150 research outputs found
Constraints on Nucleon Decay via "Invisible" Modes from the Sudbury Neutrino Observatory
- Author
- Ahmed SN
- Anthony AE
- Beier EW
- Bellerive A
- Biller SD
- Boger J
- Boulay MG
- Bowler MG
- Bowles TJ
- Brice SJ
- Bullard TV
- Chan YD
- Chen M
- Chen X
- Cleveland BT
- Cox GA
- Dai X
- Dalnoki-Veress F
- Doe PJ
- Dosanjh RS
- Doucas G
- Dragowsky MR
- Duba CA
- Duncan FA
- Dunford M
- Dunmore JA
- Earle ED
- Elliott SR
- Evans HC
- Ewan GT
- Farine J
- Fergani H
- Fleurot F
- Formaggio JA
- Fowler MM
- Frame K
- Frati W
- Fulsom BG
- Gagnon N
- Graham K
- Grant DR
- Hahn RL
- Hall JC
- Hallin AL
- Hallman ED
- Hamer AS
- Handler WB
- Hargrove CK
- Harvey PJ
- Hazama R
- Heeger KM
- Heintzelman WJ
- Heise J
- Helmer RL
- Hemingway RJ
- Hime A
- Howe MA
- Jagam P
- Jelley NA
- Klein JR
- Kos MS
- Krumins AV
- Kutter T
- Kyba CC
- Labranche H
- Lange R
- Law J
- Lawson IT
- Lesko KT
- Leslie JR
- Levine I
- Luoma S
- MacLellan R
- Majerus S
- Mak HB
- Maneira J
- Marino AD
- McCauley N
- McDonald AB
- McGee S
- McGregor G
- Mifflin C
- Miknaitis KK
- Miller GG
- Moffat BA
- Nally CW
- Neubauer MS
- Nickel BG
- Noble AJ
- Norman EB
- Oblath NS
- Okada CE
- Ollerhead RW
- Orrell JL
- Oser SM
- Ouellet C
- Peeters SJ
- Poon AW
- Robertson BC
- Robertson RG
- Rollin E
- Rosendahl SS
- Rusu VL
- Schwendener MH
- Simard O
- Simpson JJ
- Sims CJ
- Sinclair D
- Skensved P
- Smith MW
- Starinsky N
- Stokstad RG
- Stonehill LC
- Tafirout R
- Takeuchi Y
- Tesić G
- Thomson M
- Thorman M
- Tseung HW
- Van Berg R
- Van de Water RG
- Virtue CJ
- Wall BL
- Waller D
- Waltham CE
- Wark DL
- West N
- Wilhelmy JB
- Wilkerson JF
- Wilson JR
- Wittich P
- Wouters JM
- Yeh M
- Zuber K
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2004
- Field of study
Data from the Sudbury Neutrino Observatory have been used to constrain the
lifetime for nucleon decay to ``invisible'' modes, such as n -> 3 nu. The
analysis was based on a search for gamma-rays from the de-excitation of the
residual nucleus that would result from the disappearance of either a proton or
neutron from O16. A limit of tau_inv > 2 x 10^{29} years is obtained at 90%
confidence for either neutron or proton decay modes. This is about an order of
magnitude more stringent than previous constraints on invisible proton decay
modes and 400 times more stringent than similar neutron modes.Comment: Update includes missing efficiency factor (limits change by factor of
2) Submitted to Physical Review Letter
First Neutrino Observations from the Sudbury Neutrino Observatory
- Author
- Ahmad QR
- Allen RG
- Andersen T
- Barton JC
- Beier EW
- Bigu J
- Biller S
- Black R
- Blevis I
- Boardman R
- Boger J
- Bonvin E
- Boulay MG
- Bowler M
- Bowles TJ
- Brice SJ
- Browne MC
- Buhler G
- Bullard TV
- Cameron J
- Chan YD
- Chen HH
- Chen M
- Chen X
- Chon MC
- Cleveland B
- Cowan JHM
- Cowen DF
- Dalnoki-Veress F
- Davidson W
- Doe PJ
- Doucas G
- Dragowsky M
- Duba CA
- Duncan FA
- Earle ED
- Elliott SR
- Evans HC
- Ewan GT
- Fardon R
- Farine J
- Fergami H
- Ferraris F
- Ford RJ
- Fowler MM
- Frame K
- Frank ED
- Frati W
- Germani JV
- Gil S
- Goldschmidt A
- Grant DR
- Hahn RL
- Hallin AL
- Hallman ED
- Hamer A
- Hamian AA
- Haq RU
- Hargrove CK
- Harvey PJ
- Heeger KM
- Heise J
- Helmer R
- Hepburn JD
- Heron H
- Hewett J
- Hime A
- Howard C
- Hykawy JG
- Isaac MCP
- Jagam P
- Jelley NA
- Jillings C
- Jonkmans G
- Keener PT
- Kirch K
- Klein JR
- Knox AB
- Komar RJ
- Kutter T
- Kyba C
- Law J
- Lawson IT
- Lay M
- Lee HW
- Lesko KT
- Leslie JR
- Levine I
- Locke W
- Lyon J
- MacGregor G
- Majerus S
- Mak HB
- Marino AD
- McCaulay N
- McDonald AB
- McDonald AB
- McDonald DS
- McFarlane K
- McLatchie W
- Meijer Drees R
- Moffat BA
- Moorhead M
- Nally CW
- Neubauer MS
- Newcomer FM
- Ng HS
- Noble T
- Norman EB
- Novikov VM
- O'Neill M
- Okada CE
- Ollerhead RW
- Omori M
- Orrell J
- Poon AWP
- Roberge A
- Robertson BC
- Robertson RGH
- Rowley JK
- Rusu V
- Saettler E
- Schaffer K
- Schubank R
- Schuelke A
- Schwendener MH
- Seifert H
- Shatkay M
- Shewchuk C
- Simpson JJ
- Sinclair D
- Skensved P
- Smith AR
- Smith MWE
- Steiger TD
- Stokstad RG
- Sur B
- Tafirout R
- Tagg N
- Tanner NW
- Taplin R
- Thorman M
- Trent PT
- Tserkovnyak Y
- van Berg R
- van de Water RG
- Virtue CJ
- Waltham CE
- Wang JX
- Wark DL
- West N
- Wilhelmy JB
- Wilkerson JF
- Wittich P
- Wouters JM
- Yeh M
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2000
- Field of study
The first neutrino observations from the Sudbury Neutrino Observatory are
presented from preliminary analyses. Based on energy, direction and location,
the data in the region of interest appear to be dominated by 8B solar
neutrinos, detected by the charged current reaction on deuterium and elastic
scattering from electrons, with very little background. Measurements of
radioactive backgrounds indicate that the measurement of all active neutrino
types via the neutral current reaction on deuterium will be possible with small
systematic uncertainties. Quantitative results for the fluxes observed with
these reactions will be provided when further calibrations have been completed.Comment: Latex, 7 pages, 10 figures, Invited paper at Neutrino 2000
Conference, Sudbury, Canada, June 16-21, 2000 to be published in the
Proceeding
Distinct fibroblast lineages determine dermal architecture in skin development and repair
- Author
- A Giangreco
- Anne C. Ferguson-Smith
- BA Schmidt
- Beate M. Lichtenberger
- Ben D. Simons
- C Gomez
- CA Collins
- D Gay
- DG Janson
- E Festa
- E Magnúsdóttir
- EJ Robertson
- EN Arwert
- Esther Hoste
- Fiona M. Watt
- FJ Staal
- G Egawa
- GC Gurtner
- Guillaume Pavlovic
- Kai Kretzschmar
- KB Jensen
- LE Rivers
- M Ito
- M Shah
- Marika Charalambous
- ME Page
- MH Lesko
- MV Plikus
- P Martin
- R Kalluri
- RJ Van Exan
- RR Driskell
- RR Driskell
- Ryan R. Driskell
- S Dulauroy
- S Kawamoto
- Sacri R. Ferron
- TG Hamilton
- V Horsley
- V Silva-Vargas
- Yann Herault
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2013
- Field of study
This work was funded by the Wellcome Trust (F.M.W., A.C.F.-S.),
the Medical Research Council (MRC) (F.M.W., A.C.F.-S.) and the European Union FP7
programme: TUMIC (F.M.W.), HEALING (F.M.W.) and EpigeneSys (A.C.F.-S.). B.M.L. is
the recipient of a FEBS long-term fellowship. K.K. is the recipient of a MRC PhD
Studentship. The authors acknowledge financial support from the Department of
Health via theNational Institute forHealth Research (NIHR) comprehensive Biomedical
Research Centre award to Guy’s & St Thomas’ NHS Foundation Trust in partnership
with King’s College London (KCL) and King’s College Hospital NHS Foundation
Trust. Input from M. Mastrogiannaki, A. Reimer and B. Trappmann is gratefully
acknowledged
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
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- 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
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- Girgis S
- Girone M
- Givernaud A
- Gizhko A
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- Godinovic N
- Godshalk A
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- Goh J
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- Goncharov M
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Peer reviewe
Genetic instability in the tumor microenvironment: a new look at an old neighbor
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- A Chen
- A Lochter
- A Mantovani
- A Orimo
- A Palumbo
- A Patocs
- A Planche
- A Ribas
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- A Toullec
- AC Lesko
- AD Sharrocks
- AJ Trimboli
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- B Yu
- BR Achyut
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- C-W Peng
- CA Macintosh
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- D Bacman
- D Hanahan
- D Hanahan
- D Trachootham
- DC Damin
- DC Radisky
- DC Radisky
- DG DeNardo
- DG DeNardo
- DJ Schwartzentruber
- DL Holliday
- E Farmaki
- EG Oliveira Barros De
- F Balkwill
- F Colotta
- F D’Anselmi
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- Luis Felipe Ribeiro Pinto
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- 'Springer Science and Business Media LLC'
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- Field of study
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
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search has been performed for heavy resonances decaying to ZZ or ZW in 2l2q final states, with two charged leptons (l = e, mu) produced by the decay of a Z boson, and two quarks produced by the decay of a W or Z boson. The analysis is sensitive to resonances with masses in the range from 400 to 4500 GeV. Two categories are defined based on the merged or resolved reconstruction of the hadronically decaying vector boson, optimized for high- and low-mass resonances, respectively. The search is based on data collected during 2016 by the CMS experiment at the LHC in proton-proton collisions with a center-of-mass energy of root s = 13 TeV, corresponding to an integrated luminosity of 35.9 fb(-1). No excess is observed in the data above the standard model background expectation. Upper limits on the production cross section of heavy, narrow spin-1 and spin-2 resonances are derived as a function of the resonance mass, and exclusion limits on the production of W' bosons and bulk graviton particles are calculated in the framework of the heavy vector triplet model and warped extra dimensions, respectively.A search for dark matter produced in association with top quarks in proton-proton collisions at a center-of-mass energy of 13 TeV is presented. The data set used corresponds to an integrated luminosity of 35.9 fb(-1) recorded with the CMS detector at the LHC. Whereas previous searches for neutral scalar or pseudoscalar mediators considered dark matter production in association with a top quark pair only, this analysis also includes production modes with a single top quark. The results are derived from the combination of multiple selection categories that are defined to target either the single top quark or the top quark pair signature. No significant deviations with respect to the standard model predictions are observed. The results are interpreted in the context of a simplified model in which a scalar or pseudoscalar mediator particle couples to a top quark and subsequently decays into dark matter particles. Scalar and pseudoscalar mediator particles with masses below 290 and 300 GeV, respectively, are excluded at 95% confidence level, assuming a dark matter particle mass of 1 GeV and mediator couplings to fermions and dark matter particles equal to unity.Peer reviewe
Search for the pair production of light top squarks in the e(+/-)mu(-/+) final state in proton-proton collisions at root s=13 TeV
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- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta G
- Adam W
- Adams MR
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- Publication venue
- Publication date
- 01/01/2019
- Field of study
A search for the production of a pair of top squarks at the LHC is presented. This search targets a region of parameter space where the kinematics of top squark pair production and top quark pair production are very similar, because of the mass difference between the top squark and the neutralino being close to the top quark mass. The search is performed with 35.9 fb(-1) of proton-proton collisions at a centre-of-mass energy of root s = 13 TeV, collected by the CMS detector in 2016, using events containing one electron-muon pair with opposite charge. The search is based on a precise estimate of the top quark pair background, and the use of the M-T2 variable, which combines the transverse mass of each lepton and the missing transverse momentum. No excess of events is found over the standard model predictions. Exclusion limits are placed at 95% confidence level on the production of top squarks up to masses of 208 GeV for models with a mass difference between the top squark and the lightest neutralino close to that of the top quark.Peer reviewe
Observation of a New Excited Beauty Strange Baryon Decaying to Ξb- π+π-
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- Aarup Petersen H
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- Yusli MN
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- Zorbilmez C
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- Zuolo D
- Zygala L
- Álvarez Fernández A
- Özçelik Ö
- Publication venue
- American Physical Society
- Publication date
- 01/01/2021
- Field of study
The Ξb-π+π- invariant mass spectrum is investigated with an event sample of proton-proton collisions at s=13 TeV, collected by the CMS experiment at the LHC in 2016-2018 and corresponding to an integrated luminosity of 140 fb-1. The ground state Ξb- is reconstructed via its decays to J/ψΞ- and J/ψΛK-. A narrow resonance, labeled Ξb(6100)-, is observed at a Ξb-π+π- invariant mass of 6100.3±0.2(stat)±0.1(syst)±0.6(Ξb-) MeV, where the last uncertainty reflects the precision of the Ξb- baryon mass. The upper limit on the Ξb(6100)- natural width is determined to be 1.9 MeV at 95% confidence level. The low Ξb(6100)- signal yield observed in data does not allow a measurement of the quantum numbers of the new state. However, following analogies with the established excited Ξc baryon states, the new Ξb(6100)- resonance and its decay sequence are consistent with the orbitally excited Ξb- baryon, with spin and parity quantum numbers JP=3/2-
Search for strongly interacting massive particles generating trackless jets in proton-proton collisions at s = 13 TeV
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- Zarubin A
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- Zecchinelli AG
- Zeinali M
- Zenaiev O
- Zeuner WD
- Zghiche A
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- Zielinski K
- Ziemons T
- Zientek M
- Zlebcik R
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
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- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez Fernández A
- Österberg K
- Özçelik Ö
- Široký J
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
A search for dark matter in the form of strongly interacting massive particles (SIMPs) using the CMS detector at the LHC is presented. The SIMPs would be produced in pairs that manifest themselves as pairs of jets without tracks. The energy fraction of jets carried by charged particles is used as a key discriminator to suppress efficiently the large multijet background, and the remaining background is estimated directly from data. The search is performed using proton-proton collision data corresponding to an integrated luminosity of 16.1 fb - 1 , collected with the CMS detector in 2016. No significant excess of events is observed above the expected background. For the simplified dark matter model under consideration, SIMPs with masses up to 100 GeV are excluded and further sensitivity is explored towards higher masses
Measurement of B_{s}^{0} meson production in pp and PbPb collisions at \sqrt{SNN}
- Author
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- Vorobyev A
- Voutilainen M
- Voytishin N
- Wadud MA
- Wagner SR
- Walczak M
- Walia G
- Walker M
- Wallny R
- Walsh R
- Waltenberger W
- Wamorkar T
- Wang B
- Wang D
- Wang F
- Wang H
- Wang J
- Wang L
- Wang M
- Wang Q
- Wang S
- Wang TW
- Wang X
- Wang Y
- Wang Z
- Waqas M
- Wardle N
- Wasserbaech S
- Wayand S
- Wayne M
- Weber HA
- Weber M
- 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
- Wimpenny S
- 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
- Wright D
- Wright J
- Wu Z
- Wulz C-E
- Wurthwein F
- Wyslouch B
- Xia F
- Xiao M
- Xiao R
- Xie S
- Xie W
- Xu Q
- Yagil A
- Yalvac M
- Yang UK
- Yang YC
- Yates BR
- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
- 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
- Zhang F
- Zhang H
- Zhang J
- Zhang S
- Zhang Z
- Zhao J
- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zito G
- Zobec J
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Publication venue
- 'Elsevier BV'
- Publication date
- 10/09/2019
- Field of study
The production cross sections of B_{s}^{0} mesons and charge conjugates are measured in proton-proton (pp) and PbPb collisions via the exclusive decay channel B_{s}^{0}→J/ψϕ→μ^{+}μ^{−}K^{+}K^{−} at a center-of-mass energy of 5.02 TeV per nucleon pair and within the rapidity range |y|<2.4 using the CMS detector at the LHC. The pp measurement is performed as a function of transverse momentum (p_{T}) of the B_{s}^{0} mesons in the range of 7 to 50 GeV/c and is compared to the predictions of perturbative QCD calculations. The B_{s}^{0} production yield in PbPb collisions is measured in two p_{T} intervals, 7 to 15 and 15 to 50 GeV/c, and compared to the yield in pp collisions in the same kinematic region. The nuclear modification factor (R_{AA}) is found to be 1.5±0.6(stat)±0.5(syst) for 7–15 GeV/c, and 0.87±0.30(stat)±0.17(syst) for 15–50 GeV/c, respectively. Within current uncertainties, the B_{s}^{0} results are consistent with models of strangeness enhancement, and suppression by parton energy loss, as observed for the B+ mesons
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