865 research outputs found
sustainability in cereal crop production in mediterranean environments
- Author
- Publication venue
- Publication date
- 01/01/2015
- Field of study
The continuous increase of the world population (a growth of about one-third is expected by 2050), together with an even larger increase in food demand (especially in emerging countries), will lead in the next 30 years to the necessity to produce 70 % more food. To keep the pace with food demand, global cereal production would need to increase by 40 % overall, or by some 900 million tons between the present and 2050. Single countries can either increase production or increase net imports or a combination of both
The Synthetic Plasmodium falciparum Circumsporozoite Peptide PfCS102 as a Malaria Vaccine Candidate: A Randomized Controlled Phase I Trial
- Author
- A Bonelo
- A Lalvani
- A Malik
- Blaise Genton
- Christophe Reymond
- David Joseph Diemert
- DL Doolan
- DL Doolan
- EH Nardin
- F Dubovsky
- Floriana Lurati-Ruiz
- François Spertini
- Giampietro Corradin
- Hildur E. Blythman
- J Renggli
- JA Lopez
- JA Lopez
- JA Lopez
- JA Stoute
- JG Beeson
- JM Gonzalez
- K Arun Kumar
- K Marsh
- KE Kester
- KE Kester
- MA Roggero
- N Garcon
- Opokua Ofori-Anyinam
- P Potocnjak
- P Sun
- R Audran
- R Schwenk
- Régine Audran
- TC Luke
- U Blum-Tirouvanziam
- U Blum-Tirouvanziam
- V Meraldi
- W Ripley Ballou
- WH Reece
- WR Weiss
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2009
- Field of study
BACKGROUND: Fully efficient vaccines against malaria pre-erythrocytic stage are still lacking. The objective of this dose/adjuvant-finding study was to evaluate the safety, reactogenicity and immunogenicity of a vaccine candidate based on a peptide spanning the C-terminal region of Plasmodium falciparum circumsporozoite protein (PfCS102) in malaria naive adults. METHODOLOGY AND PRINCIPAL FINDINGS: Thirty-six healthy malaria-naive adults were randomly distributed into three dose blocks (10, 30 and 100 microg) and vaccinated with PfCS102 in combination with either Montanide ISA 720 or GSK proprietary Adjuvant System AS02A at days 0, 60, and 180. Primary end-point (safety and reactogenicity) was based on the frequency of adverse events (AE) and of abnormal biological safety tests; secondary-end point (immunogenicity) on P. falciparum specific cell-mediated immunity and antibody response before and after immunization. The two adjuvant formulations were well tolerated and their safety profile was good. Most AEs were local and, when systemic, involved mainly fatigue and headache. Half the volunteers in AS02A groups experienced severe AEs (mainly erythema). After the third injection, 34 of 35 volunteers developed anti-PfCS102 and anti-sporozoite antibodies, and 28 of 35 demonstrated T-cell proliferative responses and IFN-gamma production. Five of 22 HLA-A2 and HLA-A3 volunteers displayed PfCS102 specific IFN-gamma secreting CD8(+) T cell responses. Responses were only marginally boosted after the 3(rd) vaccination and remained stable for 6 months. For both adjuvants, the dose of 10 microg was less immunogenic in comparison to 30 and 100 microg that induced similar responses. AS02A formulations with 30 microg or 100 microg PfCS102 induced about 10-folds higher antibody and IFN-gamma responses than Montanide formulations. CONCLUSIONS/SIGNIFICANCE: PfCS102 peptide was safe and highly immunogenic, allowing the design of more advanced trials to test its potential for protection. Two or three immunizations with a dose of 30 microg formulated with AS02A appeared the most appropriate choice for such studies. TRIAL REGISTRATION: Swissmedic.ch 2002 DR 1227
Molecular and cellular mechanisms underlying the evolution of form and function in the amniote jaw.
- Author
- A Abzhanov
- A Abzhanov
- A Abzhanov
- A Baggiolini
- A Baroffio
- A Beverdam
- A Chevallier
- A Davidian
- A del Rio
- A Graham
- A Graham
- A Hosseini
- A Rinon
- A Roycroft
- A Sharir
- A Shellard
- A Subramanian
- AA Pitsillides
- AE Adams
- AE Merrill
- AG Robling
- AG Robling
- AH Jheon
- AJ Hughes
- AL Romanoff
- AL Tavares
- ALP Tavares
- AM Bailleul
- AM Bailleul
- AM Lucas
- AS Pollard
- AS Romer
- AS Romer
- AS Tucker
- AS Tucker
- AW Crompton
- AW Crompton
- B Christ
- B McBratney-Owen
- B Ruhin
- BA Moore-Scott
- BD Matthews
- BF Eames
- BF Eames
- BF Kingsbury
- BK Hall
- BK Hall
- BK Hall
- BK Hall
- BK Hall
- BK Hall
- BK Hall
- BK Hall
- BK Hall
- BK Hall
- BK Hall
- BL Pruitt
- C Attanasio
- C Gans
- C Gegenbaur
- C Holliday
- C Mitgutsch
- C Patterson
- C Reichert
- CI Lorda-Diez
- CL Hammond
- CS Le Lievre
- CS Le Lièvre
- CT Miller
- CV Baker
- CV Baker
- CW Benkman
- CW Benkman
- D Hu
- D Hu
- D Hu
- D Hu
- D Noden
- DD Davis
- DE Clouthier
- DG Wilkinson
- DJ Evans
- DL Stemple
- DM Noden
- DM Noden
- DM Noden
- DM Noden
- DM Noden
- DM Noden
- DM Noden
- DM Noden
- DM Noden
- DM Noden
- DM Noden
- DM Noden
- DR Carter
- DR Cordero
- E Berthet
- E Blitz
- E Blitz
- E Dupin
- E Gaupp
- E Jarvik
- E Theveneau
- E Tzahor
- E Tzahor
- E Zelzer
- EC Olesnicky Killian
- EF Allin
- EL Ealba
- EM Sefton
- EP Allis
- EP Allis
- EP Allis
- ER Lankester
- ES Goodrich
- ES Goodrich
- ES Russell
- F Lescroart
- F Liu
- FJ Smith
- FL Landacre
- FV Jotereau
- FW Chamberlain
- G Andres
- G Balooch
- G Couly
- G Couly
- G Couly
- G Kardon
- G Kardon
- G Köntges
- G Wagner
- G Zweers
- GA Zweers
- GA Zweers
- GA Zweers
- GB Muller
- GF Couly
- GF Couly
- GM Morriss-Kay
- GR de Beer
- GR de Beer
- GR de Beer
- H Vinkka
- HB Shaffer
- HJ Chong
- HL Hamilton
- HL Szabo-Rogers
- HP Shih
- I Bothe
- I Raizman
- I Rot-Nikcevic
- J Apostolakos
- J Fang
- J Grenier
- J Hall
- J Jeong
- J Kahn
- J Ruberte
- J Stutzmann
- JA Helms
- JB Gross
- JB Platt
- JF Webb
- JJ Baumel
- JJ Schoenebeck
- JJ Schoenebeck
- JL Chang
- JL Fish
- JL Fish
- JL Fish
- JL Fish
- JM Brito
- JM Richman
- JM Tabler
- JN Thompson
- JP Golding
- JR Merida-Velasco
- JR Merida-Velasco
- JR Robbins
- JS Kingsley
- JW Kingsbury
- K Hayashi
- K Sheehan-Rooney
- K Yasui
- KC Woronowicz
- KC Wu
- KE Haworth
- KJ Lamb
- KK Smith
- KK Smith
- KK Smith
- KK Smith
- KS Thomson
- KW Li
- KW Tosney
- L LeResche
- L Olsson
- L Ramage
- LB Ruest
- LS Gammill
- LS Stone
- LS Stone
- M Bancroft
- M Benjamin
- M Bronner-Fraser
- M Bronner-Fraser
- M Hoso
- M Jollie
- M Jollie
- M Jollie
- M Jollie
- M Linde-Medina
- M Minoux
- M Persson
- M Qiu
- M Qiu
- M Sieber-Blum
- M Simoes-Costa
- M Takechi
- M Tokita
- M Tokita
- MA Selleck
- MA Shkoukani
- MAJ Selleck
- MJ Depew
- MJ Depew
- MJ Depew
- MJ Depew
- ML Martik
- ML Moss
- ML Moss
- MM Dawson
- MM Smith
- MM Smith
- MN Spyropoulos
- MR Sanchez-Villagra
- MR Sánchez-Villagra
- MS Tyler
- MSY Lee
- N Anthwal
- N Anthwal
- N Anthwal
- N Wang
- NC Jones
- NJ Giori
- NM Young
- NM Young
- NN Soni
- NS Bradley
- O Campas
- O Rieppel
- OP Hamill
- P Betancur
- P Danaisawadi
- P Hunt
- P Kissel
- P Kulesa
- P Murray
- P Murray
- P Thorogood
- P Wu
- P Wu
- PA Trainor
- PA Trainor
- PA Trainor
- PA Trainor
- PA Trainor
- PA Trainor
- PA Trainor
- PD Henion
- PDF Murray
- PH Francis-West
- PS Verma
- PY Lwigale
- R Cerny
- R Derynck
- R Diogo
- R Luo
- R Mallarino
- R McBeath
- R McLennan
- R McLennan
- R Owen
- R Owen
- R Presley
- R Presley
- R Sambasivan
- R Sambasivan
- R Schweitzer
- RA Schneider
- RA Schneider
- RA Schneider
- RA Schneider
- RA Schneider
- RA Schneider
- RA Schneider
- RA Schneider
- RA Schneider
- RA Yuodelis
- RC Garcez
- RC Mootoosamy
- RC Solem
- RG Harrison
- RG Northcutt
- RG Northcutt
- RJ Gorlin
- RL Carroll
- RL Zusi
- RW Oppenheim
- RW Oppenheim
- RW Oppenheim
- RW Shufeldt
- S Alappat
- S Amin
- S Creuzet
- S Dupont
- S Ekanayake
- S Hörstadius
- S Kavumpurath
- S Krispin
- S Kuraku
- S Kuratani
- S Kuratani
- S Kuratani
- S Kuratani
- S Kuratani
- S Kuratani
- S Kuratani
- S Lamichhaney
- S Lautenschlager
- S Lautenschlager
- S Murakami
- S Shibata
- S Tajbakhsh
- S Thomopoulos
- S Wadhwa
- SC Ahlgren
- SC Ahlgren
- SH Lee
- SH Reynolds
- SJ Gould
- SJ Mathew
- SL Horowitz
- SL Prescott
- SL Washburn
- SR Roberts
- SW Herring
- T Hems
- T Hirasawa
- T Kantomaa
- T Maeda
- T Mammoto
- T Matsuoka
- T Miyashita
- T Rowe
- T Sato
- T Sauka-Spengler
- T Sauka-Spengler
- T Square
- T Thomas
- T Yoshida
- TA Appel
- TA Mitsiadis
- TA Mitsiadis
- TC Fitzgerald
- TE Parsons
- TG Boyd
- TH Huxley
- TH Huxley
- TL Vincent
- V Govindarajan
- V Hamburger
- V Hamburger
- V Shone
- VL Naples
- W Maier
- WA Beresford
- WA Beresford
- WE Reif
- WF Van den Heuvel
- WG Hall
- WJ Moore
- WJ Moore
- WK Parker
- WM McLeod
- X Jiang
- X Li
- XL Tu
- Y Hashimoto
- Y Shigetani
- Y Shigetani
- Y Shwartz
- Y Song
- Y Sugimoto
- Publication venue
- eScholarship, University of California
- Publication date
- 01/01/2019
- Field of study
The amniote jaw complex is a remarkable amalgamation of derivatives from distinct embryonic cell lineages. During development, the cells in these lineages experience concerted movements, migrations, and signaling interactions that take them from their initial origins to their final destinations and imbue their derivatives with aspects of form including their axial orientation, anatomical identity, size, and shape. Perturbations along the way can produce defects and disease, but also generate the variation necessary for jaw evolution and adaptation. We focus on molecular and cellular mechanisms that regulate form in the amniote jaw complex, and that enable structural and functional integration. Special emphasis is placed on the role of cranial neural crest mesenchyme (NCM) during the species-specific patterning of bone, cartilage, tendon, muscle, and other jaw tissues. We also address the effects of biomechanical forces during jaw development and discuss ways in which certain molecular and cellular responses add adaptive and evolutionary plasticity to jaw morphology. Overall, we highlight how variation in molecular and cellular programs can promote the phenomenal diversity and functional morphology achieved during amniote jaw evolution or lead to the range of jaw defects and disease that affect the human condition
Geckos decouple fore- and hind limb kinematics in response to changes in incline
- Author
- A Biewener
- A Biewener
- A Schmidt
- A Schmidt
- A Seyfarth
- A Zaaf
- A Zaaf
- AG Gillies
- AJ Clark
- Aleksandra V. Birn-Jeffery
- AP Russell
- AP Russell
- AP Russell
- AR Lammers
- AV Birn-Jeffery
- AV Birn-Jeffery
- B Chen
- BC Jayne
- C Krause
- CR Taylor
- CT Farley
- CT Farley
- CT Moritz
- DF Hoyt
- DJ Irschick
- DJ Irschick
- DL Claussen
- DV Lee
- FC Pinch
- GB Gillis
- GC Hill
- H Li
- I Nisky
- J Iriarte-Díaz
- J Lees
- JA Nyakatura
- JH Zar
- JJ Chen
- JL Raab
- JL Smith
- K Autumn
- K Autumn
- K Autumn
- K Autumn
- K Autumn
- KL Foster
- LC Spezzano
- MA Daley
- MA Daley
- MA Daley
- MA Daley
- MH Dickinson
- MK Johnson
- N Heglund
- N Stevens
- NB Webster
- NC Holt
- P Carlson-Kuhta
- R Blickhan
- R Blickhan
- R Ruibal
- RJ Full
- RJ Williams
- RL Marsh
- RL Nudds
- SK Lauer
- T Hagey
- TA McMahon
- TC Crook
- TE Higham
- TE Higham
- TE Higham
- TE Higham
- TE Higham
- Timothy E. Higham
- TJ Roberts
- TJ Roberts
- TL Hedrick
- TL Kivell
- WJ Stewart
- Y Blum
- Y Blum
- Y Blum
- Y Tian
- Z Wang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
This work is supported by an NSF grant (NSF IOS-1147043) to TE
Hepatopulmonary syndrome in patients with chronic liver disease: role of pulse oximetry
- Author
- A Regev
- AGN Agusti
- C Babbs
- CJ Dickinson
- CJ Dickinson
- Claudia Müller
- CR Hind
- ED Robin
- G Teuber
- GA Abrams
- GA Abrams
- Hans-Peter Allgaier
- Hinrich Hamm
- Hubert Erich Blum
- JD Wolfe
- JM Hourani
- KL Swanson
- Klaus-Peter Maier
- M Altman
- M Flückiger
- M Krowka
- Manfred Olschewski
- MJ Krowka
- MJ Krowka
- MK Whyte
- MR Arguedas
- MR Hales
- P Schenk
- PA Lange
- PA Lange
- Peter Deibert
- R Pacca
- R Rodriguez-Roisin
- R Rodriguez-Roisin
- R Rydell
- RNH Pugh
- S Sherlock
- SB Fox
- Stefanie Loesch
- T Furukawa
- TB Kinane
- TC Kennedy
- V Izquierdo
- V Scott
- WE Hopkins
- Publication venue
- BioMed Central
- Publication date
- 25/04/2006
- Field of study
BACKGROUND: Hepatopulmonary syndrome (HPS) is a rare complication of liver diseases of different etiologies and may indicate a poor prognosis. Therefore, a simple non-invasive screening method to detect HPS would be highly desirable. In this study pulse oximetry was evaluated to identify patients with HPS. METHODS: In 316 consecutive patients with liver cirrhosis (n = 245), chronic hepatitis (n = 69) or non-cirrhotic portal hypertension (n = 2) arterial oxygen saturation (SaO(2)) was determined using a pulse oximeter. In patients with SaO(2 )≤92% in supine position and/or a decrease of ≥4% after change from supine to upright position further diagnostic procedures were performed, including contrast-enhanced echocardiography and perfusion lung scan. RESULTS: Seventeen patients (5.4%) had a pathological SaO(2). Four patients (1.3%) had HPS. HPS patients had a significant lower mean SaO(2 )in supine (89.7%, SD 5.4 vs. 96.0%, SD 2.3; p = 0.003) and upright position (84.3%, SD 5.0 vs. 96.0%, SD 2.4; p = 0.001) and had a lower mean PaO(2 )(56.2 mm Hg, SD 15.2 vs. 71.2 mm Hg, SD 20.2; p = 0.02) as compared to patients without HPS. The mean ΔSaO(2 )(difference between supine and upright position) was 5.50 (SD 7) in HPS patients compared to non-HPS patients who showed no change (p = 0.001). There was a strong correlation between shunt volume and the SaO(2 )values (R = -0.94). CONCLUSION: Arterial SaO(2 )determination in supine and upright position is a useful non-invasive screening test for HPS and correlates well with the intrapulmonary shunt volume
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
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- Chakraborty D
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of √s = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pT≥20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
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- 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
Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at √s = 7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abulaitia Y
- Acharya BS
- Adamczyk L
- Adams DL
- Addy TN
- Adelman J
- Adomeit S
- Adye T
- Agatonovic-Jovin T
- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Allbrooke BMM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alviggi MG
- Amako K
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Anduaga XS
- Angelidakis S
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- Anghinolfi F
- Anh TV
- Anisenkov AV
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- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
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- Argyropoulos S
- Arik E
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- Armbruster AJ
- Arnaez O
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of √s = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentre−of−massframeisusedtosuppressthelargemulti−jetbackground.Thecross−sectionforeventswithahadronicallydecayingWorZboson,withtransversemomentum{{p}_{{\rm T}}}\gt 320\;{\rm Ge}{\rm V}andpseudorapidity|\eta |\lt 1.9,ismeasuredtobe{{\sigma }_{W+Z}}=8.5\pm 1.7$ pb and is compared to next-to-leading-order calculations. The selected events are further used to study jet grooming techniques
Search for the neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
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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
Search for direct pair production of the top squark in all-hadronic final states in proton-proton collisions at s√=8 TeV with the ATLAS detector
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- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
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- Abolins M
- AbouZeid OS
- Abramowicz H
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- Acharya BS
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- Adomeit S
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- Akesson TPA
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- Akimov AV
- Alberghi GL
- Albert J
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- Alconada Verzini MJ
- Aleksa M
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- Alexa C
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- Yao L
- Yao W-M
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- Yen AL
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- Yildiz HD
- Yilmaz M
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- Zanzi D
- Zeitnitz C
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- Zemla A
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- Zhemchugov A
- Zhong J
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fb−1 of proton–proton collision data at √s = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via t˜→tχ˜01 or t˜→ bχ˜±1 →bW(∗)χ˜01 , where χ˜01 (χ˜±1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of t˜ → tχ˜01 . For a branching fraction of 100%, top squark masses in the range 270–645 GeV are excluded for χ˜01 masses below 30 GeV. For a branching fraction of 50% to either t˜ → tχ˜01 or t˜ → bχ˜±1 , and assuming the χ˜±1 mass to be twice the χ˜01 mass, top squark masses in the range 250–550 GeV are excluded for χ˜01 masses below 60 GeV
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