2,149 research outputs found
Spontaneously occurring melanoma in animals and their relevance to human melanoma
- Author
- Publication venue
- 'Wiley'
- Publication date
- 01/09/2020
- Field of study
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
- BrĂŒmmer 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
- Coböken 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
- DulinĆski 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
- Göttlicher 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
- JeleĆ 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
- KotanĆski A
- Kowalski H
- Kowalski T
- Krakauer D
- Kuze M
- Kuzmin VA
- Kçira D
- Kötz 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
- Löhr B
- Löwe 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
- MaĆczak 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
- OkrasiĆski 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
- PrzybycieĆ M
- PrzybycieĆ 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
- RoldĆn 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
- WrĆblewski AK
- Wu JT
- Wölfle 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 ± 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
Search for rare quark-annihilation decays, B --> Ds(*) Phi
- Author
- Abe T
- Abrams GS
- Adye T
- Ahmed M
- Ahmed S
- Alam MS
- Albert J
- Aleksan R
- Allen MT
- Allison J
- Allmendinger T
- Altenburg D
- Andreassen R
- Andreotti M
- Angelini C
- Anulli F
- Arnaud N
- Aston D
- Aubert B
- Azzolini V
- Baak M
- Back JJ
- Baldini-Ferroli R
- Band HR
- Banerjee S
- Barate R
- Bard DJ
- Barlow NR
- Barlow RJ
- Barrett M
- Bartoldus R
- Batignani G
- Battaglia M
- Bauer JM
- Beck TW
- Behera PK
- Bellini F
- Benayoun M
- Benelli G
- Berger N
- Bernard D
- Berryhill JW
- Best D
- Bettarini S
- Bettoni D
- Bevan AJ
- Bhimji W
- Bhuyan B
- Bianchi F
- Biasini M
- Biesiada J
- Blanc F
- Blaylock G
- Blinov AE
- Blinov VE
- Bloom PC
- Blount NL
- Bomben M
- Bona M
- Bondioli M
- Bonneaud GR
- Bosisio L
- Boutigny D
- Bowerman DA
- Boyarski AM
- Boyd JT
- Bozzi C
- Brandenburg G
- Brandt T
- Brau J
- Breon AB
- Brose J
- Brown CL
- Brown CM
- Brown DN
- Brown DN
- Bruinsma M
- Brunet S
- Bucci F
- Buchanan C
- Buchmueller OL
- Bugg W
- Bukin AD
- Bula R
- Bulten H
- Buono LD
- Burchat PR
- Burke JP
- Button-Shafer J
- Buzzo A
- Cahn RN
- Calabrese R
- Calcaterra A
- Calderini G
- Campagnari C
- Capra R
- Carpinelli M
- Cartaro C
- Cavallo N
- Cavoto G
- Cenci R
- Chai X
- Chaisanguanthum KS
- Chao M
- Charles E
- Charles MJ
- Chauveau J
- Chavez CA
- Chen A
- Chen C
- Chen E
- Chen JC
- Chen S
- Chen X
- Cheng B
- Cheng CH
- Chia YM
- Cibinetto G
- Clark PJ
- Claus R
- Cochran J
- Coleman JP
- Collaboration BABAR
- Contri R
- Convery MR
- Cossutti F
- Cote D
- Cottingham WN
- Couderc F
- Covarelli R
- Cowan G
- Cowan R
- Crawley HB
- Cremaldi L
- Cristinziani M
- Cuhadar-Donszelmann T
- Cunha A
- Curry S
- D'Orazio A
- Dahmes B
- Dallapiccola C
- Danielson N
- Dasu S
- Datta M
- Dauncey PD
- David P
- Davier M
- Davis CL
- Day CT
- de la Vaissiere C
- de Monchenault GH
- de Sangro R
- del Re D
- Diberder FL
- Dickopp M
- Dingfelder JC
- Dittongo S
- Dong D
- Dong L
- Dorfan J
- Druzhinin VP
- Dubitzky RS
- Dubois-Felsmann GP
- Dujmic D
- Dunwoodie W
- Dvoretskii A
- Eckhart EA
- Eckmann R
- Edgar CL
- Edwards AJ
- Egede U
- Eichenbaum AM
- Eigen G
- Eisner AM
- Elmer P
- Emery S
- Ernst JA
- Eschenburg V
- Eschrich I
- Eyges V
- Fabozzi F
- Faccini R
- Fan S
- Feltresi E
- Ferrarotto F
- Ferroni F
- Field RC
- Finocchiaro G
- Flacco CJ
- Flack RL
- Flaecher HU
- Flood KT
- Ford KE
- Ford WT
- Forster IJ
- Forti F
- Fortin D
- Foulkes SD
- Franek B
- Frey R
- Fritsch M
- Fry JR
- Fulsom BG
- Gabathuler E
- Gaidot A
- Gaillard JR
- Galeazzi F
- Gallo F
- Gamba D
- Gamet R
- Gan KK
- Ganzhur SF
- Gary JW
- Gaspero M
- Gatto C
- George KA
- Gill MS
- Gioi LL
- Giorgi MA
- Giroux X
- Gladney L
- Glanzman T
- Godang R
- Goetzen K
- Golubev VB
- Gopal GP
- Gowdy SJ
- Gradl W
- Graham MT
- Grancagnolo S
- Grauges E
- Graziani G
- Green MG
- Grenier P
- Gritsan AV
- Groot ND
- Grosdidier G
- Groysman Y
- Guo QH
- Hadavand HK
- Hadig T
- Haire M
- Halyo V
- Hamano K
- Hamon O
- Harrison PF
- Harrison TJ
- Hart AJ
- Hartfiel BL
- Hast C
- Hauke A
- Hawkes CM
- Hearty C
- Held T
- Hertzbach SS
- Heusch CA
- Hill EJ
- Hirschauer JF
- Hitlin DG
- Hocker A
- Hodgkinson MC
- Hollar JJ
- Hong TM
- Honscheid K
- Hopkins DA
- Hryn'ova T
- Hufnagel D
- Hulsbergen WD
- Hutchcroft DE
- Igonkina O
- Innes WR
- Izen JM
- Jackson PD
- Jackson PS
- Jacobsen RG
- Jawahery A
- Jessop CP
- John MJJ
- Johnson JR
- Judd D
- Kadel RW
- Kadyk J
- Kagan H
- Karyotakis Y
- Kass R
- Kelly MP
- Kelsey MH
- Kerth LT
- Khan A
- Kim H
- Kim P
- Kirkby D
- Kitayama I
- Klose V
- Knecht NS
- Koch H
- Kocian ML
- Koeneke K
- Kofler R
- Kolomensky YG
- Kovalskyi D
- Kowalewski R
- Kozanecki W
- Kravchenko EA
- Kreisel A
- Krishnamurthy M
- Kroeger R
- Kroseberg J
- Kukartsev G
- Kutter PE
- Kyberd P
- Lacker HM
- Lae CK
- Lafferty GD
- Lanceri L
- Lange DJ
- Langenegger U
- Lankford AJ
- Latham TE
- Latour E
- Lau YP
- Lazzaro A
- Lees JP
- Legendre M
- Leith DWGS
- Lepeltier V
- Leruste P
- Lewandowski B
- Li H
- Li X
- Libby J
- Lista L
- Liu R
- Lockman WS
- Lodovico FD
- Lombardo V
- London GW
- Long O
- LoSecco JM
- Lou XC
- Lu C
- Lu M
- Luitz S
- Lund P
- Luppi E
- Lusiani A
- Luth V
- Lutz AM
- Lynch G
- Lynch HL
- MacFarlane DB
- Macri MM
- Mader WF
- Majewski SA
- Malcles J
- Mallik U
- Mancinelli G
- Mandelkern M
- Marchiori G
- Marco ED
- Margoni M
- Marks J
- Marsiske H
- Martinez-Vidal F
- Mattison TS
- Mayer B
- Mazur MA
- Mazzoni MA
- McKenna JA
- McMahon TR
- Meadows BT
- Mellado B
- Menges W
- Messner R
- Meyer WT
- Mihalyi A
- Minamora JS
- Mir LM
- Mohanty GB
- Mohapatra AK
- Mommsen RK
- Monge MR
- Monorchio D
- Moore TB
- Morandin M
- Morgan SE
- Morganti M
- Morganti S
- Morii M
- Muheim F
- Muller DR
- Naisbit MT
- Nardo GD
- Narsky I
- Nash JA
- Nauenberg U
- Neal H
- Negrini M
- Neri N
- Nesom G
- Nicholson H
- Nikolich MB
- Nogowski R
- Nugent IM
- O'Grady CP
- Ocariz J
- Oddone PJ
- Ofte I
- Olaiya EO
- Olivas A
- Olsen J
- Onuchin AP
- Orimoto TJ
- Otto S
- Oyanguren A
- Ozcan VE
- Paar HP
- Pacetti S
- Palano A
- Palombo F
- Pan Y
- Panetta J
- Panvini RS
- Paoloni E
- Paolucci P
- Pappagallo M
- Parry RJ
- Passaggio S
- Patel PM
- Patrignani C
- Patteri P
- Payne DJ
- Pelizaeus M
- Perazzo A
- Perl M
- Peruzzi IM
- Peters K
- Petersen BA
- Petersen TC
- Petzold A
- Piatenko T
- Piccolo D
- Piccolo M
- Piemontese L
- Pierini M
- Pioppi M
- Piredda G
- Plaszczynski S
- Playfer S
- Poireau V
- Polci F
- Pompili A
- Porter FC
- Posocco M
- Potter CT
- Prell S
- Prepost R
- Pripstein M
- Pulliam T
- Purohit MV
- Qi ND
- Rahatlou S
- Rahimi AM
- Rahmat R
- Rama M
- Ratcliff BN
- Raven G
- Reidy J
- Ricca GD
- Ricciardi S
- Richman JD
- Ritchie JL
- Rizzo G
- Roat C
- Roberts DA
- Robertson SH
- Robutti E
- Rodier S
- Roe NA
- Roethel W
- Ronan MT
- Roney JM
- Rong G
- Roodman A
- Roos L
- Rosenberg EI
- Rotondo M
- Roudeau P
- Rubin AE
- Ruddick WO
- Ryd A
- Sacco R
- Saeed MA
- Saleem M
- Salnikov AA
- Salvatore F
- Samuel A
- Sanders DA
- Santroni A
- Saremi S
- Satpathy A
- Schalk T
- Schenk S
- Schindler RH
- Schofield KC
- Schott G
- Schrenk S
- Schroder H
- Schroeder T
- Schubert J
- Schubert KR
- Schumm BA
- Schune MH
- Schwiening J
- Schwierz R
- Schwitters RF
- Sciacca C
- Sciolla G
- Seiden A
- Sekula SJ
- Serednyakov SI
- Sharma V
- Shen BC
- Simi G
- Simonetto F
- Sinev NB
- Skovpen YI
- Smith AJS
- Smith JG
- Snoek HL
- Snyder A
- Sobie RJ
- Soffer A
- Sokoloff MD
- Solodov EP
- Spaan B
- Spanier SM
- Spitznagel M
- Spradlin P
- Staengle H
- Steinke M
- Stelzer J
- Stocchi A
- Stoker DP
- Stroili R
- Strom D
- Strube J
- Stugu B
- Su D
- Sullivan MK
- Summers DJ
- Sundermann JE
- Suzuki K
- Swain SK
- Tan P
- Taras P
- Taylor F
- Tehrani FS
- Telnov AV
- Teodorescu L
- Ter-Antonyan R
- Therin G
- Thiebaux C
- Thompson JM
- Tisserand V
- Toki WH
- Torrence E
- Tosi S
- Touramanis C
- Ulmer KA
- Uwer U
- Va'vra J
- van Bakel N
- Vasileiadis G
- Vasseur G
- Vazquez WP
- Verderi M
- Verkerke W
- Vetere ML
- Viaud FB
- Vitale L
- Voci C
- Voena C
- Wagner SR
- Wagoner DE
- Waldi R
- Walsh J
- Wang K
- Wang P
- Wang WF
- Wappler FR
- Watson AT
- Weaver M
- Weidemann AW
- Weinstein AJR
- Wenzel WA
- Wilden L
- Williams DC
- Williams JC
- Willocq SY
- Wilson FF
- Wilson JR
- Wilson MG
- Wilson RJ
- Winklmeier F
- Wisniewski WJ
- Wittgen M
- Wong QK
- Wormser G
- Wright DH
- Wright DM
- Wu J
- Wu SL
- Xie Y
- Yamamoto RK
- Yarritu AK
- Ye S
- Yeche C
- Yi JI
- Yi K
- Young CC
- Yu Z
- Yushkov AN
- Zain SB
- Zallo A
- Zeng Q
- Zghiche A
- Zhang J
- Zhang L
- Zhao HW
- Zhu YS
- Ziegler V
- Zito M
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 12/12/2005
- Field of study
We report on searches for B- --> Ds- Phi and B- --> Ds*- Phi. In the context
of the Standard Model, these decays are expected to be highly suppressed since
they proceed through annihilation of the b and u-bar quarks in the B- meson.
Our results are based on 234 million Upsilon(4S) --> B Bbar decays collected
with the BABAR detector at SLAC. We find no evidence for these decays, and we
set Bayesian 90% confidence level upper limits on the branching fractions BF(B-
--> Ds- Phi) Ds*- Phi)<1.2x10^(-5). These results
are consistent with Standard Model expectations.Comment: 8 pages, 3 postscript figues, submitted to Phys. Rev. D (Rapid
Communications
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
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- Wood JS
- Worm SD
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- Wyslouch B
- Xiao H
- Xie S
- Xu M
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- 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
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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
X-ray emission from the Sombrero galaxy: discrete sources
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Acosta D
- Acosta JG
- Acosta MV
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Agostino L
- Agram JL
- Aguilar-Benitez M
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- Ahmad M
- Ahmad WH
- Ahmed I
- Ahuja S
- Akchurin N
- Akgun B
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- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
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- Alexander J
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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
- Antonelli L
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
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- Baarmand MM
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- Bauerdick LAT
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- Bedoya CF
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- Zumerle 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
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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- Ciesielski R
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- Cipriano PMR
- Cirino G
- Cittolin S
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- Civinini C
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- CMS Collaboration
- Cockerill DJA
- Codispoti G
- Colafranceschi S
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- Costantini S
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- Cutajar M
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- D'Agnolo RT
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- Yilmaz Y
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- Yun JC
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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
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
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- Agostino L
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- Capiluppi P
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- Chang YW
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- Christiansen T
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- Ciulli V
- Civinini C
- Claes DR
- Clare R
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- Clement E
- Clerbaux B
- Cline D
- CMS Collaboration
- Coarasa Perez JA
- Cockerill DJA
- Codispoti G
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- Cooper SI
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- Correa Martins Junior M
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- Costantini S
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- Coughlan JA
- Cousins R
- Covarelli R
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- Cox PT
- Creanza D
- Cremaldi LM
- Cripps N
- Cuevas J
- Cuffiani M
- Cumalat JP
- Cuplov V
- Cushman P
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- Custodio A
- Cutajar M
- Cutts D
- Cwiok M
- Czellar S
- D'Agnolo RT
- D'Alessandro R
- D'Alfonso M
- D'Enterria D
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- Da Costa EM
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- Dahms T
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- Damgov J
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- De La Cruz B
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- de Monchenault GH
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- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
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- Zarubin A
- Zatserklyaniy A
- Zeinali M
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- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
The azimuthal anisotropy of charged particles in PbPb collisions at
nucleon-nucleon center-of-mass energy of 2.76 TeV is measured with the CMS
detector at the LHC over an extended transverse momentum (pt) range up to
approximately 60 GeV. The data cover both the low-pt region associated with
hydrodynamic flow phenomena and the high-pt region where the anisotropies may
reflect the path-length dependence of parton energy loss in the created medium.
The anisotropy parameter (v2) of the particles is extracted by correlating
charged tracks with respect to the event-plane reconstructed by using the
energy deposited in forward-angle calorimeters. For the six bins of collision
centrality studied, spanning the range of 0-60% most-central events, the
observed v2 values are found to first increase with pt, reaching a maximum
around pt = 3 GeV, and then to gradually decrease to almost zero, with the
decline persisting up to at least pt = 40 GeV over the full centrality range
measured.Comment: Replaced with published version. Added journal reference and DO
Search for new physics with same-sign isolated dilepton events with jets and missing transverse energy
- Author
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- Abbiendi G
- Abbrescia M
- Abdullin S
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- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
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- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
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- Zielinski M
- Zito G
- Zou W
- Zucchetta A
- Zumerle G
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
A search for new physics is performed in events with two same-sign isolated
leptons, hadronic jets, and missing transverse energy in the final state. The
analysis is based on a data sample corresponding to an integrated luminosity of
4.98 inverse femtobarns produced in pp collisions at a center-of-mass energy of
7 TeV collected by the CMS experiment at the LHC. This constitutes a factor of
140 increase in integrated luminosity over previously published results. The
observed yields agree with the standard model predictions and thus no evidence
for new physics is found. The observations are used to set upper limits on
possible new physics contributions and to constrain supersymmetric models. To
facilitate the interpretation of the data in a broader range of new physics
scenarios, information on the event selection, detector response, and
efficiencies is provided.Comment: Published in Physical Review Letter
Compressed representation of a partially defined integer function over multiple arguments
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdelalim AA
- Abdullin S
- Abdulsalam A
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- Zhokin A
- Zhu RY
- Zhukov V
- Zhukova V
- Zielinski M
- Zito G
- Zotto P
- Zou W
- Zsigmond AJ
- Zucchetta A
- Zumerle G
- Zuranski A
- 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
Observation of associated near-side and away-side long-range correlations in âsNN=5.02ââTeV proton-lead collisions with the ATLAS detector
- Author
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- Yamanaka T
- Yamauchi K
- Yamazaki T
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- Yilmaz M
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- Yorita K
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- Youssef S
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- Yurkewicz A
- Zabinski B
- Zaidan R
- Zaitsev AM
- Zambito S
- Zanello L
- Zanzi D
- Zaytsev A
- Zeitnitz C
- Zeman M
- Zemla A
- Zenin O
- ZeniĆĄ T
- Zerwas D
- Zevi Della Porta G
- Zhang D
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- Zhemchugov A
- Zhong J
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- Zhuang X
- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
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- Zobernig G
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- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2012
- Field of study
Two-particle correlations in relative azimuthal angle (ÎÏ) and pseudorapidity (Îη) are measured in âsNN=5.02ââTeV p+Pb collisions using the ATLAS detector at the LHC. The measurements are performed using approximately 1ââÎŒb-1 of data as a function of transverse momentum (pT) and the transverse energy (ÎŁETPb) summed over 3.1<η<4.9 in the direction of the Pb beam. The correlation function, constructed from charged particles, exhibits a long-range (2<|Îη|<5) ânear-sideâ (ÎÏâŒ0) correlation that grows rapidly with increasing ÎŁETPb. A long-range âaway-sideâ (ÎÏâŒÏ) correlation, obtained by subtracting the expected contributions from recoiling dijets and other sources estimated using events with small ÎŁETPb, is found to match the near-side correlation in magnitude, shape (in Îη and ÎÏ) and ÎŁETPb dependence. The resultant ÎÏ correlation is approximately symmetric about Ï/2, and is consistent with a dominant cosâĄ2ÎÏ modulation for all ÎŁETPb ranges and particle pT
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