4,731 research outputs found
Dynamics and ordering of weakly Brownian particles in directional drying
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2017
- Field of study
Drying of particle suspensions is an ubiquitous phenomenon with many natural
and practical applications. In particular, in unidirectional drying, the
evaporation of the solvent induces flows which accumulate particles at the
liquid/air interface. The progressive build-up of a dense region of particles
can be used, in particular, in the processing of advanced materials and
architectures while the development of heterogeneities and defects in such
systems is critical to their function. A lot of attention has thus been paid to
correlate the flow and particles dynamics to the ordering of particles.
However, dynamic observation at the particle scale and its correlation with
local particle ordering are still missing. Here we show by measuring the
particle velocities with high frame rate laser scanning confocal microscopy
that the ordering of weakly Brownian particles during directional drying in a
Hele-Shaw cell opened on one side depends on the particle velocity. Under the
ambient and experimental conditions presented in the following, the particle
velocities accumulate in two branches. A higher degree of ordering is found for
the branch of faster particle velocity which we explain by an increase in the
pressure drop which drags the particles into a denser packing as the flow
velocity increases. This counter-intuitive behaviour is the opposite to what is
found with Brownian particles, which can reorganize by Brownian motion into
denser packing during drying, as long as the flow velocity is not too high.
These results show that different kinetic conditions can be used to obtain
dense, defect-free regions of particles after drying. In particular, it
suggests that rapid, directional drying could be used to control the
crystallinity of particle deposits.Comment: 10 pages, 12 figure
Polyproline is a minimal antifreeze protein mimetic and enhances the cryopreservation of cell monolayers
- Author
- Publication venue
- 'Wiley'
- Publication date
- 22/11/2017
- Field of study
Tissue engineering, gene therapy, drug screening and emerging regenerative medicine therapies are fundamentally reliant on high-quality adherent cell culture, but current methods to cryopreserve cells in this format can give low cell yields and requires large volumes of solvent 'antifreezes'. Herein we report polyproline is a minimum (bio)synthetic mimic of antifreeze proteins, which is accessible by solution, solid phase and recombinant methods. We demonstrate that polyproline has ice recrystallization inhibition activity linked to its amphipathic helix and that it enhances the DMSO- cryopreservation of adherent cell lines. Polyproline may be a versatile additive in the emerging field of macromolecular cryoprotectants
Investigation of interface properties of Ni/Cu multilayers by high kinetic energy photoelectron spectroscopy
- Author
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- Field of study
ĐĐ˝ŃокŃиОннО-ŃОкŃиŃĐľŃкиК ŃОк в Đ°ĐşŃŃĐľŃŃŃво и гинокОНОгии
- Author
- Publication venue
- ĐĐĐĐŁ
- Publication date
- 01/01/2000
- Field of study
ШĐРТĐĐĐĄĐЧĐĐĄĐĐĐ /ĐĐĐĐĐ /ĐĐТĐФĐĐĐĐĐ /ТĐĐ ĐĄĐĐТĐĐŚĐĐĐĐŻĐĐФĐĐĐŚĐĐŻ /ĐĐĄĐĐĐĐĐĄĐĐĐ ĐĐĐĐĐĐĐ /ĐĐĄĐ /ĐĄĐĐРТĐĐĐĐРТ ĐĐ ĐĐĐĐĐĐĐŹĐĐŤĐĐĐĐТĐĐ ĐĐĐĐŹĐĐŤĐ ĐĐФĐĐĐŚĐĐ /ĐĐĄĐĐĐХТĐĐ ĐĐТĐĐĐĐŻĐĐĐĐĐĐĐĐĐĐЧĐĐĄĐĐĐ ĐĽĐĐ ĐŁĐ ĐĐЧĐĐĄĐĐĐ ĐĐĐĐ ĐĐŚĐ
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
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- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2012
- Field of study
The performance of muon reconstruction, identification, and triggering in CMS
has been studied using 40 inverse picobarns of data collected in pp collisions
at sqrt(s) = 7 TeV at the LHC in 2010. A few benchmark sets of selection
criteria covering a wide range of physics analysis needs have been examined.
For all considered selections, the efficiency to reconstruct and identify a
muon with a transverse momentum pT larger than a few GeV is above 95% over the
whole region of pseudorapidity covered by the CMS muon system, abs(eta) < 2.4,
while the probability to misidentify a hadron as a muon is well below 1%. The
efficiency to trigger on single muons with pT above a few GeV is higher than
90% over the full eta range, and typically substantially better. The overall
momentum scale is measured to a precision of 0.2% with muons from Z decays. The
transverse momentum resolution varies from 1% to 6% depending on pseudorapidity
for muons with pT below 100 GeV and, using cosmic rays, it is shown to be
better than 10% in the central region up to pT = 1 TeV. Observed distributions
of all quantities are well reproduced by the Monte Carlo simulation.Comment: Replaced with published version. Added journal reference and DO
Search for the standard model Higgs boson at LEP
- Author
- Abbaneo D
- Abbaneo D
- Abbiendi G
- Abbiendi G
- Abdallah J
- Abreu P
- Achard P
- Adam W
- Adriani O
- Adzic P
- Affholderbach K
- Aguilar-Benitez M
- Ainsley C
- Akesson PF
- Albrecht T
- Alcaraz J
- Alderweireld T
- Alemanni G
- Alemany-Fernandez R
- Alexander G
- Allaby J
- Allison J
- Allmendinger T
- Allport PP
- Aloisio A
- Alviggi MG
- Amaldi U
- Amapane N
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- Anagnostou G
- Anashkin E
- Anderhub H
- Anderson KJ
- Andreazza A
- Andreev VP
- Andringa S
- Anjos N
- Anselmo F
- Antilogus P
- Antonelli A
- Antonelli M
- Apel WD
- Arcelli S
- Arefiev A
- Armstrong SR
- Arnoud Y
- Asai S
- Ask S
- Asman B
- Augustin JE
- Augustinus A
- Awunor O
- Axen D
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- Aziz T
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- Vallage B
- van Dalen JA
- Van Dam P
- van de Walle RT
- van Dierendonck D
- Van Eldik J
- van Gulik R
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- Vicinanza D
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- Vogel H
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- von Wimmersperg-Toeller JH
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- Waller D
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- Wienemann P
- Wilkens H
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- Wu J
- Wu SL
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- Wunsch M
- Wyatt TR
- Wynhoff S
- Xia L
- Xie Y
- Xu R
- Xu ZZ
- Xue S
- Yamamoto J
- Yamashita S
- Yang BZ
- Yang CG
- Yang HJ
- Yang M
- Yeh SC
- Yuan C
- Yushchenko O
- Zachariadou K
- Zalewska A
- Zalewski P
- Zalite A
- Zalite Y
- Zavrtanik D
- Zeitnitz C
- Zer-Zion D
- Zhang J
- Zhang L
- Zhang ZP
- Zhao J
- Zhao W
- Zhu GY
- Zhu RY
- Zhuang HL
- Zhuravlov V
- Zichichi A
- Ziegler T
- Zilizi G
- Zimin NI
- Zimmermann B
- Zintchenko A
- Zito G
- Zivkovic L
- Zobernig G
- Zoller M
- Zupan M
- Publication venue
- ELSEVIER SCIENCE BV
- Publication date
- 17/07/2003
- Field of study
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
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- Kyriakis A
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- Sfiligoi I
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- Sharp P
- Sheldon P
- Shepherd-Themistocleous CH
- Shi X
- Shipkowski SP
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- Tsang KV
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- Yetkin T
- 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
- Zheng Y
- Zhokin A
- Zhu B
- Zhu RY
- Zhukov V
- Zhukova V
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- Zoeller MH
- Zotto P
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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
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- Yilmaz Y
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- Ziebarth EB
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- 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
Azimuthal anisotropy of charged particles at high transverse momenta in PbPb collisions at sqrt(s[NN]) = 2.76 TeV
- Author
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abdulsalam A
- Acosta D
- Acosta JG
- Acosta MV
- Adair A
- Adam N
- Adam W
- Adams MR
- Adams T
- Adiguzel A
- Adler V
- Adzic P
- Afanasiev S
- Agostino L
- Agram JL
- Aguilar-Benitez M
- Aguilo E
- Ahmad M
- Ahmad WH
- Ahuja S
- Akchurin N
- Akgun B
- Akgun U
- Akin IV
- Alagoz E
- Albajar C
- Albayrak EA
- Albergo S
- Albrow M
- Alcaraz Maestre J
- Alda Junior WL
- Alexander J
- Aliev T
- Alimena J
- Almeida N
- Alverson G
- Alves GA
- Amapane N
- Amsler C
- Anagnostou G
- Anastassov A
- Anderson J
- Anderson M
- Andrea J
- Andreev V
- Andreev V
- Andreev Y
- Andrews W
- Anghel IM
- Anjos TS
- Antonelli L
- Antunovic Z
- Apanasevich L
- Appelt E
- Apresyan A
- Arce P
- Arcidiacono R
- Arenton MW
- Arfaei H
- Argiro S
- Arneodo M
- Arora S
- Asawatangtrakuldee C
- Asghar MI
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- Autermann C
- Auzinger G
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- Avetisyan A
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- Azhgirey I
- Aziz T
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- Azzurri P
- Baarmand MM
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- Bagliesi G
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- Bakirci MN
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- Banerjee S
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- Bauerdick LAT
- Baumgartel D
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- Bayshev I
- Bazterra VE
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- Beaudette F
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- Behr J
- Behrenhoff W
- Behrens U
- Belforte S
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- Belknap D
- Bell AJ
- Bellan R
- Belotelov I
- Belyaev A
- Belyaev A
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- Novaes SF
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- Obertino MM
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- Paramesvaran S
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- Patel R
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- Patterson JR
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- Perelygin V
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- Perloff A
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- Perrey H
- Perries S
- Perrotta A
- Perrozzi L
- Peruzzi M
- Pesaresi M
- Peterman A
- Petkov P
- Petrakou E
- Petridis K
- Petrilli A
- Petrov V
- Petrucciani G
- Petrukhin A
- Petrushanko S
- Petyt D
- Pfeiffer A
- Piccolo D
- Piedra Gomez J
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- Pierro GA
- Pieta H
- Pietsch N
- Pimiae M
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- Pioppi M
- Piotrzkowski K
- Piparo D
- Piperov S
- Piroue P
- Pitzl D
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- Plestina R
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- Polatoz A
- Polese G
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- Poll A
- Pollack B
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- Pooth O
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- Potenza A
- Potenza R
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- Prado Da Silva WL
- Primavera F
- Prokofyev O
- Prosper H
- Ptochos F
- Puerta Pelayo J
- Pugliese G
- Puigh D
- Puljak I
- Qazi S
- Qian SJ
- Quan X
- Quast G
- Quertenmont L
- Rabbertz K
- Racz A
- Radburn-Smith BC
- Radi A
- Radicci V
- Radics B
- Ragazzi S
- Rahatlou S
- Rahbaran B
- Rahmat R
- Raics P
- Raidal M
- Rakness G
- Ralph D
- Rander J
- Ranieri R
- Ranjan K
- Rappoccio S
- Raspereza A
- Rathjens D
- Ratnikov F
- Ratnikova N
- Ratti SP
- Raupach F
- Raval A
- Raymond DM
- Razis PA
- Rebane L
- Rebassoo F
- Redaelli N
- Redjimi R
- Redondo I
- Reece W
- Reid ID
- Reis T
- Reithler H
- Rekovic V
- Remington R
- Renker D
- Rennefeld J
- Reucroft S
- Reyes-Santos MA
- Ribnik J
- Riccardi C
- Richards A
- Richman J
- Riedl C
- Rikova MI
- Rinkevicius A
- Rios AAO
- Rizzi A
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- Roberts J
- Robles J
- Robmann P
- Rodenburg M
- Rodozov M
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- Rodrigues Antunes J
- Rodriguez JL
- Rodriguez-Marrero AY
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- Roland C
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- Rolandi G
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- Romeo F
- Romero A
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- Rommerskirchen T
- Rompotis N
- Ronchese P
- Ronga FJ
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- Rosowsky A
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- Sanchez MCDLB
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- Schleper P
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- Schmitt M
- Schmitz SA
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- Schott G
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- Sguazzoni G
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- Sharma A
- Sharma A
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- Shepherd-Themistocleous CH
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- Shoaib M
- Shrestha S
- Shreyber I
- Shukla P
- Shumeiko N
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- Sirois Y
- Siroli G
- Sirunyan AM
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- Spalding WJ
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- Stoynev S
- Strauss J
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- Vaandering EW
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- Van Onsem GP
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- Wissing C
- Wittich P
- Wittmer B
- Woehri HK
- Wolf M
- Wolf R
- Womersley WJ
- Won S
- Wood D
- Wood J
- Wood JS
- Worm SD
- Wright D
- Wrochna G
- Wu W
- Wuerthwein F
- Wulz C-E
- Wyslouch B
- Xiao H
- Xie S
- Xu M
- Yagil A
- Yalvac M
- Yang F
- Yang M
- Yang Y
- Yang ZC
- Yazgan E
- Yelton J
- Yetkin T
- Yi K
- Yildirim E
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoo J
- Yoon AS
- York A
- Yu I
- Yu SS
- Yumiceva F
- Yun JC
- Zabel J
- Zabi A
- Zablocki J
- Zaganidis N
- Zakaria M
- Zalewski P
- Zanetti M
- Zang J
- 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 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. CustĂłdio
- 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. GĂźth
- A. H. Ball
- A. Harel
- A. Heikkinen
- A. Heister
- A. Hektor
- A. HervĂŠ
- 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
- A. Korpela
- A. Korytov
- A. Kraan
- A. Krokhotin
- A. Kropivnitskaya
- A. Kubik
- A. Kumar
- A. Kumar
- A. Kumar
- A. Kyriakis
- A. Lanaro
- A. Lanev
- A. Lath
- A. Ledovskoy
- A. Leonidov
- A. Linn
- A. Lopez
- A. Lopez Virto
- A. Lucaroni
- A. Luthra
- A. LĂŠonard
- A. M. Guler
- A. M. Rossi
- A. M. Sirunyan
- A. Marinov
- A. Markina
- A. Markou
- A. Martelli
- A. Massironi
- A. Melo
- A. Messineo
- A. Mestvirishvili
- A. Meyer
- A. Moeller
- A. Mohammadi
- A. Mohapatra
- A. Montanari
- A. Morelos Pineda
- A. Mott
- A. Mussgiller
- A. Nappi
- A. Nayak
- A. Nikitenko
- A. Nowack
- A. NĂźrnberg
- A. O. M. Iorio
- A. Oehler
- A. Olbrechts
- A. Ostapchuk
- A. Ozpineci
- A. P. R. Gay
- A. P. Singh
- A. Panagiotou
- A. Papageorgiou
- A. Pashenkov
- A. Penzo
- A. Perieanu
- A. Perloff
- A. Perrotta
- A. Peterman
- A. Petrilli
- A. Petrukhin
- A. Pfeiffer
- A. Pin
- A. Polatoz
- A. Poll
- A. Pompili
- A. Potenza
- A. Pozdnyakov
- A. Racz
- A. Radi
- A. Raspereza
- A. Raval
- A. Richards
- A. Rinkevicius
- A. Rizzi
- A. Romero
- A. Rose
- A. Rosowsky
- A. Ruiz-Jimeno
- A. Ryd
- A. S. Yoon
- A. Safonov
- A. Saha
- A. Sakharov
- A. Santocchia
- A. Santoro
- A. Savin
- A. Scheurer
- A. Schmidt
- A. Sharma
- A. Sharma
- A. Sill
- A. Singovsky
- A. Skuja
- A. Snigirev
- A. Sobol
- A. Solano
- A. Sparrow
- A. Spiridonov
- A. Stahl
- A. Staiano
- A. Starodumov
- A. Svyatkovskiy
- A. Sznajder
- A. SĂĄnchez-HernĂĄndez
- A. T. Laasanen
- A. T. Meneguzzo
- A. T. Serban
- A. Tapper
- A. Tatarinov
- A. Taurok
- A. Thea
- A. Tiko
- A. Toropin
- A. Tricomi
- A. Tropiano
- A. Tsirou
- A. Tumasyan
- A. Uzunian
- A. V. Gritsan
- A. Van Spilbeeck
- A. Vartak
- A. Venturi
- A. Vilela Pereira
- A. Vinogradov
- A. Volkov
- A. Volodko
- A. Vorobyev
- A. Whitbeck
- A. Y. RodrĂguez-Marrero
- A. Yagil
- A. York
- A. Zabi
- A. Zarubin
- A. Zatserklyaniy
- A. Zhokin
- A. Zuranski
- A.-C. Le Bihan
- A.-M. Magnan
- An. Vorobyev
- ATLAS collaboration
- B. A. Barnett
- B. Akgun
- B. Alver
- B. Betchart
- B. Bilin
- B. Bilki
- B. Blumenfeld
- B. Boimska
- B. Bylsma
- B. C. Choudhary
- B. C. Radburn-Smith
- B. Calvert
- B. Caponeri
- B. Casal
- B. Clerbaux
- B. Cox
- B. CurĂŠ
- B. Dahmes
- B. De La Cruz
- B. Diamond
- B. Dorney
- B. Fabbro
- B. Francis
- B. Frisch
- B. Gobbo
- B. Gomber
- B. Gomez Moreno
- B. Hegner
- B. Heltsley
- B. Heyburn
- B. Hong
- B. Hooberman
- B. Ille
- B. Isildak
- B. Kargoll
- B. Kim
- B. Klein
- B. Klima
- B. Kreis
- B. Lee
- B. Lutz
- B. Mangano
- B. Marangelli
- B. Mathias
- B. Millan Mejias
- B. Mura
- B. P. Padley
- B. Parida
- B. Pavlov
- B. Pollack
- B. R. Drell
- B. Rahbaran
- B. Roland
- B. Rutherford
- B. Safarzadeh
- B. Scurlock
- B. Snook
- B. Stieger
- B. Tali
- B. Ujvari
- B. W. Kennedy
- B. Wittmer
- B. Wyslouch
- B. Zhu
- C Anastasiou
- C Anastasiou
- C Anastasiou
- C. A. Bernardes
- C. A. Carrillo Montoya
- C. Albajar
- C. Amsler
- C. Asawatangtrakuldee
- C. Autermann
- C. Bardak
- C. Barth
- C. Battilana
- C. Baty
- C. Bernet
- C. Biino
- C. Botta
- C. Boulahouache
- C. Brew
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- S. Nourbakhsh
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- W. Dominik
- W. Erdmann
- W. Ferguson
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- W. Gabella
- W. H. Smith
- W. Haj Ahmad
- W. Hopkins
- W. J. Spalding
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- W. Luo
- W. Lustermann
- W. Martin
- W. Reece
- W. Sakumoto
- W. Sun
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- W. To
- W. Van Doninck
- W. Waltenberger
- W. Wu
- W. Zou
- W.-S. Hou
- X. Janssen
- X. Meng
- X. Quan
- X. Shi
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- X. Wang
- Y. Assran
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- 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
- âŚ