659 research outputs found
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
- 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
- Ackers M
- Adams DL
- Addy TN
- Adelman J
- Aderholz M
- Adomeit S
- Adragna P
- Adye T
- Aefsky S
- Aguilar-Saavedra JA
- Aharrouche M
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- Zwalinski L
- 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
- Akimoto G
- Akimov AV
- Akiyama A
- 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
- Almenar CC
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- Aloisio A
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- Yoosootiniya R
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- Zhemchugov A
- Zheng S
- Zhong J
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- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
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- Zinonos Z
- Ziolkowski M
- Zitoun R
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- 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 √s = 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 pT≥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 60≤pT<800 GeV, and is maximally 14 % for pT<30 GeV in the most forward region 3. 2≤{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
Performance of the CMS Cathode Strip Chambers with Cosmic Rays
- Author
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- Wilson J. A.
- Wilson M. G.
- Wimpenny S
- Wingerter-Seez I.
- Wingham M
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- Witherell M
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- Wlochal M
- Wohri HK
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- Wolter M. W.
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- Womersley WJ
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- Wood JS
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- Wraight K.
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- Wrochna G
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- Wulf E.
- Wulz CE
- Wurthwein F
- Wynne B. M.
- Wyslouch B
- Xaplanteris L.
- Xella S.
- Xie S
- Xie S.
- Xie Z
- Xu D.
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- Yagil A
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- Yamamoto A
- Yan M
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- Yarba J
- Yaselli I
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- Yi K
- Yilmaz Y
- Yohay R
- Yoo HD
- Yoon AS
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- Yumiceva F
- Yun JC
- Yuste C
- Zabi A
- Zabolotny W
- Zachariadou A
- Zalewski P
- Zampieri A
- Zanetti M
- Zang SL
- Zarubin A
- Zatzerklyany A
- Zeidler C
- Zeinali M
- Zeise M
- Zelepoukine S
- Zeuner WD
- Zeyrek M
- Zhang J
- Zhang L
- Zhang Y
- Zhang Z
- Zheng Y
- Zhiltsov V
- Zhokin A
- Zhu B
- Zhu K
- Zhu RY
- Zhukov V
- Zhukova V
- Ziebarth EB
- Zielinski M
- Zilizi G
- Zinonos Z
- Zito G
- Zoeller MH
- Zotto P
- Zub S
- Zumerle G
- Zuranski A
- Zuyeuski R
- Zych P
- Publication venue
- 'IOP Publishing'
- Publication date
- 01/01/2009
- Field of study
The Cathode Strip Chambers (CSCs) constitute the primary muon tracking device
in the CMS endcaps. Their performance has been evaluated using data taken
during a cosmic ray run in fall 2008. Measured noise levels are low, with the
number of noisy channels well below 1%. Coordinate resolution was measured for
all types of chambers, and fall in the range 47 microns to 243 microns. The
efficiencies for local charged track triggers, for hit and for segments
reconstruction were measured, and are above 99%. The timing resolution per
layer is approximately 5 ns
Proteome from patients with metabolic syndrome is regulated by quantity and quality of dietary lipids
- Author
- A Alipour
- A Caimari
- A Camargo
- A Camargo
- A Gorg
- A Muñoz
- AD Peairs
- AK Perry
- Antonio Camargo
- AT Hastie
- B Garcia-Alvarez
- BJ Webb-Robertson
- C Cruz-Teno
- C Phillips
- C Richard
- Carmen Marin
- CC Allain
- CJ Briggs
- CM Lin
- CM Redman
- D Fuchs
- DA Jones
- DI Shaw
- DR Stauffer
- E Marchlik
- Elena M. Yubero-Serrano
- F D’Acquisto
- Francisco J. Tinahones
- Francisco Pérez-Jiménez
- G Bucolo
- G Chiva-Blanch
- GH Li
- Helen M. Roche
- HJ Chen
- I Palomo
- J López-Miranda
- J Skoble
- J Skrha
- Javier Delgado-Lista
- JF Swisher
- José López-Miranda
- L Gewin
- Lorena González-Guardia
- M Bouwens
- M Bouwens
- M Hernández-Presa
- M Matsuda
- M Ni
- M Redondo
- M Yamakami
- M Yamakami
- María M. Malagón
- MD Welch
- MF Gregor
- MR Bennett
- MS Cooke
- Oriol Alberto Rangel-Zúñiga
- P Hu
- P Perez-Martinez
- P Perez-Martinez
- Pablo Pérez-Martínez
- Patricia Peña-Orihuela
- R Estruch
- RA Milligan
- RC Piper
- S Averaimo
- S Grundy
- SE Calvano
- SM Grundy
- T Fulop
- U Rescher
- W Roberts
- WT Friedewald
- X Xie
- Y Murakumo
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Background: Metabolic syndrome is a multi-component disorder associated to a high risk of cardiovascular disease.
Its etiology is the result of a complex interaction between genetic and environmental factors, including dietary
habits. We aimed to identify the target proteins modulated by the long-term consumption of four diets differing in
the quality and quantity of lipids in the whole proteome of peripheral blood mononuclear cells (PBMC).
Results: A randomized, controlled trial conducted within the LIPGENE study assigned 24 MetS patients for 12 weeks
each to 1 of 4 diets: a) high-saturated fatty acid (HSFA), b) high-monounsaturated fatty acid (HMUFA), c) low-fat,
high-complex carbohydrate diets supplemented with placebo (LFHCC) and d) low-fat, high-complex carbohydrate
diets supplemented with long chain (LC) n-3 polyunsaturated fatty acids (PUFA) (LFHCC n-3). We analyzed the
changes induced in the proteome of both nuclear and cytoplasmic fractions of PBMC using 2-D proteomic analysis.
Sixty-seven proteins were differentially expressed after the long-term consumption of the four diets. The HSFA diet
induced the expression of proteins responding to oxidative stress, degradation of ubiquitinated proteins and DNA
repair. However, HMUFA, LFHCC and LFHCC n-3 diets down-regulated pro-inflammatory and oxidative stress-related
proteins and DNA repairing proteins.
Conclusion: The long-term consumption of HSFA, compared to HMUFA, LFHCC and LFHCC n-3, seems to increase the
cardiovascular disease (CVD) risk factors associated with metabolic syndrome, such as inflammation and oxidative stress,
and seem lead to DNA damage as a consequence of high oxidative stress
2 nd Brazilian Consensus on Chagas Disease, 2015
- Author
- Abad-Franch F
- Abad-Franch F
- Abad-Franch F
- Abad-Franch F
- Abad-Franch F
- Abílio Augusto Fragata Filho
- Acquatella H
- Akhavan D
- Alberto Novaes Ramos Jr.
- Alejandro Luquetti
- Alejandro Marcel Hasslocher-Moreno
- Alessandra Viana Cardoso
- Almeida EA
- Almeida EA
- Almeida EA
- Almeida EA
- Almeida-Filho OC
- Altclas J
- Altclas JD
- Alves RM
- Ana Maria Jansen
- Ana Yecê das Neves Pinto
- Andrade AL
- Andrade SG
- Andréa Silvestre de Sousa
- Angheben A
- Anis Rassi
- Anis Rassi Jr.
- Antonio Walter Ferreira
- Antônio Carlos Silveira
- Barcán L
- Baroldi G
- Barreto ML
- Bern C
- Bern C
- Bern C
- Bern C
- Bern C
- Bestetti RB
- Bestetti RB
- Bestetti RB
- Bitto C
- Bocchi EA
- Bocchi EA
- Bocchi EA
- Brener Z
- Brener Z
- Britto CC
- Brutus L
- Brücher BL
- Bua J
- Buekens P
- Camargo ME
- Camargo ME
- Camargo ME
- Camargo ME
- Campos SV
- Cançado JR
- Carlier Y
- Carlier Y
- CarlierI Y
- Carrasco HA
- Carvalho VB
- Castro AM
- Castro CN
- Castro I
- Cerisola JA
- Cerisola JA
- Chagas C
- Chiale PA
- Chiari E
- Chiari E
- Chiari E
- Chippaux JP
- Constança Felícia De Paoli de Carvalho Britto
- Cordova E
- Coura JR
- Coura JR
- Coura JR
- Coura JR
- Coura JR
- Coura JR
- Coura JR
- Cunha GP
- D'Albuquerque LA
- Dalmo Correia
- Davila DF
- Dayse Elisabeth Campos
- De Rissio AM
- Del Castilho M
- Dias E
- Dias JC
- Dias JC
- Dias JC
- Dias JC
- Dias JCP
- Dias JCP
- Dias JCP
- Dias JCP
- Dias JCP
- Dias JCP
- Dias JCP
- Dias JCP
- Dias JCP
- Dias JP
- Divina Seila de Oliveira Marques
- Drumond JAG
- Duhamel B
- Egler Chiari
- Eliane Dias Gontijo
- Eliane Furtado Moreira
- Eliane Lages Silva
- Eros Antonio de Almeida
- Fabbro DL
- Fabiane Scalabrini Pinto
- Ferguson MK
- Fernando Abad-Franch
- Ferreira AW
- Ferreira HO
- Ferreira HO
- Ferreira MS
- Fonseca FM
- Fragata Filho AA
- França LCM
- Freilij H
- Freitas H
- Freitas VL
- Gallerano RH
- Garcia S
- Garzon SA
- Gebrekristos HT
- Glaucia Manzan Queiroz Andrade
- Gontijo ED
- González-Tomé MI
- Guariento ME
- Heller E
- Herwaldt BL
- Higuchi ML
- Higuchi ML
- Higuchi ML
- Hijar G
- Hotez PJ
- Hotez PJ
- Howard EJ
- Ianni BM
- Inoue H
- Joffre Marcondes de Rezende
- José Antonio Marin-Neto
- José Renan da Cunha Melo
- José Rodrigues Coura
- João Carlos Pinto Dias
- Junqueira AC
- Jörg ME
- Júnior Rassi A
- Lana M
- Leeuwenburgh I
- Lima-Costa MF
- Livramento JA
- Lopes ER
- Lorosa ES
- Lugones HS
- Luquetti AO
- Luquetti AO
- Luquetti AO
- Luquetti AO
- Lúcia Maria da Cunha Galvão
- Macêdo VO
- Macêdo VO
- Mady C
- Maegawa FA
- Maguire JH
- Mahoney RT
- Mallimaci MC
- Maria Aparecida Shikanai-Yasuda
- Marin-Neto JA
- Marin-Neto JA
- Marin-Neto JA
- Marin-Neto JA
- Marin-Neto JA
- Martes ACB
- Martinelli Filho M
- Martins-Melo FR
- Martins-Melo FR
- Martins-Melo FR
- Martins-Melo FR
- Martins-Melo FR
- Martins-Melo FR
- Martins-Melo FR
- Mayara Maia Lima
- Medeiros MB
- Meier-Ruge WA
- Mendes EV
- Messenger LA
- Molina I
- Moncayo A
- Montera MW
- Moraes-Souza H
- Morais BB
- Morillo CA
- Mougabure-Cueto G
- Nishioka SA
- Nisida IV
- Norman FF
- Noya BA
- Noêmia Barbosa Carvalho
- Nóbrega AA
- Nóbrega AA
- Oliveira Júnior W
- Oliveira Júnior W
- Oliveira RB
- Ostermayer AL
- Ozaki Y
- Padilla-Torres SD
- Parada H
- Pasricha PJ
- Passos ADC
- Pazin-Filho A
- Pereira Barretto AC
- Perez-Ramirez L
- Pessoa GCA
- Pessoa GCA
- Pinazo MJ
- Pinotti HW
- Pinto AY
- Pinto AY
- Pinto AYN
- Pinto AYN
- Pinto AYN
- Portela-Lindoso AAB
- Porto CC
- Prata A
- Prata A
- Prata A
- Prata A
- Pérez-Ayala A
- Pérez-Molina JA
- Rafaella Albuquerque e Silva
- Ramos G
- Ramos Júnior AN
- Ramos Júnior AN
- Ramos Júnior AN
- Rassi A
- Rassi A
- Rassi Jr A
- Rassi Júnior A
- Rassi Júnior A
- Rassi Júnior A
- Rassi Júnior A
- Rassi Júnior A
- Reis-Neto JA
- Renato Vieira Alves
- Requena-Méndez A
- Rezende JM
- Riarte A
- Ribeiro dos Santos R
- Roberti RR
- Rocha A
- Rocha MOC
- Rodriguez-Salas LA
- Romaña C
- Roque AL
- Roque AL
- Rosália Morais Torres
- Roux E
- Roux E
- Russomando G
- Salas NA
- Salvatella R
- Samuel J
- Sangenis LH
- Santo AH
- Santos CB
- Sartori AM
- Scanavacca M
- Scapellato PG
- Schijman AG
- Schmunis GA
- Sebastião Aldo da Silva Valente
- Sergio Salles Xavier
- Shaw J
- Shikanai-Yasuda MA
- Shikanai-Yasuda MA
- Shikanai-Yasuda MA
- Silva CP
- Silvana Eloi Santos
- Silveira AC
- Silveira AC
- Silveira AC
- Silveira C
- Silveira JF
- Simone Monzani Vivaldini
- Simões MV
- Sosa Estani S
- Sosa-Estani S
- Sousa AA
- Sousa AS
- Souza DSM
- Spiess AE
- Spina-França A
- Stavropoulos SN
- Strasen J
- Suelene Mamede Oliveira
- Swanstrom LL
- Sánchez-Camargo CL
- Torrico F
- Valença-Barbosa C
- Ventura-Garcia L
- Vera da Costa Valente
- Veruska Maia da Costa
- Victora CG
- Victora CG
- Villela E
- Vinhaes MC
- Viotti R
- Viotti R
- Viotti RJ
- Voller A
- Wendell S
- Wilson de Oliveira Jr.
- Xavier SC
- Xavier SC
- Xavier SS
- Xavier SS
- Yun O
- Zicker F
- Zimerman LI
- Zingales B
- Zingales B
- Publication venue
- 'FapUNIFESP (SciELO)'
- Publication date
- 01/01/2016
- Field of study
Abstract Chagas disease is a neglected chronic condition with a high burden of morbidity and mortality. It has considerable psychological, social, and economic impacts. The disease represents a significant public health issue in Brazil, with different regional patterns. This document presents the evidence that resulted in the Brazilian Consensus on Chagas Disease. The objective was to review and standardize strategies for diagnosis, treatment, prevention, and control of Chagas disease in the country, based on the available scientific evidence. The consensus is based on the articulation and strategic contribution of renowned Brazilian experts with knowledge and experience on various aspects of the disease. It is the result of a close collaboration between the Brazilian Society of Tropical Medicine and the Ministry of Health. It is hoped that this document will strengthen the development of integrated actions against Chagas disease in the country, focusing on epidemiology, management, comprehensive care (including families and communities), communication, information, education, and research
LRRK2 Biology from structure to dysfunction: research progresses, but the themes remain the same
- Author
- A Abeliovich
- A Beilina
- A Elbaz
- A Gardet
- A Grunewald
- A Kumar
- A Mamais
- A Salasova
- A Schaffner
- A Trancikova
- A Trancikova
- A Witoelar
- A Zimprich
- A Zimprich
- AB West
- AB West
- AH Schapira
- AJ Schwab
- AM Arranz
- AM Schreij
- B Dehay
- B Kim
- BA Matikainen-Ankney
- BJ Ryan
- BM Law
- C Bedford
- C Manzoni
- C Manzoni
- C Manzoni
- C Manzoni
- C Paisan-Ruiz
- C Stark
- C Tapia-Rojas
- C van der Merwe
- C Vilarino-Guell
- CC Ho
- CE Krebs
- CH Hsieh
- CH Hsu
- CH Hsu
- CH Lin
- CH Ng
- CJ Gloeckner
- CJ Gloeckner
- CL Klein
- D Chan
- D Perdiz
- D Wang
- DA Beccano-Kelly
- DA MacLeod
- Daniel C. Berwick
- DC Angeles
- DC Angeles
- DC Berwick
- DC Berwick
- DC Berwick
- DC Berwick
- DC Berwick
- DD Feng
- DL Moore
- DS Schwarz
- E Deyaert
- E Lobbestael
- E Ohta
- E Purlyte
- E Schurr
- E Ungewickell
- ED Plowey
- Elisa Greggio
- Emilie Giaime
- ES Sweet
- F Cicchetti
- F Kawakami
- F Kawakami
- F L'Episcopo
- FR Zhang
- G Guaitoli
- G Piccoli
- George R. Heaton
- H Houlden
- H Jia
- H Mortiboys
- HJ Cho
- HJ Yun
- HL Melrose
- HL Melrose
- HN Nguyen
- I Agalliu
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- S Bandres-Ciga
- S Biskup
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- S Gehrke
- S Kaushik
- S Matta
- S Saez-Atienzar
- S Sen
- S Tsujii
- S Werner
- SF Soukup
- SJ Cherra 3rd
- SJ Cherra 3rd
- SJ Orenstein
- SK Kalia
- Sonia Azeggagh
- SR Pfeffer
- T Eguchi
- T Kuwahara
- TB Sherer
- TM Dawson
- V Kumar
- VF Taelman
- VK Godena
- X Li
- X Li
- Y Imai
- Y Imai
- Y Li
- Y Ma
- Y Tong
- Y Tong
- Y Xiong
- Y Yuan
- Z Berger
- Z Gan-Or
- Z Liu
- Z Liu
- Z Sheng
- Z Wang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2019
- Field of study
Since the discovery of leucine-rich repeat kinase 2 (LRRK2) as a protein that is likely central to the aetiology of Parkinson's disease, a considerable amount of work has gone into uncovering its basic cellular function. This effort has led to the implication of LRRK2 in a bewildering range of cell biological processes and pathways, and probable roles in a number of seemingly unrelated medical conditions. In this review we summarise current knowledge of the basic biochemistry and cellular function of LRRK2. Topics covered include the identification of phosphorylation substrates of LRRK2 kinase activity, in particular Rab proteins, and advances in understanding the activation of LRRK2 kinase activity via dimerisation and association with membranes, especially via interaction with Rab29. We also discuss biochemical studies that shed light on the complex LRRK2 GTPase activity, evidence of roles for LRRK2 in a range of cell signalling pathways that are likely cell type specific, and studies linking LRRK2 to the cell biology of organelles. The latter includes the involvement of LRRK2 in autophagy, endocytosis, and processes at the trans-Golgi network, the endoplasmic reticulum and also key microtubule-based cellular structures. We further propose a mechanism linking LRRK2 dimerisation, GTPase function and membrane recruitment with LRRK2 kinase activation by Rab29. Together these data paint a picture of a research field that in many ways is moving forward with great momentum, but in other ways has not changed fundamentally. Many key advances have been made, but very often they seem to lead back to the same places
Search for Supersymmetry with Gauge-Mediated Breaking in Diphoton Events with Missing Transverse Energy at CDF II
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- Publication venue
- Publication date
- 01/01/2010
- Field of study
accepted to Phys. Rev. LettWe present the results of a search for supersymmetry with gauge-mediated breaking and \NONE\to\gamma\Gravitino in the γγ+missing transverse energy final state. In 2.6±0.2 \invfb of ppˉ collisions at s=1.96 TeV recorded by the CDF II detector we observe no candidate events, consistent with a standard model background expectation of 1.4±0.4 events. We set limits on the cross section at the 95% C.L. and place the world's best limit of 149\gevc on the \none mass at τχ~10$We present the results of a search for supersymmetry with gauge-mediated breaking and χ˜10→γG˜ in the γγ+missing transverse energy final state. In 2.6±0.2 fb-1 of pp̅ collisions at √s=1.96 TeV recorded by the CDF II detector we observe no candidate events, consistent with a standard model background expectation of 1.4±0.4 events. We set limits on the cross section at the 95% C.L. and place the world’s best limit of 149 GeV/c2 on the χ˜10 mass at τχ˜10≪1 ns. We also exclude regions in the χ˜10 mass-lifetime plane for τχ˜10≲2 ns.Peer reviewe
Measurements of branching fraction ratios and CP asymmetries in B+/- ->D_CP K+/- decays in hadron collisions
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- Ttito Guzman P
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- Yun JC
- Zanetti A
- Zeng Y
- Zhang X
- Zheng Y
- Zucchelli Selli S. Zheng Y
- Zucchelli Sos D. Lopez
- Publication venue
- Publication date
- 05/11/2009
- Field of study
We reconstruct B+/- -> D K+/- decays in a data sample collected by the CDF II detector at the Tevatron collider corresponding to 1 fb-1 of integrated luminosity. We select decay modes where the D meson decays to either K- pi+ (flavor eigenstate) or K- K+, pi- pi+ (CP-even eigenstates), and measure the direct CP asymmetry A_CP+ = 0.39 +/- 0.17(stat) +/- 0.04(syst), and the double ratio of CP-even to flavor eigenstate branching fractions R_CP+ = 1.30 +/- 0.24(stat) +/- 0.12(syst). These measurements will improve the determination of the CKM angle gamma. They are performed here for the first time using data from hadron collisions.We reconstruct B±→DK± decays in a data sample collected by the CDF II detector at the Tevatron collider corresponding to 1 fb-1 of integrated luminosity. We select decay modes where the D meson decays to either K-π+ (flavor eigenstate) or K-K+, π-π+ (CP-even eigenstates), and measure the direct CP asymmetry ACP+=0.39±0.17(stat)±0.04(syst), and the double ratio of CP-even to flavor eigenstate branching fractions RCP+=1.30±0.24(stat)±0.12(syst). These measurements will improve the determination of the Cabibbo-Kobayashi-Maskawa angle γ. They are performed here for the first time using data from hadron collisions.Peer reviewe
A922 Sequential measurement of 1 hour creatinine clearance (1-CRCL) in critically ill patients at risk of acute kidney injury (AKI)
- Author
- Abbott TE
- Abdallah RI
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- Japan Septic Disseminated Intravascular Coagulation (JSEPTIC DIC) study group
- Jardim JJ
- Jardim M
- Jareño A
- Javadpour S
- Jayasinghe S
- Jean-Baptiste S
- Jean-Baptiste S
- Jensen AE
- Jensen JU
- Jeon YD
- Jeon YD
- Jeong IY
- Jeong IY
- Jeong WY
- Jeong WY
- Jian Z
- Jiao LR
- Jibaja M
- Jimenez-Herrera MF
- Jiménez GJ
- Jo YH
- Joachim J
- Jochmans S
- John G
- Jonas M
- Jonas M
- Jonas M
- Jones C
- Joshi R
- Joshi V
- Jovaisa T
- JSEPTIC (Japanese Society of Education for Physicians and Trainees in Intensive Care) Clinical Trial Group
- Juan WC
- Juanas CA
- Judickas S
- Juez A
- Juliarena A
- Jun IG
- Jun IG
- Jung K
- Jung KW
- Junior JM
- Kaczirek K
- Kaese S
- Kalani N
- Kalenka A
- Kalfon P
- Kamali E
- Kaminsky GE
- Kaneko M
- Kang M
- Kang M
- Kang PL
- Kang PL
- Kang PL
- Kang PL
- Kang Y
- Kao KC
- Kappler F
- Kara A
- Karachi F
- Karanjia N
- Karbing DS
- Karsten E
- Kasdan H
- Kashiya S
- Kashyap R
- Katabami K
- Katabami K
- Katabami K
- Katabami K
- Katira BH
- Kavanagh BP
- Kawamura N
- Kawano S
- Kay FU
- Kayaaslan B
- Kayambu G
- Kazutoshi F
- Ke MW
- Ke MW
- Keep J
- Keep J
- Keller E
- Kellner F
- Kelly JM
- Kenardy J
- Keough E
- Kerhuel L
- Kerr C
- Kezyte G
- Khadjibaev A
- Khaliq W
- Khine H
- Kim DJ
- Kim HJ
- Kim JM
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- Kim JW
- Kim KS
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- Kim KS
- Kim MH
- Kim MH
- Kim W
- Kimmoun A
- King HS
- Kinnear J
- Kirakli C
- Kirakli C
- Kirca H
- Kirman M
- Kirwan CJ
- Kittnar O
- Klapsing P
- Klaus DA
- Kleinpell R
- Kluge S
- Knafelj R
- Knight LD
- Ko JI
- Ko SB
- Kobayashi A
- Koco E
- Kodate A
- Kodate A
- Kodate A
- Kokkini S
- Kolnikova I
- Komuro T
- Kondili E
- Kongpolprom N
- Kooner G
- Kostalas M
- Kosuk ME
- Kotsopoulos A
- Kou PS
- Kouatchet A
- Kovacikova L
- Kox M
- Kraegpoeth A
- Krenn CG
- Krishna B
- Kristof J
- Kruger A
- Kruger A
- Krüger A
- Ku NS
- Ku NS
- Kubik M
- Kubota K
- Kuebler WM
- Kulaga EV
- Kulkarni AP
- Kumari BK
- Kumbamu A
- Kunze-Szikszay N
- Kurmukov IA
- Kurth T
- Kurtz P
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- Kwon HM
- Kwon HM
- Kwon WY
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- Kye YC
- Kyle UG
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- Labaune MA
- Labra C
- Lacerda P
- Laerkner E
- Lafaurie M
- Lafuente E
- Lagonidis D
- Lagos R
- Lahmer T
- Lai CC
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- Lapteva K
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- Larsson JS
- Latini R
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- Latini R
- Latorre J
- Lattuada M
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- Lau YH
- Laurent A
- Lauretta MP
- Laureys S
- Lavrentieva A
- Lawrence N
- Lazzeri EH
- Le Brocque R
- Lebherz-Eichinger D
- Lebiedz P
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- Lebut J
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- Legrand M
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- Leonard H
- Leone M
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- Lerma FA
- Lesmes SP
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- Letizia T
- Levrat Q
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- Li SH
- Liao X
- Lichtenstein D
- Lim TH
- Limuti R
- Lin KC
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- Lin WC
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- Lipcsey M
- Lischinsky A
- Lissonde F
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- Litchfield K
- Liu CP
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- Liu D
- Llaurado-Serra M
- Llorente B
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- Longhi L
- Lopes JA
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- Lortat-Jacob B
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- Ly H
- Lázaro AS
- López AR
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- Macfarlane B
- MacKay A
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- Mackey G
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- Macrì M
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- Maekawa K
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- Maertens B
- Maggiorini M
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- Magnanimi E
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- Mainardi JL
- Maistry N
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- Mezidi M
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- Mimoz O
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- Olaechea P
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- Revel N
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- Stretti F
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- Álvarez JT
- Álvarez-Lerma F
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2016
- Field of study
Meeting abstrac
Inclusive Search for Standard Model Higgs Boson Production in the WW Decay Channel using the CDF II Detector
- Author
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- Publication venue
- Publication date
- 01/01/2010
- Field of study
We present a search for standard model (SM) Higgs boson production using ppbar collision data at sqrt(s) = 1.96 TeV, collected with the CDF II detector and corresponding to an integrated luminosity of 4.8 fb-1. We search for Higgs bosons produced in all processes with a significant production rate and decaying to two W bosons. We find no evidence for SM Higgs boson production and place upper limits at the 95% confidence level on the SM production cross section (sigma(H)) for values of the Higgs boson mass (m_H) in the range from 110 to 200 GeV. These limits are the most stringent for m_H > 130 GeV and are 1.29 above the predicted value of sigma(H) for mH = 165 GeV.We present a search for standard model (SM) Higgs boson production using pp̅ collision data at √s=1.96 TeV, collected with the CDF II detector and corresponding to an integrated luminosity of 4.8 fb-1. We search for Higgs bosons produced in all processes with a significant production rate and decaying to two W bosons. We find no evidence for SM Higgs boson production and place upper limits at the 95% confidence level on the SM production cross section (σH) for values of the Higgs boson mass (mH) in the range from 110 to 200 GeV. These limits are the most stringent for mH>130 GeV and are 1.29 above the predicted value of σH for mH=165 GeV.Peer reviewe
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