77 research outputs found
A closed form unwrapping method for a spherical omnidirectional view sensor
- Author
- A Agrawal
- B Micusik
- B Micusik
- C Geyer
- C Geyer
- C Geyer
- C Harris
- C Mei
- D Scaramuzza
- D Scaramuzza
- DW Rees
- F Wu
- J Gaspar
- J Hong
- J Lei
- JP Barreto
- K Yamazawa
- L Puig
- Mou Ling Dennis Wong
- N Winters
- Nguan Soon Chong
- P Vasseur
- R Swaminathan
- RA Hicks
- RI Hartley
- RO Duda
- S Baker
- S Baker
- S Derrien
- S Gasparini
- SW Jeng
- W Sturzl
- X Ying
- X Ying
- XM Deng
- Y Wu
- Y Yagi
- Yau Hee Kho
- Z Zhang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Proteomic analysis of acquired tamoxifen resistance in MCF-7 cells reveals expression signatures associated with enhanced migration
- Author
- A Biroccio
- A Heil
- A Migliaccio
- A Pierce
- AC Borley
- AE Gururaj
- AF Leary
- AF Leary
- AM Wärri
- AR Pico
- AW Hamburger
- B Gyorffy
- Bridgette M Collins-Burow
- C Zhou
- Changhua Zhou
- CK Osborne
- CK Osborne
- DM Brantley-Sieders
- DP Zelinski
- DP Zelinski
- E Shumay
- E Tokunaga
- EA Musgrove
- Elizabeth C Martin
- G Arpino
- G Hua
- Guangdi Wang
- H Chen
- H Kurokawa
- HT Tan
- Ian Townley
- IR Hutcheson
- J Austermann
- J Shou
- JM Gee
- JM Knowlden
- JM Mataraza
- L Soucek
- LM Berstein
- LV July
- Lyndsay V Rhodes
- M Kanehisa
- M Kanehisa
- M Kanehisa
- M Koltzscher
- M Lu
- M Redondo
- M Zilli
- Matthew E Burow
- MC Gutierrez
- MC Zimmermann
- Melyssa R Bratton
- MH Jeng
- MK Fuentes
- MP van Iersel
- N Hiramoto-Yamaki
- N Kang
- NA Franken
- P Fan
- P Fan
- PD Thomas
- Qiang Zhang
- Qiu Zhong
- R Cubas
- R Donato
- R Schiff
- RA McClelland
- RI Nicholson
- RI Nicholson
- S Hiscox
- S Hiscox
- S Masri
- S Massarweh
- SR Johnston
- SS Larsen
- Steven Elliott
- T Arumugam
- T Arumugam
- T Itoh
- TD Schmittgen
- WB Fang
- X Wan
- Y Chen
- Y Guo
- Y Gökmen-Polar
- Y Meng
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Femara® and the future: tailoring treatment and combination therapies with Femara
- Author
- A Argiris
- A Awada
- A Boulay
- A Brodie
- A Howell
- A Naderi
- A Naderi
- A Urruticoechea
- AH Bild
- B Aun
- BM Fendly
- CK Osborne
- CK Osborne
- CM Perou
- CR King
- CW Adams
- CW Wong
- Cynthia Ma
- D Jelovac
- DJ Slamon
- E Munzone
- EJ Filardo
- EJ Filardo
- G Arpino
- G Konecny
- GE Konecny
- GJ Clark
- GJ Sabnis
- H Ji
- H Mouridsen
- HS Rugo
- I Farmer
- I Shin
- J Baselga
- J Frasor
- J Rudloff
- J Shou
- JF Robertson
- JH Clark
- JM Gee
- JM Knowlden
- K Yu
- L Li
- L Witters
- LA Martin
- LE Shaw
- LJ van ’t Veer
- LM Berstein
- LR Kelland
- M Lacroix
- Matthew Ellis
- MH Jeng
- MJ Vijver van de
- N Alami
- P Carter
- PK Marcom
- Q Chu
- R Nahta
- RD Mass
- RI Nicholson
- RJ Santen
- RJ Santen
- RX Song
- S Laere Van
- S Masamura
- S Massarweh
- S Paik
- S Paik
- SF Doisneau-Sixou
- SL Moulder
- SR Johnston
- T Itoh
- T Kirkegaard
- T Sorlie
- T Sorlie
- TA Traina
- W Miller
- W Xia
- W Yue
- W Yue
- WR Miller
- Y Wang
- Publication venue
- Springer US
- Publication date
- 01/01/2007
- Field of study
Long-term estrogen deprivation treatment for breast cancer can, in some patients, lead to the activation of alternate cellular pathways, resulting in the re-emergence of the disease. This is a distressing scenario for oncologists and patients, but recent intensive molecular and biochemical studies are beginning to unravel these pathways, revealing opportunities for new targeted treatments. Far from making present therapies redundant, these new discoveries open the door to novel combination therapies that promise to provide enhanced efficacy or overcome treatment resistance. Letrozole, one of the most potent aromatase inhibitors, is the ideal candidate for combination therapy; indeed, it is one of the most intensively studied aromatase inhibitors in the evolving combinatorial setting. Complementary to the use of combination therapy is the development of molecular tools to identify patients who will benefit the most from these new treatments. Microarray gene profiling studies, designed to detect letrozole-responsive targets, are currently under way to understand how the use of the drug can be tailored more efficiently to specific patient needs
Steroids in kidney transplant patients
- Author
- A Chakraborty
- A Humar
- AD Kirk
- AJ Matas
- AK Trull
- B Chernow
- B Fellstrom
- B Sawitzki
- B Sprangers
- BJ Browne
- BL Kasiske
- CP Johnson
- DE Hricik
- DE Hricik
- DE Hricik
- DE Hricik
- DK Turgeon
- E Morelon
- ES Woodle
- ES Woodle
- European Mycophenolate Mofetil Cooperative Study Group
- European Mycophenolate Mofetil Cooperative Study Group
- F Kaller
- F Vincenti
- FJ Frey
- FL Luan
- G Ciancio
- G Opelz
- G Opelz
- G Opelz
- G Opelz
- H Bergrem
- HU Meier-Kriesche
- HU Meier-Kriesche
- HU Meier-Kriesche
- J Pascual
- JD Baxter
- JD Eason
- JD Schold
- JJ Augustine
- JJ Augustine
- JJ Curtis
- JJ Curtis
- JR Weisinger
- JS Bromberg
- K Solez
- KL Slayter
- KM Tornatore
- KM Tornatore
- Linda Awdishu
- M Baltzan
- M Miozzari
- M Naesens
- MG Patel
- MS Kumar Anil
- MSA Kumar
- MSA Kumar
- N Ahsan
- NM Desai
- NR Sinclair
- R Udelsman
- RG Gill
- RI Milsap
- Robert W. Steiner
- S Brouarda
- S Bunnapradist
- S Imani
- S Jeng
- S Lam
- S Rota
- SJ Wassner
- SK Mittal
- SP McDonald
- SR Knight
- T Oettl
- T Satterwhite
- TH Mathew
- TR Srinivas
- U.S. Renal Transplant Mycophenolate Mofetil Study Group
- WE Braun
- WJ Jusko
- WJ Jusko
- WY Almawi
- Publication venue
- Springer-Verlag
- Publication date
- 01/01/2011
- Field of study
Any evaluation of steroids in kidney transplantation is hampered by individual variability in metabolism, the lack of clinically available steroid blood levels, and overall little attention to steroid exposure. Many feel that steroids were an essential part of chronic immunosuppression in past decades but may no longer be necessary in low-risk populations when our newer and more potent drugs are used. Potential differences in long-term outcome will be unapparent in short-term antibody induction studies in low-risk patients, particularly with low on steroid doses, as may have happened in the recent, well-done Astellas trial. In many studies, the evidence for the superiority of mycophenolate (MMF) and tacrolimus (TAC) was not as strong as the evidence for the benefit of steroids in the Canadian cyclosporine study. As the practice of steroid withdrawal has increased, we have not seen the improvement in long-term graft survival that many expected with our newer agents. Steroids have immunosuppressive effects even in doses that are low by historic standards, and side effects may not justify their abandonment
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
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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
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- Abercrombie D
- Abu Zeid S
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- Yusli MN
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- Zanetti M
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- Zeuner WD
- Zeyrek M
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- Zhaozhong S
- Zhokin A
- Zhu DH
- Zhu RY
- Zhukov V
- Zientek M
- Zito G
- Zobec J
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- Zorbakir IS
- 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
Combination of CMS searches for heavy resonances decaying to pairs of bosons or leptons
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- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
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- Wickramage N
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- Yang UK
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- Yates BR
- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
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- Yu D
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- Yumiceva F
- Yusli MN
- Zabi A
- Zaganidis N
- Zahid S
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- Zanetti A
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- Zarubin A
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- Zecchinelli AG
- Zenaiev O
- Zenz SC
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- Zghiche A
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- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zlebcik R
- 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
- Publication date
- 01/01/2019
- Field of study
CMS Collaboration: et al.A statistical combination of searches for heavy resonances decaying to pairs of bosons or leptons is presented. The data correspond to an integrated luminosity of 35.9 fb collected during 2016 by the CMS experiment at the LHC in proton-proton collisions at a center-of-mass energy of 13 TeV. The data are found to be consistent with expectations from the standard model background. Exclusion limits are set in the context of models of spin-1 heavy vector triplets and of spin-2 bulk gravitons. For mass-degenerate W′ and Z′ resonances that predominantly couple to the standard model gauge bosons, the mass exclusion at 95% confidence level of heavy vector bosons is extended to 4.5 TeV as compared to 3.8 TeV determined from the best individual channel. This excluded mass increases to 5.0 TeV if the resonances couple predominantly to fermions.Individuals have received support from the Marie-Curie program and the European Research Council and Horizon 2020 Grant, contract Nos. 675440, 752730, and 765710 (European Union); the Programa Estatal de Fomento de la Investigación Científica y Técnica de Excelencia María de Maeztu, grant MDM-2015-0509 and the Programa Severo Ochoa del Principado de Asturias
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
- Ackert A
- Acosta D
- Acosta JG
- Acosta M Vazquez
- Adam W
- Adams MR
- Adams T
- Adzic P
- Afanasiev S
- Agapitos A
- Agaras MN
- Aggarwal A
- Aggleton R
- Agram J-L
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmed I
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
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- Albajar C
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- Alcaraz Maestre J
- Alda Junior WL
- Aleksandrov A
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- Ali MAB Md
- Alimena J
- Allen B
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- Alvarez Fernandez A
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- Alves FL
- Alves GA
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- Pozzobon N
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- Primavera F
- Prokofyev O
- Prosper H
- Psallidas A
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- Pugliese G
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- Redondo I
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- Rossi AM
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- Roy A
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- Royon C
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- Ruiz Alvarez JD
- Ruiz del Arbol P Martinez
- Ruiz Vargas JC
- Ruiz-Jimeno A
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- Ryutin R
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- Safonov A
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- Santocchia A
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- Sguazzoni G
- Shah Aashaq
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- Shalhout S
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- Shopova M
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- Solestizi L Alunni
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- Spiegel L
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- Tonelli Manganote EJ
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- Topsis-Giotis I
- Torassa E
- Toropin A
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- Tos K
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- Tsirou A
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- Tumasyan A
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- Ulmer KA
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- Uribe Estrada C
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- Vaandering EW
- Vadruccio D
- Vai I
- Vaitkus J
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- Vilela Pereira A
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- Virdee T
- Viret S
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- Vlasov E
- Vlimant JR
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- Volkov A
- Volobouev I
- Vormwald B
- Vorobiev I
- Vorobyev A
- Voutilainen M
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- Wickramage N
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- Wurthwein F
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- Yang UK
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- Yohay R
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- Yu D
- Yu GB
- Yu I
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- Yumiceva F
- Yusli MN
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- Zabi A
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- Zanetti A
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- Zhukov V
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- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- 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
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- Wissing C
- Wittich P
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- Wittmer B
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- Wolf M
- Wolf R
- Wolfe E
- Womersley WJ
- Wong K
- Wood D
- 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
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- 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
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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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