703 research outputs found
Prevalence and Risk Factors of Lassa Seropositivity in Inhabitants of the Forest Region of Guinea: A Cross-Sectional Study
- Author
- Aristide Aplogan
- C Akoua-Koffi
- DE Carey
- DG Bausch
- DW Fraser
- E Fichet-Calvet
- E Fichet-Calvet
- E Lecompte
- EH Stephenson
- Elisabeth Fichet-Calvet
- GS Bowen
- H Wulff
- IS Lukashevich
- J Ter Meulen
- J ter Meulen
- JB McCormick
- JB McCormick
- JD Frame
- Kekoura Koulemou
- Lamine Koivogui
- LL Rodriguez
- LS Lukashevich
- MD Bajani
- MH Monson
- MT Jay
- N'Faly Magassouba
- Philippe J. Guerin
- Rebecca F. Grais
- Rosamund Lewis
- RT Emond
- S Atkin
- S Gunther
- S Gunther
- S Saltzmann
- Serap Aksoy
- SH Khan
- Solen Kernéis
- SP Fisher-Hoch
- SP Fisher-Hoch
- TG Ksiazek
- TP Monath
- TP Monath
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2009
- Field of study
Lassa fever is a viral haemorrhagic fever endemic in West Africa, mainly transmitted to humans by multimammate rats. Several modes of virus transmission are suspected: aerosolisation of the virus, contact with infected rodent excreta, and consumption of rodent meat. Person-to-person transmission also occurs via contact with body fluids of infected persons (blood, urine) and is responsible for numerous outbreaks, mostly in healthcare facilities. Our objective was to precisely describe risk factors for Lassa fever in both rural and urban communities of forest Guinea. For each participant, a standardized questionnaire was completed and a blood sample tested for Lassa virus antibodies. A total of 1424 subjects were interviewed and 977 blood samples tested. The prevalence of Lassa virus antibodies was estimated at 12.9% and 10.0% in rural and urban areas, respectively. The two risk factors were: to have, in the past twelve months, undergone an injection, or lived with someone displaying a haemorrhage. Contrary to our expectation, no factors related to contact with rodents were identified. It is still probable that transmission occurs via indirect contact between rodents and humans in households, but our results highlight the importance of person-to-person transmission via close contact and nosocomial exposure
Treatment of Late Stage Disease in a Model of Arenaviral Hemorrhagic Fever: T-705 Efficacy and Reduced Toxicity Suggests an Alternative to Ribavirin
- Author
- BB Gowen
- BB Gowen
- BB Gowen
- BB Gowen
- Brian B. Gowen
- DA Enria
- DF Smee
- Donald F. Smee
- FA Murphy
- JB McCormick
- JD Morrey
- Jeffery O. Hall
- John D. Morrey
- John R. Stevens
- K Takahashi
- Kevin W. Bailey
- Kie-Hoon Jung
- KT McKee Jr
- L Borio
- L Hedstrom
- LJ Reed
- LS Folley
- M Buchmeier
- Min-Hui Wong
- PE Kilgore
- Peter Sommer
- RH Kenyon
- RH Kenyon
- RW Sidwell
- S Delgado
- S Gunther
- S Rubinstein
- SH Khan
- Y Furuta
- Yousuke Furuta
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2008
- Field of study
A growing number of arenaviruses are known to cause viral hemorrhagic fever (HF), a severe and life-threatening syndrome characterized by fever, malaise, and increased vascular permeability. Ribavirin, the only licensed antiviral indicated for the treatment of certain arenaviral HFs, has had mixed success and significant toxicity. Since severe arenaviral infections initially do not present with distinguishing symptoms and are difficult to clinically diagnose at early stages, it is of utmost importance to identify antiviral therapies effective at later stages of infection. We have previously reported that T-705, a substituted pyrazine derivative currently under development as an anti-influenza drug, is highly active in hamsters infected with Pichinde virus when the drug is administered orally early during the course of infection. Here we demonstrate that T-705 offers significant protection against this lethal arenaviral infection in hamsters when treatment is begun after the animals are ill and the day before the animals begin to succumb to disease. Importantly, this coincides with the time when peak viral loads are present in most organs and considerable tissue damage is evident. We also show that T-705 is as effective as, and less toxic than, ribavirin, as infected T-705-treated hamsters on average maintain their weight better and recover more rapidly than animals treated with ribavirin. Further, there was no added benefit to combination therapy with T-705 and ribavirin. Finally, pharmacokinetic data indicate that plasma T-705 levels following oral administration are markedly reduced during the latter stages of disease, and may contribute to the reduced efficacy seen when treatment is withheld until day 7 of infection. Our findings support further pre-clinical development of T-705 for the treatment of severe arenaviral infections
A human brainstem glioma xenograft model enabled for bioluminescence imaging
- Author
- A Broniscer
- A Rehemtulla
- Anuradha Banerjee
- BS Carson Sr
- C Giannini
- Charles D. James
- E Dinca
- Eduard B. Dinca
- G Yaz
- GH Huynh
- GI Jallo
- GI Jallo
- HS Gunther
- J Lee
- JL Finlay
- JN Sarkaria
- K Hasegawa
- K Tokuda
- M Edinger
- Michael D. Prados
- Nalin Gupta
- NG Avgeropoulos
- P Oztopcu
- PF Recinos
- Q Wu
- R Hashizume
- RG Thorne
- Rintaro Hashizume
- RJ Gilbertson
- S Gross
- SH Kang
- T Ozawa
- T Ozawa
- T Ozawa
- T Ozawa
- Tomoko Ozawa
- Publication venue
- Springer US
- Publication date
- 01/01/2009
- Field of study
Despite the use of radiation and chemotherapy, the prognosis for children with diffuse brainstem gliomas is extremely poor. There is a need for relevant brainstem tumor models that can be used to test new therapeutic agents and delivery systems in pre-clinical studies. We report the development of a brainstem-tumor model in rats and the application of bioluminescence imaging (BLI) for monitoring tumor growth and response to therapy as part of this model. Luciferase-modified human glioblastoma cells from five different tumor cell sources (either cell lines or serially-passaged xenografts) were implanted into the pontine tegmentum of athymic rats using an implantable guide-screw system. Tumor growth was monitored by BLI and tumor volume was calculated by three-dimensional measurements from serial histopathologic sections. To evaluate if this model would allow detection of therapeutic response, rats bearing brainstem U-87 MG or GS2 glioblastoma xenografts were treated with the DNA methylating agent temozolomide (TMZ). For each of the tumor cell sources tested, BLI monitoring revealed progressive tumor growth in all animals, and symptoms caused by tumor burden were evident 26â29Â days after implantation of U-87 MG, U-251 MG, GBM6, and GBM14 cells, and 37â47Â days after implantation of GS2 cells. Histopathologic analysis revealed tumor growth within the pons in all rats and BLI correlated quantitatively with tumor volume. Variable infiltration was evident among the different tumors, with GS2 tumor cells exhibiting the greatest degree of infiltration. TMZ treatment groups were included for experiments involving U-87 MG and GS2 cells, and in each case TMZ delayed tumor growth, as indicated by BLI monitoring, and significantly extended survival of animal subjects. Our results demonstrate the development of a brainstem tumor model in athymic rats, in which tumor growth and response to therapy can be accurately monitored by BLI. This model is well suited for pre-clinical testing of therapeutics that are being considered for treatment of patients with brainstem tumors
Unexpected High Digestion Rate of Cooked Starch by the Ct-Maltase-Glucoamylase Small Intestine Mucosal α-Glucosidase Subunit
- Author
- A Dahlqvist
- A Dahlqvist
- A Dahlqvist
- A Faraj
- A Ă kerberg
- AH-M Lin
- AKE Akerberg
- AM Ugolev
- AM Ugolev
- Amy Hui-Mei Lin
- BL Nichols
- BL Nichols
- BL Nichols
- Bruce R. Hamaker
- Buford L. Nichols
- BV McCleary
- D French
- David R. Rose
- E Lebenthal
- EH Van Beers
- F Saura-Calixto
- G Semenza
- G Semenza
- H Englyst
- H Heymann
- H Heymann
- H-J Chung
- Hassan Y. Naim
- HB McMichael
- HN Englyst
- HN Englyst
- I Goni
- J Larner
- JF Robyt
- JG Muir
- Juliet Ann Gerrard
- K Hiromi
- L Sim
- Lyann Sim
- Megazyme
- MG Sajilata
- P Layer
- P McClean
- P Trinder
- R Quezada-Calvillo
- R Quezada-Calvillo
- R Quezada-Calvillo
- RC Eerlingen
- RC Eerlingen
- Roberto Quezada-Calvillo
- S Gunther
- S Gunther
- S Hizukuri
- SH SĂRensen
- SJ Henning
- SJ Henning
- Stephen E. Avery
- Z Ao
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
For starch digestion to glucose, two luminal α-amylases and four gut mucosal α-glucosidase subunits are employed. The aim of this research was to investigate, for the first time, direct digestion capability of individual mucosal α-glucosidases on cooked (gelatinized) starch. Gelatinized normal maize starch was digested with N- and C-terminal subunits of recombinant mammalian maltase-glucoamylase (MGAM) and sucrase-isomaltase (SI) of varying amounts and digestion periods. Without the aid of α-amylase, Ct-MGAM demonstrated an unexpected rapid and high digestion degree near 80%, while other subunits showed 20 to 30% digestion. These findings suggest that Ct-MGAM assists α-amylase in digesting starch molecules and potentially may compensate for developmental or pathological amylase deficiencies
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
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- Bruncko D
- Bruneliere R
- Brunet S
- Bruni A
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- 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
- Dudziak F
- Duehrssen M
- Duerdoth IP
- Dueren M
- Duflot L
- Dufour M-A
- Dunford M
- Duxfield R
- Dwuznik M
- Dydak F
- Ebenstein WL
- Ebke J
- Eckert S
- Eckweiler S
- Edmonds K
- Edwards CA
- Edwards NC
- Ehrenfeld W
- Ehrich T
- Eifert T
- Eigen G
- Einsweiler K
- Eisenhandler E
- Ekelof T
- El Kacimi M
- El Moursli RC
- Ellert M
- Elles S
- Ellinghaus F
- Ellis K
- Ellis N
- Elmsheuser J
- Elsing M
- Emeliyanov D
- Engelmann R
- Engl A
- Epp B
- Eppig A
- Erdmann J
- Ereditato A
- Eriksson D
- Ernst J
- Ernst M
- Ernwein J
- Errede D
- Errede S
- Ertel E
- Escalier M
- Eschrich IG
- Escobar C
- Esposito B
- Etienne F
- Etienvre AI
- Etzion E
- Evangelakou D
- Evans H
- Fabbri L
- Fabre C
- Fajardo LSG
- Fakhrutdinov RM
- FalCiano S
- Fang Y
- Fanti M
- Farbin A
- Farilla A
- Farley J
- Farooque T
- Farrington SM
- Farthouat P
- Fassnacht P
- Fassouliotis D
- Fatholahzadeh B
- Favareto A
- Fayard L
- Fazio S
- Febbraro R
- Federic P
- Fedin OL
- Fedorko W
- Fehling-Kaschek M
- Feligioni L
- Fellmann D
- Felzmann CU
- Feng EJ
- Fengd C
- Fenyuk AB
- Ferencei J
- Ferland J
- Fernando W
- Ferrag S
- Ferrando BMS
- Ferrando J
- Ferrara V
- Ferrari A
- Ferrari P
- Ferrari R
- Ferrer A
- Ferrer JAV
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- Yilmaz M
- Yoosootiniya R
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- Zhemchugov A
- Zheng S
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- Zieminska D
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- Zinonos Z
- Ziolkowski M
- Zitoun R
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- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- 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 inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV 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
- Ackers M
- 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
- Alam MA
- Alam MS
- Albrand S
- Aleksa M
- Aleksandrov IN
- Aleppo M
- 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
- Alonso J
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- 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
- Antonelli S
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arms KE
- Armstrong SR
- 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
- Auerbach B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avramidou R
- Axen D
- Ay C
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
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
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abi B
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abulaitia Y
- Acharya BS
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- Adelman J
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- Aguilar-Saavedra JA
- Agustoni M
- Ahlen SP
- Ahmadov F
- Aielli G
- Akesson TP
- Akimoto G
- Akimov AV
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- Alconada Verzini MJ
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- Aleksandrov IN
- Alexa C
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- Alexandre G
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- Allbrooke BMM
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- Allport PP
- Allwood-Spiers SE
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- Dewhurst A
- Dhaliwal S
- Di Ciaccio A
- Di Ciaccio L
- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Girolamo B
- Di Mattia A
- Di Micco B
- Di Nardo R
- Di Simone A
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- Djama F
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- do Vale MAB
- Doan TKO
- Dobos D
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- Doglioni C
- Doherty T
- Dohmae T
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- Dolezal Z
- Dolgoshein BA
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- Dubreuil E
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- Dueren M
- Duflot L
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- Dunford M
- Dwuznik M
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- Eigen G
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- Ekelof T
- El Kacimi M
- El Moursli A
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- Ellert M
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- Ellinghaus F
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- Ellis N
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- Elmsheuser J
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- Elsing M
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- Emeliyanov D
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- Enari Y
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- Endner OC
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- Endo M
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- Engelmann R
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- Erdmann J
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- Ereditato A
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- Eriksson D
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- Ernis G
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- Ernwein J
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- Errede D
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- Errede S
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- Ertel E
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- Escalier M
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- Esch H
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- Escobar C
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- Espinal Curull X
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- Esposito B
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- Etienne F
- Etienne F
- Etienvre AI
- Etienvre AI
- Etzion E
- Etzion E
- Evans H
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- Fabbri L
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- Facini G
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- Fakhrutdinov RM
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- Falciano S
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- Faltova J
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- Fang Y
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- Fanti M
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- Farbin A
- Farbin A
- Farilla A
- Farilla A
- Farooque T
- Farooque T
- Farrell S
- Farrell S
- Farrington SM
- Farrington SM
- Farthouat P
- Farthouat P
- Fassi F
- Fassi F
- Fassnacht P
- Fassnacht P
- Fassouliotis D
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- Favareto A
- Favareto A
- Fayard L
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- Federic P
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- Fedin OL
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- Fedorko W
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- Fehling-Kaschek M
- Fehling-Kaschek M
- Feigl S
- Feigl S
- Feligioni L
- Feligioni L
- Feng C
- Feng C
- Feng EJ
- Feng EJ
- Feng H
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- Fenyuk AB
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- Fernando W
- Fernando W
- Ferrag S
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- Ferrando BMS
- Ferrando J
- Ferrando J
- Ferrara V
- Ferrara V
- Ferrari A
- Ferrari A
- Ferrari P
- Ferrari P
- Ferrari R
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- Ferrer A
- Ferrer A
- Ferrere D
- Ferrere D
- Ferretti C
- Ferretti C
- Fiascaris M
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- Fiedler F
- Fiedler F
- Filipcic A
- Filipcic A
- Filipuzzi M
- Filipuzzi M
- Filthaut F
- Filthaut F
- Fincke-Keeler M
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- Finelli KD
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- Fiolhais MCN
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- Fiorini L
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- Firan A
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- Fischer J
- Fischer J
- Fisher MJ
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- Fitzgerald EA
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- Flechl M
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- Fleck I
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- Fleischmann P
- Fleischmann P
- Fleischmann S
- Fleischmann S
- Fletcher G
- Fletcher G
- Fletcher GT
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- Flick T
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- 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
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- Francavilla P
- Francavilla P
- Franchini M
- Franchini M
- Franchino S
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- Francis D
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- Franklin M
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- Franz S
- Franz S
- Fraternali M
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- Fratin S
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- French ST
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- Friedrich C
- Friedrich C
- Friedrich F
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- Froidevaux D
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- Frost JA
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- Fulsom BG
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- Gabizon O
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- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gabrielli A
- Gadatsch S
- Gadatsch S
- Gadomski S
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- Gagliardi G
- Gagliardi G
- Gagnon P
- Gagnon P
- Galea C
- Galea C
- Galhardo B
- Galhardo B
- Gallas EJ
- Gallas EJ
- Gallo V
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- Gallop BJ
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- Gallus P
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- Gandrajula RP
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- Gao J
- Gao YS
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- Gaob J
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- Garcia Navarro JE
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- Garcia BRM
- Garcia C
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- Garcia JAB
- Garcia-Sciveres M
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- Gardner RW
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- Garelli N
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- Garonne V
- Garonne V
- Garrido MDMC
- Gatti C
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- Gaudio G
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- Gaur B
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- Gauthier L
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- Gauzzi P
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- Gavrilenko IL
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- Gay C
- Gay C
- Gaycken G
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- Gazis EN
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- Ge P
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- Gecse Z
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- Gee CNP
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- Geerts DAA
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- Geich-Gimbel C
- Geich-Gimbel C
- Gellerstedt K
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- Gemme C
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- Gemmell A
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- Genest MH
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- Gentile S
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- George M
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- George S
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- Gerbaudo D
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- Gershon A
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- Ghazlane H
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- Ghodbane N
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- Giacobbe B
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- Giagu S
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- Giangiobbe V
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- Giannetti P
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- Gianotti F
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- Gibbard B
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- Gillam TPS
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- Gillberg D
- Gillberg D
- Gillman AR
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- Gingrich DM
- Gingrich M
- Giokaris N
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- Giordani MP
- Giordani MP
- Giordano R
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- Giorgi FM
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- Giraud PF
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- Giugni D
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- Giuliani C
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- Giunta M
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- Gjelsten BK
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- Gorini E
- Gorini E
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- Gornicki E
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- Goshaw AT
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- Gostkin MI
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- Gratchev V
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- Yang H
- Yang UK
- Yang Y
- Yanush S
- Yao L
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yen AL
- Yildirim E
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Yoshihara K
- Young C
- Young CJS
- Youssef S
- Yu DR
- Yu J
- Yu J
- Yu JM
- Yuan L
- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
- Zhou L
- Zhou N
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- 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 direct pair production of the top squark in all-hadronic final states in proton-proton collisions at sâ=8 TeV with the ATLAS detector
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- Zhemchugov A
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- Zurzolo G
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The results of a search for direct pair production of the scalar partner to the top quark using an integrated luminosity of 20.1fbâ1 of protonâproton collision data at âs = 8 TeV recorded with the ATLAS detector at the LHC are reported. The top squark is assumed to decay via tËâtÏË01 or tËâ bÏ˱1 âbW(â)ÏË01 , where ÏË01 (Ï˱1 ) denotes the lightest neutralino (chargino) in supersymmetric models. The search targets a fully-hadronic final state in events with four or more jets and large missing transverse momentum. No significant excess over the Standard Model background prediction is observed, and exclusion limits are reported in terms of the top squark and neutralino masses and as a function of the branching fraction of tË â tÏË01 . For a branching fraction of 100%, top squark masses in the range 270â645 GeV are excluded for ÏË01 masses below 30 GeV. For a branching fraction of 50% to either tË â tÏË01 or tË â bÏ˱1 , and assuming the Ï˱1 mass to be twice the ÏË01 mass, top squark masses in the range 250â550 GeV are excluded for ÏË01 masses below 60 GeV
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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- Yang UK
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- Yanush S
- Yao L
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- Yilmaz M
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- Youssef S
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- Zaidan R
- Zaitsev AM
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- ZeniĆĄ T
- Zerwas D
- Zevi Della Porta G
- Zhang D
- Zhang H
- Zhang J
- Zhang L
- Zhang X
- Zhang Z
- Zhao L
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- ZivkoviÄ L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (ÎÏ) and pseudorapidity (Îη) are measured in âsNN=5.02ââTeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1ââÎŒb-1 of data as a function of transverse momentum (pT) and the transverse energy (ÎŁETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Îη|<5) ânear-sideâ (ÎÏâŒ0) correlation that grows rapidly with increasing ÎŁETPb. A long-range âaway-sideâ (ÎÏâŒÏ) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ÎŁETPb, is found to match the near-side correlation in magnitude, shape (in Îη and ÎÏ) and ÎŁETPb dependence. The resultant ÎÏ correlation is approximately symmetric about Ï/2, and is consistent with a dominant cosâĄ2ÎÏ modulation for all ÎŁETPb ranges and particle pT
Influence of calcination temperature on structural and magnetic properties of nanocomposites formed by Co-ferrite dispersed in sol-gel silica matrix using tetrakis(2-hydroxyethyl) orthosilicate as precursor
- Author
- AC Pierre
- AK Giri
- AK Giri
- BD Cullity
- C Caizer
- CJ Brinker
- CL Chien
- DW Johnson
- E Manova
- E Veena Gopalan
- H Izutsu
- I Anton
- I Gill
- J Popplewell
- J Wang
- JH Paterson
- JMD Coey
- K Raj
- KH Wu
- KH Wu
- KI Arshak
- KVPM Shafi
- L Guang-She
- L Gunther
- M Gharagozlou
- M Lal
- M Meyer
- M Rajendran
- Mehrnaz Gharagozlou
- MH Kryder
- NA Grigorieva
- NDS Mohallem
- P Priyadharsini
- P Ravindranathan
- RD McMickael
- S Ammar
- SH Xiao
- SM Prokes
- V Pillai
- X Huang
- XH Huang
- XH Huang
- Y Shi
- Y Wang
- YP Sui
- ZH Zhou
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
Effects of calcination temperatures varying from 400 to 1000°C on structural and magnetic properties of nanocomposites formed by Co-ferrite dispersed in the sol-gel silica matrix using tetrakis(2-hydroxyethyl) orthosilicate (THEOS) as water-soluble silica precursor have been investigated. Studies carried out using XRD, FT-IR, TEM, STA (TG-DTG-DTA) and VSM techniques. Results indicated that magnetic properties of samples such as superparamagnetism and ferromagnetism showed great dependence on the variation of the crystallinity and particle size caused by the calcination temperature. The crystallization, saturation magnetization Ms and remenant magnetization Mr increased as the calcination temperature increased. But the variation of coercivity Hc was not in accordance with that of Ms and Mr, indicating that Hc is not determined only by the crystallinity and size of CoFe2O4 nanoparticles. TEM images showed spherical nanoparticles dispersed in the silica network with sizes of 10-30 nm. Results showed that the well-established silica network provided nucleation locations for CoFe2O4 nanoparticles to confinement the coarsening and aggregation of nanoparticles. THEOS as silica matrix network provides an ideal nucleation environment to disperse CoFe2O4 nanoparticles and thus to confine them to aggregate and coarsen. By using THEOS as water-soluble silica precursor over the currently used TEOS and TMOS, the organic solvents are not needed owing to the complete solubility of THEOS in water. Synthesized nanocomposites with adjustable particle sizes and controllable magnetic properties make the applicability of Co-ferrite even more versatile
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