696 research outputs found
Iceland is an episodic source of atmospheric ice-nucleating particles relevant for mixed-phase clouds.
- Author
- Publication venue
- Sci Adv
- Publication date
- 01/01/2020
- Field of study
Ice-nucleating particles (INPs) have the potential to remove much of the liquid water in climatically important mid- to high-latitude shallow supercooled clouds, markedly reducing their albedo. The INP sources at these latitudes are very poorly defined, but it is known that there are substantial dust sources across the high latitudes, such as Iceland. Here, we show that Icelandic dust emissions are sporadically an important source of INPs at mid to high latitudes by combining ice-nucleating active site density measurements of aircraft-collected Icelandic dust samples with a global aerosol model. Because Iceland is only one of many high-latitude dust sources, we anticipate that the combined effect of all these sources may strongly contribute to the INP population in the mid- and high-latitude northern hemisphere. This is important because these emissions are directly relevant for the cloud-phase climate feedback and because high-latitude dust emissions are expected to increase in a warmer climate
Interaction of dense breast patterns with other breast cancer risk factors in a case–control study
- Author
- Publication venue
- Nature Publishing Group
- Publication date
- Field of study
Availability and quality of anti-malarials among private sector outlets in Myanmar in 2012: results from a large, community-based, cross-sectional survey before a large-scale intervention
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 14/07/2015
- Field of study
BACKGROUND: Global malaria control efforts are threatened by the spread and emergence of artemisinin-resistant Plasmodium falciparum parasites. In 2012, the widespread sale of partial courses of artemisinin-based monotherapy was suspected to take place in the highly accessed, weakly regulated private sector in Myanmar, posing potentially major threats to drug resistance. This study investigated the presence of artemisinin-based monotherapies in the Myanmar private sector, particularly as partial courses of therapy, to inform the targeting of future interventions to stop artemisinin resistance. METHODS: A large cross-sectional survey comprised of a screening questionnaire was conducted across 26 townships in Myanmar between March and May, 2012. For outlets that stocked anti-malarials at the time of survey, a stock audit was conducted, and for outlets that stocked anti-malarials within 3 months of the survey, a provider survey was conducted. RESULTS: A total of 3,658 outlets were screened, 83% were retailers (pharmacies, itinerant drug vendors and general retailers) and 17% were healthcare providers (private facilities and health workers). Of the 3,658 outlets screened, 1,359 outlets (32%) stocked at least one anti-malarial at the time of study. Oral artemisinin-based monotherapy comprised of 33% of self-reported anti-malarials dispensing volumes found. The vast majority of artemisinin-based monotherapy was sold by retailers, where 63% confirmed that they sold partial courses of therapy by cutting blister packets. Very few retailers (5%) had malaria rapid diagnostic tests available, and quality-assured artemisinin-based combination therapy was virtually nonexistent among retailers. CONCLUSION: Informal private pharmacies, itinerant drug vendors and general retailers should be targeted for interventions to improve malaria treatment practices in Myanmar, particularly those that threaten the emergence and spread of artemisinin resistance
Percentage density, Wolfe's and Tabár's mammographic patterns: agreement and association with risk factors for breast cancer
- Author
- AF Saftlas
- AM Oza
- American College of Radiology
- AY El Bastawissi
- C Atkinson
- C Byrne
- CA Haiman
- CH van Gils
- CK Chow
- CM Rutter
- CM Vachon
- DA Harrison
- DV Spicer
- E Couto
- E Funkhouser
- E Sala
- E Sala
- E Warner
- Eiliv Lund
- G Maskarinec
- G Maskarinec
- G Maskarinec
- G Maskarinec
- G Ursin
- G Ursin
- G Ursin
- GA Greendale
- GA Greendale
- Gertraud Maskarinec
- Giske Ursin
- I Andersson
- Inger T Gram
- IT Gram
- IT Gram
- IT Gram
- J Brisson
- J Cuzick
- JL Fleiss
- JN Wolfe
- JN Wolfe
- JN Wolfe
- JP Myles
- JW Byng
- LA Venta
- M Freedman
- N Bjurstam
- NF Boyd
- NF Boyd
- NF Boyd
- Nils Bjurstam
- PM Vacek
- R Warren
- RM Warren
- RW Jakes
- RW Jakes
- S Ciatto
- Yngve Bremnes
- Publication venue
- BioMed Central
- Publication date
- 01/01/2005
- Field of study
INTRODUCTION: The purpose of this report was to classify mammograms according to four methods and to examine their agreement and their relationship to selected risk factors for breast cancer. METHOD: Mammograms and epidemiological data were collected from 987 women, aged 55 to 71 years, attending the Norwegian Breast Cancer Screening Program. Two readers each classified the mammograms according to a quantitative method (Cumulus or Madena software) and one reader according to two qualitative methods (Wolfe and Tabár patterns). Mammograms classified in the reader-specific upper quartile of percentage density, Wolfe's P2 and DY patterns, or Tabár's IV and V patterns, were categorized as high-risk density patterns and the remaining mammograms as low-risk density patterns. We calculated intra-reader and inter-reader agreement and estimated prevalence odds ratios of having high-risk mammographic density patterns according to selected risk factors for breast cancer. RESULTS: The Pearson correlation coefficient was 0.86 for the two quantitative density measurements. There was moderate agreement between the Wolfe and Tabár classifications (Kappa = 0.51; 95% confidence interval 0.46 to 0.56). Age at screening, number of children and body mass index (BMI) showed a statistically significant inverse relationship with high-risk density patterns for all four methods (all P < 0.05). After adjustment for percentage density, the Wolfe classification was not associated with any of the risk factors for breast cancer, whereas the association with number of children and BMI remained statistically significant for the Tabár classification. Adjustment for Wolfe or Tabár patterns did not alter the associations between these risk factors and percentage mammographic density. CONCLUSION: The four assessments methods seem to capture the same overall associations with risk factors for breast cancer. Our results indicate that the quantitative methods convey additional information over the qualitative methods
Chromosomal organization and phylogenetic relationships in Hypochaeris species (Asteraceae) from Brazil
- Author
- Aagaard JE
- André L.L. Vanzela
- Baldwin BG
- Barghi N
- Castilho A
- Cerbah M
- Cerbah M
- Cerbah M
- Cerbah M
- Cipriani G
- Claudete de Fátima Ruas
- Coelho ASG
- Cuadrado A
- Doyle JJ
- Dunemann F
- Fukui K
- Galasso IT
- Galasso IT
- Garrido MA
- Gerlach WL
- Gerlach WL
- Hall KL
- Heslop-Harrison JS
- Heslop-Harrison JS
- Hoey BK
- Jeferson N. Fregonezi
- Kazan K
- Leitch IJ
- Mantel N
- Margarida L.R. de Aguiar-Perecin
- Melissa O. Santos
- Nelson I. Matzenbacher
- Paulo Maurício Ruas
- Ran Y
- Rohlf FJ
- Ruas CF
- Ruas CF
- Samuel R
- Samuel R
- Santala M
- Schubert I
- Schwarzacher T
- Siljak-Yakovlev S
- Stebbins GL
- Stuessy TF
- Welsh J
- Williams JGK
- Wu J
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
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
- Dosil Suarez A
- Dovbnya A
- Dreimanis K
- Dufour L
- Dujany G
- Dungs K
- Durante P
- Dzhelyadin R
- Dziurda A
- Dzyuba A
- Easo S
- Ebert M
- Egede U
- Egorychev V
- Eidelman S
- Eisenhardt S
- Eitschberger U
- Ekelhof R
- Eklund L
- Elsasser Ch
- Ely S
- Esen S
- Evans HM
- Evans T
- Falabella A
- Farber C
- Farley N
- Farry S
- Fay R
- Fazzini D
- Ferguson D
- Fernandez Albor V
- Fernandez Prieto A
- Ferrari F
- Ferreira Rodrigues F
- Ferro-Luzzi M
- Filippov S
- Fini RA
- Fiore M
- Fiorini M
- Firlej M
- Fitzpatrick C
- Fiutowski T
- Fleuret F
- Fohl K
- Fontana M
- Fontanelli F
- Forshaw DC
- Forty R
- Frank M
- Frei C
- Fu J
- Furfaro E
- Gallas Torreira A
- Galli D
- Gallorini S
- Gambetta S
- Gandara M Grabalosa
- Gandelman M
- Gandini P
- Gao Y
- Garcia Martin LM
- Garcia Pardinas J
- Garcia L Castillo
- Garra Tico J
- Garrido L
- Garsed PJ
- Gascon D
- Gaspar C
- Gavardi L
- Gazzoni G
- Gerick D
- Gersabeck E
- Gersabeck M
- Gershon T
- Ghez Ph
- Giani S
- Gibson V
- Girard OG
- Giubega L
- Gizdov K
- Gligorov VV
- Gobel C
- Golubkov D
- Golutvin A
- Gomes A
- Gomez R Vazquez
- Gorelov IV
- Gotti C
- Graciani Diaz R
- Grauges E
- Graverini E
- Graziani G
- Grecu A
- 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
- Kenyon IR
- Kenzie M
- Ketel T
- Khairullin E
- Khanji B
- Khurewathanakul C
- Kirn T
- Klaver S
- Klimaszewski K
- Koliiev S
- Kolpin M
- Komarov I
- Koopman RF
- Koppenburg P
- Kozachuk A
- Kozeiha M
- Kravchuk L
- Kreplin K
- Kreps M
- Krokovny P
- Kruse F
- Krzemien W
- Kucewicz W
- Kucharczyk M
- Kudryavtsev V
- 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
- Leflat A
- Lefrancois J
- Lemaitre F
- Lemos Cid E
- Leroy O
- Lesiak T
- Leverington B
- Li Y
- Likhomanenko T
- Lima V Franco
- Lindner R
- Linn C
- Lionetto F
- Liu B
- Liu X
- Loh D
- Longstaff I
- Lopes JH
- Lucchesi D
- Lucio Martinez M
- Luo H
- Lupato A
- Luppi E
- Lupton O
- Lusiani A
- Lyu X
- Machefert F
- Maciuc F
- Maev O
- Maguire K
- Malde S
- Malinin A
- Maltsev T
- Manca G
- Mancinelli G
- Manning P
- Maratas J
- Marchand JF
- Marconi U
- Marin Benito C
- Marino P
- Marks J
- Martellotti G
- Martin M
- Martinelli M
- Martinez Santos D
- Martinez Vidal F
- Martins Tostes D
- Massacrier LM
- Massafferri A
- Matev R
- Mathad A
- Mathe Z
- Matteuzzi C
- Mauri A
- Maurin B
- Mazurov A
- McCann M
- McCarthy J
- McNab A
- McNulty R
- Meadows B
- Meier F
- Meissner M
- Melnychuk D
- Merk M
- Merli A
- Michielin E
- Milanes DA
- Minard M-N
- Mitzel DS
- Mogini A
- Molina Rodriguez J
- Monroy IA
- Monteil S
- Morandin M
- Morawski P
- Morda A
- Morello MJ
- Moron J
- Morris AB
- Mountain R
- Muheim F
- Mulder M
- Muller D
- Muller J
- Muller K
- Muller V
- Mussini M
- Naik P
- Nakada T
- Nandakumar R
- Nandi A
- Nasteva I
- Navarro A Puig
- Needham M
- Neri N
- Neubert S
- Neufeld N
- Neuner M
- Nguyen AD
- Nguyen-Mau C
- Nieswand S
- Niet R
- Nikitin N
- Nikodem T
- Novoselov A
- O'Hanlon DP
- Oblakowska-Mucha A
- Obraztsov V
- Ogilvy S
- Oldeman R
- Onderwater CJG
- Otalora Goicochea JM
- Otto A
- Owen P
- Oyanguren A
- Pais PR
- Palano A
- Palombo F
- Palutan M
- Panman J
- Papanestis A
- Pappagallo M
- Pappalardo LL
- Parker W
- Parkes C
- Passaleva G
- Pastore A
- Patel GD
- Patel M
- Patrignani C
- Pearce A
- Pellegrino A
- Penso G
- Perazzini S
- Perez D Campora
- Perez DH Campora
- Perez P Rodriguez
- Perret P
- Pescatore L
- Petridis K
- Petrolini A
- Petrov A
- 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
- Polyakov I
- Polycarpo E
- 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
- Sanmartin Sedes B
- Santacesaria R
- Santamarina Rios C
- Santimaria M
- Santovetti E
- Sarti A
- Satriano C
- Satta A
- Saunders DM
- Savrina D
- Schael S
- Schellenberg M
- Schiller M
- Schindler H
- Schlupp M
- Schmelling M
- Schmelzer T
- Schmidt B
- Schneider O
- Schopper A
- Schubert K
- Schubiger M
- Schune M-H
- Schwemmer R
- Sciascia B
- Sciubba A
- Semennikov A
- Sergi A
- Serra N
- Serrano J
- Sestini L
- 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
Evidence for the h_b(1P) meson in the decay Upsilon(3S) --> pi0 h_b(1P)
- Author
- Adametz A.
- Adye T.
- Ahmed H.
- Alam M. S.
- Albert J.
- Allen M. T.
- Alwyn K. E.
- Andreassen R.
- Angelini C.
- Anh TV
- Anulli F.
- Arnaud N.
- Asgeirsson D. J.
- Aston D.
- Atmacan H.
- Ayad R.
- Bailey D.
- Baldini-Ferroli R.
- Band H. R.
- Banerjee Sw.
- Bard D. J.
- Barlow R. J.
- Bartoldus R.
- Batignani G.
- Behera P. K.
- Bellis M.
- Ben-Haim E.
- Benitez J. F.
- Bernard D.
- Bernlochner F. U.
- Bettarini S.
- Bettoni D.
- Bevan A. J.
- Bhuyan B.
- Bianchi F.
- Biasini M.
- Biassoni P.
- Bingham I.
- Blinov V. E.
- Bloom P. C.
- Blount N. L.
- Bomben M.
- Bondioli M.
- Bonneaud G. R.
- Bozzi C.
- Brau J.
- Briand H.
- Brown D. N.
- Brown D. N.
- Buenger C.
- Burchat P. R.
- Buzykaev A. R.
- Cakir IT
- Calabrese R.
- Calcaterra A.
- Calderini G.
- Campagnari C.
- Carpinelli M.
- Cartaro C.
- Casarosa G.
- Castanheira MTD
- Castelli G.
- Cavoto G.
- Cenci R.
- Cervelli A.
- Chauveau J.
- Chavez C. A.
- Chen C.
- Chen X. R.
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- Zucchelli S. Stradling AR
- Zucchelli SVazquez F.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2011
- Field of study
Using a sample of 122 million Upsilon(3S) events recorded with the BaBar
detector at the PEP-II asymmetric-energy e+e- collider at SLAC, we search for
the hb(1P) spin-singlet partner of the P-wave chi_{bJ}(1P) states in the
sequential decay Upsilon(3S) --> pi0 h_b(1P), h_b(1P) --> gamma eta_b(1S). We
observe an excess of events above background in the distribution of the recoil
mass against the pi0 at mass 9902 +/- 4(stat.) +/- 2(syst.) MeV/c^2. The width
of the observed signal is consistent with experimental resolution, and its
significance is 3.1sigma, including systematic uncertainties. We obtain the
value (4.3 +/- 1.1(stat.) +/- 0.9(syst.)) x 10^{-4} for the product branching
fraction BF(Upsilon(3S)-->pi0 h_b) x BF(h_b-->gamma eta_b).Comment: 8 pages, 4 postscript figures, submitted to Phys. Rev. D (Rapid
Communications
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
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- Zieminska D
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- Ziolkowski M
- Zitoun R
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- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
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
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alvarez Estevez M
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arcangeletti C
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
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- Artoni G
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- Asbah N
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Augsten K
- Avolio G
- Ayoub MK
- Azuelos G
- Bachacou H
- Bachas K
- Backes M
- Backman F
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
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- Baldin EM
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- Bannoura AAE
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- Barnett RM
- Barnovska-Blenessy Z
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- Barr AJ
- Barreiro F
- Barsov S
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- Yexley MR
- Yigitbasi E
- Yildiz HD
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- Zanzi D
- Zaripovas DR
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
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- Zimine N
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- Zinonos Z
- Ziolkowski M
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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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