122 research outputs found
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MRI cross sectional atlas of normal canine cervical musculoskeletal structure
- Publication venue
- Research in Veterinary Science
- Publication date
- 05/10/2016
- Field of study
Although magnetic resonance imaging (MRI) has been increasingly used as a diagnostic tool for cervical spine injuries in canines, a comprehensive normal MRI anatomy of the canine cervical spine muscles is lacking. Therefore, the purpose of this study was to build a magnetic resonance imaging atlas of the normal cross sectional anatomy of the muscles of the canine cervical spine. MRI scans were performed on a canine cadaver using a combination of T1 and T2-weighted images in the transverse, sagittal and dorsal planes acquired at a slice thickness of 1 mm. Muscle contours were traced manually in each slice, using local osseous structures as reference points for muscle identification. Twenty-two muscles were traced in 401 slices in the cervical region. A three dimensional surface model of all the contoured muscles was created to illustrate the complex geometrical arrangement of canine neck muscles. The cross-sectional area of the muscles was measured at the mid-level of each vertebra. The accuracy of the location of the mapped muscles was verified by comparing the sagittal view of the 3D model of muscles with still photographs obtained from anatomic canine cadaver dissection. We believe that this information will provide a unique and valuable resource for veterinary researchers, clinicians and surgeons who wish to evaluate MRI images of the cervical spine. It will also serve as the foundation for ongoing work to develop a computational model of the canine cervical spine in which anatomical information is combined with electromyographic, kinematic and kinetic data.This work was supported in part by Fitzpatrick Referrals Ltd., through the One Health/One Medicine Fellowship at The Ohio State University
Recommended from our members
An EMG-driven biomechanical model of the canine cervical spine
- Publication venue
- Journal of Electromyography and Kinesiology
- Publication date
- 01/02/2017
- Field of study
Due to the frequency of cervical spine injuries in canines, the purpose of this effort was to develop an EMG-driven dynamic model of the canine cervical spine to assess a biomechanical understanding that enables one to investigate the risk of neck disorders. A canine subject was recruited in this investigation in order to collect subject specific data. Reflective markers and a motion capture system were used for kinematic measurement; surface electrodes were used to record electromyography signals, and with the aid of force plate kinetics were recorded. A 3D model of the canine subject was reconstructed from an MRI dataset. Muscles lines of action were defined through a new technique with the aid of 3D white light scanner. The model performed well with a 0.73 weighted R2 value in all three planes. The weighted average absolute error of the predicted moment was less than 10% of the external moment. The proposed model is a canine specific forward-dynamics model that precisely tracks the canine subject head and neck motion, calculates the muscle force generated from the twelve major moment producing muscles, and estimates resulting loads on specific spinal tissues.This work was supported in part by Fitzpatrick Referrals Ltd., through the One Health/One Medicine Fellowship at The Ohio State University
Positively selected amino acid replacements within the RuBisCO enzyme of oak trees are associated with ecological adaptations
- Author
- A Brooks
- A Occhialini
- AE Carmo-Silva
- AR Portis Jr
- Arnau Mir
- ArĂĄntzazu Molins
- C Hermida-Carrera
- C Ishikawa
- CA Raines
- Carmen Hermida-Carrera
- CC Yang
- CM Ott
- D Posada
- D Posada
- D Sancho-Knapik
- DB Jordan
- DJ Orr
- DM Weinreich
- Domingo Sancho-Knapik
- DS Kubien
- E Delgado
- E Kellogg
- Eustaquio Gil-PelegrĂn
- F Ronquist
- F Soleimanian
- FM Codoñer
- G James
- GG Tcherkez
- H Miwa
- H Steinkellner
- HH Yeoh
- HH Yeoh
- I Andersson
- I Kanevski
- J Berry
- J Dutheil
- J Ehleringer
- J Flexas
- J Flexas
- J Galmes
- J Galmes
- J Galmés
- J Galmés
- J Galmés
- J Galmés
- JA Raven
- Jairo Rocha
- JD Thompson
- Jeroni Galmés
- JN Young
- José Javier Peguero-Pina
- JR Seemann
- K Morita
- K Tamura
- K Uemura
- L Breiman
- L Corcuera
- L Sen
- M Makowski
- M Schwabacher
- M Simard
- M Wang
- MA Fares
- Mario A. Fares
- Maxim V. Kapralov
- MC Peel
- MDI Hozain
- MV Kapralov
- MV Kapralov
- MV Kapralov
- MV Kapralov
- O Ghannoum
- P Manos
- PA Christin
- PS Manos
- R Govaerts
- R Nielsen
- R Piredda
- RE Sharwood
- RE Sharwood
- RF Sage
- RJ Ellis
- RJ Spreitzer
- RJ Spreitzer
- S Iida
- S Kato
- S Knight
- S Ueno
- SM Whitney
- SM Whitney
- T Genkov
- TA Hall
- Tzen-Yuh Chiang
- W Yamori
- X Jiang
- XG Zhu
- XG Zhu
- XH Zhang
- Y Savir
- YC Du
- Z Yang
- Z Yang
- Z Yang
- Ăngel FernĂĄndez
- Ă Niinemets
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/01/2017
- Field of study
Phylogenetic analysis by maximum likelihood (PAML) has become the standard approach to study positive selection at the molecular level, but other methods may provide complementary ways to identify amino acid replacements associated with particular conditions. Here, we compare results of the decision tree (DT) model method with ones of PAML using the key photosynthetic enzyme RuBisCO as a model system to study molecular adaptation to particular ecological conditions in oaks (Quercus). We sequenced the chloroplast rbcL gene encoding RuBisCO large subunit in 158 Quercus species, covering about a third of the global genus diversity. It has been hypothesized that RuBisCO has evolved differentially depending on the environmental conditions and leaf traits governing internal gas diffusion patterns. Here, we show, using PAML, that amino acid replacements at the residue positions 95, 145, 251, 262 and 328 of the RuBisCO large subunit have been the subject of positive selection along particular Quercus lineages associated with the leaf traits and climate characteristics. In parallel, the DT model identified amino acid replacements at sites 95, 219, 262 and 328 being associated with the leaf traits and climate characteristics, exhibiting partial overlap with the results obtained using PAML
Charged-particle distributions at low transverse momentum in âs=13 13 TeV pp interactions measured with the ATLAS detector at the LHC
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Aben R
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adam ER
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agricola J
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Alberich LC
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alstaty M
- Alviggi MG
- Amadio BT
- Amako K
- Amelung C
- Amidei D
- Amorim A
- Amoroso S
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjos N
- Annovi A
- Antel C
- Antonelli M
- Antonov A
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Aranda CP
- Araque JP
- Araya ST
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armadans RC
- Armbruster AJ
- Armitage LJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asman B
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Axen B
- Ayoub MK
- Azuelos G
- Baak MA
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Backhaus M
- Bagiacchi P
- Bagnaia P
- Bai Y
- Baines JT
- Baker OK
- Baldin EM
- Balek P
- Balestri T
- Balli F
- Balunas WK
- Banas E
- Banerjee S
- Bannoura AAE
- Barajas CAC
- Barak L
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M-S
- Barklow T
- Barlow N
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batley JR
- Battaglia M
- Bauce M
- Bauer F
- Bawa HS
- Beacham JB
- Beattie MD
- Beau T
- Beauchemin PH
- Bechtle P
- Beck HP
- Becker K
- Becker M
- Beckingham M
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beemster LJ
- Beermann TA
- Begel M
- Behr JK
- Belanger-Champagne C
- Bell AS
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellomo M
- Belotskiy K
- Beltramello O
- Belyaev NL
- Benary O
- Benchekroun D
- Bender M
- Bendtz K
- Benekos N
- Benhammou Y
- Benitez J
- Benjamin DP
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Beringer J
- Berlendis S
- Berlingen JM
- Bernard NR
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertella C
- Bertoli G
- Bertolucci F
- Bertram IA
- Bertsche C
- Bertsche D
- Besjes GJ
- Bessner M
- Besson N
- Betancourt C
- Bethke S
- Bevan AJ
- Bhimji W
- Bianchi RM
- Bianchini L
- Bianco M
- Biebel O
- Biedermann D
- Bielski R
- Biesuz NV
- Biglietti M
- Bilokon H
- Bindi M
- Binet S
- Bingul A
- Bini C
- Biondi S
- Bjergaard DM
- Black CW
- Black JE
- Black KM
- Blackburn D
- Blair RE
- Blanchard J-B
- Blanco JE
- Blazek T
- Bloch I
- Blocker C
- Blum W
- Blumenschein U
- Blunier S
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Bock C
- Boehler M
- Boeriu OEV
- Boerner D
- Bogaerts JA
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
- Boldyrev AS
- Bomben M
- Bona M
- Boonekamp M
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Bortolotto V
- Bos K
- Boscherini D
- Bosman M
- Boudreau J
- Bouffard J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Boutle SK
- Boveia A
- Boyd J
- Boyko IR
- Bracinik J
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Bravo AG
- Brendlinger K
- Brennan AJ
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Bristow TM
- Britton D
- Britzger D
- Brochu FM
- Brock I
- Brock R
- Brooijmans G
- Brooks T
- Brooks WK
- Brosamer J
- Brost E
- Broughton JH
- Bruncko D
- Bruneliere R
- Bruni A
- Bruni G
- Bruni LS
- Brunt BH
- Bruschi M
- Bruscino N
- Bryant P
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buehrer F
- Bugge MK
- Bulekov O
- Bullock D
- Burckhart H
- Burdin S
- Burgard CD
- Burghgrave B
- Burka K
- Burke S
- Burmeister I
- Burr JTP
- Busato E
- Buscher D
- Buscher V
- Bussey P
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund OB
- Caforio D
- Cairo VM
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvet D
- Calvet S
- Calvet TP
- Camarda S
- Camarri P
- Cameron D
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Canepa A
- Cantero J
- Cantrill R
- Cao T
- Caprini I
- Caprini M
- Capua M
- Caputo R
- Carbone RM
- Cardarelli R
- Cardillo F
- Carli I
- Carli T
- Carlino G
- Carminati L
- Caron S
- Carquin E
- Carrillo-Montoya GD
- Carter JR
- Carvalho J
- Casadei D
- Casado MP
- Casolino M
- Casper DW
- Castaneda-Miranda E
- Castelijn R
- Castelli A
- Castillo IS
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cattai A
- Caudron J
- Cavaliere V
- Cavallaro E
- Cavalli D
- Cavalli-Sforza M
- Cavasinni V
- Ceradini F
- Cerio BC
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cerv M
- Cervelli A
- Cetin SA
- Chafaq A
- Chakraborty D
- Chan SK
- Chan YL
- Chang P
- Chapman JD
- Charlton DG
- Chatterjee A
- Chau CC
- Che S
- Cheatham S
- Chegwidden A
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen K
- Chen S
- Chen S
- Chen X
- Chen Y
- Cheng HC
- Cheng HJ
- Cheng Y
- Cheplakov A
- Cheremushkina E
- Chernyatin V
- Cheu E
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chizhov MV
- Choi K
- Chomont AR
- Chouridou S
- Chow BKB
- Christodoulou V
- Chromek-Burckhart D
- Chudoba J
- Chuinard AJ
- Chwastowski JJ
- Chytka L
- Ciapetti G
- Ciftci AK
- Cinca D
- Cindro V
- Cioara IA
- Ciocca C
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubancan M
- Clark A
- Clark BL
- Clark MR
- Clark PJ
- Clarke RN
- Clement C
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Codina EP
- Coffey L
- Colasurdo L
- Cole B
- Colijn AP
- Collaboration ATLAS
- Collot J
- Colombo T
- Compostella G
- Coniavitis E
- Connell SH
- Connelly IA
- Consorti V
- Constantinescu S
- Conti G
- Conventi F
- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Cormier KJR
- Cornelissen T
- Corradi M
- Correia AMH
- Corriveau F
- Corso-Radu A
- Cortes-Gonzalez A
- Cortiana G
- Costa G
- Costa MJ
- Costanzo D
- Cottin G
- Coutinho YA
- Cowan G
- Cox BE
- Cranmer K
- Crawley SJ
- Cree G
- Crepe-Renaudin S
- Crescioli F
- Cribbs WA
- Cristinziani M
- Croft V
- Crosetti G
- Cummings J
- Curatolo M
- Cuth J
- Cuthbert C
- Czirr H
- Czodrowski P
- D'amen G
- D'Auria S
- D'Onofrio M
- da Costa JBG
- Da Costa JGPF
- Da Via C
- Dabrowski W
- Dado T
- Dai T
- Dale O
- Dallaire F
- Dallapiccola C
- Dam M
- Damazio DO
- Dandoy JR
- Dang NP
- Daniells AC
- Dann NS
- Danninger M
- Dao V
- Darbo G
- Darmora S
- Dassoulas J
- Dattagupta A
- Davey W
- David C
- Davidek T
- Davies M
- Davison P
- Dawe E
- Dawson I
- Daya-Ishmukhametova RK
- de Andrade Filho LM
- de Asmundis R
- De Benedetti A
- De Bruin PHS
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- de la Hoz SG
- De la Torre H
- de Lima DEF
- De Lorenzi F
- De Maria A
- De Mendizabal JB
- De Pedis D
- De Regie JBDV
- de Renstrom PAB
- De Salvo A
- De Sanctis U
- De Santo A
- De Sousa MJDCS
- De K
- Dearnaley WJ
- Debbe R
- Debenedetti C
- Dedovich DV
- Dehghanian N
- Deigaard I
- Del Gaudio M
- Del Peso J
- Del Prete T
- Delgado AT
- Delgove D
- Deliot F
- Delitzsch CM
- Deliyergiyev M
- Dell'Acqua A
- Dell'Asta L
- Dell'Orso M
- Della Pietra M
- della Volpe D
- Delmastro M
- Delsart PA
- DeMarco DA
- Demers S
- Demichev M
- Demilly A
- Denis RDS
- Denisov SP
- Denysiuk D
- Derendarz D
- Derkaoui JE
- Derue F
- Dervan P
- Desch K
- Deterre C
- Dette K
- Devesa MR
- Deviveiros PO
- Dewhurst A
- Dhaliwal S
- Di Ciaccio A
- Di Ciaccio L
- Di Clemente WK
- Di Donato C
- Di Girolamo A
- Di Girolamo B
- Di Micco B
- Di Nardo R
- Di Simone A
- Di Sipio R
- Di Valentino D
- Diaconu C
- Diamond M
- Dias FA
- Diaz MA
- Diehl EB
- Dietrich J
- Diglio S
- Dimitrievska A
- Dingfelder J
- Dita P
- Dita S
- Dittus F
- Djama F
- Djobava T
- Djuvsland JI
- do Vale MAB
- Dobos D
- Dobre M
- Doglioni C
- Dohmae T
- Dolejsi J
- Dolezal Z
- Dolgoshein BA
- Donadelli M
- Donati S
- Dondero P
- Donini J
- Donszelmann TC
- Dopke J
- Doria A
- Dos Santos SPA
- Dova MT
- Doyle AT
- Drechsler E
- Dris M
- Du Y
- Duarte-Campderros J
- Duchovni E
- Duckeck G
- Ducu OA
- Duda D
- Dudarev A
- Duffield EM
- Duflot L
- Duguid L
- Duhrssen M
- Dumancic M
- Dunford M
- Duren M
- Durglishvili A
- Duschinger D
- Dutta B
- Dyndal M
- Eckardt C
- Ecker KM
- Edgar RC
- Edwards NC
- Eifert T
- Eigen G
- Einsweiler K
- Ekelof T
- El Kacimi M
- El Moursli RC
- Ellajosyula V
- Ellert M
- Elles S
- Ellinghaus F
- Elliot AA
- Ellis N
- Elmsheuser J
- Elsing M
- Emeliyanov D
- Enari Y
- Endner OC
- Endo M
- Ennis JS
- Erdmann J
- Ereditato A
- Ernis G
- Ernst J
- Ernst M
- Errede S
- Ertel E
- Escalier M
- Esch H
- Escobar C
- Esposito B
- Etienvre AI
- Etzion E
- Evans H
- Ezhilov A
- Fabbri F
- Fabbri L
- Facini G
- Fakhrutdinov RM
- Falciano S
- Falla RJ
- Faltova J
- Fang Y
- Fanti M
- Farbin A
- Farilla A
- Farina C
- Farina EM
- Farooque T
- Farrell S
- Farrington SM
- Farthouat P
- Fassi F
- Fassnacht P
- Fassouliotis D
- Favareto A
- Fawcett WJ
- Fayard L
- Fedin OL
- Fedorko W
- Feigl S
- Feligioni L
- Feng C
- Feng EJ
- Feng H
- Fenyuk AB
- Feremeng L
- Ferrando J
- Ferrari A
- Ferrari P
- Ferrari R
- Ferrer A
- Ferrer JAV
- Ferrere D
- Ferretti C
- Fiedler F
- Filipcic A
- Filipuzzi M
- Filthaut F
- Fincke-Keeler M
- Finelli KD
- Fiolhais MCN
- Fiorini L
- Firan A
- Fischer A
- Fischer C
- Fischer J
- Fisher WC
- Flaschel N
- Fleck I
- Fleischmann P
- Fletcher GT
- Fletcher RRM
- Flick T
- Floderus A
- Flowerdew MJ
- Forcolin GT
- Formica A
- Forti A
- Foster AG
- Fournier D
- Fox H
- Fracchia S
- Francavilla P
- Franchini M
- Francis D
- Franconi L
- Franklin M
- Frate M
- Fraternali M
- Freeborn D
- Fressard-Batraneanu SM
- Friedrich F
- Froidevaux D
- Frost JA
- Fukunaga C
- Fusayasu T
- Fuster J
- Gabaldon C
- Gabizon O
- Gabrielli A
- Gabrielli A
- Gach GP
- Gadatsch S
- Gadomski S
- Gagliardi G
- Gagnon LG
- Gagnon P
- Galea C
- Galhardo B
- Gallas EJ
- Gallop BJ
- Gallus P
- Galster G
- Gan KK
- Gao J
- Gao Y
- Gao YS
- Garcia BRM
- Garcia C
- Garcia RFN
- Garcia-Sciveres M
- Gardner RW
- Garelli N
- Garonne V
- Garrido MDMC
- Gatti C
- Gaudiello A
- Gaudio G
- Gaur B
- Gauthier L
- Gavrilenko IL
- Gay C
- Gaycken G
- Gazis EN
- Gecse Z
- Gee CNP
- Geich-Gimbel C
- Geisen M
- Geisler MP
- Gemme C
- Genest MH
- Geng C
- Gentile S
- Gentsos C
- George S
- Gerbaudo D
- Gershon A
- Ghasemi S
- Ghazlane H
- Ghneimat M
- Giacobbe B
- Giagu S
- Giannelli MF
- Giannetti P
- Gibbard B
- Gibson SM
- Gignac M
- Gilchriese M
- Gillam TPS
- Gillberg D
- Gilles G
- Gimenez VC
- Gingrich DM
- Giokaris N
- Giordani MP
- Giorgi FM
- Giorgi FM
- Giraud PF
- Giromini P
- Giugni D
- Giuli F
- Giuliani C
- Giulini M
- Gjelsten BK
- Gkaitatzis S
- Gkialas I
- Gkougkousis EL
- Gladilin LK
- Glasman C
- Glatzer J
- Glaysher PCF
- Glazov A
- Goblirsch-Kolb M
- Godlewski J
- Goldfarb S
- Golling T
- Golubkov D
- Gomes A
- Goncalo R
- Gonella G
- Gonella L
- Gongadze A
- Gonzalez BA
- Gonzalez-Sevilla S
- Goossens L
- Gorbounov PA
- Gordon HA
- Gorelov I
- Gorini B
- Gorini E
- Gorisek A
- Gornicki E
- Goshaw AT
- Gossling C
- Gostkin MI
- Goudet CR
- Goujdami D
- Goussiou AG
- Govender N
- Gozani E
- Graber L
- Grabowska-Bold I
- Gradin POJ
- Grafstrom P
- Gramling J
- Gramstad E
- Grancagnolo S
- Gratchev V
- Gravila PM
- Gray HM
- Graziani E
- Greenwood ZD
- Grefe C
- Gregersen K
- Gregor IM
- Grenier P
- Grevtsov K
- Griffiths J
- Grillo AA
- Grimm K
- Grinstein S
- Gris P
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- Zieminska D
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- Zobernig G
- Zoccoli A
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Measurements of distributions of charged particles produced in protonâproton collisions with a centre-of-mass energy of 13 TeV are presented. The data were recorded by the ATLAS detector at the LHC and correspond to an integrated luminosity of 151 ÎŒb â1 ÎŒbâ1 . The particles are required to have a transverse momentum greater than 100 MeV and an absolute pseudorapidity less than 2.5. The charged-particle multiplicity, its dependence on transverse momentum and pseudorapidity and the dependence of the mean transverse momentum on multiplicity are measured in events containing at least two charged particles satisfying the above kinematic criteria. The results are corrected for detector effects and compared to the predictions from several Monte Carlo event generators
Measurement of the W±Z boson pair-production cross section in pp collisions at âs=13TeV with the ATLAS detector
- Author
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- Aad G
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- Abdallah J
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- Youssef S
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- Yusuff I
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanello L
- Zanzi D
- Zeitnitz C
- Zeman M
- Zemla A
- Zeng JC
- Zeng Q
- Zengel K
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
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- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang R
- Zhang R
- Zhang X
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhong J
- Zhou B
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- Zhou L
- Zhou M
- Zhou N
- Zhu CG
- Zhu H
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- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zu Theenhausen HM
- zur Nedden M
- Zwalinski L
- Publication venue
- Netherlands
- Publication date
- 01/01/2016
- Field of study
published_or_final_versio
Search for anomalous couplings in the W tb vertex from the measurement of double differential angular decay rates of single top quarks produced in the t-channel with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
- Abolins M
- AbouZeid OS
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agricola J
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Alimonti G
- Alio L
- Alison J
- Alkire SP
- Allbrooke BMM
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Altheimer A
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amram N
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjos N
- Annovi A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armadans RC
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- Korolkov I
- Korolkova EV
- Kortner O
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- Kosek T
- Kostyukhin VV
- Kotov VM
- Kotwal A
- Kourkoumeli-Charalampidi A
- Kourkoumelis C
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- Le Dortz O
- Le Guirriec E
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 13/10/2015
- Field of study
The electroweak production and subsequent decay of single top quarks is determined by the properties of the Wtb vertex. This vertex can be described by the complex parameters of an effective Lagrangian. An analysis of angular distributions of the decay products of single top quarks produced in the t -channel constrains these parameters simultaneously. The analysis described in this paper uses 4.6 fbâ1 of proton-proton collision data at âs =7 TeV collected with the ATLAS detector at the LHC. Two parameters are measured simultaneously in this analysis. The fraction f 1 of decays containing transversely polarised W bosons is measured to be 0.37 ± 0.07 (stat.âsyst.). The phase ÎŽ â between amplitudes for transversely and longitudinally polarised W bosons recoiling against left-handed b-quarks is measured to be â0.014Ï Â± 0.036Ï (stat.âsyst.). The correlation in the measurement of these parameters is 0.15. These values result in two-dimensional limits at the 95% confidence level on the ratio of the complex coupling parameters g R and V L, yielding Re[g R /V L] â [â0.36, 0.10] and Im[g R /V L] â [â0.17, 0.23] with a correlation of 0.11. The results are in good agreement with the predictions of the Standard Model
Anatomy of the sign-problem in heavy-dense QCD
- Author
- Adam E Romero
- Aranda C Padilla
- Arjanovic MM
- Armadans R Caminal
- Astigarraga ME Pozo
- Barajas CA Chavez
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- Zurzolo G
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
QCD at finite densities of heavy quarks is investigated
using the density-of-states method. The phase factor
expectation value of the quark determinant is calculated to
unprecedented precision as a function of the chemical potential.
Results are validated using those from a reweighting
approach where the latter can produce a significant signalto-noise
ratio. We confirm the particleâhole symmetry at low
temperatures, find a strong sign problem at intermediate values
of the chemical potential, and an inverse Silver Blaze
feature for chemical potentials close to the onset value: here,
the phase-quenched theory underestimates the density of the
full theory
Determination of the ratio of b-quark fragmentation fractions fs/fd in pp collisions at âs = 7 TeV with the ATLAS Detector
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Aben R
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- Acharya BS
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- Agricola J
- Aguilar-Saavedra JA
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- Akesson TPA
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- Alberghi GL
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- Aleksandrov IN
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- Yusuff I
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- Zalieckas J
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- Zhemchugov A
- Zhong J
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- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
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- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zurzolo G
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2015
- Field of study
With an integrated luminosity of 2.47ââfbâ1 recorded by the ATLAS experiment at the LHC, the exclusive decays B 0sâJ/ÏÏ and B0dâJ/ÏK*0 of B mesons produced in pp collisions at âs=7ââTeV are used to determine the ratio of fragmentation fractions fs/fd. From the observed B0sâJ/ÏÏ and B0dâJ/ÏK*0 yields, the quantity (fs/fd)[B(B0sâJ/ÏÏ)/B(B 0dâJ/ÏK*0)] is measured to be 0.199±0.004(stat)±0.008(syst). Using a recent theory prediction for [B(B0sâJ/ÏÏ)/B(B0dâJ/ÏK*0)] yields (fs/fd)=0.240±0.004(stat)±0.010(syst)±0.017(th). This result is based on a new approach that provides a significant improvement of the world average
Measurement of the inelastic proton-proton cross section at âs=13 TeV with the ATLAS detector at the LHC
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Aben R
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adamczyk L
- Adams DL
- Adelman J
- Adomeit S
- Adye T
- Affolder AA
- Agatonovic-Jovin T
- Agricola J
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akerstedt H
- Akesson TPA
- Akimov AV
- Alberghi GL
- Albert J
- Albrand S
- Alconada Verzini MJ
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alstaty M
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amako K
- Amaral Coutinho Y
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amorim A
- Amoroso S
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Anger P
- Angerami A
- Anghinolfi F
- Anisenkov AV
- Anjos N
- Annovi A
- Antel C
- Antonelli M
- Antonov A
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Araya ST
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armadans RC
- Armbruster AJ
- Armitage LJ
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- Kondrashova N
- Konig AC
- Kono T
- Konoplich R
- Konstantinidis N
- Kopeliansky R
- Koperny S
- Kopp AK
- Korcyl K
- Kordas K
- Korn A
- Korol AA
- Korolkov I
- Korolkova EV
- Kortner O
- Kortner S
- Kosek T
- Kostyukhin VV
- Kotwal A
- Kourkoumeli-Charalampidi A
- Kourkoumelis C
- Kouskoura V
- Kowalewska AB
- Kowalewski R
- Kowalski TZ
- Kozakai C
- Kozanecki W
- Kozhin AS
- Kramarenko VA
- Kramberger G
- Krasnopevtsev D
- Krasny MW
- Krasznahorkay A
- Kravchenko A
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- Kuechler JT
- Kuehn S
- Kugel A
- Kuger F
- Kuhl A
- Kuhl T
- Kukhtin V
- Kukla R
- Kulchitsky Y
- Kuleshov S
- Kuna M
- Kunigo T
- Kupco A
- Kurashige H
- Kurochkin YA
- Kus V
- Kuutmann EB
- Kuwertz ES
- Kuze M
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- Kyriazopoulos D
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- Landgraf U
- Landon MPJ
- Lanfermann MC
- Lang VS
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- Lankford AJ
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- Lanza A
- Laplace S
- Lapoire C
- Laporte JF
- Lari T
- Lassnig M
- Latour BMD
- Laurelli P
- Lavrijsen W
- Law AT
- Laycock P
- Lazovich T
- Lazzaroni M
- Le Dortz O
- Le Guirriec E
- Le Quilleuc EP
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- LeCompte T
- Ledroit-Guillon F
- Lee CA
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- Leggett C
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- Lei X
- Leight WA
- Leisos A
- Leister AG
- Leite MAL
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- Lemmer B
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- Limosani A
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- Lin TH
- Lindquist BE
- Lionti AE
- Lipeles E
- Lipniacka A
- Lisovyi M
- Liss TM
- Lister A
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- Liu B
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- Lloyd SL
- Lo Sterzo F
- Lobodzinska E
- Loch P
- Lockman WS
- Loebinger FK
- Loesel PJ
- Loevschall-Jensen AE
- Loew KM
- Loginov A
- Lohse T
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- Lopes L
- Lopez Paz I
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- Lounis A
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- Lukas W
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- Macchiolo A
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- Martyniuk AC
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- Mashinistov R
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2015
- Field of study
This Letter presents a measurement of the inelastic proton-proton cross section using 60ââÎŒb â1 of pp collisions at a center-of-mass energy âs of 13 TeV with the ATLAS detector at the LHC. Inelastic interactions are selected using rings of plastic scintillators in the forward region (2.0710 â6 , where M X is the larger invariant mass of the two hadronic systems separated by the largest rapidity gap in the event. In this Ο range the scintillators are highly efficient. For diffractive events this corresponds to cases where at least one proton dissociates to a system with M X >13ââGeV . The measured cross section is compared with a range of theoretical predictions. When extrapolated to the full phase space, a cross section of 78.1±2.9ââmb is measured, consistent with the inelastic cross section increasing with center-of-mass energy
Measurement of W+Wâ production in association with one jet in protonâproton collisions at sqrt(s) = 8TeV with the ATLAS detector
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- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2016
- Field of study
The production of W boson pairs in association with one jet in pp collisions at View the MathML sources=8 TeV is studied using data corresponding to an integrated luminosity of 20.3 fbâ1 collected by the ATLAS detector during 2012 at the CERN Large Hadron Collider. The cross section is measured in a fiducial phase-space region defined by the presence of exactly one electron and one muon, missing transverse momentum and exactly one jet with a transverse momentum above 25 GeV and a pseudorapidity of |η|<4.5|η|<4.5. The leptons are required to have opposite electric charge and to pass transverse momentum and pseudorapidity requirements. The fiducial cross section is found to be View the MathML sourceÏWWfid,1-jet=136±6(stat)±14(syst)±3(lumi) fb. In combination with a previous measurement restricted to leptonic final states with no associated jets, the fiducial cross section of WW production with zero or one jet is measured to be View the MathML sourceÏWWfid,â€1-jet=511±9(stat)±26(syst)±10(lumi) fb. The ratio of fiducial cross sections in final states with one and zero jets is determined to be 0.36±0.050.36±0.05. Finally, a total cross section extrapolated from the fiducial measurement of WW production with zero or one associated jet is reported. The measurements are compared to theoretical predictions and found in good agreement
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