1,585 research outputs found
Rare Z-decay into light CP-odd Higgs bosons: a comparative study in different new physics models
- Author
- A Arhrib
- A Arhrib
- A Belyaev
- A Dedes
- A Djouadi
- A Djouadi
- A Djouadi
- A Djouadi
- A Menon
- AG Akeroyd
- AG Akeroyd
- AG Akeroyd
- ALEPH collaboration
- BA Dobrescu
- C Amsler
- C BalĂĄzs
- C Panagiotakopoulos
- C Panagiotakopoulos
- C Panagiotakopoulos
- D Atwood
- D Buskulic
- D Chang
- D Das
- DJ Miller
- E Keith
- F Borzumati
- F Domingo
- F Franke
- F Larios
- F Larios
- G Abbiendi
- G Abbiendi
- G Abbiendi
- G Abbiendi
- G Altarelli
- G BĂŠlanger
- G BĂŠlanger
- G BĂŠlanger
- G Hiller
- H-S Goh
- HE Logan
- J Abdallah
- J Abdallah
- J Cao
- J Cao
- J Cao
- J Cao
- J Cao
- J Dunkley
- J Kalinowski
- J Kurowska
- JF Gunion
- JF Gunion
- JF Gunion
- JF Gunion
- JI Illana
- Jin Min Yang
- JM Yang
- JR Ellis
- Junjie Cao
- K Cheung
- K MĂśnig
- K-m Cheung
- M Aoki
- M Davier
- M Drees
- M Krawczyk
- M Krawczyk
- M Krawczyk
- MA Perez
- MA Perez
- ME Peskin
- O Deschamps
- R Barate
- R Dermisek
- R Dermisek
- R Dermisek
- R Dermisek
- R Dermisek
- R Dermisek
- R Dermisek
- RM Barnett
- RM Barnett
- S Andreas
- S Schael
- S Su
- SP Martin
- T Besmer
- TJ Weiler
- U Ellwanger
- U Ellwanger
- U Ellwanger
- U Ellwanger
- V Barger
- V Barger
- X-G He
- X-G He
- Y Grossman
- Z Heng
- Zhaoxia Heng
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 07/11/2010
- Field of study
Various new physics models predict a light CP-odd Higgs boson (labeled as
a) and open up new decay modes for Z-boson, such as ZâfËâfa,
ZâaÎł and Zâaaa, which could be explored at the GigaZ option of
the ILC. In this work we investigate these rare decays in several new physics
models, namely the type-II two Higgs doublet model (type-II 2HDM), the
lepton-specific two Higgs doublet model (L2HDM), the nearly minimal
supersymetric standard model (nMSSM) and the next-to-minimal supersymmetric
standard model (NMSSM). We find that in the parameter space allowed by current
experiments, the branching ratios can reach 10â4 for ZâfËâfa
(f=b,Ď), 10â9 for ZâaÎł and 10â3 for Zâaaa, which
implies that the decays ZâfËâfa and Zâaaa may be accessible
at the GigaZ option. Moreover, since different models predict different
patterns of the branching ratios, the measurement of these rare decays at the
GigaZ may be utilized to distinguish the models.Comment: Version in JHEP (discussions added, errors corrected
Higgs boson production in photon-photon collision at ILC: a comparative study in different little Higgs models
- Author
- A Belyaev
- A Djouadi
- A Freitas
- AG Dias
- C Amsler
- C CsĂĄki
- C CsĂĄki
- C-R Chen
- CO Dib
- CX Yue
- D Zeppenfeld
- DE Kaplan
- Fuqiang Xu
- G Cacciapaglia
- G Jikia
- G Marandella
- GA Gonzalez-Sprinberg
- H Cai
- H-C Cheng
- H-C Cheng
- H-C Cheng
- HE Logan
- I Low
- I Low
- J Hubisz
- J Hubisz
- J-j Cao
- J-j Cao
- J-J Cao
- J-J Liu
- JF Gunion
- Jin Min Yang
- JL Hewett
- K Cheung
- K Cheung
- K Cheung
- K Hsieh
- K-m Cheung
- L Wang
- L Wang
- L Wang
- L Wang
- Lei Wang
- M Asano
- M DĂźhrssen
- M Schmaltz
- M-C Chen
- M-C Chen
- N Arkani-Hamed
- N Arkani-Hamed
- N Arkani-Hamed
- OJP Eboli
- P Niezurawski
- RS Hundi
- S Chang
- S Chang
- S Soldner-Rembold
- T Gregoire
- T Han
- T Han
- T Han
- W Kilian
- W Skiba
- X-F Han
- X-F Han
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 07/01/2010
- Field of study
We study the process \gamma\gamma->h->bb_bar at ILC as a probe of different
little Higgs models, including the simplest little Higgs model (SLH), the
littlest Higgs model (LH), and two types of littlest Higgs models with T-parity
(LHT-I, LHT-II). Compared with the Standard Model (SM) prediction, the
production rate is found to be sizably altered in these little Higgs models
and, more interestingly, different models give different predictions. We find
that the production rate can be possibly enhanced only in the LHT-II for some
part of the parameter space, while in all other cases the rate is suppressed.
The suppression can be 10% in the LH and as much as 60% in both the SLH and the
LHT-I/LHT-II. The severe suppression in the SLH happens for a large \tan\beta
and a small m_h, in which the new decay mode h->\eta\eta (\eta is a light
pseudo-scalar) is dominant; while for the LHT-I/LHT-II the large suppression
occurs when f and m_h are both small so that the new decay mode h->A_H A_H is
dominant. Therefore, the precision measurement of such a production process at
the ILC will allow for a test of these models and even distinguish between
different scenarios.Comment: Version in JHEP (h-g-g & h-gamma-gamma expressions added
Multiscale modelling and analysis of signalling processes in tissues with non-periodic distribution of cells
- Author
- A Abdulle
- A Abdulle
- A ChavarrĂa-Krauser
- A Marciniak-Czochra
- A-M Matache
- AG Belyaev
- CPD Wheeler-Jones
- CS Peskin
- D Chenais
- D Cioranescu
- D Cioranescu
- D Cioranescu
- D Cioranescu
- G Nguetseng
- GA Chechkin
- J Dixmier
- J Hornung
- M Briane
- M Briane
- M Ptashnyk
- M Ptashnyk
- ML Mascarenhas
- OA LadyĹženskaja
- R Alexandre
- RE Showalter
- S Shkoller
- SA Meier
- TL van Noorden
- W E
- Y Efendiev
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Physics of Neutron Star Crusts
- Author
- A Bohr
- A Bulgac
- A Burrows
- A Cumming
- A Gelfert
- A Melatos
- A Schwenk
- A Sedrakian
- A Sedrakian
- A Spitkovsky
- A Zeilinger
- AA Abrikosov
- AB Migdal
- AD Kaminker
- AD Kaminker
- AD Kaminker
- AD Kaminker
- AD Sedrakian
- AD Sedrakian
- AF Andreev
- AG Lyne
- AG Lyne
- AI Chugunov
- AI Chugunov
- AK Dutta
- AL Fetter
- AL Piro
- AL Piro
- AL Piro
- AL Piro
- AL Watts
- AS Botvina
- AY Potekhin
- AY Potekhin
- B Abbott
- B Abbott
- B Carter
- B Carter
- B Carter
- B Carter
- B Carter
- B Carter
- B Carter
- B Carter
- B Carter
- B Carter
- B Carter
- B Carter
- B Carter
- B Carter
- B Carter
- B Carter
- B Haskell
- B Haskell
- B HĂźttner
- B JĂśnsson
- B Link
- B Link
- B Link
- B Link
- BM Pontecorvo
- BM Pontecorvo
- C Barat
- C Cutler
- C Kittel
- C Monrozeau
- C Peralta
- C Peralta
- CJ Gorter
- CJ Horowitz
- CJ Jog
- CJ Pethick
- CJ Pethick
- CJ Pethick
- CL Inman
- CP Lorenz
- CP Lorenz
- D Chakrabarty
- D Harding
- D Legut
- D Page
- DA Kirszhnits
- DA Kirzhnits
- DG Ravenhall
- DG Ravenhall
- DG Yakovlev
- DG Yakovlev
- DG Yakovlev
- DG Yakovlev
- DG Yakovlev
- DJ Dean
- DK Galloway
- DR Tilley
- DS Tsakadze
- DZ Freedman
- E Chabanat
- E Chabanat
- E Chabanat
- E Flowers
- E Flowers
- E Flowers
- E Gourgoulhon
- E Khan
- E Vigezzi
- E Wigner
- EB Sonin
- EE Kolomeitseiv
- EF Brown
- EJ Yarmchuk
- EL Andronikashvili
- EM Cackett
- F Barranco
- F Barranco
- F Blasio de
- F Douchin
- F Douchin
- F Douchin
- F Douchin
- F Haberl
- F Hund
- F Hund
- F London
- F Montani
- FD Mackie
- FJ Dyson
- FV Blasio de
- FV Blasio de
- FV Blasio de
- FV Blasio de
- FV Blasio de
- FV Blasio de
- G Audi
- G Baym
- G Baym
- G Baym
- G Baym
- G Baym
- G Gori
- G Greenstein
- G Hobbs
- G MartĂnez-Pinedo
- G Mendell
- G Watanabe
- G Watanabe
- G Watanabe
- GA Williams
- GL Israel
- GM Gandelman
- GM Gandelman
- GS Bisnovatyi-Kogan
- H Grigorian
- H Horner
- H Schatz
- H Schatz
- H Shen
- H Shen
- H Sonoda
- H Sotani
- H-T Janka
- H-Y Chiu
- H-Y Chiu
- I Easson
- I Easson
- I Prigogine
- I Slaus
- IH Stairs
- IM Khalatnikov
- J Bardeen
- J Bardeen
- J DechargĂŠ
- J Dobaczewski
- J Grindlay
- J Kohanoff
- J McKenna
- J Miralda-EscudĂŠ
- J Shaham
- J Ventura
- J-R Buchler
- JA Sauls
- JB Hartle
- JB Kinney
- JC Slater
- JD Gelfand
- JF Annett
- JJM Zand inât
- JM Lattimer
- JM Lattimer
- JM Lattimer
- JM Lattimer
- JM Ziman
- JR Oppenheimer
- JR Stone
- JS Heyl
- JS Tsakadze
- JW Negele
- JW Negele
- JWT Hessels
- K Fuchs
- K Glampedakis
- K Glampedakis
- K Glampedakis
- K Iida
- K Iida
- K Iida
- K Langanke
- K Oyamatsu
- K Oyamatsu
- K Oyamatsu
- K Sato
- K Shimizu
- K Sumiyoshi
- K Sumiyoshi
- K Sumiyoshi
- KP Levenfish
- KS Cheng
- L Bildsten
- L Bildsten
- L Lindblom
- L Lindblom
- L Onsager
- L Samuelsson
- L Tisza
- L Villain
- LB Leinson
- LB Leinson
- LD Landau
- LD Landau
- LD Landau
- LD Landau
- LG Cao
- LJ Campbell
- LM Franco
- LP Gorkov
- M Alford
- M Arnould
- M Baldo
- M Baldo
- M Baldo
- M Baldo
- M Baldo
- M Bejger
- M Bender
- M Brack
- M Colpi
- M Farine
- M Hashimoto
- M Hirasawa
- M Lassaut
- M Matsuo
- M Matsuzaki
- M Morii
- M Motokowa
- M Onsi
- M Onsi
- M Prakash
- M Ruderman
- M Ruderman
- M Ruderman
- M Ruderman
- M Ruderman
- M Ruderman
- M Ruderman
- M Vavoulidis
- MA Alpar
- MA Alpar
- MA Alpar
- MA Alpar
- MA Alpar
- MB Larson
- ME Gusakov
- MY Fujimoto
- N Andersson
- N Andersson
- N Andersson
- N Andersson
- N Andersson
- N Andersson
- N Andersson
- N Bohr
- N Chamel
- N Chamel
- N Chamel
- N Chamel
- N Chamel
- N Chamel
- N Chamel
- N Itoh
- N Itoh
- N Itoh
- N Messios
- N Sandulescu
- N Sandulescu
- N Wang
- O Morsch
- O Penrose
- OL Caballero
- OY Gnedin
- P Avogadro
- P Bonche
- P Bonche
- P Donati
- P Donati
- P Donati
- P GĂśgelein
- P Haensel
- P Haensel
- P Haensel
- P Haensel
- P Haensel
- P Haensel
- P Haensel
- P Haensel
- P Jaikumar
- P Jaranowski
- P Kaaret
- P Magierski
- P Nozières
- P Ring
- PB Jones
- PB Jones
- PB Jones
- PB Jones
- PG Gennes de
- PG Gennes de
- PJ Feibelman
- PM Pizzochero
- PM Pizzochero
- PM Woods
- PN McDermott
- PS Shternin
- PS Shternin
- PS Shternin
- PW Anderson
- PW Anderson
- R Beig
- R Combescot
- R Giacconi
- R Nandkumar
- R Ogasawara
- R Prix
- R Prix
- R Ruderman
- R Smoluchowski
- RA Broglia
- RA Duine
- RA Wolf
- RC Duncan
- RC Tolman
- RE Packard
- RE Rutledge
- RI Epstein
- RI Epstein
- RP Feynman
- RP Feynman
- RP Feynman
- S Balibar
- S Bonazzola
- S DallâOsso
- S Goriely
- S Goriely
- S Gupta
- S Heinz
- S Ogata
- SB RĂźster
- SL Shapiro
- ST Belyaev
- T Ellis
- T Maruyama
- T Papenbrock
- T Strohmayer
- T Strohmayer
- T Wong
- TE Sterne
- TE Strohmayer
- TE Strohmayer
- TE Strohmayer
- TE Strohmayer
- TE Strohmayer
- TE Strohmayer
- TJ BĂźrvenich
- TV Shabanova
- U Geppert
- U Lee
- U Lombardo
- VI Ritus
- VI Ritus
- VK Tkachenko
- VK Tkachenko
- VL Ginzburg
- VL Ginzburg
- VL Ginzburg
- VM Kaspi
- VM Kaspi
- VM Kaspi
- VR Pandharipande
- VR Pandharipande
- W Hillebrandt
- W Ketterle
- W Kohn
- WF Vinen
- WG Newton
- Y Levin
- Y Levin
- Y Mochizuki
- Y Pomeau
- Y Yu
- YL Vartanyan
- Z Medin
- à Elgarøy
- à Elgarøy
- à Elgarøy
- Publication venue
- 'Living Reviews'
- Publication date
- 01/01/2008
- Field of study
The physics of neutron star crusts is vast, involving many different research
fields, from nuclear and condensed matter physics to general relativity. This
review summarizes the progress, which has been achieved over the last few
years, in modeling neutron star crusts, both at the microscopic and macroscopic
levels. The confrontation of these theoretical models with observations is also
briefly discussed.Comment: 182 pages, published version available at
<http://www.livingreviews.org/lrr-2008-10
Search for CP violation in D+âĎĎ+ and D+sâK0SĎ+ decays
- Author
- Aaij R
- Adeva B
- Adinolfi M
- Adrover C
- Affolder A
- Ajaltouni Z
- Akiba KC
- Albor VF
- Albrecht J
- Alessio F
- Alexander M
- Ali S
- Alkhazov G
- Altarelli MP
- Alvarez AP
- Alves AA
- Amato S
- Amerio S
- Amhis Y
- Anderlini L
- Anderson J
- Andreassen R
- Appleby RB
- Archilli F
- Artamonov A
- Artuso M
- Aslanides E
- Auriemma G
- Bachmann S
- Back JJ
- Baesso C
- Balagura V
- Baldini W
- Barlow RJ
- Barschel C
- Barsuk S
- Barter W
- Bauer T
- Bay A
- Beddow J
- Bedeschi F
- Bediaga I
- Belogurov S
- Belous K
- Belyaev I
- Ben-Haim E
- Benayoun M
- Bencivenni G
- Benson S
- Benton J
- Berezhnoy A
- Bernet R
- Beteta CA
- Bettler M-O
- Bien A
- Bifani S
- Bird T
- Bizzeti A
- Bjørnstad PM
- Blake T
- Blanc F
- Blouw J
- Blusk S
- Bocci V
- Bondar A
- Bondar N
- Bonivento W
- Borghi S
- Borgia A
- Bowcock TJV
- Bowen E
- Bozzi C
- Brambach T
- Bressieux J
- Brett D
- Britsch M
- Britton T
- Brook NH
- Brown H
- Burducea I
- Bursche A
- Busetto G
- Buytaert J
- Cadeddu S
- Callot O
- Calvi M
- Camboni A
- Campana P
- Carbone A
- Carboni G
- Cardinale R
- Cardini A
- Cardoso LAG
- Carranza-Mejia H
- Carson L
- Cartelle PA
- Casasus MP
- Casse G
- Cattaneo M
- Cauet C
- Charles M
- Charpentier P
- Chen P
- Chiapolini N
- Chrzaszcz M
- Ciba K
- Ciezarek G
- Clarke PEL
- Clemencic M
- Cliff HV
- Closier J
- Coca C
- Coco V
- Cogan J
- Cogneras E
- Collins P
- Comerma-Montells A
- Contu A
- Cook A
- Coombes M
- Coquereau S
- Corti G
- Coutinho RS
- Couturier B
- Cowan GA
- Craik D
- Cunliffe S
- Currie R
- David P
- David PNY
- De Bonis I
- De Bruyn K
- De Capua S
- De Cian M
- De Miranda JM
- De Oyanguren Campos M
- De Paula L
- De Silva W
- De Simone P
- Decamp D
- Deckenhoff M
- Del Buono L
- Derkach D
- Deschamps O
- Dettori F
- Di Canto A
- Diaz RG
- Dijkstra H
- Dogaru M
- Donleavy S
- Dordei F
- dos Reis AC
- Dossett D
- Dovbnya A
- Dupertuis F
- Dzhelyadin R
- Dziurda A
- Dzyuba A
- DâAmbrosio C
- Easo S
- Egede U
- Egorychev V
- Eidelman S
- Eisenhardt S
- Eitschberger U
- Ekelhof R
- Eklund L
- El Rifai I
- Elsasser C
- Elsby D
- Falabella A
- Fardell G
- Farinelli C
- Farry S
- Fave V
- Ferguson D
- Ferro-Luzzi M
- Filippov S
- Fitzpatrick C
- Fontana M
- Fontanelli F
- Forty R
- Francisco O
- Frank M
- Frei C
- Frosini M
- Furcas S
- Furfaro E
- Färber C
- Galli D
- Gandelman M
- Gandini P
- Gao Y
- Garofoli J
- Garosi P
- Garrido L
- Gaspar C
- Gauld R
- Gersabeck E
- Gersabeck M
- Gershon T
- Ghez P
- Gibson V
- Gioi LL
- Gligorov VV
- Goicochea JMO
- Golubkov D
- Golutvin A
- Gomes A
- Gomez MC
- Gordon H
- GraugĂŠs E
- Graziani G
- Grecu A
- Greening E
- Gregson S
- GrĂźnberg O
- Gui B
- Gushchin E
- Gutierrez OA
- Guz Y
- Gys T
- GĂĄndara MG
- GĂśbel C
- Hadjivasiliou C
- Haefeli G
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- Hansmann-Menzemer S
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- Hutchcroft D
- Hynds D
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- Idzik M
- Ilten P
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- Jaton P
- Jing F
- John M
- Johnson D
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- Karacson M
- Karbach TM
- Kenyon IR
- Kerzel U
- Ketel T
- Keune A
- Khanji B
- Kochebina O
- Komarov I
- Koopman RF
- Koppenburg P
- Korolev M
- Kozlinskiy A
- Kravchuk L
- Kreplin K
- Kreps M
- Krocker G
- Krokovny P
- Kruse F
- Kucharczyk M
- Kudryavtsev V
- Kvaratskheliya T
- La Thi VN
- Lacarrere D
- Lafferty G
- Lai A
- Lambert D
- Lambert RW
- Lanciotti E
- Lanfranchi G
- Langenbruch C
- Latham T
- Lazzeroni C
- Le Gac R
- Lees J-P
- Leflat A
- Lefrançois J
- Lefèvre R
- Leo S
- Leroy O
- Leverington B
- Li Y
- Liles M
- Lindner R
- Linn C
- Liu B
- Liu G
- Lohn S
- Lopes JH
- Lopez Asamar E
- Lopez-March N
- Lu H
- Lucchesi D
- Luisier J
- Luo H
- Machefert F
- Machikhiliyan IV
- Maciuc F
- Maev O
- Malde S
- Manca G
- Mancinelli G
- Marconi U
- Marks J
- Martellotti G
- Martens A
- Martin L
- Martinelli M
- Massafferri A
- Matev R
- Mathe Z
- Matteuzzi C
- Maurice E
- Mazurov A
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- Mcnab A
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- Meier F
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- Molina VR
- Monteil S
- Moran D
- Morata JAH
- Morawski P
- Morello MJ
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- Mous I
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- Muresan R
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- MĂźller K
- Naik P
- Nakada T
- Nandakumar R
- Nasteva I
- Needham M
- Neufeld N
- Nguyen AD
- Nguyen TD
- Nguyen-Mau C
- Nicol M
- Niess V
- Niet R
- Nikitin N
- Nikodem T
- Nomerotski A
- Novoselov A
- Oblakowska-Mucha A
- Obraztsov V
- Oggero S
- Ogilvy S
- Okhrimenko O
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- Orlandea M
- Owen P
- Pal BK
- Palano A
- Palutan M
- Panman J
- Papanestis A
- Pappagallo M
- Parkes C
- Parkinson CJ
- Passaleva G
- Patel GD
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- Pellegrino A
- Penso G
- Perazzini S
- Perego DL
- Perez Trigo E
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- Perrin-Terrin M
- Pessina G
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- Petrolini A
- Phan A
- Picatoste Olloqui E
- Pietrzyk B
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- Pinci D
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- Polci F
- Polok G
- Poluektov A
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- Popov D
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- Potterat C
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- Prisciandaro J
- Pugatch V
- Puig Navarro A
- Punzi G
- Qian W
- Rademacker JH
- Rakotomiaramanana B
- Rangel MS
- Raniuk I
- Rauschmayr N
- Raven G
- Redford S
- Reid MM
- Ricciardi S
- Richards A
- Rinnert K
- Roa Romero DA
- Robbe P
- Rodrigues E
- Rodrigues FF
- Rodriguez Perez P
- Rodriguez JM
- Roiser S
- Romanovsky V
- Romero Vidal A
- Rouvinet J
- Ruf T
- Ruffini F
- Ruiz Valls P
- Ruiz H
- Sabatino G
- Saborido Silva JJ
- Sagidova N
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- Sanmartin Sedes B
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- Sciascia B
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- van den Brand J
- van Eijk D
- van Herwijnen E
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- van Tilburg J
- Vazquez Gomez R
- Vazquez Regueiro P
- Vecchi S
- Velthuis JJ
- Veltri M
- Veneziano G
- Vesterinen M
- Viaud B
- Vidal XC
- Vieira D
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- Vollhardt A
- Volyanskyy D
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- Voong D
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- Vorobyev V
- Voss H
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- Websdale D
- Whitehead M
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- Wiechczynski J
- Wiedner D
- Wiggers L
- Wilkinson G
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- Witek M
- Wotton SA
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- Wu S
- Wyllie K
- Xie Y
- Xing F
- Xing Z
- Yang Z
- Young R
- Yuan X
- Yushchenko O
- Yzquierdo AP-C
- Zangoli M
- Zavertyaev M
- Zhang F
- Zhang L
- Zhang WC
- Zhang Y
- Zhelezov A
- Zhokhov A
- Zhong L
- Zvyagin A
- Publication venue
- Springer
- Publication date
- 01/01/2013
- Field of study
A search for CP violation in D + â ĎĎ + decays is performed using data collected in 2011 by the LHCb experiment corresponding to an integrated luminosity of 1.0 fbâ1 at a centre of mass energy of 7 TeV. The CP -violating asymmetry is measured to be (â0.04 Âą 0.14 Âą 0.14)% for candidates with K â K + mass within 20 MeV/c 2 of the Ď meson mass. A search for a CP -violating asymmetry that varies across the Ď mass region of the D + â K â K + Ď + Dalitz plot is also performed, and no evidence for CP violation is found. In addition, the CP asymmetry in the D+sâK0SĎ+ decay is measured to be (0.61 Âą 0.83 Âą 0.14)%
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at â s = 8 TeV with the ATLAS detector
- Author
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fbâ1 of â s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
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- Yilmaz Y
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- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
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- Zeinali M
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- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- Yilmaz Y
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- Yumiceva F
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- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Compressed representation of a partially defined integer function over multiple arguments
- Author
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- Abbiendi G
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
In OLAP (OnLine Analitical Processing) data are analysed in an n-dimensional cube. The cube may be represented as a partially defined function over n arguments. Considering that often the function is not defined everywhere, we ask: is there a known way of representing the function or the points in which it is defined, in a more compact manner than the trivial one
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
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- Abbiendi G
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- Volkov A
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- Volodko A
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- Winn D
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- Wissing C
- Wittich P
- Wittmer B
- Woehri HK
- Wolf M
- Wolf R
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- Won S
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- Wood JS
- Worm SD
- Wright D
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- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yalvac M
- Yang F
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
The azimuthal anisotropy of charged particles in PbPb collisions at
nucleon-nucleon center-of-mass energy of 2.76 TeV is measured with the CMS
detector at the LHC over an extended transverse momentum (pt) range up to
approximately 60 GeV. The data cover both the low-pt region associated with
hydrodynamic flow phenomena and the high-pt region where the anisotropies may
reflect the path-length dependence of parton energy loss in the created medium.
The anisotropy parameter (v2) of the particles is extracted by correlating
charged tracks with respect to the event-plane reconstructed by using the
energy deposited in forward-angle calorimeters. For the six bins of collision
centrality studied, spanning the range of 0-60% most-central events, the
observed v2 values are found to first increase with pt, reaching a maximum
around pt = 3 GeV, and then to gradually decrease to almost zero, with the
decline persisting up to at least pt = 40 GeV over the full centrality range
measured.Comment: Replaced with published version. Added journal reference and DO
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