6,264 research outputs found
Estimating the Creation and Removal Date of Fracking Ponds Using Trend Analysis of Landsat Imagery
- Publication venue
- The Cupola: Scholarship at Gettysburg College
- Publication date
- 05/01/2018
- Field of study
Hydraulic fracturing, or fracking, is a process of introducing liquid at high pressure to create fractures in shale rock formations, thus releasing natural gas. Flowback and produced water from fracking operations is typically stored in temporary open-air earthen impoundments, or frack ponds. Unfortunately, in the United States there is no public record of the location of impoundments, or the dates that impoundments are created or removed. In this study we use a dataset of drilling-related impoundments in Pennsylvania identified through the FrackFinder project led by SkyTruth, an environmental non-profit. For each impoundment location, we compiled all low cloud Landsat imagery from 2000 to 2016 and created a monthly time series for three bands: red, near-infrared (NIR), and the Normalized Difference Vegetation Index (NDVI). We identified the approximate date of creation and removal of impoundments from sudden breaks in the time series. To verify our method, we compared the results to date ranges derived from photointerpretation of all available historical imagery on Google Earth for a subset of impoundments. Based on our analysis, we found that the number of impoundments built annually increased rapidly from 2006 to 2010, and then slowed from 2010 to 2013. Since newer impoundments tend to be larger, however, the total impoundment area has continued to increase. The methods described in this study would be appropriate for finding the creation and removal date of a variety of industrial land use changes at known locations
Implementation of On-Line Data Reduction Algorithms in the CMS Endcap Preshower Data Concentrator Card
- Author
- Publication venue
- Publication date
- 16/11/2006
- Field of study
The CMS Endcap Preshower (ES) sub-detector comprises 4288 silicon sensors, each containing 32 strips. The data are transferred from the detector to the counting room via 1208 optical fibres running at 800Mbps. Each fibre carries data from 2, 3 or 4 sensors. For the readout of the Preshower, a VME-based system - the Endcap Preshower Data Concentrator Card (ES-DCC) is currently under development. The main objective of each readout board is to acquire on-detector data from up to 36 optical links, perform on-line data reduction (zero suppression) and pass the concentrated data to the CMS event builder. This document presents the conceptual design of the Reduction Algorithms as well as their implementation into the ES-DCC FPGAs. The algorithms implemented into the ES-DCC resulted in a reduction factor of ~20
Radiation hardness qualification of PbWO4 scintillation crystals for the CMS Electromagnetic Calorimeter
- Author
- A Askew
- A Bartoloni
- A Borisevitch
- A Bornheim
- A Cecilia
- A David
- A De Benedetti
- A Dolgopolov
- A Elliott-Peisert
- A Fedorov
- A Ghezzi
- A Givernaud
- A Go
- A Honma
- A Inyakin
- A K Mohanty
- A Kyriakis
- A Ledovskoy
- A Markou
- A Nardulli
- A Nikitenko
- A Palma
- A Papadakis
- A Pullia
- A Rosowsky
- A Singovsky
- A Sirunyan
- A Topkar
- A Uzunian
- A Zabi
- A. Annenkov .
- B Betev
- B C Choudhary
- B Camanzi
- B Cox
- B Fabbro
- B Gobbo
- B Heltsley
- B Ille
- B W Kennedy
- C Baty
- C Bernet
- C Biino
- C Charlot
- C H Shepherd-Themistocleous
- C Jessop
- C M Kuo
- C Marchica
- C Markou
- C Mavrommatis
- C Rogan
- C Rovelli
- C Seez
- C Siamitros
- C Thiebaux
- C Timlin
- CMS collaboration
- CMS collaboration
- D Andelin
- D Bandurin
- D Barney
- D Del Re
- D Denegri
- D Dutta
- D Franci
- D G Cussans
- D G Phillips
- D J A Cockerill
- D Jovanovic
- D Krpic
- D Loukas
- D Maletic
- D R Da Silva Di Calafiori
- D Renker
- D Sillou
- D Wardrope
- E A Chen
- E Auffray
- E Di Marco
- E Locci
- E Longo
- E Petrakou
- E. Auffray
- E. Auffray
- E. Auffray .
- F A Triantis
- F Cavallari
- F Cossutti
- F Ferri
- F Moortgat
- F Nessi-Tedaldi
- F Pauss
- F Ptochos
- F Stöckli
- F X Gentit
- G Daskalakis
- G Della Ricca
- G Dissertori
- G Drobychev
- G Franzoni
- G Hamel de Monchenault
- G Organtini
- G W S Hou
- H B Newman
- H El Mamouni
- H F Heath
- I Anicin
- I Dafinei
- I Evangelou
- I Papadakis
- I Papadopoulos
- I Puljak
- I Yaselli
- I. Dafinei
- I. Dafinei
- I. Dafinei .
- J Blaha
- J Bourotte
- J Descamps
- J Fay
- J G Shiu
- J H Williams
- J Haupt
- J L Faure
- J Malclès
- J Nash
- J Puzovic
- J R Patterson
- J Rander
- J Silva
- J Swain
- J Varela
- J Veverka
- J Weng
- J Zhang
- J-P Peigneux
- J. Sykora
- K Deiters
- K Freudenreich
- K Kaadze
- K Theofilatos
- K Ueno
- K W Bell
- K Zhu
- L Djambazov
- L Dobrzynski
- L M Barone
- L Pant
- L Sala
- L Y Zhang
- M Balazs
- M Besancon
- M Buehler
- M Dejardin
- M Diemoz
- M Dittmar
- M Djordjevic
- M Dzelalija
- M Gataullin
- M Haguenauer
- M Hansen
- M Huhtinen
- M J Ryan
- M Korjik
- M Lebeau
- M Lethuillier
- M M Obertino
- M Malberti
- M Marone
- M Paganoni
- M Ronquest
- M Schneegans
- M Takahashi
- M Titov
- M W Arenton
- M Wang
- M Weber
- M. Nikl .
- N Almeida
- N Cartiglia
- N Godinovic
- N Golubev
- N Grant
- N Krasnikov
- N Manthos
- N Marinelli
- N Pastrone
- N Redaelli
- N Tyurin
- O Missevitch
- O Teller
- P A Razis
- P Adzic
- P Bloch
- P Busson
- P Chang
- P D Luckey
- P Depasse
- P Govoni
- P Gras
- P Jarry
- P Kokkas
- P Kyberd
- P Lecomte
- P Lecoq
- P Meridiani
- P Milenovic
- P Miné
- P Musella
- P Nedelec
- P Negri
- P Paganini
- P Parracho
- P Piroué
- P R Hobson
- P Ribeiro
- P Rumerio
- P Sharp
- P Shukla
- P Silva
- P Verrecchia
- P. Bohacek .
- P. Lecoq
- Q Ingram
- R Arcidiacono
- R Beuselinck
- R Chipaux
- R Hirosky
- R K Choudhury
- R K Shivpuri
- R M Brown
- R Paramatti
- R Rusack
- R Salerno
- R Y Zhu
- R Yohay
- R. Chipaux
- R. Chipaux
- R. Chipaux .
- S Argiro
- S Baccaro
- S Baffioni
- S Beauceron
- S Conetti
- S Cooper
- S Drndarevic
- S Ganjour
- S Gascon
- S Gninenko
- S K Kataria
- S Kailas
- S Ragazzi
- S Rahatlou
- S Reucroft
- S Troshin
- S V Rusakov
- S W Lin
- S Zelepoukine
- T Camporesi
- T Kolberg
- T Orimoto
- T Punz
- T Tabarelli de Fatis
- T Virdee
- The CMS Electromagnetic Calorimeter Group
- V J Smith
- V Kachanov
- V Litvine
- V Matveev
- V Tancini
- V Timciuc
- W Funk
- W Hintz
- W Lin
- W Lustermann
- W T Chen
- Y H Chang
- Y Hsiung
- Y Kubota
- Y Ma
- Y Maravin
- Y Musienko
- Y Sirois
- Y Yang
- Z Antunovic
- Z Chen
- Publication venue
- 'IOP Publishing'
- Publication date
- 21/12/2009
- Field of study
This is the Pre-print version of the Article. The official published version can be accessed from the link below - Copyright @ 2010 IOPEnsuring the radiation hardness of PbWO4 crystals was one of the main priorities during the construction of the electromagnetic calorimeter of the CMS experiment at CERN. The production on an industrial scale of radiation hard crystals and their certification over a period of several years represented a difficult challenge both for CMS and for the crystal suppliers. The present article reviews the related scientific and technological problems encountered
Intercalibration of the barrel electromagnetic calorimeter of the CMS experiment at start-up
- Author
- A. Askew
- A. Bartoloni
- A. Bornheim
- A. David
- A. De Min
- A. De Min
- A. Elliott-Peisert
- A. Ghezzi
- A. Givernaud
- A. Go
- A. Honma
- A. Kyriakis
- A. Ledovskoy
- A. Markou
- A. Nardulli
- A. Nikitenko
- A. Palma
- A. Papadakis
- A. Pullia
- A. Rosowsky
- A. Singovsky
- A. Sirunyan
- A. Tcheremoukhine
- A. Tobias
- A. Topkar
- A. Uzunian
- A. Zabi
- A.B. Lodge
- A.D. Min
- A.K. Mohanty
- A.L. Lintern
- A.M. Brett
- B. Betev
- B. Camanzi
- B. Cox
- B. Fabbro
- B. Gobbo
- B. Heltsley
- B. Ille
- B. Panev
- B.C. Choudhary
- B.J. Smith
- B.W. Kennedy
- C. Baty
- C. Bernet
- C. Biino
- C. Charlot
- C. Combaret
- C. Gargiulo
- C. Jessop
- C. Lynch
- C. Marchica
- C. Markou
- C. Mavrommatis
- C. Rogan
- C. Rovelli
- C. Seez
- C. Siamitros
- C. Thiebaux
- C. Timlin
- C.H. Shepherd-Themistocleous
- C.M. Kuo
- D. Andelin
- D. Bandurin
- D. Barney
- D. Britton
- D. Del Re
- D. Denegri
- D. Dutta
- D. Franci
- D. Gong
- D. Jovanovic
- D. Krpic
- D. Loukas
- D. Maletic
- D. Renker
- D. Schinzel
- D. Sillou
- D. Wardrope
- D.G. Cussans
- D.G. Phillips
- D.J.A. Cockerill
- D.L. Evans
- D.R. Da Silva Di Calafiori
- D.R. Da Silva Di Calafiori
- Daniele Del Re
- E. Auffray
- E. Carrera
- E. Di Marco
- E. Locci
- E. Petrakou
- E. Vlassov
- E.A. Chen
- E.D. Marco
- Egidio Longo
- F. Cavallari
- F. Cossutti
- F. Ferri
- F. Moortgat
- F. Nessi-Tedaldi
- F. Pauss
- F. Ptochos
- F. Rondeaux
- F. Santanastasio
- F. Stockli
- F.A. Triantis
- F.X. Gentit
- G. Anagnostou
- G. Daskalakis
- G. Davatz
- G. Della Ricca
- G. Della Ricca
- G. Dissertori
- G. Franzoni
- G. Hamel De Monchenault
- G. Leshev
- G. Maurelli
- G. Milleret
- G.H. De
- G.W.S. Hou
- Giovanni Organtini
- H. El Mamouni
- H. El Mamouni
- H. Mahlke-Krueger
- H. Mathez
- H. Suter
- H.B. Newman
- H.F. Heath
- H.P. Von
- H.P. Von Gunten
- I. Anicin
- I. Dafinei
- I. Evangelou
- I. Mandjavidze
- I. Papadakis
- I. Papadopoulos
- I. Puljak
- I. Yaselli
- J. Blaha
- J. Bourotte
- J. Descamps
- J. Fay
- J. Gilly
- J. Malcles
- J. Nash
- J. Puzovic
- J. Rander
- J. Silva
- J. Swain
- J. Varela
- J. Veverka
- J. Weng
- J. Zhang
- J.A. Hill
- J.E. Duboscq
- J.G. Shiu
- J.H. Williams
- J.L. Faure
- J.M. Reymond
- J.P. Guillaud
- J.R. Patterson
- K. Deiters
- K. Freudenreich
- K. Kaadze
- K. Kloukinas
- K. Theofilatos
- K. Ueno
- K. Zhu
- K.W. Bell
- L. Djambazov
- L. Dobrzynski
- L. Guevara Riveros
- L. Pant
- L. Sala
- L.Y. Zhang
- Luciano Maria Barone
- M. Anfreville
- M. Balazs
- M. Bercher
- M. Besancon
- M. Buehler
- M. Cerutti
- M. Dejardin
- M. Diemoz
- M. Dittmar
- M. Djordjevic
- M. Dzelalija
- M. Gataullin
- M. Haguenauer
- M. Hansen
- M. Husejko
- M. Lebeau
- M. Lethuillier
- M. Malberti
- M. Marone
- M. Mur
- M. Paganoni
- M. Ronquest
- M. Sproston
- M. Takahashi
- M. Titov
- M. Wang
- M. Weber
- M.D. Ghodgaonkar
- M.J. Ryan
- M.M. Obertino
- M.W. Arenton
- Marco E. Di
- N. Almeida
- N. Cartiglia
- N. Godinovic
- N. Golubev
- N. Grant
- N. Krasnikov
- N. Manthos
- N. Marinelli
- N. Pastrone
- N. Redaelli
- N. Tyurin
- N. Zamiatin
- O. Atramentov
- O. Teller
- P. Adzic
- P. Bloch
- P. Busson
- P. Chang
- P. Depasse
- P. Govoni
- P. Gras
- P. Jarry
- P. Kokkas
- P. Kumar
- P. Kyberd
- P. Lecomte
- P. Lecoq
- P. Meridiani
- P. Milenovic
- P. Mine
- P. Musella
- P. Nedelec
- P. Negri
- P. Paganini
- P. Parracho
- P. Piroue
- P. Ribeiro
- P. Rumerio
- P. Sharp
- P. Shukla
- P. Silva
- P. Verrecchia
- P. Vichoudis
- P.A. Razis
- P.D. Luckey
- P.R. Hobson
- P.S. Flower
- Q. Ingram
- R. Alemany-Fernandez
- R. Arcidiacono
- R. Benetta
- R. Beuselinck
- R. Chipaux
- R. Della Negra
- R. Della Negra
- R. Hirosky
- R. Imlay
- R. Paramatti
- R. Rusack
- R. Salerno
- R. Yohay
- R.J.S. Greenhalgh
- R.K. Choudhury
- R.K. Shivpuri
- R.M. Brown
- R.Y. Zhu
- S. Argiro
- S. Baccaro
- S. Baffioni
- S. Beauceron
- S. Blyth
- S. Conetti
- S. Drndarevic
- S. Ganjour
- S. Gascon
- S. Gninenko
- S. Kailas
- S. Ragazzi
- S. Reucroft
- S. Troshin
- S. Zelepoukine
- S.K. Kataria
- S.V. Rusakov
- S.W. Lin
- Shahram Rahatlou
- T. Camporesi
- T. Kolberg
- T. Orimoto
- T. Punz
- T. Romanteau
- T. Tabarelli De Fatis
- T. Virdee
- T.T. De
- The Cms Electromagnetic Calorimeter Group
- U. Berthon
- U. Roeser
- V. Kachanov
- V. Litvine
- V. Matveev
- V. Tancini
- V. Timciuc
- V.J. Smith
- W. Funk
- W. Hintz
- W. Lin
- W. Lustermann
- W.T. Chen
- Y. Geerebaert
- Y. Gershtein
- Y. Hsiung
- Y. Kubota
- Y. Ma
- Y. Maravin
- Y. Musienko
- Y. Sirois
- Y. Yang
- Y.H. Chang
- Z. Antunovic
- Z. Chen
- Publication venue
- International School of Advanced Studies
- Publication date
- 01/01/2008
- Field of study
Calibration of the relative response of the individual channels of the barrel electromagnetic calorimeter of the CMS detector was accomplished, before installation, with cosmic ray muons and test beams. One fourth of the calorimeter was exposed to a beam of high energy electrons and the relative calibration of the channels, the intercalibration, was found to be reproducible to a precision of about 0.3%. Additionally, data were collected with cosmic rays for the entire ECAL barrel during the commissioning phase. By comparing the intercalibration constants obtained with the electron beam data with those from the cosmic ray data, it is demonstrated that the latter provide an intercalibration precision of 1.5% over most of the barrel ECAL. The best intercalibration precision is expected to come from the analysis of events collected in situ during the LHC operation. Using data collected with both electrons and pion beams, several aspects of the intercalibration procedures based on electrons or neutral pions were investigated
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
- 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
- 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
- Burkett K
- Busson P
- 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
- Campbell A
- 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
- Castro E
- Caudron J
- Caulfield M
- Cavallari F
- Cavallo FR
- Cavallo N
- Cavanaugh R
- Ceard L
- 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
- 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
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- Zeinali M
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- 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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- Christiansen T
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- Clerbaux B
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- CMS Collaboration
- Cockerill DJA
- Codispoti G
- Colafranceschi S
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- Cole JE
- Colino N
- Collard C
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- Conetti S
- Contardo D
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- Conway J
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- Cooper SI
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- Cornelis T
- Correa Martins Junior M
- Cortezon EP
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- Costantini S
- Coughlan JA
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- Cuevas J
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- Cwiok M
- Czellar S
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- Da Costa EM
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- 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
Constraints on the χ_(c1) versus χ_(c2) polarizations in proton-proton collisions at √s = 8 TeV
- Author
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- Zorbakir I. S.
- Zorbilmez C.
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- Zuolo D.
- Álvarez Fernández A.
- Özçelik Ö.
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 24/04/2020
- Field of study
The polarizations of promptly produced χ_(c1) and χ_(c2) mesons are studied using data collected by the CMS experiment at the LHC, in proton-proton collisions at √s=8 TeV. The χ_c states are reconstructed via their radiative decays χ_c → J/ψγ, with the photons being measured through conversions to e⁺e⁻, which allows the two states to be well resolved. The polarizations are measured in the helicity frame, through the analysis of the χ_(c2) to χ_(c1) yield ratio as a function of the polar or azimuthal angle of the positive muon emitted in the J/ψ → μ⁺μ⁻ decay, in three bins of J/ψ transverse momentum. While no differences are seen between the two states in terms of azimuthal decay angle distributions, they are observed to have significantly different polar anisotropies. The measurement favors a scenario where at least one of the two states is strongly polarized along the helicity quantization axis, in agreement with nonrelativistic quantum chromodynamics predictions. This is the first measurement of significantly polarized quarkonia produced at high transverse momentum
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