1,269 research outputs found
Temperature dependence on the mass susceptibility and mass magnetization of superparamagnetic MnâZnâferrite nanoparticles as contrast agents for magnetic imaging of oil and gas reservoirs
- Author
- Publication venue
- 'Informa UK Limited'
- Publication date
- 01/01/2018
- Field of study
The mass susceptibility (Ïmass) and mass magnetization (Mmass) were determined for a series of ternary manganese and zinc ferrite nanoparticles (MnâZn ferrite NPs, MnxZn1âxFe2O4) with different Mn:Zn ratios (0.08 †x †4.67), prepared by the thermal decomposition reaction of the appropriate metal acetylacetonate complexes, and for the binary homologs (MxFe3âxO4, where M = Mn or Zn). Alteration of the Mn:Zn ratio in MnâZn ferrite NPs does not significantly affect the particle size. At room temperature and low applied field strength the mass susceptibility increases sharply as the Mn:Zn ratio increases, but above a ratio of 0.4 further increase in the amount of manganese results in the mass susceptibility decreasing slightly, reaching a plateau above Mn:Zn â 2. The compositional dependence of the mass magnetization shows less of a variation at room temperature and high applied fields. The temperature dependence of the mass magnetization of MnâZn ferrite NPs is significantly less for Mn-rich compositions making them more suitable for downhole imaging at higher temperatures (>100 °C). For non-shale reservoirs, replacement of nMag by Mn-rich MnâZn ferrites will allow for significant signal-to-noise enhancement of 6.5Ă over NP magnetite
Mendelian randomization study of B-type natriuretic peptide and type 2 diabetes: evidence of causal association from population studies
- Author
- A Meirhaeghe
- AB Ropero
- AG Tabak
- Aline Meirhaeghe
- BF Voight
- C Newton-Cheh
- C Sengenes
- Claudia Langenberg
- DC Thomas
- DE Lanfear
- DJ Halsall
- E McFadden
- H Choquet
- InĂȘs Barroso
- JA Taylor
- K Miyashita
- Kay-Tee Khaw
- KT Khaw
- LR Potter
- M Halbirk
- N Chainani-Wu
- N Day
- Naveed Sattar
- NC Onland-Moret
- Nicholas J. Wareham
- NM De Silva
- Paul Welsh
- R van Kimmenade
- Rachel Mary Freathy
- RH Ritchie
- RJ Loos
- Robert Luben
- Roman Pfister
- S Soriano
- SF Mohammed
- Stephen Sharp
- T Lauritzen
- TJ Wang
- TJ Wang
- TJ Wang
- V Didelez
- V Salomaa
- Veikko Salomaa
- WS Huang
- Y Takeishi
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/01/2011
- Field of study
<p>Background: Genetic and epidemiological evidence suggests an inverse association between B-type natriuretic peptide (BNP) levels in blood and risk of type 2 diabetes (T2D), but the prospective association of BNP with T2D is uncertain, and it is unclear whether the association is confounded.</p>
<p>Methods and Findings: We analysed the association between levels of the N-terminal fragment of pro-BNP (NT-pro-BNP) in blood and risk of incident T2D in a prospective case-cohort study and genotyped the variant rs198389 within the BNP locus in three T2D case-control studies. We combined our results with existing data in a meta-analysis of 11 case-control studies. Using a Mendelian randomization approach, we compared the observed association between rs198389 and T2D to that expected from the NT-pro-BNP level to T2D association and the NT-pro-BNP difference per C allele of rs198389. In participants of our case-cohort study who were free of T2D and cardiovascular disease at baseline, we observed a 21% (95% CI 3%-36%) decreased risk of incident T2D per one standard deviation (SD) higher log-transformed NT-pro-BNP levels in analysis adjusted for age, sex, body mass index, systolic blood pressure, smoking, family history of T2D, history of hypertension, and levels of triglycerides, high-density lipoprotein cholesterol, and low-density lipoprotein cholesterol. The association between rs198389 and T2D observed in case-control studies (odds ratio = 0.94 per C allele, 95% CI 0.91-0.97) was similar to that expected (0.96, 0.93-0.98) based on the pooled estimate for the log-NT-pro-BNP level to T2D association derived from a meta-analysis of our study and published data (hazard ratio = 0.82 per SD, 0.74-0.90) and the difference in NT-pro-BNP levels (0.22 SD, 0.15-0.29) per C allele of rs198389. No significant associations were observed between the rs198389 genotype and potential confounders.</p>
<p>Conclusions: Our results provide evidence for a potential causal role of the BNP system in the aetiology of T2D. Further studies are needed to investigate the mechanisms underlying this association and possibilities for preventive interventions.</p>
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Application of multidisciplinary analysis to gene expression.
- Author
- Andries Erik (University of New Mexico, Albuquerque, NM)
- Ar Kerem (University of New Mexico, Albuquerque, NM)
- Cowie Jim R. (New Mexico State University, Las Cruces, NM)
- Davidson George S.
- Fields Chris (New Mexico State University, Las Cruces, NM)
- Haaland David Michael
- Helman Paul (University of New Mexico, Albuquerque, NM)
- Kang Huining (University of New Mexico, Albuquerque, NM)
- Martin Shawn Bryan
- Mosquera-Caro Monica P. (University of New Mexico, Albuquerque, NM)
- Murphy Maurice H. (University of New Mexico, Albuquerque, NM)
- Potter Jeffrey (University of New Mexico, Albuquerque, NM)
- Sibirtsev Valeriy (New Mexico State University, Las Cruces, NM)
- Wang Xuefel (University of New Mexico, Albuquerque, NM)
- Willman Cheryl L. (University of New Mexico, Albuquerque, NM)
- Xu Yuexian (University of New Mexico, Albuquerque, NM)
- Publication venue
- Sandia National Laboratories
- Publication date
- 01/01/2004
- Field of study
Molecular analysis of cancer, at the genomic level, could lead to individualized patient diagnostics and treatments. The developments to follow will signal a significant paradigm shift in the clinical management of human cancer. Despite our initial hopes, however, it seems that simple analysis of microarray data cannot elucidate clinically significant gene functions and mechanisms. Extracting biological information from microarray data requires a complicated path involving multidisciplinary teams of biomedical researchers, computer scientists, mathematicians, statisticians, and computational linguists. The integration of the diverse outputs of each team is the limiting factor in the progress to discover candidate genes and pathways associated with the molecular biology of cancer. Specifically, one must deal with sets of significant genes identified by each method and extract whatever useful information may be found by comparing these different gene lists. Here we present our experience with such comparisons, and share methods developed in the analysis of an infant leukemia cohort studied on Affymetrix HG-U95A arrays. In particular, spatial gene clustering, hyper-dimensional projections, and computational linguistics were used to compare different gene lists. In spatial gene clustering, different gene lists are grouped together and visualized on a three-dimensional expression map, where genes with similar expressions are co-located. In another approach, projections from gene expression space onto a sphere clarify how groups of genes can jointly have more predictive power than groups of individually selected genes. Finally, online literature is automatically rearranged to present information about genes common to multiple groups, or to contrast the differences between the lists. The combination of these methods has improved our understanding of infant leukemia. While the complicated reality of the biology dashed our initial, optimistic hopes for simple answers from microarrays, we have made progress by combining very different analytic approaches
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SVEP1 as a Genetic Modifier of TEK-Related Primary Congenital Glaucoma.
- Author
- Anagnos E
- Bradfield YS
- Carmona S
- Craig JE
- Dan Y
- Egas C
- Elahi E
- Higuchi EC
- Huang SJ
- Jin J
- Jody NM
- LaMartina SM
- Lawson BM
- Limviphuvadh V
- Maroofian R
- Martin JS
- Martin SM
- Maurer-Stroh S
- Motlagh BF
- Narooie-Nejad M
- Potter HD
- Quaggin SE
- Siggs OM
- Silva ED
- SimÔes MJ
- Souma T
- Souzeau E
- Stangel N
- Suri F
- Tompson SW
- Whisenhunt KN
- Young TL
- Zhang X
- Publication venue
- 'Association for Research in Vision and Ophthalmology (ARVO)'
- Publication date
- 07/10/2020
- Field of study
Purpose: Affecting children by age 3, primary congenital glaucoma (PCG) can cause debilitating vision loss by the developmental impairment of aqueous drainage resulting in high intraocular pressure (IOP), globe enlargement, and optic neuropathy. TEK haploinsufficiency accounts for 5% of PCG in diverse populations, with low penetrance explained by variable dysgenesis of Schlemm's canal (SC) in mice. We report eight families with TEK-related PCG, and provide evidence for SVEP1 as a disease modifier in family 8 with a higher penetrance and severity. Methods: Exome sequencing identified coding/splice site variants with an allele frequency less than 0.0001 (gnomAD). TEK variant effects were assayed in construct-transfected HEK293 cells via detection of autophosphorylated (active) TEK protein. An enucleated eye from an affected member of family 8 was examined via histology. SVEP1 expression in developing outflow tissues was detected by immunofluorescent staining of 7-day mouse anterior segments. SVEP1 stimulation of TEK expression in human umbilical vascular endothelial cells (HUVECs) was measured by TaqMan quantitative PCR. Results: Heterozygous TEK loss-of-function alleles were identified in eight PCG families, with parent-child disease transmission observed in two pedigrees. Family 8 exhibited greater disease penetrance and severity, histology revealed absence of SC in one eye, and SVEP1:p.R997C was identified in four of the five affected individuals. During SC development, SVEP1 is secreted by surrounding tissues. SVEP1:p.R997C abrogates stimulation of TEK expression by HUVECs. Conclusions: We provide further evidence for PCG caused by TEK haploinsufficiency, affirm autosomal dominant inheritance in two pedigrees, and propose SVEP1 as a modifier of TEK expression during SC development, affecting disease penetrance and severity
Molecular and life-history effects of a natural toxin on herbivorous and non-target soil arthropods
- Author
- A Conesa
- A. E. Elaine van Ommen Kloeke
- AK Dutta-Roy
- AL Gimsing
- AL Gimsing
- BA Halkier
- Bjarne Styrishave
- CA Edwards
- CC Hoerger
- CG Mao
- Cornelis A. M. van Gestel
- D Bickel
- DA Wardle
- Dick Roelofs
- F Hahne
- GK Smyth
- GK Smyth
- H Merzendorfer
- HP Egmond van
- ISO
- J Filser
- J Jensen
- J Pentek
- Jacintha Ellers
- JD Hayes
- JN Matthiessen
- K Endlweber
- K Saito
- KL Cheung
- L Haanstra
- L Lazzeri
- LH Heckmann
- M Berg
- M Broerse
- M Leon Paumen
- M Timmermans
- M Traka
- Martin Hansen
- ME Ritchie
- MJ Potter
- MT Fountain
- NM Dam van
- NM Straalen van
- PD Brown
- RJ Hopkins
- RR Sokal
- T Shinoda
- UC Brinch
- Y Benjamini
- ZLL He
- Publication venue
- Springer US
- Publication date
- 01/01/2012
- Field of study
Natural toxins, such as isothiocyanate (ITC), are harmful secondary metabolites produced by plants. Many natural toxins occur in commercial crops, yet their possible negative repercussions on especially non-target soil organisms are largely unknown. This study examined life-history and gene transcriptional responses to 2-phenylethyl ITC on two soil arthropod species: Folsomia candida and Protaphorura fimata. To that end the standardized ISO guideline for ecotoxicological tests and a microarray for F. candida were used. The dissipation of 2-phenylethyl ITC in natural soil was investigated using GC-MS/MS for quantification. Half-lives, tested at four concentration levels in natural soil, were on average 16Â h with biodegradation as the plausible main removal process. Regardless, toxic effects on reproduction were shown for F. candida and P. fimata, with EC50 values of around 11.5Â nmol/g soil illustrating the toxic character of this compound. Gene expression profiles revealed the importance of fatty acid metabolism at low exposure concentrations (EC10), which is associated with the lipophilic nature of 2-phenylethyl ITC. At higher concentrations (EC50) gene expression became more ubiquitous with over-expression of especially stress-related genes and sugar metabolism. The regulation of a gene encoding a precursor of follistatin, furthermore, implied the inhibition of reproduction and may be an important molecular target that can be linked to the observed adverse effect of life-history traits
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
- 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
- Akdogana T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama A
- Aktas 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
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
- Almenar CC
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- 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
- Asner D
- 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
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Barrillon P
- Bartoldus R
- Barton AE
- 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
- Bechtle P
- Beck GA
- Beck HP
- 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
- Ben Ami S
- Benary O
- Benchekroun D
- Benchouk C
- Bendel M
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Beretta M
- 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
- Boeriu 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
- Broggi F
- Bromberg C
- Brooijmans G
- Brooks WK
- Brown G
- Brown H
- Bruncko D
- Bruneliere R
- Brunet S
- Bruni A
- Bruni G
- Bruschi M
- BScher V
- Buanes T
- Bucci F
- Buchanan J
- Buchanan NJ
- Buchholz P
- Buckingham RM
- Buckley AG
- Buda SI
- Budagov IA
- Budick B
- 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
- Caballero J
- Caforio D
- Cakir IT
- Cakir O
- Calafiura P
- Calderini G
- Calfayan P
- Calkins R
- Caloba LP
- Caloi R
- Calvet D
- Calvet S
- Camarri P
- Cambiaghi M
- Cameron D
- Camilocci ES
- Campana S
- Campanelli M
- Canale V
- Canelli F
- Canepaa A
- Cantero J
- Capasso L
- Caprini I
- Caprini M
- Capriotti D
- Capua M
- Caputo R
- Caramarcu C
- Cardarelli R
- Carli T
- Carlino G
- Carminati L
- Caron B
- Caron S
- 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 D
- Cavalli-Sforza M
- Cavasinni V
- Ceradini F
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cetin SA
- Cevenini F
- Chafaq A
- Chakraborty D
- Chan K
- Chapleau B
- Chapman JD
- Chapman JW
- Chareyre E
- Charlton DG
- Chavda V
- Cheatham S
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen S
- Chen T
- Chen X
- Cheng S
- Cheong ALF
- Cheplakov A
- Chepurnov VF
- Chernyatin V
- Cheu E
- Cheung SL
- Chevalier L
- Chiefari G
- Chikovani L
- Childers JT
- Chilingarov A
- Chiodini G
- Chizhov MV
- Choudalakis G
- Chouridou S
- Christidi IA
- Christov A
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Ciapetti G
- Ciba K
- Ciftci AK
- Ciftci R
- Cinca D
- Cindro V
- Ciobotaru MD
- Cioccaa C
- Ciocio A
- Cirilli M
- Citterio M
- Ciubancan M
- Clark A
- Clark PJ
- Cleland W
- Clemens JC
- Clement B
- Clement C
- Clifft RW
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Codina EP
- Coe P
- Cogan JG
- Coggeshall J
- Cogneras E
- Cojocaru CD
- Colas J
- Colijn AP
- Collaboration ATLAS
- Collard C
- Collins NJ
- Collins-Tooth C
- Collot J
- Colon G
- Coniavitis E
- Conidi MC
- Consonni M
- Consorti V
- Constantinescu S
- Conta C
- Conventi F
- Cook J
- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Copic K
- Cornelissen T
- Corradi M
- Correia AMH
- Corriveau F
- Corso-Radu A
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Costin T
- Cote D
- Courneyea L
- Cowan G
- Cowden C
- Cox BE
- Cranmer K
- Cranshaw J
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Crosetti G
- Crupi R
- Cuciuc 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 Costa JGPF
- Da Silva PVM
- Da Via C
- Dabrowski W
- Dai T
- Dallapiccola C
- Daly CH
- Dam M
- Damazio DO
- Dameri M
- Damiani DS
- Danielsson HO
- Dannheim D
- Dao V
- Darbo G
- Darlea GL
- Daum C
- Dauvergne JP
- Davey W
- Davidek T
- Davidson N
- Davidson R
- Davies E
- Davies M
- Davison AR
- Davygora Y
- Dawe E
- Dawson I
- Dawson JW
- Daya-Ishmukhametova RK
- de Asmundis R
- De Castro S
- De Cecco S
- De Graat J
- De Groot N
- De Jong P
- De la Hoz SG
- De la Taille C
- De la Torre H
- De Lima JGR
- De Lotto B
- De Mora L
- De Nooij L
- De Pedis D
- De Regie JBDV
- De Renstrom PAB
- De Salvo 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
- Del Prete T
- Deliyergiyev M
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- Della Porta GZ
- della Volpe D
- Delmastro M
- Delpierre P
- Delruelle N
- Delsart PA
- Deluca C
- Demers S
- Demichev M
- Demirkoz B
- Deng J
- Deng W
- Denis RDS
- Denisov SP
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Devetak E
- Deviveiros PO
- Dewhurst A
- DeWilde B
- Dhaliwal S
- Dhullipudi R
- Di Ciaccio A
- Di Ciaccio L
- Di 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
- Diblen F
- Diehl EB
- Dietrich J
- Dietzscha TA
- Diglio S
- Dingfelder J
- Dionisi C
- Dita P
- Dita S
- Dittus F
- Djama F
- Djobava T
- do Vale MAB
- Do ValleWemans A
- Doan TKO
- Dobbs M
- Dobinson R
- Dobos D
- Dobson E
- Dobson M
- Dodd J
- Doglioni C
- Doherty T
- Dohmae T
- Doi Y
- Dolejsi J
- Dolenc I
- Dolezal Z
- Dolgoshein BA
- Donadelli M
- Donega M
- Donini J
- Donszelmann TC
- Dopke J
- Doria A
- Dos Anjos A
- Dos Santos DR
- Dosil M
- Dotti A
- Dova MT
- Dowell JD
- Doxiadis AD
- Doyle AT
- Drasal Z
- Drees J
- Dressnandt N
- Drevermann H
- Driouichi C
- Dris M
- Dubbert J
- Dubbs T
- Dube S
- Duchovni E
- Duckeck G
- Dudarev A
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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
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at â s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fbâ1 of â s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Search for high-mass resonances decaying to dilepton final states in pp collisions at sâ=7 TeV with the ATLAS detector
- Author
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- Yilmaz M
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- Zaidan R
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- Zajacova Z
- Zanello L
- Zanzi D
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- Zhao Z
- 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
- 01/01/2012
- Field of study
The ATLAS detector at the Large Hadron Collider is used to search for high-mass resonances decaying to an electron-positron pair or a muon-antimuon pair. The search is sensitive to heavy neutral ZâČ gauge bosons, Randall-Sundrum gravitons, Z * bosons, techni-mesons, Kaluza-Klein Z/Îł bosons, and bosons predicted by Torsion models. Results are presented based on an analysis of pp collisions at a center-of-mass energy of 7 TeV corresponding to an integrated luminosity of 4.9 fbâ1 in the e + e â channel and 5.0 fbâ1 in the ÎŒ + ÎŒ âchannel. A Z âČ boson with Standard Model-like couplings is excluded at 95 % confidence level for masses below 2.22 TeV. A Randall-Sundrum graviton with coupling k/MPl=0.1 is excluded at 95 % confidence level for masses below 2.16 TeV. Limits on the other models are also presented, including Technicolor and Minimal ZâČ Models
Observation of associated near-side and away-side long-range correlations in âsNN=5.02ââTeV proton-lead collisions with the ATLAS detector
- Author
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- Yilmaz M
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- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJ
- Youssef S
- Yu D
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- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- ZeniĆĄ T
- Zerwas D
- Zevi Della Porta G
- Zhang D
- Zhang H
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- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
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- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- ZivkoviÄ L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (ÎÏ) and pseudorapidity (Îη) are measured in âsNN=5.02ââTeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1ââÎŒb-1 of data as a function of transverse momentum (pT) and the transverse energy (ÎŁETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Îη|<5) ânear-sideâ (ÎÏâŒ0) correlation that grows rapidly with increasing ÎŁETPb. A long-range âaway-sideâ (ÎÏâŒÏ) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ÎŁETPb, is found to match the near-side correlation in magnitude, shape (in Îη and ÎÏ) and ÎŁETPb dependence. The resultant ÎÏ correlation is approximately symmetric about Ï/2, and is consistent with a dominant cosâĄ2ÎÏ modulation for all ÎŁETPb ranges and particle pT
Search for R-parity-violating supersymmetry in events with four or more leptons in sqrt(s) =7 TeV pp collisions with the ATLAS detector
- Author
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- Yamanaka T
- Yamazaki T
- Yamazaki Y
- Yan Z
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- 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
- Young CJ
- Youssef S
- Yu D
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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
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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 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
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