170 research outputs found
Modeling and energy consumption evaluation of a stochastic wireless sensor network
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- 'Springer Science and Business Media LLC'
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- Field of study
Measurement of the Bottom-Strange Meson Mixing Phase in the Full CDF Data Set
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- Terada LS
- Terman A
- Tettamanti G
- Thevissen K
- Thom
- Thome
- Thompson
- Thompson CB
- Thomson
- Thorburn A
- Thumm M
- Tian F
- Tian Y
- Toback
- Tocchini-Valentini G
- Tokar
- Tolkovsky AM
- Tollefson
- Tomino Y
- Tomura
- Tonelli
- Tooze SA
- Torre
- Torretta
- Totaro
- Tournier C
- Tower J
- Towns R
- Trajkovic V
- Travassos LH
- Trovato
- Tsai TF
- Tschan MP
- Tsubata T
- Tsung A
- Turk B
- Turner LS
- Tyagi SC
- Tönges L
- U.
- U.K.
- Uchiyama Y
- Ueno T
- Ukegawa
- Umekawa M
- Umemiya-Shira
- Uozumi
- V.
- V.
- V.
- V.
- V.
- V.
- V.
- V.
- V.
- V.
- V.E.
- Varganov
- Velev
- Vellidis
- Vidal
- Vila
- Vilar
- VizĂĄn
- Vogel
- Volpi
- VĂĄzquez
- W.
- W.
- W.
- W.
- W.-M.
- W.C.
- W.H.
- W.K.
- Wagner
- Wagner
- Wakisaka
- Wallny
- Wang
- Warburton
- Waters
- Wester
- Whiteson
- Wick
- Wicklund
- Wicklund
- Wilbur
- Williams
- Wilson
- Wilson
- Winer
- Wittich
- Wolbers
- Wolfe
- Wright
- Wu
- Wu
- X.
- Y.
- Y.
- Y.
- Y.
- Y.
- Y.
- Y.
- Y.
- Y.C.
- Y.C.
- Y.D.
- Y.J.
- Y.K.
- Y.S.
- Yamamoto
- Yamato
- Yang
- Yang
- Yang
- Yao
- Yeh
- Yi
- Yoh
- Yorita
- Yoshida
- Yu
- Yu
- Yu
- Yun
- Z.
- Zanetti
- Zeng
- Zhou
- Zucchelli
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
We report a measurement of the bottom-strange meson mixing phase \beta_s
using the time evolution of B0_s -> J/\psi (->\mu+\mu-) \phi (-> K+ K-) decays
in which the quark-flavor content of the bottom-strange meson is identified at
production. This measurement uses the full data set of proton-antiproton
collisions at sqrt(s)= 1.96 TeV collected by the Collider Detector experiment
at the Fermilab Tevatron, corresponding to 9.6 fb-1 of integrated luminosity.
We report confidence regions in the two-dimensional space of \beta_s and the
B0_s decay-width difference \Delta\Gamma_s, and measure \beta_s in [-\pi/2,
-1.51] U [-0.06, 0.30] U [1.26, \pi/2] at the 68% confidence level, in
agreement with the standard model expectation. Assuming the standard model
value of \beta_s, we also determine \Delta\Gamma_s = 0.068 +- 0.026 (stat) +-
0.009 (syst) ps-1 and the mean B0_s lifetime, \tau_s = 1.528 +- 0.019 (stat) +-
0.009 (syst) ps, which are consistent and competitive with determinations by
other experiments.Comment: 8 pages, 2 figures, Phys. Rev. Lett 109, 171802 (2012
The Interaction Between Pubertal Timing and Peer Popularity for Boys and Girls: An Integration of Biological and Interpersonal Perspectives on Adolescent Depression
- Author
- A Angold
- A Angold
- A Caspi
- A Furnham
- A Michael
- AC Carle
- AC Petersen
- AHN Cillessen
- AHN Cillessen
- AJ Rose
- AM Greca La
- BB Brown
- BL Hankin
- C Benjet
- Caroline B. Adelman
- CB Stroud
- CE Rucker
- CJ Boyatzis
- CK McBride
- CS Conley
- D Carlson Jones
- D Eder
- E Nadeem
- E Stice
- ES Chevron
- Evelien A. P. Poelen
- FD Alsaker
- GC Patton
- GN Holmbeck
- Hanneke A. Teunissen
- J Brooks-Gunn
- J Canals
- J Kroger
- J Rierdan
- JA Graber
- JC Cogan
- JD Coie
- JG Parker
- JM Siegel
- JT Parkhurst
- KD Rudolph
- KD Rudolph
- KD Rudolph
- KM LaFontana
- LD Dorn
- LD Dorn
- LJ Crockett
- LY Abramson
- LY Abramson
- M Kovacs
- M Kovacs
- ME Herman-Giddens
- Mitchell J. Prinstein
- MJ Prinstein
- MJ Prinstein
- MR Smucker
- R Kaltiala-Heino
- RC Savin-Williams
- Renske Spijkerman
- RK Silbereisen
- RM Lee
- RM Lerner
- Ron H. J. Scholte
- Rutger C. M. E. Engels
- S Fergus
- SE Finkel
- SL Bem
- SP Hinshaw
- SS Wang
- TD Little
- TRG Gladstone
- WM Craig
- X Ge
- X Ge
- X Ge
- XL Jiang
- Publication venue
- Springer US
- Publication date
- 01/01/2010
- Field of study
The transition to adolescence marks a time of sharply increased vulnerability to the development of depression, particularly among girls. Past research has examined isolated risk factors from individual theoretical models (e.g., biological, interpersonal, and cognitive) of depression, but few have examined integrative models. This study investigated the conjoint effects of early pubertal timing and popularity in the longitudinal prediction of depressive symptoms. A total of 319 girls and 294 boys (ages 11â14) provided information on their pubertal status, depressive symptoms, and the social status (i.e., popularity) of their peers. Adolescents completed a second measure of depressive symptoms 11Â months after the initial time point. Findings supported an integrated biological-interpersonal model in explaining the development of depressive symptoms during adolescence. Early pubertal development was associated with increase in depressive symptoms only when accompanied by low levels of popularity. High levels of popularity buffered the association between early pubertal development and later depressive symptoms. Unexpectedly, these results were significant both for girls and boys. Results are discussed in terms of dynamic systems theories
An Anomalous Type IV Secretion System in Rickettsia Is Evolutionarily Conserved
- Author
- A Angot
- A Beijersbergen
- A Carle
- A Covacci
- A Das
- A Karnholz
- A Krogh
- A Paschos
- A Rambaut
- A Shamaei-Tousi
- A Stern
- AB den Hartigh
- Abdu F. Azad
- AC Darling
- AC Vergunst
- AF Azad
- AF Azad
- AF Azad
- AJ Dijkstra
- AL Jones
- AL Jones
- AL Koch
- AR Mushegian
- AS Betzner
- AS Juncker
- B Nystedt
- BR Berger
- BR Berger
- Bruno S. Sobral
- C Baron
- C Baron
- C Baron
- C Baron
- C Dehio
- C Hoppner
- CC Chao
- CC Chao
- CE Beaupre
- CI Kado
- CR Roy
- D Fernandez
- D Fernandez
- D Hofreuter
- D Maher
- D Medini
- D Posada
- D Zahrl
- DH Walker
- DL Burns
- DR Stothard
- DV Thompson
- DV Ward
- DV Ward
- DW Ellison
- E Cascales
- E Cascales
- E Cascales
- E De Buck
- E Lanka
- E Rances
- ED Segal
- EE Snyder
- EJ van Asselt
- EM Dale
- EM Lai
- EM Lai
- EM Lai
- EM Lai
- EV Koonin
- F Ronquist
- G Blanc
- G Koraimann
- G Patey
- G Salmond
- G Segal
- G Segal
- GA Kuldau
- GD Baldridge
- GD Baldridge
- GE Crooks
- GJ Olsen
- GM Spudich
- GW Tyson
- H Ge
- H Lehnherr
- H Nagai
- H Ogata
- H Ogata
- H Ogata
- H Ogata
- H Schmidt-Eisenlohr
- H Schmidt-Eisenlohr
- HH Fuxelius
- HH Fuxelius
- HJ Yeo
- HJ Yeo
- HL Saenz
- I Draskovic
- J Andrzejewska
- J Bohne
- J Hall
- J Peters
- J Tanaka
- J Winiecka-Krusnell
- J Winiecka-Krusnell
- J Winiecka-Krusnell
- J Zupan
- J Zupan
- JA Malek
- JA Sexton
- JC Wilgenbusch
- JD Bendtsen
- JD Robertus
- JE Ward
- JE Ward
- JE Ward Jr
- JE Ward Jr
- JE Ward Jr
- JJ Gillespie
- JJ Gillespie
- JJ Martinez
- Joao C. Setubal
- Joseph J. Gillespie
- JP Huelsenbeck
- JP Vogel
- K Arnold
- K Shirasu
- K Shirasu
- KA Aly
- KE Finberg
- KJ Fullner
- KJ Fullner
- KM Stephens
- KP Williams
- L Krall
- L Terradot
- LA Weinert
- LB Anderson
- M Bayer
- M Bayer
- M Dozot
- M Duckely
- M Horn
- M Kalkum
- M Lessl
- M Llosa
- M Ogawa
- M Rohde
- M Watarai
- M. Sayeedur Rahman
- MA Escobar
- Micah J. Worley
- ML Boschiroli
- MP McLeod
- MR Brown
- MV La
- MW Gray
- MY Abajy
- N Bayan
- N Ohashi
- NC Ammerman
- NH Cho
- Nicole C. Ammerman
- NT Blackburn
- O Draper
- P Bandyopadhyay
- P Guyon
- PJ Christie
- PJ Christie
- PJ Christie
- PJ Christie
- PJ Christie
- PJ Christie
- PK Judd
- PK Judd
- Q Yuan
- R Bayliss
- R Cox
- R Eisenbrandt
- R Eisenbrandt
- R Middleton
- R Schulein
- RB Kumar
- RC Edgar
- RC Edgar
- RL Harris
- S Backert
- S Bailey
- S Hapfelmeier
- S Hare
- S Hare
- S Kutter
- S Masui
- S Metzger
- S Okamoto
- S Rashkova
- SC Winans
- SC Winans
- SE Stachel
- SG Andersson
- SG Andersson
- SG Andersson
- Sheila M. Dreher-Lesnick
- SJ Jakubowski
- SJ Jakubowski
- SJ Jakubowski
- SM Dreher-Lesnick
- Stefan Bereswill
- T Tzfira
- T Tzfira
- TA Dang
- TB Cao
- TD Lawley
- TD Schneider
- TJ Rowbotham
- TR Fritsche
- TS Lin
- V Citovsky
- V Norris
- V Sagulenko
- W Fischer
- W Pansegrau
- W Vollmer
- WG Weisburg
- YR Thorstenson
- Z Cheng
- Z Liu
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2009
- Field of study
Bacterial type IV secretion systems (T4SSs) comprise a diverse transporter family functioning in conjugation, competence, and effector molecule (DNA and/or protein) translocation. Thirteen genome sequences from Rickettsia, obligate intracellular symbionts/pathogens of a wide range of eukaryotes, have revealed a reduced T4SS relative to the Agrobacterium tumefaciens archetype (vir). However, the Rickettsia T4SS has not been functionally characterized for its role in symbiosis/virulence, and none of its substrates are known.Superimposition of T4SS structural/functional information over previously identified Rickettsia components implicate a functional Rickettsia T4SS. virB4, virB8 and virB9 are duplicated, yet only one copy of each has the conserved features of similar genes in other T4SSs. An extraordinarily duplicated VirB6 gene encodes five hydrophobic proteins conserved only in a short region known to be involved in DNA transfer in A. tumefaciens. virB1, virB2 and virB7 are newly identified, revealing a Rickettsia T4SS lacking only virB5 relative to the vir archetype. Phylogeny estimation suggests vertical inheritance of all components, despite gene rearrangements into an archipelago of five islets. Similarities of Rickettsia VirB7/VirB9 to ComB7/ComB9 proteins of epsilon-proteobacteria, as well as phylogenetic affinities to the Legionella lvh T4SS, imply the Rickettsiales ancestor acquired a vir-like locus from distantly related bacteria, perhaps while residing in a protozoan host. Modern modifications of these systems likely reflect diversification with various eukaryotic host cells.We present the rvh (Rickettsiales vir homolog) T4SS, an evolutionary conserved transporter with an unknown role in rickettsial biology. This work lays the foundation for future laboratory characterization of this system, and also identifies the Legionella lvh T4SS as a suitable genetic model
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
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams E
- Adams MR
- Adams T
- Adloff C
- Adzic P
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmed A
- Ahuja S
- Aime C
- Akchurin N
- Akgun B
- Akpinar A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aldaya Martin M
- AldĂĄ JĂșnior WL
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Allen B
- Almond J
- Alvarez Gonzalez B
- Alverson G
- Alves GA
- Aly R
- Alyari M
- Amapane N
- Amendola C
- Amin N
- Amram O
- Amsler C
- Anagnostou G
- Andrea J
- Andreev V
- Andreev Y
- Andrews MB
- Androsov K
- Antchev G
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Apyan A
- Araujo M
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arneodo M
- Aruta C
- Asavapibhop B
- Asawatangtrakuldee C
- Asenov P
- Asghar MI
- Asilar E
- Askew A
- Asmuss P
- Aspell P
- Atakisi IO
- Atanassov I
- Ather MW
- Attikis A
- Auffray E
- Aushev T
- Auzinger G
- Avati V
- Avery P
- Avila C
- Awais A
- Awan MIM
- Ayala E
- Ayala G
- Aydogmus Sen F
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzurri P
- Baarmand MM
- Babaev A
- Babounikau I
- Bacchetta N
- Bachiller I
- Bachtis M
- Backhaus M
- Baden A
- Baechler J
- Baginyan A
- Bagliesi G
- Bahinipati S
- Baillon P
- Bainbridge R
- Bakas G
- Bakhshiansohi H
- Bakirci MN
- Baldenegro Barrera C
- Ball AH
- Ban Y
- Band R
- Bandyopadhyay H
- Banerjee S
- Banerjee S
- Bansal S
- Barbagli G
- Barberis E
- Bargassa P
- Baringer P
- Barnes VE
- Barney D
- Baron O
- Barrio Luna M
- Bartek R
- Bartosik N
- BartĂłk M
- Bastos D
- Battilana C
- Baty A
- Bauer G
- Bauerdick LAT
- Baxter S
- Bayshev I
- Bean A
- Beauceron S
- Beaudette F
- Becerril Gonzalez H
- Bechtel J
- Bedoya CF
- Beghin D
- Behera PK
- Behera SC
- Behnke O
- Bein S
- Belchior Batista Das Chagas E
- Belforte S
- Bell KW
- Bellan R
- Belloni A
- Bellora A
- Belyaev A
- Belyaev A
- Benaglia A
- Benato L
- Bencze G
- Bendavid J
- Benecke A
- Benelli G
- Beni N
- Benitez JF
- Benussi L
- Berardi V
- Berenguer Antequera J
- Beretvas A
- Bergauer T
- Berger P
- Berger T
- Beri SB
- BermĂșdez MartĂnez A
- Bernardes CA
- Bernet C
- Berretti M
- Berry D
- Berryhill J
- Bertacchi V
- Besancon M
- Beschi A
- Bhal E
- Bhardwaj A
- Bharti M
- Bhat MA
- Bhat PC
- Bhatnagar V
- Bhattacharya R
- Bhattacharya S
- Bhattacharya S
- Bhattacharya S
- Bheesette S
- Bhowmik D
- Bhowmik S
- Bhyun JH
- Bi R
- Bialkowska H
- Bianchini L
- Bianco M
- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilin B
- Bin Anuar AA
- Bisello D
- Black K
- Blekman F
- Blinov V
- Bloch D
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Boccali T
- Bocci A
- Bodek A
- Boimska B
- Boletti A
- Bologna S
- Bols ES
- Bonacorsi D
- Bonanomi M
- Bonham B
- Bonomally S
- Boos E
- Boran F
- Borchsh V
- Borg J
- Borgonovi L
- Bornheim A
- Borras K
- Bortignon P
- Bose T
- Bossini E
- Botta C
- Botta V
- Bottigli U
- Boudoul G
- Bouhali O
- Bourgatte G
- Bourilkov D
- Bozzo M
- Bragagnolo A
- Braghieri A
- Braibant-Giacomelli S
- Brainerd C
- Brandao Malbouisson H
- Brandt S
- Branson JG
- Breedon R
- Breeze S
- Brew C
- Brigljevic V
- Brinkerhoff A
- Brivio F
- Brochero Cifuentes JA
- Brom J-M
- Brondolin E
- Brooke JJ
- Brown RM
- Brunner D
- Bruno G
- Brzhechko D
- BrĂŒcken E
- Bucci R
- Buccilli A
- Buchanan J
- Buchmuller O
- Buchot Perraguin A
- Bueghly J
- Bundock A
- Bunkowski K
- Buontempo S
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- Burkhardt H
- Burkle B
- Burt K
- Bury F
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- Butalla S
- Butler JN
- Butler PH
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- Bylinkin A
- Bylsma B
- Cabrera A
- Cabrillo IJ
- Cadamuro L
- Cafagna FS
- Caillol C
- Cakir A
- Calandri A
- Calderon De La Barca Sanchez M
- Calderon A
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- Calzaferri S
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- Caminada L
- Campagnari C
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- Camporesi T
- Candelise V
- Canelli MF
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- Cankocak K
- Capeans Garrido M
- Capiluppi P
- Cappati A
- Caputo C
- Caraway B
- Cardini A
- Cardwell B
- Carle A
- Carlin R
- Carrera Jarrin E
- Carrillo Montoya CA
- Carrillo Moreno S
- Cartiglia N
- Carvalho Antunes De Oliveira A
- Carvalho W
- Casarsa M
- Caspart R
- Cassese A
- Castaldi R
- Castaneda Hernandez A
- Castilla-Valdez H
- Castro A
- Catanesi MG
- Cavallari F
- Cavallo FR
- Cavallo N
- Cavanaugh R
- Ceard L
- Ceccarelli R
- Cepaitis V
- Cepeda M
- Cerati GB
- Cerci S
- Cerminara G
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- Cerri O
- Cetorelli F
- Chabert EC
- Chahal GS
- Chang P
- Chang P
- Chanon N
- Chao Y
- Chapon E
- Charaf O
- Charlot C
- Chatterjee RM
- Chatterjee S
- Chaudhary G
- Chauhan S
- Chauhan S
- Chawla R
- Chazin Quero B
- Checchia P
- Chekhovsky V
- Chen C
- Chen GM
- Chen HS
- Chen KF
- Chen M
- Chen PH
- Chen X
- Chen Y
- Chen Y
- Chen Z
- Chenarani S
- Cheng T
- Cheng Y
- Cherepanov V
- Chernyavskaya N
- Chertok M
- Cheung HWK
- Chhibra SS
- Chiarito B
- Chinellato J
- Chistov R
- Chlebana F
- Cho S
- Choi J
- Choi S
- Choi Y
- Chou JP
- Choudhary BC
- Choudhury S
- Chu J
- Chudasama R
- Chwalek T
- Ciangottini D
- Ciocca C
- Ciocci MA
- Cipriani M
- Ciriolo V
- Cirkovic P
- Citron M
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clement E
- Clerbaux B
- CMS Collaboration<sup>â </sup>
- Cockerill DJA
- Coelho E
- Colaleo A
- Cole JE
- Colino N
- Collard C
- Colling D
- Cometti S
- Connor P
- Consuegra RodrĂguez S
- Contardo D
- Conway J
- Conway R
- Cooper SI
- Cooperstein S
- Corcodilos L
- Cornelis T
- Cosby C
- Cossutti F
- Costa M
- Costa S
- Coubez X
- Couderc F
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- Cranshaw DJ
- Creanza D
- Cremonesi M
- Cristella L
- CsanĂĄd M
- CsörgĆ T
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cummings G
- Cussans D
- Cutts D
- Czellar S
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
- D'Hondt J
- Da Costa EM
- Da Rold A
- Da Silveira GG
- Dabrowski A
- Daci N
- Dalchenko M
- Dallavalle GM
- Damarseckin S
- Damgov J
- Danilov M
- Danilov V
- Daponte V
- Darwish MR
- Das P
- Das S
- Dasgupta A
- Dash D
- Daskalakis G
- Dasu S
- Datta A
- Dauncey P
- David A
- David P
- Davies G
- Davignon O
- De Barbaro P
- De Boer W
- De Bruyn I
- De Castro Manzano P
- De Clercq J
- De Cosa A
- De Filippis N
- De Guio F
- De Iorio A
- De Jesus Damiao D
- De La Cruz B
- De La Cruz-Burelo E
- De Lentdecker G
- De Leo K
- De Leonardis F
- De Palma M
- De Roeck A
- De TrocĂłniz JF
- De Wit A
- De Wolf EA
- Deelen N
- Defranchis MM
- Deile M
- Dejardin M
- Del Burgo R
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- Delannoy AG
- Delcourt M
- Delgado Peris A
- Delgado A
- Dell'Orso R
- Della Negra M
- Della Ricca G
- Demaria N
- Demina R
- Demiragli Z
- Demiroglu ZS
- Denegri D
- Depasse P
- Dermenev A
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- Dewanjee RK
- Dezoort G
- Dharmaratna WGD
- Dhingra N
- Di Croce D
- Di Domenico MR
- Di Florio A
- Di Marco E
- Di Maria R
- Di Mattia A
- Di Pilato A
- Diab B
- Diamantopoulou M
- Diaz D
- Didukh L
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- Dildick S
- Dilsiz K
- Dimitrov A
- Dimova T
- Dinardo ME
- Dini P
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- Dissertori G
- Dittmann J
- Dittmar M
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- Dobson M
- Dobur D
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- Dolek F
- Dolen J
- Dominguez A
- DomĂnguez Damiani D
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- Donertas IS
- Dordevic M
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- Dorney B
- Doroba K
- Dorsett A
- Doubek M
- Dozen C
- Dragicevic M
- Dremin I
- Dreyer T
- Droll A
- Druzhkin D
- Duarte Campderros J
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- Dubinin M
- Dudko L
- Dugad S
- Duh YT
- Dulemba JL
- Dumanoglu I
- Dupont N
- Durgut S
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- Dziwok C
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- Eckerlin G
- Ecklund KM
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- Eerola P
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- El Mamouni H
- El Morabit K
- Elgammal S
- Eliseev D
- Elkafrawy T
- Elliott-Peisert A
- Ellis KV
- Ellithi Kamel A
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- Ăsterberg K
- Ăzçelik Ă
- Ć irokĂœ 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 the inclusive and differential Higgs boson production cross sections in the decay mode to a pair of Ï Leptons in pp collisions at sqrt[s]=13ââTeV
- Author
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- Aarup Petersen H
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- Zorbilmez C
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- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Ălvarez FernĂĄndez A
- Ăzçelik Ă
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2022
- Field of study
Measurements of the inclusive and differential fiducial cross sections of the Higgs boson are presented, using the Ï lepton decay channel. The differential cross sections are measured as functions of the Higgs boson transverse momentum, jet multiplicity, and transverse momentum of the leading jet in the event, if any. The analysis is performed using proton-proton collision data collected with the CMS detector at the LHC at a center-of-mass energy of 13ââTeV and corresponding to an integrated luminosity of 138ââfb^{-1}. These are the first differential measurements of the Higgs boson cross section in the final state of two Ï leptons. In final states with a large jet multiplicity or with a Lorentz-boosted Higgs boson, these measurements constitute a significant improvement over measurements performed in other final states
Evidence for Top Quark Production in Nucleus-Nucleus Collisions
- Author
- Aarrestad TK
- Aarup Petersen H
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Consuegra RodrĂguez S
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- Cooperstein S
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- Ălvarez FernĂĄndez A
- Ăzçelik Ă
- 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
- Abercrombie D
- Acharya H
- Acosta D
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- Ăzçelik Ă
- 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
Observation of the B-s(0) -> X(3872)phi Decay
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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
Observation of a New Excited Beauty Strange Baryon Decaying to Îb- Ï+Ï-
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- Ăzçelik Ă
- Publication venue
- American Physical Society
- Publication date
- 01/01/2021
- Field of study
The Îb-Ï+Ï- 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 Îb- is reconstructed via its decays to J/ÏÎ- and J/ÏÎK-. A narrow resonance, labeled Îb(6100)-, is observed at a Îb-Ï+Ï- invariant mass of 6100.3±0.2(stat)±0.1(syst)±0.6(Îb-) MeV, where the last uncertainty reflects the precision of the Îb- baryon mass. The upper limit on the Îb(6100)- natural width is determined to be 1.9 MeV at 95% confidence level. The low Îb(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 Îc baryon states, the new Îb(6100)- resonance and its decay sequence are consistent with the orbitally excited Îb- baryon, with spin and parity quantum numbers JP=3/2-
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