192 research outputs found
Functions of Intermittent Locomotion in Mustached Tamarins (Saguinus mystax)
- Author
- A Treves
- AC Smith
- AG McAdam
- AG Pook
- BG Galef
- BT Hirsch
- C Ique
- C Schradin
- CA Peres
- CP Schaik van
- DL Kramer
- E Fernandez-Juricic
- E Pennisi
- EB Edwards
- Eckhard W. Heymann
- EW Heymann
- EW Heymann
- EW Heymann
- EW Heymann
- EZ Cameron
- F Encarnación
- G Cowlishaw
- G Martell
- HM Buchanan-Smith
- HM Buchanan-Smith
- HR Pulliam
- I Girard
- J Terborgh
- J Zar
- LA Ebensperger
- M Cords
- M Stojan-Dolar
- MA Tornow
- MC Yáber
- ME Jones
- MF Land
- MJ Childress
- Mojca Stojan-Dolar
- MR Oversluijs Vasquez
- N Shahuano Tello
- NG Caine
- P Löttker
- P Martin
- PA Garber
- PA Garber
- PA Garber
- R Avery
- R Steenbeek
- RA Hill
- RA Vasquez
- RB Weinstein
- RB Weinstein
- RB Weinstein
- RB Weinstein
- RW Wrangham
- S Boinski
- T Caro
- TM Williams
- TT Struhsaker
- TV Hancock
- VL Billat
- W Trouilloud
- WD Hamilton
- Publication venue
- Springer US
- Publication date
- 01/01/2010
- Field of study
Many animals interrupt their moving with brief pauses, which appear to serve several different functions. We examined the function of such intermittent locomotion in wild living mustached tamarins (Saguinus mystax), small arboreal New World primates that form mixed-species groups with saddleback tamarins (Saguinus fuscicollis). We investigated how different environmental and social factors affect pausing during locomotion and used these data to infer the function of this behavior. As measures of intermittent locomotion, we used percentage of time spent pausing and pause rate. We considered 3 possible functions that are not mutually exclusive: increased endurance, route planning, and antipredator vigilance. Mustached tamarins spent on average (mean ± SE) 55.1 ± 1.0% of time pausing, which makes effective resource exploitation more time consuming and needs to be outweighed by correspondingly large benefits. Percentage of time spent pausing decreased in larger mixed-species groups vs. smaller mixed-species groups and decreased with height and in monkeys carrying infants. It was not affected by sex, age, spatial arrangement, or single-species group size. Pause rate increased in individuals traveling independently compared to those traveling in file, but was not affected by other factors. The group size effect in mixed-species groups lends support to the notion that pausing during locomotion is an antipredator tactic that can be reduced in the increased safety of larger groups, but other results suggest that additional functions, particularly route planning, are also of great importance. Benefits in terms of predator confusion and group movement coordination are also likely to play a role and remain a topic for further research
The range of the golden-mantle tamarin, Saguinus tripartitus (Milne Edwards, 1878): distributions and sympatry of four tamarin species in Colombia, Ecuador, and northern Peru
- Author
- A Bravo
- AB Rylands
- AB Rylands
- AG Pook
- AJ Moore
- Anthony B. Rylands
- AR Borman
- C Freese
- CA Peres
- CA Peres
- CE Kostrub
- Christian Matauschek
- CP Groves
- CP Groves
- D Tirira
- DA Nickle
- Eckhard W. Heymann
- EW Heymann
- EW Heymann
- EW Heymann
- EW Heymann
- EW Heymann
- F Röhe
- FD Ávila-Pires de
- Filomeno Encarnación
- HM Buchanan-Smith
- HM Buchanan-Smith
- J Hernández-Camacho
- J Hernández-Camacho
- J Terborgh
- JA Nyakatura
- JC Bicca-Marques
- JM Cheverud
- K Izawa
- M Moynihan
- M Yoneda
- N Vargas Tovar
- O Montenegro
- P Hershkovitz
- P Hershkovitz
- P Hershkovitz
- P Soini
- PA Garber
- PA Garber
- PA Keddy
- PH Napier
- R Aquino
- R Aquino
- R Castro
- R Ulloa Vaca
- RJ Putman
- Rolando Aquino
- Russell A. Mittermeier
- RW Thorington Jr
- S la Torre de
- S la Torre de
- S la Torre de
- S la Torre de
- SJ Cropp
- Stella de la Torre
- TR Defler
- TR Defler
- TW Schoener
- TW Schoener
- VL Albuja
- Publication venue
- Springer Japan
- Publication date
- 01/01/2010
- Field of study
A detailed understanding of the range of the golden-mantle tamarin, Saguinus tripartitus (Milne Edwards, 1878), in Amazonian Peru and Ecuador is of particular relevance, not only because it is poorly known but also because it was on the basis of its supposed sympatry with the saddleback tamarin (S. fuscicollis lagonotus) that Thorington (Am J Primatol 15:367–371, 1988) argued that it is a distinct species rather than a saddleback tamarin subspecies, as was believed by Hershkovitz (Living new world monkeys, vol I. The University of Chicago Press, Chicago, 1977). A number of surveys have been carried out since 1988 in the supposed range of S. tripartitus, in both Ecuador and Peru. Here we summarize and discuss these issues and provide a new suggestion for the geographic range of this species; that is, between the ríos Napo and Curaray in Peru and extending east into Ecuador. We also review current evidence for the distributions of Spix’s black-mantle tamarin (S. nigricollis nigricollis), Graells’ black-mantle tamarin (S. n. graellsi), and the saddleback tamarin (S. fuscicollis lagonotus), which are also poorly known, and examine the evidence regarding sympatry between them. We conclude that despite the existence of a number of specimens with collecting localities that indicate overlap in their geographic ranges, the fact that the four tamarin species are of similar size and undoubtedly very similar in their feeding habits militates strongly against the occurrence of sympatry among them
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
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- Fiorendi S
- Fiori F
- Fischer R
- Fisk I
- Flacher H
- Flanagan W
- Flechl M
- Flix J
- Florent A
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- Florez C
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- Flowers S
- Flügge G
- Focardi E
- Foerster M
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- 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
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- Garcia-Bellido A
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- Gasparini F
- Gasparini U
- Gastler D
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- Gavrilov V
- Geenen H
- Geffert P
- Geiser A
- Geisler M
- Gelli S
- Gelé D
- Gennai S
- George C
- George J
- Geralis T
- Gerber CE
- Gerosa R
- Gershtein Y
- Geurts FJM
- Ghete VM
- Ghezzi A
- Ghosh S
- Ghosh S
- Giacomelli P
- Giakoumopoulou VA
- Giammanco A
- Giassi A
- Giffels M
- Gigi D
- Gilbert A
- Gill K
- Gilmore J
- Giordano F
- Girgis S
- Girone M
- Givernaud A
- Gizhko A
- Glege F
- Glushkov I
- Gninenko S
- Go Y
- Godinovic N
- Godshalk A
- Goebel K
- Goerlach U
- Goh J
- Gokbulut G
- Goldouzian R
- Goldstein J
- Golf F
- Golovtsov V
- Golubev N
- Golutvin I
- Gomber B
- Gomez Ceballos G
- Gomez G
- Gomez JA
- Gomez JP
- Goncharov M
- Gonzalez Caballero I
- Gonzalez Lopez O
- Gonzalez Suarez R
- Gonzalez D
- Goodell J
- Gorbounov N
- Gorbunov I
- Gori V
- Gottschalk E
- Gouskos L
- Gouzevitch M
- Govoni P
- Goy Lopez S
- Gozzelino A
- Grab C
- Grados Luyando JM
- Gran J
- Grandi C
- Granier de Cassagnac R
- Gras P
- Gray L
- Grebenyuk A
- Green D
- Greene S
- Gregores EM
- Grenier G
- Gribushin A
- Grimes M
- Grippo MT
- Gritsan AV
- Grothe M
- Grunewald M
- Grynyov B
- Grünendahl S
- Guchait M
- Gude A
- Guiducci L
- Guilbaud M
- Gul M
- Guler Y
- Gulhan D
- Gundacker S
- Gunnellini P
- Gupta R
- Gurpinar E
- Gurrola A
- Gurtu A
- Gutay L
- Guthoff M
- Gutsche O
- Gyun D
- Gómez Espinosa TA
- Górski M
- Görner M
- Gülmez E
- Güth A
- Ha S
- Haddad Y
- Hadjiiska R
- Hadley NJ
- Hagopian S
- Hagopian V
- Hahn KA
- Haitz D
- Hajdu C
- Hakala J
- Halkiadakis E
- Hall G
- Haller J
- Hamel de Monchenault G
- Hammer J
- Han J
- Hansen P
- Hanson G
- Harb A
- Hardenbrook J
- Harder K
- Hare D
- Harper S
- Harr R
- Harrington C
- Harris P
- Harris RM
- Hart A
- Hartl C
- Hartmann F
- Hasegawa S
- Hassan Q
- Hatakeyama K
- Hauk J
- Hauser J
- Haytmyradov M
- Heath GP
- Heath HF
- Hebbeker T
- Hebda P
- Hegeman J
- Heidegger C
- Heideman J
- Heidemann C
- Heilman J
- Heindl M
- Heindl SM
- Heintz U
- Heister A
- Heller R
- Hempel M
- Henderson C
- Hensel C
- Heracleous N
- Heredia-De La Cruz I
- Hernandez JM
- Hernandez-Almada A
- Herndon M
- Hervé A
- Hidas D
- Hidas P
- Hildreth M
- Hill C
- Hindrichs O
- Hinzmann A
- Hirosky R
- Hirschauer J
- Hits D
- Hobson PR
- Hoehle F
- Hoepfner K
- Hoffmann M
- Hofman DJ
- Hohlmann M
- Hollar J
- Holzner A
- Hong B
- Hoorani HR
- Horisberger R
- Hortiangtham A
- Horvath D
- Hos I
- Hoss J
- Hou W-S
- Hreus T
- Hrubec J
- Hsiung Y
- Hsu D
- Hu Z
- Huang T
- Huertas Guativa LM
- Hughes E
- Hughes R
- Hurtado Anampa K
- Husemann U
- Härkönen J
- Höing RS
- Hörmann N
- Iaselli G
- Iashvili I
- Iaydjiev P
- Ibrahim ZA
- Ignatenko M
- Iiyama Y
- Iles G
- Ille B
- Incandela J
- Ingram Q
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- Publication venue
- Publication date
- 01/01/2016
- Field of study
Peer reviewe
Search for strongly interacting massive particles generating trackless jets in proton-proton collisions at s = 13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- Wolf R
- Wolfe E
- Wong K
- Wong WY
- Wood D
- Woodard A
- Wozniak KA
- Wozniewski S
- Wright D
- Wu Z
- Wuchterl S
- Wulz C-E
- Wuyckens S
- Wyslouch B
- Würthwein F
- Xia F
- Xiao J
- Xiao M
- Xiao R
- Xie S
- Xie W
- Yagil A
- Yalvac M
- Yan F
- Yang UK
- Yang YC
- Yao Y
- Yarar H
- Yates BR
- Yazgan E
- Ye Z
- Yetkin EA
- Yi K
- Yohay R
- Yoo HD
- Yoo J
- Yoon I
- You Z
- Yu D
- Yu GB
- Yu I
- Yu SS
- Yuan L
- Yuan S
- Yuldashev BS
- Yumiceva F
- Yusli MN
- Zabi A
- Zacharopoulou A
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli AG
- Zeinali M
- Zenaiev O
- Zeuner WD
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang S
- Zhang W
- Zhang Y
- Zhang Z
- Zhao J
- Zhokin A
- Zhu DH
- Zhu RY
- Zich J
- Zielinski K
- Ziemons T
- Zientek M
- Zlebcik R
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- 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
Combination of CMS searches for heavy resonances decaying to pairs of bosons or leptons
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams MR
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- Adan D Perez
- Adzic P
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- Agapitos A
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
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- Ahmad W Haj
- Ahuja S
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- Alcaraz Maestre J
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- Krolikowski J
- Kropivnitskaya A
- Kruecker D
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- Kubota Y
- Kucher I
- Kudella S
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- Kuo CM
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- Lagarde F
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- Lehti S
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- Lelas D
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- Neutelings I
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- Novak A
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- Obertino MM
- Obraztsov S
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- Ojalvo I
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- Organtini G
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- Padula Sandra S
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- Palencia Cortezon E
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- Postiau N
- Potenza R
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- Pozdnyakov A
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- Prado Da Silva WL
- Presilla M
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- Prisciandaro J
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- Rane A
- Ranieri A
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- Rappoccio S
- Raspereza A
- Rastogi A
- Rath Y
- Rathjens D
- Ratti SP
- Rauch MP
- Rauco G
- Ravera F
- Raymond DM
- Razis PA
- Re V
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- Rebello Teles P
- Redjimi R
- Redondo I
- Regnard S
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- Reimers A
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- Reithler H
- Rembser J
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- Rodriguez Bouza V
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- Roguljic M
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- Rolandi G
- Romeo F
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- Ronchese P
- Roozbahani B
- Rorie J
- Rose A
- Rosenzweig D
- Roskas C
- Roskes J
- Rosowsky A
- Rossi A
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- Rossin R
- Rout PK
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- Rovere M
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- Ruggles T
- Ruini D
- Ruiz del Arbol P Martinez
- Ruiz-Jimeno A
- Rumerio P
- Rusack R
- Ruspa M
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- Ryutin R
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- Saggio A
- Sagir S
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- Sandeep K
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- Santanastasio F
- Santocchia A
- Santoro A
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- Sauvan JB
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- Scodellaro L
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- Seitz C
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- Sekmen S
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- Seo SH
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- Sevilla M Franco
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- Sfar H Rejeb
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- Shah Aashaq
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- Shopova M
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- Sirois Y
- Siroli GP
- Sirunyan AM
- Skatchkov N
- Skinnari L
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- Skuja A
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- Smirnov I
- Smirnov V
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- Snow GR
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- Sola V
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- Tiwari PC
- Tkaczyk S
- Tlisov D
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- Toropin A
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- Tos K
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- Tran NV
- Treille D
- Trevisani N
- Triantis FA
- Tricomi A
- Triossi A
- Tripathi M
- Trocino D
- Trocsanyi ZL
- Troshin S
- Trovato M
- Tsamalaidze Z
- Tsiakkouri D
- Tsipolitis G
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- Tumasyan A
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- Tuominen E
- Tuominiemi J
- Turkcapar S
- Turkot O
- Tuuva T
- Tuve C
- Tytgat M
- Tyurin N
- Uchida K
- Ujvari B
- Ulmer KA
- Ulrich R
- Undleeb S
- Uniyal R
- Uplegger L
- Uribe Estrada C
- Usai E
- Uvarov L
- Uzunian A
- Vaandering EW
- Vagnerini A
- Vai I
- Vaitkus J
- Valencia Palomo L
- Valuev V
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- Van Parijs I
- Van Putte S
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- Vander Velde C
- Vanlaer P
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- Veelken C
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- Velkovska J
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- Venditti R
- Venturi A
- Verbeke W
- Verdini PG
- Veres GI
- Verma Ravindra Kumar
- Vermassen B
- Vernieri C
- Verweij M
- Verwilligen P
- Verzetti M
- Verzocchi M
- Veszpremi V
- Vesztergombi G
- Vidal R
- Vila I
- Vilela Pereira A
- Viliani L
- Virdee T
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- Vitulo P
- Vizan Garcia JM
- Vlasov E
- Vlimant JR
- Voevodina E
- Volkov A
- Volobouev I
- Vormwald B
- Vorobiev I
- Vorobyev A
- Voutilainen M
- Voytishin N
- Wadud MA
- Wagner SR
- Walczak M
- Walia G
- Wallny R
- Walsh R
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- Wamorkar T
- Wang B
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- Wang J
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- Wang X
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- Waqas M
- Wardle N
- Watson I
- Wayne M
- Weber HA
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- Wei H
- Weinberg M
- Wen Y
- Wertz S
- West C
- Wetzel J
- Whitbeck A
- Wichmann K
- Wickramage N
- Wiedenbeck S
- Wiederkehr SA
- Wightman A
- Williams J
- Williams T
- Willmott C
- 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
- Woodard A
- Woods N
- Wright D
- Wright J
- Wrthwein F
- Wu Z
- Wulz C-E
- Wyslouch B
- Xia F
- Xiao M
- Xiao R
- Xie S
- Xie W
- Yagil A
- Yalvac M
- Yang UK
- Yang YC
- Yates BR
- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
- Yoon I
- 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
- Zecchinelli AG
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zghiche A
- Zhang A
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- Zhang J
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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
Evidence for Top Quark Production in Nucleus-Nucleus Collisions
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- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
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- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2019
- Field of study
Peer reviewe
Search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks in proton-proton collisions at root s=13TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
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- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks is performed in proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC. The analyzed data sample corresponds to an integrated luminosity of 35.9 fb(-1). The signal is characterized by a large missing transverse momentum recoiling against a bottom quark-antiquark system that has a large Lorentz boost. The number of events observed in the data is consistent with the standard model background prediction. Results are interpreted in terms of limits both on parameters of the type-2 two-Higgs doublet model extended by an additional light pseudoscalar boson a (2HDM+a) and on parameters of a baryonic Z simplified model. The 2HDM+a model is tested experimentally for the first time. For the baryonic Z model, the presented results constitute the most stringent constraints to date.Peer reviewe
Search for dark matter produced in association with a single top quark or a top quark pair in proton-proton collisions at s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- 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
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- Yusli MN
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- Zuolo D
- 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
- 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 G
- 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
- Alexakhin V
- 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 GL 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
- 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
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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 the B-s(0) -> X(3872)phi Decay
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- Acharya H
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- Publication venue
- Publication date
- 01/01/2020
- Field of study
Using a data sample of proton-proton collisions at root s = 13 TeV, corresponding to an integrated luminosity of 140 fb(-1) collected by the CMS experiment in 2016-2018, the B-s(0) -> X(3872)phi decay is observed. Decays into J/psi pi(+)pi(-) and K+K- are used to reconstruct, respectively, the X(3872) and phi. The ratio of the product of branching fractions B[B-s(0) -> X(3872)phi]B[X(3872) -> J/psi pi(+)pi(-)] to the product B[B-s(0) ->psi(2S)phi]B[psi(2S) -> J/psi pi(+)pi(-)] is measured to be [2.21 +/- 0.29(stat) +/- 0.17(syst)]%. The ratio B[B-s(0) -> X(3872)phi]/B[B-0 -> X(3872)K-0] is found to be consistent with one, while the ratio B[B-s(0) -> X(3872)phi]/B[B+-> X(3872)K+] is two times smaller. This suggests a difference in the production dynamics of the X(3872) in B-0 and B(0)s meson decays compared to B+. The reported observation may shed new light on the nature of the X(3872) particle.Peer reviewe
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