119 research outputs found
Structural Characteristics and Stellar Composition of Low Surface Brightness Disk Galaxies
- Author
- A Grafe
- A Posner
- AD Richmond
- AJ Dessler
- AJ Ridley
- AM Jorgensen
- AM Jorgensen
- BJ Anderson
- BT Tsurutani
- CE Mcllwain
- CE Rasmussen
- CJ Pollock
- CR Chappell
- CSP Brandt
- DC Delcourt
- DC Hamilton
- DE Rowland
- DG Mitchell
- DR Weimer
- DT Young
- EC Roelof
- GD Reeves
- GD Reeves
- GL Siscoe
- H-C Yeh
- IA Daglis
- IA Daglis
- IA Daglis
- II Alexeev
- J Birn
- JB Cladis
- JD Craven
- JE Borovsky
- JU Kozyra
- JU Kozyra
- JU Kozyra
- JU Kozyra
- JU Kozyra
- LA Frank
- LR Lyons
- M Grande
- M Liemohn
- M Nose
- M Sugiura
- M-C Fok
- M-C Fok
- M-C Fok
- M-C Fok
- ME Greenspan
- MF Thomsen
- MG Henderson
- MS Gussenhoven
- MW Chen
- MW Chen
- MW Chen
- MW Liemohn
- MW Liemohn
- MW Liemohn
- MW Liemohn
- MW Liemohn
- MW Liemohn
- MW Liemohn
- N Sckopke
- NE Turner
- NU Crooker
- P Michelis de
- PC Anderson
- PH Reiff
- RA Langel
- RA Wolf
- RD Belian
- RK Burton
- RL Carovillano
- RL McPherron
- RL Rairden
- S Sazykin
- S Takahashi
- S-L Akasofu
- SJ Bame
- SP Christon
- SY Fu
- TE Moore
- TE Moore
- TI Pulkkinen
- TR Brien
- TW Garner
- VK Jordanova
- VK Jordanova
- VK Jordanova
- VK Jordanova
- VK Jordanova
- W Lennartsson
- W Lyatsky
- WD Gonzalez
- WH Campbell
- WJ Burke
- WJ Burke
- Y Ebihara
- Y Ebihara
- Y Kamide
- Y Kamide
- Publication venue
- Publication date
- 01/11/1993
- Field of study
We present UBVI surface photometry of a sample of low surface brightness
(LSB) disk galaxies. LSB disk galaxies are fairly well described as exponential
disks with no preferred value for either scale length, central surface
brightness, or rotational velocity. Indeed, the distribution of scale lengths
is indistinguishable from that of high surface brightness spirals, indicating
that dynamically similar galaxies (e.g., those with comparable Rv^2) exist over
a large range in surface density.
These LSB galaxies are strikingly blue. The complete lack of correlation
between central surface brightness and color rules out any fading scenario.
Similarly, the oxygen abundances inferred from HII region spectra are
uncorrelated with color so the low metallicities are not the primary cause of
the blue colors. While these are difficult to interpret in the absence of
significant star formation, the most plausible scenario is a stellar population
with a young mean age stemming from late formation and subsequent slow
evolution.
These properties suggest that LSB disks formed from low initial overdensities
with correspondingly late collapse times.Comment: Astronomical Journal, in press 45 pages uuencoded postscript (368K)
including 9 multipart figures also available by anonymous ftp @
ftp.ast.cam.ac.uk /pub/ssm/phot.uu CAP-30-210442962983742937
New Perspectives on Substorm Injections
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/1998
- Field of study
There has been significant progress in understanding substorm injections since the Third International Conference on Substorms in 1996. Progress has come from a combination of new theories, quantitative modeling, and observations--particularly multi-satellite observations. There is now mounting evidence that fast convective flows are the mechanism that directly couples substorm processes in the mid tail, where reconnection occurs, with substorm processes the inner magnetosphere where Pi2 pulsations, auroral breakups, and substorm injections occur. This paper presents evidence that those flows combined with an earthward-propagating compressional wave are responsible for substorm injections and discusses how that model can account for various substorm injection signatures
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
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- Du R
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- Dube S
- Dubinin M
- Duchardt D
- Dudenas V
- Dudero PR
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- 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
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- Fabozzi F
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- Ferencek D
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- Fernandez Bedoya C
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- Ferraioli C
- Ferreira Parracho PG
- Ferri F
- Ferro F
- Field RD
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- Fiorendi S
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- Fisk I
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- Fonseca De Souza S
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- Ford WT
- Forthomme L
- Foudas C
- Fouz MC
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- Francois B
- Franzoni G
- Freeman J
- Friedl M
- Friese R
- Frueboes T
- Frühwirth R
- Fulcher J
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- Furic IK
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- Godinovic N
- Godshalk A
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- Goldouzian R
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- Haller J
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- Herndon M
- Hervé A
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- Horvath D
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- Huertas Guativa LM
- Hughes E
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- 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
- Innocente V
- Innocenti GM
- Iorio AOM
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- Ivanov A
- Ivanov Y
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- Jacob J
- Jafari A
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- Jeitler M
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- Josa MI
- Joshi U
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- Juodagalvis A
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- Kaestli HC
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- Kalsi AK
- Kamalieddin R
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- Kangal EE
- Kao SC
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- Kapoor A
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- Karapinar G
- Karapostoli G
- Karchin PE
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- Karmgard DJ
- Karneyeu A
- Kasemann M
- Kasieczka G
- Katkov I
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- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zeinali M
- Zenoni F
- Zenz SC
- Zeuner WD
- Zevi Della Porta G
- Zeyrek M
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhao J
- Zhokin A
- Zhu RY
- Zhukov V
- Zhukova V
- Zolkapli Z
- Zorbilmez C
- Zotto P
- Zou D
- Zsigmond AJ
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- Publication date
- 01/01/2016
- Field of study
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
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- Atakisi IO
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- Ather MW
- Attikis A
- Auffray E
- Aushev T
- Autermann C
- Auzinger G
- Avdeeva E
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- Aziz T
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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
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
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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
Measurement of B_{s}^{0} meson production in pp and PbPb collisions at \sqrt{SNN}
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdelalim AA
- Abdullah WATW
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- 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
- Ahmed I
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Al-bataineh A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aleksandrov A
- Alexander J
- Alhusseini M
- Ali MABM
- Alimena J
- Allen B
- Almond J
- Alvarez Fernandez A
- Alvarez JDR
- Alverson G
- Alves FL
- Alves GA
- Alyari M
- Amapane N
- Ambrogi F
- Amendola C
- Amin N
- Amsler C
- Anagnostou G
- Anampa KH
- Anderson D
- Andrea J
- Andreev V
- Andreev Y
- Andrews MB
- Androsov K
- Angioni GLP
- Antonelli L
- Antropov I
- Antunes De Oliveira AC
- 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 M
- Asilar E
- Askew A
- Atakisi IO
- Ather MW
- Attikis A
- Auffray E
- Aushev T
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avila C
- Ayala E
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
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- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
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- Yu I
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- Yumiceva F
- Yusli MN
- Zabi A
- Zaganidis N
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zghiche A
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- Zhu DH
- Zhu RY
- Zientek M
- Zito G
- Zobec J
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
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- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Publication venue
- 'Elsevier BV'
- Publication date
- 10/09/2019
- Field of study
The production cross sections of B_{s}^{0} mesons and charge conjugates are measured in proton-proton (pp) and PbPb collisions via the exclusive decay channel B_{s}^{0}→J/ψϕ→μ^{+}μ^{−}K^{+}K^{−} at a center-of-mass energy of 5.02 TeV per nucleon pair and within the rapidity range |y|<2.4 using the CMS detector at the LHC. The pp measurement is performed as a function of transverse momentum (p_{T}) of the B_{s}^{0} mesons in the range of 7 to 50 GeV/c and is compared to the predictions of perturbative QCD calculations. The B_{s}^{0} production yield in PbPb collisions is measured in two p_{T} intervals, 7 to 15 and 15 to 50 GeV/c, and compared to the yield in pp collisions in the same kinematic region. The nuclear modification factor (R_{AA}) is found to be 1.5±0.6(stat)±0.5(syst) for 7–15 GeV/c, and 0.87±0.30(stat)±0.17(syst) for 15–50 GeV/c, respectively. Within current uncertainties, the B_{s}^{0} results are consistent with models of strangeness enhancement, and suppression by parton energy loss, as observed for the B+ mesons
Search for Higgs boson pair production in the gamma gamma b(b)over-bar final state in pp collisions at root s=13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WAT Wan
- Abdullin S
- 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
- Al-bataineh A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Alda Junior WL
- Aleksandrov A
- Alexander J
- Ali MAB Md
- Alimena J
- Allen B
- Almond J
- Alvarez Fernandez A
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- Alves FL
- Alves GA
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- Ambrogi F
- Amendola C
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- Amsler C
- Anagnostou G
- Anampa K Hurtado
- Anderson D
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- Andreev Yu
- Andrews MB
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- Angioni GL Pinna
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- Arenton MW
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- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search is presented for the production of a pair of Higgs bosons, where one decays into two photons and the other one into a bottom quark-antiquark pair. The analysis is performed using proton-proton collision data at root s = 13 TeV recorded in 2016 by the CMS detector at the LHC, corresponding to an integrated luminosity of 35.9 fb(-1) . The results are in agreement with standard model (SM) predictions. In a search for resonant production, upper limits are set on the cross section for new spin-0 or spin-2 particles. For the SM-like nonresonant production hypothesis, the data exclude a product of cross section and branching fraction larger than 2.0 fb at 95% confidence level (CL), corresponding to about 24 times the SM prediction. Values of the effective Higgs boson self-coupling K X are constrained to be within the range -11 < K-lambda < 17 at 95% CL, assuming all other Higgs boson couplings are at their SM value. The constraints on K-lambda, are the most restrictive to date. (C) 2018 The Author(s). Published by Elsevier B.V.Peer reviewe
Measurement of the tt¯ production cross section, the top quark mass, and the strong coupling constant using dilepton events in pp collisions at √s = 13 TeV
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- Abbaneo D
- Abbiendi G
- Abbrescia M
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- Yoo J
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- Yumiceva F
- Yusli MN
- Zabi A
- Zaganidis N
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zghiche A
- Zhang A
- Zhang F
- Zhang H
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- Zhang Z
- Zhao J
- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zobec J
- Zoi I
- Zolkapli Z
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- Zorbilmez C
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- Zuolo D
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 29/04/2019
- Field of study
A measurement of the top quark–antiquark pair production cross section σtt¯ in proton–proton collisions at a centre-of-mass energy of 13TeV is presented. The data correspond to an integrated luminosity of 35.9fb−1, recorded by the CMS experiment at the CERN LHC in 2016. Dilepton events (e ± μ ∓, μ+μ−, e+e−) are selected and the cross section is measured from a likelihood fit. For a top quark mass parameter in the simulation of mMCt=172.5GeV the fit yields a measured cross section σtt¯=803±2(stat)±25(syst)±20(lumi)pb, in agreement with the expectation from the standard model calculation at next-to-next-to-leading order. A simultaneous fit of the cross section and the top quark mass parameter in the POWHEG simulation is performed. The measured value of mMCt=172.33±0.14(stat)+0.66−0.72(syst)GeV is in good agreement with previous measurements. The resulting cross section is used, together with the theoretical prediction, to determine the top quark mass and to extract a value of the strong coupling constant with different sets of parton distribution functions
Search for 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
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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
Measurement of the WZ production cross section in pp collisions at root s=13 Tev
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- Scharf C
- Scheuch F
- Schieck J
- Schleper P
- Schmidt A
- Schmitt MH
- Schnaible C
- Schnetzer S
- Schoerner-Sadenius T
- Schofbeck R
- Schomakers C
- Schonenberger M
- Schroeder M
- Schulte JF
- Schulz J
- Schumann S
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- Sciacca C
- Scodellaro L
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- Sevilla MF
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- Sieber G
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- Siroli GP
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- Steggemann J
- Steinbrueck G
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- Strauss J
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- Stupak J
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- Suarez Andres I
- Suarez I
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- Sudic L
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- Sultanov G
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- Troendle D
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- Tuominiemi J
- Tuovinen E
- Turkcapar S
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- Tzeng YM
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- Ujvari B
- Ulmer KA
- Ulrich R
- Undleeb S
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- Veszpremi V
- Vesztergombi G
- Veverka J
- Vidal R
- Vignali MC
- Vila I
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- Vorobiev I
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- Wulsin HW
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- Wurthwein F
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- Xia F
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- Publication venue
- Publication date
- 01/01/2015
- Field of study
Peer reviewe
- …