5,601 research outputs found
Complex patterns of local adaptation in teosinte
- Author
- Barthakur
- Beaumont
- Beaumont
- Bomblies
- Bradburd
- Bradbury
- Buckler
- Chalker-Scott
- Charlesworth
- Cheng
- Chia
- Clausen
- Cook
- Coop
- Cutter
- De
- Dobzhansky
- Doebley
- Doyle
- Earl
- Eckert
- Eckert
- Endler
- Etges
- Excoffier
- Excoffier
- Falush
- Fang
- Feder
- Flint-Garcia
- Foll
- Ford
- Fournier-Level
- Fukunaga
- Fumagalli
- Galinat
- Ganal
- Gerke
- Gore
- Goudet
- Grant
- Green
- Gregory
- Gusev
- Hancock
- Hancock
- Hijmans
- Hufford
- Hufford
- Hufford
- Hufford
- Hung
- Huynh
- Iltis
- Jackson
- Jeffrey Ross-Ibarra
- Kato
- Kato
- Keller
- Kirkpatrick
- Kirkpatrick
- Lauter
- Le Corre
- Lewontin
- Li
- Loveless
- Lowry
- Lowry
- Mano
- Mathieson
- Matthew B. Hufford
- Medina
- Meyerowitz
- Moeller
- Moeller
- Oksanen
- Olsson
- Patterson
- Platt
- Poggio
- R Core Team
- Rosenberg
- Ross-Ibarra
- Saghai-Maroof
- Salvi
- Sanchez
- Scheet
- Schnable
- Sheldon
- Siol
- Smith
- Smith
- Sofiane Mezmouk
- St. Onge
- Storz
- Studer
- Städler
- Tanja Pyhäjärvi
- Ting
- Toomajian
- Turner
- Turner
- van Heerwaarden
- van Heerwaarden
- Wang
- Weber
- Weber
- Weir
- Wilkes
- Wolfgruber
- Wright
- Yang
- Publication venue
- 'Oxford University Press (OUP)'
- Publication date
- 02/08/2012
- Field of study
Populations of widely distributed species often encounter and adapt to
specific environmental conditions. However, comprehensive characterization of
the genetic basis of adaptation is demanding, requiring genome-wide genotype
data, multiple sampled populations, and a good understanding of population
structure. We have used environmental and high-density genotype data to
describe the genetic basis of local adaptation in 21 populations of teosinte,
the wild ancestor of maize. We found that altitude, dispersal events and
admixture among subspecies formed a complex hierarchical genetic structure
within teosinte. Patterns of linkage disequilibrium revealed four mega-base
scale inversions that segregated among populations and had altitudinal clines.
Based on patterns of differentiation and correlation with environmental
variation, inversions and nongenic regions play an important role in local
adaptation of teosinte. Further, we note that strongly differentiated
individual populations can bias the identification of adaptive loci. The role
of inversions in local adaptation has been predicted by theory and requires
attention as genome-wide data become available for additional plant species.
These results also suggest a potentially important role for noncoding
variation, especially in large plant genomes in which the gene space represents
a fraction of the entire genome
The effect of arm training on thermoregulatory responses and calf volume during upper body exercise
- Author
- AM Nevil
- B Dawson
- B Saltin
- BA Stamford
- CW Ho
- D Theisen
- D Theisen
- D Theisen
- DB Dill
- DJ Loveless
- DR Seals
- F Yamazaki
- G Ahlborg
- G Havenith
- G Tew
- H Wakabayashi
- JA Stolwijk
- JM Johnson
- JM Johnson
- JO Holloszy
- JR Magel
- JVGA Durnin
- LB Rowell
- LB Rowell
- LE Armstrong
- LH Aulick
- Lindsay Bottoms
- M Loftin
- M Saito
- Michael Price
- MJ Price
- MT Hopman
- N Gant
- O Bar-Or
- PA Pilardeau
- PC Fehling
- PE Gates
- RA Mostardi
- S Volianitis
- Y Boegli
- YN Bhambhani
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2014
- Field of study
The final publication is available at Springer via https://doi.org/10.1007/s00421-014-2842-9.PURPOSE: The smaller muscle mass of the upper body compared to the lower body may elicit a smaller thermoregulatory stimulus during exercise and thus produce novel training-induced thermoregulatory adaptations. Therefore, the principal aim of the study was to examine the effect of arm training on thermoregulatory responses during submaximal exercise. METHODS: Thirteen healthy male participants (Mean ± SD age 27.8 ± 5.0 years, body mass 74.8 ± 9.5 kg) took part in 8 weeks of arm crank ergometry training. Thermoregulatory and calf blood flow responses were measured during 30 min of arm cranking at 60% peak power (W peak) pre-, and post-training and post-training at the same absolute intensity as pre-training. Core temperature and skin temperatures were measured, along with heat flow at the calf, thigh, upper arm and chest. Calf blood flow using venous occlusion plethysmography was performed pre- and post-exercise and calf volume was determined during exercise. RESULTS: The upper body training reduced aural temperature (0.1 ± 0.3 °C) and heat storage (0.3 ± 0.2 J g(-1)) at a given power output as a result of increased whole body sweating and heat flow. Arm crank training produced a smaller change in calf volume post-training at the same absolute exercise intensity (-1.2 ± 0.8% compared to -2.2 ± 0.9% pre-training; P < 0.05) suggesting reduced leg vasoconstriction. CONCLUSION: Training improved the main markers of aerobic fitness. However, the results of this study suggest arm crank training additionally elicits physiological responses specific to the lower body which may aid thermoregulation.Peer reviewedFinal Accepted Versio
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
- Brümmer 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 Trocóniz 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
- Dulinński Z
- Durkin LS
- Eckert M
- Edmonds JK
- Eisenberg Y
- Eisenhardt S
- Engelen J
- Epperson D
- Ermolov PF
- Eskreys A
- Fagerstroem C-P
- Feld L
- Fernández JP
- Ferrero MI
- Figiel J
- Filges D
- Fleck JI
- Foster B
- Foudas C
- Fricke U
- Frisken WR
- Fusayasu T
- Galea R
- Gallo E
- García 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
- Große-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
- Hernández JM
- Hervás 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
- Jeleń 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
- Kotanński 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
- Martínez M
- Maselli S
- Massam T
- Matsushita T
- Mattingly MCK
- Mattingly S
- Mańczak 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
- Okrasiński 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
- Przybycień M
- Przybycień 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
- Roldńn 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
- Terrón 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
- Voß 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
- Wrńblewski 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
Recommended from our members
A Search for Dark Higgs Bosons
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- Acosta JG
- Adam N
- Adametz A.
- Adye T.
- Ahmed H.
- Akar S.
- Akchurin N
- Alagoz E
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- Albert J.
- Alver B
- Alverson G
- Anastassov A
- Anderson M
- Andreassen R.
- Angelini C.
- Antonelli L
- Anulli F.
- Appelt E
- Arenton MW
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- Asgeirsson D. J.
- Aston D.
- Atmacan H.
- Atramentov O
- Ayad R.
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- Banerjee Sw
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- Barker A
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- Bartoldus R.
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- Baumgartel D
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- Bean A
- Behera P. K.
- Behn E.
- Bellinger JN
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- Bendavid J
- Benelli G
- Benitez J. F.
- Bernard D.
- Bernlochner F. U.
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- Wulsin H. W.
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- Ziegler J
- Ziegler V.
- Zielinski M
- Zuranski A
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2012
- Field of study
Recent astrophysical and terrestrial experiments have motivated the proposal
of a dark sector with GeV-scale gauge boson force carriers and new Higgs
bosons. We present a search for a dark Higgs boson using 516 fb-1 of data
collected with the BABAR detector. We do not observe a significant signal and
we set 90% confidence level upper limits on the product of the Standard
Model-dark sector mixing angle and the dark sector coupling constant.Comment: 7 pages, 5 postscript figures, published version with improved plots
for b/w printin
Performance of CMS muon reconstruction in pp collision events at sqrt(s) = 7 TeV
- Author
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- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
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- Yu I
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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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- 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
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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- 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
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
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahmed I
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
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- Allfrey P
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- 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
- Antunes JR
- Antunovic Z
- Apanasevich L
- Apollinari G
- Appelt E
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- Arenton MW
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- Brigljevic V
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- Brona G
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- Castaldi R
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- Chan M
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- Chang YH
- Chang YH
- Chang YW
- Chanon N
- Chao Y
- Charaf O
- Charlot C
- Chasco M
- Chatterjee A
- Chauhan S
- Checchia P
- Chen GM
- Chen HS
- Chen J
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- Chen KH
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- Chertok M
- Chetluru V
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- Cifuentes JAB
- Cihangir S
- Cimmino A
- 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
- Cole P
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- Collard C
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- Conetti S
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- Cooper SI
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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
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- Daskalakis G
- Dasu S
- Daubie E
- David A
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- de Barbaro P
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- de Cassagnac RG
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- de Fatis TT
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- De Gruttola M
- De Guio F
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- De La Cruz B
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- de Monchenault GH
- De Palma M
- De Roeck A
- De Souza SF
- de Troconiz JF
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- Di Marco E
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- Dimitrov A
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- Drouhin F
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- Etesami SM
- Eugster J
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- Evangelou I
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- Wood JS
- Worm SD
- Wright D
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- Wulz CE
- Wurthwein F
- Wyslouch B
- Xiao H
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- Yetkin T
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- Yilmaz Y
- Yohay R
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- Yoon AS
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- Yu I
- Yu SS
- Yumiceva F
- Yun JC
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- 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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- Zhang Z
- Zheng Y
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- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Ziegler J
- Zielinski M
- Zito G
- Zoeller MH
- Zorbilmez C
- Zotto P
- Zou W
- Zumerle G
- Zuranski A
- 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
Search for the standard model Higgs boson in the H to ZZ to 2l 2nu channel in pp collisions at sqrt(s) = 7 TeV
- Author
- A Bredenstein
- A Bredenstein
- A Djouadi
- A Djouadi
- A Martin
- A. A. Ocampo Rios
- A. Adair
- A. Adiguzel
- A. Anastassov
- A. Apresyan
- A. Aranyi
- A. Askew
- A. Attikis
- A. Avetisyan
- A. B. Meyer
- A. Baden
- A. Barker
- A. Bean
- A. Belyaev
- A. Belyaev
- A. Benaglia
- A. Beretvas
- A. Bethani
- A. Bhatti
- A. Biselli
- A. Bocci
- A. Bodek
- A. Bonato
- A. Bornheim
- A. Branca
- A. Brinkerhoff
- A. Burgmeier
- A. C. Benvenuti
- A. C. Mignerey
- A. Cabrera
- A. Cakir
- A. Calderon
- A. Campbell
- A. Castro
- A. Chatterjee
- A. Cimmino
- A. Colaleo
- A. Custódio
- A. David
- A. De Benedetti
- A. De Cosa
- A. De Roeck
- A. Deisher
- A. Delgado Peris
- A. Dermenev
- A. Dierlamm
- A. Dimitrov
- A. Dominguez
- A. Drozdetskiy
- A. Elliott-Peisert
- A. Ellithi Kamel
- A. Ershov
- A. Everett
- A. F. Barfuss
- A. F. Osorio Oliveros
- A. Fahim
- A. Falkiewicz
- A. Fanfani
- A. Ferapontov
- A. Ferrando
- A. Flossdorf
- A. Gaddi
- A. Garcia-Bellido
- A. Gaz
- A. Geiser
- A. Ghezzi
- A. Giammanco
- A. Giassi
- A. Gilbert
- A. Givernaud
- A. Godshalk
- A. Gozzelino
- A. Graziano
- A. Gribushin
- A. Gude
- A. Guneratne Bryer
- A. Gurrola
- A. Gurtu
- A. Güth
- A. H. Ball
- A. Harel
- A. Heikkinen
- A. Heister
- A. Hektor
- A. Hervé
- A. Hinzmann
- A. Holzner
- A. Hunt
- A. Ivanov
- A. J. Bell
- A. Jafari
- A. K. Mohanty
- A. K. Sanchez
- A. Kalinowski
- A. Kalogeropoulos
- A. Kamenev
- A. Kapusi
- A. Karadzhinova
- A. Kayis Topaksu
- A. Khan
- A. Kharchilava
- A. Khukhunaishvili
- A. Knutsson
- A. Kopecky
- A. Korablev
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- V. Kim
- V. Konoplyanikov
- V. Kozhuharov
- V. Krutelyov
- V. Krychkine
- V. Kumar
- V. Lemaitre
- V. M. Ghete
- V. Maroussov
- V. Matveev
- V. Monaco
- V. Mossolov
- V. Murzin
- V. Oguri
- V. Oreshkin
- V. O’Dell
- V. Palichik
- V. Patras
- V. Pavlunin
- V. Perelygin
- V. Petrov
- V. Popov
- V. Rekovic
- V. Savrin
- V. Sharma
- V. Sharma
- V. Smirnov
- V. Sola
- V. Sordini
- V. Stolin
- V. Sulimov
- V. Tcholakov
- V. Timciuc
- V. Valuev
- V. Veeraraghavan
- V. Veszpremi
- V. Zhukov
- V. Zhukova
- W. A. Khan
- W. Adam
- W. Andrews
- W. Behrenhoff
- W. Bertl
- W. Bialas
- W. Busza
- W. Carvalho
- W. Clarida
- W. Cooper
- W. D. Teo
- W. D. Zeuner
- W. De Boer
- W. Dominik
- W. Erdmann
- W. Ferguson
- W. Flanagan
- W. Funk
- W. Gabella
- W. H. Smith
- W. Haj Ahmad
- W. Hopkins
- W. J. Spalding
- W. J. Womersley
- W. Johns
- W. Kiesenhofer
- W. Ko
- W. L. Aldá
- W. L. Prado Da Silva
- W. Lange
- W. Li
- W. Li
- W. Lin
- W. Lohmann
- W. Luo
- W. Lustermann
- W. Martin
- W. Reece
- W. Sakumoto
- W. Sun
- W. T. Ford
- W. To
- W. Van Doninck
- W. Waltenberger
- W. Wu
- W. Zou
- W.-S. Hou
- X. Janssen
- X. Meng
- X. Quan
- X. Shi
- X. T. Huang
- X. Wang
- Y. Assran
- Y. Bai
- Y. Ban
- Y. Chao
- Y. Chen
- Y. Cho
- Y. Choi
- Y. Eshaq
- Y. F. Liu
- Y. Fu
- Y. Gao
- Y. Gershtein
- Y. Gotra
- Y. Guo
- Y. H. Chang
- Y. H. Chang
- Y. Hsiung
- Y. Iiyama
- Y. Ivanov
- Y. J. Lei
- Y. J. Lu
- Y. K. Choi
- Y. Kim
- Y. Kubota
- Y. Kuessel
- Y. Lu
- Y. M. Tzeng
- Y. Ma
- Y. Mao
- Y. Maravin
- Y. Musienko
- Y. Onel
- Y. Pakhotin
- Y. Roh
- Y. S. Chung
- Y. Sirois
- Y. Tschudi
- Y. Tu
- Y. W. Chang
- Y. Weng
- Y. Yang
- Y. Yilmaz
- Y. Zheng
- Y.-J. Lee
- Yu. Andreev
- Z. Antunovic
- Z. C. Yang
- Z. Chen
- Z. Hatherell
- Z. Hu
- Z. J. Guo
- Z. K. Liu
- Z. L. Trocsanyi
- Z. Szillasi
- Z. Wan
- Z. Wang
- Z. Zhang
- Zero J. Kim
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2012
- Field of study
A search for the standard model Higgs boson in the H to ZZ to 2l 2nu decay
channel, where l = e or mu, in pp collisions at a center-of-mass energy of 7
TeV is presented. The data were collected at the LHC, with the CMS detector,
and correspond to an integrated luminosity of 4.6 inverse femtobarns. No
significant excess is observed above the background expectation, and upper
limits are set on the Higgs boson production cross section. The presence of the
standard model Higgs boson with a mass in the 270-440 GeV range is excluded at
95% confidence level.Comment: Submitted to JHE
Measurement of the Z/gamma* + b-jet cross section in pp collisions at 7 TeV
- Author
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- Abbiendi G.
- Abbrescia M.
- Abdullin S.
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- 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
Performance of the CMS Cathode Strip Chambers with Cosmic Rays
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- Zachariadou A
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- Zeinali M
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- Zelepoukine S
- Zeuner WD
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- 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
- …