76 research outputs found
Rotor blade construction for circulation control aircraft
- Publication venue
- Publication date
- 02/12/1986
- Field of study
A circulation control aircraft rotor blade having a spanwise Coanda surface 16 and a plurality of spanwise extending flexible composite material panels 18 cooperating with the surface to define slots for the discharge of compressed air from within the blade with each panel having first flexure means 60 associated with screw adjustments 36 for establishing a slot opening preload and second flexure means 62 associated with screw adjustments 38 for establishing a slot maximum opening
A Climate Change Vulnerability Assessment of California's At-Risk Birds
- Author
- AE McKechnie
- B Macwirter
- B Smit
- B Young
- BL Turner
- C Both
- C Both
- C Parmesan
- C Rosenzweig
- CD Thomas
- CD Thomas
- D Bunn
- D Stralberg
- David Hyrenbach
- EL Rowland
- F Jiguet
- F Jiguet
- G-R Walther
- H Galbraith
- HP Possingham
- J Bernardo
- JA Wiens
- JD Ligon
- JL Isaac
- JM Hughes
- JM Lenihan
- JM West
- KL Laidre
- Lyann A. Comrack
- M van de Pol
- MA Schroeder
- MF Carter
- MS Warren
- N Saino
- Nathaniel E. Seavy
- NE Heller
- P Glick
- PF Donald
- R Julliard
- RK Heikkinen
- Ryan T. DiGaudio
- SE Williams
- SG Wolf
- SH Schneider
- SR Beissinger
- SR Loarie
- TE Dahl
- Thomas Gardali
- TL Root
- TW Richardson
- WB Monahan
- WD Shuford
- WW Weathers
- Y Yom-Tov
- Publication venue
- Public Library of Science
- Publication date
- 02/03/2012
- Field of study
Conservationists must develop new strategies and adapt existing tools to address the consequences of anthropogenic climate change. To support statewide climate change adaptation, we developed a framework for assessing climate change vulnerability of California's at-risk birds and integrating it into the existing California Bird Species of Special Concern list. We defined climate vulnerability as the amount of evidence that climate change will negatively impact a population. We quantified climate vulnerability by scoring sensitivity (intrinsic characteristics of an organism that make it vulnerable) and exposure (the magnitude of climate change expected) for each taxon. Using the combined sensitivity and exposure scores as an index, we ranked 358 avian taxa, and classified 128 as vulnerable to climate change. Birds associated with wetlands had the largest representation on the list relative to other habitat groups. Of the 29 state or federally listed taxa, 21 were also classified as climate vulnerable, further raising their conservation concern. Integrating climate vulnerability and California's Bird Species of Special Concern list resulted in the addition of five taxa and an increase in priority rank for ten. Our process illustrates a simple, immediate action that can be taken to inform climate change adaptation strategies for wildlife
Search for high-mass resonances decaying to dilepton final states in pp collisions at sâ=7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- 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 R
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TPA
- Akimoto G
- Akimov AV
- 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
- Allbrooke BMM
- 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
- 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
- Arce ATH
- Arfaoui S
- Arguin J-F
- Argyropoulos S
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnal V
- Arnault C
- 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
- Avramidou R
- Axen D
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker MD
- Baker OK
- Baker S
- Balek P
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Barrillon P
- 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 AK
- Becker S
- Beckingham M
- Becks KH
- Beddall A
- Beddall AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Beemster LJ
- Begel M
- Behera PK
- Beimforde M
- Belanger-Champagne C
- Belenguer MJ
- 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
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Berge D
- Berger N
- Berghaus F
- Berglund E
- Beringer J
- Bernat R
- 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
- Biscarat C
- Bittner B
- Black CW
- Black KM
- Blair RE
- Blanchard J-B
- Blanchot G
- Blazek T
- Bloch I
- Blocker C
- Blocki J
- Blonde A
- Blum W
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Boddy CR
- Boehler M
- Boek J
- Boelaert N
- 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 R
- 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
- Britton D
- Brochu FM
- Brock I
- Brock R
- Broggi F
- Bromberg C
- Bronner J
- Brooijmans G
- Brooks T
- Brooks WK
- Brown G
- Brown H
- Bruckman de Renstrom PA
- Bruncko D
- Bruneliere R
- Brunet S
- Bruni A
- Bruni G
- Bruschi M
- 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
- Butler B
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Byszewski M
- Cabrera Urban S
- Caforio D
- Cakir IT
- Cakir O
- Calafiura P
- Calderini G
- Calfayan P
- Calkins R
- Caloba LP
- Caloi R
- 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
- Capasso L
- Caprini I
- Caprini M
- Capriotti D
- Capua M
- Caputo R
- Cardarelli R
- Carli T
- Carlino G
- Carminati L
- Caron B
- Caron S
- Carquin E
- Carrillo-Montoya GD
- Carter AA
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Cascella M
- Caso C
- Castaneda Hernandez AM
- Castaneda-Miranda E
- Castanheira MTD
- Castillo IS
- Castillo LRF
- Castro NF
- Cataldi G
- Catastini R
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- Cavalcanti TP
- Cavaliere V
- Cavalleri P
- Cavalli D
- Cavalli-Sforza M
- Cavasinni 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
- Chareyre E
- 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 G
- Chikovani L
- Childers JT
- Chilingarov A
- Chiodini G
- 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
- Ciocca C
- Ciocio A
- Cirilli M
- Cirkovic R
- 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
- Cogneras E
- Colas J
- Cole S
- Colijn AP
- Collaboration A
- 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 T
- Corradi M
- Correia AMH
- Corriveau F
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Cote D
- Courneyea L
- Cowan G
- Cowden C
- 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
- Czyczula 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 W
- Dafinca A
- Dai T
- 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
- de Jong P
- De la Taille C
- De la Torre H
- de Lima DEF
- de Lima JGR
- De Lorenzi F
- de Mora L
- De Nooij L
- De Pedis D
- De Regie JBDV
- De Salvo A
- De Sanctis U
- De Santo A
- De Zorzi G
- De K
- Dearnaley WJ
- Debbe R
- Debenedetti C
- Dechenaux B
- Dedovich DV
- Degenhardt J
- Del Peso J
- Del Prete T
- Delemontex T
- Deliyergiyev M
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- della Porta GZ
- della Volpe D
- Delmastro M
- Delsart PA
- Deluca C
- Demers S
- Demichev M
- Demirkoz B
- Denis RDS
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Devetak E
- Deviveiros PO
- Dewhurst A
- DeWilde B
- Dhaliwal S
- Dhullipudi R
- Di Ciaccio A
- Di Ciaccio L
- Di Donato C
- Di Girolamo A
- Di Girolamo B
- Di Luise S
- Di Mattia A
- Di Micco B
- Di Nardo R
- Di Simone A
- Di Sipio R
- Diaz MA
- Diehl EB
- Dietrich J
- Dietzsch TA
- Diglio S
- Dingfelder J
- Dinut F
- Dionisi C
- Dita P
- Dita S
- Dittus F
- Djama F
- Djobava T
- do Vale MAB
- Doan TKO
- Dobbs M
- Dobos D
- Dobson E
- Dodd J
- Doglioni C
- Doherty T
- Dohmae T
- Doi Y
- Dolejsi J
- Dolenc I
- Dolezal Z
- Dolgoshein BA
- Donadelli M
- Donini J
- Donszelmann TC
- Dopke J
- Doria A
- Dos Anjos A
- Dos Santos DR
- Dotti A
- Dova MT
- Doxiadis AD
- Doyle AT
- Dressnandt N
- Dris M
- Dubbert J
- Dube S
- Duchovni E
- Duckeck G
- Duda D
- Dudarev A
- Dudziak F
- Duehrssen M
- Duerdoth IP
- Dueren M
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- Dufour M-A
- Duguid L
- Dunford M
- Duxfield R
- Dwuznik M
- Ebenstein WL
- Ebke J
- Eckweiler S
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- Edson W
- Edwards CA
- Edwards NC
- Ehrenfeld W
- Eifert T
- Eigen G
- Einsweiler K
- Eisenhandler E
- Ekelof T
- El Kacimi M
- El Moursli RC
- Ellert M
- Elles S
- Ellinghaus F
- Ellis K
- Ellis N
- Elmsheuser J
- Elsing M
- Emeliyanov D
- Engelmann R
- Engl A
- Epp B
- Erdmann J
- Ereditato A
- Eriksson D
- Ernst J
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- Ernwein J
- Errede D
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- Ertel E
- Escalier M
- Esch H
- Eschrich IG
- Escobar C
- Espinal Curull X
- Esposito B
- Etienne F
- Etienvre AI
- Etzion E
- Evangelakou D
- Evans H
- Fabbri L
- Fabre C
- Fajardo LSG
- Fakhrutdinov RM
- Falciano S
- Fang Y
- Fanti M
- Farbin A
- Farilla A
- Farley J
- Farooque T
- Farrell S
- Farrington SM
- Farthouat P
- Fassi F
- Fassnacht P
- Fassouliotis D
- Fatholahzadeh B
- Favareto A
- Fayard L
- Fazio S
- Febbraro R
- Federic P
- Fedin OL
- Fedorko W
- Fehling-Kaschek M
- Feligioni L
- Feng C
- Feng EJ
- Fenyuk AB
- Ferencei J
- Fernando W
- Ferrag S
- Ferrando BMS
- Ferrando J
- Ferrara V
- Ferrari A
- Ferrari P
- Ferrari R
- Ferrer A
- Ferrere D
- Ferretti C
- Fiascaris M
- Fiedler F
- Filipcic A
- Filthaut F
- Fincke-Keeler M
- Fiolhais MCN
- Fiorini L
- Firan A
- Fischer G
- Fisher MJ
- Flechl M
- Fleck I
- Fleckner J
- Fleischmann P
- Fleischmann S
- Flick T
- Floderus A
- Flowerdew MJ
- Formica A
- Forti A
- Fortin D
- Fournier D
- Fowler AJ
- Fox H
- Francavilla P
- Franchini M
- Franchino S
- Francis D
- Frank T
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- Franz S
- Fraternali M
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- Fukunaga C
- Fulsom BG
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- Gadomski S
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- Gallop BJ
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- Glitza KW
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- Goessling C
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- Goodson JJ
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- Grancagnolo F
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- Grassi V
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- Greenshaw T
- Greenwood ZD
- Gregersen K
- Gregor IM
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- Guicheney C
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- Hadley DR
- Haefner P
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- Hajduk Z
- Hakobyan H
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- Harvey A
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- Hasegawa Y
- Hassani S
- Haug S
- Hauschild M
- Hauser R
- Havranek M
- Hawkes CM
- Hawkings RJ
- Hawkins AD
- Hayakawa T
- Hayashi T
- Hayden D
- Hays CP
- Hayward HS
- Haywood SJ
- Head SJ
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- Heim S
- Heinemann B
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- Heller M
- Hellman S
- Hellmich D
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- Henderson RCW
- Henke M
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- Hensel C
- Hernandez Jimenez Y
- Hernandez CM
- Hernandez DP
- Herrberg R
- Herrera CM
- Herten G
- Hertenberger R
- Hervas L
- Hesketh GG
- Hessey NP
- Higon-Rodriguez E
- Hill JC
- Hiller KH
- Hillert S
- Hillier SJ
- Hinchliffe I
- Hines E
- Hirose M
- Hirsch F
- Hirschbuehl D
- Hobbs J
- Hod N
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- Zobernig G
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- zur Nedden M
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- 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 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
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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- Yamauchi K
- Yamazaki T
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- Yang UK
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- Yanush S
- Yao L
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- Yen AL
- Yilmaz M
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- Yorita K
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- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
- Yu DR
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- ZeniĆĄ T
- Zerwas D
- Zevi Della Porta G
- Zhang D
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- ZivkoviÄ L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (ÎÏ) and pseudorapidity (Îη) are measured in âsNN=5.02ââTeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1ââÎŒb-1 of data as a function of transverse momentum (pT) and the transverse energy (ÎŁETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Îη|<5) ânear-sideâ (ÎÏâŒ0) correlation that grows rapidly with increasing ÎŁETPb. A long-range âaway-sideâ (ÎÏâŒÏ) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ÎŁETPb, is found to match the near-side correlation in magnitude, shape (in Îη and ÎÏ) and ÎŁETPb dependence. The resultant ÎÏ correlation is approximately symmetric about Ï/2, and is consistent with a dominant cosâĄ2ÎÏ modulation for all ÎŁETPb ranges and particle pT
Search for R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
- 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
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- 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 the neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
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- Abdallah J
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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
Search for direct production of charginos and neutralinos in events with three leptons and missing transverse momentum in âs=7 TeV pp collisions with the ATLAS detector
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- Ab FR
- Abajyan T
- Abbott B
- Abdallah J
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- Abdinov O
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- Abreu H
- Acharya BS
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- Aharrouche M
- Ahlen SP
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
A search for the direct production of charginos and neutralinos in final states with three electrons or muons and missing transverse momentum is presented. The analysis is based on 4.7 fb(-1) of root s = 7 TeV proton-proton collision data delivered by the Large Hadron Collider and recorded with the ATLAS detector. Observations are consistent with Standard Model expectations in three signal regions that are either depleted or enriched in Z-boson decays. Upper limits at 95% confidence level are set in R-parity conserving phenomenological minimal supersymmetric models and in simplified models, significantly extending previous results. (C) 2012 CERN. Published by Elsevier B.V. All rights reserved
Search for direct production of charginos and neutralinos in events with three leptons and missing transverse momentum in âs=7 TeV pp collisions with the ATLAS detector
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- Abajyan T
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- Abdallah J
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- Publication venue
- Physics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics
- Publication date
- 01/01/2012
- Field of study
A search for the direct production of charginos and neutralinos in final
states with three electrons or muons and missing transverse momentum is
presented. The analysis is based on 4.7 fb-1 of sqrt(s) = 7 TeV proton-proton
collision data delivered by the Large Hadron Collider and recorded with the
ATLAS detector. Observations are consistent with Standard Model expectations in
three signal regions that are either depleted or enriched in Z-boson decays.
Upper limits at 95% confidence level are set in R-parity conserving
phenomenological minimal supersymmetric models and in simplified models,
significantly extending previous results
Search for light top squark pair production in final states with leptons and b -jets with the ATLAS detector in sâ=7 TeV proton-proton collisions
- Author
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- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
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- Publication venue
- Publication date
- 01/01/2012
- Field of study
The results of a search for pair production of light top squarks are presented, using 4.7 fb^-1 of sqrt(s) = 7 TeV proton-proton collisions collected with the ATLAS detector at the Large Hadron Collider. This search targets top squarks with masses similar to, or lighter than, the top quark mass. Final states containing exclusively one or two leptons (e, mu), large missing transverse momentum, light-jets and b-jets are used to reconstruct the top squark pair system. Global mass scale variables are used to separate the signal from a large ttbar background. No excess over the Standard Model expectations is found. The results are interpreted in the framework of the Minimal Supersymmetric Standard Model, assuming the top squark decays exclusively to a chargino and a b-quark. Light top squarks with masses between 123-167 GeV are excluded for neutralino masses around 55 GeV
Search for long-lived, heavy particles in final states with a muon and multi-track displaced vertex in protonâproton collisions at √<span style="text-decoration:overline">s</span>=7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- 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
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- Publication venue
- Elsevier
- Publication date
- 01/01/2013
- Field of study
Many extensions of the Standard Model posit the existence of heavy particles with long lifetimes. In this Letter, results are presented of a search for events containing one or more such particles, which decay at a significant distance from their production point, using a final state containing charged hadrons and an associated muon. This analysis uses a data sample of protonâproton collisions at √s=7 TeV corresponding to an integrated luminosity of 4.4 fbâ1 collected in 2011 by the ATLAS detector operating at the Large Hadron Collider. Results are interpreted in the context of R-parity violating supersymmetric scenarios. No events in the signal region are observed and limits are set on the production cross section for pair production of supersymmetric particles, multiplied by the square of the branching fraction for a neutralino to decay to charged hadrons and a muon, based on the scenario where both of the produced supersymmetric particles give rise to neutralinos that decay in this way. However, since the search strategy is based on triggering on and reconstructing the decay products of individual long-lived particles, irrespective of the rest of the event, these limits can easily be reinterpreted in scenarios with different numbers of long-lived particles per event. The limits are presented as a function of neutralino lifetime, and for a range of squark and neutralino masses
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