652 research outputs found
Visualization of Directional Beaming of Weakly Localized Raman from a Random Network of Silicon Nanowires
- Publication venue
- 'Royal College of Obstetricians & Gynaecologists (RCOG)'
- Publication date
- 21/07/2021
- Field of study
Disordered optical media are an emerging class of materials that can strongly scatter light. These materials are useful to investigate light transport phenomena and for applications in imaging, sensing and energy storage. While coherent light can be generated using such materials, its directional emission is typically hampered by their strong scattering nature. Here, the authors directly image Rayleigh scattering, photoluminescence and weakly localized Raman light from a random network of silicon nanowires via real-space microscopy and Fourier imaging. Direct imaging enables us to gain insight on the light transport mechanisms in the random material, to visualize its weak localization length and to demonstrate out-of-plane beaming of the scattered coherent Raman light. The direct visualization of coherent light beaming in such random networks of silicon nanowires offers novel opportunities for fundamental studies of light propagation in disordered media. It also opens venues for the development of next generation optical devices based on disordered structures, such as sensors, light sources, and optical switches
Fracture and damage localization in volcanic edifice rocks from El Hierro, Stromboli and Tenerife
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
© 2018 The Author(s). We present elastic wave velocity and strength data from a suite of three volcanic rocks taken from the volcanic edifices of El Hierro and Tenerife (Canary Islands, Spain), and Stromboli (Aeolian Islands, Italy). These rocks span a range of porosity and are taken from volcanoes that suffer from edifice instability. We measure elastic wave velocities at known incident angles to the generated through-going fault as a function of imposed strain, and examine the effect of the damage zone on P-wave velocity. Such data are important as field measurements of elastic wave tomography are key tools for understanding volcanic regions, yet hidden fractures are likely to have a significant effect on elastic wave velocity. We then use elastic wave velocity evolution to calculate concomitant crack density evolution which ranges from 0 to 0.17: highest values were correlated to the damage zone in rocks with the highest initial porosity
Automatic evaluation of body-related words among young women: an experimental study
- Author
- A Labarge
- A Moors
- A Roefs
- AG Greenwald
- AL Ahern
- American Psychiatric Association
- B Gawronski
- BA Teachman
- C Crandall
- C Schoemaker
- CP Herman
- CP Herman
- D Hargreaves
- D Trampe
- DM Garner
- E Loftus
- E Stice
- EJ Strahan
- G Cafri
- GH Bower
- GR Bessenoff
- H Markus
- I Ajzen
- IV Blair
- J Bargh
- J De Houwer
- J Dovidio
- J Polivy
- J Rudiger
- JA Bargh
- JA Cattarin
- JA McGrane
- Jacquelyn Cranney
- JH Neely
- JK Thompson
- JK Thompson
- K Klauer
- K Watts
- Kaaren J Watts
- KC Klauer
- LE Britton
- LM Groesz
- LR Vartanian
- M Altabe
- M Lavin
- M Powell
- M Tiggemann
- M Tiggemann
- M Tiggemann
- MJ Ferguson
- NS Spillane
- P van den Berg
- R Joshi
- R Puhl
- R Warren
- RH Fazio
- RH Fazio
- RH Fazio
- RH Fazio
- RM Calogero
- RM Shiffrin
- RR Wilcox
- RS Wyer
- S Chaiken
- T Cash
- T Cash
- T Cash
- T Cash
- T Cash
- TL Tylka
- WBG Jarvis
- Publication venue
- BioMed Central
- Publication date
- 01/01/2010
- Field of study
Background: Sociocultural models of body image disturbance have linked the development of body dissatisfaction and eating disorders to exposure to media messages depicting the unrealistically slender female physique. Previous research has demonstrated that exposure to images depicting the thin female ideal has negative effects on some females’ levels of body dissatisfaction. Much of this research, however, has utilised relatively long stimulus exposure times; thereby focusing on effortful and conscious processing of body-related stimuli. Relatively little is known about the nature of females’ affective responses to the textual components of body-related stimuli, especially when these stimuli are only briefly encountered. The primary aim of the current research was to determine whether young women automatically evaluate body-related words and whether these responses are associated with body image concerns, including self-reported levels of appearance schematicity, thin internalisation, body dissatisfaction, and dietary restraint. Methods: An affective priming task was used to investigate whether females automatically evaluate body-related words, and whether this is associated with self-reported body image concerns. In a within-participants experimental design, the valence congruence of the prime and target pairs was manipulated. Participants selected body words as primes in Experiment 1 (N = 27), while normatively selected body words were primes in Experiment 2 (N = 50). Each prime was presented briefly, followed by a target word which participants judged as “good” or “bad”. The dependent variable was response latency to the target. Results: Automatic evaluation was evident: responding to congruent pairs was faster than responding to incongruent pairs. Body image concerns were unrelated to automaticity. Conclusions: The findings suggest that brief encounters with body words are likely to prompt automatic evaluation in all young women, and that this process proceeds unintentionally and efficiently, without conscious guidance. The potential implications for higher order, conscious information processing is discussed
Foveal cone photoreceptor involvement in primary open-angle glaucoma
- Author
- Publication venue
- Springer-Verlag
- Publication date
- 01/01/2010
- Field of study
Looking the Part: Social Status Cues Shape Race Perception
- Author
- A Noymer
- AK Ho
- Aliya Saperstein
- AM Penner
- Andrew M. Penner
- CN Macrae
- D Peery
- DE Rumelhart
- DT Levin
- E Balcetis
- E Castano
- ER Smith
- GW Allport
- H Hill
- IV Blair
- J Halberstadt
- J Hurwitz
- JA Bargh
- JB Freeman
- JB Freeman
- JB Freeman
- JB Freeman
- JB Freeman
- JL Eberhardt
- JL Eberhardt
- JL McClelland
- Jonathan B. Freeman
- JP Smith
- K Hugenberg
- K Pauker
- K Sexton
- LA Hirschfeld
- M Gilens
- M Hane
- M Omi
- M Usher
- Matthias Scheutz
- MJ Spivey
- MJ Spivey
- Nalini Ambady
- NJ Ratcliff
- OH MacLin
- P Devine
- P Smolensky
- PG Schyns
- PL Smith
- RB Adams
- RH Fazio
- S Grossberg
- Sam Gilbert
- SL Zeger
- ST Fiske
- TT Rogers
- V Blanz
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
It is commonly believed that race is perceived through another's facial features, such as skin color. In the present research, we demonstrate that cues to social status that often surround a face systematically change the perception of its race. Participants categorized the race of faces that varied along White–Black morph continua and that were presented with high-status or low-status attire. Low-status attire increased the likelihood of categorization as Black, whereas high-status attire increased the likelihood of categorization as White; and this influence grew stronger as race became more ambiguous (Experiment 1). When faces with high-status attire were categorized as Black or faces with low-status attire were categorized as White, participants' hand movements nevertheless revealed a simultaneous attraction to select the other race-category response (stereotypically tied to the status cue) before arriving at a final categorization. Further, this attraction effect grew as race became more ambiguous (Experiment 2). Computational simulations then demonstrated that these effects may be accounted for by a neurally plausible person categorization system, in which contextual cues come to trigger stereotypes that in turn influence race perception. Together, the findings show how stereotypes interact with physical cues to shape person categorization, and suggest that social and contextual factors guide the perception of race
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- 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
- Ackers M
- 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
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Alam MA
- Alam MS
- Albrand S
- Aleksa M
- Aleksandrov IN
- Aleppo M
- 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
- Alonso J
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- 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
- Antonelli S
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arms KE
- Armstrong SR
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auerbach B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- 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
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
- Baker S
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- 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
- Barr AJ
- Barreiro F
- Barrera CO
- Barrillon P
- Bartoldus R
- Barton AE
- Bartsch D
- 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 HP
- Beckingham M
- Becks KH
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bee C
- Begel M
- Behera PK
- Beimforde M
- Belanger-Champagne C
- Belenguer MJ
- Belhorma B
- Bell PJ
- Bell WH
- Bella G
- Bella LA
- Bellagamba L
- Bellina F
- Bellomo G
- Bellomo M
- Belloni A
- Belotskiy K
- Beltramello O
- Ben Ami S
- Benary O
- Benchekroun D
- Benchouk C
- Bendel M
- Benedict BH
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- 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
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Bingul A
- Bini C
- Biscarat C
- Bischof R
- Bitenc U
- Black KM
- Blair RE
- Blanchard J-B
- Blanchot G
- Blocker C
- Blocki J
- Blondel A
- Blum W
- Blumenschein U
- Boaretto C
- Bobbink GJ
- Bobrovnikov VB
- Bocci A
- Bock R
- Boddy CR
- Boehler M
- Boek J
- Boelaert N
- Boeser S
- Bogaerts JA
- Bogdanchikov A
- Bogouch A
- Bohm C
- Boisvert V
- Bold T
- Boldea V
- Bona M
- Boonekamp M
- Boorman G
- Booth CN
- Booth JRA
- Booth P
- 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
- Boulahouache C
- Bourdarios C
- Bousson N
- Boveia A
- Boyd J
- Boyko IR
- Bozhko NI
- Bozovic-Jelisavcic I
- Braccini S
- Bracinik J
- Braem A
- Brambilla E
- Branchini P
- Branco MDO
- 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
- Brett ND
- Bright-Thomas PG
- Britton D
- Brochu FM
- Brock I
- Brock R
- Brodbeck TJ
- Brodet E
- Broggi F
- Bromberg C
- Brooijmans G
- Brooks WK
- Brown G
- Brubaker E
- Bruncko D
- Bruneliere R
- Brunet S
- Bruni A
- Bruni G
- Bruschi M
- Buanes T
- Bucci F
- Buchanan J
- Buchanan NJ
- Buchholz P
- Buckingham RM
- Buckley AG
- Buda SI
- Budagov IA
- Budick B
- Buescher V
- Bueso XP
- Bugge L
- Buira-Clark D
- Buis EJ
- 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
- Byatt T
- Cabrera Urban S
- Caccia M
- Caforio D
- Cakir IT
- Cakir O
- Calafiura P
- Calderini G
- Calfayan P
- Calkins R
- Caloba LP
- Caloi R
- Calvet D
- Calvet S
- Camard A
- Camarri P
- Cambiaghi M
- Cameron D
- Camillocci ES
- Cammin J
- Campana S
- Campanelli M
- Canale V
- Canelli F
- Canepa A
- Cantero J
- Capasso L
- Caprini I
- Caprini M
- Caprio M
- Capriotti D
- Capua M
- Caputo R
- Caramarcu C
- Cardarelli R
- Carli T
- Carlino G
- Carminati L
- Caron B
- Caron S
- Carpentieri C
- Carter AA
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Cascella M
- Caso C
- Castaneda-Miranda E
- Castanheira MTD
- Castillo Gimenez V
- Castillo LRF
- Castro NF
- Cataldi G
- Cataneo F
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- Cavalcanti TP
- Cavallari A
- Cavalleri P
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Cazzato A
- Ceradini F
- Cerna C
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervetto M
- 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
- Chen H
- Chen L
- Chen S
- Chen T
- Chen X
- Cheng S
- Cheong ALF
- Cheplakov A
- Chepurnov VF
- Cherkaoui El Moursli R
- Chernyatin V
- Cheu E
- Cheung SL
- Chevalier L
- Chevallier F
- 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
- Ciftci AK
- Ciftci R
- Cinca D
- Cindro V
- Ciobotaru MD
- Ciocca C
- Ciocio A
- Cirilli 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
- Coe P
- Cogan JG
- Coggeshall J
- Cogneras E
- Cojocaru CD
- Colas J
- Colijn AP
- Collaboration A
- Collard C
- Collins NJ
- Collins-Tooth C
- Collot J
- Colon G
- Coluccia R
- Comune G
- Conde Muino P
- Coniavitis E
- Conidi MC
- Consonni M
- Constantinescu S
- Conta C
- Conventi F
- Cook J
- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Cooper-Smith NJ
- Copic K
- Cornelissen T
- Corradi M
- Correard S
- Correia AMH
- Corriveau F
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Costin T
- Cote D
- Coura Torres R
- Courneyea L
- Cowan G
- Cowden C
- Cox BE
- Cranmer K
- Crepe-Renaudin S
- Cristinziani M
- Crosetti G
- Crupi R
- Cuneo S
- Curatolo M
- Curtis CJ
- Cwetanski P
- Czirr H
- Czyczula Z
- D'Auria S
- D'Onofrio M
- D'Orazio A
- da Costa JBG
- Da Rocha Gesualdi Mello A
- Da Silva PVM
- Da Via C
- Dabrowski W
- Dahlhoff A
- Dai T
- Dallapiccola C
- Dallison SJ
- Dam M
- Damazio DO
- Dameri M
- Damiani DS
- Danielsson HO
- Dankers R
- Dannheim D
- Dao V
- Darbo G
- Darlea GL
- Daum C
- Dauvergne JP
- Davey W
- Davidek T
- Davidson N
- Davidson R
- Davies M
- Davison AR
- Dawe E
- Dawson I
- Dawson JW
- Daya RK
- de Asmundis R
- De Castro S
- De Cecco S
- de Graat J
- De Groot N
- de Jong P
- De La Cruz-Burelo E
- De La Taille C
- de Lima JGR
- De Lotto B
- De Mora L
- De Nooij L
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- de Saintignon P
- De Salvo A
- De Sanctis U
- De Santo A
- De K
- Dean S
- Dedes G
- Dedovich DV
- Degenhardt J
- Dehchar M
- Deile M
- Del Papa C
- Del Peso J
- Del Prete T
- 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
- Denisov SP
- Dennis C
- 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 Nardo R
- Di Simone A
- Di Sipio R
- Diaz MA
- Diblen F
- Diehl EB
- Dietl H
- Dietrich J
- Dietzsch TA
- Diglio S
- Dingfelder J
- Dionisi C
- Dita P
- Dita S
- Dittus F
- Djama F
- Djilkibaev R
- Djobava T
- do Vale MAB
- Do Valle Wemans A
- Doan TKO
- Dobbs M
- Dobinson R
- Dobos D
- Dobson E
- Dobson M
- Dodd J
- Dogan OB
- Doglioni C
- Doherty T
- Dohmae T
- Doi Y
- Dolejsi J
- Dolenc I
- Dolezal Z
- Dolgoshein BA
- Donadelli M
- Donega M
- Donini J
- Donszelmann TC
- Dopke J
- Doria A
- Dos Anjos A
- Dos Santos DR
- Dosil M
- Dotti A
- Dova MT
- Dowell JD
- Doxiadis AD
- Doyle AT
- Drasal Z
- Drees J
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- Drevermann H
- Driouichi C
- Dris M
- Drohan JG
- Dubbert J
- Dubbs T
- Dube S
- Duchovni E
- Duckeck G
- Dudarev A
- Dudziak F
- Duehrssen M
- Duerdoth IP
- Dueren M
- Duflot L
- Dufour M-A
- Dunford M
- Duxfield R
- Dwuznik M
- Dydak F
- Dzahini D
- Ebke J
- Eckert S
- Eckweiler S
- Edmonds K
- Edwards CA
- Efthymiopoulos I
- Ehrenfeld W
- Ehrich T
- Eifert T
- Eigen G
- Einsweiler K
- Eisenhandler E
- Ekelof T
- El Kacimi M
- Ellert M
- Elles S
- Ellinghaus F
- Ellis K
- Ellis N
- Elmsheuser J
- Elsing M
- Ely R
- Emeliyanov D
- Engelmann R
- Engl A
- Epp B
- Eppig A
- Erdmann J
- Ereditato A
- Eriksson D
- Ernst J
- Ernst M
- Ernwein J
- Errede D
- Errede S
- Ertel E
- Escalier M
- Eschrich IG
- Escobar C
- Espinal Curull X
- Esposito B
- Etienne F
- Etienvre AI
- Etzion E
- Evangelakou D
- Evans H
- Fabbri L
- Fabre C
- Facius K
- Fajardo LSG
- Fakhrutdinov RM
- Falciano S
- Falou AC
- Fang Y
- Fanti M
- Farbin A
- Farilla A
- Farley J
- Farooque T
- Farrington SM
- Farthouat P
- Fasching D
- Fassnacht P
- Fassouliotis D
- Fatholahzadeh B
- Favareto A
- Fayard L
- Fazio S
- Febbraro R
- Federic P
- Fedin OL
- Fedorko I
- Fedorko W
- Fehling-Kaschek M
- Feligioni L
- Fellmann D
- Felzmann CU
- Feng C
- Feng EJ
- Fenyuk AB
- Ferencei J
- Ferguson D
- Ferland J
- Fernandes B
- Fernando W
- Ferrag S
- Ferrando BMS
- Ferrando J
- Ferrara V
- Ferrari A
- Ferrari P
- Ferrari R
- Ferrer A
- Ferrer ML
- Ferrere D
- Ferretti C
- Ferro F
- Fiascaris M
- Fiedler F
- Filipcic A
- Filippas A
- Filthaut F
- Fincke-Keeler M
- Fiolhais MCN
- Fiorini L
- Firan A
- Fischer G
- Fischer P
- Fisher MJ
- Fisher SM
- Flammer J
- Flechl M
- Fleck I
- Fleckner J
- Fleischmann P
- Fleischmann S
- Flick T
- Flowerdew MJ
- Foehlisch F
- Fokitis M
- Forbush DA
- Formica A
- Forti A
- Fortin D
- Foster JM
- Fournier D
- Foussat A
- Fowler AJ
- Fowler K
- Fox H
- Francavilla P
- Franchino S
- Francis D
- Frank T
- Franklin M
- Franz S
- Fraternali M
- Fratina S
- French ST
- Froeschl R
- Froidevaux D
- Frost JA
- Fukunaga C
- Fuster J
- Gabaldon C
- Gabizon O
- Gadfort T
- Gadomski S
- Gagliardi G
- Gagnon P
- Galea C
- Gallas EJ
- Gallas MV
- Gallo V
- Gallop BJ
- Gallus P
- Galtieri AB
- Galyaev E
- Gan KK
- Gao YS
- Gapienko VA
- Gaponenko A
- Garberson F
- Garcia C
- Garcia YR
- Garcia-Sciveres M
- Gardner RW
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- Zhemchugov A
- Zheng S
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- Zhuravlov V
- Zieminska D
- Zilka B
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- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Search for 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
- Amelung C
- Ammosov VV
- Amor Dos Santos SP
- Amorim A
- 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
- Anisenkov A
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Aoun S
- Bella LA
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Arfaoui S
- Arguin J-F
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
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- Arutinov D
- Asai S
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- Astbury A
- Atkinson M
- Aubert B
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- Augsten K
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- Avolio G
- Avramidou R
- Axen D
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
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- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Mayes JB
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
- Baker MD
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- Bangert A
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- Galtieri AB
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- Barnett RM
- Baroncelli A
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- da Costa JBG
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- Bartoldus R
- Barton AE
- Bartsch V
- Basye A
- Bates RL
- Batkova L
- Batley JR
- Battaglia A
- Battistin M
- Bauer F
- Bawa HS
- Beale S
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- Beauchemin PH
- Beccherle R
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- Beddall AJ
- Beddall A
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- Bee CP
- Beemster LJ
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- Yamamura T
- Yamanaka T
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yao Y
- Yasu Y
- Smit GVY
- Ye J
- Ye S
- 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
- Zhang H
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- Zhao Z
- Zhemchugov A
- Zhong J
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- Zhu CG
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- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Collaboration ATLAS
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2008
- Field of study
A search for new phenomena in final states with four or more leptons (electrons or muons) is presented. The analysis is based on 4.7 fb−1 of s=7TeV proton-proton collisions delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in two signal regions: one that requires moderate values of missing transverse momentum and another that requires large effective mass. The results are interpreted in a simplified model of R-parity-violating supersymmetry in which a 95% CL exclusion region is set for charged wino masses up to 540 GeV. In an R-parity-violating MSUGRA/CMSSM model, values of m 1/2 up to 820 GeV are excluded for 10 < tan β < 40
Search for high-mass resonances decaying to dilepton final states in pp collisions at s√=7 TeV with the ATLAS detector
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- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
- Aben R
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- Yilmaz M
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- Yoshihara K
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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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- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
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- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- Springer
- Publication date
- 01/01/2012
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral Z′ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/γ bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fb−1 in the e + e − channel and 5.0 fb−1 in the μ + μ −channel. A Z ′ boson with Standard Model-like couplings is excluded at 95 % confidence level for masses below 2.22 TeV. A Randall-Sundrum graviton with coupling k/MPl=0.1 is excluded at 95 % confidence level for masses below 2.16 TeV. Limits on the other models are also presented, including Technicolor and Minimal Z′ Models
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
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- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
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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
Industrial Systems Biology of Saccharomyces cerevisiae Enables Novel Succinic Acid Cell Factory.
- Author
- A Fazio
- B Regenberg
- C Bro
- C Verudyn
- D Cimini
- DA Aliverdieva
- DG Fisk
- Donatella Cimini
- H Song
- I Nookaew
- J Förster
- J Nielsen
- J Nielsen
- JB McKinlay
- Jens Nielsen
- JG Zeikus
- JI Castrillo
- JL Adrio
- JM Otero
- José Manuel Otero
- JP van Dijken
- JS Edwards
- K Jantama
- Kiran R. Patil
- KR Patil
- Lisbeth Olsson
- LR Lynd
- M Sauer
- MJ Herrgård
- MW Covert
- N Eredeniz
- NC Duarte
- PC Lee
- RD Gietz
- RM Zelle
- S Wattanachaisaereekul
- Scott E. Baker
- Simon G. Poulsen
- SM Paley
- T Wilke
- TW Christianson
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/01/2013
- Field of study
Saccharomyces cerevisiae is the most well characterized eukaryote, the preferred microbial cell factory for the largest industrial biotechnology product (bioethanol), and a robust commerically compatible scaffold to be exploitted for diverse chemical production. Succinic acid is a highly sought after added-value chemical for which there is no native pre-disposition for production and accmulation in S. cerevisiae. The genome-scale metabolic network reconstruction of S. cerevisiae enabled in silico gene deletion predictions using an evolutionary programming method to couple biomass and succinate production. Glycine and serine, both essential amino acids required for biomass formation, are formed from both glycolytic and TCA cycle intermediates. Succinate formation results from the isocitrate lyase catalyzed conversion of isocitrate, and from the alpha-keto-glutarate dehydrogenase catalyzed conversion of alpha-keto-glutarate. Succinate is subsequently depleted by the succinate dehydrogenase complex. The metabolic engineering strategy identified included deletion of the primary succinate consuming reaction, Sdh3p, and interruption of glycolysis derived serine by deletion of 3-phosphoglycerate dehydrogenase, Ser3p/Ser33p. Pursuing these targets, a multi-gene deletion strain was constructed, and directed evolution with selection used to identify a succinate producing mutant. Physiological characterization coupled with integrated data analysis of transcriptome data in the metabolically engineered strain were used to identify 2nd-round metabolic engineering targets. The resulting strain represents a 30-fold improvement in succinate titer, and a 43-fold improvement in succinate yield on biomass, with only a 2.8-fold decrease in the specific growth rate compared to the reference strain. Intuitive genetic targets for either over-expression or interruption of succinate producing or consuming pathways, respectively, do not lead to increased succinate. Rather, we demonstrate how systems biology tools coupled with directed evolution and selection allows non-intuitive, rapid and substantial re-direction of carbon fluxes in S. cerevisiae, and hence show proof of concept that this is a potentially attractive cell factory for over-producing different platform chemicals
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