131 research outputs found
The A-B transition in superfluid helium-3 under confinement in a thin slab geometry
- Author
- A Bianchi
- AI Larkin
- AJ Leggett
- AJ Leggett
- AJ Leggett
- AJ Leggett
- AJ Leggett
- AL Fetter
- AMR Schechter
- AP Mackenzie
- B Fellmuth
- BA Olsen
- C Bauerle
- D-K Hong
- DI Bradley
- DI Bradley
- DS Greywall
- G Wallis
- GE Volovik
- GE Volovik
- GW Morley
- H Choi
- H Mayaffre
- J Hara
- J Xu
- JA Sauls
- JA Sauls
- JE Berthold
- JJ Wiman
- JJ Wiman
- JM Parpia
- JM Parpia
- LJ Buchholtz
- LV Levitin
- LV Levitin
- M Bartkowiak
- M Bartkowiak
- M Rice
- MR Freeman
- MW Zwierlein
- P Fulde
- P Schiffer
- P Zheng
- PJ Hakonen
- PW Anderson
- R Blaauwgeers
- R Blaauwgeers
- R Combescot
- R Joynt
- RG Bennett
- S Dimov
- S-HH Tye
- SC Steel
- SM Tholen
- T Kawae
- TM Rice
- TWB Kibble
- V Ambegaokar
- V Kotsubo
- VB Eltsov
- VMH Ruutu
- VV Dmitriev
- WH Zurek
- XL Qui
- Y Kuroda
- Y Maeno
- Y Nagato
- YA Liao
- YH Tang
- Yu Bunkov
- YuM Bunkov
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 23/10/2016
- Field of study
The influence of confinement on the topological phases of superfluid 3He is
studied using the torsional pendulum method. We focus on the phase transition
between the chiral A-phase and the time-reversal-invariant B-phase, motivated
by the prediction of a spatiallymodulated (stripe) phase at the A-B phase
boundary. We confine superfluid 3He to a single 1.08 {\mu}m thick nanofluidic
cavity incorporated into a high-precision torsion pendulum, and map the phase
diagram between 0.1 and 5.6 bar. We observe only small supercooling of the
A-phase, in comparison to bulk or when confined in aerogel. This has a
non-monotonic pressure dependence, suggesting that a new intrinsic B-phase
nucleation mechanism operates under confinement, mediated by the putative
stripe phase. Both the phase diagram and the relative superfluid fraction of
the A and B phases, show that strong coupling is present at all pressures, with
implications for the stability of the stripe phase.Comment: 6 figures, 1 table + supplemental informatio
Bacterial Gut Symbionts Contribute to Seed Digestion in an Omnivorous Beetle
- Author
- A Brauman
- A Heggenstaller
- A Honěk
- A Honěk
- A Tholen
- A Vasanthakumar
- AB Czarnetzki
- AE Douglas
- AE Douglas
- AE Douglas
- AL Mauchline
- AS Ba
- B Kromp
- BC Campbell
- CR Cox
- DG Cochran
- DR Lane
- E Zientz
- EM Janson
- FD Menalled
- GD Inglis
- GD Jones
- GE Ball
- GE Brust
- GE Brust
- GH Thomas
- H Feldhaar
- H Li
- HB Jorgensen
- HK Allen
- I Kounatidis
- I SYSTAT Software
- JA Morales-Ramos
- JD Bewley
- JD Martin
- JE Hobbie
- JG Lundgren
- JG Lundgren
- JG Lundgren
- JG Lundgren
- JG Lundgren
- Jonathan G. Lundgren
- JR Cole
- KE Ashelford
- KI Mohr
- L Akman
- L Macovei
- M Coll
- M Egert
- Marcel Van der Heijden
- MB Blackburn
- MD Hunter
- MG Kaufman
- MG Kaufman
- MM Martin
- MM Martin
- N Brinkmann
- NA Broderick
- NA Moran
- NA Moran
- NH Nguyen
- P Azambuja
- P Buchner
- P Klimeš
- PD Schloss
- PR Westerman
- PR Westerman
- R Gil
- R van der Hoeven
- R. Michael Lehman
- RJ Dillon
- RJ Dillon
- RM Lehman
- S Ennahar
- S Shigenobu
- SF Altschul
- SM Chandler
- SS Prado
- SS Prado
- SW Woolfolk
- SW Woolfolk
- SY Park
- T Hosokawa
- T Huber
- T Yamashita
- TF Doring
- TG Forsythe
- TN Zhavoronkova
- TZ Brandmayr
- VM Kirk
- VM Kirk
- W-T Liu
- Y Kikuchi
- Y Yu
- Publication venue
- Public Library of Science
- Publication date
- 01/05/2010
- Field of study
Obligate bacterial symbionts alter the diets of host animals in numerous ways, but the ecological roles of facultative bacterial residents that colonize insect guts remain unclear. Carabid beetles are a common group of beneficial insects appreciated for their ability to consume insect prey and seeds, but the contributions of microbes to diet diversification in this and similar groups of facultative granivores are largely unknown.Using 16S rRNA gene clone libraries and terminal restriction fragment (tRF) length polymorphism analyses of these genes, we examined the bacterial communities within the guts of facultatively granivorous, adult Harpalus pensylvanicus (Carabidae), fed one of five dietary treatments: 1) an untreated Field population, 2) Seeds with antibiotics (seeds were from Chenopodium album), 3) Seeds without antibiotics, 4) Prey with antibiotics (prey were Acheta domesticus eggs), and 5) Prey without antibiotics. The number of seeds and prey consumed by each beetle were recorded following treatment. Harpalus pensylvanicus possessed a fairly simple gut community of approximately 3-4 bacterial operational taxonomic units (OTU) per beetle that were affiliated with the Gammaproteobacteria, Bacilli, Alphaproteobacteria, and Mollicutes. Bacterial communities of the host varied among the diet and antibiotic treatments. The field population and beetles fed seeds without antibiotics had the closest matching bacterial communities, and the communities in the beetles fed antibiotics were more closely related to each other than to those of the beetles that did not receive antibiotics. Antibiotics reduced and altered the bacterial communities found in the beetle guts. Moreover, beetles fed antibiotics ate fewer seeds, and those beetles that harbored the bacterium Enterococcus faecalis consumed more seeds on average than those lacking this symbiont.We conclude that the relationships between the bacterium E. faecalis and this factultative granivore's ability to consume seeds merit further investigation, and that facultative associations with symbiotic bacteria have important implications for the nutritional ecology of their hosts
Transcriptome dynamics and molecular cross-talk between bovine oocyte and its companion cumulus cells
- Author
- A Atef
- A Bettegowda
- A Hall
- A Regassa
- AL Bishop
- AN Fatehi
- BC Vanderhyden
- BC Vanderhyden
- BC Vanderhyden
- C Looft
- C Vozzi
- CG Liang
- CG Liang
- CM Bailey
- CS Chen
- D Rieger
- D Riveline
- D Tesfaye
- D Tesfaye
- DG de Matos
- DG de Matos
- DL Russell
- E Memili
- E Memili
- E Rodriguez-Gonzalez
- E Tholen
- EA Turley
- EL Howard
- F Gebauer
- F Otsuka
- F Rabahi
- F Rings
- GK Smyth
- H Hizaki
- H Tatemoto
- H Torner
- HT van Tol
- IM Joyce
- J Lesley
- J Nichols
- J Zhou
- JA Whelan
- JH Ralph
- JJ Eppig
- JJ Eppig
- JJ Eppig
- JJ Eppig
- JJ Eppig
- JJ Eppig
- K Schellander
- K Suzuki
- K Tremblay
- KP McNatty
- KR Dunning
- L Gregory
- L Zhang
- LJ McKenzie
- LY Bourguignon
- M Ashburner
- M Assidi
- M Hamel
- M Hoelker
- M Pujol
- M Shimada
- M Yokoo
- MA Simpson
- MD Calder
- MD Calder
- Melanie L Sutton-McDowall
- ML Sutton-McDowall
- MM Matzuk
- N Kimura
- N Kimura
- N Mah
- N Martinek
- N Yew
- P Lucidi
- P Tajik
- PT Brower
- R Buccione
- R De La Fuente
- R Li
- R Prochazka
- RA Irizarry
- RB Gilchrist
- RB Gilchrist
- RB Gilchrist
- RB Gilchrist
- RE Thomas
- RJ Webb
- RL Herlands
- RM Moor
- S Assou
- S Assou
- S Hashimoto
- S Tanghe
- SA Ochsner
- SM Downs
- T Fair
- T Hunt
- T Saito
- TS Hussein
- TS Hussein
- U Cinar
- V Botquin
- VY Rawe
- Y Fukui
- Y Zhang
- YQ Su
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
<p>Abstract</p> <p>Background</p> <p>The bi-directional communication between the oocyte and its companion cumulus cells (CCs) is crucial for development and functions of both cell types. Transcripts that are exclusively expressed either in oocytes or CCs and molecular mechanisms affected due to removal of the communication axis between the two cell types is not investigated at a larger scale. The main objectives of this study were: 1. To identify transcripts exclusively expressed either in oocyte or CCs and 2. To identify those which are differentially expressed when the oocyte is cultured with or without its companion CCs and vice versa.</p> <p>Results</p> <p>We analyzed transcriptome profile of different oocyte and CC samples using Affymetrix GeneChip Bovine Genome array containing 23000 transcripts. Out of 13162 genes detected in germinal vesicle (GV) oocytes and their companion CCs, 1516 and 2727 are exclusively expressed in oocytes and CCs, respectively, while 8919 are expressed in both. Similarly, of 13602 genes detected in metaphase II (MII) oocytes and CCs, 1423 and 3100 are exclusively expressed in oocytes and CCs, respectively, while 9079 are expressed in both. A total of 265 transcripts are differentially expressed between oocytes cultured with (OO + CCs) and without (OO - CCs) CCs, of which 217 and 48 are over expressed in the former and the later groups, respectively. Similarly, 566 transcripts are differentially expressed when CCs mature with (CCs + OO) or without (CCs - OO) their enclosed oocytes. Of these, 320 and 246 are over expressed in CCs + OO and CCs - OO, respectively.</p> <p>While oocyte specific transcripts include those involved in transcription (<it>IRF6, POU5F1, MYF5, MED18</it>), translation (<it>EIF2AK1, EIF4ENIF1</it>) and CCs specific ones include those involved in carbohydrate metabolism (<it>HYAL1, PFKL, PYGL, MPI</it>), protein metabolic processes (<it>IHH, APOA1, PLOD1</it>), steroid biosynthetic process (<it>APOA1, CYP11A1, HSD3B1, HSD3B7</it>). Similarly, while transcripts over expressed in OO + CCs are involved in carbohydrate metabolism (<it>ACO1, 2</it>), molecular transport (<it>GAPDH, GFPT1</it>) and nucleic acid metabolism (<it>CBS, NOS2</it>), those over expressed in CCs + OO are involved in cellular growth and proliferation (<it>FOS, GADD45A</it>), cell cycle (<it>HAS2, VEGFA</it>), cellular development (<it>AMD1, AURKA, DPP4</it>) and gene expression (<it>FOSB, TGFB2</it>).</p> <p>Conclusion</p> <p>In conclusion, this study has generated large scale gene expression data from different oocyte and CCs samples that would provide insights into gene functions and interactions within and across different pathways that are involved in the maturation of bovine oocytes. Moreover, the presence or absence of oocyte and CC factors during bovine oocyte maturation can have a profound effect on transcript abundance of each cell types, thereby showing the prevailing molecular cross-talk between oocytes and their corresponding CCs.</p
Search for Dark Matter and Supersymmetry with a Compressed Mass Spectrum in the Vector Boson Fusion Topology in Proton-Proton Collisions at root s=8 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adair A
- Adam W
- Adams JR
- Adams MR
- Adams T
- Adiguzel A
- Adzic P
- Agapitos A
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akchurin N
- Akgun B
- Al-bataineh A
- Albergo S
- Albrow M
- Alcaraz Maestre J
- Aldaya Martin M
- Alderweireldt S
- Aldá Júnior WL
- Aleksandrov A
- Alexander J
- Alimena J
- Almond J
- Alunni Solestizi L
- Alverson G
- Alves FL
- Alves GA
- Alyari M
- Amapane N
- Amsler C
- Anagnostou G
- Anderson D
- Anderson I
- Andrea J
- Andreev V
- Andreev Yu
- Andrews MB
- Androsov K
- Anelli C
- Antonelli L
- Antropov I
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Apyan A
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arneodo M
- Asavapibhop B
- Asawatangtrakuldee C
- Asilar E
- Asin I
- Askew A
- Ata M
- Attikis A
- Aubin A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Avila C
- Awad A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Baber M
- Bacchetta N
- Bachmair F
- Bachtis M
- Baden A
- Baffioni S
- Bagliesi G
- Bahinipati S
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Ball AH
- Ball F
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Barbagli G
- Barberis E
- Barbieri R
- Bargassa P
- Baringer P
- Barker A
- Barnes VE
- Barney D
- Baron O
- Barone L
- Barria P
- Bartek R
- Barth C
- Bartosik N
- Bartók M
- Baskakov A
- Battilana C
- Baty A
- Bauerdick LAT
- Baumgartel D
- Baus C
- Bayshev I
- Bean A
- Beauceron S
- Beaudette F
- Beck L
- Beernaert K
- Behera PK
- Behnamian H
- Behnke O
- Behrens U
- Bein S
- Beirão Da Cruz E Silva C
- Belchior Batista Das Chagas E
- Belforte S
- Beliy N
- Belknap DA
- Bell KW
- Bellan R
- Belloni A
- Beluffi C
- Belyaev A
- Belyaev A
- Benato L
- Bencze G
- Bendavid J
- Benedetti D
- Benelli G
- Beni N
- Benussi L
- Benvenuti AC
- Beranek S
- Beretvas A
- Bergauer T
- Berger J
- Beri SB
- Bernardes CA
- Bernardini J
- Bernet C
- Berry D
- Berry E
- Berryhill J
- Bertl W
- Besancon M
- Betchart B
- Betts RR
- Bhandari R
- Bhardwaj A
- Bhat PC
- Bhatnagar V
- Bhattacharya R
- Bhattacharya S
- Bhattacharya S
- Bhawandeep U
- Bhopatkar V
- Bhowmik S
- Bi R
- Bialkowska H
- Bian JG
- Bianchini L
- Bianco S
- Bierwagen K
- Biino C
- Bilei GM
- Bilin B
- Bilki B
- Bilmis S
- Bin Anuar AA
- Bisello D
- Bitioukov S
- Blekman F
- 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
- Bonato A
- Bondu O
- Boos E
- Bornheim A
- Borras K
- Bortignon P
- Borzou A
- Bose S
- Bose T
- Botta C
- Boudoul G
- Bouhali O
- Bourilkov D
- Bouvier E
- Bradmiller-Feld J
- Braghieri A
- Braibant-Giacomelli S
- Brandstetter J
- Brandt S
- Branson JG
- Breedon R
- Breto G
- Brew C
- Brianza L
- Brigliadori L
- Brigljevic V
- Brinkerhoff A
- Brinson J
- Brito L
- Brivio F
- Brochero Cifuentes JA
- Brochet S
- Brodski M
- Brom J-M
- Brondolin E
- Brooke JJ
- Brown RM
- Brun H
- Bruner C
- Bruno G
- Buchmuller O
- Bucinskaite I
- Bundock A
- Bunin P
- Bunkowski K
- Bunn J
- Buontempo S
- Burkett K
- Burns D
- Burns D
- Burt K
- Burton D
- Busson P
- Busza W
- Butler JN
- Butler PH
- Buttignol M
- Butz E
- Bylsma B
- Byszuk A
- Bäni L
- Cabrera A
- Cabrillo IJ
- Cadamuro L
- Caillol C
- Cakir A
- Calabria C
- Calamba A
- Calderon De La Barca Sanchez M
- Calderon A
- Cali IA
- Call K
- Calligaris L
- Calpas B
- Calvelli V
- Calvert B
- Calvo E
- Caminada L
- Campagnari C
- Campanini R
- Campbell A
- Camporesi T
- Candelise V
- Canelli MF
- Cankocak K
- Capiluppi P
- Caputo C
- Carlin R
- Carlson B
- Carnes A
- Carrera Jarrin E
- Carrillo Montoya CA
- Carrillo Moreno S
- Cartiglia N
- Carvalho Antunes De Oliveira A
- Carvalho W
- Carver M
- Casal B
- Casarsa M
- Casasso S
- Casimiro Linares E
- Castaldi R
- Castaneda Hernandez A
- Castello R
- Castilla-Valdez H
- Castiñeiras De Saa JR
- Castle J
- Castro A
- Caudron A
- Cavallari F
- Cavallo FR
- Cavallo N
- Cavanaugh R
- Ceard L
- Celik A
- Centis Vignali M
- Cepeda M
- Cerati GB
- Cerminara G
- Cerrada M
- Chabert EC
- Chamizo Llatas M
- Chang P
- Chang YH
- Chang YW
- Chanon N
- Chao Y
- Chaparro Sierra LF
- Chapon E
- Charaf O
- Charlot C
- Chasco M
- Chatterjee A
- Chatterjee K
- Chatterjee RM
- Chauhan S
- Chauhan S
- Chaves J
- Chawla R
- Checchia P
- Chen GM
- Chen HS
- Chen KF
- Chen KH
- Chen M
- Chen PH
- Chen Y
- Chen Y
- Chen Z
- Chenarani S
- Cheng T
- Cherepanov V
- Chertok M
- Cheung HWK
- Chhibra SS
- Chierici R
- Chinellato J
- Chiochia V
- Chiorboli M
- Chistov R
- Chlebana F
- Cho S
- Choi M
- Choi S
- Choi Y
- Chou JP
- Choudhary BC
- Choudhury S
- Chtchipounov L
- Chu J
- Chudasama R
- Chwalek T
- Ciangottini D
- Cieri D
- Cihangir S
- Cimmino A
- Ciocci MA
- Cipriani M
- Cirkovic P
- Citron M
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clarida W
- Clarke C
- Clement E
- Clerbaux B
- Cockerill DJA
- Cocoros A
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
- Colino N
- Collard C
- Colling D
- Colombo F
- Connor P
- Contardo D
- Conte E
- Contreras-Campana C
- Contreras-Campana E
- Conway J
- Conway R
- Cooper SI
- Cornelis T
- Corpe L
- Correa Martins Junior M
- Cossutti F
- Costa M
- Costa S
- Costanza F
- Coubez X
- Couderc F
- Coughlan JA
- Courbon B
- Cousins R
- Covarelli R
- Cowden C
- Cox B
- Cox PT
- Creanza D
- Cremonesi M
- Cristella L
- Cuevas J
- Cuffiani M
- Cumalat JP
- Curras E
- Curry D
- Cussans D
- Custódio A
- Cutts D
- Czellar S
- Da Costa EM
- Da Silveira GG
- Dabrowski A
- Daci N
- Dahmes B
- Dalchenko M
- Dallavalle GM
- Dall’Osso M
- Damarseckin S
- Damgov J
- Danilov M
- Daponte V
- Das S
- Daskalakis G
- Dasu S
- Dauncey P
- David A
- Davies G
- Davignon O
- de Barbaro P
- De Boer W
- De Bruyn I
- De Castro Manzano P
- De Cosa A
- De Filippis N
- De Gruttola M
- De Guio F
- De Jesus Damiao D
- De La Cruz B
- De La Cruz-Burelo E
- De Lentdecker G
- De Mattia M
- De Nardo G
- De Oliveira Martins C
- De Palma M
- De Roeck A
- de Trocóniz JF
- De Visscher S
- De Wit A
- De Wolf EA
- Degano A
- Deiters K
- Dejardin M
- Del Re D
- Delaere C
- Delannoy AG
- Delannoy H
- Delcourt M
- Delgado Peris A
- Delgado A
- Della Negra M
- Della Ricca G
- Dell’Orso R
- 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
- Di Francesco A
- Di Guida S
- Di Marco E
- Di Matteo L
- Di Mattia A
- Diamond B
- Diemoz M
- Dierlamm A
- Dietz C
- Dietz-Laursonn E
- Diez Pardos C
- Dildick S
- Dilsiz K
- Dimitrov A
- Dinardo ME
- Dishaw A
- Dissertori G
- Dittmann J
- Dittmar M
- Dittmer S
- Doan TH
- Dobson M
- Dobur D
- Dodd L
- Dogra S
- Dolen J
- Dolinska G
- Dominguez A
- Donato S
- Donegà M
- Dordevic M
- Dorigo T
- Dorney B
- Doroba K
- Dosselli U
- Dozen C
- Draeger AR
- Dragicevic M
- Dragoiu C
- Dremin I
- Dreyer T
- Driga O
- du Pree T
- Du R
- Duarte J
- Dube S
- Dubinin M
- Duchardt D
- Dudenas V
- Dudero PR
- Dudko L
- Dugad S
- Duggan D
- Duh YT
- Dumanoglu I
- Dunne P
- Dupont N
- Durgut S
- Duric S
- Durkin LS
- Dutt S
- Dutta D
- Dutta S
- Dutta V
- Dünser M
- D’Agnolo RT
- D’Alessandro R
- D’Alfonso M
- d’Enterria D
- D’Hondt J
- D’imperio G
- Eckerlin G
- Ecklund KM
- Eckstein D
- Eerola P
- Eggert N
- Eichhorn T
- El Mamouni H
- Elgammal S
- Eller P
- Elliott-Peisert A
- Ellison J
- Elmer P
- Elumakhov D
- Elvira VD
- Elwood A
- Eminizer N
- Endres M
- Eno SC
- Epshteyn V
- Erbacher R
- Erdmann M
- Erdmann W
- Erdogan Y
- Erdweg S
- Erfle J
- Ershov A
- Erö J
- Escalante Del Valle A
- Esch T
- Eshaq Y
- Eskandari Tadavani E
- Esposito M
- Etesami SM
- Eusebi R
- Evangelou I
- Evans A
- Evdokimov O
- Everaerts P
- Fabbri F
- Fabbri F
- Fabbro B
- Fabozzi F
- Faccioli P
- Fagot A
- Fahim A
- Fan J
- Fanfani A
- Fang W
- Fangmeier C
- Fanò L
- Fartoukh S
- Fasanella D
- Fasanella G
- Faulkner J
- Faure JL
- Favaro C
- Favart L
- Fay J
- Fedi G
- Fehling D
- Felcini M
- Feld L
- Feng L
- Ferapontov A
- Ferbel T
- Ferencek D
- Ferguson T
- Fernandez Bedoya C
- Fernandez Menendez J
- Fernandez Perez Tomei TR
- Fernandez M
- Fernández Ramos JP
- Ferraioli C
- Ferreira Parracho PG
- Ferri F
- Ferro F
- Field RD
- Filipovic N
- Finco L
- Finger M
- Finger M
- Fink S
- Finkel A
- Fiore L
- Fiorendi S
- Fiori F
- Fischer R
- Fisk I
- Flacher H
- Flanagan W
- Flechl M
- Flix J
- Florent A
- Flores C
- Florez C
- Flouris G
- Flowers K
- Flowers S
- Flügge G
- Focardi E
- Foerster M
- Folgueras S
- Fonseca De Souza S
- Fontaine J-C
- Ford WT
- Forthomme L
- Foudas C
- Fouz MC
- Francis B
- Franco Sevilla M
- Francois B
- Franzoni G
- Freeman J
- Friedl M
- Friese R
- Frueboes T
- Frühwirth R
- Fulcher J
- Funk G
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- Publication venue
- Publication date
- 01/01/2016
- Field of study
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
- Acosta D
- 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 the pair production of light top squarks in the e(+/-)mu(-/+) final state in proton-proton collisions at root s=13 TeV
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- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
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- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuolo D
- 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
Measurement of B_{s}^{0} meson production in pp and PbPb collisions at \sqrt{SNN}
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- 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
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
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- Acosta JG
- Acosta M Vazquez
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- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search is presented for the production of a pair of Higgs bosons, where one decays into two photons and the other one into a bottom quark-antiquark pair. The analysis is performed using proton-proton collision data at root s = 13 TeV recorded in 2016 by the CMS detector at the LHC, corresponding to an integrated luminosity of 35.9 fb(-1) . The results are in agreement with standard model (SM) predictions. In a search for resonant production, upper limits are set on the cross section for new spin-0 or spin-2 particles. For the SM-like nonresonant production hypothesis, the data exclude a product of cross section and branching fraction larger than 2.0 fb at 95% confidence level (CL), corresponding to about 24 times the SM prediction. Values of the effective Higgs boson self-coupling K X are constrained to be within the range -11 < K-lambda < 17 at 95% CL, assuming all other Higgs boson couplings are at their SM value. The constraints on K-lambda, are the most restrictive to date. (C) 2018 The Author(s). Published by Elsevier B.V.Peer reviewe
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
- Acharya H
- Ackert A
- Acosta D
- Acosta JG
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- 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
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- Wissing C
- Wittich P
- Wittmann J
- Wittmer B
- Woehrmann C
- Wolf M
- Wolf R
- Wolfe E
- Womersley WJ
- Wong K
- 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
Search for an exotic decay of the Higgs boson to a pair of light pseudoscalars in the final state with two bquarks and two tau leptons in proton-proton collisions at root s=13 TeV The CMS Collaboration
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdelalim AA
- Abdullah Wan WAT
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adam W
- Adams MR
- Adams T
- Adzic P
- Agapitos A
- Agaras MN
- Aggleton R
- Agram JL
- 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 Md MAB
- Alimena J
- Allen B
- Almond J
- Alvarez Fernandez A
- Alves FL
- Alves GA
- Alyari M
- Amapane N
- Ambrogi F
- Amendola C
- Amin N
- Amsler C
- Anagnostou G
- Anampa Hurtado K
- Anderson D
- Andrea J
- Andreev V
- Andreev Yu
- Andrews MB
- Androsov K
- Angioni Pinna GL
- Antonelli L
- Antropov I
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Apyan A
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- Arcidiacono R
- Arenton MW
- Argiro S
- Arndt T
- Arneodo M
- Asavapibhop B
- Asawatangtrakuldee C
- Asghar MI
- Asilar E
- Askew A
- 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
- 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 Sanz DA
- 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
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- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search for an exotic decay of the Higgs boson to a pair of light pseudoscalar bosons is performed for the first time in the final state with two b quarks and two tau leptons. The search is motivated in the context of models of physics beyond the standard model (SM), such as two Higgs doublet models extended with a complex scalar singlet (2HDM + S), which include the next-to-minimal supersymmetric SM (NMSSM). The results are based on a data set of proton-proton collisions corresponding to an integrated luminosity of 35.9 fb(-1), accumulated by the CMS experiment at the LHC in 2016 at a center-of-mass energy of 13 TeV. Masses of the pseudoscalar boson between 15 and 60 GeVare probed, and no excess of events above the SM expectation is observed. Upper limits between 3 and 12% are set on the branching fraction B(h -> aa -> 2 tau 2b) assuming the SM production of the Higgs boson. Upper limits are also set on the branching fraction of the Higgs boson to two light pseudoscalar bosons in different 2HDM + S scenarios. Assuming the SM production cross section for the Higgs boson, the upper limit on this quantity is as low as 20% for a mass of the pseudoscalar of 40 GeV in the NMSSM. (C) 2018 The Author(s). Published by Elsevier B.V.Peer reviewe
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