692 research outputs found
Higgs production in CP-violating supersymmetric cascade decays: probing the `open hole' at the Large Hadron Collider
- Author
- A Bartl
- A Datta
- A Datta
- A Pilaftsis
- A Pilaftsis
- A Pilaftsis
- A Pilaftsis
- A Roeck De
- AC Fowler
- D Chang
- DA Demir
- DA Demir
- DK Ghosh
- DK Ghosh
- E Accomando
- F Deppisch
- FF Deppisch
- G Abbiendi
- G Weiglein
- GD Kribs
- GD Kribs
- GL Kane
- HL Lai
- J Pumplin
- JR Ellis
- JR Ellis
- JS Lee
- JS Lee
- JS Lee
- KE Williams
- M Brhlik
- M Frank
- ML Mangano
- MS Carena
- MS Carena
- O Kittel
- P Bandyopadhyay
- P Bandyopadhyay
- P Bandyopadhyay
- P Draper
- P Nath
- Priyotosh Bandyopadhyay
- PZ Skands
- R Barate
- S Abel
- S Heinemeyer
- S Pokorski
- S Schael
- SP Das
- SP Das
- SW Ham
- SW Ham
- SY Choi
- SY Choi
- SY Choi
- T Falk
- T Hahn
- T Ibrahim
- T Ibrahim
- T Ibrahim
- U Chattopadhyay
- Y Kizukuri
- Z Li
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 09/12/2011
- Field of study
A benchmark CP-violating supersymmetric scenario (known as 'CPX-scenario' in
the literature) is studied in the context of the Large Hadron Collider (LHC).
It is shown that the LHC, with low to moderate accumulated luminosity, will be
able to probe the existing `hole' in the mh1ââ-tanÎČ plane, which
cannot be ruled out by the LEP data. We explore the parameter space with
cascade decay of third generation squarks and gluino with CP-violating decay
branching fractions. We propose a multi-channel analysis to probe this
parameter space some of which are background free at an integrated luminosity
of 5-10 fbâ1. Specially, multi-lepton final states (3\l,\, 4\l and like
sign di-lepton) are almost background free and have 5Ï reach for the
corresponding signals with very early data of LHC for both 14 TeV and 7 TeV
center of mass energy.Comment: 24 pages, 9 figures, references added as in the journal versio
Balanced Schnyder woods for planar triangulations: an experimental study with applications to graph drawing and graph separators
- Author
- Publication venue
- Publication date
- 19/08/2019
- Field of study
In this work we consider balanced Schnyder woods for planar graphs, which are
Schnyder woods where the number of incoming edges of each color at each vertex
is balanced as much as possible. We provide a simple linear-time heuristic
leading to obtain well balanced Schnyder woods in practice. As test
applications we consider two important algorithmic problems: the computation of
Schnyder drawings and of small cycle separators. While not being able to
provide theoretical guarantees, our experimental results (on a wide collection
of planar graphs) suggest that the use of balanced Schnyder woods leads to an
improvement of the quality of the layout of Schnyder drawings, and provides an
efficient tool for computing short and balanced cycle separators.Comment: Appears in the Proceedings of the 27th International Symposium on
Graph Drawing and Network Visualization (GD 2019
Discovery of mating in the major African livestock pathogen Trypanosoma congolense
- Author
- A MacLeod
- A MacLeod
- A Tait
- A Tait
- A Tait
- AC Hoare
- AL Hughes
- Alana Black
- Alison Tweedie
- AM Schurko
- Andreas Schoenefeld
- Andy Tait
- Annette MacLeod
- B Haubold
- C. Michael R. Turner
- Christiane Hertz-Fowler
- CJ Young
- D Faye
- DK Masiga
- DL Hartl
- DR Page
- F Balloux
- FG Razakandrainibe
- G Benson
- G Evanno
- Gina L. Pinchbeck
- GL Pinchbeck
- J Maynard Smith
- J Sternberg
- JK Gashumba
- JK Pritchard
- JR Stevens
- JR Stevens
- K Lewicka
- Laurent RĂ©nia
- Liam J. Morrison
- LJ Morrison
- LJ Morrison
- LJ Morrison
- M Hope
- M Koffi
- M Raymond
- M Tibayrenc
- M Tibayrenc
- M Tibayrenc
- MA Ramesh
- MW Gaunt
- NM El-Sayed
- P Stenberg
- PH Holmes
- PMA Shaw
- R Peakall
- Robert M. Christley
- S Geerts
- T de Meeus
- T Mzilahowa
- TJ Anderson
- V Jamonneau
- W Gibson
- W Gibson
- W Gibson
- W Gibson
- W Weir
- WP Hedrick
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/01/2009
- Field of study
The protozoan parasite, Trypanosoma congolense, is one of the most economically important pathogens of livestock in Africa and, through its impact on cattle health and productivity, has a significant effect on human health and well being. Despite the importance of this parasite our knowledge of some of the fundamental biological processes is limited. For example, it is unknown whether mating takes place. In this paper we have taken a population genetics based approach to address this question. The availability of genome sequence of the parasite allowed us to identify polymorphic microsatellite markers, which were used to genotype T. congolense isolates from livestock in a discrete geographical area of The Gambia. The data showed a high level of diversity with a large number of distinct genotypes, but a deficit in heterozygotes. Further analysis identified cryptic genetic subdivision into four sub-populations. In one of these, parasite genotypic diversity could only be explained by the occurrence of frequent mating in T. congolense. These data are completely inconsistent with previous suggestions that the parasite expands asexually in the absence of mating. The discovery of mating in this species of trypanosome has significant consequences for the spread of critical traits, such as drug resistance, as well as for fundamental aspects of the biology and epidemiology of this neglected but economically important pathogen
Important ectoparasites of Alpaca (Vicugna pacos)
- Author
- A Foster
- AC Cicchino
- CF Curtis
- E Hoffman
- FHM Borgsteede
- G Leguia
- GL DÂŽAlteiro
- GL DÂŽAlteiro
- HI Burri
- HJWM Cremers
- J Alvarado
- J Neveu-Lemaire
- JD Plant
- JL Vaughan
- JL Vaughan
- K Mellanby
- M Petrikowski
- MA Aba
- ME Fowler
- NM Nayel
- NM Nayel
- NM Nayel
- NW Frame
- P Bates
- P Bates
- P Cui
- P Lau
- RAW Rosychuk
- RL Palma
- RP Hunter
- RP Hunter
- S Bornstein
- SA Tait
- Set Bornstein
- T Geurden
- Publication venue
- BioMed Central
- Publication date
- 01/01/2010
- Field of study
High Natality Rates of Endangered Steller Sea Lions in Kenai Fjords, Alaska and Perceptions of Population Status in the Gulf of Alaska
- Author
- AE York
- Alan M. Springer
- AM Doroff
- AM Springer
- AM Springer
- AW Trites
- C Brownie
- CC Kaplan
- CM Hurvich
- CP Donnelly
- D DeMaster
- DAS Rosen
- DG Calkins
- DP Costa
- EE Holmes
- EE Holmes
- G Beauplet
- G Bell
- GL Hadley
- H Akaike
- IL Boyd
- IL Boyd
- J McKenzie
- JD Nichols
- JL Sease
- JM Maniscalco
- JM Maniscalco
- John M. Maniscalco
- JW Testa
- KA Burek
- KL Mashburn
- KL Raum-Suryan
- KW Pitcher
- KW Pitcher
- KW Pitcher
- LD Rea
- LL Eberhardt
- LL Milette
- LW Fritz
- LW Fritz
- LW Fritz
- M Horning
- MD Berman
- MJ Myers
- NJ Lunn
- OA Mathisen
- Pamela Parker
- PJ Anderson
- R Choquet
- R Dalton
- RL Merrick
- S Atkinson
- S Creel
- S Hamel
- SL Fowler
- SL Fowler
- SR Hare
- W Dabin
- WR Hood
- Yan Ropert-Coudert
- Publication venue
- Public Library of Science
- Publication date
- 08/04/2010
- Field of study
Steller sea lions experienced a dramatic population collapse of more than 80% in the late 1970s through the 1990s across their western range in Alaska. One of several competing hypotheses about the cause holds that reduced female reproductive rates (natality) substantively contributed to the decline and continue to limit recovery in the Gulf of Alaska despite the fact that there have been very few attempts to directly measure natality in this species. We conducted a longitudinal study of natality among individual Steller sea lions (nâ=â151) at a rookery and nearby haulouts in Kenai Fjords, Gulf of Alaska during 2003â2009. Multi-state models were built and tested in Program MARK to estimate survival, resighting, and state transition probabilities dependent on whether or not a female gave birth in the previous year. The models that most closely fit the data suggested that females which gave birth had a higher probability of surviving and giving birth in the following year compared to females that did not give birth, indicating some females are more fit than others. Natality, estimated at 69%, was similar to natality for Steller sea lions in the Gulf of Alaska prior to their decline (67%) and much greater than the published estimate for the 2000s (43%) which was hypothesized from an inferential population dynamic model. Reasons for the disparity are discussed, and could be resolved by additional longitudinal estimates of natality at this and other rookeries over changing ocean climate regimes. Such estimates would provide an appropriate assessment of a key parameter of population dynamics in this endangered species which has heretofore been lacking. Without support for depressed natality as the explanation for a lack of recovery of Steller sea lions in the Gulf of Alaska, alternative hypotheses must be more seriously considered
Changes in magnetic resonance mammography due to hormone replacement therapy
- Author
- A Ozdemir
- A Rieber
- Ansgar Malich
- B Martin
- Christiane Marx
- CK Kuhl
- CM Vachon
- DA Grimes
- Dieter Sauner
- DV Spicer
- E Banks
- GL Ottesen
- H Neubauer
- I Persson
- JA Harvey
- JC Litherland
- JR Daling
- JR Reichenbach
- JS Taylor
- JW Rich-Edwards
- L Bogin
- M Gibaldi
- M MĂŒller-Schimpfle
- M Stampfer
- MC Pike
- PA Fowler
- R Lindsay
- RC Marugg
- SH Heywang-Köbrunner
- SJ Graham
- Stefan OR Pfleiderer
- Steffen Sachse
- Susanne Wurdinger
- TR Nelson
- U Germer
- WA Kaiser
- Werner A Kaiser
- Z Hussain
- Publication venue
- BioMed Central
- Publication date
- 16/03/2004
- Field of study
BACKGROUND: The aim of the present article is to investigate effects of hormone replacement therapy (HRT) on contrast medium enhancement patterns in postmenopausal patients during magnetic resonance mammography (MRM). MATERIALS AND METHODS: Two hundred and fifteen patients receiving hormonal medication were divided into four groups: 150 patients with 1 MRM during HRT (group A), 13 patients with 2 MRMs under HRT (group B), 30 patients with 1 MRM during HRT and 1 MRM after HRT withdrawal (group C), and 22 women with 1 MRM after HRT withdrawal (group D). Dynamic MRM was performed at 1.5 Tesla. Signal intensity changes were characterized by five time curves: minimal enhancement (type I), weak continuous enhancement (type II), strong continuous enhancement (type III), and a steep initial slope followed by a plateau phenomenon (type IV) or a washout effect (type V). RESULTS: Of all 193 patients under HRT (group A + group B + group C), 60 patients (31.1%) showed curve type I, 88 patients (45.6%) showed type II and 45 patients (23.3%) showed type III. There were significant differences to 52 patients after HRT withdrawal (group C + group D) (P < 0.0001), with 42 patients (80.8%) for curve type I, 8 patients (15.4%) for type II, and 2 patients (3.8%) for type III. In both MRM sessions in group B, 69% of the patients showed identical curve types without significant differences (P = 0.375). In group C, 28 of 30 patients (93%) dropped to lower curve types with significant differences in curve types during and after HRT (P < 0.0001). CONCLUSION: The majority of patients receiving postmenopausal HRT showed bilateral symmetrical, continuous enhancement without evidence of a plateau phenomenon or a washout effect due to HRT in MRM. Hormonal effects could be proven and were reproducible and reversible
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
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asner D
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Bachy G
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker MD
- Baker OK
- Baker S
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barashkou A
- 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 F
- Barrera CO
- Barrillon P
- Bartoldus R
- Barton AE
- Bartsch D
- Bartsch V
- Bates RL
- Batkova L
- Batley JR
- Battaglia A
- Battistin M
- Battistoni G
- Bauer F
- Bawa HS
- Beare B
- Beau T
- Beauchemin PH
- Beccherle R
- Bechtle P
- Beck GA
- Beck HP
- Beckingham M
- Becks KH
- Beddall A
- Beddall AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Begel M
- Behera PK
- Beimforde M
- Belanger-Champagne C
- Belenguer MJ
- Bell PJ
- Bell WH
- Bella G
- Bella LA
- Bellagamba L
- Bellina F
- Bellomo M
- Belloni A
- Beloborodova O
- Belotskiy K
- Beltramello O
- Ben Ami S
- Benary O
- Benchekroun D
- Benchouk C
- Bendel M
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Beretta M
- Berge D
- Berger N
- Berghaus F
- Berglund E
- Beringer J
- Bernardet K
- Bernat P
- Bernhard R
- Bernius C
- Berry T
- Bertin A
- Bertinelli F
- Bertolucci F
- Besana MI
- Besson N
- Bethke S
- Bhimji W
- Bianchi RM
- Bianco M
- Biebel O
- Bieniek SP
- Bierwagen K
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
- Bingul A
- Bini C
- Biscarat C
- Bitenc U
- Black KM
- Blair RE
- Blanchard J-B
- Blanchot G
- Blazek T
- Blocker C
- Blocki J
- Blondel A
- Blum W
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VB
- Bocchetta SS
- Bocci A
- Boddy CR
- Boehler M
- Boek J
- Boelaert N
- Boeriu OEV
- Boeser S
- Bogaerts JA
- Bogdanchikov A
- Bogouch A
- Bohm C
- Boisvert V
- Bold T
- Boldea V
- Bolnet NM
- Bona M
- Bondarenko VG
- Bondioli M
- Boonekamp M
- Boorman G
- Booth CN
- Bordoni S
- Borer C
- Borisov A
- Borissov G
- Borjanovic I
- Borroni S
- Bos K
- Boscherini D
- Bosman M
- Boterenbrood H
- Botterill D
- Bouchami J
- Boudreau J
- Bouhova-Thacker EV
- Bourdarios C
- Bousson N
- Boveia A
- Boyd J
- Boyko IR
- Bozhko NI
- Bozovic-Jelisavcic I
- Bracinik J
- Braem A
- Branchini P
- Brandenburg GW
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Brelier B
- Bremer J
- Brenner R
- Bressler S
- Breton D
- Britton D
- Brochu FM
- Brock I
- Brock R
- Brodbeck TJ
- Brodet E
- Broggi F
- Bromberg C
- Brooijmans G
- Brooks WK
- Brown G
- Brown H
- Bruncko D
- Bruneliere R
- Brunet S
- Bruni A
- Bruni G
- Bruschi M
- BScher V
- Buanes T
- Bucci F
- Buchanan J
- Buchanan NJ
- Buchholz P
- Buckingham RM
- Buckley AG
- Buda SI
- Budagov IA
- Budick B
- Bueso XP
- Bugge L
- Buira-Clark D
- Bulekov O
- Bunse M
- Buran T
- Burckhart H
- Burdin S
- Burgess T
- Burke S
- Busato E
- Bussey P
- Buszello CP
- Butin F
- Butler B
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Caballero J
- Caforio D
- Cakir IT
- Cakir O
- Calafiura P
- Calderini G
- Calfayan P
- Calkins R
- Caloba LP
- Caloi R
- Calvet D
- Calvet S
- Camarri P
- Cambiaghi M
- Cameron D
- Camilocci ES
- Campana S
- Campanelli M
- Canale V
- Canelli F
- Canepaa A
- Cantero J
- Capasso L
- Caprini I
- Caprini M
- Capriotti D
- Capua M
- Caputo R
- Caramarcu C
- Cardarelli R
- Carli T
- Carlino G
- Carminati L
- Caron B
- Caron S
- Carter AA
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Cascella M
- Caso C
- Castaneda-Miranda E
- Castanheira MTD
- Castillo LRF
- Castro NF
- Cataldi G
- Cataneo F
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- Cauz D
- Cavalcanti TP
- Cavalleri P
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Ceradini F
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cetin SA
- Cevenini F
- Chafaq A
- Chakraborty D
- Chan K
- Chapleau B
- Chapman JD
- Chapman JW
- Chareyre E
- Charlton DG
- Chavda V
- Cheatham S
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen S
- Chen T
- Chen X
- Cheng S
- Cheong ALF
- Cheplakov A
- Chepurnov VF
- Chernyatin V
- Cheu E
- Cheung SL
- Chevalier L
- Chiefari G
- Chikovani L
- Childers JT
- Chilingarov A
- Chiodini G
- Chizhov MV
- Choudalakis G
- Chouridou S
- Christidi IA
- Christov A
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Ciapetti G
- Ciba K
- Ciftci AK
- Ciftci R
- Cinca D
- Cindro V
- Ciobotaru MD
- Cioccaa C
- Ciocio A
- Cirilli M
- Citterio M
- Ciubancan M
- Clark A
- Clark PJ
- Cleland W
- Clemens JC
- Clement B
- Clement C
- Clifft RW
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Codina EP
- Coe P
- Cogan JG
- Coggeshall J
- Cogneras E
- Cojocaru CD
- Colas J
- Colijn AP
- Collaboration ATLAS
- Collard C
- Collins NJ
- Collins-Tooth C
- Collot J
- Colon G
- Coniavitis E
- Conidi MC
- Consonni M
- Consorti V
- Constantinescu S
- Conta C
- Conventi F
- Cook J
- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Copic K
- Cornelissen T
- Corradi M
- Correia AMH
- Corriveau F
- Corso-Radu A
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Costin T
- Cote D
- Courneyea L
- Cowan G
- Cowden C
- Cox BE
- Cranmer K
- Cranshaw J
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Crosetti G
- Crupi R
- Cuciuc C-M
- Curatolo M
- Curtis CJ
- Curull XE
- Cwetanski P
- Czirr H
- Czyczula Z
- D'Auria S
- D'Onofrio M
- D'Orazio A
- Da Costa JBG
- Da Costa JGPF
- Da Silva PVM
- Da Via C
- Dabrowski W
- Dai T
- Dallapiccola C
- Daly CH
- Dam M
- Damazio DO
- Dameri M
- Damiani DS
- Danielsson HO
- Dannheim D
- Dao V
- Darbo G
- Darlea GL
- Daum C
- Dauvergne JP
- Davey W
- Davidek T
- Davidson N
- Davidson R
- Davies E
- Davies M
- Davison AR
- Davygora Y
- Dawe E
- Dawson I
- Dawson JW
- Daya-Ishmukhametova RK
- de Asmundis R
- De Castro S
- De Cecco S
- De Graat J
- De Groot N
- De Jong P
- De la Hoz SG
- De la Taille C
- De la Torre H
- De Lima JGR
- De Lotto B
- De Mora L
- De Nooij L
- De Pedis D
- De Regie JBDV
- De Renstrom PAB
- De Salvo A
- De Sanctis U
- De Santo A
- De K
- Dean S
- Debbe R
- Dedovich DV
- Degenhardt J
- Dehchar M
- Del Papa C
- Del Peso J
- Del Prete T
- Deliyergiyev M
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- Della Porta GZ
- della Volpe D
- Delmastro M
- Delpierre P
- Delruelle N
- Delsart PA
- Deluca C
- Demers S
- Demichev M
- Demirkoz B
- Deng J
- Deng W
- Denis RDS
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Devetak E
- Deviveiros PO
- Dewhurst A
- DeWilde B
- Dhaliwal S
- Dhullipudi R
- Di Ciaccio A
- Di Ciaccio L
- Di Girolamo A
- Di Girolamo B
- Di Luise S
- Di Mattia A
- Di Micco B
- Di Nardo R
- Di Simone A
- Di Sipio R
- Diaz MA
- Diblen F
- Diehl EB
- Dietrich J
- Dietzscha TA
- Diglio S
- Dingfelder J
- Dionisi C
- Dita P
- Dita S
- Dittus F
- Djama F
- Djobava T
- do Vale MAB
- Do ValleWemans A
- Doan TKO
- Dobbs M
- Dobinson R
- Dobos D
- Dobson E
- Dobson M
- Dodd J
- Doglioni C
- Doherty T
- Dohmae T
- Doi Y
- Dolejsi J
- Dolenc I
- Dolezal Z
- Dolgoshein BA
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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 âs = 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 pTâ„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 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{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
- Author
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- Abdallah J
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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
Observation of associated near-side and away-side long-range correlations in âsNN=5.02ââTeV 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
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- Abreu H
- Acharya BS
- Adamczyk L
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- Addy TN
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- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahles F
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- 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
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- Aliev M
- Alimonti G
- Alison J
- Allbrooke BM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
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- Alonso A
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- Alvarez Gonzalez B
- Alviggi MG
- Amako K
- Amelung C
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- Amor Dos Santos SP
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- Yamamura T
- Yamanaka T
- Yamauchi K
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yen AL
- 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
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- ZeniĆĄ T
- Zerwas D
- Zevi Della Porta G
- Zhang D
- Zhang H
- Zhang J
- Zhang L
- 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
- ZivkoviÄ 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 (ÎÏ) and pseudorapidity (Îη) are measured in âsNN=5.02ââTeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1ââÎŒb-1 of data as a function of transverse momentum (pT) and the transverse energy (ÎŁETPb) 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<|Îη|<5) ânear-sideâ (ÎÏâŒ0) correlation that grows rapidly with increasing ÎŁETPb. A long-range âaway-sideâ (ÎÏâŒÏ) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ÎŁETPb, is found to match the near-side correlation in magnitude, shape (in Îη and ÎÏ) and ÎŁETPb dependence. The resultant ÎÏ correlation is approximately symmetric about Ï/2, and is consistent with a dominant cosâĄ2ÎÏ modulation for all ÎŁETPb 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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- Abajyan T
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- Abdallah J
- Khalek SA
- Abdelalim AA
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- Yamaguchi H
- Yamamoto A
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- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamazaki T
- Yamazaki Y
- Yan Z
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- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yao Y
- Yasu Y
- Smit GVY
- Ye J
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- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
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- 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
- Zinonos Z
- Zerwas D
- della Porta GZ
- Zhang D
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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
- 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 fbâ1 of sâ=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 ÎČ < 40
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