804 research outputs found
Multidimensional analyses to assess the relations between treatment choices by physicians and patients’ characteristics: the example of COPD
- Author
- AL Ries
- B Celli
- B Scherrer
- Bertrand Delclaux
- BR Celli
- BR Celli
- Bruno Scherrer
- Christos Chouaid
- CR Jenkins
- D Tashkin
- DE O’Donnell
- DE O’Donnell
- DP Tashkin
- DP Tashkin
- DP Tashkin
- G Jebrak
- Hervé Pégliasco
- JA Wedzicha
- JD Lebreton
- Jean-Michel Marcos
- JR Hurst
- K Fitch
- K Tatsumi
- L-P Boulet
- M Decramer
- N Roche
- National Heart Lung and Blood Institute
- Nicolas Roche
- P Legendre
- PM Calverley
- PR Burgel
- PR Burgel
- R de Marco
- SD Aaron
- Yan Martinat
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Species replacement dominates megabenthos beta diversity in a remote seamount setting
- Author
- A Genin
- A Stevenson
- A Vilmi
- A Williams
- AA Rowden
- AA Rowden
- AM Quattrini
- AR Baco
- C Yesson
- CR McClain
- CR McClain
- CR McClain
- CR McClain
- CR McClain
- DP Tittensor
- EJW Jones
- H Staudigel
- J Heino
- J Sarrazin
- JJ Lennon
- JR Hein
- K Wishner
- KL Howell
- KO Kvile
- L Lundsten
- L Watling
- L Watling
- L-A Henry
- LA Henry
- LA Levin
- LA Levin
- M Costello
- M Wagstaff
- MR Clark
- MR Clark
- MR Clark
- N Kumar
- P Legendre
- P Legendre
- P Wessel
- R Turnewitsch
- RL O’Driscoll
- S Brault
- S Samadi
- SERGIO P. ÁVILA
- TA Schlacher
- TD O’Hara
- TD O’Hara
- W.J. Emery
- X Wang
- Zahra Alsaffar
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
Seamounts are proposed to be hotspots of deep-sea biodiversity, a pattern potentially arising from increased productivity in a heterogeneous landscape leading to either high species co-existence or species turnover (beta diversity). However, studies on individual seamounts remain rare, hindering our understanding of the underlying causes of local changes in beta diversity. Here, we investigated processes behind beta diversity using ROV video, coupled with oceanographic and quantitative terrain parameters, over a depth gradient in Annan Seamount, Equatorial Atlantic. By applying recently developed beta diversity analyses, we identified ecologically unique sites and distinguished between two beta diversity processes: species replacement and changes in species richness. The total beta diversity was high with an index of 0.92 out of 1 and was dominated by species replacement (68%). Species replacement was affected by depth-related variables, including temperature and water mass in addition to the aspect and local elevation of the seabed. In contrast, changes in species richness component were affected only by the water mass. Water mass, along with substrate also affected differences in species abundance. This study identified, for the first time on seamount megabenthos, the different beta diversity components and drivers, which can contribute towards understanding and protecting regional deep-sea biodiversity
Search for rare quark-annihilation decays, B --> Ds(*) Phi
- Author
- Abe T
- Abrams GS
- Adye T
- Ahmed M
- Ahmed S
- Alam MS
- Albert J
- Aleksan R
- Allen MT
- Allison J
- Allmendinger T
- Altenburg D
- Andreassen R
- Andreotti M
- Angelini C
- Anulli F
- Arnaud N
- Aston D
- Aubert B
- Azzolini V
- Baak M
- Back JJ
- Baldini-Ferroli R
- Band HR
- Banerjee S
- Barate R
- Bard DJ
- Barlow NR
- Barlow RJ
- Barrett M
- Bartoldus R
- Batignani G
- Battaglia M
- Bauer JM
- Beck TW
- Behera PK
- Bellini F
- Benayoun M
- Benelli G
- Berger N
- Bernard D
- Berryhill JW
- Best D
- Bettarini S
- Bettoni D
- Bevan AJ
- Bhimji W
- Bhuyan B
- Bianchi F
- Biasini M
- Biesiada J
- Blanc F
- Blaylock G
- Blinov AE
- Blinov VE
- Bloom PC
- Blount NL
- Bomben M
- Bona M
- Bondioli M
- Bonneaud GR
- Bosisio L
- Boutigny D
- Bowerman DA
- Boyarski AM
- Boyd JT
- Bozzi C
- Brandenburg G
- Brandt T
- Brau J
- Breon AB
- Brose J
- Brown CL
- Brown CM
- Brown DN
- Brown DN
- Bruinsma M
- Brunet S
- Bucci F
- Buchanan C
- Buchmueller OL
- Bugg W
- Bukin AD
- Bula R
- Bulten H
- Buono LD
- Burchat PR
- Burke JP
- Button-Shafer J
- Buzzo A
- Cahn RN
- Calabrese R
- Calcaterra A
- Calderini G
- Campagnari C
- Capra R
- Carpinelli M
- Cartaro C
- Cavallo N
- Cavoto G
- Cenci R
- Chai X
- Chaisanguanthum KS
- Chao M
- Charles E
- Charles MJ
- Chauveau J
- Chavez CA
- Chen A
- Chen C
- Chen E
- Chen JC
- Chen S
- Chen X
- Cheng B
- Cheng CH
- Chia YM
- Cibinetto G
- Clark PJ
- Claus R
- Cochran J
- Coleman JP
- Collaboration BABAR
- Contri R
- Convery MR
- Cossutti F
- Cote D
- Cottingham WN
- Couderc F
- Covarelli R
- Cowan G
- Cowan R
- Crawley HB
- Cremaldi L
- Cristinziani M
- Cuhadar-Donszelmann T
- Cunha A
- Curry S
- D'Orazio A
- Dahmes B
- Dallapiccola C
- Danielson N
- Dasu S
- Datta M
- Dauncey PD
- David P
- Davier M
- Davis CL
- Day CT
- de la Vaissiere C
- de Monchenault GH
- de Sangro R
- del Re D
- Diberder FL
- Dickopp M
- Dingfelder JC
- Dittongo S
- Dong D
- Dong L
- Dorfan J
- Druzhinin VP
- Dubitzky RS
- Dubois-Felsmann GP
- Dujmic D
- Dunwoodie W
- Dvoretskii A
- Eckhart EA
- Eckmann R
- Edgar CL
- Edwards AJ
- Egede U
- Eichenbaum AM
- Eigen G
- Eisner AM
- Elmer P
- Emery S
- Ernst JA
- Eschenburg V
- Eschrich I
- Eyges V
- Fabozzi F
- Faccini R
- Fan S
- Feltresi E
- Ferrarotto F
- Ferroni F
- Field RC
- Finocchiaro G
- Flacco CJ
- Flack RL
- Flaecher HU
- Flood KT
- Ford KE
- Ford WT
- Forster IJ
- Forti F
- Fortin D
- Foulkes SD
- Franek B
- Frey R
- Fritsch M
- Fry JR
- Fulsom BG
- Gabathuler E
- Gaidot A
- Gaillard JR
- Galeazzi F
- Gallo F
- Gamba D
- Gamet R
- Gan KK
- Ganzhur SF
- Gary JW
- Gaspero M
- Gatto C
- George KA
- Gill MS
- Gioi LL
- Giorgi MA
- Giroux X
- Gladney L
- Glanzman T
- Godang R
- Goetzen K
- Golubev VB
- Gopal GP
- Gowdy SJ
- Gradl W
- Graham MT
- Grancagnolo S
- Grauges E
- Graziani G
- Green MG
- Grenier P
- Gritsan AV
- Groot ND
- Grosdidier G
- Groysman Y
- Guo QH
- Hadavand HK
- Hadig T
- Haire M
- Halyo V
- Hamano K
- Hamon O
- Harrison PF
- Harrison TJ
- Hart AJ
- Hartfiel BL
- Hast C
- Hauke A
- Hawkes CM
- Hearty C
- Held T
- Hertzbach SS
- Heusch CA
- Hill EJ
- Hirschauer JF
- Hitlin DG
- Hocker A
- Hodgkinson MC
- Hollar JJ
- Hong TM
- Honscheid K
- Hopkins DA
- Hryn'ova T
- Hufnagel D
- Hulsbergen WD
- Hutchcroft DE
- Igonkina O
- Innes WR
- Izen JM
- Jackson PD
- Jackson PS
- Jacobsen RG
- Jawahery A
- Jessop CP
- John MJJ
- Johnson JR
- Judd D
- Kadel RW
- Kadyk J
- Kagan H
- Karyotakis Y
- Kass R
- Kelly MP
- Kelsey MH
- Kerth LT
- Khan A
- Kim H
- Kim P
- Kirkby D
- Kitayama I
- Klose V
- Knecht NS
- Koch H
- Kocian ML
- Koeneke K
- Kofler R
- Kolomensky YG
- Kovalskyi D
- Kowalewski R
- Kozanecki W
- Kravchenko EA
- Kreisel A
- Krishnamurthy M
- Kroeger R
- Kroseberg J
- Kukartsev G
- Kutter PE
- Kyberd P
- Lacker HM
- Lae CK
- Lafferty GD
- Lanceri L
- Lange DJ
- Langenegger U
- Lankford AJ
- Latham TE
- Latour E
- Lau YP
- Lazzaro A
- Lees JP
- Legendre M
- Leith DWGS
- Lepeltier V
- Leruste P
- Lewandowski B
- Li H
- Li X
- Libby J
- Lista L
- Liu R
- Lockman WS
- Lodovico FD
- Lombardo V
- London GW
- Long O
- LoSecco JM
- Lou XC
- Lu C
- Lu M
- Luitz S
- Lund P
- Luppi E
- Lusiani A
- Luth V
- Lutz AM
- Lynch G
- Lynch HL
- MacFarlane DB
- Macri MM
- Mader WF
- Majewski SA
- Malcles J
- Mallik U
- Mancinelli G
- Mandelkern M
- Marchiori G
- Marco ED
- Margoni M
- Marks J
- Marsiske H
- Martinez-Vidal F
- Mattison TS
- Mayer B
- Mazur MA
- Mazzoni MA
- McKenna JA
- McMahon TR
- Meadows BT
- Mellado B
- Menges W
- Messner R
- Meyer WT
- Mihalyi A
- Minamora JS
- Mir LM
- Mohanty GB
- Mohapatra AK
- Mommsen RK
- Monge MR
- Monorchio D
- Moore TB
- Morandin M
- Morgan SE
- Morganti M
- Morganti S
- Morii M
- Muheim F
- Muller DR
- Naisbit MT
- Nardo GD
- Narsky I
- Nash JA
- Nauenberg U
- Neal H
- Negrini M
- Neri N
- Nesom G
- Nicholson H
- Nikolich MB
- Nogowski R
- Nugent IM
- O'Grady CP
- Ocariz J
- Oddone PJ
- Ofte I
- Olaiya EO
- Olivas A
- Olsen J
- Onuchin AP
- Orimoto TJ
- Otto S
- Oyanguren A
- Ozcan VE
- Paar HP
- Pacetti S
- Palano A
- Palombo F
- Pan Y
- Panetta J
- Panvini RS
- Paoloni E
- Paolucci P
- Pappagallo M
- Parry RJ
- Passaggio S
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Pelizaeus M
- Perazzo A
- Perl M
- Peruzzi IM
- Peters K
- Petersen BA
- Petersen TC
- Petzold A
- Piatenko T
- Piccolo D
- Piccolo M
- Piemontese L
- Pierini M
- Pioppi M
- Piredda G
- Plaszczynski S
- Playfer S
- Poireau V
- Polci F
- Pompili A
- Porter FC
- Posocco M
- Potter CT
- Prell S
- Prepost R
- Pripstein M
- Pulliam T
- Purohit MV
- Qi ND
- Rahatlou S
- Rahimi AM
- Rahmat R
- Rama M
- Ratcliff BN
- Raven G
- Reidy J
- Ricca GD
- Ricciardi S
- Richman JD
- Ritchie JL
- Rizzo G
- Roat C
- Roberts DA
- Robertson SH
- Robutti E
- Rodier S
- Roe NA
- Roethel W
- Ronan MT
- Roney JM
- Rong G
- Roodman A
- Roos L
- Rosenberg EI
- Rotondo M
- Roudeau P
- Rubin AE
- Ruddick WO
- Ryd A
- Sacco R
- Saeed MA
- Saleem M
- Salnikov AA
- Salvatore F
- Samuel A
- Sanders DA
- Santroni A
- Saremi S
- Satpathy A
- Schalk T
- Schenk S
- Schindler RH
- Schofield KC
- Schott G
- Schrenk S
- Schroder H
- Schroeder T
- Schubert J
- Schubert KR
- Schumm BA
- Schune MH
- Schwiening J
- Schwierz R
- Schwitters RF
- Sciacca C
- Sciolla G
- Seiden A
- Sekula SJ
- Serednyakov SI
- Sharma V
- Shen BC
- Simi G
- Simonetto F
- Sinev NB
- Skovpen YI
- Smith AJS
- Smith JG
- Snoek HL
- Snyder A
- Sobie RJ
- Soffer A
- Sokoloff MD
- Solodov EP
- Spaan B
- Spanier SM
- Spitznagel M
- Spradlin P
- Staengle H
- Steinke M
- Stelzer J
- Stocchi A
- Stoker DP
- Stroili R
- Strom D
- Strube J
- Stugu B
- Su D
- Sullivan MK
- Summers DJ
- Sundermann JE
- Suzuki K
- Swain SK
- Tan P
- Taras P
- Taylor F
- Tehrani FS
- Telnov AV
- Teodorescu L
- Ter-Antonyan R
- Therin G
- Thiebaux C
- Thompson JM
- Tisserand V
- Toki WH
- Torrence E
- Tosi S
- Touramanis C
- Ulmer KA
- Uwer U
- Va'vra J
- van Bakel N
- Vasileiadis G
- Vasseur G
- Vazquez WP
- Verderi M
- Verkerke W
- Vetere ML
- Viaud FB
- Vitale L
- Voci C
- Voena C
- Wagner SR
- Wagoner DE
- Waldi R
- Walsh J
- Wang K
- Wang P
- Wang WF
- Wappler FR
- Watson AT
- Weaver M
- Weidemann AW
- Weinstein AJR
- Wenzel WA
- Wilden L
- Williams DC
- Williams JC
- Willocq SY
- Wilson FF
- Wilson JR
- Wilson MG
- Wilson RJ
- Winklmeier F
- Wisniewski WJ
- Wittgen M
- Wong QK
- Wormser G
- Wright DH
- Wright DM
- Wu J
- Wu SL
- Xie Y
- Yamamoto RK
- Yarritu AK
- Ye S
- Yeche C
- Yi JI
- Yi K
- Young CC
- Yu Z
- Yushkov AN
- Zain SB
- Zallo A
- Zeng Q
- Zghiche A
- Zhang J
- Zhang L
- Zhao HW
- Zhu YS
- Ziegler V
- Zito M
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 12/12/2005
- Field of study
We report on searches for B- --> Ds- Phi and B- --> Ds*- Phi. In the context
of the Standard Model, these decays are expected to be highly suppressed since
they proceed through annihilation of the b and u-bar quarks in the B- meson.
Our results are based on 234 million Upsilon(4S) --> B Bbar decays collected
with the BABAR detector at SLAC. We find no evidence for these decays, and we
set Bayesian 90% confidence level upper limits on the branching fractions BF(B-
--> Ds- Phi) Ds*- Phi)<1.2x10^(-5). These results
are consistent with Standard Model expectations.Comment: 8 pages, 3 postscript figues, submitted to Phys. Rev. D (Rapid
Communications
Testing the Goodness of Supplementary Feeding to Enhance Population Viability in an Endangered Vulture
- Author
- A Margalida
- A Margalida
- A Margalida
- A Margalida
- A Margalida
- A Sanz
- Andy Hector
- Antoni Margalida
- BE Sæther
- BK Williams
- CP Chamberlain
- Daniel Oro
- DP Whitfield
- G Blanco
- G Blanco
- G Tavecchia
- G Tavecchia
- GC White
- GN Robb
- IPP Owens
- JA Lemus
- JA Sesé
- JD Lebreton
- JL Tella
- JM Cushing
- JM Halley
- José Antonio Donázar
- LM González
- LS Mills
- M Cardillo
- M Carrete
- M Carrete
- M Carrete
- M Gilbert
- M Hernández
- M Schaub
- Martina Carrete
- P Inchausti
- P Mundy
- PM Bennett
- R Choquet
- R Cluthbert
- R Heredia
- R Heredia
- R Lande
- Rafael Heredia
- RE Green
- RJ Antor
- S Legendre
- SR Wilbur
- V Bretagnolle
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2008
- Field of study
[Background]: Human-predator conflicts are directly or indirectly threatening many species with extinction. Thus, biologists are urged to find simple solutions to complex situations while avoiding unforeseen conservation outcomes. The provision of supplementary food at artificial feeding sites (AFS) is frequently used in the conservation of scavenger bird populations currently suffering from indirect poisoning, although no scientific studies on its effectiveness have been conducted.[Methodology/Principal Findings]: We used a long-term data set of 95 individually marked birds from the largest European core of the endangered bearded vulture (Gypaetus barbatus) to test the long-term effects of specific AFS for bearded vultures on their survival rates (by CMR models) and population dynamics (by Monte Carlo simulations) in an area where fatalities derived from illegal poisoning and the use of other toxics like veterinary drugs have increased over the last several years. Our data support the positive relationship between the use of AFS and survival. However, contrary to theoretical predictions (e.g. high and more stable adult survival among long-lived species), the use of AFS increased only survival of pre-adults. Moreover, AFS buffered the effects of illegal poisoning on this age-class, while adult survival decreased over years. Our simulations predicted a maximum value of extinction probability over a time horizon of 50 years. Population projections run with survival rates expected in scenarios without poisoning predicted the situation of least conservation concern, while including only AFS can maintain a large floater surplus that may delay population decline but fails to reduce poisoning risk among adults.[Conclusions/Significance]: Although AFS are not effective to save bearded vultures from an expected population decline, they delay population extinction and can be a useful tool for prolonging population viability while combating illegal and indirect poisoning. The eradication of different sources of poisoning is of top priority to ensure the long-term viability of this and many other species.Financial support for AM was obtained from the Departament of Medi Ambient i Habitatge of Generalitat de Catalunya and Ministry of Environment. MC was supported by an Excellence post-doctoral contract (Junta de Andalucía).Peer reviewe
Observation of associated near-side and away-side long-range correlations in √sNN=5.02 TeV proton-lead collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- Abouzeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Allbrooke BM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alvarez Gonzalez B
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov A
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Aperio Bella L
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce AT
- Arfaoui S
- Arguin JF
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Astbury A
- Atkinson M
- ATLAS Collaboration The
- Auerbach B
- Auge E
- Augsten K
- Aurousseau M
- Avolio G
- Axen D
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Backus Mayes J
- Badescu E
- Bagnaia P
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
- Baker S
- Balek P
- Balli F
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barak L
- Baranov SP
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro Guimarães da Costa J
- Barreiro F
- Bartoldus R
- Barton AE
- Bartsch V
- Basye A
- Bates RL
- Batkova L
- Batley JR
- Battaglia A
- Battistin M
- Bauer F
- Bawa HS
- Beale S
- Beau T
- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck HP
- Becker K
- Becker S
- Beckingham M
- Becks KH
- Beddall A
- Beddall AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Beemster LJ
- Beermann TA
- Begel M
- Behar Harpaz S
- Belanger-Champagne C
- Bell PJ
- Bell WH
- Bella G
- Bellagamba L
- Bellomo M
- Belloni A
- Beloborodova O
- Belotskiy K
- Beltramello O
- Benary O
- Benchekroun D
- Bendtz K
- Benekos N
- Benhammou Y
- Benhar Noccioli E
- Benitez Garcia JA
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Berge D
- Bergeaas Kuutmann E
- Berger N
- Berghaus F
- Berglund E
- Beringer J
- Bernat P
- Bernhard R
- Bernius C
- Bernlochner FU
- Berry T
- Bertella C
- Bertin A
- Bertolucci F
- Besana MI
- Besjes GJ
- Besson N
- Bethke S
- Bhimji W
- Bianchi RM
- Bianchini L
- Bianco M
- Biebel O
- Bieniek SP
- Bierwagen K
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
- Bingul A
- Bini C
- Biscarat C
- Bittner B
- Black CW
- Black JE
- Black KM
- Blair RE
- Blanchard JB
- Blazek T
- Bloch I
- Blocker C
- Blocki J
- Blum W
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boddy CR
- Boehler M
- Boek J
- Boek TT
- Boelaert N
- Bogaerts JA
- Bogdanchikov A
- Bogouch A
- Bohm C
- Bohm J
- Boisvert V
- Bold T
- Boldea V
- Bolnet NM
- Bomben M
- Bona M
- Boonekamp M
- Bordoni S
- Borer C
- Borisov A
- Borissov G
- Borjanovic I
- Borri M
- Borroni S
- Bortfeldt J
- Bortolotto V
- Bos K
- Boscherini D
- Bosman M
- Boterenbrood H
- Bouchami J
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Bousson N
- Boutouil S
- Boveia A
- Boyd J
- Boyko IR
- Bozovic-Jelisavcic I
- Bracinik J
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- Zaidan R
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- Zemla A
- Zenin O
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- Zevi Della Porta G
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- Zhemchugov A
- Zhong J
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- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivković L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (Δϕ) and pseudorapidity (Δη) are measured in √sNN=5.02 TeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1 μb-1 of data as a function of transverse momentum (pT) and the transverse energy (ΣETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Δη|<5) “near-side” (Δϕ∼0) correlation that grows rapidly with increasing ΣETPb. A long-range “away-side” (Δϕ∼π) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ΣETPb, is found to match the near-side correlation in magnitude, shape (in Δη and Δϕ) and ΣETPb dependence. The resultant Δϕ correlation is approximately symmetric about π/2, and is consistent with a dominant cos2Δϕ modulation for all ΣETPb ranges and particle pT
Search for R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
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- Ye J
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- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
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- Zeitnitz C
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- Zemla A
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- Zenin O
- Zenis T
- Zinonos Z
- Zerwas D
- della Porta GZ
- Zhang D
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- Zhao Z
- Zhemchugov A
- Zhong J
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- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Collaboration ATLAS
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2008
- Field of study
A search for new phenomena in final states with four or more leptons (electrons or muons) is presented. The analysis is based on 4.7 fb−1 of s=7TeV proton-proton collisions delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in two signal regions: one that requires moderate values of missing transverse momentum and another that requires large effective mass. The results are interpreted in a simplified model of R-parity-violating supersymmetry in which a 95% CL exclusion region is set for charged wino masses up to 540 GeV. In an R-parity-violating MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are excluded for 10 < tan β < 40
Search for high-mass resonances decaying to dilepton final states in pp collisions at s√=7 TeV with the ATLAS detector
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- Abajyan T
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- Abdallah J
- Abdelalim AA
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- Meguro T
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- Schamov AG
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- Schegelsky VA
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- Scherzer MI
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- Schorlemmer ALS
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- Schroeder TV
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- Schultens MJ
- Schultes J
- Schultz-Coulon H-C
- Schulz H
- Schumacher M
- Schumm BA
- Schune P
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- Schwartzman A
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- Schwemling P
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- Schwierz R
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- Searcy J
- Sedov G
- Sedykh E
- Seidel SC
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- Seixas JM
- Sekhniaidze G
- Sekula SJ
- Selbach KE
- Seliverstov DM
- Sellden B
- Sellers G
- Seman M
- Semprini-Cesari N
- Serfon C
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- Serkin L
- Seuster R
- Severini H
- Sfyrla A
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- Shamim M
- Shan LY
- Shank JT
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- Shatalov PB
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- Sherwood P
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- Shimojima M
- Shin T
- Shiyakova M
- Shmeleva A
- Shochet MJ
- Short D
- Shrestha S
- Shulga E
- Shupe MA
- Sicho P
- Sidoti A
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- Simonyan M
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- Sinev NB
- Sipica V
- Siragusa G
- Sircar A
- Sisakyan AN
- Sivoklokov SY
- Sjoelin J
- Sjursen TB
- Skinnari LA
- Skottowe HP
- Skovpen K
- Skubic P
- Slater NM
- Slavicek T
- Sliwa K
- Smakhtin V
- Smart BH
- Smestad L
- Smirnov SY
- Smirnov Y
- Smirnova LN
- Smirnova O
- Smit GVY
- Smith BC
- Smith D
- Smith KM
- Smizanska M
- Smolek K
- Snesarev AA
- Snow J
- Snow SW
- Snyder S
- Sobie R
- Sodomka J
- Soffer A
- Soh DA
- Soiovyallv V
- Solans CA
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- Soldatov EY
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- Solodkov AA
- Solovyev V
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- Stanescu-Bellu M
- Stanitzki MM
- Stapnes S
- Starchenko EA
- Stark J
- Staroba P
- Starovoitov P
- Staszewski R
- Staude A
- Stavina P
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- Steinbach P
- Steinberg P
- Stekl I
- Stelzer B
- Stelzer HJ
- Stelzer-Chilton O
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- Stoicea G
- Stonjek S
- Strachota P
- Stradling AR
- Straessner A
- Strandberg J
- Strandberg S
- Strandlie A
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- Stroehmer R
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- Stroynowski R
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- Stumer I
- Stupak J
- Sturm P
- Styles NA
- Su D
- Subramania HS
- Subramaniam R
- Succurro A
- Sugaya Y
- Suhr C
- Suk M
- Sulin VV
- Sultansoy S
- Sumida T
- Sun X
- Sundermann JE
- Suruliz K
- Susinno G
- Sutton MR
- Suzuki Y
- Suzuki Y
- Svatos M
- Swedish S
- Sykora I
- Sykora T
- Ta D
- Tackmann K
- Taffard A
- Tafirout R
- Taiblum N
- Takahashi Y
- Takai H
- Takashima R
- Takeda H
- Takeshita T
- Takubo Y
- Talby M
- Talyshev A
- Tamsett MC
- Tan KG
- Tanaka J
- Tanaka R
- Tanaka S
- Tanaka S
- Tanasijczuk AJ
- Tani K
- Tannoury N
- Tapprogge S
- Tardif D
- Tarem S
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- Tartarelli GF
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- Temming KK
- Ten Kate H
- Teng PK
- Terada S
- Terashi K
- Terron J
- Testa M
- Teuscher RJ
- Therhaag JJ
- Theveneaux-Pelzer T
- Thoma S
- Thomas JP
- Thompson AS
- Thompson EN
- Thompson PD
- Thompson PD
- Thomsen LA
- Thomson E
- Thomson M
- Thong WM
- Thun RP
- Tian F
- Tibbetts MJ
- Tic T
- Tikhomirov VO
- Tikhonov YA
- Timoshenko S
- Tiouchichine E
- Tipton P
- Tisserant S
- Todorov T
- Todorova-Nova S
- Toggerson B
- Tojo J
- Tokar S
- Tokushuku K
- Tollefson K
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- Trigger IM
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- Tripiana MF
- Triplett N
- Trischuk W
- Trocme B
- Troncon C
- Trottier-McDonald M
- True P
- Trzebinski M
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- Tsarouchas C
- Tseng JC-L
- Tsiakiris M
- Tsiareshka P
- Tsionou D
- Tsipolitis G
- Tsiskaridze S
- Tsiskaridze V
- Tskhadadze EG
- Tsukerman II
- Tsulaia V
- Tsung J-W
- Tsuno S
- Tsybychev D
- Tua A
- Tudorache A
- Tudorache V
- Tuggle JM
- Tuna AN
- Turala M
- Turecek D
- Turlay E
- Turra R
- Tuts PM
- Tykhonov A
- Tylmad M
- Tyndel M
- Tzanakos G
- Uchida K
- Ueda I
- Ueno R
- Ugland M
- Uhlenbrock M
- Uhrmacher M
- Ukegawa F
- Unal G
- Undrus A
- Unel G
- Unno Y
- Urbaniec D
- Urquijo P
- Usai G
- Uslenghi M
- Vacavant L
- Vacek V
- Vachon B
- Vague FV
- Vahsen S
- Valenta J
- Valentinetti S
- Valero A
- Valkar S
- Valladolid Gallego E
- Vallecorsa S
- Valls Ferrer JA
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- Van der Deijl PC
- van der Geer R
- van der Graaf H
- van der Leeuw R
- van der Poe E
- van der Ster D
- van Eldik N
- van Gemmeren P
- van Huysduynen LH
- van Vulpen I
- Vanadia M
- Vandelli W
- Vaniachine A
- Vankov P
- Vannucci F
- Vari R
- Varnes EW
- Varol T
- Varouchas D
- Vartapetian A
- Varvell KE
- Vassilakopoulos VI
- Vazeille F
- Vazquez JGP
- Vegni G
- Veillet JI
- Veloso F
- Veness R
- Veneziano S
- Ventura A
- Ventura D
- Venturi M
- Venturi N
- Vercesi V
- Verducci M
- Verkerke W
- Vermeulen JC
- Vest A
- Vetterli MC
- Vichou I
- Vickey T
- Viehhauser GHA
- Viel S
- Villa M
- Villaplana Perez M
- Vilucchi E
- Vincter MG
- Vinek E
- Vinogradov VB
- Virchaux M
- Virzi J
- Vitells O
- Viti M
- Vivarelli I
- Vlachos S
- Vladoiu D
- Vlasak M
- Vogel A
- Vokac P
- Volpi G
- Volpi M
- Volpini G
- von der Schmitt H
- von Radziewski H
- von Toerne E
- Vorobel V
- Vorwerk V
- Vos M
- Voss R
- Voss TT
- Vossebeld JH
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wahlen H
- Wahrmund S
- Wakabayashi J
- Walch S
- Walder J
- Walker R
- Walkowiak W
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- Waller P
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- Wang C
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- Wang J
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- Wang R
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- Wang T
- Warburton A
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- Wardrope DR
- Warsinsky M
- Washbrook A
- Wasicki C
- Watanabe I
- Watkins PM
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- Watson IJ
- Watson MF
- Watts G
- Watts S
- Waugh AT
- Waugh BM
- Weber MS
- Webster JS
- Weidberg AR
- Weigell P
- Weingarten J
- Weiser C
- Wells PS
- Wemans ADV
- Wenaus T
- Wendland D
- Wengler T
- Wengu Z
- Wenig S
- Wermes N
- Werner M
- Werner P
- Werth M
- Wessels M
- Wetter J
- Weydert C
- Whalen K
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- White S
- Whitehead SR
- Whiteson D
- Whittington D
- Wicek F
- Wicke D
- Wickens FJ
- Wiedenmann W
- Wielers M
- Wienemann P
- Wiglesworth C
- Wiik-Fuchs LAM
- Wijeratne PA
- Wildauer A
- Wildt MA
- Wilhelm I
- Wilkens HG
- Will JZ
- Williams E
- Williams HH
- Willis W
- Willocoq S
- Wilson A
- Wilson JA
- Wilson MG
- Wingerter-Seez I
- Winkelmann S
- Winklmeier F
- Wittgen M
- Wollstadt SJ
- Wolter MW
- Wolters H
- Wong WC
- Wooden G
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wozniak KW
- Wraight K
- Wright M
- Wrona B
- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wynne BM
- Xella S
- Xiao M
- Xie S
- Xu C
- Xu D
- Xu L
- Yabsley B
- Yacoob S
- Yagci KD
- Yamada M
- Yamaguchi H
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yao Y
- Yasu Y
- Ye J
- Ye S
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
- Yu DR
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang H
- Zhang J
- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 01/01/2012
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral Z′ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/γ bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fb−1 in the e + e − channel and 5.0 fb−1 in the μ + μ −channel. A Z ′ boson with Standard Model-like couplings is excluded at 95 % confidence level for masses below 2.22 TeV. A Randall-Sundrum graviton with coupling k/MPl=0.1 is excluded at 95 % confidence level for masses below 2.16 TeV. Limits on the other models are also presented, including Technicolor and Minimal Z′ Models
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
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- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
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- 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
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
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
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- Zarzhitsky P
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- Zhemchugov A
- Zheng S
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- Zhuravlov V
- Zieminska D
- Zimmermann R
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- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
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- Zwalinski L
- 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
Search for the neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
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- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or τ lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, φ, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan β in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
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