501 research outputs found
Developing a digital intervention for cancer survivors: an evidence-, theory- and person-based approach
- Author
- A OâCathain
- AC Marcus
- AC Tricco
- AC Wootten
- AC Wootten
- Adam WA Geraghty
- AJ Mitchell
- AP Kassianos
- AS Anderson
- B Thewes
- B Thewes
- C Charlier
- C Schwedhelm
- C Taylor
- CE Short
- CF Sharpley
- CK McMullen
- CM Ruland
- CR Green
- CR May
- DC Snyder
- E McCaughan
- E McCaughan
- E Staples
- EE Pauwels
- G Prue
- GT Deimling
- H Arksey
- H Baumeister
- H McAlpine
- J Brunet
- J Elliott
- J Midtgaard
- Janet Harden
- JE Owen
- JK Vallance
- K Bell
- K Bradbury
- K Bradbury
- K De Cocker
- K Dieperink
- K Erwin
- KM Carpenter
- KS Courneya
- KS Courneya
- KT Ashing-Giwa
- KY Wen
- LF Brown
- LJ Ware
- LKB Eldredge
- M Coleman
- M Duncan
- M LamortâBouchĂ©
- M Ramirez
- M Wallace
- M-L Luoma
- MC Morey
- MM Reeves
- MY Ho
- O Hedestig
- P Craig
- P Little
- R Band
- R Crane-Okada
- R OâBrien
- RA Willems
- Rachel Walker
- S Darlow
- S Hansen
- S Khangura
- S Michie
- S Michie
- S Michie
- S Michie
- S Simard
- SJ Hardcastle
- SK Baxter
- SM Miller
- T Corbett
- T Wilson
- Teresa Corbett
- TL Raque-Bogdan
- Y Hong
- YH Yun
- Z Chen
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 02/09/2019
- Field of study
This paper illustrates a rigorous approach to developing digital interventions using an evidence-, theory- and person-based approach. Intervention planning included a rapid scoping review which identified cancer survivorsâ needs, including barriers and facilitators to intervention success. Review evidence (N=49 papers) informed the interventionâs Guiding Principles, theory-based behavioural analysis and logic model. The intervention was optimised based on feedback on a prototype intervention through interviews (N=96) with cancer survivors and focus groups with NHS staff and cancer charity workers (N=31). Interviews with cancer survivors highlighted barriers to engagement, such as concerns about physical activity worsening fatigue. Focus groups highlighted concerns about support appointment length and how to support distressed participants. Feedback informed intervention modifications, to maximise acceptability, feasibility and likelihood of behaviour change. Our systematic method for understanding user views enabled us to anticipate and address important barriers to engagement. This methodology may be useful to others developing digital interventions
Turbulence and galactic structure
- Author
- A Immeli
- A Immeli
- A Shukurov
- AMN Ferguson
- AN Kolmogorov
- B Robertson
- BG Elmegreen
- BG Elmegreen
- BG Elmegreen
- BG Elmegreen
- BG Elmegreen
- C Heiles
- CA Norman
- CD Matzner
- CF Gammie
- CG Hoopes
- D Lynden-Bell
- D Pfenniger
- D Puche
- DL Block
- DM Elmegreen
- DM Elmegreen
- DM Elmegreen
- DNC Lin
- E Vazquez-Semadeni
- EC Ostriker
- F Athanassoula
- F Bournaud
- G Bertin
- G Vaucouleurs
- H Hasan
- H Saio
- H Tran
- I Berentzen
- J Ballesteros-Paredes
- J Cho
- J Cho
- JJ Dalcanton
- JM Dickey
- JM Stone
- JV Feitzinger
- JV Feitzinger
- K Wada
- K Wada
- K Wada
- L Cowie
- L Hartmann
- L Simard
- M Gerin
- M Noguchi
- M Noguchi
- M-M Mac-Low
- M-M Mac-Low
- M-M Mac-Low
- MA Avillez
- MP Schwarz
- MR Bate
- MW Regan
- N Benitez
- OY Gnedin
- P Padoan
- PS Li
- PWJL Brand
- Q Zhang
- R Bouwens
- RC Buta
- RC Kennicutt
- RS Klessen
- S Boldyrev
- S Boldyrev
- S Kim
- S Ravindranath
- S Stanimirovic
- V Reshetnikov
- VP Debattista
- Y Li
- Y Yoshii
- Y Zhou
- YN Efremov
- YN Efremov
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2004
- Field of study
Interstellar turbulence is driven over a wide range of scales by processes
including spiral arm instabilities and supernovae, and it affects the rate and
morphology of star formation, energy dissipation, and angular momentum transfer
in galaxy disks. Star formation is initiated on large scales by gravitational
instabilities which control the overall rate through the long dynamical time
corresponding to the average ISM density. Stars form at much higher densities
than average, however, and at much faster rates locally, so the slow average
rate arises because the fraction of the gas mass that forms stars at any one
time is low, ~10^{-4}. This low fraction is determined by turbulence
compression, and is apparently independent of specific cloud formation
processes which all operate at lower densities. Turbulence compression also
accounts for the formation of most stars in clusters, along with the cluster
mass spectrum, and it gives a hierarchical distribution to the positions of
these clusters and to star-forming regions in general. Turbulent motions appear
to be very fast in irregular galaxies at high redshift, possibly having speeds
equal to several tenths of the rotation speed in view of the morphology of
chain galaxies and their face-on counterparts. The origin of this turbulence is
not evident, but some of it could come from accretion onto the disk. Such high
turbulence could help drive an early epoch of gas inflow through viscous
torques in galaxies where spiral arms and bars are weak. Such evolution may
lead to bulge or bar formation, or to bar re-formation if a previous bar
dissolved. We show evidence that the bar fraction is about constant with
redshift out to z~1, and model the formation and destruction rates of bars
required to achieve this constancy.Comment: in: Penetrating Bars through Masks of Cosmic Dust: The Hubble Tuning
Fork strikes a New Note, Eds., K. Freeman, D. Block, I. Puerari, R. Groess,
Dordrecht: Kluwer, in press (presented at a conference in South Africa, June
7-12, 2004). 19 pgs, 5 figure
Efficacy of bifenthrin-impregnated bednets against Anopheles funestus and pyrethroid-resistant Anopheles gambiae in North Cameroon
- Author
- AN Asidi
- C Fanello
- C Lengeler
- CF Curtis
- CF Curtis
- CG Nevill
- F Chandre
- F Chandre
- F Darriet
- F Darriet
- F Darriet
- F Darriet
- F Darriet
- Fabrice Chandre
- FN Binka
- Frédéric Darriet
- Frédéric Simard
- H Huang
- J Etang
- J Etang
- J Mouchet
- JD Lines
- Jean-Marc Hougard
- JM Hougard
- JM Hougard
- JM Hougard
- Josiane Etang
- K Hargreaves
- M Zaim
- M Zaim
- MC Henry
- Mouhamadou Chouaibou
- MT Gillies
- N Elissa
- P Carnevale
- P Guillet
- PL Alonso
- R N'Guessan
- RBM partnership
- RD McAbee
- U D'Alessandro
- WHO
- WHO
- Publication venue
- BioMed Central
- Publication date
- 01/01/2006
- Field of study
BACKGROUND: Recent field studies indicated that insecticide-treated bednets (ITNs) maintain their efficacy despite a high frequency of the knock-down resistance (kdr) gene in Anopheles gambiae populations. It was essential to evaluate ITNs efficacy in areas with metabolic-based resistance. METHODS: Bifenthrin was used in this experiment because it is considered a promising candidate for bednets impregnation. Nets were treated at 50 mg/m(2), a dose that has high insecticidal activity on kdr mosquitoes and at 5 mg/m(2), a dose that kills 95% of susceptible mosquitoes under laboratory conditions with 3 minutes exposure. Bednets were holed to mimic physical damage. The trial was conducted in three experimental huts from Pitoa, North-Cameroon where Anopheles gambiae displays metabolic resistance and cohabits with An. funestus. RESULTS: Bifenthrin at 50 mg/m(2 )significantly reduced anophelines' entry rate (>80%). This was not observed at 5 mg/m(2). Both treatments increased exophily in An. gambiae, and to a lesser extent in An. funestus. With bifenthrin at high dosage, over 60% reduction in blood feeding and 75â90% mortality rates were observed in both vectors. Despite presence of holes, only a single An. gambiae and two An. funestus females were collected inside the treated net, and all were found dead. The same trends were observed with low dosage bifenthrin though in most cases, no significant difference was found with the untreated control net. CONCLUSION: Bifenthrin-impregnated bednets at 50 mg/m(2 )were efficient in the reduction of human-vector contact in Pitoa. Considerable personal protection was gained against An. funestus and metabolic pyrethroid resistant An. gambiae populations
Genetic Structure of the Tiger Mosquito, Aedes albopictus, in Cameroon (Central Africa)
- Author
- A El Mousadik
- A Zalewski
- AH Hawley
- AJ Cornel
- B Kamgang
- Basile Kamgang
- BS Weir
- C Paupy
- C Paupy
- C Van Oosterhout
- CEG Smith
- CF Ayres
- Christophe Paupy
- CN Peyrefitte
- CY Kow
- CĂ©cile Brengues
- D Fontenille
- D Porreta
- Didier Fontenille
- DJ Gubler
- DJ Gubler
- EJ Scholte
- EM Leroy
- F Ronquist
- F Rousset
- F Simard
- F Tajima
- Flobert Njiokou
- Frédéric Simard
- G Dalla Pozza
- G Evanno
- H Delatte
- HM Savage
- I Morlais
- J Birungi
- J Bonacum
- J Felsenstein
- J Goudet
- J Rozas
- JAA Nylander
- JD Thompson
- JJ Kolbe
- JK Pritchard
- K Belkhir
- K Liu
- L Mousson
- M Nei
- M Nei
- M Raymond
- NG Gratz
- P Reiter
- P Reiter
- Pedro Lagerblad Oliveira
- R Lourenço-de-Oliveira
- RB Tesh
- RDM Page
- RT Maia
- S Holm
- S Kambhampati
- S Mas-Coma
- S Urbanelli
- S Usmani-Brown
- WA Hawley
- YX Fu
- YX Fu
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
Background: Aedes albopictus (Skuse, 1884) (Diptera: Culicidae), a mosquito native to Asia, has recently invaded all five continents. In Central Africa it was first reported in the early 2000s, and has since been implicated in the emergence of arboviruses such as dengue and chikungunya in this region. Recent genetic studies of invasive species have shown that multiple introductions are a key factor for successful expansion in new areas. As a result, phenotypic characters such as vector competence and insecticide susceptibility may vary within invasive pest species, potentially affecting vector efficiency and pest management. Here we assessed the genetic variability and population genetics of Ae. albopictus isolates in Cameroon (Central Africa), thereby deducing their likely geographic origin. Methods and Results: Mosquitoes were sampled in 2007 in 12 localities in southern Cameroon and analyzed for polymorphism at six microsatellite loci and in two mitochondrial DNA regions (ND5 and COI). All the microsatellite markers were successfully amplified and were polymorphic, showing moderate genetic structureamong geographic populations (F-ST = 0.068, P<0.0001). Analysis of mtDNA sequences revealed four haplotypes each for the COI and ND5 genes, with a dominant haplotype shared by all Cameroonian samples. The weak genetic variation estimated from the mtDNA genes is consistent with the recent arrival of Ae. albopictus in Cameroon. Phylogeographic analysis based on COI polymorphism indicated that Ae. albopictus populations from Cameroon are related to tropical rather than temperate or subtropical outgroups. Conclusion: The moderate genetic diversity observed among Cameroonian Ae. albopictus isolates is in keeping with recent introduction and spread in this country. The genetic structure of natural populations points to multiple introductions from tropical regions
Field site selection: getting it right first time around
- Author
- Abdel Hameed Nugud
- Ahmed Babiker
- AT Shousha
- Badria El Sayed
- Bart GJ Knols
- BB El Sayed
- CA Hill
- CF Curtis
- Colin A Malcolm
- CS Lofgren
- DA Dame
- Didier Fontenille
- DJ Lewis
- EF Knipling
- F Simard
- G Davidson
- H Laven
- H Laven
- IAEA
- JC Denys
- KK Grover
- Mark Q Benedict
- MC Thomson
- MJ Donnelly
- MJB Vreysen
- MYH Dukeen
- R Bellini
- R Girod
- R Girod
- R Girod
- RB Hichton
- RJ Stern
- Romain Girod
- RS Patterson
- RS Patterson
- SG Breeland
- SM Asman
- TB Ageep
- United Nations Office for the Coordination of Humanitarian Affairs (OCHA)
- V Lotteau
- V Petrarca
- WK Reisen
- Publication venue
- BioMed Central
- Publication date
- 01/01/2009
- Field of study
The selection of suitable field sites for integrated control of Anopheles mosquitoes using the sterile insect technique (SIT) requires consideration of the full gamut of factors facing most proposed control strategies, but four criteria identify an ideal site: 1) a single malaria vector, 2) an unstructured, relatively low density target population, 3) isolation of the target population and 4) actual or potential malaria incidence. Such a site can exist in a diverse range of situations or can be created. Two contrasting SIT field sites are examined here: the desert-flanked Dongola Reach of the Nile River in Northern State, Sudan, where malaria is endemic, and the island of La Reunion, where autochthonous malaria is rare but risk is persistent. The single malaria-transmitting vector at both sites is Anopheles arabiensis. In Sudan, the target area is a narrow 500 km corridor stretching from the rocky terrain at the Fourth Cataract - just above the new Merowe Dam, to the northernmost edge of the species range, close to Egypt. Vector distribution and temporal changes in density depend on the Nile level, ambient temperature and human activities. On La Reunion, the An. arabiensis population is coastal, limited and divided into three areas by altitude and exposure to the trade winds on the east coast. Mosquito vectors for other diseases are an issue at both sites, but of primary importance on La Reunion due to the recent chikungunya epidemic. The similarities and differences between these two sites in terms of suitability are discussed in the context of area-wide integrated vector management incorporating the SIT
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
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adragna P
- Adye T
- Aesky S
- Agar-Savedra JA
- Agustoni M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- 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 BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- 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
- Andrieux M-L
- Anduaga XS
- Angelidakis S
- Anger P
- Angerami A
- Anghinolfi F
- Anh TV
- Anisenkov A
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Arfaoui S
- Arguin J-F
- 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
- Astbury A
- Atkinson M
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Avolio G
- Axen A
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
- Baker S
- Balek P
- 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 N
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Barojas CAC
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- 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
- Begel M
- Behera PK
- Beimforde N
- Belanger-Champagne C
- Belenguer AJ
- Bell PJ
- Bell WH
- Bella G
- Bella LA
- Bellagamba L
- Bellomo M
- Belloni A
- Beloborodova O
- Belotskiy K
- Beltramello O
- Benary O
- Benchekroun D
- Bendtz K
- Benekos N
- Benhammou Y
- Benjarnin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Berge D
- Berger N
- Berghaus F
- Berglund E
- Beringer J
- Berlingen JM
- Bernat P
- Bernhard R
- Bernius C
- 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
- Bioelaert N
- Biscarat C
- Bittner B
- Black CW
- Black KM
- Blair RE
- Blanchard J-B
- 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
- Boeriu OEV
- 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
- Boveia A
- Boyd J
- Boyko IR
- Bozovic-Jelisavcic I
- Bracinik J
- Branchini P
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Brazzale SF
- Brelier B
- Bremer J
- Brendlinger K
- Brenner R
- Bressler S
- Bristow TM
- Britton D
- Brochu FM
- Brock I
- Brock R
- Broggi F
- Bromberg C
- Bronner J
- Brooijmans G
- Brooks T
- Brooks WK
- Brown G
- Bruncko D
- Bruneliere R
- Brunet S
- Bruni A
- Bruni G
- Bruschi M
- Bryngemark L
- Buanes T
- Buat Q
- Bucci F
- Buchanan J
- Buchholz P
- Buckingham RM
- Buckley AG
- Buda SI
- Budagov IA
- Budick B
- Buescher V
- Bueso XP
- Bugge L
- Bulekov O
- Bundock AC
- Bunse M
- Buran T
- Burckhart H
- Burdin S
- Burgess T
- Burke S
- Busato E
- Bussey P
- Bustos ACF
- Buszello CP
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- Butler JM
- Buttar CM
- Butterworth JM
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- Cabrera Urban S
- Cadfort T
- Caforio D
- Cakir IT
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- Calafiura P
- Calderini G
- Calfayan P
- Calkins R
- Caloba LP
- Caloi H
- Calvet D
- Calvet S
- Camarri P
- Cameron D
- Camillocci ES
- Caminada LM
- Caminal Armadans R
- Campana S
- Campanelli M
- Canale V
- Canelli F
- Canepa A
- Cantero J
- Cantrill R
- Caprini I
- Caprini M
- Capriotti D
- Capua M
- Caputo R
- Cardarelli R
- Carli T
- Carlino G
- Carminati L
- Caron S
- Carquin E
- Carrillo-Montoya GD
- Carter AA
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Cascella M
- Caso C
- Castaneda-Miranda E
- Castanheira MTD
- Castillo Gimenez V
- Castillo IS
- Castillo LRF
- Castro NF
- Cataldi C
- Catastini P
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani C
- Caughron S
- Cavalcanti TP
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- Cavalli-Sforza M
- Cavsinni V
- Ceradini F
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cetin SA
- Chafaq A
- Chakraborty D
- Chalupkova I
- Chan K
- Chang P
- Chapleau B
- Chapman JD
- Chapman JW
- Charlton DG
- Chavda V
- Cheatham S
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen S
- Chen X
- Chen Y
- Cheng Y
- Cheplakov A
- Chernyatin V
- Cheu E
- Cheung SL
- Chevalier L
- Chiefari C
- Chikovani L
- Childers JT
- Chilingarov A
- Chiodini C
- Chisholm AS
- Chislett RT
- Chitan A
- Chizhov MV
- Choudalakis G
- Chouridou S
- Christidi IA
- Christov A
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Ciapetti G
- Ciftci AK
- Ciftci R
- Cinca D
- Cindro V
- Ciocio A
- Cirilli N
- Cirkovic P
- Citron ZH
- Citterio M
- Ciubancan M
- Clark A
- Clark PJ
- Clarke RN
- Cleland W
- Clemens JC
- Clement B
- Clement C
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Codina EP
- Coffey L
- Cogan JG
- Coggeshall J
- Colas J
- Cole S
- Colijn AP
- Collaboration ATLAS
- Collins NJ
- Collins-Tooth C
- Collot J
- Colombo T
- Colon G
- Compostella G
- Conde Muino P
- Coniavitis E
- Conidi MC
- Consonni SM
- Consorti V
- Constantinescu S
- Conta C
- Conti G
- Conventi F
- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Copic K
- Cornelissen F
- Corradi M
- Correia AMH
- Corriveau F
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Cote D
- Courneyea L
- Cowan G
- Cox BE
- Cranmer K
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Crosetti G
- Cuciuc C-M
- Cummings J
- Curatolo M
- Curtis CJ
- Cuthbert C
- Cwetanski P
- Czirr H
- Czodrowski P
- Czyezula Z
- D'Auria S
- D'Onofrio M
- D'Orazio A
- da Costa JBG
- Da Costa JGPF
- Da Cunha Sargedas De Sousa MJ
- Da Via C
- Dabrowski V
- Dafinca A
- Dai T
- Dallaire F
- Dallapiccola C
- Dam M
- Damazio DO
- Dameri M
- Damiani DS
- Danielsson HO
- Dao V
- Darbo G
- Darlea GL
- Dassoulas JA
- Davey W
- Davidek T
- Davidson N
- Davidson R
- Davies E
- Davies M
- Davignon O
- Davison AR
- Davygora Y
- Dawe E
- Dawson I
- Daya-Ishmukhametova RK
- de Asmundis R
- De Castro S
- De Cecco S
- de Graat J
- De Groot N
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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 Ï 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, Ï, 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 ÎČ in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
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
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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
Observation of associated near-side and away-side long-range correlations in âsNN=5.02ââTeV proton-lead collisions with the ATLAS detector
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- Yang UK
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- Yanush S
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- Yen AL
- Yilmaz M
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- Yorita K
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- Yoshihara K
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- Young CJ
- Youssef S
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- 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
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Khalek SA
- 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
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MS
- 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 BMM
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Gonzalez BA
- Alviggi MG
- Amako K
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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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- Zerwas D
- della Porta GZ
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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
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- 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
Search for high-mass resonances decaying to dilepton final states in pp collisions at sâ=7 TeV with the ATLAS detector
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- Yanush S
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- Yilmaz M
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- Youssef S
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- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
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- Zenin O
- Zenis T
- Zerwas 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
- 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
- 23/11/2012
- 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 ZâČ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/Îł 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 fbâ1 in the e + e â channel and 5.0 fbâ1 in the ÎŒ + ÎŒ âchannel. A Z âČ 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 ZâČ Models
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