8 research outputs found
Second-order semi-implicit projection methods for micromagnetics simulations
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2019
- Field of study
Micromagnetics simulations require accurate approximation of the magnetiza- tion dynamics described by the Landau-Lifshitz-Gilbert equation, which is non- linear, nonlocal, and has a non-convex constraint, posing interesting challenges in developing numerical methods. In this paper, we propose two second-order semi-implicit projection methods based on the second-order backward differen- tiation formula and the second-order interpolation formula using the informa- tion at previous two temporal steps. Unconditional unique solvability of both methods is proved, with their second-order accuracy verified through numerical examples in both 1D and 3D. The efficiency of both methods is compared to that of another two popular methods. In addition, we test the robustness of both methods for the first benchmark problem with a ferromagnetic thin film material from National Institute of Standards and Technology
Reinforced and superinsulating silica aerogel through in situ cross-linking with silane terminated prepolymers
- Author
- Publication venue
- Publication date
- 08/06/2018
- Field of study
Silica aerogels have only half the thermal conductivity of conventional insulation, but their application potential is limited by the poor mechanical properties. The fragility arises from the thin necks between the silica nanoparticle building blocks. Here, we produce strong silica aerogels through co-gelation of the polyethoxydisiloxane precursor with a variety of silane terminated prepolymers that reinforce the inter- particle necks, followed by hydrophobization and supercritical CO2 drying. All prepolymers enabled the synthesis of aerogels with excellent thermal and mechanical properties, but the shortest prepolymer (∼2–3 nm long) yielded the best results. The hybrid aerogels can sustain uniaxial compression without brittle rupture to at least 80% strain for all prepolymer concentrations (5–50 wt%), leading to a final strength of up to 21 MPa, an E modulus up to 3.4 MPa, and an up to 400 times lower dust release rate. In contrast to classical reinforcement strategies, the mechanical improvement does not come with a penalty in thermal conductivity, which remains between 14 and 17 mW m−1 K−1. The hybrid aerogels are a unique class of superinsulating materials with superior thermal and mechanical properties and a scalable production process
Off-line Evaluation of Indoor Positioning Systems in Different Scenarios: The Experiences from IPIN 2020 Competition
- Author
- Antsfeld L
- Asai Y
- Bao L
- Barsocchi P
- Chen B
- Chen R
- Chidlovskii B
- Chien Y-R
- Costa A
- Crivello A
- De Cock C
- Dong Y
- Dzama J
- Fan Y
- Fang S-H
- Fukatani N
- Fukushima Y
- Ge W
- Girolami M
- Gu Z
- Hayashida N
- Huang C
- Huang L
- Hung C-H
- Ichikari R
- Ji X
- Jiang H
- Jie Y-C
- Jimenez AR
- Jin G
- Kaichi T
- Kram S
- Kuang J
- Kurata T
- Lee N-T
- Leep BS
- Li H
- Li W
- Li Y
- Lim BZ
- Liu T
- Liu Y
- Liue X
- Luo H
- Ma C
- Meneses F
- Moreira A
- Mutschler C
- Nagae S
- Nagata Y
- Nicolau MJ
- Niu X
- Oh HL
- Ohta N
- Opiela M
- Ortiz M
- Palumbo F
- Pendao C
- Peng A
- Perez-Navarro A
- Plets D
- Poslad S
- Potorti F
- Quezada-Gaibor D
- Renaudin V
- Seco F
- Selviah DR
- Shimomura R
- Silva I
- Stahlke M
- Teo WJ
- Torres-Sospedra J
- Urano K
- Wang Y
- Wangd W
- Wangh Q
- Wei D
- Wei D
- Wei D
- Wei D
- Wu Y
- Wu Z
- Wub B
- Xia M
- Xie D
- Xiong H
- Xu S
- Yamaguchi M
- Yan D
- Yang C
- Yean S
- Yonamoto Y
- Yoshida T
- Young S-R
- Yu Y
- Yua C-C
- Yuan H
- Yuj C-A
- Zhang L
- Zhang W
- Zhangc W
- Zhangi P
- Zhao F
- Zheng L
- Zhou B
- Zhu N
- Publication venue
- 'Institute of Electrical and Electronics Engineers (IEEE)'
- Publication date
- 01/01/2021
- Field of study
Every year, for ten years now, the IPIN competition has aimed at evaluating real-world indoor localisation systems by testing them in a realistic environment, with realistic movement, using the EvAAL framework. The competition provided a unique overview of the state-of-the-art of systems, technologies, and methods for indoor positioning and navigation purposes. Through fair comparison of the performance achieved by each system, the competition was able to identify the most promising approaches and to pinpoint the most critical working conditions. In 2020, the competition included 5 diverse off-site off-site Tracks, each resembling real use cases and challenges for indoor positioning. The results in terms of participation and accuracy of the proposed systems have been encouraging. The best performing competitors obtained a third quartile of error of 1m for the Smartphone Track and 0.5m for the Footmounted IMU Track. While not running on physical systems, but only as algorithms, these results represent impressive achievements
Search for diphoton events with large missing transverse momentum in 1 fb(-1) of 7 TeV proton-proton collision data with the ATLAS detector ATLAS Collaboration
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alison J
- Aliyev M
- Alley M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ami SB
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Bachy G
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker MD
- Baker OK
- Baker S
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barashkou A
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baron AE
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Barrillon P
- Bartoldus R
- Bartsch D
- Bartsch V
- Bates RL
- Batkova L
- Batley JR
- Battaglia A
- Battistin M
- Battistoni G
- Bauer F
- Bawa HS
- Beare B
- Beau T
- Beauchemin PH
- Beccherle R
- Becht P
- Beck HP
- Becker S
- Beckingham M
- Becks KH
- Beddall A
- Beddall AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Begel M
- Behera PK
- Beimforde M
- Belanger-Champagne C
- Belenguer MJ
- Bell PJ
- Bell WH
- Bella G
- Bella LA
- Bellagamba L
- Bellina F
- Bellomo M
- Belloni A
- Beloborodova O
- Belotskiy K
- Beltramello O
- Benary O
- Benchekroun D
- Benchouk C
- Bendel M
- 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
- Bieniek SP
- Bierwagen K
- Biesiada J
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
- Bingul A
- Bini C
- Biscarat C
- Bitenc U
- Black KM
- Blair RE
- Blanchard J-B
- Blanchot G
- Blazek T
- Blocker C
- Blocki J
- Blondel A
- Blum W
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VB
- Bocchetta SS
- Bocci A
- Boddy CR
- Boehler M
- Boek J
- Boelaert N
- Boeriub OEV
- Boeser S
- Bogaerts JA
- Bogdanchikov A
- Bogouch A
- Bohm C
- Boisvert V
- Bold T
- Boldea V
- Bolnet NM
- Bona M
- Bondarenko VG
- Bondioli M
- Boonekamp M
- Boorman G
- Booth CN
- Bordoni S
- Borer C
- Borisov A
- Borissov G
- Borjanovic I
- Borroni S
- Bos K
- Boscherini D
- Bosman M
- Boterenbrood H
- Botterill D
- Bouchami J
- Boudreau J
- Bouhova-Thacker EV
- Bourdarios C
- Bousson N
- Boveia A
- Boyd J
- Boyko IR
- Bozhko NI
- Bozovic-Jelisavcic I
- Bracinik J
- Braem A
- Branchini P
- Brandenburg GW
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Brelier B
- Bremer J
- Brenner R
- Bressler S
- Breton D
- Britton D
- Brochu FM
- Brock I
- Brock R
- Brodbeck TJ
- Brodet E
- Broggia F
- Bromberg C
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- Brooksb WK
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- Brunet S
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- Buckingham RM
- Buckley AG
- Budaa SI
- Budagov IA
- Budick B
- Buescher V
- Bueso XP
- Bugge L
- Buira-Clark D
- Bulekov O
- Bunse M
- Buran T
- Burckhart H
- Burdin S
- Burgess T
- Burke S
- Busato E
- Bussey P
- Buszello CP
- Butin F
- Butler B
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
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- Cakira O
- Cakire IT
- Calafiura P
- Calderini G
- Calfayan P
- Calkins R
- Calobaa LP
- Caloia R
- Calvet D
- Calvet S
- Camarri P
- Cambiaghia M
- Cameron D
- Camillocci ES
- Campana S
- Campanelli M
- Canalea V
- Canelli F
- Canepaa A
- Cantero J
- Capassoa L
- Caprinia I
- Caprinia M
- Capriotti D
- Capua M
- Caputo R
- Cardarelli R
- Carli T
- Carlinoa G
- Carminati L
- Caron S
- Carona B
- Carter AA
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Cascella M
- Caso C
- Castaneda-Miranda E
- Castanheira MTD
- Castillo LRF
- Castro NF
- Cataldi G
- Cataneo F
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- Cauz D
- Cavalcanti TP
- Cavalleri P
- Cavalli-Sforza M
- Cavallia D
- Cavasinni V
- Ceradini F
- Cerqueiraa AS
- Cerri A
- Cerrito L
- Cerutti F
- Cetinb SA
- Cevenini F
- Chafaqa A
- Chakraborty D
- Chan K
- Chapleau B
- Chapman JD
- Chapman JW
- Chareyre E
- Charlton DG
- Chavda V
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- Chekanov S
- Chekulaeva SV
- Chelkov GA
- Chelstowska MA
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- Chepurnov VF
- Chernyatin V
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- Chikovania L
- Childersa JT
- Chilingarov A
- Chiodinia G
- Chizhov MV
- Choudalakis G
- Chouridou S
- Christidi IA
- Christov A
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Ciapetti G
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- Ciobotaru MD
- Ciocca C
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- Clark PJ
- Cleland W
- Clemens JC
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- Collaboration ATLAS
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- Cooper-Sarkar AM
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- Corradia M
- Correia AMH
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- Crescioli F
- Cristinziani M
- Crosetti G
- Crupi R
- Cuciuca C-M
- Curatolo M
- Curtis CJ
- Curull XE
- Cwetanski P
- Czirr H
- Czyczula Z
- D'Auria S
- D'Onofrio M
- D'Orazio A
- da Costa JBG
- Da Silvaa PVM
- Da Via C
- Dabrowski W
- Dai T
- Dallapiccola C
- Dam M
- Damazio DO
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- Damiani DS
- Danielsson HO
- Dannheim D
- Dao V
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- Darleab GL
- Daum C
- Davey W
- Davidek T
- Davidson N
- Davidson R
- Davies E
- Davies M
- Davison AR
- Davygoraa Y
- Dawe E
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- Dawson JW
- Daya RK
- de Asmundis R
- De Castro S
- De Cecco S
- De Graat J
- De Groot N
- de Jong P
- De la Hoz SG
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- De la Torre H
- de Lima JGR
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- De Mora L
- De Nooij L
- De Pedisa D
- De Regie JBDV
- de Renstrom PAB
- De Salvoa A
- De Sanctis U
- De Santo A
- De K
- Dean S
- Debbe R
- Dedovich DV
- Degenhardt J
- Dehchar M
- Del Papa C
- Del Peso J
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- della Porta GZ
- della Volpe D
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- Delruelle N
- Delsart PA
- Deluca C
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- Demichev M
- Demirkoz B
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- 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
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- Di Girolamo A
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- Di Luise S
- Di Mattia A
- Di Micco B
- Di Nardo R
- Di Simone A
- Di Sipio R
- Diaza MA
- Diblenc F
- Diehl EB
- Dietrich J
- Dietzscha TA
- Diglio S
- Dingfelder J
- Dionisi C
- Ditaa P
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- Dittus F
- Djama F
- Djobavab T
- do Vale MAB
- Doan TKO
- Dobbs M
- Dobinson R
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- Dobson M
- Dodd J
- Doglioni C
- Doherty T
- Dohmae T
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- Dolgoshein BA
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- Duehrssen M
- Duerdoth IP
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- Duflot L
- Dufour M-A
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- Gerlach P
- Gershon A
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- Publication venue
- Publication date
- 01/01/2012
- Field of study
A search for diphoton events with large missing transverse momentum has been performed using 1.07 fb -1 of proton-proton collision data at s=7 TeV recorded with the ATLAS detector. No excess of events was observed above the Standard Model prediction and 95% Confidence Level (CL) upper limits are set on the production cross section for new physics. The limits depend on each model parameter space and vary as follows: Λ<(22-129) fb in the context of a generalised model of gauge-mediated supersymmetry breaking (GGM) with a bino-like lightest neutralino, σ<(27-91) fb in the context of a minimal model of gauge-mediated supersymmetry breaking (SPS8), and σ<(15-27) fb in the context of a specific model with one universal extra dimension (UED). A 95% CL lower limit of 805 GeV, for bino masses above 50 GeV, is set on the GGM gluino mass. Lower limits of 145 TeV and 1.23 TeV are set on the SPS8 breaking scale Λ and on the UED compactification scale 1/R, respectively. These limits provide the most stringent tests of these models to date. © 2012 CERN
Measurement of the isolated diphoton cross-section in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
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- Abdesselam Abdelmalek
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- Publication venue
- Publication date
- 21/12/2010
- Field of study
The ATLAS experiment has measured the production cross-section of events with
two isolated photons in the final state, in proton-proton collisions at sqrt(s)
= 7 TeV. The full data set acquired in 2010 is used, corresponding to an
integrated luminosity of 37 pb^-1. The background, consisting of hadronic jets
and isolated electrons, is estimated with fully data-driven techniques and
subtracted. The differential cross-sections, as functions of the di-photon
mass, total transverse momentum and azimuthal separation, are presented and
compared to the predictions of next-to-leading-order QCD.Comment: 15 pages plus author list (27 pages total), 9 figures, 2 tables,
final version to appear in Physical Review
Search for diphoton events with large missing transverse momentum in 1 fb<sup>-1</sup> of 7 TeV proton–proton collision data 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
- 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
- Akiyama A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alison J
- Aliyev M
- Alley M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ami SB
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Bachy G
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker MD
- Baker OK
- Baker S
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barashkou A
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baron AE
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Barrillon P
- Bartoldus R
- Bartsch D
- Bartsch V
- Bates RL
- Batkova L
- Batley JR
- Battaglia A
- Battistin M
- Battistoni G
- Bauer F
- Bawa HS
- Beare B
- Beau T
- Beauchemin PH
- Beccherle R
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- Becks KH
- Beddall A
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- Zitoun R
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- Zsenei A
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- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2012
- Field of study
A search for diphoton events with large missing transverse momentum has been performed using 1.07 fb−1of proton–proton collision data at √s=7 TeV recorded with the ATLAS detector. No excess of events was observed above the Standard Model prediction and 95% Confidence Level (CL) upper limits are set on the production cross section for new physics. The limits depend on each model parameter space and vary as follows: σ<(22–129) fb in the context of a generalised model of gauge-mediated supersymmetry breaking (GGM) with a bino-like lightest neutralino, σ<(27–91) fb in the context of a minimal model of gauge-mediated supersymmetry breaking (SPS8), and σ< (15–27) fb in the context of a specific model with one universal extra dimension (UED). A 95% CL lower limit of 805 GeV, for bino masses above 50 GeV, is set on the GGM gluino mass. Lower limits of 145 TeV and 1.23 TeV are set on the SPS8 breaking scale ∧ and on the UED compactification scale 1/R, respectively. These limits provide the most stringent tests of these models to date
Search for diphoton events with large missing transverse momentum in 1 fb(-1) of 7 TeV proton-proton collision data with the ATLAS detector ATLAS Collaboration
- Author
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- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
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- Zhao Z
- Zhaob Z
- Zhemchugov A
- Zhemchugov A
- Zheng S
- Zhenga S
- Zhong J
- Zhong J
- Zhou B
- Zhou B
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- Zhu H
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- Zhuang X
- Zhuang X
- Zhub Y
- Zhud CG
- Zhuravlov V
- Zhuravlov V
- Zieminska D
- Zieminska D
- Zimmermann R
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Ziolkowski M
- Zitoun R
- Zitoun R
- Zivkovic L
- Zivkovic L
- Zmouchko VV
- Zmouchko VV
- Zobernig G
- Zobernig G
- Zoccoli A
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zsenei A
- zur Nedden M
- Zutshi V
- Zutshi V
- Zwalinski L
- Zwalinski Lng X
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2012
- Field of study
A search for diphoton events with large missing transverse momentum has been performed using 1.07 fb(-1) of proton-proton collision data at root s = 7 TeV recorded with the ATLAS detector. No excess of events was observed above the Standard Model prediction and 95% Confidence Level (CL) upper limits are set on the production cross section for new physics. The limits depend on each model parameter space and vary as follows: sigma < (22-129) fb in the context of a generalised model of gauge-mediated supersymmetry breaking (GGM) with a bino-like lightest neutralino, sigma < (27-91) fb in the context of a minimal model of gauge-mediated supersymmetry breaking (SPS8), and sigma < (15-27) fb in the context of a specific model with one universal extra dimension (UED). A 95% CL lower limit of 805 GeV, for bino masses above 50 GeV, is set on the GGM gluino mass. Lower limits of 145 TeV and 1.23 TeV are set on the SPS8 breaking scale Lambda and on the UED compactification scale 1/R, respectively. These limits provide the most stringent tests of these models to date. (C) 2012 CERN. Published by Elsevier B.V. All rights reserved. RI Sivoklokov, Sergey/D-8150-2012; Li, Xuefei/C-3861-2012; Smirnov, Sergei/F-1014-2011; Gladilin, Leonid/B-5226-2011; Barreiro, Fernando/D-9808-2012; Prokoshin, Fedor/E-2795-2012; Fazio, Salvatore /G-5156-2010; Orlov, Ilya/E-6611-2012; Doyle, Anthony/C-5889-2009; Alexa, Calin/F-6345-2010; Moorhead, Gareth/B-6634-2009; Livan, Michele/D-7531-2012; Takai, Helio/C-3301-2012; Petrucci, Fabrizio/G-8348-2012; Jones, Roger/H-5578-2011; Fabbri, Laura/H-3442-2012; Kurashige, Hisaya/H-4916-2012; Villa, Mauro/C-9883-2009; Delmastro, Marco/I-5599-201
Search for diphoton events with large missing transverse momentum in 1 fb(-1) of 7 TeV proton-proton collision data with the ATLAS detector ATLAS Collaboration
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alison J
- Aliyev M
- Alley M
- Allport PP
- Allwood Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ami SB
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux ML
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin JF
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asquith L
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- Svatos M
- Sviridov YM
- Swedish S
- Sykora T
- Sykoraa I
- Szeless B
- Ta D
- Tackmann K
- Taffard A
- Tafirouta R
- Taiblum N
- Takahashi Y
- Takai H
- Takashima R
- Takeda H
- Takeshita T
- Talby M
- Talyshev A
- Tamsett MC
- Tanaka J
- Tanaka R
- Tanaka S
- Tanaka S
- Tanaka Y
- Tani K
- Tannoury N
- Tappern GP
- Tapprogge S
- Tardif D
- Tarem S
- Tarrade F
- Tartarellia GF
- Tas P
- Tasevsky M
- Tassi E
- Tatarkhanov M
- Tayalatid Y
- Taylor C
- Taylor FE
- Taylor GN
- Taylorb W
- Tehrani FS
- Teinturier M
- Teixeira Dias P
- Temming KK
- Ten Kate H
- Teng PK
- Terada S
- Terashi K
- Terron J
- Terwort M
- Testa M
- Teuscher RJ
- Thadome J
- Therhaag J
- Theveneaux Pelzer T
- Thioye M
- Thoma S
- Thomas JP
- Thompson AS
- Thompson EN
- Thompson PD
- Thompson PD
- Thomson E
- Thomson M
- Thun RP
- Tian F
- Tic T
- Tikhomirov VO
- Tikhonov YA
- Timmermans CJWP
- Tipton P
- Tisserant S
- Tobias J
- Toczek B
- Todorov T
- Todorova Nova S
- Toggerson B
- Tojo J
- Tokar S
- Tokunaga K
- Tokushuku K
- Tollefson K
- Tomoto M
- Tompkins L
- Toms K
- Tonga G
- Tonoyan A
- Topfel C
- Topilin ND
- Torchiani I
- Toro RC
- Torregrosa EF
- Torrence E
- Torres H
- Toth J
- Touchard F
- Tovey DR
- Traynor D
- Trefzger T
- Tremblet L
- Tricoli A
- Triggera IM
- Trincaz Duvoid S
- Trinh TN
- Tripiana MF
- Trischuk W
- Trivedi A
- Trocme B
- Troncona C
- Trottier McDonald M
- Trzupek A
- Tsarouchas C
- Tseng JCL
- Tsiakiris M
- Tsiareshka PV
- Tsionou D
- Tsipolitis G
- Tsiskaridze V
- Tskhadadzea EG
- Tsukerman II
- Tsulaia V
- Tsung JW
- Tsunoo S
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- Tua A
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- Tuggle JM
- Turala M
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- Tyrvainen H
- Tzanakos G
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- Ueda I
- Ueno R
- Ugland M
- Uhlenbrock M
- Uhrmacher M
- Ukegawa F
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- Underwood DG
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- Valentea P
- Valentinetti S
- Valkar S
- Vallecorsa S
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- van der Kraaij E
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- van der Poel E
- van der Ster D
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- van Gemmeren P
- van Huysduynen LH
- van Kesteren Z
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- Vandelli W
- Vandoni G
- Vaniachine A
- Vankov P
- Vannucci F
- Vaque FV
- Varia R
- Varouchas D
- Vartapetian A
- Varvell KE
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- Vazeille F
- Vegni G
- Veillet JJ
- Vellidis C
- Velosoa F
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- Ventura A
- Ventura D
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- Verge LM
- Verkerke W
- Vermeulen JC
- Vest A
- Vetterli MC
- Vichou I
- Vickey T
- Viegas FJTA
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- Viel S
- Villa M
- Vilucchi E
- Vincter MG
- Vinek E
- Vinogradov VB
- Virchaux M
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- Vitells O
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- Vivarelli I
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- Vladoiu D
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- Vukot I
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- Wilkens HG
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- Wingerter Seez I
- Winkelmann S
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- Yoosoofmiya R
- Yorita K
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- Youssef S
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- Yuan L
- Yurkewicz A
- Zaets VG
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zeitnitz C
- Zeller M
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenisa T
- Zenonos Z
- Zenz S
- Zerwas D
- Zhand Z
- Zhang D
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- Zhang Z
- Zhang Z
- Zhangd X
- Zhao L
- Zhao L
- Zhao T
- Zhao T
- Zhao Z
- Zhaob Z
- Zhemchugov A
- Zhemchugov A
- Zheng S
- Zhenga S
- Zhong J
- Zhong J
- Zhou B
- Zhou B
- Zhou N
- Zhou N
- Zhou Y
- Zhou Y
- Zhu CG
- Zhu H
- Zhu H
- Zhu J
- Zhu J
- Zhu Y
- Zhuang X
- Zhuang X
- Zhub Y
- Zhud CG
- Zhuravlov V
- Zhuravlov V
- Zieminska D
- Zieminska D
- Zimmermann R
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Ziolkowski M
- Zitoun R
- Zitoun R
- Zivkovic L
- Zivkovic L
- Zmouchko VV
- Zmouchko VV
- Zobernig G
- Zobernig G
- Zoccoli A
- Zoccoli A
- Zolnierowski Y
- Zsenei A
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- zur Nedden M
- Zutshi V
- Zutshi V
- Zwalinski L.
- Zwalinski Lng X
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2012
- Field of study
A search for diphoton events with large missing transverse momentum has been performed using 1.07 fb(-1) of proton-proton collision data at root s = 7 TeV recorded with the ATLAS detector. No excess of events was observed above the Standard Model prediction and 95% Confidence Level (CL) upper limits are set on the production cross section for new physics. The limits depend on each model parameter space and vary as follows: sigma < (22-129) fb in the context of a generalised model of gauge-mediated supersymmetry breaking (GGM) with a bino-like lightest neutralino, sigma < (27-91) fb in the context of a minimal model of gauge-mediated supersymmetry breaking (SPS8), and sigma < (15-27) fb in the context of a specific model with one universal extra dimension (UED). A 95% CL lower limit of 805 GeV, for bino masses above 50 GeV, is set on the GGM gluino mass. Lower limits of 145 TeV and 1.23 TeV are set on the SPS8 breaking scale Lambda and on the UED compactification scale 1/R, respectively. These limits provide the most stringent tests of these models to date. (C) 2012 CERN. Published by Elsevier B.V. All rights reserved