119 research outputs found
Role of Alpha-Synuclein Protein Levels in Mitochondrial Morphology and Cell Survival in Cell Lines
- Author
- A Abeliovich
- A Iwai
- AB Knott
- AE Kingsbury
- CC Stichel
- Chuanzhen Lu
- CM Tanner
- DD Song
- DE Cabin
- DH Cho
- DH Cho
- DT Chang
- F Kamp
- G Andringa
- H Chen
- H Chen
- H Du
- H Mortiboys
- Huaibin Cai
- I Eisenberg
- J Bereiter-Hahn
- JA Javitch
- JV Steidl
- K Nakamura
- K Wirdefeldt
- KM Fung
- L Devi
- L Maroteaux
- LJ Martin
- M Vila
- MG Spillantini
- Min Zhu
- MR Cookson
- MS Parihar
- N Ishihara
- O von Bohlen und Halbach
- P Piccini
- PH Weinreb
- R Raghavan
- RE Heikkila
- RL Nussbaum
- S Buttner
- S Ltic
- SA Detmer
- VN Uversky
- VN Uversky
- W Bruening
- W Dauer
- Wenwei Li
- WJ Koopman
- WW Li
- X Wang
- Y Yang
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
α-Synuclein is highly associated with some neurodegeneration and malignancies. Overexpressing wild-type or mutant α-synuclein promotes neuronal death by mitochondrial dysfunction, the underlying mechanisms of which remain poorly defined. It was recently reported that α-synuclein expression could directly lead to mitochondrial fragmentation in vitro and in vivo, which may be due to α-synuclein localization on mitochondria. Here, we applied a double staining method to demonstrate mitochondrial morphogenetic changes in cells overexpressed with α-synuclein. We show that mitochondrial localization of α-synuclein was increased following its overexpression in three distinct cell lines, including HeLa, SH-SY5Y, and PC12 cells, but no alteration in mitochondrial morphology was detected. However, α-synuclein knockdown prevents MPP+-induced mitochondrial fragmentation in SH-SY5Y and PC12 cells. These data suggest that α-synuclein protein levels hardly affect mitochondrial morphology in normal cell lines, but may have some influence on that under certain environmental conditions
The role of biological fluid and dynamic flow in the behavior and cellular interactions of gold nanoparticles
- Author
- A Babu
- AP Walczak
- B Zhao
- BD Chithrani
- BM Stacy
- E Frohlich
- E Heikkila
- EA Untener
- EC Cho
- EH Jeong
- Emily K. Breitner
- F Joris
- G Oberdorster
- G Saumon
- HU Simon
- J Kusunose
- J Li
- JG Teeguarden
- JM Zook
- JS Nowak
- K Katayama
- KK Comfort
- KK Comfort
- KK Comfort
- KK Comfort
- KM Tsoi
- Kristen K. Comfort
- LK Braydich-Stolle
- M Sethi
- ME Kusek
- N Odzak
- N Ucciferri
- PM Hinderliter
- R Kessler
- R Ma
- R Podila
- RR Arvizo
- S Arora
- S BarathManiKanth
- S Fuchs
- S Sharifi
- SA Berger
- Saber M. Hussain
- W Stopford
- WJ Stark
- Z Li
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Current opinion on the role of testosterone in the development of prostate cancer: a dynamic model
- Author
- A Darago
- A Discacciati
- A Feustel
- A Feustel
- A Haider
- A Jemal
- A Marczynska
- A Morgentaler
- A Morgentaler
- A Morgentaler
- A Morgentaler
- A Neschadim
- A Netter
- A Nimrod
- AD Berger
- AH Wu
- AK Roy
- AM Nomura
- American Cancer Society
- Amy B. Dailey
- AS Prasad
- AS Prasad
- AS Prasad
- AV Patel
- AW Hsing
- AW Roddam
- B Ettinger
- B Xu
- BA Mohr
- Brandie D. Taylor
- BW Craig
- C Andreini
- C Carson 3rd
- C Chen
- C Couillard
- C Huggins
- C Huggins
- C Wang
- C Wang
- CA Heinlein
- CD Mullins
- CH Bock
- CJ Frederickson
- CJ Frederickson
- CL Hanchette
- D Hofer
- DA Svetec
- DM Kelly
- E Barrett-Connor
- E Giovannucci
- E Wehr
- EA Platz
- EH Allott
- EL Rhoden
- EM John
- ES Orwoll
- FJ Hayes
- FK Habib
- G Karimi
- GB Martin
- GG Schwartz
- GG Schwartz
- GG Schwartz
- GR Schrodt
- HA Feldman
- HA Guess
- HB Carter
- HC Heitkamp
- HJ Litman
- Hui Hu
- HW Baker
- I Cheng
- IG Levy
- J Khoo
- J Lindzey
- JE Fowler Jr
- JF Dorgan
- JK Parsons
- JS Finkelstein
- K McDavid
- K Nimptsch
- KJ Bell
- L Ellis
- LC Costello
- LC Costello
- LD Hayes
- LJ Gooren
- LJ Vatten
- LS Marks
- M Brys
- M Marcelli
- ME Taplin
- MT Schweizer
- N Orsini
- NM Wright
- P Whelan
- PH Gann
- R Gilbert
- R Hartoma
- R Heikkila
- R Ramasamy
- R Ross
- R Sih
- RB Franklin
- RC Travis
- RJ MacInnis
- RL Ferrini
- RR Hajjar
- S Pilz
- S Rohrmann
- S Young-McCaughan
- SA Oliveria
- SJ Winters
- SM Gapstur
- SS Harris
- SS Harris
- T Goel
- T Okamura
- TC Chen
- TK Jensen
- TM Lane
- W Maret
- WC Buschemeyer 3rd
- WJ Kraemer
- WR Miller
- Xiaohui Xu
- Xinguang Chen
- Publication venue
- Springer Nature
- Publication date
- 01/01/2015
- Field of study
Background: Since the landmark study conducted by Huggins and Hodges in 1941, a failure to distinguish between the role of testosterone in prostate cancer development and progression has led to the prevailing opinion that high levels of testosterone increase the risk of prostate cancer. To date, this claim remains unproven.
Presentation of the Hypothesis: We present a novel dynamic mode of the relationship between testosterone and prostate cancer by hypothesizing that the magnitude of age-related declines in testosterone, rather than a static level of testosterone measured at a single point, may trigger and promote the development of prostate cancer.
Testing of the Hypothesis: Although not easily testable currently, prospective cohort studies with population-representative samples and repeated measurements of testosterone or retrospective cohorts with stored blood samples from different ages are warranted in future to test the hypothesis.
Implications of the Hypothesis: Our dynamic model can satisfactorily explain the observed age patterns of prostate cancer incidence, the apparent conflicts in epidemiological findings on testosterone and risk of prostate cancer, racial disparities in prostate cancer incidence, risk factors associated with prostate cancer, and the role of testosterone in prostate cancer progression. Our dynamic model may also have implications for testosterone replacement therapy
Search for 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
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aleksandrov A
- 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 L 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
- 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
- Bakirci MN
- 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
- Barnyakov A
- Baron O
- Barone L
- Barria P
- Barrio Luna M
- Bartek R
- Barth C
- Bartok M
- Bartosik N
- Baselga M
- Baskakov A
- Bat A
- Battilana C
- Baty A
- Bauer G
- Bauerdick LAT
- Baur S
- Bayshev I
- Bean A
- Beauceron S
- Beaudette F
- Becerra DA Sanz
- 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
- Benitez JF
- Benussi L
- Benvenuti AC
- Beretvas A
- Bergauer T
- Berger P
- Beri SB
- Bernardes CA
- Bernet C
- Berry D
- Berryhill J
- Bertsche D
- Besancon M
- Beschi A
- Betts RR
- Bhandari R
- Bhardwaj A
- Bhardwaj R
- Bharti M
- Bhat MA
- Bhat PC
- Bhatnagar V
- Bhattacharya R
- Bhattacharya S
- 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
- Bisello D
- 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
- Bonacorsi D
- Bondu O
- Boos E
- Boran F
- Boren S
- Borg J
- Borgonovi L
- Bornheim A
- Borras K
- Borrello L
- Bortignon P
- Bose T
- Botta C
- Botta V
- Boudoul G
- Bouhali O
- Bourilkov D
- Bouvier E
- Bowen J
- Bragagnolo A
- Braghieri A
- Braibant-Giacomelli S
- Brainerd C
- Brandstetter J
- Brandt S
- Branson JG
- Bravo C
- Breedon R
- Breeze S
- Brew C
- Brigljevic V
- Brinkerhoff A
- Brivio F
- Brochero Cifuentes JA
- Brochet S
- Brodski M
- Brom J-M
- Brondolin E
- Brooke JJ
- Brown RM
- Brun H
- Bruno G
- Brzhechko D
- Bucci R
- Buccilli A
- Buchanan J
- Buchmuller O
- Bueghly J
- Bundock A
- 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
- Cappati A
- Caputo C
- Carlin R
- Carlsmith D
- Carnes A
- Carrera Jarrin E
- Carrillo Montoya CA
- Carrillo Moreno S
- Cartiglia N
- Carvalho W
- Casarsa M
- Caspart R
- Castaldi R
- Castaneda Hernandez A
- Castilla-Valdez H
- Castle J
- Castro A
- Cavallari F
- Cavallo FR
- Cavallo N
- Cavanaugh R
- Ceballos G Gomez
- Cecchi C
- Celik A
- Cenna F
- Cepeda M
- Cerati GB
- Cerci D Sunar
- Cerci S
- Cerminara G
- Cerrada M
- Chabert EC
- Chadeeva M
- Chang P
- Chang P
- 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 T
- Cheng Y
- Cherepanov V
- Chernyavskaya N
- Chertok M
- Cheung HWK
- Chhibra SS
- Chierici R
- Chinellato J
- Chlebana F
- Cho S
- Choi S
- Choi Y
- Chou JP
- Choudhary BC
- Choudhury S
- Chowdhury 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
- Correia Silva G
- Cossutti F
- Costa M
- Coubez X
- Couderc F
- Coughlan JA
- Courbon B
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- Creanza D
- Cremonesi M
- Cristella L
- Csanad M
- Cucciati G
- Cuevas J
- Cuffiani M
- Cumalat JP
- Curry D
- Cussans D
- Cutts D
- Czellar S
- D'Alessandro R
- D'Alfonso M
- d'Enterria D
- D'Hondt J
- Da Costa EM
- Da Rold A
- Da Silveira GG
- Dabrowski A
- Daci N
- Dalchenko M
- Dall'Osso M
- Dallavalle GM
- Damarseckin S
- Damgov J
- Damiani D Dominguez
- 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 Iorio A
- 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 Marco E
- Di Maria R
- Di Mattia A
- Diemoz M
- Dierlamm A
- Dildick S
- Dilsiz K
- Dimitrov A
- Dimova T
- Dinardo ME
- Dissertori G
- Dittmann J
- Dittmar M
- Dittmer S
- Doan TH
- Dobson M
- Dobur D
- Dodd L
- Dolek F
- Dolen J
- Dominguez A
- Donato S
- Donega M
- Dordevic M
- Dorfer C
- Dorigo T
- Dorney B
- Doroba K
- Dosselli U
- Dozen C
- Dragicevic M
- Dremin I
- Dreyer T
- Duarte Campderros J
- Duarte J
- Dube S
- Dubinin M
- Duchardt D
- Dudenas V
- Dudero PR
- Dudko L
- Dugad S
- Duh YT
- Dulemba JL
- Dunser M
- Dupont N
- Duran-Osuna MC
- Durgut S
- Duric S
- Durkin LS
- Dutt S
- Dutta D
- Dutta S
- Dutta V
- Ebrahimi A
- Eckerlin G
- Ecklund KM
- Eerola P
- Ehataht K
- Eichhorn T
- El Mamouni H
- El Morabit K
- Elayavalli R Kunnawalkam
- Elgammal S
- Elliott-Peisert A
- Elmer P
- Elumakhov D
- Elvira VD
- Elwood A
- Eminizer N
- Eno SC
- Epshteyn V
- Erbacher R
- Erdmann M
- Erdmann W
- Erdweg S
- Eren E
- Erice C
- Eroe J
- Errico F
- Ershov A
- Esch T
- Eskut E
- Etesami SM
- Eusebi R
- Evangelou I
- Evans A
- Evdokimov O
- Everaerts P
- Eysermans J
- Fabbri F
- Fabbri F
- Fabozzi F
- Faccioli P
- Fagot A
- Fallavollita F
- Fallon C
- Faltermann N
- Fanfani A
- Fang W
- Fangmeier C
- Fano L
- Fasanella D
- Fasanella G
- Faure JL
- Favart L
- Fay J
- Fedi G
- Fehling D
- Felcini M
- Feld L
- Feng L
- Feng Y
- Ferbel T
- Ferencek D
- Ferguson T
- Fernandez Bedoya C
- Fernandez Manteca PJ
- Fernandez Menendez J
- Fernandez Perez Tomei TR
- Fernandez Ramos JP
- Fernandez M
- Ferraioli C
- Ferri F
- Ferro F
- Field RD
- Fienga F
- Filipovic N
- Finco L
- Finger M
- Fiore L
- Fiorendi S
- Fiori F
- Fischer R
- Flacher H
- Flechl M
- Flix J
- Florent A
- Flores C
- Florez C
- Flouris G
- Flowers S
- Fluegge G
- Focardi E
- Folgueras S
- Fonseca De Souza S
- Fontaine J-C
- Fontanesi E
- Ford WT
- Foudas C
- Fouz MC
- Francis B
- Francois B
- Franzoni G
- Freed S
- Freeman J
- Freer C
- Freund B
- Frueboes T
- Fruehwirth R
- Fulcher J
- Funk G
- Funk W
- Gadrat S
- Galanti M
- Galati G
- Galinhas B
- Gallinaro M
- Gallo E
- Galloni C
- Gandrajula RP
- Gandrakota A
- Ganjour S
- Gao X
- Garcia Alonso A
- Garcia-Bellido A
- Garcia-Ferrero J
- Garg RB
- Garutti E
- Gary JW
- Gascon S
- Gasparini F
- Gasparini U
- Gastler D
- Gavrilenko M
- Gavrilov V
- Gecse Z
- Geiser A
- Gele D
- Gelli S
- Gelmi A
- Gennai S
- Geralis T
- Gerber CE
- Gerosa R
- Gershtein Y
- Geurts FJM
- Ghete VM
- Ghezzi A
- Ghosh S
- Ghosh S
- Giacomelli P
- Giammanco A
- Gianneios P
- Giannini L
- Giassi A
- Giffels M
- Gigi D
- Gilbert A
- Gilbert D
- Gill K
- Gilmore J
- Girgis S
- Givernaud A
- Glege F
- Gleyzer SV
- Gninenko S
- Go Y
- Godinovic N
- Godizov A
- Godshalk A
- Goerlach U
- Goh J
- Gokbulut G
- Gola M
- Goldouzian R
- Goldstein J
- Golf F
- Golovtsov V
- Golubev N
- Golutvin I
- Gomber B
- Gomez Espinosa TA
- Gomez G
- Goncharov M
- Gonzalez Caballero I
- Gonzalez Fernandez JR
- Gonzalez Hernandez CF
- Gonzalez Lopez O
- Gonzalez D
- Gonzalez ID Sandoval
- Gonzalez J Suarez
- Gorbunov I
- Gorski M
- Gottschalk E
- Gouskos L
- Gouzevitch M
- Govoni P
- Goy Lopez S
- Gozzelino A
- Grab C
- Grandi C
- Gras P
- Gray L
- Grebenyuk A
- Green D
- Greene S
- Gregores EM
- Grenier G
- Gribushin A
- Grippo MT
- Gritsan AV
- Grohsjean A
- Grothe M
- Gruchala M
- Grunendahl S
- Grunewald M
- Grynyov B
- Guchait M
- Gueth A
- Guiducci L
- Guilbaud M
- Gul M
- Guler Y
- Gulhan D
- Gulmez E
- Gunnellini P
- Gupta R
- Gurpinar E
- Gurrola A
- Gutay L
- Guthoff M
- Gutsche O
- Gyun D
- Ha S
- Haddad Y
- Hadjiiska R
- Hadley M
- Hadley NJ
- Hagopian S
- Hagopian V
- Hahn KA
- Hajdu C
- Hakala J
- Halkiadakis E
- Hall G
- Haller J
- Han J
- Hangal DA
- Hanlon J
- Hansen P
- Hanson G
- Haranko M
- Harb A
- Hardenbrook J
- Harder K
- Harper S
- Harr R
- Harrendorf MA
- Harrington C
- Harris P
- Harris RM
- Hart A
- Hartmann F
- Hasegawa S
- Hashemi B
- Hassan Q
- Hatakeyama K
- Hauk J
- Hauser J
- Havukainen J
- Haytmyradov M
- Heath GP
- Heath HF
- Hebbeker T
- Hegde V
- Hegeman J
- Heidegger C
- Heideman J
- Heidemann C
- Heikkila JK
- Heindl M
- Heindl SM
- Heintz U
- Heller R
- Henderson C
- Hensel C
- Heredia-De La Cruz I
- Hernandez JM
- Herndon M
- Herve A
- Higginbotham S
- Hildreth M
- Hill C
- Hiltbrand J
- Hindrichs O
- Hinzmann A
- Hirosky R
- Hirschauer J
- Hits D
- Hlushchenko O
- Hobson PR
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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 production of W^{\pm} W^{\pm} W^{\mp} events at \sqrt{s} = 13 TeV
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- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
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- Acharya H
- Acosta D
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- Zorbilmez C
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- Zumerle G
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- Zuolo D
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/07/2019
- Field of study
A search for the production of events containing three W bosons predicted by the standard model is reported. The search is based on a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV recorded by the CMS experiment at the CERN LHC and corresponding to a total integrated luminosity of 35.9 fb^{-1}. The search is performed in final states with three leptons (electrons or muons), or with two same-charge leptons plus two jets. The observed (expected) significance of the signal for W^{\pm} W^{\pm} W^{\mp} production is 0.60 (1.78) standard deviations, and the ratio of the measured signal yield to that expected from the standard model is 0.34_{-0.34}^{+0.62}. Limits are placed on three anomalous quartic gauge couplings and on the production of massive axionlike particles
Measurement of B_{s}^{0} meson production in pp and PbPb collisions at \sqrt{SNN}
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
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- Abdullah WATW
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- Postiau N
- Potenza R
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- Prieels C
- Primavera F
- Priyanka P
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- Psallidas A
- Ptochos F
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- Pugliese G
- Puljak I
- Purohit A
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- Rane A
- Ranieri A
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- Raspereza A
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- Redondo I
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- Roozbahani B
- Rorie J
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- Seitz C
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- Sheldon P
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- Sirois Y
- Siroli GP
- Sirunyan AM
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- Skinnari L
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- Smirnov I
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- Teroerde M
- Teyssier D
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- Tiwari PC
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- Tomalin IR
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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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- Verweij M
- Verwilligen P
- Verzetti M
- Verzocchi M
- Veszpremi V
- Vesztergombi G
- Vidal R
- Vila I
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- Viliani L
- Virdee T
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- Vlasov E
- Vlimant JR
- Voevodina E
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- 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
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- Waqas M
- Wardle N
- Wasserbaech S
- Wayand S
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- 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
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- 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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- Wulz C-E
- Wurthwein F
- Wyslouch B
- Xia F
- Xiao M
- Xiao R
- Xie S
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- 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
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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
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
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- Abercrombie D
- 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
- 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
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- Wolf M
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- Wolfe E
- Womersley WJ
- Wong K
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- Wood J
- Woodard A
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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
- 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
- Arcaro D
- 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
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- Belyaev A
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- 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
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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
Search for contact interactions and large extra dimensions in the dilepton mass spectra from proton-proton collisions at \sqrt{s} = 13 TeV
- Author
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- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
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- Abercrombie D
- Abu Zeid S
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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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