736 research outputs found
Non-steroidal neuromuscular blocking agents to re-establish paralysis after reversal of rocuronium-induced neuromuscular block with sugammadex
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Verifying 4D gated radiotherapy using time-integrated electronic portal imaging: a phantom and clinical study
- Author
- A Van Esch
- B Gagel
- Ben J Slotman
- C Eccles
- C Nelson
- CJ Haasbeek
- CM Richardson
- DP Gierga
- E Rietzel
- E Yorke
- EC Ford
- Frank GM de Geest
- Frank J Lagerwaard
- G Mageras
- G Starkschall
- GS Mageras
- H Shirato
- HC De Boer
- HD Kubo
- JD Hoisak
- Johan P Cuijpers
- John R van Sörnsen de Koste
- JR Van Sörnsen de Koste
- JR Van Sörnsen de Koste
- LA Dawson
- Li X allen
- M Guckenberger
- M Imura
- N Koch
- PB Greer
- PJ Keall
- R George
- R Koshani
- RI Berbeco
- RI Berbeco
- RW Underberg
- RW Underberg
- RW Underberg
- Suresh Senan
- T Neicu
- T Pan
- VR Kini
- YG Van der Geld
- Publication venue
- BioMed Central
- Publication date
- 01/01/2007
- Field of study
<p>Abstract</p> <p>Background</p> <p>Respiration-gated radiotherapy (RGRT) can decrease treatment toxicity by allowing for smaller treatment volumes for mobile tumors. RGRT is commonly performed using external surrogates of tumor motion. We describe the use of time-integrated electronic portal imaging (TI-EPI) to verify the position of internal structures during RGRT delivery</p> <p>Methods</p> <p>TI-EPI portals were generated by continuously collecting exit dose data (aSi500 EPID, Portal vision, Varian Medical Systems) when a respiratory motion phantom was irradiated during expiration, inspiration and free breathing phases. RGRT was delivered using the Varian RPM system, and grey value profile plots over a fixed trajectory were used to study object positions. Time-related positional information was derived by subtracting grey values from TI-EPI portals sharing the pixel matrix. TI-EPI portals were also collected in 2 patients undergoing RPM-triggered RGRT for a lung and hepatic tumor (with fiducial markers), and corresponding planning 4-dimensional CT (4DCT) scans were analyzed for motion amplitude.</p> <p>Results</p> <p>Integral grey values of phantom TI-EPI portals correlated well with mean object position in all respiratory phases. Cranio-caudal motion of internal structures ranged from 17.5–20.0 mm on planning 4DCT scans. TI-EPI of bronchial images reproduced with a mean value of 5.3 mm (1 SD 3.0 mm) located cranial to planned position. Mean hepatic fiducial markers reproduced with 3.2 mm (SD 2.2 mm) caudal to planned position. After bony alignment to exclude set-up errors, mean displacement in the two structures was 2.8 mm and 1.4 mm, respectively, and corresponding reproducibility in anatomy improved to 1.6 mm (1 SD).</p> <p>Conclusion</p> <p>TI-EPI appears to be a promising method for verifying delivery of RGRT. The RPM system was a good indirect surrogate of internal anatomy, but use of TI-EPI allowed for a direct link between anatomy and breathing patterns.</p
Recommended temperature metrics for carbon budget estimates, model evaluation and climate policy
- Author
- A Schmidt
- AH MacDougall
- AH MacDougall
- AP Schurer
- B Huang
- C Deser
- C-F Schleussner
- C-Y Wang
- Carl-Friedrich Schleussner
- CK Folland
- CL Quéré
- CP Morice
- D Jiménez-de-la-Cuesta
- DA Ridley
- DP Dee
- E Comyn-Platt
- E Hawkins
- E Volodin
- G Foster
- G Myhre
- GA Schmidt
- GJ Boer
- H. Damon Matthews
- HD Matthews
- HD Matthews
- HD Matthews
- I Medhaug
- J Rogelj
- J Rogelj
- JA Lowe
- JJ Kennedy
- JJ Kennedy
- JL Lean
- Joeri Rogelj
- K Cowtan
- K Cowtan
- K Haustein
- K Rypdal
- K Wolter
- K Zickfeld
- Katarzyna B. Tokarska
- KB Tokarska
- KB Tokarska
- KE Taylor
- KE Trenberth
- M Huber
- M Meinshausen
- M Richardson
- M Richardson
- Martin B. Stolpe
- MH England
- N Mengis
- Nathan P. Gillett
- NJL Lenssen
- NP Gillett
- NP Gillett
- OA Saenko
- P Goodwin
- P Pfleiderer
- Peter Pfleiderer
- R Gelaro
- RE Benestad
- RJ Millar
- S Hirahara
- S Outten
- T Turkington
- V Eyring
- VK Arora
- VK Arora
- Y Kosaka
- Y Kosaka
- Z Hausfather
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 23/10/2019
- Field of study
Recent estimates of the amount of carbon dioxide that can still be emitted while achieving the Paris Agreement temperature goals are larger than previously thought. One potential reason for these larger estimates may be the different temperature metrics used to estimate the observed global mean warming for the historical period, as they affect the size of the remaining carbon budget. Here we explain the reasons behind these remaining carbon budget increases, and discuss how methodological choices of the global mean temperature metric and the reference period influence estimates of the remaining carbon budget. We argue that the choice of the temperature metric should depend on the domain of application. For scientific estimates of total or remaining carbon budgets, globally averaged surface air temperature estimates should be used consistently for the past and the future. However, when used to inform the achievement of the Paris Agreement goal, a temperature metric consistent with the science that was underlying and directly informed the Paris Agreement should be applied. The resulting remaining carbon budgets should be calculated using the appropriate metric or adjusted to reflect these differences among temperature metrics. Transparency and understanding of the implications of such choices are crucial to providing useful information that can bridge the science–policy gap
Linking personality to larval energy reserves in rainbow trout (Oncorhynchus mykiss).
- Author
- A Sih
- AJ Frost
- AM Bell
- C Barr
- C Deleaniz
- C Summers
- CM Coppens
- D Nettle
- D Reale
- D Reale
- D Reale
- D Wilson
- E Brännäs
- E Höglund
- EA Daubert
- Erik Höglund
- Gonzalo G. de Polavieja
- HD Freeman
- I Barber
- I Weigensberg
- J Bernardo
- J Cote
- J Koolhaas
- J Stamps
- J Vaz-Serrano
- JA Stamps
- JL Lukkes
- JM Koolhaas
- JM Koolhaas
- K Lesch
- K van Oers
- KA Pavlov
- KCF Fone
- LF Jensen
- M Wolf
- M Wolf
- MA Andersson
- Madelene Åberg Andersson
- N Metcalfe
- NA Dochtermann
- NJ Dingemanse
- R Plomin
- S Dall
- S Einum
- S Einum
- S Gosling
- S Gosling
- S Winberg
- SF de Boer
- SJ Suomi
- T Mousseau
- T Price
- T Regnier
- TGG Groothuis
- Ø Øverli
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/01/2012
- Field of study
There is a surging interest in the evolution, ecology and physiology of personality differences. However, most of the studies in this research area have been performed in adult animals. Trait variations expressed early in development and how they are related to the ontogeny of an animal's personality are far less studied. Genetic differences as well as environmental factors causing functional variability of the central serotonergic system have been related to personality differences in vertebrates, including humans. Such gene-environment interplay suggests that the central serotonergic system plays an important role in the ontogeny of personality traits. In salmonid fishes, the timing of emergence from spawning nests is related to energy reserves, aggression, and social dominance. However, it is currently unknown how the size of the yolk reserve is reflected on aggression and dominance, or if these traits are linked to differences in serotonergic transmission in newly emerged larvae. In this study we investigated the relationship between yolk reserves, social dominance, and serotonergic transmission in newly emerged rainbow trout (Oncorhynchus mykiss) larvae. This was conducted by allowing larvae with the same emergence time, but with different yolk sizes, to interact in pairs for 24 h. The results show that individuals with larger yolks performed more aggressive acts, resulting in a suppression of aggression in individuals with smaller yolks. A higher brain serotonergic activity confirmed subordination in larvae with small yolks. The relationship between social dominance and yolk size was present in siblings, demonstrating a link between interfamily variation in energy reserves and aggression, and suggests that larger yolk reserves fuel a more aggressive personality during the initial territorial establishment in salmonid fishes. Furthermore, socially naïve larvae with big yolks had lower serotonin levels, suggesting that other factors than the social environment causes variation in serotonergic transmission, underlying individual variation in aggressive behavior
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alda Junior WL
- Alexander J
- Aliev T
- Almeida N
- Alver B
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Aranyi A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arisaka K
- Arneodo M
- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
- Assran Y
- Ata M
- Atac M
- Atramentov O
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baeni L
- Baesso P
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Bakken JA
- Balazs M
- Ball AH
- Ball G
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Banzuzi K
- Barbagli G
- Barberis E
- Barbone L
- Bardak C
- Barfuss AF
- Bargassa P
- Barge D
- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
- Barone L
- Barrett M
- Bartalini P
- Barth C
- Basegmez S
- Basso L
- Battilana C
- Baty C
- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bayshev I
- Bazterra VE
- Bean A
- Beauceron S
- Beaudette F
- Beaupere N
- Bedjidian M
- Beernaert K
- Behrenhoff W
- Behrens U
- Belforte S
- Beliy N
- Belknap D
- Bell AJ
- Bell KW
- Bellan P
- Bellan R
- Bellato M
- Bellinger JN
- Belotelov I
- Belyaev A
- Belyaev A
- Benaglia A
- Bencze G
- Bendavid J
- Benedetti D
- Benelli G
- Benhabib L
- Beni N
- Benucci L
- Benussi L
- Benvenuti AC
- Beranek S
- Beretvas A
- Bergauer T
- Berger J
- Bergholz M
- Beri SB
- Bernardes CA
- Bernardini J
- Bernet C
- Berry D
- Berry E
- Berryhill J
- Bertl W
- Berzano U
- Besancon M
- Betchart B
- Bethani A
- Betts RR
- Beuselinck R
- Bhat PC
- Bhatnagar V
- Bhattacharya S
- Bhattacharya S
- Bhatti A
- Bialas W
- Bialkowska H
- Bian JG
- Bianchi G
- Bianchini L
- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilin B
- Bilinskas MJ
- Bilki B
- Bilmis S
- Biselli A
- Bisello D
- Bitioukov S
- Blekman F
- Blobel V
- Bloch D
- Bloch I
- Bloch P
- Bloom K
- Bluj M
- Blumenfeld B
- Blyweert S
- Bobrovskyi S
- Boccali T
- Bocci A
- Bochenek J
- Bodek A
- Bodin D
- Boimska B
- Boldizsar L
- Bolla G
- Bolognesi S
- Bolton T
- Bonacorsi D
- Bonato A
- Bondu O
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- Boos E
- Bornheim A
- Borras K
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- Bortignon P
- Bortoletto D
- Bose S
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- Bostock F
- Botta C
- Boudoul G
- Boulahouache C
- Boumediene D
- Bourilkov D
- Boutemeur M
- Boutle S
- Braibant-Giacomelli S
- Branca A
- Branson JG
- Breedon R
- Breto G
- Breuker H
- Brew C
- Brigliadori L
- Brigljevic V
- Brinkerhoff A
- Broccolo G
- Brochero Cifuentes JA
- Brom JM
- Brona G
- Brooke JJ
- Broutin C
- Brown RM
- Brownson E
- Brun H
- Bruno G
- Bryer AG
- Buchmann MA
- Buchmuller O
- Bunkowski K
- Bunn J
- Buontempo S
- Burgmeier A
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- Busza W
- Butler JN
- Butler PH
- Butt J
- Butz E
- Bylsma B
- Cabrera A
- Cabrillo IJ
- Caebergs T
- Cakir A
- Calabria C
- Calderon De La Barca Sanchez M
- Calderon A
- Cali IA
- Calligaris L
- Callner J
- Calvert B
- Calvo E
- Campagnari C
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- Camporesi T
- Capiluppi P
- Caponeri B
- Cappello G
- Cardaci M
- Carlin R
- Carlsmith D
- Carrillo Moreno S
- Carroll R
- Cartiglia N
- Carvalho W
- Casal B
- Casimiro Linares E
- Castaldi R
- Castello R
- Castilla-Valdez H
- Castro A
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- Caudron J
- Caulfield M
- Cavallari F
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- Ceballos GG
- Cepeda M
- Cerati GB
- Cerci DS
- Cerci S
- Cerizza G
- Cerminara G
- Cerrada M
- Chabert EC
- Chadwick M
- Chakaberia I
- Chamizo Llatas M
- Chan M
- Chang P
- Chang S
- Chang YH
- Chang YH
- Chang YW
- Chanon N
- Chao Y
- Charaf O
- Charlot C
- Chasco M
- Chasserat J
- Chatrchyan S
- Chatterjee A
- Chauhan S
- Checchia P
- Chen GM
- Chen HS
- Chen J
- Chen KF
- Chen KH
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- Chen Y
- Chen Z
- Cherepanov V
- Chertok M
- Chetluru V
- Cheung HWK
- Chhibra SS
- Chierici R
- Chiochia V
- Chiorboli M
- Chlebana F
- Cho Y
- Choi M
- Choi S
- Choi Y
- Choi YK
- Chou JP
- Choudhary BC
- Choudhury RK
- Choudhury S
- Christiansen T
- Chuang SH
- Chung J
- Chung YS
- Chwalek T
- Ciesielski R
- Cihangir S
- Cimmino A
- Cipriano PMR
- Cirino G
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clarida W
- Clement E
- Clerbaux B
- Cline D
- CMS Collaboration
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
- Colino N
- Collard C
- Colling D
- Conetti S
- Contardo D
- Conte E
- Contreras-Campana C
- Contreras-Campana E
- Conway J
- Conway R
- Cooper SI
- Cooper W
- Cornelis T
- Correa Martins Junior M
- Cortezon EP
- Cossutti F
- Costa M
- Costa S
- Costantini S
- Coughlan JA
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- Creanza D
- Cremaldi LM
- Cripps N
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cuplov V
- Cure B
- Cushman P
- Cussans D
- Custodio A
- Cutajar M
- Cutts D
- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
- D'Hondt J
- Da Costa EM
- Daci N
- Dahmes B
- Dahms T
- Dallavalle GM
- Damgov J
- Damiao DD
- Dammann D
- Danielson T
- Das S
- Daskalakis G
- Dasu S
- Daubie E
- Dauncey P
- David A
- Davids M
- Davies G
- de Barbaro P
- De Benedetti A
- De Boer W
- de Cassagnac RG
- De Cosa A
- de Fatis TT
- De Filippis N
- De Gruttola M
- De Guio F
- De Jeneret JD
- De La Cruz B
- De La Cruz-Burelo E
- De Lentdecker G
- De Mattia M
- de Monchenault GH
- De Oliveira Martins C
- De Palma M
- De Roeck A
- de Troconiz JF
- De Visscher S
- De Wolf EA
- Deisher A
- Deiters K
- Dejardin M
- del Arbol PMR
- Del Re D
- Delaere C
- Delgado Peris A
- Deliomeroglu M
- Dell'Orso R
- Della Negra M
- Della Ricca G
- Demaria N
- Demina R
- Demortier L
- Denegri D
- Deniz M
- Depasse P
- Dermenev A
- Dero V
- Dhingra N
- Di Giovanni GP
- Di Guida S
- Di Marco E
- Di Matteo L
- Diamond B
- Dias FA
- Diemoz M
- Dierlamm A
- Dietz C
- Dietz-Laursonn E
- Diez Pardos C
- Dimitrov A
- Dinardo ME
- Dirkes G
- Dissertori G
- Dittmar M
- Djordjevic M
- Dobrzynski L
- Dobson M
- Dobur D
- Doesburg R
- Dogangun O
- Dolen J
- Dominguez Vazquez D
- Dominguez A
- Dominik W
- Don CKK
- Dorigo T
- Dorney B
- Doroba K
- Dozen C
- Draeger J
- Dragicevic M
- Dragoiu C
- Drell BR
- Dremin I
- Drouhin F
- Drozdetskiy A
- du Pree T
- Duarte Campderros J
- Duarte J
- Dubinin M
- Dudero PR
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- Duenser M
- Dugad S
- Duggan D
- Dumanoglu I
- Dupont-Sagorin N
- Duric S
- Duris J
- Durkin LS
- Duru F
- Dutta D
- Dutta S
- Dutta V
- Dzelalija M
- Eads M
- Eartly DP
- Eckerlin G
- Ecklund KM
- Eckstein D
- Edelhoff M
- Edelmaier CJ
- Eerola P
- Efron J
- Eggert N
- Ekmedzic M
- El Mamouni H
- Elgammal S
- Elliott-Peisert A
- Ellison J
- Elmer P
- Elvira VD
- Enderle H
- Engh D
- Eno SC
- Epshteyn V
- Erbacher R
- Erdmann M
- Erdmann W
- Erfle J
- Erhan S
- Ero J
- Erofeeva M
- Ershov A
- Esen S
- Eshaq Y
- Eskut E
- Etesami SM
- Eugster J
- Eusebi R
- Evangelou I
- Evans D
- Everaerts P
- Everett A
- Evstyukhin S
- Fabbri F
- Fabbri F
- Fabbricatore P
- Fabbro B
- Fabjan C
- Fabozzi F
- Faccioli P
- Fahim A
- Falkiewicz A
- Fanelli C
- Fanfani A
- Fano L
- Fantasia C
- Farrell C
- Fasanella D
- Fassi F
- Faure JL
- Favaro C
- Favart D
- Fay J
- Fedi G
- Fehling D
- Feindt M
- Felcini M
- Feld L
- Ferapontov A
- Ferencek D
- Ferguson T
- Ferguson W
- Fernandez Bedoya C
- Fernandez Menendez J
- Fernandez Perez Tomei TR
- Fernandez Ramos JP
- Fernandez M
- Ferrando A
- Ferri F
- Ferro C
- Field RD
- Finger M
- Finger M
- Fiore L
- Fiorendi S
- Fiori F
- Fisher M
- Fisk I
- Flacher H
- Flanagan W
- Flix J
- Florez C
- Flossdorf A
- Flowers K
- Flucke G
- Flugge G
- Foa L
- Focardi E
- Folgueras S
- Fonseca De Souza S
- Fontaine J-C
- Ford WT
- Forthomme L
- Foudas C
- Fouz MC
- Franci D
- Francis B
- Franzoni G
- Frazier R
- Freeman J
- Freudenreich K
- Friedl M
- Friis E
- Frisch B
- Frosali S
- Frueboes T
- Fruhwirth R
- Fu Y
- Fulcher J
- Funk W
- Furic IK
- Futyan D
- Gabathuler K
- Gabella W
- Gabusi M
- Gaddi A
- Galanti M
- Gallinaro M
- Gallo E
- Gamsizkan H
- Ganguly S
- Ganjour S
- Gao Y
- Garcia G
- Garcia-Abia P
- Garcia-Bellido A
- Gardner M
- Garrido RGR
- Gartner J
- Gary JW
- Gascon S
- Gasparini F
- Gataullin M
- Gaultney V
- Gauthier L
- Gavrilov V
- Gay APR
- Gaz A
- Gebbert U
- Geenen H
- Geffert P
- Geiser A
- Geisler M
- Gele D
- Genchev V
- Gennai S
- Georgiou G
- Geralis T
- Gerbaudo D
- Gerber CE
- Gershtein Y
- Gerwig H
- Geurts FJM
- Ghete VM
- Ghezzi A
- Giacomelli P
- Giammanco A
- Giassi A
- Gibbons LK
- Giffels M
- Gigi D
- Gilbert A
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- Gilmore J
- Giordano D
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- Girgis S
- Giunta M
- Giurgiu G
- Givernaud A
- Glege F
- Gleyzer SV
- Gninenko S
- Goadhouse S
- Gobbo B
- Godang R
- Godinovic N
- Godshalk A
- Goerlach U
- Goerner M
- Goh J
- Gokbulut G
- Gokieli R
- Goldberg S
- Goldenzweig P
- Goldstein J
- Golf F
- Gollapinni S
- Golovtsov V
- Golubev N
- Golunov A
- Golutvin I
- Gomber B
- Gomez Moreno B
- Gomez G
- Gomez JA
- Goncharov M
- Gonzalez Caballero I
- Gonzalez Lopez O
- Gonzalez Sanchez J
- Gonzalez JS
- Gonzi S
- Goodell J
- Gorbounov N
- Gorski M
- Gotra Y
- Gottschalk E
- Goulianos K
- Gouskos L
- Gouzevitch M
- Govoni P
- Gowdy S
- Goy Lopez S
- Gozzelino A
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- Grachov O
- Gramenitski I
- Grandi C
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- Grassi M
- Gray L
- Gray R
- Graziano A
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- Gregoire G
- Gregores EM
- Gribushin A
- Griffiths S
- Grigelionis I
- Grimes M
- Grishin V
- Gritsan AV
- Grogg KS
- Gronberg J
- Grothe M
- Grundler U
- Grunewald M
- Gruschke J
- Guchait M
- Gude A
- Gueth A
- Guida R
- Guiducci L
- Guler AM
- Gulmez E
- Guo S
- Guo Y
- Guo ZJ
- Gupta R
- Guragain S
- Gurrola A
- Gurtu A
- Gutay L
- Guthoff M
- Gutsche O
- Gyun D
- Haas J
- Hackstein C
- Hadjiiska R
- Hadley NJ
- Hagopian S
- Hagopian V
- Haguenauer M
- Hahn KA
- Hajdu C
- Halkiadakis E
- Hall G
- Hall-Wilton R
- Halyo V
- Hammad GH
- Hammer J
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- Harr R
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- Harris RM
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- Yilmaz Y
- Yohay R
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
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- Ziebarth EB
- Ziegler J
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- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
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- Acosta MV
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- Wrochna G
- Wu W
- Wuerthwein F
- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yalvac M
- Yang F
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Compressed representation of a partially defined integer function over multiple arguments
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta MV
- Adair A
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agram J-L
- Aguilar-Benitez M
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
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- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
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- Amsler C
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- Anastassov A
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- Andreev V
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- Andreev Y
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- Antonelli L
- Antunovic Z
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- Zhang L
- Zheng Y
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- Publication venue
- Publication date
- 01/01/2013
- Field of study
In OLAP (OnLine Analitical Processing) data are analysed in an n-dimensional cube. The cube may be represented as a partially defined function over n arguments. Considering that often the function is not defined everywhere, we ask: is there a known way of representing the function or the points in which it is defined, in a more compact manner than the trivial one
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
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- Adam W
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- Adzic P
- Afanasiev S
- Agostino L
- Agram JL
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- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
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- Alcaraz Maestre J
- Alda Junior WL
- Alexander J
- Aliev T
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- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunovic Z
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- Arcidiacono R
- Arenton MW
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- Avery P
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- Xiao H
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
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- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
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- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
The azimuthal anisotropy of charged particles in PbPb collisions at
nucleon-nucleon center-of-mass energy of 2.76 TeV is measured with the CMS
detector at the LHC over an extended transverse momentum (pt) range up to
approximately 60 GeV. The data cover both the low-pt region associated with
hydrodynamic flow phenomena and the high-pt region where the anisotropies may
reflect the path-length dependence of parton energy loss in the created medium.
The anisotropy parameter (v2) of the particles is extracted by correlating
charged tracks with respect to the event-plane reconstructed by using the
energy deposited in forward-angle calorimeters. For the six bins of collision
centrality studied, spanning the range of 0-60% most-central events, the
observed v2 values are found to first increase with pt, reaching a maximum
around pt = 3 GeV, and then to gradually decrease to almost zero, with the
decline persisting up to at least pt = 40 GeV over the full centrality range
measured.Comment: Replaced with published version. Added journal reference and DO
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Pozzobon N
- Prado Da Silva WL
- Primavera F
- Prokofyev O
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- Safonov A
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- Saoulidou N
- Sarkar S
- Sarycheva L
- Sasseville M
- Sauerland P
- Savin A
- Savrin V
- Scarborough T
- Schaefer C
- Schael S
- Schettler H
- Scheurer A
- Schilling F-P
- Schizzi A
- Schlein P
- Schleper P
- Schlieckau E
- Schmidt A
- Schmidt R
- Schmitt M
- Schmitz SA
- Schnetzer S
- Schoefbeck R
- Schoerner-Sadenius T
- Schott G
- Schroeder M
- Schul N
- Schum T
- Schwick C
- Scodellaro L
- Searle M
- Seez C
- Segala M
- Segoni I
- Seidel M
- Seitz C
- Seixas J
- Sekmen S
- Sellers P
- Selvaggi G
- Selvaggi M
- Semenov S
- Sen N
- Sen S
- Sengupta S
- Senkin S
- Seo E
- Seo H
- Serban AT
- Serin M
- Sever R
- Sexton-Kennedy E
- Sguazzoni G
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- Sharan M
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- Sharma A
- Sharma S
- Sharma V
- Sharma V
- Sharp P
- Sheldon P
- Shepherd-Themistocleous CH
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- Shipsey I
- Shiu JG
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- Shmatov S
- Shoaib M
- Shrestha S
- Shreyber I
- Shukla P
- Shumeiko N
- Sibille J
- Siegrist P
- Sigamani M
- Sikler F
- Silkworth C
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- Silvers D
- Silverwood H
- Silvestris L
- Simon M
- Simon S
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- Simonis HJ
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- Singh G
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- Singovsky A
- Sinthuprasith T
- Sirois Y
- Siroli G
- Sirunyan AM
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- Skuja A
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- Soares MS
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- Wyslouch B
- Xiao H
- Xie S
- Xu M
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- Yang F
- Yang M
- Yang Y
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- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
- Zhokin A
- Zhu B
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- Zhukov V
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- Zielinski M
- Zito G
- Zou W
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
A search for new physics is performed in events with two same-sign isolated
leptons, hadronic jets, and missing transverse energy in the final state. The
analysis is based on a data sample corresponding to an integrated luminosity of
4.98 inverse femtobarns produced in pp collisions at a center-of-mass energy of
7 TeV collected by the CMS experiment at the LHC. This constitutes a factor of
140 increase in integrated luminosity over previously published results. The
observed yields agree with the standard model predictions and thus no evidence
for new physics is found. The observations are used to set upper limits on
possible new physics contributions and to constrain supersymmetric models. To
facilitate the interpretation of the data in a broader range of new physics
scenarios, information on the event selection, detector response, and
efficiencies is provided.Comment: Published in Physical Review Letter
- …