1,216 research outputs found
Pennsylvanian-Early Triassic stratigraphy in the Alborz Mountains (Iran)
- Author
- Al-Belushi
- Alda Nicora
- Altiner
- Angiolini
- Assereto
- Baghbani
- Baghbani
- Balme
- Bensh
- Besse
- Boncheva
- Broglio Loriga
- Brönnimann
- Brönnimann
- Chateauneuf
- Chernyshev
- Dario Sciunnach
- Davydov
- Elliott
- Fantini Sestini
- Fantini Sestini
- Fantini Sestini
- Fantini Sestini
- Fantini Sestini
- Feinberg
- Flügel
- Flügel
- Flügel
- Foster
- Fraiser
- Gaetani
- Gansser
- Garzanti
- Ghavidel-Syooki
- Glaus
- Grant
- Gregory D. Price
- Hammer
- Haq
- Helby
- Heravi
- Hirsch
- Holzer
- Horacek
- Insalaco
- Isbell
- Jafar Sabouri
- Jenny
- Jenny
- Jenny
- Jin
- Jin
- Kalashnikov
- Katsumi Ueno
- Ketat
- Khaler
- Kireeva
- Kobayashi
- Korte
- Lasemi
- Leven
- Leven
- Leven
- Leven
- Leven
- Lucia Angiolini
- Lys
- Maurizio Gaetani
- Meissami
- Meissami
- Michael H. Stephenson
- Nazemi
- Posenato
- Roberto Rettori
- Ruban
- Rui
- Ruttner
- Savary
- Schellwien
- Sciunnach
- Seyed-Emami
- Shapiro
- Sharland
- Shi
- Stampfli
- Stephenson
- Stephenson
- Ueno
- Van Wagoner
- Wardlaw
- Zaninetti
- Zaninetti
- Zolotova
- Publication venue
- 'Geological Society of London'
- Publication date
- 01/01/2009
- Field of study
New fieldwork was carried out in the central and eastern Alborz, addressing the sedimentary succession from the Pennsylvanian to the Early Triassic. A regional synthesis is proposed, based on sedimentary analysis and a wide collection of new palaeontological data. The Moscovian Qezelqaleh Formation, deposited in a mixed coastal marine and alluvial setting, is present in a restricted area of the eastern Alborz, transgressing on the Lower Carboniferous Mobarak and Dozdehband formations. The late Gzhelian–early Sakmarian Dorud Group is instead distributed over most of the studied area, being absent only in a narrow belt to the SE. The Dorud Group is typically tripartite, with a terrigenous unit in the lower part (Toyeh Formation), a carbonate intermediate part (Emarat and Ghosnavi formations, the former particularly rich in fusulinids), and a terrigenous upper unit (Shah Zeid Formation), which however seems to be confined to the central Alborz. A major gap in sedimentation occurred before the deposition of the overlying Ruteh Limestone, a thick package of packstone–wackestone interpreted as a carbonate ramp of Middle Permian age (Wordian–Capitanian). The Ruteh Limestone is absent in the eastern part of the range, and everywhere ends with an emersion surface, that may be karstified or covered by a lateritic soil.
The Late Permian transgression was directed southwards in the central Alborz, where marine facies (Nesen Formation) are more common. Time-equivalent alluvial fans with marsh intercalations and lateritic soils (Qeshlaq Formation) are present in the east. Towards the end of the Permian most of the Alborz emerged, the marine facies being restricted to a small area on the Caspian side of the central Alborz. There, the Permo-Triassic boundary interval is somewhat similar to the Abadeh–Shahreza belt in central Iran, and contains oolites, flat microbialites and domal stromatolites, forming the base of the Elikah Formation. The P–T boundary is established on the basis of conodonts, small foraminifera and stable isotope data. The development of the lower and middle part of the Elikah Formation, still Early Triassic in age, contains vermicular bioturbated mudstone/wackestone, and anachronostic-facies-like gastropod oolites and flat pebble conglomerates.
Three major factors control the sedimentary evolution. The succession is in phase with global sea-level curve in the Moscovian and from the Middle Permian upwards. It is out of phase around the Carboniferous–Permian boundary, when the Dorud Group was deposited during a global lowstand of sealevel. When the global deglaciation started in the Sakmarian, sedimentation stopped in the Alborz and the area emerged. Therefore, there is a consistent geodynamic control. From the Middle Permian upwards, passive margin conditions control the sedimentary evolution of the basin, which had its depocentre(s) to the north. Climate also had a significant role, as the Alborz drifted quickly northwards with other central Iran blocks towards the Turan active margin. It passed from a southern latitude through the aridity belt in the Middle Permian, across the equatorial humid belt in the Late Permian and reached the northern arid tropical belt in the Triassic
Origin and evolution of water oxidation before the last common ancestor of the Cyanobacteria
- Author
- A. William Rutherford
- Anisimova
- Arato
- Arnold
- Bader
- Beanland
- Blankenship
- Campbell
- Cardona
- Cardona
- Chu
- Chu
- Clausen
- Cox
- Criscuolo
- Cser
- Dagan
- Dau
- Debus
- Debus
- Deusch
- Diner
- Dismukes
- Erickson
- Ferreira
- Fine
- Flannery
- Gan
- Gan
- Giorgi
- Gould
- Gouy
- Guindon
- Gupta
- Guskov
- Hasegawa
- Hillier
- Hoganson
- Hohmann-Marriott
- Huson
- Ishikita
- Ishikita
- James W. Murray
- Jia
- Johnson
- Kiss
- Klimov
- Kopp
- Koyama
- Kulkarni
- Kuroda
- Lambreva
- Larom
- Larsson
- Lartillot
- Lee
- Lidholm
- Linke
- Loll
- Lyons
- Marin
- Merry
- Metz
- Michel
- Michel
- Mimuro
- Muh
- Mulo
- Mulo
- Murray
- Murray
- Nakamura
- Nitschke
- Nixon
- Nixon
- Nixon
- Ochoa de Alda
- Oettmeier
- Ogami
- Park
- Petrouleas
- Qian
- Rappaport
- Rasmussen
- Raymond
- Rippka
- Robinson
- Rodriguez-Ezpeleta
- Roose
- Rutherford
- Rutherford
- Saito
- Sauer
- Saw
- Sedoud
- Service
- Shevela
- Shi
- Shih
- Sicora
- Sicora
- Siegbahn
- Sievers
- Sugiura
- Sugiura
- Sugiura
- Sugiura
- Summerfield
- Tanai Cardona
- Tichy
- Toepel
- Turner
- Ulas
- Umena
- Vass
- Vassiliev
- Vermaas
- Vermaas
- Vermaas
- Vinyard
- Waldbauer
- Wegener
- Yoon
- Zehr
- Zhang
- Zhang
- Zimmermann
- Publication venue
- 'Oxford University Press (OUP)'
- Publication date
- 01/02/2015
- Field of study
Photosystem II, the water oxidizing enzyme, altered the course of evolution by filling the atmosphere with oxygen. Here, we reconstruct the origin and evolution of water oxidation at an unprecedented level of detail by studying the phylogeny of all D1 subunits, the main protein coordinating the water oxidizing cluster (Mn4CaO5) of Photosystem II. We show that D1 exists in several forms making well-defined clades, some of which could have evolved before the origin of water oxidation and presenting many atypical characteristics. The most ancient form is found in the genome of Gloeobacter kilaueensis JS-1 and this has a C-terminus with a higher sequence identity to D2 than to any other D1. Two other groups of early evolving D1 correspond to those expressed under prolonged far-red illumination and in darkness. These atypical D1 forms are characterized by a dramatically different Mn4CaO5 binding site and a Photosystem II containing such a site may assemble an unconventional metal cluster. The first D1 forms with a full set of ligands to the Mn4CaO5 cluster are grouped with D1 proteins expressed only under low oxygen concentrations and the latest evolving form is the dominant type of D1 found in all cyanobacteria and plastids. In addition, we show that the plastid ancestor had a D1 more similar to those in early branching Synechococcus. We suggest each one of these forms of D1 originated from transitional forms at different stages towards the innovation and optimization of water oxidation before the last common ancestor of all known cyanobacteria
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
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- Bhatti A
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- Bian JG
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- Bilei GM
- Bilin B
- Bilinskas MJ
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- Biselli A
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- Bitioukov S
- Blekman F
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- Bondu O
- Bontenackels M
- 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
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- Boutemeur M
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- 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
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- Burgmeier A
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- Busson P
- Busza W
- Butler JN
- Butler PH
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- Butz E
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- Cabrera A
- Cabrillo IJ
- Caebergs T
- Cakir A
- Calabria C
- Calderon De La Barca Sanchez M
- Calderon A
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- Callner J
- Calvert B
- Calvo E
- Campagnari C
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- Cappello G
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- Carlsmith D
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- Casal B
- Casimiro Linares E
- Castaldi R
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- Castilla-Valdez H
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- Caudron J
- Caulfield M
- Cavallari F
- Cavallo FR
- Cavallo N
- Cavanaugh R
- Ceard L
- Ceballos GG
- Cepeda M
- Cerati GB
- Cerci DS
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- Cerizza G
- Cerminara G
- Cerrada M
- Chabert EC
- Chadwick M
- Chakaberia I
- Chamizo Llatas M
- Chan M
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- Chang YH
- Chang YH
- Chang YW
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- Chao Y
- Charaf O
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- Chasco M
- Chasserat J
- Chatrchyan S
- Chatterjee A
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- Cherepanov V
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- Chetluru V
- Cheung HWK
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- Choudhary BC
- Choudhury RK
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- Chuang SH
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- Ciesielski R
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- Cimmino A
- Cipriano PMR
- Cirino G
- Cittolin S
- Ciulli V
- Civinini C
- Claes DR
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- 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
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- del Arbol PMR
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- Dero V
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- Di Giovanni GP
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- Di Marco E
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- Diamond B
- Dias FA
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- Djordjevic M
- Dobrzynski L
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- Edelmaier CJ
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- Elvira VD
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- Fehling D
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- Ferapontov A
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- Fernandez Perez Tomei TR
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- Field RD
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- Finger M
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- Fisk I
- Flacher H
- Flanagan W
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- Flossdorf A
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- Gary JW
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- Golovtsov V
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- Grigelionis I
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- Gruschke J
- Guchait M
- Gude A
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- Guo ZJ
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- Gurtu A
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- Yilmaz Y
- Yohay R
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- 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
- Zarubin A
- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
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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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- 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
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
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Afanasiev S
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
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- Akin IV
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- Alcaraz Maestre J
- Alda Junior WL
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- Aliev T
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- Alverson G
- Alves GA
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- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
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- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
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- Chang S
- Chang YH
- Chang YH
- Chang YW
- Chanon N
- Chao Y
- Charaf O
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- Chasco M
- Chasserat J
- Chatrchyan S
- Chatterjee A
- Chauhan S
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- Chen GM
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- 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
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- Correa Martins Junior M
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- Costantini S
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- Coughlan JA
- Cousins R
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- Cox PT
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- Cremaldi LM
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- Cumalat JP
- Cuplov V
- Cushman P
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- Wissing C
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- Wittmer B
- Woehri HK
- Wolf M
- Wolf R
- Womersley WJ
- Won S
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- Wood JS
- Worm SD
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- 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
- 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
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
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- Yilmaz Y
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- 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
Measurement of the Z/gamma* + b-jet cross section in pp collisions at 7 TeV
- Author
- Abbaneo D.
- Abbiendi G.
- Abbrescia M.
- Abdullin S.
- Acosta D.
- Acosta J. G.
- Acosta M. Vazquez
- Adair A.
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- Adler V.
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- Aguilar-Benitez M.
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- Battilana C.
- Baty C.
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- Belyaev A.
- Benaglia A.
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- Bendavid J.
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- Benelli G.
- Benhabib L.
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- Berryhill J.
- Bertl W.
- Berzano U.
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- Betchart B.
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- Blobel V.
- Bloch D.
- Bloch I.
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- Bodek A.
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- Boldizsar L.
- Bolla G.
- Bolognesi S.
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- Bonacorsi D.
- Bonato A.
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- Bontenackels M.
- Boos E.
- Bornheim A.
- Borras K.
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- Bortignon P.
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- Bose S.
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- Bostock F.
- Botta C.
- Boudoul G.
- Boulahouache C.
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- Yun J. C.
- Zabel J.
- Zabi A.
- Zablocki J.
- Zaganidis N.
- Zakaria M.
- Zalewski P.
- Zanetti M.
- Zang J.
- Zang S. L.
- Zarubin A.
- Zatserklyaniy A.
- Zeinali M.
- Zeise M.
- Zeuner W. D.
- Zeyrek M.
- Zhang J.
- Zhang Z.
- Zheng Y.
- Zhokin A.
- Zhu B.
- Zhu R. Y.
- Zhukov V.
- Zhukova V.
- Ziebarth E. B.
- Ziegler J.
- Zielinski M.
- Zito G.
- Zoeller M. H.
- Zotto P.
- Zou W.
- Zumerle G.
- Zuranski A.
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
The production of b jets in association with a Z/gamma* boson is studied
using proton-proton collisions delivered by the LHC at a centre-of-mass energy
of 7 TeV and recorded by the CMS detector. The inclusive cross section for
Z/gamma* + b-jet production is measured in a sample corresponding to an
integrated luminosity of 2.2 inverse femtobarns. The Z/gamma* + b-jet cross
section with Z/gamma* to ll (where ll = ee or mu mu) for events with the
invariant mass 60 < M(ll) < 120 GeV, at least one b jet at the hadron level
with pT > 25 GeV and abs(eta) < 2.1, and a separation between the leptons and
the jets of Delta R > 0.5 is found to be 5.84 +/- 0.08 (stat.) +/- 0.72 (syst.)
+(0.25)/-(0.55) (theory) pb. The kinematic properties of the events are also
studied and found to be in agreement with the predictions made by the MadGraph
event generator with the parton shower and the hadronisation performed by
PYTHIA.Comment: Submitted to the Journal of High Energy Physic
Compressed representation of a partially defined integer function over multiple arguments
- Author
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- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
- Abdulsalam A
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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
Measurement of jet fragmentation into charged particles in pp and PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
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- Anagnostou G
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- Yilmaz Y
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- Yun JC
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- Zablocki J
- Zaganidis N
- Zakaria M
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- Zanetti M
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- 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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- Zielinski M
- Zito G
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- Zou W
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
Jet fragmentation in pp and PbPb collisions at a centre-of-mass energy of
2.76 TeV per nucleon pair was studied using data collected with the CMS
detector at the LHC. Fragmentation functions are constructed using
charged-particle tracks with transverse momenta pt > 4 GeV for dijet events
with a leading jet of pt > 100 GeV. The fragmentation functions in PbPb events
are compared to those in pp data as a function of collision centrality, as well
as dijet-pt imbalance. Special emphasis is placed on the most central PbPb
events including dijets with unbalanced momentum, indicative of energy loss of
the hard scattered parent partons. The fragmentation patterns for both the
leading and subleading jets in PbPb collisions agree with those seen in pp data
at 2.76 TeV. The results provide evidence that, despite the large parton energy
loss observed in PbPb collisions, the partition of the remaining momentum
within the jet cone into high-pt particles is not strongly modified in
comparison to that observed for jets in vacuum.Comment: Submitted to the Journal of High Energy Physic
Linear and Branched Glyco-Lipopeptide Vaccines Follow Distinct Cross-Presentation Pathways and Generate Different Magnitudes of Antitumor Immunity
- Author
- A Hosmalin
- A Margalit
- A Roth
- AA Chentoufi
- AA Chentoufi
- AA Chentoufi
- AB Nesburn
- AL Ackerman
- AL Sorensen
- AL Sorensen
- Alda Shi
- AM Ercolini
- Anthony B. Nesburn
- AR Hearn
- B Monzavi-Karbassi
- C Bourgeois
- C Durier
- C Hotta
- C Mesa
- C Shepherd
- C Vazquez-Martin
- CC Peeters
- CE Ruby
- D Dorfel
- DC Jackson
- Derya Unutmaz
- DM Lubaroff
- E Belnoue
- E Davila
- E Lazoura
- E Maraskovsky
- G Curigliano
- G Curigliano
- G Dasgupta
- G Deliyannis
- G Hoeffel
- G Moron
- Gargi Dasgupta
- GF Springer
- GT Belz
- H Gahery
- H Gahery
- H Norell
- I Bettahi
- I Bettahi
- I Bettahi
- I Vicente-Suarez
- Ilham Bettahi
- JA Hollenbaugh
- JC Manimala
- JC Tseng
- JY Kang
- KC Roy
- KL Rock
- KN Khan
- KN Syrigos
- L BenMohamed
- L BenMohamed
- L BenMohamed
- L BenMohamed
- L BenMohamed
- L BenMohamed
- L BenMohamed
- L Chen
- Lbachir BenMohamed
- LM Weiner
- M Andrieu
- M Larsson
- M Svensson
- M Triantafilou
- MA Tarp
- MKt Lee
- MV Dhodapkar
- N Monu
- N Petrovsky
- NA Pfender
- O Renaudet
- Olivier Renaudet
- P Nava-Parada
- P Schnorrer
- P van der Bruggen
- Pascal Dumy
- PB Watchmaker
- Q Zhu
- R Belizaire
- R Lo-Man
- R Spohn
- S Bay
- S Borsutzky
- S Casillas
- S Grigalevicius
- S Hakomori
- S Ingale
- S Ingale
- S Khan
- S Radhakrishnan
- S Samanta
- S Vichier-Guerre
- S Vichier-Guerre
- SD Xiang
- SF Slovin
- SJ Keding
- T Buskas
- T Fehr
- T Warger
- TA Groothuis
- TR Smith
- V Kudryashov
- VG Moron
- WR Heath
- X Qi
- X Zhang
- X Zhang
- X Zhu
- Publication venue
- Public Library of Science
- Publication date
- 01/06/2010
- Field of study
Glyco-lipopeptides, a form of lipid-tailed glyco-peptide, are currently under intense investigation as B- and T-cell based vaccine immunotherapy for many cancers. However, the cellular and molecular mechanisms of glyco-lipopeptides (GLPs) immunogenicity and the position of the lipid moiety on immunogenicity and protective efficacy of GLPs remain to be determined.We have constructed two structural analogues of HER-2 glyco-lipopeptide (HER-GLP) by synthesizing a chimeric peptide made of one universal CD4(+) epitope (PADRE) and one HER-2 CD8(+) T-cell epitope (HER(420-429)). The C-terminal end of the resulting CD4-CD8 chimeric peptide was coupled to a tumor carbohydrate B-cell epitope, based on a regioselectively addressable functionalized templates (RAFT), made of four alpha-GalNAc molecules. The resulting HER glyco-peptide (HER-GP) was then linked to a palmitic acid moiety, attached either at the N-terminal end (linear HER-GLP-1) or in the middle between the CD4+ and CD8+ T cell epitopes (branched HER-GLP-2). We have investigated the uptake, processing and cross-presentation pathways of the two HER-GLP vaccine constructs, and assessed whether the position of linkage of the lipid moiety would affect the B- and T-cell immunogenicity and protective efficacy. Immunization of mice revealed that the linear HER-GLP-1 induced a stronger and longer lasting HER(420-429)-specific IFN-gamma producing CD8(+) T cell response, while the branched HER-GLP-2 induced a stronger tumor-specific IgG response. The linear HER-GLP-1 was taken up easily by dendritic cells (DCs), induced stronger DCs maturation and produced a potent TLR- 2-dependent T-cell activation. The linear and branched HER-GLP molecules appeared to follow two different cross-presentation pathways. While regression of established tumors was induced by both linear HER-GLP-1 and branched HER-GLP-2, the inhibition of tumor growth was significantly higher in HER-GLP-1 immunized mice (p<0.005).These findings have important implications for the development of effective GLP based immunotherapeutic strategies against cancers
- …