880 research outputs found
A thyroid hormone regulated asymmetric responsive centre is correlated with eye migration during flatfish metamorphosis
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/08/2018
- Field of study
Flatfish metamorphosis is a unique post-embryonic developmental event in which thyroid hormones (THs) drive the development of symmetric pelagic larva into asymmetric benthic juveniles. One of the eyes migrates to join the other eye on the opposite side of the head. Developmental mechanisms at the basis of the acquisition of flatfish anatomical asymmetry remain an open question. Here we demonstrate that an TH responsive asymmetric centre, determined by deiodinase 2 expression, ventrally juxtaposed to the migrating eye in sole (Solea senegalensis) correlates with asymmetric cranial ossification that in turn drives eye migration. Besides skin pigmentation that is asymmetric between dorsal and ventral sides, only the most anterior head region delimited by the eyes becomes asymmetric whereas the remainder of the head and organs therein stay symmetric. Sub-ocular ossification is common to all flatfish analysed to date, so we propose that this newly discovered mechanism is universal and is associated with eye migration in all flatfish.Fundacao para a Ciencia e Tecnologia (FCT) [SFRH/BPD/66808/2009, IF/01274/2014]; FCT [SFRH/BPD/79105/2011, SFRH/BPD/89889/2012, PTDC/MAR/115005/2009, PEst-C/MAR/LA0015/2011, UID/Multi/04326/2013, Pest-OE/EQB/LA0023/2013, UID/BIM/04773/2013]; European Regional Development Fund through COMPETE; INIA; EU [RTA2013-00023-C02-01
Search for CP violation in D0 and D+ decays
- Author
- JM. Link
- VS. Paolone
- M. Reyes
- PM. Yager
- JC. Anjos
- I. Bediaga
- C. Gobel
- J. Magnin
- JM. de Miranda
- IM. Pepe
- AC. dos Reis
- FRA. Simao
- S. Carrillo
- E. Casimiro
- H. Mendez
- A. Sanchez-Hernandez
- C. Uribe
- F. Vazquez
- L. Cinquini
- JP. Cumalat
- JE. Ramirez
- B. O'Reilly
- EW. Vaandering
- JN. Butler
- HWK. Cheung
- I. Gaines
- PH. Garbincius
- LA. Garren
- E. Gottschalk
- SA. Gourlay
- PH. Kasper
- AE. Kreymer
- S. Bianco
- FL. Fabbri
- S. Sarwar
- A. Zallo
- C. Cawlfield
- R. Kutschke
- DY. Kim
- KS. Park
- A. Rahimi
- J. Wiss
- R. Gardner
- YS. Chung
- JS. Kang
- BR. Ko
- JW. Kwak
- KB. Lee
- SS. Myung
- H. Park
- G. Alimonti
- M. Boschini
- D. Brambilla
- B. Caccianiga
- A. Calandrino
- P. D'Angelo
- M. DiCorato
- P. Dini
- M. Giammarchi
- P. Inzani
- F. Leveraro
- S. Malvezzi
- D. Menasce
- M. Mezzadri
- L. Milazzo
- L. Moroni
- D. Pedrini
- F. Prelz
- M. Rovere
- A. Sala
- S. Sala
- TF. Davenport
- V. Arena
- G. Boca
- G. Bonomi
- G. Gianini
- G. Liguori
- M. Merlo
- D. Pantea
- SP. Ratti
- C. Riccardi
- P. Torre
- L. Viola
- P. Vitulo
- H. Hernandez
- AM. Lopez
- L. Mendez
- A. Mirles
- E. Montiel
- D. Olaya
- J. Quinones
- C. Rivera
- Y. Zhang
- N. Copty
- M. Purohit
- JR. Wilson
- K. Cho
- T. Handler
- D. Engh
- WE. Johns
- M. Hosack
- MS. Nehring
- M. Sales
- PD. Sheldon
- K. Stenson
- MS. Webster
- M. Sheaff
- YJ. Kwon
- Publication venue
- Publication date
- 01/01/2000
- Field of study
A high statistics sample of photoproduced charm particles from the FOCUS
(E831) experiment at Fermilab has been used to search for CP violation in the
Cabibbo suppressed decay modes D+ to K-K+pi+, D0 to K-K+ and D0 to pi-pi+. We
have measured the following CP asymmetry parameters: A_CP(K-K+pi+) = +0.006 +/-
0.011 +/- 0.005, A_CP(K-K+) = -0.001 +/- 0.022 +/- 0.015 and A_CP(pi-pi+) =
+0.048 +/- 0.039 +/- 0.025 where the first error is statistical and the second
error is systematic. These asymmetries are consistent with zero with smaller
errors than previous measurements.Comment: 12 pages, 4 figure
A Study of D0 --> K0(S) K0(S) X Decay Channels
- Author
- A. Cerutti
- A. Kryemadhi
- A. Massafferri
- A. Paris
- A. Rahimi
- A. Sanchez-Hernandez
- A. Zallo
- AA. Machado
- AC. dos Reis
- AE. Kreymer
- AM. Lopez
- B. O'Reilly
- BR. Ko
- C. Castromonte
- C. Cawlfield
- C. Gobel
- C. Pontoglio
- C. Riccardi
- C. Uribe
- D. Engh
- D. Menasce
- D. Pantea
- D. Pedrini
- DL. Pegna
- DY. Kim
- E. Casimiro
- E. Cuautle
- E. Gottschalk
- E. Luiggi
- E. Polycarpo
- EW. Vaandering
- F. Leveraro
- F. Prelz
- F. Vazquez
- FL. Fabbri
- G. Alimonti
- G. Boca
- G. Bonomi
- G. Chiodini
- G. Gianini
- G. Liguori
- H. Hernandez
- H. Mendez
- H. Park
- HWK. Cheung
- I. Bediaga
- I. Gaines
- I. Segoni
- IM. Pepe
- J. Magnin
- J. Otalora
- J. Quinones
- J. Wiss
- JC. Anjos
- JE. Ramirez
- JM. de Miranda
- JM. Link
- JN. Butler
- JP. Cumalat
- JR. Wilson
- JS. Kang
- JW. Kwak
- K. Cho
- K. Stenson
- KB. Lee
- L. Agostino
- L. Benussi
- L. Cinquini
- L. Edera
- L. Moroni
- LA. Garren
- M. Boschini
- M. DiCorato
- M. Hosack
- M. Mezzadri
- M. Nehring
- M. Reyes
- M. Rovere
- M. Sheaff
- M. Wang
- M. Webster
- MM. Merlo
- P. D'Angelo
- P. Dini
- P. Inzani
- P. Vitulo
- PD. Sheldon
- PH. Garbincius
- PH. Kasper
- PM. Yager
- R. Gardner
- R. Kutschke
- R. Mitchell
- S. Barberis
- S. Bianco
- S. Carrillo
- S. Erba
- S. Malvezzi
- S. Sala
- SP. Ratti
- T. Handler
- TF. Davenport
- V. Arena
- V. Frisullo
- WE. Johns
- Y. Zhang
- YS. Chung
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2005
- Field of study
Using data from the FOCUS experiment (FNAL-E831), we report on the decay of
D0 mesons into final states containing more than one KS0â. We present
evidence for two Cabibbo favored decay modes, D0âKS0âKS0âKâÏ+ and
D0âKS0âKS0âK+Ïâ, and measure their combined branching fraction
relative to D0âKË0Ï+Ïâ to be Î(D0âKË0Ï+Ïâ)Î(D0âKS0âKS0âK±Ïâ)â = 0.0106
± 0.0019 ± 0.0010. Further, we report new measurements of
Î(D0âKË0Ï+Ïâ)Î(D0âKS0âKS0âKS0â)â =
0.0179 ± 0.0027 ± 0.0026, Î(D0âKË0Ï+Ïâ)Î(D0âK0KË0)â = 0.0144 ± 0.0032 ± 0.0016,
and Î(D0âKË0Ï+Ïâ)Î(D0âKS0âKS0âÏ+Ïâ)â = 0.0208 ± 0.0035 ± 0.0021 where the first error is
statistical and the second is systematic.Comment: 11 pages, 3 figures, typos correcte
Exploring Relationship between Perception Indicators and Mitigation Behaviors of Soil Erosion in Undergraduate Students in Sonora, Mexico
- Author
- Publication venue
- 'MDPI AG'
- Publication date
- 01/08/2021
- Field of study
Soil erosion represents a critical socio-economic and environmental hazard for Mexico and the world. Given that soil erosion is a phenomenon influenced by human activities, it is essential to know the level of cultural perspectives on this matter. An instrument with eight scales was applied to 275 university students from a northwestern Mexican city, which measured the knowledge about soil erosion, self-efficacy in solving the problem, future perspectives, perceived consequences, obstacles to addressing soil erosion, and mitigation intentions and behaviors. To analyze the relationship between the scales and the intentions and behaviors of soil erosion mitigation, a model of structural equations was tested. In summary, the participants know the problem of soil erosion, its impacts, and recognize risks to human and environmental health. They also know their important role within soil conservation; however, they identified significant obstacles to action. This study determined that each indicator has a correlation with soil erosion mitigation intentions except for the obstacles. The indicators that had the greatest positive relationship in mitigation intentions were knowledge, self-efficacy, and the perspective of the future. The implications of these results open the landscape to the creation of efficient strategies to mitigate soil erosion in this region and Mexico.</jats:p
TRANSPORTING CHILDREN IN CARS AND THE USE OF CHILD SAFETY RESTRAINT SYSTEMS
- Author
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
Evaluation of condyle defects using different reconstruction protocols of cone-beam computed tomography
- Author
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- Field of study
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
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- 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
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- Caputo R
- Caramarcu C
- Cardarelli R
- Carli T
- Carlino G
- Carminati L
- Caron B
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- 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
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- 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
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- Yilmaz M
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- Zhemchugov A
- Zheng S
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- Zitoun R
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- 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
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
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- Zhemchugov A
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- Zimin NI
- Zimmermann R
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- Zobernig G
- Zoccoli A
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- 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
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
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- Zhemchugov A
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- Zieminska D
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- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
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- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- 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
Analysis of paternal lineages in Brazilian and African populations
- Author
- Abe-Sandes K
- Alves C
- Arroyo-Pardo E
- Beleza S
- Bento AM
- Bortolini MC
- Cainé L
- Carvalho-Silva DR
- Corte Real F
- Domingues PM
- Excoffier L
- Francisco Corte Real
- GusmĂŁo L
- GusmĂŁo L
- GusmĂŁo L
- GĂłes ACS
- GĂłis CC
- Karafet TM
- Kloosterman AD
- Leite FPN
- Leonor GusmĂŁo
- Lisa Andrade
- Marrero AR
- MartĂn P
- MÂȘ JoĂŁo Anjos
- MĂłnica Carvalho
- Nei M
- Palha TJBF
- Pedro Brito
- Ribeiro D
- Schneider PM
- Silva DA
- SĂĄnchez-Diz P
- Thomas MG
- Toscanini U
- Trovoada MJ
- VirgĂnia Lopes
- Publication venue
- Sociedade Brasileira de Genética
- Publication date
- 01/01/2010
- Field of study
The present-day Brazilian population is a consequence of the admixture of various peoples of very different origins, namely, Amerindians, Europeans and Africans. The proportion of each genetic contribution is known to be very heterogeneous throughout the country. The aim of the present study was to compare the male lineages present in two distinct Brazilian populations, as well as to evaluate the African contribution to their male genetic substrate. Thus, two Brazilian population samples from Manaus (State of Amazon) and RibeirĂŁo Preto (State of SĂŁo Paulo) and three African samples from Guinea Bissau, Angola and Mozambique were typed for a set of nine Y chromosome specific STRs. The data were compared with those from African, Amerindian and European populations. By using Y-STR haplotype information, low genetic distances were found between the Manaus and RibeirĂŁo Preto populations, as well as between these and others from Iberia. Likewise, no significant distances were observed between any of the African samples from Angola, Mozambique and Guinea Bissau. Highly significant Rst values were found between both Brazilian samples and all the African and Amerindian populations. The absence of a significant Sub-Saharan African male component resulting from the slave trade, and the low frequency in Amerindian ancestry Y-lineages in the Manaus and RibeirĂŁo Preto population samples are in accordance with the accentuated gender asymmetry in admixture processes that has been systematically reported in colonial South American populations
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