200 research outputs found
IR Sounder Small Satellite for Polar Orbit Weather Measurements
- Publication venue
- DigitalCommons@USU
- Publication date
- 13/08/2015
- Field of study
The National Environmental Satellite, Data, and Information Service (NESDIS) acquires and manages the Nation\u27s operational environmental satellites. NESDIS environmental satellite observations support a variety of civil and military environmental monitoring missions, including weather and climate prediction. A key input to weather forecast and climate models are atmospheric sounder observations from polar-orbiting satellites. These satellites are traditionally large, complex, and expensive, and take several years to design and build. The community must look for ways to reduce the cost and complexity of environmental satellites while meeting weather and climate sensing needs. This paper describes a new IR sounder concept that significantly reduces the size, mass, complexity, and consequent costs. This is accomplished through higher spectral resolution and the use of new large-area focal plane arrays, combined with novel dispersive optical design. In this design, one spectrometer with one FPA is required to perform both temperature and humidity sounding by imaging both bands onto the same FPA with an order sorting filter to separate the two bands. This paper details the design of the sensor and validation of sensor noise performance. Additionally, a thermal and spacecraft design are discussed to show the feasibility of a small-satellite scale instrument
Quantum phase transitions of light
- Author
- A Albus
- A Imamoğlu
- A Wallraff
- AD Greentree
- AD Greentree
- AD Greentree
- Andrew D. Greentree
- B-S Song
- C Cohen-Tannoudji
- Charles Tahan
- D Jaksch
- D van Oosten
- D van Oosten
- DN Jamieson
- DS Rokhsar
- E Ozbay
- ET Jaynes
- F Illuminati
- H Altug
- H Fehrmann
- Jared H. Cole
- JM Kosterlitz
- JW Baldwin
- K Sheshadri
- KM Birnbaum
- Lloyd C. L. Hollenberg
- M Cramer
- M Freedman
- M Greiner
- M Lewenstein
- M Trupke
- M Weidinger
- MPA Fisher
- P Grangier
- P Olivero
- PA Lee
- PB Littlewood
- Ph Tamarat
- RJ Lang
- S Rebić
- S Tomljenovic-Hanic
- V Hussin
- VW Scarola
- W Krauth
- W Krauth
- W Krauth
- ZW Xie
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2006
- Field of study
Recently, condensed matter and atomic experiments have reached a length-scale
and temperature regime where new quantum collective phenomena emerge. Finding
such physics in systems of photons, however, is problematic, as photons
typically do not interact with each other and can be created or destroyed at
will. Here, we introduce a physical system of photons that exhibits strongly
correlated dynamics on a meso-scale. By adding photons to a two-dimensional
array of coupled optical cavities each containing a single two-level atom in
the photon-blockade regime, we form dressed states, or polaritons, that are
both long-lived and strongly interacting. Our zero temperature results predict
that this photonic system will undergo a characteristic Mott insulator
(excitations localised on each site) to superfluid (excitations delocalised
across the lattice) quantum phase transition. Each cavity's impressive photon
out-coupling potential may lead to actual devices based on these quantum
many-body effects, as well as observable, tunable quantum simulators. We
explicitly show that such phenomena may be observable in micro-machined diamond
containing nitrogen-vacancy colour centres and superconducting microwave
strip-line resonators.Comment: 11 pages, 5 figures (2 in colour
Analysis of Soil Freeze/Thaw Signatures During Slapex F/T Campaign
- Author
- Publication venue
- Publication date
- Field of study
Permanently frozen and seasonally frozen soils occur over a large portion of the Earth's land surface. Changes in the freeze/thaw state of the land surface reflects major changes in thermal and hydraulic properties as well as acting as a "switch" for many ecological processes. In short, soil freeze/thaw state is a fundamental land surface variable in the water and energy cycles, and it connects to the carbon cycle. Surface freeze/thaw state is observable by passive and active microwave sensors. For example, NASA's Soil Moisture Active Passive (SMAP) mission includes a freeze/thaw data product. Such satellite sensing offers routine all-season and all-weather global observations of soil freeze/thaw state with the application of suitable algorithms. We describe early finding from the SLAPex Freeze/Thaw campaign, believed to be the first airborne campaign of its type, focusing on soil freeze/thaw
Exo-C: a probe-scale space observatory for direct imaging and spectroscopy of extrasolar planetary systems
- Author
- Belikov Ruslan
- Brenner Michael P.
- Brugarolas Paul B.
- Bryden Geoffrey
- Cahoy Kerri
- Chakrabarti Supriya
- Dekens Frank G.
- Dubovitsky Serge
- Effinger Robert T.
- Hirsch Brian
- Kissil Andrew
- Krist John E.
- Lang Jared J.
- Marley Mark S.
- McElwain Michael W.
- Meadows Victoria S.
- Nissen Joel
- Oseas Jeffrey M.
- Pong Chris
- Serabyn Eugene
- Stapelfeldt Karl R.
- Sunada Eric
- Trauger John T.
- Unwin Stephen C.
- Warfield Keith R.
- Publication venue
- 'SPIE-Intl Soc Optical Eng'
- Publication date
- 16/03/2018
- Field of study
"Exo-C" is NASAs first community study of a modest aperture space telescope mission that is optimized for high contrast observations of exoplanetary systems. The mission will be capable of taking optical spectra of nearby exoplanets in reflected light, discovering previously undetected planets, and imaging structure in a large sample of circumstellar disks. It will obtain unique science results on planets down to super-Earth sizes and serve as a technology pathfinder toward an eventual flagship-class mission to find and characterize habitable Earth-like exoplanets. We present the mission/payload design and highlight steps to reduce mission cost/risk relative to previous mission concepts. Key elements are an unobscured telescope aperture, an internal coronagraph with deformable mirrors for precise wavefront control, and an orbit and observatory design chosen for high thermal stability. Exo-C has a similar telescope aperture, orbit, lifetime, and spacecraft bus requirements to the highly successful Kepler mission (which is our cost reference). Much of the needed technology development is being pursued under the WFIRST coronagraph study and would support a mission start in 2017, should NASA decide to proceed. This paper summarizes the study final report completed in March 2015.United States. National Aeronautics and Space Administration. Astrophysics Divisio
Exo-C: a probe-scale space observatory for direct imaging and spectroscopy of extrasolar planetary systems
- Author
- Belikov Ruslan
- Brenner Michael P.
- Brugarolas Paul B.
- Bryden Geoffrey
- Cahoy Kerri L.
- Chakrabarti Supriya
- Dekens Frank G.
- Dubovitsky Serge
- Effinger Robert T.
- Hirsch Brian
- Kissil Andrew
- Krist John E.
- Lang Jared J.
- Marley Mark S.
- McElwain Michael W.
- Meadows Victoria S.
- Nissen Joel
- Oseas Jeffrey M.
- Pong Chris
- Serabyn Eugene
- Stapelfeldt Karl R.
- Sunada Eric
- Trauger John T.
- Unwin Stephen C.
- Warfield Keith R.
- Publication venue
- Society of Photo-optical Instrumentation Engineers (SPIE)
- Publication date
- 16/09/2015
- Field of study
"Exo-C" is NASAs first community study of a modest aperture space telescope mission that is optimized for high contrast observations of exoplanetary systems. The mission will be capable of taking optical spectra of nearby exoplanets in reflected light, discovering previously undetected planets, and imaging structure in a large sample of circumstellar disks. It will obtain unique science results on planets down to super-Earth sizes and serve as a technology pathfinder toward an eventual flagship-class mission to find and characterize habitable Earth-like exoplanets. We present the mission/payload design and highlight steps to reduce mission cost/risk relative to previous mission concepts. Key elements are an unobscured telescope aperture, an internal coronagraph with deformable mirrors for precise wavefront control, and an orbit and observatory design chosen for high thermal stability. Exo-C has a similar telescope aperture, orbit, lifetime, and spacecraft bus requirements to the highly successful Kepler mission (which is our cost reference). Much of the needed technology development is being pursued under the WFIRST coronagraph study and would support a mission start in 2017, should NASA decide to proceed. This paper summarizes the study final report completed in March 2015
Observation of associated near-side and away-side long-range correlations in √sNN=5.02 TeV proton-lead collisions with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdel Khalek S
- Abdelalim AA
- Abdinov O
- Aben R
- Abi B
- Abolins M
- Abouzeid OS
- 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
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
- Alam MA
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Allbrooke BM
- Allison LJ
- Allport PP
- Allwood-Spiers SE
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alonso F
- Altheimer A
- Alvarez Gonzalez B
- 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
- 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
- Aperio Bella L
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce AT
- Arfaoui S
- Arguin JF
- 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
- Astalos R
- Astbury A
- Atkinson M
- ATLAS Collaboration The
- Auerbach B
- Auge E
- Augsten K
- Aurousseau M
- Avolio G
- Axen D
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Backus Mayes J
- Badescu E
- Bagnaia P
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker OK
- Baker S
- Balek P
- Balli F
- 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 M
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro Guimarães da Costa J
- Barreiro F
- 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
- Beermann TA
- Begel M
- Behar Harpaz S
- Belanger-Champagne C
- Bell PJ
- Bell WH
- Bella G
- Bellagamba L
- Bellomo M
- Belloni A
- Beloborodova O
- Belotskiy K
- Beltramello O
- Benary O
- Benchekroun D
- Bendtz K
- Benekos N
- Benhammou Y
- Benhar Noccioli E
- Benitez Garcia JA
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Berge D
- Bergeaas Kuutmann E
- Berger N
- Berghaus F
- Berglund E
- Beringer J
- Bernat P
- Bernhard R
- Bernius C
- Bernlochner FU
- 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 JE
- Black KM
- Blair RE
- Blanchard JB
- 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
- Boelaert N
- 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
- Boutouil S
- 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
- Bruckman de Renstrom PA
- 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
- Bugge L
- Bulekov O
- Bundock AC
- Bunse M
- Buran T
- Burckhart H
- Burdin S
- Burgess T
- Burke S
- Busato E
- Bussey P
- Buszello CP
- Butler B
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Byszewski M
- Büscher V
- Cabrera Urbán S
- Caforio D
- Cakir O
- Calafiura P
- Calderini G
- Calfayan P
- Calkins R
- Caloba LP
- Caloi R
- Calvet D
- Calvet S
- Camacho Toro R
- Camarri P
- Cameron D
- Caminada LM
- Caminal Armadans R
- Campana S
- Campanelli M
- Canale V
- Canelli F
- Canepa A
- Cantero J
- Cantrill R
- Cao T
- Capeans Garrido MD
- 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
- Castillo Gimenez V
- Castro NF
- Cataldi G
- Catastini P
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- 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
- Charlton DG
- Chavda V
- Chavez Barajas CA
- Cheatham S
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen S
- Chen X
- Chen Y
- Cheng Y
- Cheplakov A
- Cherkaoui El Moursli R
- 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
- Chow BK
- Christidi IA
- Christov A
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Ciapetti G
- Ciftci AK
- Ciftci R
- Cinca D
- Cindro V
- Ciocio A
- Cirilli M
- 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
- Coffey L
- Cogan JG
- Coggeshall J
- Colas J
- Cole B
- Cole S
- Colijn AP
- Collins NJ
- Collins-Tooth C
- Collot J
- Colombo T
- Colon G
- Compostella G
- Conde Muiño 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
- Corriveau F
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Cottin G
- Courneyea L
- Cowan G
- Cox BE
- Cranmer K
- Crescioli F
- Cristinziani M
- Crosetti G
- Crépé-Renaudin S
- Cuciuc CM
- Cuenca Almenar C
- Cuhadar Donszelmann T
- Cummings J
- Curatolo M
- Curtis CJ
- Cuthbert C
- Cwetanski P
- Czirr H
- Czodrowski P
- Czyczula Z
- Côté D
- D'Auria S
- D'Onofrio M
- D'Orazio A
- Da Cunha Sargedas De Sousa MJ
- Da Via C
- Dabrowski W
- Dafinca A
- Dai T
- Dallaire F
- Dallapiccola C
- Dam 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 Lorenzi F
- De Nooij L
- De Pedis D
- De Salvo A
- De Sanctis U
- De Santo A
- De Vivie De Regie JB
- 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 Volpe D
- Delmastro M
- Delsart PA
- Deluca C
- Demers S
- Demichev M
- Demirkoz B
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- 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
- Dindar Yagci K
- Dingfelder J
- Dinut F
- Dionisi C
- Dita P
- Dita S
- Dittus F
- Djama F
- Djobava T
- do Vale MA
- Do Valle Wemans A
- Doan TK
- Dobbs M
- Dobos D
- Dobson E
- Dodd J
- Doglioni C
- Doherty T
- Dohmae T
- Doi Y
- Dolejsi J
- Dolezal Z
- Dolgoshein BA
- Donadelli M
- Donini J
- Dopke J
- Doria A
- Dos Anjos A
- Dotti A
- Dova MT
- Doyle AT
- Dressnandt N
- Dris M
- Dubbert J
- Dube S
- Dubreuil E
- Duchovni E
- Duckeck G
- Duda D
- Dudarev A
- Dudziak F
- Duerdoth IP
- Duflot L
- Dufour MA
- Duguid L
- Dunford M
- Duran Yildiz H
- Duxfield R
- Dwuznik M
- Dührssen M
- Düren M
- Ebenstein WL
- Ebke J
- Eckweiler S
- Edson W
- Edwards CA
- Edwards NC
- Ehrenfeld W
- 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
- Emeliyanov D
- Engelmann R
- Engl A
- Epp B
- Erdmann J
- Ereditato A
- Eriksson D
- Ernst J
- Ernst M
- Ernwein J
- Errede D
- Errede S
- Ertel E
- Escalier M
- Esch H
- Escobar C
- Espinal Curull X
- Esposito B
- Etienne F
- Etienvre AI
- Etzion E
- Evangelakou D
- Evans H
- Fabbri L
- Fabre C
- Facini GJ
- 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
- Federic P
- Fedin OL
- Fedorko W
- Fehling-Kaschek M
- Feligioni L
- Feng C
- Feng EJ
- Fenyuk AB
- Ferencei J
- Fernando W
- Ferrag S
- Ferrando J
- Ferrara V
- Ferrari A
- Ferrari P
- Ferrari R
- Ferreira de Lima DE
- Ferrer A
- Ferrere D
- Ferretti C
- Ferretto Parodi A
- Fiascaris M
- Fiedler F
- Filipčič A
- Filthaut F
- Fincke-Keeler M
- Fiolhais MC
- Fiorini L
- Firan A
- Fischer J
- Fisher MJ
- Fitzgerald EA
- Flechl M
- Fleck I
- Fleischmann P
- Fleischmann S
- Fletcher G
- Fletcher GT
- Flick T
- Floderus A
- Flores Castillo LR
- Florez Bustos AC
- Flowerdew MJ
- Fonseca Martin T
- Formica A
- Forti A
- Fortin D
- Fournier D
- Fowler AJ
- Fox H
- Francavilla P
- Franchini M
- Franchino S
- Francis D
- Frank T
- Franklin M
- Franz S
- Fraternali M
- Fratina S
- French ST
- Friedrich C
- Friedrich F
- Froidevaux D
- Frost JA
- Fukunaga C
- Fullana Torregrosa E
- Fulsom BG
- Fuster J
- Gabaldon C
- Gabizon O
- Gadatsch S
- Gadfort T
- Gadomski S
- Gagliardi G
- Gagnon P
- Galea C
- Galhardo B
- Gallas EJ
- Gallo V
- Gallop BJ
- Gallus P
- Gan KK
- Gandrajula RP
- Gao YS
- Gaponenko A
- Garay Walls FM
- Garberson F
- Garcia-Sciveres M
- García Navarro JE
- García C
- Gardner RW
- Garelli N
- Garonne V
- Gatti C
- Gaudio G
- Gaur B
- Gauthier L
- Gauzzi P
- Gavrilenko IL
- Gay C
- Gaycken G
- Gazis EN
- Ge P
- Gecse Z
- Gee CN
- Geerts DA
- Geich-Gimbel CH
- Gellerstedt K
- Gemme C
- Gemmell A
- Genest MH
- Gentile S
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- Wooden G
- Wosiek BK
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- Wozniak KW
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- Xella S
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- Yacoob S
- Yamada M
- Yamaguchi H
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamanaka T
- Yamauchi K
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yen AL
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
- Yu DR
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- Zeniš 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
- Zivković 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 (Δϕ) and pseudorapidity (Δη) are measured in √sNN=5.02 TeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1 μb-1 of data as a function of transverse momentum (pT) and the transverse energy (ΣETPb) 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<|Δη|<5) “near-side” (Δϕ∼0) correlation that grows rapidly with increasing ΣETPb. A long-range “away-side” (Δϕ∼π) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ΣETPb, is found to match the near-side correlation in magnitude, shape (in Δη and Δϕ) and ΣETPb dependence. The resultant Δϕ correlation is approximately symmetric about π/2, and is consistent with a dominant cos2Δϕ modulation for all ΣETPb ranges and particle pT
Measurement of χ c1 and χ c2 production with s√ = 7 TeV pp collisions at ATLAS
- Author
- A Abulencia
- A. A. Carter
- A. A. Grillo
- A. A. Komar
- A. A. Korol
- A. A. Minaenko
- A. A. Nepomuceno
- A. A. Snesarev
- A. A. Solodkov
- A. A. Talyshev
- A. Ahmad
- A. Aloisio
- A. Alonso
- A. Altheimer
- A. Amorim
- A. Andreazza
- A. Angerami
- A. Annovi
- A. Antonaki
- A. Antonov
- A. Artamonov
- A. Astbury
- A. B. Fenyuk
- A. Bangert
- A. Baroncelli
- A. Bassalat
- A. Basye
- A. Beddall
- A. Bellerive
- A. Belloni
- A. Bingul
- A. Bocci
- A. Bogouch
- A. Borisov
- A. Boveia
- A. Brandt
- A. Bruni
- A. Buzatu
- A. C. Bundock
- A. C. Daniells
- A. C. Florez Bustos
- A. C. König
- A. C. Martyniuk
- A. C. Schaffer
- A. Canepa
- A. Castelli
- A. Catinaccio
- A. Cattai
- A. Cerri
- A. Cervelli
- A. Chafaq
- A. Cheplakov
- A. Chilingarov
- A. Chitan
- A. Ciocio
- A. Clark
- A. Coccaro
- A. Corso-Radu
- A. Cortes-Gonzalez
- A. D. Hawkins
- A. D. Pilkington
- A. Dafinca
- A. De Salvo
- A. De Santo
- A. Dell’Acqua
- A. Demilly
- A. Dewhurst
- A. Di Ciaccio
- A. Di Domenico
- A. Di Girolamo
- A. Di Mattia
- A. Di Simone
- A. Do Valle Wemans
- A. Doria
- A. Dos Anjos
- A. Dotti
- A. Dudarev
- A. D’Orazio
- A. E. Barton
- A. E. Kiryunin
- A. E. Loevschall-Jensen
- A. Ereditato
- A. F. Saavedra
- A. Farbin
- A. Farilla
- A. Favareto
- A. Ferrari
- A. Ferrer
- A. Ferretto Parodi
- A. Filipčič
- A. Firan
- A. Floderus
- A. Formica
- A. Forti
- A. G. Bogdanchikov
- A. G. Buckley
- A. G. Goussiou
- A. G. Leister
- A. G. Myagkov
- A. G. Olchevski
- A. Gabrielli
- A. Gabrielli
- A. Gemmell
- A. Gershon
- A. Glazov
- A. Gomes
- A. Gorišek
- A. Grohsjean
- A. Haas
- A. Hamilton
- A. Harvey
- A. Henrichs
- A. Hoecker
- A. Hoummada
- A. Huettmann
- A. I. Butt
- A. I. Etienvre
- A. I. Mincer
- A. Irles Quiles
- A. J. Armbruster
- A. J. Barr
- A. J. Beddall
- A. J. Lankford
- A. J. Lowe
- A. J. Tanasijczuk
- A. Jinaru
- A. Juste Rozas
- A. K. Ciftci
- A. K. Kopp
- A. K. Morley
- A. Kaczmarska
- A. Kapliy
- A. Kastanas
- A. Katre
- A. Khanov
- A. Khodinov
- A. Khomich
- A. Khoroshilov
- A. Klimentov
- A. Knue
- A. Korn
- A. Kotwal
- A. Koutsman
- A. Krasznahorkay
- A. Kravchenko
- A. Kruse
- A. Kugel
- A. Kupco
- A. L. Maslennikov
- A. L. Read
- A. L. S. Schorlemmer
- A. L. Yen
- A. La Rosa
- A. Lanza
- A. Larner
- A. Lehan
- A. Lewis
- A. Limosani
- A. Lipniacka
- A. Lister
- A. Lleres
- A. Loginov
- A. Lounis
- A. Lucotte
- A. M. Bach
- A. M. Cooper-Sarkar
- A. M. Henriques Correia
- A. M. Leyko
- A. M. Litke
- A. M. Nairz
- A. M. Soukharev
- A. M. Zaitsev
- A. Macchiolo
- A. Madsen
- A. Maio
- A. Manfredini
- A. Mann
- A. Manousakis-Katsikakis
- A. Marzin
- A. Mastroberardino
- A. McCarn
- A. Meade
- A. Mehta
- A. Mengarelli
- A. Messina
- A. Milov
- A. Molfetas
- A. Moraes
- A. N. Karyukhin
- A. N. Sisakyan
- A. N. Tuna
- A. Nagarkar
- A. Napier
- A. Negri
- A. Nelson
- A. Neusiedl
- A. Nikiforov
- A. Nisati
- A. Ochi
- A. Oh
- A. Olariu
- A. Olszewski
- A. Onofre
- A. Ouraou
- A. Ovcharova
- A. P. Colijn
- A. Pacheco Pages
- A. Palma
- A. Paramonov
- A. Passeri
- A. Petridis
- A. Picazio
- A. Pinder
- A. Pingel
- A. Policicchio
- A. Polini
- A. Poppleton
- A. Pranko
- A. Quadt
- A. R. Davison
- A. R. Gillman
- A. R. Stradling
- A. R. Weidberg
- A. Redelbach
- A. Reinsch
- A. Renaud
- A. Rimoldi
- A. Robichaud-Veronneau
- A. Robson
- A. Romaniouk
- A. Rose
- A. Rozanov
- A. Ruiz-Martinez
- A. Ruschke
- A. S. Boldyrev
- A. S. Cerqueira
- A. S. Chisholm
- A. S. Hard
- A. S. Kozhin
- A. S. Mete
- A. S. Randle-Conde
- A. S. Thompson
- A. Saddique
- A. Salamon
- A. Salnikov
- A. Salvucci
- A. Salzburger
- A. Sanchez
- A. Sansoni
- A. Sapronov
- A. Sbrizzi
- A. Schaelicke
- A. Schoening
- A. Schwartzman
- A. Seiden
- A. Sfyrla
- A. Shmeleva
- A. Sidoti
- A. Sircar
- A. Soffer
- A. Sood
- A. Straessner
- A. Strandlie
- A. Succurro
- A. T. Doyle
- A. T. Goshaw
- A. T. H. Arce
- A. T. Watson
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- T Sjöstrand
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- X. Chen
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- X. Hu
- X. Ju
- X. Lei
- X. Li
- X. Lou
- X. Portell Bueso
- X. Prudent
- X. Ruan
- X. S. Anduaga
- X. Sun
- X. Wang
- X. Wu
- X. Zhang
- X. Zhuang
- Y-Q Ma
- Y-Q Ma
- Y. A. Kurochkin
- Y. Abulaiti
- Y. Amaral Coutinho
- Y. Arai
- Y. Azuma
- Y. B. Pan
- Y. Bai
- Y. Benhammou
- Y. Chen
- Y. Cheng
- Y. Coadou
- Y. Davygora
- Y. Enari
- Y. F. Ryabov
- Y. Fang
- Y. Hasegawa
- Y. Hernández Jiménez
- Y. Huang
- Y. Ikegami
- Y. Inamaru
- Y. J. Schnellbach
- Y. Jiang
- Y. Kataoka
- Y. Komori
- Y. Kulchitsky
- Y. Liu
- Y. Makida
- Y. Ming
- Y. Munwes
- Y. Nagai
- Y. Nagasaka
- Y. Nakahama
- Y. Ninomiya
- Y. Okumura
- Y. Oren
- Y. Pylypchenko
- Y. Rozen
- Y. S. Gao
- Y. Sakurai
- Y. Sasaki
- Y. Silver
- Y. Smirnov
- Y. Sugaya
- Y. Suzuki
- Y. Takahashi
- Y. Takubo
- Y. Tayalati
- Y. Unno
- Y. V. Grishkevich
- Y. Wu
- Y. Yamaguchi
- Y. Yamazaki
- Y. Yang
- Y. Yasu
- Y. Zhu
- Yu. A. Tikhonov
- Z. Czyczula
- Z. D. Greenwood
- Z. Dolezal
- Z. Gecse
- Z. H. Citron
- Z. Hajduk
- Z. Hubacek
- Z. J. Grout
- Z. Kohout
- Z. L. Ren
- Z. Liang
- Z. Marshall
- Z. Rurikova
- Z. V. Krumshteyn
- Z. Vykydal
- Z. Weng
- Z. Yan
- Z. Zhang
- Z. Zhao
- Z. Zinonos
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The prompt and non-prompt production cross-sections for the χ c1 and χ c2 charmonium states are measured in pp collisions at s√ = 7 TeV with the ATLAS detector at the LHC using 4.5 fb−1 of integrated luminosity. The χ c states are reconstructed through the radiative decay χ c → J/ψγ (with J/ψ → μ + μ −) where photons are reconstructed from γ → e + e − conversions. The production rate of the χ c2 state relative to the χ c1 state is measured for prompt and non-prompt χ c as a function of J/ψ transverse momentum. The prompt χ c cross-sections are combined with existing measurements of prompt J/ψ production to derive the fraction of prompt J/ψ produced in feed-down from χ c decays. The fractions of χ c1 and χ c2 produced in b-hadron decays are also measured
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
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- Wooden G
- Wosiek BK
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- Yen AL
- Yilmaz M
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- Yorita K
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- Yoshihara K
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- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
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- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- 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
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- zur Nedden M
- Zutshi V
- Zwalinski L
- 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 R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
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- Abajyan T
- Abbott B
- Abdallah J
- Khalek SA
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- Yilmaz M
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- Zerwas D
- della Porta GZ
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- Zhemchugov A
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- Zimmermann R
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- Zimmermann S
- Ziolkowski M
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- 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
- Author
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- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdinov O
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- Yanush S
- Yao L
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- Yilmaz M
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- Yoshihara K
- Young C
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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 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
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