implementatie Opleidingscontinuüm en Taakherschikking
- Commission of the European Communities
- D Van Dierendonck
- D Whalley
- DE Yett
- DH De Bakker
- DR Rittenhouse
- E Suzuki
- ES Williams
- G Dussault
- G Mein
- Health Policy and Economic Research Unit
- I Houkes
- I Van Ham
- I Van Ham
- J De Jonge
- J Klein Hesselink
- J Visser
- JM Boot
- JM Davidson
- Joint Learning Initiative: Human Resources for Health
- K Taylor
- L Hingstman
- L Hingstman
- LFJ van der Velden
- LFJ Van der Velden
- Lud FJ Van der Velden
- M Chambers
- M Hann
- M Kirwan
- M Van Greuningen
- M Van Veldhoven
- Malou Van Greuningen
- MJ van den Berg
- MJ van den Berg
- MJ Vernooij-Dasssen
- MW Kroneman
- N Dreesch
- N Gupta
- OECD
- OECD
- P Giessen
- P Van den Hombergh
- P Zurn
- Phil JM Heiligers
- PJM Heiligers
- R Batenburg
- R Cash
- R Karasek
- R Schuller
- RK Purvanova
- RL Lichenstein
- RM Hauser
- RW Griffin
- S Simoens
- S Simoens
- S Simoens
- T O'Dowd
- TD Brett
- TL Hall
- U Rout
- VWB Intermedical
- W Schäfer
- WB Schaufeli
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
The elegans of spindle assembly
- Author
- A Akhmanova
- A Dammermann
- A Dammermann
- A Dammermann
- A Desai
- A Khodjakov
- A Khodjakov
- A Merdes
- A Rodrigues-Martins
- AA Cuenca
- AC Groen
- AH Sathananthan
- AL Knowlton
- AL Schlaitz
- AM Mulder
- AM Saunders
- AR Barr
- AS Kashina
- AW Hunter
- B Bowerman
- B Byers
- B Sonnichsen
- BR Oakley
- C Bamba
- C Gueth-Hallonet
- C Kozlowski
- C Lloyd
- C Segbert
- C Wiese
- CA Kemp
- CA Kemp
- CA Moores
- CA Schatz
- CE Oakley
- CE Walczak
- CE Walczak
- CJ Malone
- CR Cowan
- CS Chan
- D Chretien
- D Job
- DG Albertson
- DG Albertson
- DJ Schmidt
- DL Gard
- DL Gard
- DM Glover
- DR Hamill
- DR Kellogg
- DW Buster
- DY Kim
- E Bullitt
- E Hannak
- E Hannak
- E Nogales
- E Rebollo
- Eileen O’Toole
- EM Mandelkow
- ET O’Toole
- ET O’Toole
- F Zhu
- FJ McNally
- FR Bischoff
- G Gopalan
- G Goshima
- G Yang
- Garrett Greenan
- GC Rogers
- GJ Brouhard
- H Bringmann
- H Huang
- HJ Matthies
- HP Erickson
- HY Yang
- HY Yang
- I Arnal
- I Vernos
- J Azimzadeh
- J Helenius
- J Howard
- J Howard
- J Kleylein-Sohn
- J Loncarek
- J Monen
- J Pecreaux
- J Powers
- JC Labbe
- JD Bishop
- JE Kimble
- JE Sulston
- JJ Hartman
- JM Bellanger
- JM Scholey
- JM Schumacher
- JM Schumacher
- JR Hughes
- JW Kerssemakers
- K Afshar
- K Kinoshita
- K McNally
- K Oegema
- K Oegema
- KC Slep
- KF O’Connell
- KF O’Connell
- KL McNally
- L Pelletier
- L Pelletier
- LA Amos
- LR Matthews
- M Bettencourt-Dias
- M Bornens
- M Boxem
- M Delattre
- M Galli
- M Glotzer
- M Kirkham
- M Moritz
- M Moritz
- M Moritz
- M Schuh
- M Srayko
- M Srayko
- M Srayko
- M Srayko
- M Voet van der
- MA Miller
- MA Miller
- Martin Srayko
- MF Tsou
- MH Bre
- MH Song
- MJ Lee
- ML Ellefson
- MP Rout
- MW Kirschner
- N Le Bot
- N Ozlu
- N Peel
- N Portier
- N Shiina
- N Wolf
- OJ Gruss
- P Askjaer
- P Gonczy
- P Kalab
- P Strnad
- PD Andrews
- PD Andrews
- PL Sadler
- R Basto
- R Giet
- R Habedanck
- R Heald
- R Tournebize
- RD Vale
- RK Herman
- RN Gunawardane
- RS Kochanski
- S Clark-Maguire
- S Clark-Maguire
- S Faruki
- S Lawo
- S Leidel
- S Leidel
- S Moutinho-Pereira
- S Ruchaud
- S Strome
- S Ward
- S Ward
- SF Bakhoum
- SK Dutcher
- SL Jaspersen
- SL Kline-Smith
- SM Murphy
- SM Wignall
- SS Andersen
- SS Andersen
- SW Grill
- SW Grill
- SZ Wang
- T Mitchison
- T Muller-Reichert
- T Wittmann
- T Yabe
- Thomas Müller-Reichert
- TJ Keating
- TL Megraw
- U Rath
- US Tulu
- W Lan
- WE Theurkauf
- WF Marshall
- X Zhang
- Y Nakazawa
- Y Zheng
- ZY Liang
- Publication venue
- SP Birkhäuser Verlag Basel
- Publication date
- 01/01/2010
- Field of study
The Caenorhabditis elegans one-cell embryo is a powerful system in which to study microtubule organization because this large cell assembles both meiotic and mitotic spindles within the same cytoplasm over the course of 1 h in a stereotypical manner. The fertilized oocyte assembles two consecutive acentrosomal meiotic spindles that function to reduce the replicated maternal diploid set of chromosomes to a single-copy haploid set. The resulting maternal DNA then unites with the paternal DNA to form a zygotic diploid complement, around which a centrosome-based mitotic spindle forms. The early C. elegans embryo is amenable to live-cell imaging and electron tomography, permitting a detailed structural comparison of the meiotic and mitotic modes of spindle assembly
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
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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
- Ackert A
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- Acosta JG
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search for dark matter produced in association with top quarks in proton-proton collisions at a center-of-mass energy of 13 TeV is presented. The data set used corresponds to an integrated luminosity of 35.9 fb(-1) recorded with the CMS detector at the LHC. Whereas previous searches for neutral scalar or pseudoscalar mediators considered dark matter production in association with a top quark pair only, this analysis also includes production modes with a single top quark. The results are derived from the combination of multiple selection categories that are defined to target either the single top quark or the top quark pair signature. No significant deviations with respect to the standard model predictions are observed. The results are interpreted in the context of a simplified model in which a scalar or pseudoscalar mediator particle couples to a top quark and subsequently decays into dark matter particles. Scalar and pseudoscalar mediator particles with masses below 290 and 300 GeV, respectively, are excluded at 95% confidence level, assuming a dark matter particle mass of 1 GeV and mediator couplings to fermions and dark matter particles equal to unity.Peer reviewe
Search for strongly interacting massive particles generating trackless jets in proton-proton collisions at s = 13 TeV
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- Zorbilmez C
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- Álvarez Fernández A
- Österberg K
- Özçelik Ö
- Široký J
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
A search for dark matter in the form of strongly interacting massive particles (SIMPs) using the CMS detector at the LHC is presented. The SIMPs would be produced in pairs that manifest themselves as pairs of jets without tracks. The energy fraction of jets carried by charged particles is used as a key discriminator to suppress efficiently the large multijet background, and the remaining background is estimated directly from data. The search is performed using proton-proton collision data corresponding to an integrated luminosity of 16.1 fb - 1 , collected with the CMS detector in 2016. No significant excess of events is observed above the expected background. For the simplified dark matter model under consideration, SIMPs with masses up to 100 GeV are excluded and further sensitivity is explored towards higher masses
Measurement of B_{s}^{0} meson production in pp and PbPb collisions at \sqrt{SNN}
- Author
- Aarrestad TK
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- Abbrescia M
- Abdalla H
- Abdelalim AA
- Abdullah WATW
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- Yu I
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- 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
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- Zhu DH
- Zhu RY
- Zientek M
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- 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
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
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- Abbrescia M
- Abdullah WAT Wan
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- Abu Zeid S
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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
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
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- Abbaneo D
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- Wood D
- Wood J
- Woodard A
- Woods N
- Wright D
- Wright J
- 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
- 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
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