571 research outputs found
External and internal influences on R&D alliance formation: evidence from German SMEs
- Publication venue
- Elsevier
- Publication date
- 29/11/2013
- Field of study
Relying on relational capital theory and transaction cost economics (TCE), this study identifies factors that impede or promote alliance formation in small to medium-sized enterprises (SMEs). Environmental uncertainty and knowledge intensity impede firmsâ R&D alliance formation; the focal firmâs overall trust in partners enhances alliance formation. Trust interacts positively with environmental uncertainty and knowledge intensity to affect alliance formation in SMEs. The findings reflect data from a longitudinal sample of 854 German SMEs, captured over eight years from 1999 to 2007
Does buyer-seller similarity affect buyer satisfaction with the seller firm?
- Publication venue
- Taylor & Francis
- Publication date
- 01/01/2012
- Field of study
With the increased reliance on diverse markets in multi-cultural contexts, the role that similarity can play in the relationship between a salesperson and a buyer is receiving increased attention. Similarity is regarded as the cornerstone of positive communications, and salespeople rely on the trust that can be created by this recognition of likeness. However, there are different types of similarity, and not all have an equal bearing on the salesperson-buyer relationship. In this study, we examine similarity in appearance, similarity in lifestyle, and similarity in status. Most studies go no further than examining the effect of similarity on a buyerâs satisfaction with a salesperson, and to date there appear to be few studies relating to the effect of similarity on satisfaction with a firm. This study examines the effect of similarity on a buyerâs sense of satisfaction with a firm represented by a salesperson in the banking context. The results of the study show that appearance similarity and status similarity have a significant effect on the salesperson-buyer relationship, whereas lifestyle similarity has no effect. The buyerâs satisfaction with a salesperson is found to mediate the relationship between similarity in appearance and the buyerâs satisfaction with a firm. In this paper, we discuss these findings and look at their implications for both research and practice. Findings of the study are particularly important because of New Zealandâs increasing interaction with Asia and its people, which has transformed New Zealand to become a multi-cultural and multi-ethnic country
Thermodynamic Properties of Ni-substituted LnCoO3 Perovskite
- Publication venue
- The International Institute for Science, Technology and Education (IISTE)
- Publication date
- 28/07/2015
- Field of study
With the objective of exploring the unknown thermodynamic properties of Ni-substituted LnCoO3 perovskite, we present here an investigation of the temperature-dependent (10K < T < 300K) specific heat of LnCo0.95Ni0.05O3 (Ln=Pr and Nd) family. We report here probably for the first time the specific heat along with other elastic and thermal properties of Ni doped perovskite cobaltate LnCoO3 (Ln=Pr and Nd). In addition, the results on the cohesive energy (f) in orthorhombic perovskite phase, molecular force constant (Æ), Reststrahlen frequency (uo) and Gruneisen parameter (Îł) are also presented. Keywords: Specific heat, Bulk modulus, Perovskite cobaltat
Removal and degradation of mixed dye pollutants by integrated adsorption-photocatalysis technique using 2-D MoS2/TiO2 nanocomposite
- Author
- Publication venue
- Publication date
- 01/09/2021
- Field of study
Two-dimensional (2D) Molybdenum disulfide (MoS2) has become one of the most exciting areas of research for adsorbents due to its high surface area and abundant active sites. Mainly, 2D MoS2 show promising removal of textile dye pollutants by adsorption process, but it show high affinity for anionic type of dyes, that limits its performance in mixed dye pollutants treatment. Herein, we demonstrate an integrated approach to remove mixed dye pollutants (anionic and cationic) concurrently by combining adsorption and photocatalysis process. We synthesize MoS2/TiO2 nanocomposites for different weight percentages 2.5, 5, 10, 20, 30 and 50 wt% of pre-synthesized flower-like MoS2 nanoparticle by a two-step hydrothermal method. We demonstrate a new process of two-stage adsorption/photocatalysis using high wt% of MoS2 (Stage-I) and low wt% of MoS2 (Stage-II) nanocomposites. The proposed two-stage integrated adsorption and photocatalysis process using 50% and 2.5% of MoS2 coated TiO2, respectively showed complete removal of methylene blue dye âŒ5 times faster than conventional single-stage (adsorption or photocatalysis) water treatment process. Furthermore, the feasibility of the proposed two-stage method in mixed dye pollutants removal (anionic and cationic) testified, which showed excellent performance even in doubling the dye pollutant concentration. This work brings a deeper insight into understanding the morphology and concentration of 2-D MoS2 in MoS2/TiO2 nanocomposite in tackling mixed dye pollutants and the possibilities of applying in textile dyeing industries wastewater treatment plants
Rational Mutational Analysis of a Multidrug MFS Transporter CaMdr1p of Candida albicans by Employing a Membrane Environment Based Computational Approach
- Author
- A Chandrasekaran
- A Decottignies
- A Krogh
- A Sali
- AC Tutulan-Cunita
- Ajeeta Kaushiki
- Andrew M. Lynn
- B Reva
- CD Livingstone
- CE Shannon
- CJ Law
- CP Chen
- GJ Barton
- I Sa-Correia
- IT Paulsen
- J Abramson
- JA Capra
- JD Fischer
- JL Ditty
- K Koike
- K Nakamura
- K Wang
- Khyati Kapoor
- L Guan
- L Li
- LC Martin
- M Gaur
- M Gaur
- M Schiffer
- Mohd Rehan
- N Puri
- N Sigal
- P Saini
- PC Ng
- PK Srivastava
- Q Yang
- R Egner
- R Ernst
- R Pasrija
- R Prasad
- Rajendra Prasad
- RC Edgar
- RE De
- Ritu Pasrija
- Roland Dunbrack
- S Henikoff
- S Shukla
- S Shukla
- SL Ginn
- Smriti
- SS Hannenhalli
- SS Pao
- T Cover
- W Pirovano
- WS Valdar
- Y Huang
- Y Yin
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2009
- Field of study
CaMdr1p is a multidrug MFS transporter of pathogenic Candida albicans. An over-expression of the gene encoding this protein is linked to clinically encountered azole resistance. In-depth knowledge of the structure and function of CaMdr1p is necessary for an effective design of modulators or inhibitors of this efflux transporter. Towards this goal, in this study, we have employed a membrane environment based computational approach to predict the functionally critical residues of CaMdr1p. For this, information theoretic scores which are variants of Relative Entropy (Modified Relative Entropy REM) were calculated from Multiple Sequence Alignment (MSA) by separately considering distinct physico-chemical properties of transmembrane (TM) and inter-TM regions. The residues of CaMdr1p with high REM which were predicted to be significantly important were subjected to site-directed mutational analysis. Interestingly, heterologous host Saccharomyces cerevisiae, over-expressing these mutant variants of CaMdr1p wherein these high REM residues were replaced by either alanine or leucine, demonstrated increased susceptibility to tested drugs. The hypersensitivity to drugs was supported by abrogated substrate efflux mediated by mutant variant proteins and was not attributed to their poor expression or surface localization. Additionally, by employing a distance plot from a 3D deduced model of CaMdr1p, we could also predict the role of these functionally critical residues in maintaining apparent inter-helical interactions to provide the desired fold for the proper functioning of CaMdr1p. Residues predicted to be critical for function across the family were also found to be vital from other previously published studies, implying its wider application to other membrane protein families
Observation of associated near-side and away-side long-range correlations in âsNN=5.02ââTeV 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 GuimarĂŁes 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
- BĂŒscher V
- Cabrera UrbĂĄn 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
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- 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
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- 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
- CÎté 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
- DĂŒhrssen M
- DĂŒren 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
- FilipÄiÄ 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
- GarcĂa Navarro JE
- GarcĂa 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
- George M
- George S
- Gerbaudo D
- Gerlach P
- Gershon A
- Geweniger C
- Ghazlane H
- Ghodbane N
- Giacobbe B
- Giagu S
- Giangiobbe V
- Gianotti F
- Gibbard B
- Gibson A
- Gibson SM
- Gilchriese M
- Gillam TP
- Gillberg D
- Gillman AR
- Gingrich DM
- Ginzburg J
- Giokaris N
- Giordani MP
- Giordano R
- Giorgi FM
- Giovannini P
- Giraud PF
- Giugni D
- Giunta M
- Gjelsten BK
- Gladilin LK
- Glasman C
- Glatzer J
- Glazov A
- Glonti GL
- Goddard JR
- Godfrey J
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- 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
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- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
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- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
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- Zinonos Z
- Ziolkowski M
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- 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
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
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- Acharya BS
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- Aharrouche M
- Ahlen SP
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- Ahmad A
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- Aielli G
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- Aktas A
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- Aleksandrov IN
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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 âs = 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 pTâ„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 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Measurement of the cross-section of high transverse momentum vector bosons reconstructed as single jets and studies of jet substructure in pp collisions at âs = 7 TeV with the ATLAS detector
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- Flick T
- Floderus A
- Floderus A
- Florez Bustos AC
- Flowerdew MJ
- Flowerdew MJ
- Formica A
- Formica A
- Forti A
- Forti A
- Fortin D
- Fortin D
- Fournier D
- Fournier D
- Fox H
- Fox H
- Francavilla P
- Francavilla P
- Franchini M
- Franchini M
- Franchino S
- Franchino S
- Francis D
- Francis D
- Franklin M
- Franklin M
- Franz S
- Franz S
- Fraternali M
- Fraternali M
- Fratin S
- Fratina S
- French ST
- French ST
- Friedrich C
- Friedrich C
- Friedrich F
- Friedrich F
- Froidevaux D
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- Frost JA
- Frost JA
- Fukunaga C
- Fukunaga C
- Fulsom BG
- Fulsom BG
- Fuster J
- Fuster J
- Gabaldon C
- Gabaldon C
- Gabizon O
- Gabizon O
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gadatsch S
- Gadatsch S
- Gadomski S
- Gadomski S
- Gagliardi G
- Gagliardi G
- Gagnon P
- Gagnon P
- Galea C
- Galea C
- Galhardo B
- Galhardo B
- Gallas EJ
- Gallas EJ
- Gallo V
- Gallo V
- Gallop BJ
- Gallop BJ
- Gallus P
- Gallus P
- Galster G
- Galster G
- Gan KK
- Gan KK
- Gandrajula RP
- Gandrajula RP
- Gao J
- Gao YS
- Gao YS
- Gaob J
- Garberson F
- Garberson F
- Garcia Navarro JE
- Garcia Navarro JE
- Garcia BRM
- Garcia C
- Garcia C
- Garcia JAB
- Garcia-Sciveres M
- Garcia-Sciveres M
- Gardner RW
- Gardner RW
- Garelli N
- Garelli N
- Garonne V
- Garonne V
- Garrido MDMC
- Gatti C
- Gatti C
- Gaudio G
- Gaudio G
- Gaur B
- Gaur B
- Gauthier L
- Gauthier L
- Gauzzi P
- Gauzzi P
- Gavrilenko IL
- Gavrilenko IL
- Gay C
- Gay C
- Gaycken G
- Gaycken G
- Gazis EN
- Gazis EN
- Ge P
- Ge P
- Gecse Z
- Gecse Z
- Gee CNP
- Gee CNP
- Geerts DAA
- Geerts DAA
- Geich-Gimbel C
- Geich-Gimbel C
- Gellerstedt K
- Gellerstedt K
- Gemme C
- Gemme C
- Gemmell A
- Gemmell A
- Genest MH
- Genest MH
- Gentile S
- Gentile S
- George M
- George M
- George S
- George S
- Gerbaudo D
- Gerbaudo D
- Gershon A
- Gershon A
- Ghazlane H
- Ghazlane H
- Ghodbane N
- Ghodbane N
- Giacobbe B
- Giacobbe B
- Giagu S
- Giagu S
- Giangiobbe V
- Giangiobbe V
- Giannetti P
- Giannetti P
- Gianotti F
- Gianotti F
- Gibbard B
- Gibbard B
- Gibson SM
- Gibson SM
- Gilchriese M
- Gilchriese M
- Gillam TPS
- Gillam TPS
- Gillberg D
- Gillberg D
- Gillman AR
- Gillman AR
- Gingrich DM
- Gingrich M
- Giokaris N
- Giokaris N
- Giordani MP
- Giordani MP
- Giordano R
- Giordano R
- Giorgi FM
- Giorgi FM
- Giraud PF
- Giraud PF
- Giugni D
- Giugni D
- Giuliani C
- Giuliani C
- Giunta M
- Giunta M
- Gjelsten BK
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- Gkialas I
- Gkialas I
- Gladilin LK
- Gladilin LK
- Glasman C
- Glasman C
- Glatzer J
- Glatzer J
- Glazov A
- Glazov A
- Glonti GL
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- Goblirsch-Kolb M
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- Goddard JR
- Goddard JR
- Godfrey J
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- Godlewski J
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- Goeringer C
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- Goessling C
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- Goldfarb S
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- Golubkov D
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- Gomes A
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- Gonalo R
- Goncalo R
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- Gonzalez de la Hoz S
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- Gonzalez Parra G
- Gonzalez Parra G
- Gonzalez BA
- Gonzalez-Sevilla S
- Gonzalez-Sevilla S
- Goossens L
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- Gorbounov PA
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- Gordon HA
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- Gorelov I
- Gorelov I
- Gorini B
- Gorini B
- Gorini E
- Gorini E
- Gorisek A
- Gorisek A
- Gornicki E
- Gornicki E
- Goshaw AT
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- Gostkin MI
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- Gouighri M
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- Goujdami D
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- Goulette MP
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- Goussiou AG
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- Goy C
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- Gozpinar S
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- Grabas HMX
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- Graber L
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- Grafstroem P
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- Gramstad E
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- Grancagnolo S
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- Grassi V
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- Gratchev V
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- Gray HM
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- Graziani E
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- Grebenyuk OG
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- Greenwood ZD
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- Gregersen K
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- Gregor IM
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- Grenier P
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- Griffiths J
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- Grillo AA
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- Griso SP
- Grivaz J-F
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- Grohs JP
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- Grohsjean A
- Gross AGE
- Gross E
- Grosse-Knetter J
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- Grossi GC
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- Groth-Jensen J
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- Guest D
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- Gueta O
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- Guido E
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- Gutierrez P
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- Guyot C
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- Zhemchugov A
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- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
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- Zobernig G
- Zoccoli A
- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2014
- Field of study
This paper presents a measurement of the cross-section for high transverse momentum W and Z bosons produced in pp collisions and decaying to all-hadronic final states. The data used in the analysis were recorded by the ATLAS detector at the CERN Large Hadron Collider at a centre-of-mass energy of âs = 7 TeV;{\rm Te}{\rm V}andcorrespondtoanintegratedluminosityof4.6\;{\rm f}{{{\rm b}}^{-1}}.ThemeasurementisperformedbyreconstructingtheboostedWorZbosonsinsinglejets.ThereconstructedjetmassisusedtoidentifytheWandZbosons,andajetsubstructuremethodbasedonenergyclusterinformationinthejetcentreâofâmassframeisusedtosuppressthelargemultiâjetbackground.ThecrossâsectionforeventswithahadronicallydecayingWorZboson,withtransversemomentum{{p}_{{\rm T}}}\gt 320\;{\rm Ge}{\rm V}andpseudorapidity|\eta |\lt 1.9,ismeasuredtobe{{\sigma }_{W+Z}}=8.5\pm 1.7$ pb and is compared to next-to-leading-order calculations. The selected events are further used to study jet grooming techniques
Search for 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
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- Abolins M
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- Acharya BS
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- Adelman J
- Adomeit S
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- Aguilar-Saavedra JA
- Agustoni M
- Aharrouche M
- Ahlen SP
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- Alam MS
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- Allbrooke BMM
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- Yamanaka T
- Yamazaki T
- Yamazaki Y
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- Yang H
- Yang UK
- Yang Y
- Yang Z
- Yanush S
- Yao L
- Yao Y
- Yasu Y
- Smit GVY
- Ye J
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- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- 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
- Zinonos Z
- Zerwas D
- della Porta GZ
- Zhang 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
- 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 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 high-mass resonances decaying to dilepton final states in pp collisions at sâ=7 TeV with the ATLAS detector
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- Abajyan T
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- Abdallah J
- Abdelalim AA
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- Yilmaz M
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- Youssef S
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- 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
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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
- 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
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