81 research outputs found
On-surface synthesis of graphene nanoribbons with zigzag edge topology
- Author
- A Marini
- Bo Yang
- C Bronner
- C Tao
- CA Rozzi
- Carlo A. Pignedoli
- Carlos Sánchez-Sánchez
- Daniele Passerone
- DV Kosynkin
- FJ Giessibl
- GZ Magda
- H Zhang
- J Cai
- J Cai
- J Repp
- J van der Lit
- J VandeVondele
- Jia Liu
- JP Perdew
- K Nakada
- K Wakabayashi
- KA Ritter
- Klaus Müllen
- L Bartels
- L Gross
- L Ma
- L Yang
- L Yang
- Leopold Talirz
- M Topsakal
- M Wimmer
- MY Han
- OV Yazyev
- P Giannozzi
- Pascal Ruffieux
- Prashant Shinde
- R Saito
- Roman Fasel
- RW Godby
- S Dutta
- S Goedecker
- Shiyong Wang
- Thomas Dienel
- Tim Dumslaff
- W Han
- X Li
- X Wang
- Xinliang Feng
- Y Li
- Y Li
- Y-C Chen
- Y-C Chen
- Y-W Son
- YY Li
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 16/11/2015
- Field of study
Graphene-based nanostructures exhibit a vast range of exciting electronic
properties that are absent in extended graphene. For example, quantum
confinement in carbon nanotubes and armchair graphene nanoribbons (AGNRs) leads
to the opening of substantial electronic band gaps that are directly linked to
their structural boundary conditions. Even more intriguing are nanostructures
with zigzag edges, which are expected to host spin-polarized electronic edge
states and can thus serve as key elements for graphene-based spintronics. The
most prominent example is zigzag graphene nanoribbons (ZGNRs) for which the
edge states are predicted to couple ferromagnetically along the edge and
antiferromagnetically between them. So far, a direct observation of the
spin-polarized edge states for specifically designed and controlled zigzag edge
topologies has not been achieved. This is mainly due to the limited precision
of current top-down approaches, which results in poorly defined edge
structures. Bottom-up fabrication approaches, on the other hand, were so far
only successfully applied to the growth of AGNRs and related structures. Here,
we describe the successful bottom-up synthesis of ZGNRs, which are fabricated
by the surface-assisted colligation and cyclodehydrogenation of specifically
designed precursor monomers including carbon groups that yield atomically
precise zigzag edges. Using scanning tunnelling spectroscopy we prove the
existence of edge-localized states with large energy splittings. We expect that
the availability of ZGNRs will finally allow the characterization of their
predicted spin-related properties such as spin confinement and filtering, and
ultimately add the spin degree of freedom to graphene-based circuitry.Comment: 15 pages, 4 figure
The <i>Pratylenchus penetrans</i> transcriptome as a source for the development of alternative control strategies:mining for putative genes involved in parasitism and evaluation of <i>in planta</i> RNAi
- Author
- A Bairoch
- A Garofalo
- A Goverse
- A Haegeman
- A Haegeman
- A Haegeman
- A Haegeman
- A Prior
- AG Whitehead
- B Elsworth
- B Li
- BH Park
- C Ferrandiz
- C Furlanetto
- C Klotz
- CG Duan
- CH Opperman
- D Rotenberg
- DA Benson
- DV Jayatilake
- E Ghedin
- EGJ Danchin
- EM Schwarz
- EM Schwarz
- G Dubreuil
- GZ Huang
- H Kagawa
- H-J Cho
- HMM Ibrahim
- I Esteves
- I Iberkleid
- J Fosu-Nyarko
- J Jacob
- J Sampedro
- J-A CH Tan
- JA Cotton
- JJ Dalzell
- JL Lozano-Torres
- JM Kramer
- John Jones
- Jonathan D. Eisenback
- JP Hewitson
- JP McCarter
- JS Chen
- JT Jones
- JT Jones
- K Peymen
- K Rybarczyk-Mydlowska
- Kathryn Kamo
- KC Fairfax
- L Bauters
- L Robertson
- M Burke
- M Espada
- M Mitreva
- MG Grabherr
- MGK Jones
- MS Pearson
- N Patel
- ND Rawlings
- O Hobert
- P Abad
- P Abad
- P Castillo
- P Nicol
- P Vieira
- Paulo Vieira
- QB Nguyen
- Ruchi Verma
- S Consortium
- S Eves-van den Akker
- S Götz
- S Jaubert
- S Jaubert
- S Joseph
- S Leroy
- S Sharma
- Sarah Wantoch
- SD Armstrong
- Sebastian Eves-van den Akker
- T Kikuchi
- T Kyndt
- T Tygat
- TC Vrain
- TK Dutta
- TN Petersen
- W Li
- XJ Min
- Y Mei
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 14/12/2015
- Field of study
The root lesion nematode Pratylenchus penetrans is considered one of the most economically important species within the genus. Host range studies have shown that nearly 400 plant species can be parasitized by this species. To obtain insight into the transcriptome of this migratory plant-parasitic nematode, we used Illumina mRNA sequencing analysis of a mixed population, as well as nematode reads detected in infected soybean roots 3 and 7 days after nematode infection. Over 140 million paired end reads were obtained for this species, and de novo assembly resulted in a total of 23,715 transcripts. Homology searches showed significant hit matches to 58% of the total number of transcripts using different protein and EST databases. In general, the transcriptome of P. penetrans follows common features reported for other root lesion nematode species. We also explored the efficacy of RNAi, delivered from the host, as a strategy to control P. penetrans, by targeted knock-down of selected nematode genes. Different comparisons were performed to identify putative nematode genes with a role in parasitism, resulting in the identification of transcripts with similarities to other nematode parasitism genes. Focusing on the predicted nematode secreted proteins found in this transcriptome, we observed specific members to be up-regulated at the early time points of infection. In the present study, we observed an enrichment of predicted secreted proteins along the early time points of parasitism by this species, with a significant number being pioneer candidate genes. A representative set of genes examined using RT-PCR confirms their expression during the host infection. The expression patterns of the different candidate genes raise the possibility that they might be involved in critical steps of P. penetrans parasitism. This analysis sheds light on the transcriptional changes that accompany plant infection by P. penetrans, and will aid in identifying potential gene targets for selection and use to design effective control strategies against root lesion nematodes
Trapping in irradiated p-on-n silicon sensors at fluences anticipated at the HL-LHC outer tracker
- Author
- A De Canio
- A Della Porta
- A Androsov
- A Autermann
- A Barria
- A Bellan
- A Benelli
- A Biskop
- A Boccali
- A Calligaris
- A Ceard
- A Ciocci
- A Detraz
- A Eber
- A Evdokimov
- A Fangmeier
- A Galloni
- A Geisler
- A Grippo
- A Hansen
- A Hauk
- A Heintz
- A Hollar
- A Iashvili
- A Joshi
- A Kaplon
- A Kleinwort
- A Kottelat
- A Krohn
- A Kumar
- A Kumar
- A Kumar
- A Lapsien
- A Lenzi
- A Maerschalk
- A Makouski
- A Maksimovic
- A Mallows
- A Marconi
- A Moon
- A Nayak
- A Ntomari
- A Pakulski
- A Park
- A Pernie
- A Pernot
- A Pierschel
- A Poehlsen
- A Potenza
- A Printz
- A Python
- A Ranjan
- A Rappoccio
- A Reis
- A Rivera
- A Rizzi
- A Salvati
- A Serban
- A Servoli
- A Sola
- A Solano
- A Solestizi
- A Spiegel
- A Takahashi
- A Tonelli
- A Trapani
- A Tuve
- A Ulmer
- A Vasey
- A Verdini
- A Viliani
- A Yagil
- Adam
- AG D'Angelo
- AL Abbaneo
- AM Pesaresi
- AR Erfle
- AT Spagnolo
- B De Lentdecker
- B Bolla
- B Covarelli
- B Delaere
- B Djambazov
- B Ecklund
- B Hartmann
- B Lange
- B Magalotti
- B Marionneau
- B Re
- B Rohe
- B Wlochal
- B Zwalinski
- BK O'Brien
- C Du Pree
- C Barbagli
- C Boegelspacher
- C Bosiger
- C Brom
- C Clerbaux
- C Contardo
- C Demaria
- C Edelhoff
- C Fluegge
- C Gallo
- C Gonzalez
- C Gross
- C Gruenendahl
- C Grundler
- C Hits
- C Hreus
- C Korol
- C Lander
- C Maier
- C Mussgiller
- C Nash
- C Perrini
- C Richer
- C Schleper
- C Spannagel
- C Suarez
- CE Hofman
- CM Lipton
- CS Morsani
- CV Vanlaer
- D Ahmed
- D Bloom
- D Bonnin
- D Bubna
- D Casal
- D Christiansen
- D Cooper
- D Cumalat
- D Dall'Osso
- D Dinardo
- D Donckt
- D Eichhorn
- D Faccio
- D Fano
- D Favart
- D Flacher
- D Frank
- D Gallbit
- D Gritsan
- D Halkiadakis
- D Harris
- D Horisberger
- D Langenegger
- D Menichelli
- D Moroni
- D Noonan
- D Nuttens
- D Placidi
- D Quertenmont
- D Ratti
- D Reid
- D Ricci-Tam
- D Robmann
- D Sanchez
- D Sanders
- D Schroeder
- D Watson-Daniels
- DA Basegmez
- De Palma M
- DH Shi
- DIS Trauger
- DJ Kapustka
- DM Uchida
- DR Dominguez
- DR Evdokimov
- E Lo Vetere
- E Auzinger
- E Casele
- E Charles
- E Ciangottini
- E Duggan
- E Eerola
- E Fontaine
- E Haller
- E Hammad
- E Lath
- E Lenzi
- E Meschini
- E Minuti
- E Monteil
- E Musich
- E Perrey
- E Skinnari
- E Tropiano
- E Tuovinen
- E Yin
- F Abu Zeid
- F De Boer
- F De Bruyn
- F Di Mattia
- F Becker
- F Castaldi
- F Chiochia
- F Dierlamm
- F Donato
- F Felici
- F Gaioni
- F Hauth
- F Lei
- F Ligabue
- F Monroy
- F Palla
- F Palmonari
- F Raffaelli
- F Robutti
- F Romero
- F Sala
- F Sammet
- F Savoy-Navarro
- F Squires
- F Vernieri
- F Vichoudis
- FJG Sanchez
- FJM Vila
- G Van Parijs
- G Albergo
- G Basti
- G Berruti
- G Bianchi
- G Blanchot
- G Boudoul
- G Breuker
- G Brianzi
- G Burkett
- G Calzolari
- G Castello
- G Chiorboli
- G Ciulli
- G Combaret
- G Comotti
- G Derylo
- G Dobur
- G Eckerlin
- G Eckstein
- G Eusebi
- G Fiore
- G Garcia
- G Giassi
- G Gingu
- G Gray
- G Kuensken
- G Lumb
- G Lustermann
- G Magnan
- G Malberti
- G Mazzoni
- G Mirman
- G Moya
- G Muhl
- G Passeri
- G Postema
- G Preuten
- G Sharma
- G Silvestris
- G Wellhausen
- G Wittmer
- GH Harkonen
- GM Bissi
- GZ Dutta
- H Adams
- H Behnamian
- H Blobel
- H Ceresa
- H Chramowicz
- H Feld
- H Goldstein
- H Khakzad
- H Mirabito
- H Mittag
- H Pitzl
- H Rose
- H Turner
- H Vargas
- HC Kotlinski
- HJ Steck
- I Albert
- I D'Hondt
- I Fehling
- I Kaisen
- I Lange
- I Perloff
- I Strom
- I Virto
- ID Teodorescu
- IR Garabedian
- J El Nasr-Storey
- J Barvich
- J Betchart
- J Bloch
- J Bortoletto
- J Burgmeier
- J Chaves
- J Chertok
- J Cheung
- J Christian
- J Chu
- J Cichy
- J Conway
- J D'Alfonso
- J Daci
- J Dittmer
- J Garutti
- J George
- J Godshalk
- J Grimes
- J Hahn
- J Hall
- J Hanson
- J Hobson
- J Hoffmann
- J Howell
- J Hrycyk
- J Jez
- J Kalogeropoulos
- J Kasieczka
- J Kharchilava
- J Kornmayer
- J Krammer
- J Kyre
- J Lampen
- J Lowette
- J Majumder
- J Mathieu
- J Pinna
- J Poehlsen
- J Sagir
- J Schael
- J Tersegno
- J Thompson
- J Tomalin
- J Tsirou
- J Tucker
- J Winstrom
- J Yohay
- J Zenoni
- JA Harder
- JC Andrea
- JER Alyari
- JF Petagna
- JG Cremaldi
- JG Gizhko
- JL Conte
- JM Chabert
- JP Ford
- K Azzurri
- K Bakhshiansohl
- K Bose
- K Butler
- K Caminada
- K Coughlan
- K Daguin
- K Ellison
- K Erdmann
- K Giordano
- K Harb
- K Heracleous
- K Ilic
- K Lipinski
- K Osherson
- K Pistone
- K Sevova
- K Trovato
- K Wagner
- KA Delannoy
- KH Husemann
- KM Nussbaum
- L Creanza D
- L De Callatay
- L di Calafiori
- L Akgun
- L Bachmair
- L Bainbridge
- L Biasini
- L Bilei
- L Canelli
- L Checcucci
- L Dolinska
- L Donega
- L Ferro
- L Franco
- L Giammanco
- L Goetzmann
- L Grebenyuk
- L Hosselet
- L Incandela
- L Karpinski
- L Kovacs
- L Lariccia
- L Manghisoni
- L Messineo
- L Olbrechts
- L Pagano
- L Pedrini
- L Perries
- L Randle-Conde
- L Ravera
- L Roeser
- L Selvaggi
- L Storchi
- L Summers
- L Thom
- L Tran
- L Velde
- L Voirin
- LA Spiezia
- LM Oliveros
- M del Arbol
- M Acosta
- M Bartz
- M Cariola
- M Cerati
- M Ciaranfi
- M Colombo
- M Conti
- M Conway
- M Costa
- M Covarelli
- M D'Auria
- M Dolen
- M Dorigo
- M Draeger
- M Dunser
- M Eller
- M Esser
- M Fiorendi
- M Friedl
- M Fruehwirth
- M Gennai
- M Gomez
- M Hinton
- M Hrubec
- M Jacob
- M Jindariani
- M Jung
- M Junkes
- M Loddo
- M Malik
- M Mannelli
- M Marchioro
- M Marono
- M Merkel
- M Miller
- M Moggi
- M Naseri
- M Nelson
- M Nodari
- M Olmedo
- M Onnela
- M Ostapchuk
- M Pacher
- M Paoletti
- M Perieanu
- M Perrozzi
- M Pooth
- M Raupach
- M Raymond
- M Saha
- M Santocchia
- M Schnetzer
- M Seitz
- M Simonis
- M Skhirtladze
- M Skovpen
- M Starodumov
- M Stenson
- M Stoye
- M Swartz
- M Thomson
- M Treberspurg
- M Tropea
- M Wallny
- M Weiler
- M Wilken
- M Xiao
- M Zhukov
- M Zucchetta
- MA Dell'Orso
- MA Tricomi
- Maggi G
- MR Berry
- MT Lomtadze
- MV Beliy
- MV Verdier
- My S
- N Van Spilbeeck
- N Behr
- N Bisello
- N Caebergs
- N Deroover
- N Gill
- N Jones
- N Keaveney
- N Mathez
- N Mullin
- N Rivetti
- N Ryd
- N Stupak
- N Taylor
- N Tosi
- N Uplegger
- O Gerber
- O Petrillo
- O Stahl
- P De Robertis
- P Van Onsem
- P Van Remortel
- P Arezzini
- P Bacchetta
- P Baringer
- P Bean
- P Caillol
- P Centis-Vignali
- P Echeverria
- P Fulcher
- P Grab
- P Honma
- P Johns
- P Leggat
- P Mantovani
- P Martin
- P Michotte
- P Nahn
- P Parashar
- P Petrucciani
- P Pozzobon
- P Rzonca
- P Salvatore
- P Scarlini
- P Schmidt
- P Taroni
- P Tenchini
- P Troska
- P Tuuva
- P Verlaat
- P Viret
- P Wang
- P Weber
- PG Martini
- PH Dietz
- PMR Masciovecchio
- PR Maenpaa
- Q Tavernier
- R Amsler
- R Anderson
- R Bani
- R Burt
- R Casasso
- R Caudron
- R Ciampa
- R Civinini
- R Cussans
- R Dauncey
- R Demina
- R Fedi
- R Flores
- R Freund
- R Gonzi
- R Hindrichs
- R Hoch
- R Ivanov
- R Kaestli
- R Liu
- R Maser
- R Migliore
- R Ngadiuba
- R Osipenkov
- R Pellett
- R Saizu
- R Shenai
- R Venturi
- R Walker
- RA Azzi
- RG Meier
- RJ Fernandez
- RS Moya
- S De Visscher
- S Van Mechelen
- S Van Mulders
- S Alexander
- S Bagliesi
- S Beaumont
- S Blekman
- S Bruno
- S Cappello
- S Chen
- S Claes
- S Costa
- S Deyrail
- S Fiori
- S Giordano
- S Gori
- S Hasegawa
- S Hoff
- S Hoffmann
- S Johnson
- S Kaufman
- S Malvezzi
- S Manzoni
- S Martina
- S Matulik
- S Matysek
- S McColl
- S Menasce
- S Mendez
- S Mersi
- S Michelis
- S Moll
- S Moreels
- S Muller
- S Peisert
- S Perera
- S Prosser
- S Sabes
- S Schwering
- S Sguazzoni
- S Speer
- S Stone
- S Stringer
- S Sung
- S White
- S Yang
- S Zoccarato
- S Zuber
- Selvaggi
- SR Baldin
- SS Cole
- T Barth
- T Beaulieu
- T Bhardwaj
- T Bosi
- T Daubie
- T Dragicevic
- T Fluke
- T Forthomme
- T Giubilato
- T Heindl
- T Kilminster
- T Leonard
- T Los
- T Luukka
- T Magazzu
- T Mattig
- T Mohammadi
- T Nuernberg
- T Pavis
- T Peltola
- T Scharf
- T Seva
- T Streuli
- T Swanson
- T Thomas
- T Tuominen
- T Zabel
- U Hoss
- U Hou
- U Kahlid
- U Kornmeyer
- U Meier
- U Narain
- U Rossini
- V de Cosa
- V Bartosik
- V Buhmann
- V D'Alessandro
- V Focardi
- V Gouskos
- V Steinbruck
- V Traversi
- V Vartak
- W
- W Alderweireldt
- W Bergauer
- W Butz
- W Deiters
- W Horisberger
- W Janssen
- W Klein
- W Lohmann
- W Mangano
- W Mankel
- W Waltenberger
- WE Deptuch
- WS Lu
- WT Gaz
- X Luyckx
- X Tan
- Y Agram
- Y Bertl
- Publication venue
- 'IOP Publishing'
- Publication date
- 07/05/2015
- Field of study
The degradation of signal in silicon sensors is studied under conditions expected at the CERN High-Luminosity LHC. 200 μm thick n-type silicon sensors are irradiated with protons of different energies to fluences of up to 3⋅1015 neq/cm2. Pulsed red laser light with a wavelength of 672 nm is used to generate electron-hole pairs in the sensors. The induced signals are used to determine the charge collection efficiencies separately for electrons and holes drifting through the sensor. The effective trapping rates are extracted by comparing the results to simulation. The electric field is simulated using Synopsys device simulation assuming two effective defects. The generation and drift of charge carriers are simulated in an independent simulation based on PixelAV. The effective trapping rates are determined from the measured charge collection efficiencies and the simulated and measured time-resolved current pulses are compared. The effective trapping rates determined for both electrons and holes are about 50% smaller than those obtained using standard extrapolations of studies at low fluences and suggests an improved tracker performance over initial expectations
Search for the production of W^{\pm} W^{\pm} W^{\mp} events at \sqrt{s} = 13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams MR
- Adams T
- Adan DP
- Adzic P
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmad M
- Ahmad WH
- Ahuja S
- Akbiyik M
- Akchurin N
- Akgun B
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Allen B
- Almond J
- Alvarez Fernandez A
- Alvarez Gonzalez B
- 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 LP
- Antchev G
- Antunovic Z
- Apanasevich L
- Apollinari G
- Apresyan A
- Apyan A
- Araujo M
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arneodo M
- Asavapibhop B
- Asawatangtrakuldee C
- Asenov P
- Askew A
- Asmuss P
- Assran Y
- Atakisi IO
- Ather MW
- Attikis A
- Auffray E
- Aushev T
- Autermann C
- Auzinger G
- Avati V
- Avery P
- Avila C
- Ayala E
- 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
- Bagliesi G
- Bahinipati S
- Baillon P
- Bainbridge R
- Bakas G
- Bakhshiansohi H
- Ball AH
- Ball F
- Ban Y
- Band R
- Banerjee S
- Banerjee S
- Bansal S
- Barbagli G
- Barberis E
- Bargassa P
- Baringer P
- Barker A
- Barnes VE
- Barney D
- Barnyakov A
- Baron O
- Barrera CB
- Barria P
- Barrio Luna M
- Bartek R
- Barth C
- Bartok M
- Bartosik N
- Baselga M
- Bastos D
- Bat A
- Battilana C
- Baty A
- Bauerdick LAT
- Baur S
- Bayshev I
- Bean A
- Beauceron S
- Beaudette F
- Becerra DAS
- Beernaert K
- Beghin D
- Behera PK
- Behnke O
- Behrens U
- Bein S
- Belchior Batista Das Chagas E
- Belforte S
- Bell KW
- Bellan R
- Belloni A
- Belyaev A
- Belyaev A
- Benaglia A
- Benato L
- Bencze G
- Bendavid J
- Benecke A
- Benelli G
- Beni N
- Benitez JF
- Benussi L
- Benvenuti AC
- Beretvas A
- Bergauer T
- Berger P
- Beri SB
- Bernardes CA
- Bernet C
- Berry D
- Berryhill J
- Bertacchi V
- Bertsche D
- Besancon M
- Beschi A
- Betts RR
- Bhal E
- Bhandari R
- Bhardwaj A
- Bhardwaj R
- Bharti M
- Bhat MA
- Bhat PC
- Bhatnagar V
- Bhattacharya R
- Bhattacharya S
- Bhattacharya S
- Bhattacharya S
- Bhawandeep U
- Bheesette S
- Bhopatkar V
- Bhowmik D
- Bhowmik S
- Bhyun JH
- Bi R
- Bialkowska H
- Bianchini L
- Bianco M
- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilin B
- Bilki B
- Bin Anuar AA
- Bindhu VKMN
- Bitioukov S
- Blekman F
- Blinov V
- Blobel V
- Bloch D
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- Zuolo D
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/07/2019
- Field of study
A search for the production of events containing three W bosons predicted by the standard model is reported. The search is based on a data sample of proton-proton collisions at a center-of-mass energy of 13 TeV recorded by the CMS experiment at the CERN LHC and corresponding to a total integrated luminosity of 35.9 fb^{-1}. The search is performed in final states with three leptons (electrons or muons), or with two same-charge leptons plus two jets. The observed (expected) significance of the signal for W^{\pm} W^{\pm} W^{\mp} production is 0.60 (1.78) standard deviations, and the ratio of the measured signal yield to that expected from the standard model is 0.34_{-0.34}^{+0.62}. Limits are placed on three anomalous quartic gauge couplings and on the production of massive axionlike particles
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
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- Wulz C-E
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- Xiao R
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- Xu Q
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- Yang UK
- Yang YC
- Yates BR
- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
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- Yu D
- Yu GB
- Yu I
- Yu SS
- Yuan L
- Yumiceva F
- Yusli MN
- Zabi A
- Zaganidis N
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zghiche A
- Zhang A
- Zhang F
- Zhang H
- Zhang J
- Zhang S
- Zhang Z
- Zhao J
- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zito G
- Zobec J
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Publication venue
- 'Elsevier BV'
- Publication date
- 10/09/2019
- Field of study
The production cross sections of B_{s}^{0} mesons and charge conjugates are measured in proton-proton (pp) and PbPb collisions via the exclusive decay channel B_{s}^{0}→J/ψϕ→μ^{+}μ^{−}K^{+}K^{−} at a center-of-mass energy of 5.02 TeV per nucleon pair and within the rapidity range |y|<2.4 using the CMS detector at the LHC. The pp measurement is performed as a function of transverse momentum (p_{T}) of the B_{s}^{0} mesons in the range of 7 to 50 GeV/c and is compared to the predictions of perturbative QCD calculations. The B_{s}^{0} production yield in PbPb collisions is measured in two p_{T} intervals, 7 to 15 and 15 to 50 GeV/c, and compared to the yield in pp collisions in the same kinematic region. The nuclear modification factor (R_{AA}) is found to be 1.5±0.6(stat)±0.5(syst) for 7–15 GeV/c, and 0.87±0.30(stat)±0.17(syst) for 15–50 GeV/c, respectively. Within current uncertainties, the B_{s}^{0} results are consistent with models of strangeness enhancement, and suppression by parton energy loss, as observed for the B+ mesons
Measurement of the tt¯ production cross section, the top quark mass, and the strong coupling constant using dilepton events in pp collisions at √s = 13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdalla H
- Abdullah WATW
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Acharya H
- Ackert A
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- Chen G
- Chen GM
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- Chenarani S
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- Chernyavskaya N
- Chertok M
- Cheung HWK
- Chhibra SS
- Chiarito B
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- Chinellato J
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- Chou JP
- Choudhary BC
- Choudhury S
- Chowdhury SR
- Chu J
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- Chwalek T
- Ciangottini D
- Cieri D
- Ciocci MA
- Cipriani M
- Ciriolo V
- Cirkovic P
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- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clarida W
- Clement E
- Clerbaux B
- Cockerill DJA
- Cocoros A
- Codispoti G
- Coelho E
- Colafranceschi S
- Colaleo A
- Cole JE
- Colino N
- Collard C
- Colling D
- Colombo F
- Cometti S
- Connor P
- Contardo D
- Conte E
- Contreras-Campana C
- Conway J
- Conway R
- Cooper SI
- Cooperstein S
- Cornelis T
- Correia Silva G
- Cossutti F
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- Coubez X
- Couderc F
- Coughlan JA
- Courbon B
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- Cox PT
- Creanza D
- Cremonesi M
- Cristella L
- Csanad M
- Cucciati G
- Cuevas J
- Cuffiani M
- Cumalat JP
- Curry D
- Cussans D
- Cutts D
- Czellar S
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- D'Alfonso M
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- Yusli MN
- Zabi A
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- Zalewski P
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- Zeuner WD
- Zeyrek M
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- Zientek M
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- Zoi I
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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
Measurement of the WZ production cross section in pp collisions at root s=13 Tev
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- Aarrestad TK
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- Publication venue
- Publication date
- 01/01/2015
- Field of study
Peer reviewe
Relative Modification of Prompt psi(2S) and J/psi Yields from pp to PbPb Collisions at root(S)(NN)=5.02 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam W
- Adams JR
- Adams MR
- Adams T
- Adiguzel A
- Adzic P
- Afanasiev S
- Agapitos A
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- Ahmad M
- Ahmad M
- Ahmed I
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- Publication venue
- Publication date
- 04/11/2016
- Field of study
Peer reviewe
Search for contact interactions and large extra dimensions in the dilepton mass spectra from proton-proton collisions at \sqrt{s} = 13 TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
- Abdulsalam A
- Abercrombie D
- Abu Zeid S
- Ackert A
- Acosta D
- Acosta JG
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- Adams MR
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- Wertz S
- West C
- Wetzel J
- Whitbeck A
- Wichmann K
- Wickramage N
- Wiederkehr SA
- Wightman A
- Wilkinson R
- Williams T
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- Wissing C
- Wittich P
- Wittmann J
- Wittmer B
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- Wolf M
- Wolf R
- Wolfe E
- Womersley WJ
- Wong K
- Wood D
- Wood J
- Woodard A
- Woods N
- Wright D
- Wright J
- Wu Z
- Wulsin HW
- Wulz C-E
- Wurthwein F
- Wyslouch B
- Xia F
- Xiao M
- Xiao R
- Xie S
- Xie W
- Xu Q
- Yagil A
- Yalvac M
- Yang UK
- Yang YC
- Yates BR
- Yazgan E
- Yetkin EA
- Yohay R
- Yoo HD
- Yoo J
- You C
- Yu D
- Yu GB
- Yu I
- Yu SS
- Yuan L
- Yumiceva F
- Yusli MN
- Zabi A
- Zaganidis N
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti A
- Zanetti M
- Zarubin A
- Zarucki M
- Zeinali M
- Zenaiev O
- Zenz SC
- Zeuner WD
- Zeyrek M
- Zghiche A
- Zhang A
- Zhang F
- Zhang H
- Zhang J
- Zhang Z
- Zhao J
- Zhokin A
- Zhu DH
- Zhu RY
- Zientek M
- Zito G
- Zobec J
- Zoi I
- Zolkapli Z
- Zorbakir IS
- Zorbilmez C
- Zotto P
- Zou D
- Zucchetta A
- Zumerle G
- Zuolo D
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2019
- Field of study
A search for nonresonant excesses in the invariant mass spectra of electron and muon pairs is presented. The analysis is based on data from proton-proton collisions at a center-of-mass energy of 13 TeV recorded by the CMS experiment in 2016, corresponding to a total integrated luminosity of 36 fb^{-1}. No significant deviation from the standard model is observed. Limits are set at 95% confidence level on energy scales for two general classes of nonresonant models. For a class of fermion contact interaction models, lower limits ranging from 20 to 32 TeV are set on the characteristic compositeness scale Λ. For the Arkani-Hamed, Dimopoulos, and Dvali model of large extra dimensions, the first results in the dilepton final state at 13 TeV are reported, and values of the ultraviolet cutoff parameter Λ_{T} below 6.9 TeV are excluded. A combination with recent CMS diphoton results improves this exclusion to Λ_{T} below 7.7 TeV, providing the most sensitive limits to date in nonhadronic final states
FCC-ee: The Lepton Collider: Future Circular Collider Conceptual Design Report Volume 2
- Author
- Abada A
- Abbrescia M
- AbdusSalam SS
- Abdyukhanov I
- Abramov A
- Aburaia M
- Acar AO
- Adzic PR
- Agaliotis EL
- Agrawal P
- Aguilar-Saavedra JA
- Aguilera-Verdugo JJ
- Aiba M
- Aichinger I
- Aielli G
- Akay A
- Akhundov A
- Aksakal H
- Alaniz EC
- Albacete JL
- Albergo S
- Alekou A
- Aleksa M
- Aleksan R
- Alexahin Y
- Alia RG
- Alioli S
- Allanach BC
- Allport PP
- Altinli M
- Altmannshofer W
- Ambrosio G
- Amorim D
- Amstutz O
- Anderlini L
- Andreazza A
- Andreini M
- Andriatis A
- Andris C
- Andronic A
- Angelucci M
- Antinori F
- Antipov SA
- Antonelli M
- Antonello M
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- Antusch S
- Anulli F
- Apolinario L
- Apollinari G
- Apollonio A
- Appelo D
- Appleby RB
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- Arduini G
- Ari V
- Arias S
- Armesto N
- Arnaldi R
- Arsenyev SA
- Arzeo M
- Asai S
- Aslanides E
- Assmann RW
- Astapovych D
- Atanasov M
- Atieh S
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- Auchmann B
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- Avino F
- Avrillaud G
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- Azatov A
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- Azzi P
- Azzolini O
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- Bacchiocchi E
- Bachacou H
- Baek YW
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- Ball AH
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- Barber DP
- Barducci D
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- Barna D
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- Barzi E
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- Boscherini D
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- Cervantes J
- Chaikovska I
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- Cibinetto G
- Ciftci AK
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- Cooley L
- Corcella G
- Cornell AS
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- Dam M
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- De Roeck A
- Deandrea A
- Debono CJ
- Deghaye S
- Del Bo C
- Del Duca V
- Delikaris D
- Deliot F
- Dell Porta GZ
- Dell'Acqua A
- Delle Rose L
- Delmastro M
- Delsolaro WV
- Demarteau M
- Denegri D
- Deniau L
- Denisov D
- Denizli H
- Denner A
- Derue F
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- Dev PSB
- Dewanjee RK
- Di Ciaccio A
- Di Cicco A
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- Di Nezza P
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- Diaz VG
- Dillon BM
- Doblhammer A
- Dominjon A
- Dordei F
- Drago A
- Draper P
- Drasal Z
- Drewes M
- du Pree T
- Duarte L
- Dubovyk I
- Duda P
- Dudarev A
- Dudko L
- Duellmann D
- Duenser M
- Durante M
- Dutta S
- Duval F
- Duval JM
- Dydyshka Y
- Dziewit B
- Eisenhardt S
- Eisterer M
- Ekelof T
- El Khechen D
- Ellis J
- Ellis SA
- Ellison JA
- Elsener K
- Elsing M
- Enari Y
- Englert C
- Eriksson H
- Eskola KJ
- Esposito LS
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- Faus-Golfe A
- Fawcett WJ
- Felici G
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- Ferdeghini C
- Fernandez Navarro AM
- Fernandez JA
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- Ferrara G
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- Ferreira L
- Ferrera G
- Ferro F
- Fiascaris M
- Fiorendi S
- Fiorio C
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- Fouaidy M
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- Furuseth SV
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- Gascon-Shotkin SM
- Gaudio G
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- Savelyeva S
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- Schaffer A
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- Scheuerlein C
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- Spannowsky M
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- Spiesberger H
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- Stachel J
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- Stanyard JL
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- Starikov AY
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- Publication venue
- SPRINGER HEIDELBERG
- Publication date
- 01/06/2019
- Field of study
In response to the 2013 Update of the European Strategy for Particle Physics, the Future Circular Collider (FCC) study was launched, as an international collaboration hosted by CERN. This study covers a highest-luminosity high-energy lepton collider (FCC-ee) and an energy-frontier hadron collider (FCC-hh), which could, successively, be installed in the same 100 km tunnel. The scientific capabilities of the integrated FCC programme would serve the worldwide community throughout the 21st century. The FCC study also investigates an LHC energy upgrade, using FCC-hh technology. This document constitutes the second volume of the FCC Conceptual Design Report, devoted to the electron-positron collider FCC-ee. After summarizing the physics discovery opportunities, it presents the accelerator design, performance reach, a staged operation scenario, the underlying technologies, civil engineering, technical infrastructure, and an implementation plan. FCC-ee can be built with today’s technology. Most of the FCC-ee infrastructure could be reused for FCC-hh. Combining concepts from past and present lepton colliders and adding a few novel elements, the FCC-ee design promises outstandingly high luminosity. This will make the FCC-ee a unique precision instrument to study the heaviest known particles (Z, W and H bosons and the top quark), offering great direct and indirect sensitivity to new physics
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