187 research outputs found
Characterizing the Saltol Quantitative Trait Locus for Salinity Tolerance in Rice
- Author
- A Rodriguez-Navarro
- Abdelbagi M. Ismail
- AM Ismail
- AM Ismail
- AM Ismail
- Andres Godwin Sajise
- AR Yeo
- B Garciadeblás
- C Sahi
- CN Neeraja
- Dante L. Adorada
- E Blumwald
- E Martinoia
- Eduardo Blumwald
- Ellen Tumimbang-Raiz
- EM Septiningsih
- F Hauser
- F Moradi
- F Moradi
- G Mackinney
- GB Gregorio
- Glenn B. Gregorio
- H Nakayama
- H Walia
- H Walia
- HJ Bohnert
- HX Lin
- IRRI
- James Egdane
- JD Platten
- KS Shylaraj
- M Akbar
- M. Akhlasur Rahman
- Marjorie de Ocampo
- Michael J. Thomson
- MJ Thomson
- P Bonilla
- P Mäser
- P Senadheera
- P Senadheera
- R Munns
- Rakesh K. Singh
- RK Singh
- RK Singh
- RK Singh
- S Yoshida
- S-H Kim
- T Horie
- TJ Flowers
- TU Haq
- V Chinnusamy
- Y Yamaguchi
- Zeba I. Seraj
- ZH Ren
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Enhancing AFM process productivity through improved fixturing
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Temporal Retinal Nerve Fiber Loss in Patients with Spinocerebellar Ataxia Type 1
- Author
- A Perretti
- A Petzold
- AE Harding
- Alexander U. Brandt
- AR La Spada
- C Almarcegui
- F Fortuna
- Friedemann Paul
- Hanna Zimmermann
- Jan Schroeter
- JM Gelfand
- L Schöls
- M Abele
- M Bock
- MA Mayer
- Matthias Endres
- ME McLaughlin
- MEJ van Velthoven
- MM Moschos
- Pablo Villoslada
- RC Miller
- RK Manrique
- S Banfi
- S Kang
- S Kim
- S Saidha
- S Walia
- Sarah Stricker
- T Abe
- T Abe
- T Schmitz-Hübsch
- Timm Oberwahrenbrock
- V Carelli
- V Carelli
- Y Lu
- Y Robitaille
- Publication venue
- Public Library of Science
- Publication date
- 29/07/2011
- Field of study
BACKGROUND: Autosomal dominant spinocerebellar ataxia type 1 is an adult onset progressive disorder with well characterized neurodegeneration in the cerebellum and brainstem. Beyond brain atrophy, few data exist concerning retinal and optic nerve involvement. OBJECTIVE: To evaluate retinal changes in SCA1 patients compared to age and gender matched healthy controls. METHODOLOGY/PRINCIPAL FINDINGS: Nine patients with SCA1 were prospectively recruited from the ataxia clinic and were compared to nine age and gender matched healthy controls. Both cohorts received assessment of visually evoked potentials and eye examination by optical coherence tomography to determine retinal nerve fiber layer thickness and total macular volume. While no differences were found in visually evoked potentials, SCA1 patients showed a significant reduction of mean retinal nerve fiber layer thickness (RNFLT) compared to healthy controls (84±13 µm vs. 97±8 µm, p = 0.004). Temporal areas showed the most prominent RNFLT reduction with high statistical significances (temporal-inferior: p<0.001, temporal: p<0.001, temporal-superior: p = 0.005) whereas RNFLT in nasal areas was in the range of the control group. From six SCA1 patients an additional macular scan was obtained. The comparison to the corresponding healthy control showed a slight but not significant reduction in TMV (8.22±0.68 mm(3) vs. 8.61±0.41 mm(3), p = 0.15). CONCLUSION: In SCA1 patients, we found evidence for degeneration of retinal nerve fibers. The temporal focus of the observed retinal nerve fiber layer reduction suggests an involvement of the papillo-macular bundle which resembles pathology found in toxic or mitochondrial optic nerve disease such as Leber's hereditary optic neuropathy (LHON) or dominant optic atrophy (DOA)
Parental Genome Dosage Imbalance Deregulates Imprinting in Arabidopsis
- Author
- A Erilova
- A Kawabe
- A Madlung
- AE Guitton
- B-Y Lin
- BP Dilkes
- C Baroux
- C Josefsson
- C Kohler
- C Kohler
- C Spillane
- D Haig
- D Wang
- EJ Finnegan
- F Berger
- F Berger
- Frédéric Berger
- G Makarevich
- G Makarevich
- H Sasaki
- H Walia
- IM Henry
- J McGrath
- JF Wilkins
- JM Ruijter
- JN Fitz Gerald
- Joseph R. Ecker
- KJ Livak
- L Comai
- M Alleman
- M Gehring
- M Gehring
- M Gehring
- M Ingouff
- M Luo
- M Luo
- M Luo
- M Spielman
- MA Surani
- ND Allen
- O Leblanc
- O Mittelsten Scheid
- Pauline E. Jullien
- PE Jullien
- PE Jullien
- R Feil
- RA Mosher
- RF Ditt
- RJ Scott
- RJ Scott
- RK Slotkin
- S Tiwari
- SW Chan
- SW Chan
- T Kinoshita
- T Kinoshita
- T Kinoshita
- T Kiyosue
- T Miyake
- TJ de Jong
- VL Chandler
- W Reik
- Y Choi
- Y Sotomaru
- Y Sotomaru
- Publication venue
- Public Library of Science
- Publication date
- 01/03/2010
- Field of study
In mammals and in plants, parental genome dosage imbalance deregulates embryo growth and might be involved in reproductive isolation between emerging new species. Increased dosage of maternal genomes represses growth while an increased dosage of paternal genomes has the opposite effect. These observations led to the discovery of imprinted genes, which are expressed by a single parental allele. It was further proposed in the frame of the parental conflict theory that parental genome imbalances are directly mirrored by antagonistic regulations of imprinted genes encoding maternal growth inhibitors and paternal growth enhancers. However these hypotheses were never tested directly. Here, we investigated the effect of parental genome imbalance on the expression of Arabidopsis imprinted genes FERTILIZATION INDEPENDENT SEED2 (FIS2) and FLOWERING WAGENINGEN (FWA) controlled by DNA methylation, and MEDEA (MEA) and PHERES1 (PHE1) controlled by histone methylation. Genome dosage imbalance deregulated the expression of FIS2 and PHE1 in an antagonistic manner. In addition increased dosage of inactive alleles caused a loss of imprinting of FIS2 and MEA. Although FIS2 controls histone methylation, which represses MEA and PHE1 expression, the changes of PHE1 and MEA expression could not be fully accounted for by the corresponding fluctuations of FIS2 expression. Our results show that parental genome dosage imbalance deregulates imprinting using mechanisms, which are independent from known regulators of imprinting. The complexity of the network of regulations between expressed and silenced alleles of imprinted genes activated in response to parental dosage imbalance does not support simple models derived from the parental conflict hypothesis
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
- Funk W
- Furic IK
- Futyan D
- Gadrat S
- Galanti M
- Gallinaro M
- Gallo E
- Galloni C
- Gandrajula RP
- Ganguly S
- Ganjour S
- Garabedian A
- Garay Garcia J
- Garcia G
- Garcia-Abia P
- Garcia-Bellido A
- Garcia-Ferrero J
- Gardner M
- Garg RB
- Garutti E
- Gary JW
- Gascon S
- Gasparini F
- Gasparini U
- Gastler D
- Gauthier L
- Gavrilov V
- Geenen H
- Geffert P
- Geiser A
- Geisler M
- Gelli S
- Gelé D
- Gennai S
- George C
- George J
- Geralis T
- Gerber CE
- Gerosa R
- Gershtein Y
- Geurts FJM
- Ghete VM
- Ghezzi A
- Ghosh S
- Ghosh S
- Giacomelli P
- Giakoumopoulou VA
- Giammanco A
- Giassi A
- Giffels M
- Gigi D
- Gilbert A
- Gill K
- Gilmore J
- Giordano F
- Girgis S
- Girone M
- Givernaud A
- Gizhko A
- Glege F
- Glushkov I
- Gninenko S
- Go Y
- Godinovic N
- Godshalk A
- Goebel K
- Goerlach U
- Goh J
- Gokbulut G
- Goldouzian R
- Goldstein J
- Golf F
- Golovtsov V
- Golubev N
- Golutvin I
- Gomber B
- Gomez Ceballos G
- Gomez G
- Gomez JA
- Gomez JP
- Goncharov M
- Gonzalez Caballero I
- Gonzalez Lopez O
- Gonzalez Suarez R
- Gonzalez D
- Goodell J
- Gorbounov N
- Gorbunov I
- Gori V
- Gottschalk E
- Gouskos L
- Gouzevitch M
- Govoni P
- Goy Lopez S
- Gozzelino A
- Grab C
- Grados Luyando JM
- Gran J
- Grandi C
- Granier de Cassagnac R
- Gras P
- Gray L
- Grebenyuk A
- Green D
- Greene S
- Gregores EM
- Grenier G
- Gribushin A
- Grimes M
- Grippo MT
- Gritsan AV
- Grothe M
- Grunewald M
- Grynyov B
- Grünendahl S
- Guchait M
- Gude A
- Guiducci L
- Guilbaud M
- Gul M
- Guler Y
- Gulhan D
- Gundacker S
- Gunnellini P
- Gupta R
- Gurpinar E
- Gurrola A
- Gurtu A
- Gutay L
- Guthoff M
- Gutsche O
- Gyun D
- Gómez Espinosa TA
- Górski M
- Görner M
- Gülmez E
- Güth A
- Ha S
- Haddad Y
- Hadjiiska R
- Hadley NJ
- Hagopian S
- Hagopian V
- Hahn KA
- Haitz D
- Hajdu C
- Hakala J
- Halkiadakis E
- Hall G
- Haller J
- Hamel de Monchenault G
- Hammer J
- Han J
- Hansen P
- Hanson G
- Harb A
- Hardenbrook J
- Harder K
- Hare D
- Harper S
- Harr R
- Harrington C
- Harris P
- Harris RM
- Hart A
- Hartl C
- Hartmann F
- Hasegawa S
- Hassan Q
- Hatakeyama K
- Hauk J
- Hauser J
- Haytmyradov M
- Heath GP
- Heath HF
- Hebbeker T
- Hebda P
- Hegeman J
- Heidegger C
- Heideman J
- Heidemann C
- Heilman J
- Heindl M
- Heindl SM
- Heintz U
- Heister A
- Heller R
- Hempel M
- Henderson C
- Hensel C
- Heracleous N
- Heredia-De La Cruz I
- Hernandez JM
- Hernandez-Almada A
- Herndon M
- Hervé A
- Hidas D
- Hidas P
- Hildreth M
- Hill C
- Hindrichs O
- Hinzmann A
- Hirosky R
- Hirschauer J
- Hits D
- Hobson PR
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- Zorbilmez C
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- Publication venue
- Publication date
- 01/01/2016
- Field of study
Peer reviewe
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
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- Kothekar K
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- Kovalskyi D
- Kraetschmer I
- Krammer M
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- Kreczko L
- Kreis B
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- Pitters FM
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- Polikarpov S
- Pompili A
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- Pooth O
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- Postiau N
- Potenza R
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- Poyraz D
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- Prieels C
- Primavera F
- Priyanka P
- Prokofyev O
- Prosper H
- Psallidas A
- Ptochos F
- Puerta Pelayo J
- Pugliese G
- Puljak I
- Purohit A
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- Qian SJ
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- Rabady D
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- Ramirez-Sanchez G
- Rander J
- Rane A
- Ranieri A
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- Raspereza A
- Rastogi A
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- Redjimi R
- Redondo I
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- Romeo F
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- Roozbahani B
- Rorie J
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- Ruggles T
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- Rumerio P
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- Rusinov V
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- Seidel M
- Seitz C
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- Sevilla MF
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- Shah A
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- Sheldon P
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- Shtipliyski A
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- Sirois Y
- Siroli GP
- Sirunyan AM
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- Skinnari L
- Skovpen K
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- Slabospitskii S
- Smirnov I
- Smirnov V
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- Snow GR
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- Teroerde M
- Teyssier D
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- Tiras E
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- Titterton A
- Tiwari PC
- Tkaczyk S
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- Tomalin IR
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- Tonjes MB
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- Tsipolitis G
- Tsirou A
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- Tziaferi E
- Uchida K
- Ujvari B
- Ulmer KA
- Ulrich R
- Undleeb S
- Uplegger L
- Uribe Estrada C
- Usai E
- Uvarov L
- Uzunian A
- Vaandering EW
- Vagnerini A
- Vai I
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- Vartak A
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- Velkovska J
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- Verweij M
- Verwilligen P
- Verzetti M
- Verzocchi M
- Veszpremi V
- Vesztergombi G
- Vidal R
- Vila I
- Vilar Cortabitarte R
- Vilela Pereira A
- Viliani L
- Virdee T
- Virdi AK
- Viret S
- Vischia P
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- Vlasov E
- Vlimant JR
- Voevodina E
- Volkov A
- Volobouev I
- Vormwald B
- Vorobiev I
- Vorobyev A
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- Voytishin N
- Wadud MA
- Wagner SR
- Walczak M
- Walia G
- Walker M
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- Walsh R
- Waltenberger W
- Wamorkar T
- Wang B
- Wang D
- Wang F
- Wang H
- Wang J
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- Wang Q
- Wang S
- Wang TW
- Wang X
- Wang Y
- Wang Z
- Waqas M
- Wardle N
- Wasserbaech S
- Wayand S
- Wayne M
- Weber HA
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- Wei H
- Weiler T
- Weinberg M
- Wen Y
- Wertz S
- West C
- Wetzel J
- Whitbeck A
- Wichmann K
- Wickramage N
- Wiederkehr SA
- Wightman A
- Wilkinson R
- Williams T
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- Winer BL
- Winterbottom D
- Wisecarver A
- 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
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- 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
- 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
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- 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
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- Abbaneo D
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- Abdullah WATW
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- Wurthwein F
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- Xiao R
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- Yalvac M
- Yang UK
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- Yates BR
- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
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- 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
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- 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
- 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
- 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
- Alimena J
- Allen B
- Almond J
- Alvarez Fernandez A
- 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
- 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
- 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
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- Yohay R
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- Yumiceva F
- Yusli MN
- Zabi A
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- Zahid S
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- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
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- Zenz SC
- Zeuner WD
- Zeyrek M
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- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zobec J
- Zoi I
- Zolkapli Z
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- 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 single top quark or a top quark pair in proton-proton collisions at s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Al-Bataineh A
- Albajar C
- Albergo S
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- Albrow M
- Alcaraz Maestre J
- Aleksandrov A
- Alexander J
- Alhusseini M
- Ali MAB Md
- Alimena J
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- Alvarez Fernandez A
- Alvarez JD Ruiz
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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 contact interactions and large extra dimensions in the dilepton mass spectra from proton-proton collisions at \sqrt{s} = 13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- 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
- 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
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- Alves FL
- Alves GA
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- Amendola C
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- Amsler C
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- Yusli MN
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- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2019
- Field of study
A search for nonresonant excesses in the invariant mass spectra of electron and muon pairs is presented. The analysis is based on data from proton-proton collisions at a center-of-mass energy of 13 TeV recorded by the CMS experiment in 2016, corresponding to a total integrated luminosity of 36 fb^{-1}. No significant deviation from the standard model is observed. Limits are set at 95% confidence level on energy scales for two general classes of nonresonant models. For a class of fermion contact interaction models, lower limits ranging from 20 to 32 TeV are set on the characteristic compositeness scale Λ. For the Arkani-Hamed, Dimopoulos, and Dvali model of large extra dimensions, the first results in the dilepton final state at 13 TeV are reported, and values of the ultraviolet cutoff parameter Λ_{T} below 6.9 TeV are excluded. A combination with recent CMS diphoton results improves this exclusion to Λ_{T} below 7.7 TeV, providing the most sensitive limits to date in nonhadronic final states
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