1,658 research outputs found
Shape-temperature relationship of ice crystals in mixed-phase clouds based on observations with polarimetric cloud radar: Shape-temperature relationship of ice crystals in mixed-phase cloudsbased on observations with polarimetric cloud radar
- Author
- Publication venue
- Publication date
- 19/09/2016
- Field of study
This thesis is devoted to the experimental quantitative characterization of the shape and orientation distribution of ice particles in clouds. The characterization is based on measured and modeled elevation dependencies of the polarimetric parameters differential reflectivity and correlation coefficient. The polarimetric data is obtained using a newly developed 35-GHz cloud radar MIRA-35 with hybrid polarimetric configuration and scanning capabilities. The full procedure chain of the technical implementation and the realization of the setup of the hybrid-mode cloud radar for the shape determination are presented. This includes the description of phase adjustments in the transmitting paths, the introduction of the general data processing scheme, correction of the data for the differences of amplifications and electrical path lengths in the transmitting and receiving channels, the rotation of the polarization basis by 45°, the correction of antenna effects on polarimetric measurements, the determination of spectral polarimetric variables, and the formulation of a scheme to increase the signal-to-noise ratio. Modeling of the polarimetric variables is based on existing backscattering models assuming the spheroidal representation of cloud scatterers. The parameters retrieved from the model are polarizability ratio and degree of orientation, which can be assigned to certain particle orientations and shapes.
In the thesis the first quantitative estimations of ice particle shape at the top of liquid-topped clouds are presented. Analyzed ice particles were formed in the presence of supercooled water and in the temperature range from -20 °C to -3 °C. The estimation is based on polarizability ratios of ice particles measured by the MIRA-35 with hybrid polarimetric configuration, manufactured by METEK GmbH. For the study, 22 cases observed during the ACCEPT (Analysis of the Composition of Clouds with Extended Polarization Techniques) field campaign were used. Polarizability ratios retrieved for cloud layers with cloud-top temperatures of about -5, -8, -15, and -20 °C were 1.6, 0.9, 0.6, and 0.9, respectively. Such values correspond to prolate, quasi-isotropic, oblate, and quasi-isotropic particles, respectively. Data from a free-fall chamber were used for the comparison. A good agreement of detected shapes with well-known shape{temperature dependencies observed in laboratories was found.:1 Introduction
2 Formation and development of ice particles: Laboratory studies and remote observations
2.1 Heterogeneous ice formation in the atmosphere
2.2 Laboratory investigations of ice crystal development
2.3 Polarimetric radar observations of ice microphysics
2.3.1 Polarimetry in weather radar networks
2.3.2 Polarimetry in cloud radars
2.3.3 Polarization coupling
2.4 Aims and scientific questions
3 Effects of antenna patterns on cloud radar polarimetric measurements
3.1 Measurements of complex antenna patterns
3.1.1 Problem definition
3.1.2 Measurement description
3.1.3 Results of antenna pattern measurements
3.2 Correction of LDR measurements
3.3 Discrimination between insects and clouds
4 Cloud radar MIRA-35 with hybrid mode
4.1 Implementation and phase adjustment
4.2 Processing of the coherency matrix
4.3 Correction of the coherency matrix for differences of channels
4.4 The coherency matrix in the slanted basis
4.5 Correction for the antenna coupling
4.6 Spectral polarimetric variables
4.7 Sensitivity issue
5 Shape and orientation retrieval
5.1 Backscattering model
5.2 Retrieval technique
5.3 Case study
6 Shape-temperature relationship of pristine ice crystals
6.1 Instrumentation and data set
6.2 Examples of the shape retrieval
6.2.1 Case 1: 12 October 2014, 15:00-16:00 UTC
6.2.2 Case 2: 18 October 2014, 01:00-02:00 UTC
6.2.3 Case 3: 20 October 2014, 18:00-19:00 UTC
6.2.4 Case 4: 10 November 2014, 02:00-03:00 UTC
6.2.5 Case 5: 7 November 2014, 20:00-21:00 UTC
6.3 Comparison of shape with laboratory studies
6.4 Orientation of pristine ice crystals
7 Summary and outlook
Bibliography
List of Abbreviations
List of Symbol
Relationship between temperature and apparent shape of pristine ice crystals derived from polarimetric cloud radar observations during the ACCEPT campaign
- Publication venue
- MĂŒnchen : European Geopyhsical Union
- Publication date
- 01/01/2016
- Field of study
This paper presents first quantitative estimations of apparent ice particle shape at the top of liquid-topped clouds. Analyzed ice particles were formed under mixed-phase conditions in the presence of supercooled water and in the temperature range from â20 to â3âŻÂ°C. The estimation is based on polarizability ratios of ice particles measured by a Ka-band cloud radar MIRA-35 with hybrid polarimetric configuration. Polarizability ratio is a function of the geometrical axis ratio and the dielectric properties of the observed hydrometeors. For this study, 22 cases observed during the ACCEPT (Analysis of the Composition of Clouds with Extended Polarization Techniques) field campaign were used. Polarizability ratios retrieved for cloud layers with the cloud-top temperatures of ââŒââ5, ââŒââ8, ââŒââ15, and ââŒââ20âŻÂ°C were 1.6, 0.9, 0.6, and 0.9, respectively. Such values correspond to prolate, quasi-isotropic, oblate, and quasi-isotropic particles, respectively. Data from a free-fall chamber were used for the comparison. A good agreement of detected apparent shapes with well-known shapeâtemperature dependencies observed in laboratories was found. Polarizability ratios used for the analysis were estimated for areas located close to the cloud top, where aggregation and riming processes do not strongly affect ice particles. We concluded that, in microwave scattering models, ice particles detected in these areas can be assumed to have pristine shapes. It was also found that even slight variations of ambient conditions at the cloud top with temperatures warmer than ââŒââ5âŻÂ°C can lead to rapid changes of ice crystal shape
EUREC4A's Maria S. Merian ship-based cloud and micro rain radar observations of clouds and precipitation
- Author
- Publication venue
- Publication date
- 01/09/2021
- Field of study
As part of the EUREC4A field campaign, the research vessel Maria S. Merian probed an oceanic region between 6°âN and 13.8°âN and 51°âW to 60°âW for approximately 32 days. Trade wind cumulus clouds were sampled in the trade-wind alley region east of Barbados as well as in the transition region between the trades and the intertropical convergence zone, where the ship crossed some mesoscale oceanic eddies. We collected continuous observations of cloud and precipitation profiles at unprecedented vertical resolution (7â10âm in the first 3000âm) and high temporal resolution (1â3âs) using a W-band radar and micro-rain radar (MRR-PRO), installed on an active stabilization platform to reduce the impact of ship motions on the observations. The paper describes the ship motion correction algorithm applied to the Doppler observations to extract corrected hydrometeors vertical velocities and the algorithm created to filter interference patterns in the MRR-PRO observations. Radar reflectivity, mean Doppler velocity, spectral width and skewness for W-band and attenuated reflectivity, mean Doppler velocity and rain rate for MRR-PRO are shown for a case study to demonstrate the potential of the high resolution adopted. As non-standard analysis, we also retrieved and provided liquid water path (LWP) from the 89âGHz passive channel available on the W-band radar system. All datasets and hourly and daily quicklooks are publically available. Data can be accessed and basic variables can be plotted online via the intake catalog of the online book "How to EUREC4A".Postprint (author's final draft
Different Effects of Phototherapy for Rat Glioma during Sleep and Wakefulness
- Author
- Adushkina Viktoria
- Blokhina Inna
- Dmitrenko Alexander
- Dubrovsky Alexander
- Elezarova Inna
- Evsyukova Arina
- Fedosov Ivan
- Ilyukov Egor
- Iskra Tatyana
- Krupnova Valeria
- Lykova Ekaterina
- Manzhaeva Maria
- Myagkov Dmitry
- Navolokin Nikita
- Saranceva Elena
- Semyachkina-Glushkovskaya Oxana
- Shirokov Alexander
- Telnova Valeria
- Terskov Andrey
- Tuktarov Dmitry
- Tuzhilkin Matvey
- Tzoy Maria
- Zlatogosrkaya Daria
- Publication venue
- Humboldt-UniversitÀt zu Berlin
- Publication date
- 24/01/2024
- Field of study
There is an association between sleep quality and glioma-specific outcomes, including survival. The critical role of sleep in survival among subjects with glioma may be due to sleep-induced activation of brain drainage (BD), that is dramatically suppressed in subjects with glioma. Emerging evidence demonstrates that photobiomodulation (PBM) is an effective technology for both the stimulation of BD and as an add-on therapy for glioma. Emerging evidence suggests that PBM during sleep stimulates BD more strongly than when awake. In this study on male Wistar rats, we clearly demonstrate that the PBM course during sleep vs. when awake more effectively suppresses glioma growth and increases survival compared with the control. The study of the mechanisms of this phenomenon revealed stronger effects of the PBM course in sleeping vs. awake rats on the stimulation of BD and an immune response against glioma, including an increase in the number of CD8+ in glioma cells, activation of apoptosis, and blockage of the proliferation of glioma cells. Our new technology for sleep-phototherapy opens a new strategy to improve the quality of medical care for patients with brain cancer, using promising smart-sleep and non-invasive approaches of glioma treatment.Russian Science FoundationPeer Reviewe
Machine Learning Technology for EEG-Forecast of the BloodâBrain Barrier Leakage and the Activation of the Brainâs Drainage System during Isoflurane Anesthesia
- Author
- Adushkina Viktoria
- Blokhina Inna
- Borovkova Ekaterina
- Dmitrenko Alexander
- Dubrovsky Alexander
- Elizarova Inna
- Evsukova Arina
- Fedosov Ivan
- Hramkov Alexey
- Ilyukov Egor
- Karavaev Anatoly
- Krupnova Valeria
- Kurths JĂŒrgen
- Manzhaeva Maria
- Myagkov Dmitry
- Prokhorov Mikhail
- Semenova Nadezhda
- Semyachkina-Glushkovskaya Oxana
- Sergeev Konstantin
- Shirokov Alexander
- Slepnev Andrey
- Terskov Andrey
- Tuktarov Dmitry
- Tuzhilkin Matvey
- Zlatogorskaya Daria
- Publication venue
- Humboldt-UniversitÀt zu Berlin
- Publication date
- 02/11/2023
- Field of study
Anesthesia enables the painless performance of complex surgical procedures. However, the effects of anesthesia on the brain may not be limited only by its duration. Also, anesthetic agents may cause long-lasting changes in the brain. There is growing evidence that anesthesia can disrupt the integrity of the bloodâbrain barrier (BBB), leading to neuroinflammation and neurotoxicity. However, there are no widely used methods for real-time BBB monitoring during surgery. The development of technologies for an express diagnosis of the opening of the BBB (OBBB) is a challenge for reducing post-surgical/anesthesia consequences. In this study on male rats, we demonstrate a successful application of machine learning technology, such as artificial neural networks (ANNs), to recognize the OBBB induced by isoflurane, which is widely used in surgery. The ANNs were trained on our previously presented data obtained on the sound-induced OBBB with an 85% testing accuracy. Using an optical and nonlinear analysis of the OBBB, we found that 1% isoflurane does not induce any changes in the BBB, while 4% isoflurane caused significant BBB leakage in all tested rats. Both 1% and 4% isoflurane stimulate the brainâs drainage system (BDS) in a dose-related manner. We show that ANNs can recognize the OBBB induced by 4% isoflurane in 57% of rats and BDS activation induced by 1% isoflurane in 81% of rats. These results open new perspectives for the development of clinically significant bedside technologies for EEG-monitoring of OBBB and BDS.Russian Science FoundationRussian Ministry of Science and High EducationFirst Moscow State Medical University of the Ministry of Health of the Russian Federation (Sechenov University)research center âSYMBIOSISâPeer Reviewe
Hunt for new phenomena using large jet multiplicities and missing transverse momentum with ATLAS in 4.7 fbâ1 of sâ=7TeV proton-proton collisions
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- A. A. ABDELALIM
- A. A. CARTER
- A. A. GRILLO
- A. A. KOMAR
- A. A. MINAENKO
- A. A. NEPOMUCENO
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- A. A. SOLODKOV
- A. ABDESSELAM
- A. AHMAD
- A. AKTAS
- A. ALOISIO
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- A. AMORIM
- A. ANDREAZZA
- A. ANGERAMI
- A. ANNOVI
- A. ANTONAKI
- A. ARTAMONOV
- A. ASTBURY
- A. ASTVATSATOUROV
- A. B. FENYUK
- A. B. LAZAREV
- A. BANGERT
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- P. MORETTINI
- P. N. RATOFF
- P. NECHAEVA
- P. NEMETHY
- P. NEVSKI
- P. NILSSON
- P. O. DEFAY
- P. O. DEVIVEIROS
- P. OBERSON
- P. P. ALLPORT
- P. PERRODO
- P. PERUS
- P. POFFENBERGER
- P. POSPICHAL
- P. PRALAVORIO
- P. PUZO
- P. R. NORTON
- P. RENKEL
- P. REZNICEK
- P. RUZICKA
- P. RYAN
- P. S. L. BOOTH
- P. S. MANGEARD
- P. S. MIYAGAWA
- P. S. WELLS
- P. SALA
- P. SANDHU
- P. SAVARD
- P. SAVVA
- P. SCHACHT
- P. SCHMID
- P. SHERWOOD
- P. SHIELD
- P. SICHO
- P. SINERVO
- P. SKUBIC
- P. SLATTERY
- P. SPECKMAYER
- P. STAROBA
- P. STAROVOITOV
- P. STAVINA
- P. STEINBACH
- P. STEINBERG
- P. STRACHOTA
- P. STRIZENEC
- P. T. KEENER
- P. TAS
- P. TEIXEIRA DIAS
- P. TIPTON
- P. U. E. ONYISI
- P. URQUIJO
- P. URREJOLA
- P. V. M. DA SILVA
- P. V. TSIARESHKA
- P. VALENTE
- P. VAN GEMMEREN
- P. VANKOV
- P. VINCENT
- P. VOKAC
- P. WAGNER
- P. WEBER
- P. WERNER
- P. WIENEMANN
- P. ZARZHITSKY
- P.A. MALECKI
- P.H. MARTIN
- P.H. SCHUNE
- P.H. SCHWEMLING
- PICCININI MAURIZIO
- Q. OUYANG
- Q. T. SHAO
- Q. ZHANG
- R. A. MCLAREN
- R. A. MCPHERSON
- R. A. RICHARDS
- R. ALON
- R. ASFANDIYAROV
- R. AVRAMIDOU
- R. B. NICKERSON
- R. BARTOLDUS
- R. BECCHERLE
- R. BERNHARD
- R. BISCHOF
- R. BOCK
- R. BONINO
- R. BRENNER
- R. BROCK
- R. BRUNELIERE
- R. C. JARED
- R. C. SCHOLTE
- R. C. W. HENDERSON
- R. CALKINS
- R. CALOI
- R. CAPUTO
- R. CARDARELLI
- R. CHERKAOUI EL MOURSLI
- R. CIFTCI
- R. COCO
- R. COLUCCIA
- R. COURA TORRES
- R. CRUPI
- R. D. HARRINGTON
- R. D. KASS
- R. D. S.T. DENIS
- R. D. SCHAMBERGER
- R. DANKERS
- R. DAVIDSON
- R. DE ASMUNDIS
- R. DHULLIPUDI
- R. DI NARDO
- R. DIPANJAN
- R. DJILKIBAEV
- R. DOBINSON
- R. DUXFIELD
- R. E. BLAIR
- R. E. HUGHES JONES
- R. E. LONG
- R. ELY
- R. ENGELMANN
- R. FEBBRARO
- R. FERRARI
- R. FROESCHL
- R. GIORDANO
- R. GONCALO
- R. H. HAKOBYAN
- R. HACKENBURG
- R. HARPER
- R. HARTEL
- R. HAUSER
- R. HERTENBERGER
- R. ICHIMIYA
- R. ISHMUKHAMETOV
- R. J. HAWKINGS
- R. J. HOMER
- R. J. MADARAS
- R. J. MILLER
- R. J. TEUSCHER
- R. J. THOMPSON
- R. K. DAYA
- R. KEELER
- R. KEHOE
- R. KLINGENBERG
- R. KONOPLICH
- R. KOWALEWSKI
- R. KWEE
- R. L. BATES
- R. L. MCCARTHY
- R. LAFAYE
- R. LEITNER
- R. LIFSHITZ
- R. M. BARNETT
- R. M. BIANCHI
- R. M. FAKHRUTDINOV
- R. MACKEPRANG
- R. MAENNER
- R. MAMEGHANI
- R. MANDRYSCH
- R. MARSHALL
- R. MASHINISTOV
- R. MAZINI
- R. MEERA LEBBAI
- R. MEHDIYEV
- R. MOLES VALLS
- R. MOUNT
- R. MURILLO GARCIA
- R. N. NEVES
- R. NICOLAIDOU
- R. NISIUS
- R. NUNES
- R. OSPANOV
- R. P. MIDDLETON
- R. P. TAYLOR
- R. P. THUN
- R. PENGO
- R. PERRINO
- R. PEZOA
- R. PIEGAIA
- R. PLACAKYTE
- R. POPESCU
- R. PORTER
- R. PRABHU
- R. PRAVAHAN
- R. R. RIOS
- R. R. SZCZYGIEL
- R. REECE
- R. REZVANI
- R. RICHTER
- R. S. ORR
- R. SADYKOV
- R. SANDSTROEM
- R. SANTONICO
- R. SCHWIENHORST
- R. SCHWIERZ
- R. SEUSTER
- R. SOBIE
- R. SOLUK
- R. SPIGHI
- R. SPIWOKS
- R. STAMEN
- R. STROHMER
- R. STROYNOWSKI
- R. TAFIROUT
- R. TAKASHIMA
- R. TANAKA
- R. TER ANTONYAN
- R. VAN BERG
- R. VARI
- R. VENESS
- R. VOSS
- R. VUILLERMET
- R. W. CLIFFT
- R. W. GARDNER
- R. W. L. JONES
- R. W. MOORE
- R. W. STANEK
- R. WALKER
- R. WALL
- R. WASTIE
- R. WUNSTORF
- R. YOOSOOFMIYA
- R. YOSHIDA
- R. ZAIDAN
- R. ZIMMERMANN
- R. ZITOUN
- RINALDI LORENZO
- S. A. CETIN
- S. A. GOROKHOV
- S. AEFSKY
- S. ALBRAND
- S. ANTONELLI
- S. AOUN
- S. ARFAOUI
- S. ASAI
- S. ASK
- S. B. SILVERSTEIN
- S. BAKER
- S. BANERJEE
- S. BARANOV
- S. BATHE
- S. BEHAR HARPAZ
- S. BEN AMI
- S. BENTVELSEN
- S. BERTOLUCCI
- S. BETHKE
- S. BINET
- S. BORDONI
- S. BORRONI
- S. BOSER
- S. BRACCINI
- S. BRAVO
- S. BRESSLER
- S. BRUNET
- S. BURDIN
- S. BURKE
- S. C. HSU
- S. C. LEE
- S. C. LIN
- S. C. SEIDEL
- S. CABRERA URBAN
- S. CAMPANA
- S. CARON
- S. CARRON MONTERO
- S. CAUGHRON
- S. CHARRON
- S. CHATTERJII
- S. CHEATHAM
- S. CHEKANOV
- S. CHEN
- S. CHENG
- S. CHOURIDOU
- S. COELLI
- S. CONSTANTINESCU
- S. CORREARD
- S. CREPE RENAUDIN
- S. CUNEO
- S. D'AURIA
- S. D. KOLYA
- S. DE CECCO
- S. DEAN
- S. DEMERS
- S. DHALIWAL
- S. DI LUISE
- S. DIGLIO
- S. DITA
- S. E. ALLWOOD SPIERS
- S. ECKERT
- S. ECKWEILER
- S. ELLES
- S. ERREDE
- S. FALCIANO
- S. FERRAG
- S. FICHET
- S. FLEISCHMANN
- S. FRANCHINO
- S. FRANZ
- S. FRATINA
- S. GADOMSKI
- S. GENTILE
- S. GEORGE
- S. GIAGU
- S. GOLDFARB
- S. GONZALEZ DE LA HOZ
- S. GONZALEZ SEVILLA
- S. GRANCAGNOLO
- S. GRINSTEIN
- S. H. KIM
- S. H. OH
- S. H. ROBERTSON
- S. HAAS
- S. HAIDER
- S. HAMILTON
- S. HASEGAWA
- S. HASSANI
- S. HAUG
- S. HEIM
- S. HEISTERKAMP
- S. HELLMAN
- S. HENROT VERSILLE
- S. HILLERT
- S. HORNER
- S. HORVAT
- S. HOU
- S. I. KAZI
- S. I. PARKER
- S. ISTIN
- S. J. DALLISON
- S. J. HAYWOOD
- S. J. HEAD
- S. J. HILLIER
- S. J. M. PEETERS
- S. J. MAXFIELD
- S. J. MCMAHON
- S. J. PARK
- S. J. WHEELER ELLIS
- S. JAKOBSEN
- S. JEZEQUEL
- S. JIN
- S. JOHNERT
- S. JORGENSEN
- S. K. NDERITU
- S. KABANA
- S. KAGAWA
- S. KAISER
- S. KALININ
- S. KAMA
- S. KERSTEN
- S. KLOUS
- S. KLUTH
- S. KOENIG
- S. KOLOS
- S. KONIG
- S. KOPERNY
- S. KOTOV
- S. KOVAR
- S. KUEHN
- S. KULESHOV
- S. L. CHEUNG
- S. L. LLOYD
- S. L. WU
- S. LAI
- S. LAPLACE
- S. LEVONIAN
- S. LI
- S. LIU
- S. LOCKWITZ
- S. LUCAS
- S. M. FARRINGTON
- S. M. FISHER
- S. M. GIBSON
- S. M. WANG
- S. MAJEWSKI
- S. MALTEZOS
- S. MALYUKOV
- S. MANOLOPOULOS
- S. MARTI GARCIA
- S. MATTIG
- S. MCGARVIE
- S. MEHLHASE
- S. MENKE
- S. MEUSER
- S. MICHAL
- S. MIGAS
- S. MIMA
- S. MISAWA
- S. MISCETTI
- S. MOED
- S. MOHRDIECK MOCK
- S. MONTESANO
- S. N. GOLOVNIA
- S. N. STANCU
- S. NEGRONI
- S. NEKTARIJEVIC
- S. NEMECEK
- S. O. HOLMGREN
- S. ODA
- S. ODAKA
- S. OKADA
- S. OWEN
- S. P. AHLEN
- S. P. BARANOV
- S. P. DENISOV
- S. P. KONOVALOV
- S. P. MC KEE
- S. P. WHITAKER
- S. P. YOUSSEF
- S. PALESTINI
- S. PANITKIN
- S. PATARAIA
- S. PATRICELLI
- S. PERSEMBE
- S. PODDAR
- S. POSPISIL
- S. PRASAD
- S. PROTOPOPESCU
- S. PSOROULAS
- S. R. ARMSTRONG
- S. R. WHITEHEAD
- S. RAJAGOPALAN
- S. RAJEK
- S. RESCIA
- S. RESCONI
- S. RIEKE
- S. ROBINS
- S. RODIER
- S. ROE
- S. ROLLI
- S. ROSATI
- S. RZAEVA
- S. SANDVOSS
- S. SCHAETZEL
- S. SCHLENKER
- S. SCHUH
- S. SIMION
- S. SNYDER
- S. SPAGNOLO
- S. STAPNES
- S. STONJEK
- S. STRANDBERG
- S. SUBRAMANIA
- S. SULTANSOY
- S. SUSHKOV
- S. T. FRENCH
- S. TABOADA GAMEIRO
- S. TANAKA
- S. TAPPROGGE
- S. TAREM
- S. TERADA
- S. THOMA
- S. TIMM
- S. TISSERANT
- S. TODOROVA NOVA
- S. TOKAR
- S. TRINCAZ DUVOID
- S. TSUNO
- S. V. CHEKULAEV
- S. V. KOPIKOV
- S. V. MOROZOV
- S. V. MOURAVIEV
- S. V. PELEGANCHUK
- S. VAHSEN
- S. VALKAR
- S. VALLECORSA
- S. VENEZIANO
- S. VENTURA
- S. VIRET
- S. VLACHOS
- S. W. O'NEALE
- S. W. SNOW
- S. WALSH
- S. WATTS
- S. WENDLER
- S. WENIG
- S. WHITE
- S. WILLOCQ
- S. XELLA
- S. XIE
- S. Y. NESTEROV
- S. Y.U. SIVOKLOKOV
- S. Y.U. SMIRNOV
- S. YAMAMOTO
- S. YANG
- S. YE
- S. ZENZ
- S. ZHENG
- S. ZIMMERMANN
- SBARRA CARLA
- SBRIZZI ANTONIO
- SEMPRINI CESARI NICOLA
- T. A. DIETZSCH
- T. A. MARTIN
- T. A. MULLER
- T. ADYE
- T. AKDOGAN
- T. ALEXOPOULOS
- T. ANDEEN
- T. ARGYROPOULOS
- T. B. MOORE
- T. B. SJURSEN
- T. BAIN
- T. BARBER
- T. BARILLARI
- T. BARKLOW
- T. BEAU
- T. BERRY
- T. BOLD
- T. BUANES
- T. BURAN
- T. BURGESS
- T. BYATT
- T. C. MEYER
- T. C. PETERSEN
- T. CARLI
- T. CHEN
- T. CHRISTIANSEN
- T. CORNELISSEN
- T. COSTIN
- T. CUHADAR DONSZELMANN
- T. D. STEWART
- T. DAI
- T. DAVIDEK
- T. DEL PRETE
- T. DJOBAVA
- T. DOHERTY
- T. DOHMAE
- T. DUBBS
- T. EHRICH
- T. EIFERT
- T. EKELOF
- T. FAROOQUE
- T. FLICK
- T. FONSECA MARTIN
- T. GADFORT
- T. GOLLING
- T. GOPFERT
- T. GOTTFERT
- T. GREENSHAW
- T. GUILLEMIN
- T. H. MOYE
- T. HANSL KOZANECKA
- T. HARENBERG
- T. HARUYAMA
- T. HAYAKAWA
- T. HEMPEREK
- T. HEN[SS]
- T. HOLY
- T. HORAZDOVSKY
- T. HORI
- T. HOTT
- T. HOWE
- T. HRYN'OVA
- T. I. HOLLINS
- T. INCE
- T. ISOBE
- T. J. BRODBECK
- T. J. JONES
- T. J. MCMAHON
- T. J. SLOAN
- T. K. NELSON
- T. K. O. DOAN
- T. K. OHSKA
- T. KAWAMOTO
- T. KITTELMANN
- T. KLIMKOVICH
- T. KLIOUTCHNIKOVA
- T. KLUGE
- T. KOBAYASHI
- T. KOFFAS
- T. KOHRIKI
- T. KOKOTT
- T. KONDO
- T. KONO
- T. KUBOTA
- T. KUHL
- T. LAGOURI
- T. LARI
- T. LECOMPTE
- T. LENZ
- T. LIU
- T. LODDENKOETTER
- T. LOHSE
- T. M. LISS
- T. M. MEGURO
- T. MAENO
- T. MASHIMO
- T. MASUBUCHI
- T. MATSUSHITA
- T. MOA
- T. N. ADDY
- T. N. TRINH
- T. NATTERMANN
- T. NAUMANN
- T. NIINIKOSKI
- T. NISHIYAMA
- T. NUNNEMANN
- T. NYMAN
- T. OHSHIMA
- T. OHSUGI
- T. OKUYAMA
- T. P. A. AKESSON
- T. P. SHAH
- T. PAULY
- T. R. MCMAHON
- T. RADOR
- T. SARANGI
- T. SASAKI
- T. SHIN
- T. SLAVICEK
- T. SLUKA
- T. SPREITZER
- T. STAHL
- T. STOCKMANNS
- T. SUGIMOTO
- T. SUMIDA
- T. SUZUKI
- T. SYKORA
- T. SZYMOCHA
- T. T. VOSS
- T. TAKESHITA
- T. TIC
- T. TODOROV
- T. TREFZGER
- T. VICKEY
- T. VU ANH
- T. W. JONES
- T. WENAUS
- T. WENGLER
- T. YAMAMURA
- T. YAMAZAKI
- T. Z. KOWALSKI
- T. ZENIS
- T. ZHAO
- T.H. D. PAPADOPOULOU
- U. BITENC
- U. BLUMENSCHEIN
- U. BRATZLER
- U. DE SANCTIS
- U. HUSEMANN
- U. K. YANG
- U. KLEIN
- U. KRUCHONAK
- U. LANDGRAF
- U. MALLIK
- U. PARZEFALL
- U. SCHAFER
- U. WERTHENBACH
- V. A. BEDNYAKOV
- V. A. GAPIENKO
- V. A. KANTSEROV
- V. A. KAZANIN
- V. A. KOROTKOV
- V. A. KRAMARENKO
- V. A. MITSOU
- V. A. SCHEGELSKY
- V. ANDREI
- V. B. VINOGRADOV
- V. BANSAL
- V. BARTHELD
- V. BOISVERT
- V. BOLDEA
- V. BUSCHER
- V. CANALE
- V. CASTILLO GIMENEZ
- V. CAVASINNI
- V. CHAVDA
- V. CHIARELLA
- V. CHIZHOV
- V. CINDRO
- V. D. PESHEKHONOV
- V. DAO
- V. E. OZCAN
- V. EREMIN
- V. F. CHEPURNOV
- V. FERRARA
- V. G. BONDARENKO
- V. G. ZAETS
- V. GALLO
- V. GARDE
- V. GARONNE
- V. GIAKOUMOPOULOU
- V. GIANGIOBBE
- V. GILEWSKY
- V. GOGGI
- V. GRABSKI
- V. GRASSI
- V. GRATCHEV
- V. HEDBERG
- V. I. RUD
- V. I. VASSILAKOPOULOS
- V. ISSAKOV
- V. IZZO
- V. J. GUARINO
- V. JAIN
- V. JURANEK
- V. KARTVELISHVILI
- V. KAUSHIK
- V. KHOVANSKIY
- V. KOLESNIKOV
- V. KORESHEV
- V. KRAL
- V. KUKHTIN
- V. KUS
- V. LENDERMANN
- V. M. KOTOV
- V. M. ROMANOV
- V. MALYSHEV
- V. MARTINEZ OUTSCHOORN
- V. MARTYNENKO
- V. MOELLER
- V. N. EVDOKIMOV
- V. N. GORYACHEV
- V. N. GUSHCHIN
- V. N. PANIN
- V. O'SHEA
- V. O. TIKHOMIROV
- V. P. MALEEV
- V. PAOLONE
- V. PEREZ REALE
- V. POLYCHRONAKOS
- V. R. LACUESTA
- V. RADEKA
- V. RADESCU
- V. ROJO
- V. ROSSETTI
- V. RUMIANTSEV
- V. RYADOVIKOV
- V. SAVINOV
- V. SIMAK
- V. SIPICA
- V. SMAKHTIN
- V. SOPKO
- V. TCHERNIATINE
- V. TSISKARIDZE
- V. TSULAIA
- V. V. AMMOSOV
- V. V. KABACHENKO
- V. V. KOSTYUKHIN
- V. V. LAPIN
- V. V. SULIN
- V. V. ZMOUCHKO
- V. VACEK
- V. VERCESI
- V. VOROBEL
- V. VORWERK
- V. VRBA
- V. ZAMBRANO
- V. ZHURAVLOV
- V. ZUTSHI
- VALENTINETTI SARA
- VILLA MAURO
- W. A. MANN
- W. B. QUAYLE
- W. BLUM
- W. CLELAND
- W. DABROWSKI
- W. DAVEY
- W. DENG
- W. EHRENFELD
- W. F. MADER
- W. FEDORKO
- W. FERNANDO
- W. G. PLANO
- W. G. SCOTT
- W. H. BELL
- W. IWANSKI
- W. J. MILLS
- W. J. MURRAY
- W. JI
- W. K. BROOKS
- W. KOZANECKI
- W. KUYKENDALL
- W. L. EBENSTEIN
- W. LAMPL
- W. LAU
- W. LAVRIJSEN
- W. LIEBIG
- W. M. YAO
- W. MOHR
- W. PARK
- W. QIAN
- W. S. LOCKMAN
- W. STILLER
- W. T. MEYER
- W. TAYLOR
- W. TRISCHUK
- W. VANDELLI
- W. VERKERKE
- W. WALKOWIAK
- W. WIEDENMANN
- W. WILLIS
- X. CHEN
- X. ESPINAL CURULL
- X. H. SUN
- X. LEI
- X. LI
- X. LOU
- X. PORTELL BUESO
- X. PRUDENT
- X. RUAN
- X. S. ANDUAGA
- X. WU
- X. ZHANG
- X. ZHUANG
- Y. A. KUROCHKIN
- Y. A. TIKHONOV
- Y. ARAI
- Y. AZUMA
- Y. B. PAN
- Y. BAI
- Y. BENHAMMOU
- Y. COADOU
- Y. D. TENNENBAUM KATAN
- Y. DOI
- Y. F. RYABOV
- Y. FANG
- Y. GUSAKOV
- Y. HASEGAWA
- Y. HERNANDEZ JIMENEZ
- Y. HOMMA
- Y. IKEGAMI
- Y. ILCHENKO
- Y. ISHIZAWA
- Y. ITOH
- Y. JIANG
- Y. KATAOKA
- Y. KULCHITSKY
- Y. LIU
- Y. MAHALALEL
- Y. MAKIDA
- Y. MING
- Y. MIYAZAKI
- Y. MORITA
- Y. MUNWES
- Y. NAGASAKA
- Y. OKUMURA
- Y. OREN
- Y. P. HE
- Y. PYLYPCHENKO
- Y. RODRIGUEZ GARCIA
- Y. ROZEN
- Y. S. GAO
- Y. SILVER
- Y. SMIRNOV
- Y. SUGAYA
- Y. SUZUKI
- Y. TAKAHASHI
- Y. TANAKA
- Y. TAYALATI
- Y. UNNO
- Y. V. GRISHKEVICH
- Y. XIE
- Y. YAMAZAKI
- Y. YANG
- Y. YAO
- Y. YASU
- Y. ZHOU
- Y. ZHU
- Y. ZOLNIEROWSKI
- Y.O. K. ZALITE
- Y.U. M. SVIRIDOV
- Z. CZYCZULA
- Z. D. GREENWOOD
- Z. DOLEZAL
- Z. DRASAL
- Z. HAJDUK
- Z. HUBACEK
- Z. KOHOUT
- Z. KOUPILOVA
- Z. L. REN
- Z. LIANG
- Z. MARSHALL
- Z. MENG
- Z. QIAN
- Z. QIN
- Z. RURIKOVA
- Z. TRKA
- Z. V. KRUMSHTEYN
- Z. VAN KESTEREN
- Z. YAN
- Z. YANG
- Z. ZAJACOVA
- Z. ZENONOS
- Z. ZHAN
- Z. ZHAO
- ZOCCOLI ANTONIO
- Publication venue
- Publication date
- 01/01/2012
- Field of study
Results are presented of a search for new particles decaying to large numbers of jets in association with missing transverse momentum, using 4.7 fbâ1 of pp collision data at sâ=7TeV collected by the ATLAS experiment at the Large Hadron Collider in 2011. The event selection requires missing transverse momentum, no isolated electrons or muons, and from â„6 to â„9 jets. No evidence is found for physics beyond the Standard Model. The results are interpreted in the context of a MSUGRA/CMSSM supersymmetric model, where, for large universal scalar mass m 0, gluino masses smaller than 840 GeV are excluded at the 95% confidence level, extending previously published limits. Within a simplified model containing only a gluino octet and a neutralino, gluino masses smaller than 870 GeV are similarly excluded for neutralino masses below 100 GeV
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- Author
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- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 31/12/2010
- Field of study
The inclusive and dijet production cross-sections have been measured for jets
containing b-hadrons (b-jets) in proton-proton collisions at a centre-of-mass
energy of sqrt(s) = 7 TeV, using the ATLAS detector at the LHC. The
measurements use data corresponding to an integrated luminosity of 34 pb^-1.
The b-jets are identified using either a lifetime-based method, where secondary
decay vertices of b-hadrons in jets are reconstructed using information from
the tracking detectors, or a muon-based method where the presence of a muon is
used to identify semileptonic decays of b-hadrons inside jets. The inclusive
b-jet cross-section is measured as a function of transverse momentum in the
range 20 < pT < 400 GeV and rapidity in the range |y| < 2.1. The bbbar-dijet
cross-section is measured as a function of the dijet invariant mass in the
range 110 < m_jj < 760 GeV, the azimuthal angle difference between the two jets
and the angular variable chi in two dijet mass regions. The results are
compared with next-to-leading-order QCD predictions. Good agreement is observed
between the measured cross-sections and the predictions obtained using POWHEG +
Pythia. MC@NLO + Herwig shows good agreement with the measured bbbar-dijet
cross-section. However, it does not reproduce the measured inclusive
cross-section well, particularly for central b-jets with large transverse
momenta.Comment: 10 pages plus author list (21 pages total), 8 figures, 1 table, final
version published in European Physical Journal
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
- Author
- Aad G
- Abbott B
- Abdallah J
- Abdelalim AA
- Abdesselam A
- Abdinov O
- Abi B
- Abolins M
- Abramowicz H
- Abreu H
- Acerbi E
- Acharya BS
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
- Ahlen SP
- Ahles F
- Ahmad A
- Ahsan M
- Aielli G
- Akdogana T
- Akesson TPA
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- Akimov AV
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- Aktas A
- Alam MA
- Alam MS
- Albert J
- Albrand S
- Aleksa M
- Aleksandrov IN
- Alessandria F
- Alexa C
- Alexander G
- Alexandre G
- Alexopoulos T
- Alhroob M
- Aliev M
- Alimonti G
- Alison J
- Aliyev M
- Allport PP
- Allwood-Spiers SE
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- Yilmaz M
- Yoosootiniya R
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- Yurkewicz A
- Zaets VG
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- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
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- Zeller M
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
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- Zhang Q
- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
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- Zhu CG
- Zhu H
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- Zhuang X
- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/03/2013
- Field of study
The jet energy scale and its systematic uncertainty are determined for jets measured with the ATLAS detector at the LHC in proton-proton collision data at a centre-of-mass energy of âs = 7TeV corresponding to an integrated luminosity of 38 pb-1. Jets are reconstructed with the anti-kt algorithm with distance parameters R=0. 4 or R=0. 6. Jet energy and angle corrections are determined from Monte Carlo simulations to calibrate jets with transverse momenta pTâ„20 GeV and pseudorapidities {pipe}η{pipe}<4. 5. The jet energy systematic uncertainty is estimated using the single isolated hadron response measured in situ and in test-beams, exploiting the transverse momentum balance between central and forward jets in events with dijet topologies and studying systematic variations in Monte Carlo simulations. The jet energy uncertainty is less than 2. 5 % in the central calorimeter region ({pipe}η{pipe}<0. 8) for jets with 60â€pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2â€{pipe}η{pipe}<4. 5. The jet energy is validated for jet transverse momenta up to 1 TeV to the level of a few percent using several in situ techniques by comparing a well-known reference such as the recoiling photon pT, the sum of the transverse momenta of tracks associated to the jet, or a system of low-pT jets recoiling against a high-pT jet. More sophisticated jet calibration schemes are presented based on calorimeter cell energy density weighting or hadronic properties of jets, aiming for an improved jet energy resolution and a reduced flavour dependence of the jet response. The systematic uncertainty of the jet energy determined from a combination of in situ techniques is consistent with the one derived from single hadron response measurements over a wide kinematic range. The nominal corrections and uncertainties are derived for isolated jets in an inclusive sample of high-pT jets. Special cases such as event topologies with close-by jets, or selections of samples with an enhanced content of jets originating from light quarks, heavy quarks or gluons are also discussed and the corresponding uncertainties are determined. © 2013 CERN for the benefit of the ATLAS collaboration
Observation of associated near-side and away-side long-range correlations in âsNN=5.02ââTeV proton-lead collisions with the ATLAS detector
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- Yilmaz M
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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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- Zhuravlov V
- Zibell A
- Zieminska D
- Zimin NI
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
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- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zur Nedden M
- Zutshi V
- 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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