671 research outputs found
Angular and Current-Target Correlations in Deep Inelastic Scattering at HERA
- Author
- Abbiendi G
- Abe T
- Abramowicz H
- Acosta D
- Adamczyk L
- Adamus M
- Ahn Sh
- Amelung C
- An Sh
- Anselmo F
- Antonioli P
- Arneodo M
- Bacon Tc
- Badgett Wf
- Bailey Dc
- Bailey Ds
- Bamberger A
- Barbagli G
- Bari G
- Barreiro F
- Barret O
- Bashindzhagyan Gl
- Bashkirov V
- Basile M
- Bauerdick Lat
- Bednarek B
- Behrens U
- Bellagamba L
- Bertolin A
- Bhadra S
- Bienlein Jk
- Blaikley He
- Bohnet I
- Bokel C
- Boogert S
- Bornheim A
- Borzemski P
- Boscherini D
- Botje M
- Breitweg J
- Brock I
- Brook Nh
- Brugnera Riccardo
- Brummer N
- Bruni A
- Bruni G
- Burgard C
- Burow Bd
- Bussey Pj
- Butterworth Jm
- Bylsma B
- CA ZEUS Collaboration
- Caldwell A
- Capua M
- Carlin Roberto
- Cartiglia N
- Cashmore Rj
- Castellini G
- Catterall Cd
- Chapin D
- Chekanov S
- Chwastowski J
- Ciborowski J
- Cifarelli L
- Cindolo F
- Cirio R
- Cloth P
- Coboken K
- Coldewey C
- Cole Je
- Contin A
- COOPER SARKAR Am
- Coppola N
- Cormack C
- Corradi M
- Corriveau F
- Costa M
- Cottingham Wn
- Crittenden J
- Cross R
- D'Agostini G
- Dagan S
- DAL CORSO F
- Dardo M
- DE PASQUALE S
- DE WOLF E
- Deffner R
- DEL PESO J
- Deppe O
- Derrick M
- Deshpande A
- Desler K
- Devenish Rce
- Dhawan S
- Dolgoshein Ba
- Dondana S
- Dosselli U
- Doyle At
- Drews G
- Dulinski Z
- Durkin Ls
- Dusini S
- Eckert M
- Edmonds Jk
- Eisenberg Y
- Eisenhardt S
- Engelen J
- Epperson D
- Ermolov Pf
- Eskreys A
- Fagerstroem Cp
- Fernandez Jp
- Ferrero Mi
- Figiel J
- Filges D
- Foster B
- Foudas C
- FOX MURPHY A
- Fricke U
- Frisken Wr
- Fusayasu T
- Gadaj T
- Galea R
- Gallo E
- Garcia G
- Garcia Yz
- Garfagnini Alberto
- Gendner N
- Gialas I
- Gilmore J
- Ginsburg Cm
- Giusti P
- Gladilin Lk
- Glasman C
- Goebel F
- Golubkov Ya
- Gottlicher P
- Grabosch Hj
- Graciani R
- GROSSE KNETTER J
- Grzelak G
- Haas T
- Hain W
- HALL WILTON R
- Hamatsu R
- Hanna Ds
- Harnew N
- Hart Jc
- Hartmann H
- Hartmann J
- Hartner Gf
- Hasell D
- Hayes Me
- Heapby Ea
- Heath Gp
- Heath Hf
- Hebbel K
- Heinloth K
- Heinz L
- Hernandez Jm
- Heusch C
- Hilger E
- Hirose T
- Hochman D
- Holm U
- Homma K
- Hong Sj
- Howell G
- Hughes Vw
- Iacobucci G
- Iannotti L
- Iga Y
- Inuzuka M
- Ishii T
- Jakob Hp
- Jelen K
- Jeoung Hy
- Jing Z
- Johnson Kf
- Jones Tw
- Kananov S
- Kappes A
- Karshon U
- Kasemann M
- Katz Uf
- Kcira D
- Kerger R
- Khakzad M
- Khein La
- Kim Cl
- Kim Jy
- Kisielewska D
- Kitamura S
- Klanner R
- Klimek K
- Koch W
- Koffeman E
- Kooijman P
- Koop T
- Korotkova Na
- Korzhavina Ia
- Kotanski A
- Kotz U
- Kowal Am
- Kowalski H
- Kowalski T
- Krakauer D
- Kreisel A
- Kuze M
- Kuzmin Va
- Labarga L
- Lamberti L
- Lane Jb
- Laurenti G
- Lee Jh
- Lee Sb
- Lee Sw
- Levi G
- Levman Gm
- Levy A
- Lim H
- Lim It
- Limentani S
- Lindemann L
- Ling Ty
- Liu W
- Lohr B
- Lohrmann E
- Long Kr
- Lukina Oy
- Ma Kj
- Maccarrone G
- Macdonald N
- Magill S
- Mallik U
- Margotti A
- Marini G
- Markun P
- Martin Jf
- Martinez M
- Maselli S
- Massam T
- Mastroberardino A
- Matsushita T
- Mattingly Mck
- Mattingly S
- Mccance Gj
- Mccubbin Na
- Mcfall Jd
- Mellado B
- Menary S
- MEYER LARSEN A
- Meyer A
- Milewski J
- Milite M
- Miller Db
- Monaco V
- Monig K
- Monteiro T
- Morandin M
- Moritz M
- Murray Wn
- Musgrave B
- Nagano K
- Nam Sw
- Nania R
- Nigro A
- Nishimura T
- Notz D
- Nowak Rj
- Noyes Va
- Nylander P
- Ochs A
- Oh By
- Okrasinski Jr
- Olkiewicz K
- Orr Rs
- Pac My
- Padhi S
- Palmonari F
- Park Ih
- Park Sk
- Parsons Ja
- Paul E
- Pavel N
- Pawlak Jm
- Pawlak R
- Pelfer P
- Pellegrino A
- Pelucchi F
- Peroni C
- Pesci A
- Petrucci Mc
- Pfeiffer M
- Piccioni D
- Piotrzkoswski K
- Poelz G
- Polenz S
- Polini A
- Posocco M
- Prinias A
- Proskuryakov As
- Przybycien M
- Przybycien Mb
- Puga J
- Quadt A
- Raach H
- Raso M
- Rautenberg J
- Redondo I
- Reeder Dd
- Repond J
- Ritz S
- Riveline M
- Rohde M
- Romeo Gc
- RULIKOWSKA ZAREBSKA E
- Ruske O
- Ruspa M
- Sabetfakhri A
- Sacchi R
- Sadrozinski Hfw
- Salehi H
- Sampson S
- Sartorelli G
- Saull Prb
- Savin Aa
- Saxon Dh
- Schechter A
- Schioppa M
- Schlenstedt S
- Schmidke Wb
- Schneekloth U
- Schnurbusch H
- Schwarzer O
- Sciulli F
- Scott J
- Sedgbeer Jk
- Seiden A
- Selonke F
- Shah Tp
- Shcheglova Lm
- Sideris D
- Sievers M
- Simmons D
- Sinclair Le
- Skillicorn Io
- Smalska B
- Smith Wh
- Solano A
- Solomin An
- Son D
- ST LAURENT M
- Staiano A
- Stairs Dg
- Stanco L
- Stanek R
- Stifutkin A
- Stonjek S
- Straub Pb
- Strickland E
- Stroili Roberto
- Susinno G
- Suszycki L
- Sutton Mr
- Suzuki I
- Tandler J
- Tapper Ad
- Tapper Rj
- Tassi E
- Terron J
- Tiecke W
- Tokushuku K
- Toothacker Ws
- Tsurugai T
- Tuning N
- Tymieniecka T
- Umemori K
- Vaiciulis A
- VAN SIGHEM A
- Velthuis Jj
- Verkerke W
- Viani Ald
- Voci C
- Vossebeld J
- Votano L
- Walczak R
- Walker R
- Wang Sm
- Waters Ds
- Waugh R
- Weber A
- Whitmore Jj
- Wichmann R
- Wick K
- Wieber H
- Wiggers L
- Wildschek T
- Williams Dc
- Wing M
- Wodarczyk M
- Wolf G
- Wolfle S
- Wollmer U
- Wroblewski Ak
- Yamada S
- Yamashita T
- Yamauchi K
- Yamazaki Y
- Yoshida R
- Youngman C
- Zajac J
- Zakrzewski Ja
- Zarnecki Af
- Zawiejski L
- Zetsche F
- Zeuner W
- Zhu Q
- Zichichi A
- Zotkin Sa
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/1999
- Field of study
Correlations between charged particles in deep inelastic ep scattering have
been studied in the Breit frame with the ZEUS detector at HERA using an
integrated luminosity of 6.4 pb-1. Short-range correlations are analysed in
terms of the angular separation between current-region particles within a cone
centred around the virtual photon axis. Long-range correlations between the
current and target regions have also been measured. The data support
predictions for the scaling behaviour of the angular correlations at high Q2
and for anti-correlations between the current and target regions over a large
range in Q2 and in the Bjorken scaling variable x. Analytic QCD calculations
and Monte Carlo models correctly describe the trends of the data at high Q2,
but show quantitative discrepancies. The data show differences between the
correlations in deep inelastic scattering and e+e- annihilation.Comment: 26 pages including 10 figures (submitted to Eur. J. Phys. C
Plastisol Foaming Process. Decomposition of the Foaming Agent, Polymer Behavior in the Corresponding Temperature Range and Resulting Foam Properties
- Author
- Abbiendi G
- Abe T
- Abramowicz H
- Acosta D
- Adamczyk L
- Adamus M
- Amelung C
- Anselmo F
- Antonioli P
- Arneodo M
- Ayad R
- Bacon TC
- Badgett WF
- Bailey DC
- Bailey DS
- Bamberger A
- Barbagli G
- Bari G
- Barreiro F
- Bashindzhagyan GL
- Bashkirov V
- Basile M
- Bauerdick LAT
- Bednarek B
- Behrens U
- Beier H
- Bellagamba L
- Bertolin A
- Bhadra S
- Bienlein JK
- Blaikley HE
- Bohnet I
- Bokel C
- Bornheim A
- Borzemski P
- Boscherini D
- Botje M
- Breitweg J
- Briskin G
- Brock I
- Bromley JT
- Brook NH
- Brugnera R
- Bruni A
- Bruni G
- BrĂźmmer N
- Bukowy M
- Bulmahn J
- Burow BD
- Bussey PJ
- Butterworth I
- Butterworth JM
- Bylsma B
- Caldwell A
- Campbell-Robson S
- Capua M
- Cara Romeo G
- Carlin R
- Cartiglia N
- Cases G
- Cashmore RJ
- Castellini G
- Catterall CD
- Chapin D
- Chlebana F
- Chwastowski J
- Ciborowski J
- Cifarelli L
- Cindolo F
- Cirio R
- Cloth P
- CobĂśken K
- Coldewey C
- Cole JE
- Contin A
- Cooper-Sarkar AM
- Corradi M
- Corriveau F
- Costa M
- Cottingham WN
- Crittenden J
- Cross R
- D'Agostini G
- Dagan S
- Dal Corso F
- Dardo M
- Dasu S
- de Pasquale S
- de TrocĂłniz JF
- de Wolf E
- Deffner R
- del Peso J
- Deppe O
- Derrick M
- Deshpande A
- Desler K
- Devenish RCE
- Dhawan S
- Dolgoshein BA
- Dosselli U
- Doyle AT
- Drews G
- DulinĹski Z
- Durkin LS
- Eckert M
- Edmonds JK
- Eisenberg Y
- Eisenhardt S
- Engelen J
- Epperson D
- Ermolov PF
- Eskreys A
- Fagerstroem C-P
- Feld L
- FernĂĄndez JP
- Ferrero MI
- Figiel J
- Filges D
- Fleck JI
- Foster B
- Foudas C
- Fricke U
- Frisken WR
- Fusayasu T
- Galea R
- Gallo E
- GarcĂa G
- Garfagnini A
- Gendner N
- Gialas I
- Gilkinson DJ
- Gilmore J
- Ginsburg CM
- Giusti P
- Gladilin LK
- Glasman C
- Golubkov YA
- Grabosch HJ
- Graciani R
- Grothe M
- GroĂe-Knetter J
- Grzelak G
- GĂśttlicher P
- Haas T
- Hain W
- Hall-Wilton R
- Hamatsu R
- Hanna DS
- Harnew N
- Hart JC
- Hartmann H
- Hartmann J
- Hartner GF
- Hasell D
- Hayes ME
- Heath GP
- Heath HF
- Heinloth K
- Heinz L
- HernĂĄndez JM
- HervĂĄs L
- Heusch C
- Hilger E
- Hirose T
- Hochman D
- Holm U
- Homma K
- Hong SJ
- Horstmann D
- Howell G
- Hughes VW
- Hung BHY
- Hung LW
- Iacobucci G
- Iannotti L
- Iga Y
- Inuzuka M
- Ishii T
- Jakob H-P
- JeleĹ K
- Jing Z
- Johnson KF
- Jones TW
- Joo KK
- Kananov S
- Karshon U
- Kasemann M
- Kasprzak M
- Katz UF
- Kerger R
- Khakzad M
- Khein LA
- Kim CL
- Kim JY
- Kisielewska D
- Kitamura S
- Klanner R
- Klimek K
- Koch W
- Koffeman E
- Kooijman P
- Korotkova NA
- Korzhavina IA
- KotanĹski A
- Kowalski H
- Kowalski T
- Krakauer D
- Kuze M
- Kuzmin VA
- Kçira D
- KĂśtz U
- Labarga L
- Labs J
- Lamberti L
- Lane JB
- Laurenti G
- Lee JH
- Lee SB
- Levi G
- Levman GM
- Levy A
- Lim IT
- Limentani S
- Lindemann L
- Ling TY
- Liu W
- Lohrmann E
- Long KR
- Loveless RJ
- Lukina OY
- LĂśhr B
- LĂśwe M
- Maccarrone G
- Macdonald N
- Magill S
- Mallik U
- Margotti A
- Marini G
- Markun P
- Martin JF
- MartĂnez M
- Maselli S
- Massam T
- Matsushita T
- Mattingly MCK
- Mattingly S
- MaĹczak O
- McCubbin NA
- McFall JD
- Mellado B
- Meyer A
- Meyer-Larsen A
- Mikunas D
- Milewski J
- Miller DB
- Monaco V
- Monteiro T
- Morandin M
- Muchorowski K
- Murray WN
- Musgrave B
- Nagano K
- Nam SW
- Nania R
- Nath C
- Ng JST
- Nigro A
- Notz D
- Nowak RJ
- Noyes VA
- Nylander P
- Ochs A
- Oh BY
- Ohrenberg K
- OkrasiĹski JR
- Orr RS
- Pac MY
- Palmonari F
- Park IH
- Park SK
- Parsons JA
- Paul E
- Pavel N
- Pawlak JM
- Pawlak R
- Pelfer P
- Pellegrino A
- Pelucchi F
- Peroni C
- Pesci A
- Petrucci MC
- Pfeiffer M
- Piccioni D
- Piotrzkowski K
- Poelz G
- Polenz S
- Polini A
- Posocco M
- Prinias A
- Proskuryakov AS
- PrzybycieĹ M
- PrzybycieĹ MB
- Puga J
- Quadt A
- Rahn JT
- Raso M
- Reeder DD
- Rembser C
- Repond J
- Ricci F
- Ritz S
- Riveline M
- Roco M
- Roff DG
- Rohde M
- RoldĹn J
- Romanowski TA
- Rulikowska-Zarebska E
- Ruske O
- Ruspa M
- Ryan JJ
- Sabetfakhri A
- Sacchi R
- Sadrozinski HF-W
- Salehi H
- Sampson S
- Sartorelli G
- Saunders RL
- Savin AA
- Saxon DH
- Schioppa M
- Schlenstedt S
- Schmidke WB
- Schneekloth U
- Schott W
- Schwarzer O
- Sciulli F
- Sedgbeer JK
- Seiden A
- Selonke F
- Shah TP
- Shcheglova LM
- Sideris D
- Simmons D
- Sinclair LE
- Smith WH
- Solano A
- Solomin AN
- St-Laurent M
- Staiano A
- Stairs DG
- Stamm J
- Stanco L
- Stanek R
- Stifutkin A
- Straub PB
- Strickland E
- Stroili R
- Surrow B
- Susinno G
- Suszycki L
- Sutton MR
- Suzuki I
- Talaga RL
- Tapper RJ
- Tassi E
- TerrĂłn J
- Teuscher RJ
- Tickner JR
- Tiecke H
- Tokushuku K
- Toothacker WS
- Trefzger T
- Tsurugai T
- Tuning N
- Tymieniecka T
- Uijterwaal H
- Ullmann R
- Umemori K
- Vaiciulis A
- van Sighem A
- Verkerke W
- Voci C
- Vossebeld J
- Votano L
- VoĂ T
- Vreeswijk M
- Walczak R
- Walenta AH
- Walker R
- Wang SM
- Waters DS
- Waugh R
- Wedemeyer R
- Westphal D
- Whitmore JJ
- Wichmann R
- Wick K
- Wieber H
- Wiggers L
- Williams DC
- Wing M
- Wodarczyk M
- Wolf G
- Wollmer U
- WrĹblewski AK
- Wu JT
- WĂślfle S
- Yamada S
- Yamashita T
- Yamauchi K
- Yamazaki Y
- Yoshida R
- Youngman C
- Zaja̧c J
- Zakrzewski JA
- Zamora Garcia Y
- Zarnecki AF
- Zawiejski L
- Zetsche F
- Zeuner W
- Zhang H
- Zhu Q
- Zichichi A
- Zotkin SA
- Publication venue
- WILEY
- Publication date
- 01/01/1998
- Field of study
The decomposition of azodicarbonamide, used as foaming agent in PVC - plasticizer (1/1) plastisols was studied by DSC. Nineteen different plasticizers, all belonging to the ester family, two being polymeric (polyadipates), were compared. The temperature of maximum decomposition rate (in anisothermal regime at 5 K min-1 scanning rate), ranges between 434 and 452 K. The heat of decomposition ranges between 8.7 and 12.5 J g -1. Some trends of variation of these parameters appear significant and are discussed in terms of solvent (matrix) and viscosity effects on the decomposition reactions. The shear modulus at 1 Hz frequency was determined at the temperature of maximum rate of foaming agent decomposition, and differs significantly from a sample to another. The foam density was determined at ambient temperature and the volume fraction of bubbles was used as criterion to judge the efficiency of the foaming process. The results reveal the existence of an optimal shear modulus of the order of 2 kPa that corresponds roughly to plasticizer molar masses of the order of 450 Âą 50 g mol-1. Heavier plasticizers, especially polymeric ones are too difficult to deform. Lighter plasticizers such as diethyl phthalate (DEP) deform too easily and presumably facilitate bubble collapse
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
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- Yilmaz Y
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- Yumiceva F
- Yun JC
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- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- Zang SL
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- Zatserklyaniy A
- Zeinali M
- Zeise M
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang Z
- Zheng Y
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- Zoeller MH
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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
- Acosta D
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- Acosta MV
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- Choi YK
- Chou JP
- Choudhary BC
- Choudhury RK
- Choudhury S
- Christiansen T
- Chuang SH
- Chung J
- Chung YS
- Chwalek T
- Ciesielski R
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- Cimmino A
- Cipriano PMR
- Cirino G
- Cittolin S
- Ciulli V
- Civinini C
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- 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
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
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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
- Zhang J
- Zhang Z
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- Zoeller MH
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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
X-ray emission from the Sombrero galaxy: discrete sources
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
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- Acosta MV
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- Brigljevic V
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- Butler PH
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- Caballero IG
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- Calderon A
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- Chang YH
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- Chang YW
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- Chao Y
- Charaf O
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- Chatterjee A
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- Cirino G
- Cittolin S
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- Civinini C
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- CMS Collaboration
- Cockerill DJA
- Codispoti G
- Colafranceschi S
- Colaleo A
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- Coughlan JA
- Cousins R
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- Cox PT
- Creanza D
- Cremaldi LM
- Cripps N
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cuplov V
- Cure B
- Cushman P
- Cussans D
- 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
- Da Silva WLP
- Dahmes B
- Dahms T
- Dallavalle GM
- Damgov J
- Damiao DD
- Dammann D
- Danielson T
- Darmenov N
- Das S
- Daskalakis G
- Dasu S
- Daubie E
- David A
- Davids M
- Davies G
- De Araujo FTD
- de Barbaro P
- De Benedetti A
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- de Cassagnac RG
- De Cosa A
- de Fatis TT
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- De Guio F
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- De La Cruz B
- De Lentdecker G
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- de Monchenault GH
- De Palma M
- De Roeck A
- De Souza SF
- de Troconiz JF
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- Debreczeni G
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2010
- Field of study
We present a study of discrete X-ray sources in and around the
bulge-dominated, massive Sa galaxy, Sombrero (M104), based on new and archival
Chandra observations with a total exposure of ~200 ks. With a detection limit
of L_X = 1E37 erg/s and a field of view covering a galactocentric radius of ~30
kpc (11.5 arcminute), 383 sources are detected. Cross-correlation with Spitler
et al.'s catalogue of Sombrero globular clusters (GCs) identified from HST/ACS
observations reveals 41 X-rays sources in GCs, presumably low-mass X-ray
binaries (LMXBs). We quantify the differential luminosity functions (LFs) for
both the detected GC and field LMXBs, whose power-low indices (~1.1 for the
GC-LF and ~1.6 for field-LF) are consistent with previous studies for
elliptical galaxies. With precise sky positions of the GCs without a detected
X-ray source, we further quantify, through a fluctuation analysis, the GC LF at
fainter luminosities down to 1E35 erg/s. The derived index rules out a
faint-end slope flatter than 1.1 at a 2 sigma significance, contrary to recent
findings in several elliptical galaxies and the bulge of M31. On the other
hand, the 2-6 keV unresolved emission places a tight constraint on the field
LF, implying a flattened index of ~1.0 below 1E37 erg/s. We also detect 101
sources in the halo of Sombrero. The presence of these sources cannot be
interpreted as galactic LMXBs whose spatial distribution empirically follows
the starlight. Their number is also higher than the expected number of cosmic
AGNs (52+/-11 [1 sigma]) whose surface density is constrained by deep X-ray
surveys. We suggest that either the cosmic X-ray background is unusually high
in the direction of Sombrero, or a distinct population of X-ray sources is
present in the halo of Sombrero.Comment: 11 figures, 5 tables, ApJ in pres
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
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- 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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- Wyslouch B
- Xiao H
- Xie S
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- Yalvac M
- Yang F
- Yang M
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- 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
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- CMS Collaboration
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- Dabrowski A
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- 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
- 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
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
- Albrow M
- Alcaraz Maestre J
- Alda Junior WL
- Alderweireldt S
- Alexander J
- Aliev T
- Alimena J
- Almeida N
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Andrea J
- Andreev V
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- Andreev Y
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- Antonelli L
- Antunovic Z
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- Appelt E
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- Civinini C
- Claes DR
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- Clarida W
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- Cline D
- CMS Collaboration
- Coarasa Perez JA
- Cockerill DJA
- Colafranceschi S
- Colaleo A
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- Cutajar M
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- D'Alessandro R
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- Da Costa EM
- Dabrowski A
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- Dallavalle GM
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- Daubie E
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- de Cassagnac RG
- De Cosa 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
Performance of the CMS Cathode Strip Chambers with Cosmic Rays
- Author
- Abadjiev K
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abelev B
- Acosta D
- Acosta JG
- Acosta MV
- Actis O
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- Ahmed W
- Ahuja S
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- Altsybeev I
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- Wurthwein F
- Wynne B. M.
- Wyslouch B
- Xaplanteris L.
- Xella S.
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- Xie Z
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- Yagil A
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- Yi K
- Yilmaz Y
- Yohay R
- Yoo HD
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- Yumiceva F
- Yun JC
- Yuste C
- Zabi A
- Zabolotny W
- Zachariadou A
- Zalewski P
- Zampieri A
- Zanetti M
- Zang SL
- Zarubin A
- Zatzerklyany A
- Zeidler C
- Zeinali M
- Zeise M
- Zelepoukine S
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang L
- Zhang Y
- Zhang Z
- Zheng Y
- Zhiltsov V
- Zhokin A
- Zhu B
- Zhu K
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Zielinski M
- Zilizi G
- Zinonos Z
- Zito G
- Zoeller MH
- Zotto P
- Zub S
- Zumerle G
- Zuranski A
- Zuyeuski R
- Zych P
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2009
- Field of study
The Cathode Strip Chambers (CSCs) constitute the primary muon tracking device
in the CMS endcaps. Their performance has been evaluated using data taken
during a cosmic ray run in fall 2008. Measured noise levels are low, with the
number of noisy channels well below 1%. Coordinate resolution was measured for
all types of chambers, and fall in the range 47 microns to 243 microns. The
efficiencies for local charged track triggers, for hit and for segments
reconstruction were measured, and are above 99%. The timing resolution per
layer is approximately 5 ns
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
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- 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
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