732 research outputs found
Molecular Characterization of the Gastrula in the Turtle Emys orbicularis: An Evolutionary Perspective on Gastrulation
- Author
- A Perea-Gomez
- A Simeone
- AJ Levine
- Arnaud Menuet
- Aurélie Gombault
- C Viebahn
- CD Stern
- CD Stern
- CL Peichel
- CL Yntema
- Claude Pieau
- D Acampora
- D Arendt
- Daphne Soares
- Delphine Nicolle
- DG Wilkinson
- E Gilland
- EM del Pino
- G Guyot
- H Ibrahim
- H Meinhardt
- H Meinhardt
- IM Moya
- J Pasteels
- JA Gauthier
- JC Smith
- JD Barnes
- Jean-Louis Plouhinec
- JH Fritzenwanker
- JL Plouhinec
- L Bally-Cuif
- M Chandrasekharan Nayar
- M Coolen
- M Dorizzi
- M Pannese
- M Rhinn
- M Rhinn
- M Taira
- M Taira
- Marion Coolen
- Mitsukuri
- MW Nachman
- O Voiculescu
- PW Holland
- R Keller
- R Vignali
- S Schulte-Merker
- SC Chapman
- Sylvie Mazan
- T Sauka-Spengler
- Tatjana Sauka-Spengler
- V Knezevic
- W Shawlot
- Y Kraus
- Publication venue
- 'Public Library of Science (PLoS)'
- Publication date
- 01/01/2008
- Field of study
Due to the presence of a blastopore as in amphibians, the turtle has been suggested to exemplify a transition form from an amphibian- to an avian-type gastrulation pattern. In order to test this hypothesis and gain insight into the emergence of the unique characteristics of amniotes during gastrulation, we have performed the first molecular characterization of the gastrula in a reptile, the turtle Emys orbicularis. The study of Brachyury, Lim1, Otx2 and Otx5 expression patterns points to a highly conserved dynamic of expression with amniote model organisms and makes it possible to identify the site of mesoderm internalization, which is a long-standing issue in reptiles. Analysis of Brachyury expression also highlights the presence of two distinct phases, less easily recognizable in model organisms and respectively characterized by an early ring-shaped and a later bilateral symmetrical territory. Systematic comparisons with tetrapod model organisms lead to new insights into the relationships of the blastopore/blastoporal plate system shared by all reptiles, with the blastopore of amphibians and the primitive streak of birds and mammals. The biphasic Brachyury expression pattern is also consistent with recent models of emergence of bilateral symmetry, which raises the question of its evolutionary significance
Frequency of Fabry disease in male and female haemodialysis patients in Spain
- Author
- A Sessa
- Carlos F Andrade
- CM Eng
- Daniel Rodrigues
- ED Shelley
- EM Maier
- GE Linthorst
- Gerardo Torres
- H Morita
- J Shabbeer
- Juan Macias
- Julio Herrera
- L Monserrat
- M Elleder
- M Fukushima
- M Merta
- M Spada
- M Yasuda
- Maria C Sá-Miranda
- Maria D del Pino
- Maria D Prados
- P Kotanko
- P Morais
- Paulo Gaspar
- Pedro Vidau
- Pilar R de Alegria
- PJ Meikle
- R Froissart
- R Pinto
- R Schiffmann
- Ramón Forascepi
- RJ Desnick
- RJ Desnick
- Rodrigo Delgado
- S Nakao
- S Nakao
- Sebastián Cerezo
- W Von Scheidt
- Y Nagao
- Publication venue
- BioMed Central
- Publication date
- 01/01/2010
- Field of study
<p>Abstract</p> <p>Background</p> <p>Fabry disease (FD), an X-linked lysosomal storage disorder, is caused by a reduced activity of the lysosomal enzyme α-galactosidase A. The disorder ultimately leads to organ damage (including renal failure) in males and females. However, heterozygous females usually present a milder phenotype with a later onset and a slower progression.</p> <p>Methods</p> <p>A combined enzymatic and genetic strategy was used, measuring the activity of α-galactosidase A and genotyping the α-galactosidase A gene (<it>GLA</it>) in dried blood samples (DBS) of 911 patients undergoing haemodialysis in centers across Spain.</p> <p>Results</p> <p><it>GLA </it>alterations were found in seven unrelated patients (4 males and 3 females). Two novel mutations (p.Gly346AlafsX347 and p.Val199GlyfsX203) were identified as well as a previously described mutation, R118C. The R118C mutation was present in 60% of unrelated patients with <it>GLA </it>causal mutations. The D313Y alteration, considered by some authors as a pseudo-deficiency allele, was also found in two out of seven patients.</p> <p>Conclusions</p> <p>Excluding the controversial D313Y alteration, FD presents a frequency of one in 182 individuals (0.55%) within this population of males and females undergoing haemodialysis. Moreover, our findings suggest that a number of patients with unexplained and atypical symptoms of renal disease may have FD. Screening programmes for FD in populations of individuals presenting severe kidney dysfunction, cardiac alterations or cerebrovascular disease may lead to the diagnosis of FD in those patients, the study of their families and eventually the implementation of a specific therapy.</p
Search for new phenomena in final states with an energetic jet and large missing transverse momentum in pp collisions at √ s = 8 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov A
- Al Khoury K
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alvarez Estevez M
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
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- Anastopoulos C
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- Anders CF
- Anders JK
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
- Antel C
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- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
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- Araya ST
- Arcangeletti C
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- Armbruster AJ
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- Atkin RJ
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- Bachacou H
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- Backes M
- Backman F
- Bagnaia P
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- Bahrasemani H
- Bailey AJ
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- Baines JT
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- Bakker PJ
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- Schmoeckel JC
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- Schoening A
- Scholer PG
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- Schroeder TV
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- Sebastiani CD
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- Thorpe EJ
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- Tobon CAM
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- Trincaz-Duvoid S
- Trischuk DA
- Trischuk W
- Trocme B
- Trofymov A
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- Trzebinski M
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- Tseng JC-L
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- Tsirigotis A
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- Tskhadadze EG
- Tsopoulou M
- Tsukerman II
- Tsulaia V
- Tsuno S
- Tsybychev D
- Tu Y
- Tudorache A
- Tudorache V
- Tulbure TT
- Tuna AN
- Turchikhin S
- Turgeman D
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- Van Vulpen I
- Vanadia M
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- Vandewall ER
- Vaniachine A
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- Varnes EW
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- Vasquez GA
- Vazeille F
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- Vazquez CJB
- Vazquez JGP
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- Viehhauser GHA
- Vigani L
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- Vilucchi E
- Vincter MG
- Virdee GS
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- Vivarelli I
- Vogel M
- Vokac P
- von Buddenbrock SE
- Von Toerne E
- Vorobel V
- Vorobev K
- Vos M
- Vossebeld JH
- Vozak M
- Vranjes N
- Vrba V
- Vreeswijk M
- Vuillermet R
- Vukotic I
- Wagner P
- Wagner W
- Wagner-Kuhr J
- Wahdan S
- Wahlberg H
- Walbrecht VM
- Walder J
- Walker R
- Walker SD
- Walkowiak W
- Wallangen V
- Wang AM
- Wang AZ
- Wang C
- Wang F
- Wang H
- Wang J
- Wang P
- Wang Q
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- Wang R-J
- Wang SM
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- Wang WT
- Wang WX
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- Warburton A
- Ward CP
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- Washbrook A
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- Webb AF
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- Weidberg AR
- Weingarten J
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- Wenig S
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- Werner MD
- Wessels M
- Weston TD
- Whalen K
- Whallon NL
- Wharton AM
- White A
- White AS
- White MJ
- Whiteson D
- Whitmore BW
- Wiedenmann W
- Wiel C
- Wielers M
- Wieseotte N
- Wiglesworth C
- Wiik-Fuchs LAM
- Wilkens HG
- Wilkins LJ
- Williams HH
- Williams S
- Willis C
- Willocq S
- Wingerter-Seez I
- Winkels E
- Winklmeier F
- Winston OJ
- Winter BT
- Wittgen M
- Wobisch M
- Wolf A
- Wolf TMH
- Wolff R
- Wolker R
- Wollrath J
- Wolter MW
- Wolters H
- Wong VWS
- Woods NL
- Worm SD
- Wosiek BK
- Wozniak KW
- Wraight K
- Wu SL
- Wu X
- Wu Y
- Wyatt TR
- Wynne BM
- Xella S
- Xi Z
- Xia L
- Xiao X
- Xiotidis I
- Xu D
- Xu H
- Xu L
- Xu T
- Xu W
- Xu Z
- Yabsley B
- Yacoob S
- Yajima K
- Yallup DP
- Yamaguchi N
- Yamaguchi Y
- Yamamoto A
- Yamatani M
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang HJ
- Yang HT
- Yang S
- Yang T
- Yang X
- Yang Y
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye H
- Ye J
- Ye S
- Yeletskikh I
- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yuan R
- Yue X
- Zaazoua M
- Zabinski B
- Zacharis G
- Zaffaroni E
- Zahreddine J
- Zaitsev AM
- Zakareishvili T
- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang DF
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Molecular biology of the blood-brain and the blood-cerebrospinal fluid barriers: similarities and differences
- Author
- A Chodobski
- A Chodobski
- A Lippoldt
- A Nies
- A Régina
- A Sagare
- A Schinkel
- A Suzuki
- A Zlotnik
- AD Mooradian
- AH Schinkel
- AJ Isakovic
- AJ Isakovic
- AJ Zamora
- AK Kumagai
- AL Betz
- AL Biere
- AL Hughes
- AL Olson
- AM Hartz
- AM Hartz
- AP Halestrap
- AW Vorbrodt
- AY Andreeva
- B Bauer
- B Bauer
- B Bauer
- B Gao
- B Permanne
- BE Enerson
- BT Hawkins
- BV Zlokovic
- BV Zlokovic
- BV Zlokovic
- BV Zlokovic
- BV Zlokovic
- BV Zlokovic
- BV Zlokovic
- BV Zlokovic
- C Agulhon
- C Calatozzolo
- C Crone
- C Johanson
- C Ruffer
- C Sandri
- C Shu
- CE Johanson
- CE Johanson
- CE Johanson
- CE Johanson
- CE Schwartz
- CJ Taylor
- CL Willis
- CM Van Itallie
- D Dawbarn
- D Dogrukol-Ak
- D Miecz
- D Vestweber
- D Wang
- D Westholm
- DE Scott
- DJ Begley
- DJ Roberts
- DS Dwyer
- DS Miller
- DZ Gerhart
- E Nakamura
- E Pellerin
- EE Goldmann
- EM Cornford
- EM Koehler-Stec
- F Maher
- F Verrey
- FG Russel
- G Bazzoni
- G Bazzoni
- G Schreiber
- GJ Feldman
- GL Semenza
- GL Semenza
- H Adle-Biassette
- H Al-Sarraf
- H Benveniste
- H Bronger
- H Doege
- H Koepsell
- H Kusuhara
- H Nishimura
- H Wolburg
- H Wolburg
- H Wolburg
- H Xiong
- H Zhang
- HC Wijesuriya
- HF Cserr
- HH Damkier
- HH Damkier
- HM Fields
- I Brasnjevic
- I Martin-Padura
- I Rubio-Aliaga
- I Tayarani
- I van Rooy
- IA Simpson
- ID Millar
- J Brownlees
- J Guan
- J Klepper
- J Piontek
- J Praetorius
- J Praetorius
- J Stoll
- J Szmydynger-Chodobska
- J Szmydynger-Chodobska
- JA Palha
- JB Lingrel
- JC Chavez
- JD Huber
- JE Preston
- JJ Lochhead
- JM Duarte
- K Babakhanian
- K Brockmann
- K Linnet
- K Matter
- K Mollgard
- K Mori
- K Welch
- KS Mark
- L Bergersen
- L Gonzalez-Mariscal
- L Mosconi
- LD Stegink
- LH Bergersen
- LM Roberts
- LM Roberts
- LM Tai
- M Alebouyeh
- M Arluison
- M Behl
- M Calero
- M Daood
- M Dean
- M Espejo
- M Heiskala
- M Itoh
- M King
- M Mueckler
- M Pollay
- M Rotstein
- M Saitou
- M Saitou
- M Tachikawa
- M Tsacopoulos
- MA Puchowicz
- MB Segal
- ME O'Donnell
- MG Lampugnani
- MH Tuszynski
- MJ Dresser
- MJ Williams
- ML Block
- MM Sánchez del Pino
- MO Dietrich
- MO Romanitan
- MR Del Bigio
- MW Bradbury
- N Bodor
- N Strazielle
- NJ Abbott
- NJ Abbott
- P Vigne
- PA Nicola
- PT Ronaldson
- QR Smith
- R Beschorner
- R Deane
- R Deane
- R Deane
- R Deane
- R Duelli
- R Estévez
- R Lyck
- R Spector
- RA Hawkins
- RA Hawkins
- RC Poole
- RD Bell
- RD Broadwell
- RD Broadwell
- RF Keep
- RF Keep
- RF Keep
- RJ Boado
- RJ Wurtman
- RK Bruick
- RL Leino
- RL O'Kane
- S Bröer
- S Choudhuri
- S Dauchy
- S Eyal
- S Fischer
- S Gazzin
- S Ito
- S Jacobs
- S Mori
- S Vemula
- S Vogelgesang
- SC Woods
- SD Bamforth
- SF Yan
- SI Harik
- SM Ocheltree
- SM Ocheltree
- T Kago
- T Kayano
- T Koto
- T Nishijima
- T Nitta
- T Quintela
- T Quintela
- T Quintela
- T Terai
- T Yamashita
- T Yang
- UV Berger
- VA Levin
- VV Rao
- W Kuschinsky
- W Meng
- W Zhang
- WA Banks
- WA Banks
- WA Banks
- WA Banks
- WA Banks
- WA Banks
- WA Banks
- WJ Lee
- WL Yeh
- WM Abi-Saab
- WM Pardridge
- X Alvira-Botero
- X Guo
- Y Kido
- Y Kido
- Y Li
- Y Nagata
- Y Saito
- YJ Lee
- YP Tang
- ZB Redzic
- ZB Redzic
- ZB Redzic
- ZE Sauna
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
Efficient processing of information by the central nervous system (CNS) represents an important evolutionary advantage. Thus, homeostatic mechanisms have developed that provide appropriate circumstances for neuronal signaling, including a highly controlled and stable microenvironment. To provide such a milieu for neurons, extracellular fluids of the CNS are separated from the changeable environment of blood at three major interfaces: at the brain capillaries by the blood-brain barrier (BBB), which is localized at the level of the endothelial cells and separates brain interstitial fluid (ISF) from blood; at the epithelial layer of four choroid plexuses, the blood-cerebrospinal fluid (CSF) barrier (BCSFB), which separates CSF from the CP ISF, and at the arachnoid barrier. The two barriers that represent the largest interface between blood and brain extracellular fluids, the BBB and the BCSFB, prevent the free paracellular diffusion of polar molecules by complex morphological features, including tight junctions (TJs) that interconnect the endothelial and epithelial cells, respectively. The first part of this review focuses on the molecular biology of TJs and adherens junctions in the brain capillary endothelial cells and in the CP epithelial cells. However, normal function of the CNS depends on a constant supply of essential molecules, like glucose and amino acids from the blood, exchange of electrolytes between brain extracellular fluids and blood, as well as on efficient removal of metabolic waste products and excess neurotransmitters from the brain ISF. Therefore, a number of specific transport proteins are expressed in brain capillary endothelial cells and CP epithelial cells that provide transport of nutrients and ions into the CNS and removal of waste products and ions from the CSF. The second part of this review concentrates on the molecular biology of various solute carrier (SLC) transport proteins at those two barriers and underlines differences in their expression between the two barriers. Also, many blood-borne molecules and xenobiotics can diffuse into brain ISF and then into neuronal membranes due to their physicochemical properties. Entry of these compounds could be detrimental for neural transmission and signalling. Thus, BBB and BCSFB express transport proteins that actively restrict entry of lipophilic and amphipathic substances from blood and/or remove those molecules from the brain extracellular fluids. The third part of this review concentrates on the molecular biology of ATP-binding cassette (ABC)-transporters and those SLC transporters that are involved in efflux transport of xenobiotics, their expression at the BBB and BCSFB and differences in expression in the two major blood-brain interfaces. In addition, transport and diffusion of ions by the BBB and CP epithelium are involved in the formation of fluid, the ISF and CSF, respectively, so the last part of this review discusses molecular biology of ion transporters/exchangers and ion channels in the brain endothelial and CP epithelial cells
Design concepts for the Cherenkov Telescope Array CTA: an advanced facility for ground-based high-energy gamma-ray astronomy
- Author
- Actis M
- Agnetta G
- Aharonian F
- Akhperjanian A
- Aleksic J
- Aliu E
- Allan D
- Allekotte I
- Antico F
- Antonelli LA
- Antoranz P
- Aravantinos A
- Arlen T
- Arnaldi H
- Arribas MP
- Artmann S
- Asano K
- Asorey H
- Baehr J
- Bais A
- Baixeras C
- Bajtlik S
- Balis D
- Bamba A
- Barbier C
- Barcelo M
- Barnacka A
- Barnstedt J
- Barrio JA
- Basso S
- Bastieri D
- Bauer C
- Becerra J
- Becherini Y
- Bechtol K
- Becker J
- Beckmann V
- Bednarek W
- Behera B
- Beilicke M
- Belluso M
- Benallou M
- Benbow W
- Berdugo J
- Berger K
- Bernardino T
- Bernloehr K
- Biland A
- Billotta S
- Bird T
- Birsin E
- Bissaldi E
- Blake S
- Blanch O
- Bobkov AA
- Bogacz L
- Bogdan M
- Boisson C
- Boix J
- Bolmont J
- Bonanno G
- Bonardi A
- Bonev T
- Borkowski J
- Botner O
- Bottani A
- Bourgeat M
- Boutonnet C
- Bouvier A
- Brau-Nogue S
- Braun I
- Bretz T
- Briggs MS
- Brun P
- Brunetti L
- Buckley H
- Buehler R
- Bugaev V
- Bulik T
- Busetto G
- Buson S
- Byrum K
- Cailles M
- Cameron R
- Canestrari R
- Cantu S
- Carmona E
- Carosi A
- Carr J
- Carton PH
- Casiraghi M
- Castarede H
- Catalano O
- Cavazzani S
- Cazaux S
- Cerruti B
- Cerruti M
- Chadwick M
- Chiang J
- Chikawa M
- Ciesielska M
- Cieslar M
- Cillis A
- Clerc C
- Colin P
- Colome J
- Compin M
- Conconi P
- Connaughton V
- Conrad J
- Consortium CTA
- Contreras JL
- Coppi P
- Corlier M
- Corona P
- Corpace O
- Corti D
- Cortina J
- Costantini H
- Cotter G
- Courty B
- Couturier S
- Covino S
- Croston J
- Cusumano G
- Dal Pino EMDG
- Daniel MK
- Dazzi F
- de Almeida UB
- de Cea del Pozo E
- de Jager O
- de la Calle Perez I
- De La Vega G
- De Lotto B
- de Naurois M
- de Souza V
- Deangelis A
- Decerprit B
- Deil C
- Delagnes E
- Deleglise G
- Delgado C
- Dettlaff T
- Di Paolo A
- Di Pierro F
- Diaz C
- Dick J
- Dickinson H
- Digel SW
- Dimitrov D
- Disset G
- Djannati-Ata A
- Doert M
- Domainko W
- Dorner D
- Doro M
- Dournaux J-L
- Dravins D
- Drury L
- Dubois F
- Dubois R
- Dubus G
- Dufour C
- Durand D
- Dyks J
- Dyrda M
- Edy E
- Egberts K
- Eleftheriadis C
- Elles S
- Emmanoulopoulos D
- Enomoto R
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- Wierzcholska A
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- Zech A
- Zietara K
- Ziolkowski P
- Zitelli V
- Zychowski P
- Publication venue
- Springer Verlag
- Publication date
- 01/01/2010
- Field of study
Ground-based gamma-ray astronomy has had a major breakthrough with the impressive results obtained using systems of imaging atmospheric Cherenkov telescopes. Ground-based gamma-ray astronomy has a huge potential in astrophysics, particle physics and cosmology. CTA is an international initiative to build the next generation instrument, with a factor of 5-10 improvement in sensitivity in the 100 GeV-10 TeV range and the extension to energies well below 100 GeV and above 100 TeV. CTA will consist of two arrays (one in the north, one in the south) for full sky coverage and will be operated as open observatory. The design of CTA is based on currently available technology. This document reports on the status and presents the major design concepts of CTA
Combined measurement of differential and total cross sections in the H → γγ and the H → ZZ* → 4ℓ decay channels at s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- Abouzeid OS
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- Zemaityte G
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- Zhang Z
- Zhao P
- Zhao X
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- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- Elsevier
- Publication date
- 01/01/2018
- Field of study
A combined measurement of differential and inclusive total cross sections of Higgs boson production is performed using 36.1 fb−1 of 13 TeV proton–proton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured H→γγ and H→ZZ*(→4ℓ event yields, which are combined taking into account detector efficiencies, resolution, acceptances and branching fractions. The total Higgs boson production cross section is measured to be 57.0−5.9 +6.0 (stat.) −3.3 +4.0 (syst.) pb, in agreement with the Standard Model prediction. Differential cross-section measurements are presented for the Higgs boson transverse momentum distribution, Higgs boson rapidity, number of jets produced together with the Higgs boson, and the transverse momentum of the leading jet. The results from the two decay channels are found to be compatible, and their combination agrees with the Standard Model predictions
Measurement of VH, H → b b ¯ production as a function of the vector-boson transverse momentum in 13 TeV pp collisions with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- Akilli E
- Akimov AV
- Al Khoury K
- Alberghi GL
- Alberich LC
- Albert J
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alfonsi A
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Estevez M
- Alvarez Piqueras D
- Alviggi MG
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Arabidze G
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armadans RC
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
- Arnold H
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Augsten K
- Avolio G
- Avramidou R
- Ayoub MK
- Azoulay AM
- Azuelos G
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- Zhang Y
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu CG
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- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2019
- Field of study
Cross-sections of associated production of a Higgs boson decaying into bottom-quark pairs and an electroweak gauge boson, W or Z, decaying into leptons are measured as a function of the gauge boson transverse momentum. The measurements are performed in kinematic fiducial volumes defined in the `simplified template cross-section' framework. The results are obtained using 79.8 fb-1 of proton-proton collisions recorded by the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13 TeV. All measurements are found to be in agreement with the Standard Model predictions, and limits are set on the parameters of an effective Lagrangian sensitive to modifications of the Higgs boson couplings to the electroweak gauge bosons
Search for High-Mass Resonances Decaying to τν in pp Collisions at √s=13 TeV with the ATLAS Detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
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- Casadei D
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- Castelijn R
- Castillo Gimenez V
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- Cavasinni V
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- Charlton DG
- Chau CC
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- Damazio D Oliveira
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- Zimine NI
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen H Meyer
- zur Nedden M
- Zwalinski L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2018
- Field of study
A search for high-mass resonances decaying to τν using proton-proton collisions at √s=13 TeV produced by the Large Hadron Collider is presented. Only τ-lepton decays with hadrons in the final state are considered. The data were recorded with the ATLAS detector and correspond to an integrated luminosity of 36.1 fb−1. No statistically significant excess above the standard model expectation is observed; model-independent upper limits are set on the visible τν production cross section. Heavy W′ bosons with masses less than 3.7 TeV in the sequential standard model and masses less than 2.2–3.8 TeV depending on the coupling in the nonuniversal G(221) model are excluded at the 95% credibility level
Measurement of the t¯tZ and t¯tW cross sections in proton-proton collisions at √s=13 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abbott DC
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexandre D
- Alexopoulos T
- Alhroob M
- Ali B
- Alimonti G
- Alison J
- Alkire SP
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Gonzalez B
- Alviggi MG
- Amadio BT
- Amaral Coutinho Y
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
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- Antrim DJA
- Anulli F
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- Arabidze G
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- Arduh FA
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- Armbruster AJ
- Armitage LJ
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zur Nedden M
- Zwalinski L
- Álvarez Piqueras D
- Åkesson TPA
- Šfiligoj T
- Ženiš T
- Živković L
- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2019
- Field of study
A measurement of the associated production of a top-quark pair (t¯t) with a vector boson (W, Z) in proton-proton collisions at a center-of-mass energy of 13 TeV is presented, using 36.1 fb−1 of integrated luminosity collected by the ATLAS detector at the Large Hadron Collider. Events are selected in channels with two same- or opposite-sign leptons (electrons or muons), three leptons or four leptons, and each channel is further divided into multiple regions to maximize the sensitivity of the measurement. The t¯tZ and t¯tW production cross sections are simultaneously measured using a combined fit to all regions. The best-fit values of the production cross sections are σt¯tZ=0.95±0.08stat±0.10syst pb and σt¯tW=0.87±0.13stat±0.14syst pb in agreement with the Standard Model predictions. The measurement of the t¯tZ cross section is used to set constraints on effective field theory operators which modify the t¯tZ vertex
Performance of missing transverse momentum reconstruction with the ATLAS detector using proton–proton collisions at √s = 13 TeV
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- Aaboud M
- Aad G
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- Abdinov O
- Abeloos B
- Abhayasinghe DK
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The performance of the missing transverse momentum (EmissT) reconstruction with the ATLAS detector is evaluated using data collected in proton–proton collisions at the LHC at a centre-of-mass energy of 13 TeV in 2015. To reconstruct EmissT, fully calibrated electrons, muons, photons, hadronically decaying τ -leptons, and jets reconstructed from calorimeter energy deposits and charged-particle tracks are used. These are combined with the soft hadronic activity measured by reconstructed charged-particle tracks not associated with the hard objects. Possible double counting of contributions from reconstructed charged-particle tracks from the inner detector, energy deposits in the calorimeter, and reconstructed muons from the muon spectrometer is avoided by applying a signal ambiguity resolution procedure which rejects already used signals when combining the various EmissT contributions. The individual terms as well as the overall reconstructed EmissT are evaluated with various performance metrics for scale (linearity), resolution, and sensitivity to the data-taking conditions. The method developed to determine the systematic uncertainties of the EmissT scale and resolution is discussed. Results are shown based on the full 2015 data sample corresponding to an integrated luminosity of 3.2 fb−1
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