1,737 research outputs found
Cortical microstructure in primary progressive aphasia: a multicenter study
- Author
- Publication venue
- Publication date
- 06/07/2023
- Field of study
Cortical mean diffusivity is a novel imaging metric sensitive to early changes in neurodegenerative syndromes. Higher cortical mean diffusivity values reflect microstructural disorganization and have been proposed as a sensitive biomarker that might antedate macroscopic cortical changes. We aimed to test the hypothesis that cortical mean diffusivity is more sensitive than cortical thickness to detect cortical changes in primary progressive aphasia (PPA).In this multicenter, case-control study, we recruited 120 patients with PPA (52 non-fluent, 31 semantic, and 32 logopenic variants; and 5 GRN-related PPA) as well as 89 controls from three centers. The 3-Tesla MRI protocol included structural and diffusion-weighted sequences. Disease severity was assessed with the Clinical Dementia Rating scale. Cortical thickness and cortical mean diffusivity were computed using a surface-based approach.The comparison between each PPA variant and controls revealed cortical mean diffusivity increases and cortical thinning in overlapping regions, reflecting the canonical loci of neurodegeneration of each variant. Importantly, cortical mean diffusivity increases also expanded to other PPA-related areas and correlated with disease severity in all PPA groups. Cortical mean diffusivity was also increased in patients with very mild PPA when only minimal cortical thinning was observed and showed a good correlation with measures of disease severity.Cortical mean diffusivity shows promise as a sensitive biomarker for the study of the neurodegeneration-related microstructural changes in PPA.© 2022. The Author(s)
Male age is associated with extra-pair paternity, but not with extra-pair mating behaviour
- Author
- A Dixon
- A Girndt
- AP Møller
- AP Møller
- BM Bolker
- C Shively
- CB Possamai
- D Bates
- D Lack
- D Summers-Smith
- DA Dawson
- DF Westneat
- DF Westneat
- DF Westneat
- DS Richardson
- E Akcay
- FM Hunter
- H Jensen
- H Kokko
- IR Cleasby
- J Gonzalez-Solis
- J Sundberg
- JH Wetton
- JL Dickinson
- JNM Smith
- JV Briskie
- KB Nyland
- L Schlicht
- MB Morales
- MK Schwartz
- O Sanchez-Macouzet
- PC Frederick
- PJ Weatherhead
- PO Dunn
- R Brooks
- R Development Core Team
- RH Wagner
- SA Tarof
- SC Griffith
- ST Kalinowski
- T Laskemoen
- TF Hansen
- TR Birkhead
- W Forstmeier
- W Forstmeier
- YH Hsu
- YH Hsu
- YH Hsu
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 14/11/2017
- Field of study
Extra-pair paternity is the result of copulation between a female and a male other than her social partner. In socially monogamous birds, old males are most likely to sire extra-pair offspring. The male manipulation and female choice hypotheses predict that age-specific male mating behaviour could explain this old-over-young male advantage. These hypotheses have been difficult to test because copulations and the individuals involved are hard to observe. Here, we studied the mating behaviour and pairing contexts of captive house sparrows, Passer domesticus. Our set-up mimicked the complex social environment experienced by wild house sparrows. We found that middle-aged males, which would be considered old in natural populations, gained most extra-pair paternity. However, both, female solicitation behaviour and subsequent extra-pair matings were not associated with male age. Further, copulations were more likely when solicited by females than when initiated by males (i.e. unsolicited copulations). Male initiated within-pair copulations were more common than male initiated extra-pair copulations. To conclude, our results did not support either hypothesis regarding age-specific male mating behaviour. Instead, female choice, independent of male age, governed copulation success, especially in an extra-pair context. Post-copulatory mechanisms might determine why older males sire more extra-pair offspring
Rapidity and Centrality Dependence of Proton and Anti-proton Production from Au+Au Collisions at sqrt(sNN) = 130GeV
- Author
- Adams J.
- Adler C.
- Aggarwal MM
- Ahammed Z.
- Amonett J.
- Anderson BD
- Anderson M.
- Arkhipkin D.
- Averichev GS
- Badyal SK
- Balewski J.
- Barannikova O.
- Barnby LS
- Baudot J.
- Bekele S.
- Belaga VV
- Bellwied R.
- Berger J.
- Bezverkhny BI
- Bhardwaj S.
- Bhaskar P.
- Bhati AK
- Bichsel H.
- Billmeier A.
- Bland LC
- Blyth CO
- Bonner BE
- Botje M.
- Boucham A.
- Brandin A.
- Bravar A.
- Cadman RV
- Cai XZ
- Caines H.
- Cardenas A.
- Carroll J.
- Castillo J.
- Castro M.
- Cebra D.
- Chaloupka P.
- Chattopadhyay S.
- Chen HF
- Chen Y.
- Chernenko SP
- Cherney M.
- Chikanian A.
- Choi B.
- Christie W.
- Coffin JP
- Cormier TM
- Cramer JG
- Crawford HJ
- Das D.
- Das S.
- de Moura MM
- de Toledo AS
- Derevschikov AA
- Didenko L.
- Dietel T.
- Dong X.
- Draper JE
- Du F.
- Dubey AK
- Dunin VB
- Dunlop JC
- Eckardt V.
- Efimov LG
- Emelianov V.
- Engelage J.
- Eppley G.
- Erazmus B.
- Fachini P.
- Faine V.
- Faivre J.
- Fatemi R.
- Filimonov K.
- Filip P.
- Finch E.
- Fisyak Y.
- Flierl D.
- Foley KJ
- Fu J.
- Gagliardi Carl A.
- Gagunashvili N.
- Gans J.
- Ganti MS
- Gaudichet L.
- Germain M.
- Geurts F.
- Ghazikhanian V.
- Ghosh P.
- Gonzalez JE
- Grachov O.
- Grigoriev V.
- Grosnick D.
- Guedon M.
- Guertin SM
- Gupta A.
- Gushin E.
- Gutierrez TD
- Hallman TJ
- Hardtke D.
- Harris JW
- Heinz M.
- Henry TW
- Heppelmann S.
- Herston T.
- Hippolyte B.
- Hirsch A.
- Hjort E.
- Hoffmann GW
- Horsley M.
- Huang HZ
- Huang SL
- Humanic TJ
- Igo G.
- Ishihara A.
- Jacobs P.
- Jacobs WW
- Janik M.
- Johnson I.
- Jones PG
- Judd EG
- Kabana S.
- Kaneta M.
- Kaplan M.
- Keane D.
- Kiryluk J.
- Kisiel A.
- Klay J.
- Klein SR
- Klyachko A.
- Koetke DD
- Kollegger T.
- Konstantinov AS
- Kopytine M.
- Kotchenda L.
- Kovalenko AD
- Kramer M.
- Kravtsov P.
- Krueger K.
- Kuhn C.
- Kulikov AI
- Kumar A.
- Kunde GJ
- Kunz CL
- Kutuev RK
- Kuznetsov AA
- Lamont MAC
- Landgraf JM
- Lange S.
- Lansdell CP
- Lasiuk B.
- Laue F.
- Lauret J.
- Lebedev A.
- Lednicky R.
- Leontiev VM
- LeVine MJ
- Li C.
- Li Q.
- Lindenbaum SJ
- Lisa MA
- Liu F.
- Liu L.
- Liu QJ
- Liu Z.
- Ljubicic T.
- Llope WJ
- Long H.
- Longacre RS
- Lopez-Noriega M.
- Love WA
- Ludlam T.
- Lynn D.
- Ma J.
- Ma YG
- Magestro D.
- Mahajan S.
- Mahapatra AP
- Majka R.
- Mangotra LK
- Manweiler R.
- Margetis S.
- Markert C.
- Martin L.
- Marx J.
- Matis HS
- Matulenko YA
- Mazumdar MRD
- McShane TS
- Meissner F.
- Melnick Y.
- Meschanin A.
- Messer M.
- Miller ML
- Milosevich Z.
- Minaev NG
- Mironov C.
- Mishra D.
- Mitchell J.
- Mohanty B.
- Molnar L.
- Moore CF
- Mora-Corral MJ
- Morozov V.
- Munhoz MG
- Nandi BK
- Nayak SK
- Nayak TK
- Nelson JM
- Nevski P.
- Nikitin VA
- Nogach LV
- Norman B.
- Nurushev SB
- Odyniec G.
- Ogawa A.
- Okorokov V.
- Oldenburg M.
- Olson D.
- Paic G.
- Pal S.
- Pandey SU
- Panebratsev Y.
- Panitkin SY
- Pavlinov AI
- Pawlak T.
- Perevoztchikov V.
- Peryt W.
- Petrov VA
- Phatak SC
- Picha R.
- Pluta J.
- Porile N.
- Porter J.
- Poskanzer AM
- Potekhin M.
- Potrebenikova E.
- Potukuchi BVKS
- Prindle D.
- Pruneau C.
- Putschke J.
- Rai G.
- Rakness G.
- Raniwala R.
- Raniwala S.
- Ravel O.
- Ray RL
- Razin SV
- Reichhold D.
- Reid JG
- Renault G.
- Retiere F.
- Ridiger A.
- Ritter HG
- Roberts JB
- Rogachevski OV
- Romero JL
- Rose A.
- Roy C.
- Ruan LJ
- Rykov V.
- Sahoo R.
- Sakrejda I.
- Salur S.
- Sanchez MCD
- Sandweiss J.
- Savin I.
- Schambach J.
- Scharenberg RP
- Schmitz N.
- Schroeder LS
- Schweda K.
- Seger J.
- Seliverstov D.
- Seyboth P.
- Shahaliev E.
- Shao M.
- Sharma M.
- Shestermanov KE
- Shimanskii SS
- Simon F.
- Singaraju RN
- Skoro G.
- Smirnov N.
- Snellings R.
- Sood G.
- Sorensen P.
- Sorensen P.
- Sowinski J.
- Spinka H. M.
- Srivastava B.
- Stanislaus S.
- STAR Collaboration.
- Stephenson EJ
- Stock R.
- Stolpovsky A.
- Strikhanov M.
- Stringfellow B.
- Struck C.
- Suaide AAP
- Sugarbaker E.
- Suire C.
- Sumbera M.
- Surrow B.
- Symons TJM
- Szarwas P.
- Tai A.
- Takahashi J.
- Tang AH
- Thein D.
- Thomas JH
- Tikhomirov V.
- Tokarev M.
- Tonjes MB
- Trainor TA
- Trentalange S.
- Tribble Robert E.
- Trivedi MD
- Trofimov V.
- Tsai O.
- Ullrich T.
- Underwood DG
- Van Buren G.
- Vander Molen AM
- Vasiliev AN
- Vasiliev M.
- Vigdor SE
- Viyogi YP
- Voloshin SA
- Wang F.
- Wang G.
- Wang XL
- Wang ZM
- Ward H.
- Watson JW
- Wells R.
- Westfall GD
- Whitten C.
- Wieman H.
- Willson R.
- Wissink SW
- Witt R.
- Wood J.
- Wu J.
- Xu N.
- Xu Z.
- Xu ZZ
- Yakutin AE
- Yamamoto E.
- Yang J.
- Yepes P.
- Yurevich VI
- Zanevski YV
- Zborovsky I.
- Zhang H.
- Zhang HY
- Zhang WM
- Zhang ZP
- Zolnierczuk PA
- Zoulkarneev R.
- Zoulkarneeva J.
- Zubarev AN
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 19/06/2003
- Field of study
We report on the rapidity and centrality dependence of proton and anti-proton
transverse mass distributions from Au+Au collisions at sqrt(sNN) = 130GeV as
measured by the STAR experiment at RHIC. Our results are from the rapidity and
transverse momentum range of |y|<0.5 and 0.35 <p_t<1.00GeV/c. For both protons
and anti-protons, transverse mass distributions become more convex from
peripheral to central collisions demonstrating characteristics of collective
expansion. The measured rapidity distributions and the mean transverse momenta
versus rapidity are flat within |y|<0.5. Comparisons of our data with results
from model calculations indicate that in order to obtain a consistent picture
of the proton(anti-proton) yields and transverse mass distributions the
possibility of pre-hadronic collective expansion may have to be taken into
account.Comment: 4 pages, 3 figures, 1 table, submitted to PR
Coffee consumption and the risk of malignant melanoma in the Norwegian Women and Cancer (NOWAC) Study
- Author
- A Hjartaker
- A Kyrgidis
- AG Renehan
- AH Conney
- DB Rubin
- DM Freedman
- E Loftfield
- E Lozcano-Ponce
- E Lund
- E Lund
- Elisabete Weiderpass
- F Gaascht
- FB Hu
- HT Wu
- I Sanchez-Gonzalez
- I Stensvold
- IR White
- J Ferlay
- JB Liu
- LM Nilsson
- Marko Lukic
- MB Veierod
- MB Veierod
- MB Veierod
- Mie Jareid
- P Parras
- PY Lee
- S Winkler
- SK Bohn
- SW Wu
- T Bakuradze
- TK Lee
- Tonje Braaten
- Y-P Lu
- YR Lou
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Adair A
- Adam N
- Adam W
- Adams JR
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- 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
- Alcaraz Maestre J
- Alda Junior WL
- Aldaya Martin M
- Alexander J
- Aliev T
- Alimena J
- Almeida N
- 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
- Antonelli L
- Antunovic Z
- Apanasevich L
- Appelt E
- Apresyan A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arneodo M
- Arora S
- Asawatangtrakuldee C
- Asghar MI
- Askew A
- Assran Y
- Ata M
- Attikis A
- Auffray E
- Autermann C
- Auzinger G
- Avdeeva E
- Avery P
- Avetisyan A
- Avila C
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzolini V
- Azzurri P
- Baarmand MM
- Babb J
- Bacchetta N
- Bachtis M
- Baden A
- Baeni L
- Baffioni S
- Bagliesi G
- Bai Y
- Baillon P
- Bainbridge R
- Bakhshiansohi H
- Bakirci MN
- Balazs M
- Ball AH
- Ball G
- Ban Y
- Banerjee S
- Banerjee S
- Bansal S
- Banzuzi K
- Barbagli G
- Barberis E
- Barbone L
- Barfuss AF
- Bargassa P
- Barge D
- Baringer P
- Barker A
- Barnes VE
- Barnett BA
- Barney D
- Barone L
- Bartalini P
- Barth C
- Basegmez S
- Basso L
- Battilana C
- Bauer G
- Bauerdick LAT
- Baumgartel D
- Baur U
- Bayshev I
- Bazterra VE
- Bean A
- Beauceron S
- Beaudette F
- Beaupere N
- Beernaert K
- Behr J
- Behrenhoff W
- Behrens U
- Belforte S
- Beliy N
- Belknap D
- Bell AJ
- Bell KW
- Bellan P
- Bellan R
- Belotelov I
- Belyaev A
- Belyaev A
- Benaglia A
- Bencze G
- Bendavid J
- Benedetti D
- Benelli G
- Benhabib L
- Beni N
- Benussi L
- Benvenuti AC
- Beranek S
- Beretvas A
- Bergauer T
- Berger J
- Bergholz M
- Beri SB
- Bernardes CA
- Bernet C
- Berry D
- Berry E
- Berryhill J
- Bertl W
- Besancon M
- Betchart B
- Bethani A
- Betts RR
- Beuselinck R
- Bhardwaj A
- Bhat PC
- Bhatnagar V
- Bhattacharya S
- Bhattacharya S
- Bhatti A
- Bialkowska H
- Bian JG
- Bianchi G
- Bianchini L
- Bianco S
- Biasini M
- Biino C
- Bilei GM
- Bilin B
- Bilinskas MJ
- Bilki B
- Bilmis S
- 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
- Boeser C
- Boimska B
- Bolla G
- Bolognesi S
- Bolton T
- Bonacorsi D
- Bonato A
- Bondu O
- Bontenackels M
- Boos E
- Bornheim A
- Borras K
- Borrello L
- Bortignon P
- Bortoletto D
- Bose S
- Bose T
- Bostock F
- Botta C
- Boudoul G
- Boulahouache C
- 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
- Buchmann MA
- Buchmuller O
- Bucinskaite I
- Bunin P
- Bunkowski K
- Buontempo S
- Burgmeier A
- Burkett K
- Busson P
- Busza W
- Butler JN
- Butler PH
- Butt J
- Butz E
- Bylsma B
- Cabrillo IJ
- Caebergs T
- Cakir A
- Calabria C
- Calderon A
- Cali IA
- Calligaris L
- Callner J
- Calvert B
- Calvo E
- Campagnari C
- Campbell A
- Camporesi T
- Cankocak K
- Capiluppi P
- Cappello G
- Cardaci M
- Carlin R
- Carlsmith D
- Carrillo Montoya CA
- Carrillo Moreno S
- Carroll R
- Cartiglia N
- Carvalho W
- Casal B
- Casimiro Linares E
- Castaldi R
- Castello R
- Castilla-Valdez H
- Castro A
- Castro E
- Caudron A
- Caudron J
- Cavallari F
- Cavallo FR
- Cavallo N
- Cavanaugh R
- Ceard L
- 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
- Chen M
- 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
- Cimmino A
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
- Clare R
- Clarida W
- Clement E
- Clerbaux B
- Cline D
- CMS Collaboration
- Coarasa Perez JA
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
- Cole JE
- Colino N
- Collard C
- Colling D
- Contardo D
- Conte E
- Contreras-Campana C
- Contreras-Campana E
- Conway J
- Conway R
- Cooper SI
- Cornelis T
- Correa Martins Junior M
- Cossutti F
- Costa M
- Costa S
- Costantini S
- Costanza F
- Coughlan JA
- Cousins R
- Covarelli R
- Cox B
- Cox PT
- Creanza D
- Cremaldi LM
- Cripps N
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cuplov V
- 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
- Dabrowski A
- 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 Cosa A
- de Fatis TT
- De Filippis N
- De Gruttola M
- De Guio F
- De La Barca Sanchez MC
- 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 Re D
- Delaere C
- Delgado Peris A
- 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
- Descroix A
- 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
- 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
- Dosselli U
- 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
- Duchardt D
- Dudero PR
- Dudko L
- 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
- Eads M
- Eckerlin G
- Ecklund KM
- Eckstein D
- Edelhoff M
- Edelmaier CJ
- Eerola P
- 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
- Eshaq Y
- Eskut E
- Etesami SM
- Eugster J
- Eusebi R
- Evangelou I
- Evans D
- Evdokimov O
- Everaerts P
- Everett A
- Evstyukhin S
- Fabbri F
- Fabbri F
- Fabbricatore P
- Fabbro B
- Fabjan C
- Fabozzi F
- Faccioli P
- Fahim A
- Fanfani A
- Fano L
- Fantasia C
- Farrell C
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- Yilmaz Y
- Yohay R
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- Yun JC
- Zabel J
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- 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
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
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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
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- Zeinali M
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- Zeyrek M
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- Ziebarth EB
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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
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Afanasiev S
- Agostino L
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- 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
- 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
- Zotto P
- Zou W
- 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
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
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- Adiguzel A
- Adler V
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- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
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- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
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- Amsler C
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- Andreev Y
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- Antunes JR
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- Apollinari G
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- Ciesielski R
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- Cimmino A
- Cipriano PMR
- Cirino G
- Cittolin S
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- Cutajar M
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- Ribeiro PQ
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- Rikova MI
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- Roland C
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- Romanowska-Rybinska K
- Romeo F
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- Sfiligoi I
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- Sirunyan AM
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- Vinogradov A
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- Vogel H
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- Vuosalo C
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- Wickens J
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- Winn D
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- Wissing C
- Wittich P
- Wittmer B
- Woehri HK
- Wolf M
- Wolf R
- Womersley WJ
- Won S
- Wood D
- Wood J
- Wood JS
- Worm SD
- Wright D
- Wrochna G
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- 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
Non-Standard Interactions at a Neutrino Factory: Correlations and CP violation
- Author
- A Bandyopadhyay
- A Cervera
- A Donini
- A Donini
- A Gando
- A Rujula De
- A. Donini
- AB McDonald
- AD Bross
- AM Dziewonski
- AM Gago
- B Pontecorvo
- C Biggio
- C Biggio
- D Autiero
- E Fernandez-Martinez
- EA Paschos
- F Boehm
- GL Fogli
- GL Fogli
- H Minakata
- H. Minakata
- J Bouchez
- J Burguet-Castell
- J Kopp
- J Kopp
- J Tang
- J-E Campagne
- J. López-Pavón
- JWF Valle
- K Abe
- K Abe
- K Inoue
- L Wolfenstein
- M Apollonio
- M Blennow
- MB Gavela
- MC Gonzalez-Garcia
- MC Gonzalez-Garcia
- MC Sanchez
- MH Ahn
- MM Guzzo
- N Agafonova
- NC Ribeiro
- P Adamson
- P Huber
- P Huber
- P Huber
- P Huber
- P Huber
- P Huber
- P Huber
- P Langacker
- P Lipari
- P Zucchelli
- P. Coloma
- S Antusch
- S Antusch
- S Antusch
- S Davidson
- S Geer
- S Geer
- S Goswami
- T Kajita
- T Kikuchi
- T Ota
- T Schwetz
- T Schwetz
- W Winter
- Y Grossman
- Z Berezhiani
- Z Maki
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 16/07/2011
- Field of study
We explore the potential of several Neutrino Factory (NF) setups to
constrain, discover and measure new physics effects due to Non-Standard
Interactions (NSI) in propagation through Earth matter. We first study the
impact of NSI in the measurement of θ13: we find that these could be
large due to strong correlations of θ13 with NSI parameters in the
golden channel, and the inclusion of a detector at the magic baseline is
crucial in order to reduce them as much as possible. We present, then, the
sensitivity of the considered NF setups to the NSI parameters, paying special
attention to correlations arising between them and the standard oscillation
parameters, when all NSI parameters are introduced at once. Off-diagonal NSI
parameters could be tested down to the level of 10−3, whereas the diagonal
combinations (ϵee−ϵττ) and
(ϵμμ−ϵττ) can be tested down to 10−1 and
10−2, respectively. The possibilities of observing CP violation in this
context are also explored, by presenting a first scan of the CP discovery
potential of the NF setups to the phases ϕeμ,ϕeτ and
δ. We study separately the case where CP violation comes only from
non-standard sources, and the case where it is entangled with the standard
source, δ. In case δ turns out to be CP conserving, the
interesting possibility of observing CP violation for reasonably small values
of the NSI parameters emerges.Comment: Final note added. 38 pages, 11 figure
Compressed representation of a partially defined integer function over multiple arguments
- Author
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- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
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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
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