1,061 research outputs found
Study of Bc+ decays to the K+K−π+ final state and evidence for the decay Bc+→χc0π+
- Author
- Aaij R
- Adeva B
- Adinolfi M
- Ajaltouni Z
- Akar S
- Albrecht J
- Alessio F
- Alexander M
- Ali S
- Alkhazov G
- Altarelli M Pepe
- Amato S
- Amerio S
- Amhis Y
- An L
- Anderlini L
- Andreassi G
- Andreotti M
- Andrews JE
- Appleby RB
- Archilli F
- Artamonov A
- Artuso M
- Aslanides E
- Auriemma G
- Baalouch M
- Babuschkin I
- Bachmann S
- Back JJ
- Badalov A
- Baesso C
- Baldini W
- Barlow RJ
- Barschel C
- Barsuk S
- Barter W
- Baszczyk M
- Batozskaya V
- Batsukh B
- Battista V
- Bay A
- Beaucourt L
- Beddow J
- Bedeschi F
- Bediaga I
- Bel LJ
- Bellee V
- Belloli N
- Belous K
- Belyaev I
- Ben-Haim E
- Bencivenni G
- Benson S
- Benton J
- Berezhnoy A
- Bernet R
- Bertolin A
- Betti F
- Bettler M-O
- Bezshyiko Ia
- Bifani S
- Billoir P
- Bird T
- Birnkraut A
- Bitadze A
- Bizzeti A
- Blake T
- Blanc F
- Blouw J
- Blusk S
- Bocci V
- Boettcher T
- Bondar A
- Bondar N
- Bonivento W
- Borgheresi A
- Borghi S
- Borisyak M
- Borsato M
- Bossu F
- Boubdir M
- Bowcock TJV
- Bowen E
- Bozzi C
- Braun S
- Britsch M
- Britton T
- Brodzicka J
- Buchanan E
- Burr C
- Bursche A
- Buytaert J
- Cadeddu S
- Calabrese R
- Calvi M
- Calvo Gomez M
- Camboni A
- Campana P
- Capriotti L
- Carbone A
- Carboni G
- Cardinale R
- Cardini A
- Cardoso LA Granado
- Carniti P
- Carson L
- Cartelle P Alvarez
- Carvalho Akiba K
- Casse G
- Cassina L
- Cattaneo M
- Cauet Ch
- Cavallero G
- Cazon BR Gruberg
- Cenci R
- Charles M
- Charpentier Ph
- Chatzikonstantinidis G
- Chefdeville M
- Chen S
- Cheung S-F
- Chobanova V
- Chrzaszcz M
- Cid Vidal X
- Ciezarek G
- Clarke PEL
- Clemencic M
- Cliff HV
- Closier J
- Coco V
- Cogan J
- Cogneras E
- Cogoni V
- Cojocariu L
- Collaboration Lhcb
- Collaboration LHCb
- Collazuol G
- Collins P
- Comerma-Montells A
- Contu A
- Cook A
- Coquereau S
- Corti G
- Corvo M
- Coutinho R Silva
- Couturier B
- Cowan GA
- Craik DC
- Crocombe A
- Cunliffe S
- Currie R
- D'Ambrosio C
- d'Argent P
- Dall'Occo E
- Dalseno J
- David PNY
- Davis A
- De Aguiar Francisco O
- De Bruyn K
- De Capua S
- De Cian M
- De Miranda JM
- De Paula L
- De Serio M
- De Simone P
- de Vries JA
- Dean C-T
- Decamp D
- Deckenhoff M
- Del Buono L
- Deleage N
- Demmer M
- Derkach D
- Deschamps O
- Dettori F
- Dey B
- Di Canto A
- Dijkstra H
- Dordei F
- Dorigo M
- dos Reis AC
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- Dreimanis K
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- Dujany G
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- Durante P
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- Dziurda A
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- Easo S
- Ebert M
- Egede U
- Egorychev V
- Eidelman S
- Eisenhardt S
- Eitschberger U
- Ekelhof R
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- Elsasser Ch
- Ely S
- Esen S
- Evans HM
- Evans T
- Falabella A
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- Fazzini D
- Ferguson D
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- Gersabeck M
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- Gomez R Vazquez
- Gorelov IV
- Gotti C
- Graciani Diaz R
- Grauges E
- Graverini E
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- Griffith P
- Grillo L
- Grunberg O
- Gushchin E
- Guz Yu
- Gys T
- Hadavizadeh T
- Hadjivasiliou C
- Haefeli G
- Haen C
- Haines SC
- Hall S
- Hamilton B
- Han X
- Hansmann-Menzemer S
- Harnew N
- Harnew ST
- Harrison J
- Hatch M
- He J
- Head T
- Heister A
- Hennessy K
- Henrard P
- Henry L
- Hernando Morata JA
- Hess M
- Hicheur A
- Hill D
- Hombach C
- Hopchev H
- Hulsbergen W
- Humair T
- Hushchyn M
- Hussain N
- Hutchcroft D
- Idzik M
- Ilten P
- Jacobsson R
- Jaeger A
- Jalocha J
- Jans E
- Jawahery A
- John M
- Johnson D
- Jones CR
- Joram C
- Jost B
- Jr Alves AA
- Jurik N
- Kandybei S
- Kanso W
- Karacson M
- Kariuki JM
- Karodia S
- Kecke M
- Kelsey M
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- Ketel T
- Khairullin E
- Khanji B
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- Kolpin M
- Komarov I
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- Kozeiha M
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- Kuonen AK
- Kurek K
- Kvaratskheliya T
- Lacarrere D
- Lafferty G
- Lai A
- Lambert D
- Lanfranchi G
- Langenbruch C
- Langhans B
- Latham T
- Lazzeroni C
- Le Gac R
- Lees J-P
- Lefevre R
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- Maciuc F
- Maev O
- Maguire K
- Malde S
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- Maltsev T
- Manca G
- Mancinelli G
- Manning P
- Maratas J
- Marchand JF
- Marconi U
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- Martellotti G
- Martin M
- Martinelli M
- Martinez Santos D
- Martinez Vidal F
- Martins Tostes D
- Massacrier LM
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- Matev R
- Mathad A
- Mathe Z
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- McCann M
- McCarthy J
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- McNulty R
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- Meier F
- Meissner M
- Melnychuk D
- Merk M
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- Michielin E
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- Mitzel DS
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- Molina Rodriguez J
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- Morawski P
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- Mountain R
- Muheim F
- Mulder M
- Muller D
- Muller J
- Muller K
- Muller V
- Mussini M
- Naik P
- Nakada T
- Nandakumar R
- Nandi A
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- Needham M
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- Neubert S
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- Neuner M
- Nguyen AD
- Nguyen-Mau C
- Nieswand S
- Niet R
- Nikitin N
- Nikodem T
- Novoselov A
- O'Hanlon DP
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- Otalora Goicochea JM
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- Palutan M
- Panman J
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- Pappagallo M
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- Petridis K
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- Petruzzo M
- Picatoste Olloqui E
- Pietrzyk B
- Pikies M
- Pinci D
- Pistone A
- Piucci A
- Playfer S
- Plo Casasus M
- Poikela T
- Polci F
- Poluektov A
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- Pomery GJ
- Popov A
- Popov D
- Popovici B
- Potterat C
- Price E
- Price JD
- Prisciandaro J
- Pritchard A
- Prouve C
- Pugatch V
- Punzi G
- Qian W
- Quagliani R
- Rachwal B
- Rademacker JH
- Rama M
- Ramos Pernas M
- Rangel MS
- Raniuk I
- Raven G
- Redi F
- Reichert S
- Remon Alepuz C
- Renaudin V
- Ricciardi S
- Richards S
- Rihl M
- Rinnert K
- Rives Molina V
- Robbe P
- Rodrigues AB
- Rodrigues E
- Rodriguez Lopez JA
- Rogozhnikov A
- Roiser S
- Romanovskiy V
- Romero Vidal A
- Romeu J Arnau
- Ronayne JW
- Rotondo M
- Rudolph MS
- Ruf T
- Ruiz Valls P
- Saborido Silva JJ
- Sadykhov E
- Sagidova N
- Saitta B
- Salustino Guimaraes V
- Sanchez Mayordomo C
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- Santimaria M
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- Schellenberg M
- Schiller M
- Schindler H
- Schlupp M
- Schmelling M
- Schmelzer T
- Schmidt B
- Schneider O
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- Schubert K
- Schubiger M
- Schune M-H
- Schwemmer R
- Sciascia B
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- Serrano J
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- Seyfert P
- Shapkin M
- Shapoval I
- Shcheglov Y
- Shears T
- Shekhtman L
- Shevchenko V
- Shires A
- Siddi BG
- Silva de Oliveira L
- Simi G
- Simone S
- Sirendi M
- Skidmore N
- Skwarnicki T
- Smith E
- Smith IT
- Smith J
- Smith M
- Snoek H
- Sobral CM Costa
- Sokoloff MD
- Soler FJP
- Souza De Paula B
- Souza D
- Spaan B
- Spradlin P
- Sridharan S
- Stagni F
- Stahl M
- Stahl S
- Stefko P
- Stefkova S
- Steinkamp O
- Stenyakin O
- Stenzel Martins J
- Stevenson S
- Stoica S
- Stone S
- Storaci B
- Stracka S
- Straticiuc M
- Straumann U
- Sun L
- Sutcliffe W
- Swientek K
- Syropoulos V
- Szczekowski M
- Szumlak T
- T'Jampens S
- Tayduganov A
- Tekampe T
- Teklishyn M
- Tellarini G
- Teubert F
- Thomas C
- Thomas E
- Tisserand V
- Tobin M
- Tolk S
- Tomassetti L
- Tonelli D
- Topp-Joergensen S
- Toriello F
- Torres M Cruz
- Tournefier E
- Tourneur S
- Trabelsi K
- Traill M
- Tran MT
- Tresch M
- Trisovic A
- Tsaregorodtsev A
- Tsopelas P
- Tully A
- Tuning N
- Ukleja A
- Ustyuzhanin A
- Uwer U
- Vacca C
- Vagnoni V
- Valassi A
- Valat S
- Valenti G
- Vallier A
- van Beuzekom M
- van Herwijnen E
- van Leerdam J
- van Tilburg J
- van Veghel M
- Vazquez Regueiro P
- Vazquez Sierra C
- Vecchi S
- Velthuis JJ
- Veltri M
- Veneziano G
- Venkateswaran A
- Vernet M
- Vesterinen M
- Viaud B
- Vieira D
- Vieites Diaz M
- Vilasis-Cardona X
- Volkov V
- Vollhardt A
- Voneki B
- Vorobyev A
- Vorobyev V
- Voss C
- Waldi R
- Wallace C
- Wallace R
- Walsh J
- Wang J
- Ward DR
- Wark HM
- Watson NK
- Websdale D
- Weiden A
- Whitehead M
- Wicht J
- Wilkinson G
- Wilkinson M
- Williams M
- Williams M
- Williams MP
- Williams T
- Wilson FF
- Wimberley J
- Wishahi J
- Wislicki W
- Witek M
- Wormser G
- Wotton SA
- Wraight K
- Wright S
- Wyllie K
- Xie Y
- Xing Z
- Xu Z
- Yang Z
- Yin H
- Yu J
- Yuan X
- Yushchenko O
- Zangoli M
- Zarebski KA
- Zavertyaev M
- Zhang L
- Zhang Y
- Zhang Y
- Zhelezov A
- Zheng Y
- Zhokhov A
- Zhu X
- Zhukov V
- Zucchelli S
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2016
- Field of study
A study of Bc+→K+K−π+ decays is performed for the first time
using data corresponding to an integrated luminosity of 3.0 fb−1
collected by the LHCb experiment in pp collisions at centre-of-mass energies
of 7 and 8 TeV. Evidence for the decay Bc+→χc0(→K+K−)π+
is reported with a significance of 4.0 standard deviations, resulting in the
measurement of
σ(B+)σ(Bc+)×B(Bc+→χc0π+) to
be (9.8−3.0+3.4(stat)±0.8(syst))×10−6.
Here B denotes a branching fraction while σ(Bc+) and
σ(B+) are the production cross-sections for Bc+ and B+ mesons.
An indication of bˉc weak annihilation is found for the region
m(K−π+)<1.834GeV/c2, with a significance of
2.4 standard deviations.Comment: All figures and tables, along with any supplementary material and
additional information, are available at
https://lhcbproject.web.cern.ch/lhcbproject/Publications/LHCbProjectPublic/LHCb-PAPER-2016-022.html,
link to supplemental material inserted in the reference
Expression of Drosophila virilis Retroelements and Role of Small RNAs in Their Intrastrain Transposition
- Author
- AB Kuzin
- CD Malone
- DA Petrov
- DE Dalle Nogare
- DJ Obbard
- EE Slawson
- Elena S. Zelentsova
- ER Lozovskaya
- GM Rubin
- GT Lyozin
- H Zelentsova
- HH Kazazian Jr
- IR Arkhipova
- J Brennecke
- J Brennecke
- J Vieira
- JP Blumenstiel
- KA O'Donnell
- KI Pyatkov
- KM Nishida
- L Mejlumian
- LJ Mizrokhi
- LP Zakharenko
- M Mevel-Ninio
- MB Evgen'ev
- MB Evgen'ev
- MB Evgen'ev
- MI Sokolova
- Michael B. Evgen'ev
- N Schostak
- Natalia G. Shostak
- Nikolay V. Rozhkov
- NV Rozhkov
- P Fontanillas
- Pawel Michalak
- PJ Batista
- R Moschetti
- S Chambeyron
- S Tsukahara
- TM Alberola
- VS Scheinker
- VV Kapitonov
- W Leung
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
Transposition of two retroelements (Ulysses and Penelope) mobilized in the course of hybrid dysgenesis in Drosophila virilis has been investigated by in situ hybridization on polytene chromosomes in two D. virilis strains of different cytotypes routinely used to get dysgenic progeny. The analysis has been repeatedly performed over the last two decades, and has revealed transpositions of Penelope in one of the strains, while, in the other strain, the LTR-containing element Ulysses was found to be transpositionally active. The gypsy retroelement, which has been previously shown to be transpositionally inactive in D. virilis strains, was also included in the analysis. Whole mount is situ hybridization with the ovaries revealed different subcellular distribution of the transposable elements transcripts in the strains studied. Ulysses transpositions occur only in the strain where antisense piRNAs homologous to this TE are virtually absent and the ping-pong amplification loop apparently does not take place. On the other hand small RNAs homologous to Penelope found in the other strain, belong predominantly to the siRNA category (21nt), and consist of sense and antisense species observed in approximately equal proportion. The number of Penelope copies in the latter strain has significantly increased during the last decades, probably because Penelope-derived siRNAs are not maternally inherited, while the low level of Penelope-piRNAs, which are faithfully transmitted from mother to the embryo, is not sufficient to silence this element completely. Therefore, we speculate that intrastrain transposition of the three retroelements studied is controlled predominantly at the post-transcriptional level
The Evolution of Compact Binary Star Systems
- Author
- A Ahmad
- A Blaauw
- A Bragaglia
- A Burrows
- A Burrows
- A Burrows
- A Büning
- A Cooray
- A Corongiu
- A Duquennoy
- A Gianninas
- A Heger
- A Kashi
- A Kusenko
- A Massevitch
- A Menon
- A Nebot Gómez-Morán
- A Noriega-Crespo
- A Noutsos
- A Palacios
- A Skumanich
- A Stroeer
- A Stroeer
- A Tornambé
- A Ulla
- A Wongwathanarat
- AA Zdziarski
- AC Fabian
- AE Rosenbush
- AG Kuranov
- AG Kuranov
- AG Lyne
- AG Lyne
- AG Lyne
- AG Massevich
- AG Massevitch
- AG Riess
- AH Prestwich
- AI Bogomazov
- AI Karakas
- AJ Farmer
- AJ Faulkner
- AJ Faulkner
- AJ Loveridge
- AJ Ruiter
- AJ Ruiter
- AJ Ruiter
- AJT Poelarends
- AL Kraus
- AL Piro
- AL Piro
- AL Piro
- AM Cherepashchuk
- AM Cherepashchuk
- AM Cherepashchuk
- AR King
- AR King
- AS Endal
- AS Oliveira
- AV Fedorova
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AV Tutukov
- AW Hotan
- B Külebi
- B Külebi
- B Paczyński
- B Paczyński
- B Paczyński
- B Paczyński
- B Paczyński
- B Paczyński
- B Paczyński
- B Paczyński
- B Paczyński
- B Paxton
- B Paxton
- B Voss
- B Wang
- B Warner
- B Warner
- B Willems
- B Willems
- B Willems
- B Willems
- B-Q For
- BC Barish
- BD Mason
- BD Mason
- BD Metzger
- BE Schaefer
- BJ Shappee
- BJ Shappee
- BMS Hansen
- BP Flannery
- BS Sathyaprakash
- BT Gänsicke
- BT Hayden
- BW Ritchie
- C Badenes
- C Cutler
- C Foellmi
- C Georgy
- C Georgy
- C Georgy
- C Holcomb
- C Karl
- C Kim
- C Knigge
- C Knigge
- C Motch
- C Palenzuela
- C Raskin
- C Raskin
- C Ritossa
- C Weidner
- C-A Faucher-Giguère
- C-A Faucher-Giguère
- CA Whyte
- CD Bailyn
- CD Bailyn
- CJ Deloye
- CJ Philp
- CL Fryer
- CL Fryer
- CL Fryer
- CL Fryer
- CL Fryer
- CL Rodriguez
- CO Heinke
- CR Evans
- D Bhattacharya
- D Branch
- D Foss
- D Gerosa
- D Grossman
- D Hils
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- D Kasen
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- D Raghavan
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- DA Howell
- DJ Champion
- DJ Nice
- DJ Nice
- DL Kaplan
- DM Townsley
- DM Townsley
- DR Lorimer
- DW Schuerman
- E Bear
- E Berger
- E Cappellaro
- E Cappellaro
- E Donder De
- E Donder De
- E Donder De
- E Ergma
- E Ergma
- E García-Berro
- E Kuulkers
- E Livne
- E Livne
- E Nakar
- E Pfahl
- E Pfahl
- E Pfahl
- E Pylyser
- E Schatzman
- E Schatzman
- E-M Pauli
- EE Salpeter
- EF Keane
- EI Popova
- EI Popova
- EJ Lentz
- EL Robinson
- EL Robinson
- EM Green
- EM Sion
- EM Sion
- EM Sion
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- EPJ Heuvel van den
- EPJ Heuvel van den
- EPJ Heuvel van den
- EPJ Heuvel van den
- EPJ Heuvel van den
- EPJ Heuvel van den
- EPJ Heuvel van den
- EPJ Heuvel van den
- ES Phinney
- F Acernese
- F Camilo
- F D’Antona
- F Espinosa Lara
- F Foucart
- F Herwig
- F Herwig
- F Koliopanos
- F Ozel
- F Ozel
- F Patat
- F Ricci
- F Verbunt
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- FX Timmes
- FX Timmes
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- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Nelemans
- G Pandey
- G Ramsay
- G Ramsay
- G Stasińska
- G Tovmassian
- GE Brown
- GE Brown
- GE Soberman
- GH Tovmassian
- GHA Roelofs
- GHA Roelofs
- GJ Savonije
- GL Israel
- GP Kuiper
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- Y Osaki
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- YB Zel’dovich
- YV Baryshev
- Z Barkat
- Z Han
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- Z Kopal
- Z Li
- Z-W Liu
- ZW Liu
- ÉÉ Flanagan
- Publication venue
- 'Living Reviews'
- Publication date
- 03/01/2007
- Field of study
We review the formation and evolution of compact binary stars consisting of
white dwarfs (WDs), neutron stars (NSs), and black holes (BHs). Binary NSs and
BHs are thought to be the primary astrophysical sources of gravitational waves
(GWs) within the frequency band of ground-based detectors, while compact
binaries of WDs are important sources of GWs at lower frequencies to be covered
by space interferometers (LISA). Major uncertainties in the current
understanding of properties of NSs and BHs most relevant to the GW studies are
discussed, including the treatment of the natal kicks which compact stellar
remnants acquire during the core collapse of massive stars and the common
envelope phase of binary evolution. We discuss the coalescence rates of binary
NSs and BHs and prospects for their detections, the formation and evolution of
binary WDs and their observational manifestations. Special attention is given
to AM CVn-stars -- compact binaries in which the Roche lobe is filled by
another WD or a low-mass partially degenerate helium-star, as these stars are
thought to be the best LISA verification binary GW sources.Comment: 105 pages, 18 figure
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
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- Zoeller MH
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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
X-ray emission from the Sombrero galaxy: discrete sources
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- Civinini C
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- Czellar S
- D'Agnolo RT
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- Da Costa EM
- Da Silva WLP
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- Daubie E
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- Yilmaz Y
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- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
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- Zheng Y
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- Zhukov V
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- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zorbilmez C
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2010
- Field of study
We present a study of discrete X-ray sources in and around the
bulge-dominated, massive Sa galaxy, Sombrero (M104), based on new and archival
Chandra observations with a total exposure of ~200 ks. With a detection limit
of L_X = 1E37 erg/s and a field of view covering a galactocentric radius of ~30
kpc (11.5 arcminute), 383 sources are detected. Cross-correlation with Spitler
et al.'s catalogue of Sombrero globular clusters (GCs) identified from HST/ACS
observations reveals 41 X-rays sources in GCs, presumably low-mass X-ray
binaries (LMXBs). We quantify the differential luminosity functions (LFs) for
both the detected GC and field LMXBs, whose power-low indices (~1.1 for the
GC-LF and ~1.6 for field-LF) are consistent with previous studies for
elliptical galaxies. With precise sky positions of the GCs without a detected
X-ray source, we further quantify, through a fluctuation analysis, the GC LF at
fainter luminosities down to 1E35 erg/s. The derived index rules out a
faint-end slope flatter than 1.1 at a 2 sigma significance, contrary to recent
findings in several elliptical galaxies and the bulge of M31. On the other
hand, the 2-6 keV unresolved emission places a tight constraint on the field
LF, implying a flattened index of ~1.0 below 1E37 erg/s. We also detect 101
sources in the halo of Sombrero. The presence of these sources cannot be
interpreted as galactic LMXBs whose spatial distribution empirically follows
the starlight. Their number is also higher than the expected number of cosmic
AGNs (52+/-11 [1 sigma]) whose surface density is constrained by deep X-ray
surveys. We suggest that either the cosmic X-ray background is unusually high
in the direction of Sombrero, or a distinct population of X-ray sources is
present in the halo of Sombrero.Comment: 11 figures, 5 tables, ApJ in pres
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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- Wilken R
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- Willmott C
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- Wissing C
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- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yalvac M
- Yang F
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- 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
- Zang SL
- 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
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- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zotto P
- Zou W
- 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
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
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- Adiguzel A
- Adler V
- Adzic P
- Afanasiev S
- Agostino L
- Agram JL
- Aguilar-Benitez M
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- Andreev Y
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- Chang YH
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- Chauhan S
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- Ciulli V
- Civinini C
- Claes DR
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- Clerbaux B
- Cline D
- CMS Collaboration
- Coarasa Perez JA
- Cockerill DJA
- Codispoti G
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- Costantini S
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- Coughlan JA
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- Cumalat JP
- Cuplov V
- Cushman P
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- Winer BL
- Winn D
- Winstrom L
- Wissing C
- Wittich P
- Wittmer B
- Woehri HK
- Wolf M
- Wolf R
- Womersley WJ
- Won S
- Wood D
- Wood J
- Wood JS
- Worm SD
- Wright D
- Wrochna G
- Wu W
- Wuerthwein F
- Wulz C-E
- 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
Performance of the CMS Cathode Strip Chambers with Cosmic Rays
- Author
- Abadjiev K
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abelev B
- Acosta D
- Acosta JG
- Acosta MV
- Actis O
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adolphi R
- Adzic P
- Afaq MA
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Ahmad M
- Ahmad WH
- Ahmed I
- Ahmed W
- Ahuja S
- Aisa D
- Aisa S
- Akchurin N
- Akgun B
- Akgun U
- Akimenko S
- Akin IV
- Alagoz E
- Alampi G
- Albajar C
- Albayrak EA
- Alberdi J
- Albergo S
- Albert E
- Albrow M
- Alexander J
- Alidra M
- Aliev T
- Allfrey P
- Almeida N
- Altenhofer G
- Altsybeev I
- Alver B
- Alverson G
- Alves GA
- Amaglobeli N
- Amapane N
- Ambroglini F
- Amsler C
- Anagnostou G
- Ananthan B
- Anastassov A
- Andelin D
- Anderson M
- Andrea J
- Andreev V
- Andreev Y
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2009
- Field of study
The Cathode Strip Chambers (CSCs) constitute the primary muon tracking device
in the CMS endcaps. Their performance has been evaluated using data taken
during a cosmic ray run in fall 2008. Measured noise levels are low, with the
number of noisy channels well below 1%. Coordinate resolution was measured for
all types of chambers, and fall in the range 47 microns to 243 microns. The
efficiencies for local charged track triggers, for hit and for segments
reconstruction were measured, and are above 99%. The timing resolution per
layer is approximately 5 ns
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
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- Weiler T
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- Wuerthwein F
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- Wyslouch B
- Xiao H
- Xie S
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- Yalvac M
- Yang F
- Yang M
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- Yazgan E
- Yelton J
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
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- 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
- Zielinski M
- Zito G
- Zou W
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
A search for new physics is performed in events with two same-sign isolated
leptons, hadronic jets, and missing transverse energy in the final state. The
analysis is based on a data sample corresponding to an integrated luminosity of
4.98 inverse femtobarns produced in pp collisions at a center-of-mass energy of
7 TeV collected by the CMS experiment at the LHC. This constitutes a factor of
140 increase in integrated luminosity over previously published results. The
observed yields agree with the standard model predictions and thus no evidence
for new physics is found. The observations are used to set upper limits on
possible new physics contributions and to constrain supersymmetric models. To
facilitate the interpretation of the data in a broader range of new physics
scenarios, information on the event selection, detector response, and
efficiencies is provided.Comment: Published in Physical Review Letter
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
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- Abramowicz H
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- Castillo FL
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- Catinaccio A
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- Chevalerias TJA
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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 fb−1 of √ 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
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