241 research outputs found
Chicken genome analysis reveals novel genes encoding biotin-binding proteins related to avidin family
- Author
- A Pagano
- A Sali
- AC Camproux
- AE Kel
- D Sanchez
- DR Flower
- DR Flower
- GJ Barton
- H Nielsen
- HB White III
- HB White III
- HM Berman
- HR Nordlund
- HR Nordlund
- HW Meslar
- JV Lehtonen
- L Bush
- L Bush
- LW Hillier
- M Wilchek
- MJ Wallén
- MK Ahlroth
- MK Ahlroth
- MK Ahlroth
- MK Ahlroth
- ML Gope
- MS Johnson
- MS Johnson
- N Subramanian
- NM Green
- O Livnah
- O Livnah
- OH Laitinen
- OH Laitinen
- OH Laitinen
- OH Laitinen
- OH Laitinen
- P Tuohimaa
- PB Seshagiri
- PC Weber
- PE Boardman
- RA KeinÀnen
- S Freitag
- S Kumar
- S Kumar
- SC Gill
- SW Cowan
- T Sano
- VB Bajic
- VP Hytönen
- WE Stumph
- WL DeLano
- Publication venue
- BioMed Central
- Publication date
- 01/01/2005
- Field of study
BACKGROUND: A chicken egg contains several biotin-binding proteins (BBPs), whose complete DNA and amino acid sequences are not known. In order to identify and characterise these genes and proteins we studied chicken cDNAs and genes available in the NCBI database and chicken genome database using the reported N-terminal amino acid sequences of chicken egg-yolk BBPs as search strings. RESULTS: Two separate hits showing significant homology for these N-terminal sequences were discovered. For one of these hits, the chromosomal location in the immediate proximity of the avidin gene family was found. Both of these hits encode proteins having high sequence similarity with avidin suggesting that chicken BBPs are paralogous to avidin family. In particular, almost all residues corresponding to biotin binding in avidin are conserved in these putative BBP proteins. One of the found DNA sequences, however, seems to encode a carboxy-terminal extension not present in avidin. CONCLUSION: We describe here the predicted properties of the putative BBP genes and proteins. Our present observations link BBP genes together with avidin gene family and shed more light on the genetic arrangement and variability of this family. In addition, comparative modelling revealed the potential structural elements important for the functional and structural properties of the putative BBP proteins
Inhibition of Bax protects neuronal cells from oligomeric AÎČ neurotoxicity
- Author
- A Giovanni
- A Giovanni
- A Gross
- A Letai
- A Nechushtan
- AM Davies
- DR Green
- E Gavathiotis
- F Clavaguera
- F Edlich
- FG De Felice
- GV Putcha
- GV Putcha
- HG Lee
- J Lauren
- J Whitfield
- JA Gomez
- JA Gomez
- KM Webber
- M Zornig
- MP Lambert
- N Gogolla
- N Gogolla
- NH Varvel
- PE Czabotar
- QL Ma
- R Eskes
- S Mac Fhearraigh
- SC Biswas
- SC Biswas
- SN Farrow
- SW Tait
- T Yoshida
- VP Bajic
- W Kudo
- WL Klein
- X Zhu
- X Zhu
- X Zhu
- Y Kitamura
- Y Li
- YT Hsu
- Publication venue
- Nature Publishing Group
- Publication date
- Field of study
Although oligomeric ÎČ-amyloid (AÎČ) has been suggested to have an important role in Alzheimer disease (AD), the mechanism(s) of how AÎČ induces neuronal cell death has not been fully identified. The balance of pro- and anti-apoptotic Bcl-2 family proteins (e.g., Bcl-2 and Bcl-w versus Bad, Bim and Bax) has been known to have a role in neuronal cell death and, importantly, expression levels of these proteins are reportedly altered in the vulnerable neurons in AD. However, the roles of apoptotic proteins in oligomeric AÎČ-induced cell death remain unclear in vivo or in more physiologically relevant models. In addition, no study to date has examined whether Bax is required for the toxicity of oligomeric AÎČ. Here, we found that treatment with oligomeric AÎČ increased Bim levels but decreased Bcl-2 levels, leading to the activation of Bax and neuronal cell death in hippocampal slice culture and in vivo. Furthermore, the inhibition of Bax activity either by Bax-inhibiting peptide or bax gene knockout significantly prevented oligomeric AÎČ-induced neuronal cell death. These findings are first to demonstrate that Bax has an essential role in oligomeric AÎČ-induced neuronal cell death, and that the targeting of Bax may be a therapeutic approach for AD
Combined measurement of differential and total cross sections in the HâŻââŻÎłÎł and the HâŻââŻZZ*âŻââŻ4â 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
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk 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
- 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
- Ambroz L
- Amelung C
- Amidei D
- Amor Dos Santos SP
- Amoroso S
- Amrouche CS
- 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
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- Anthony MT
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aperio Bella L
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armbruster AJ
- Armitage LJ
- Armstrong A
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- Artoni G
- Artz S
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- Asbah N
- Ashkenazi A
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Atkin RJ
- Atkinson M
- Atlas Collaboration
- Atlay NB
- Augsten K
- Avolio G
- Avramidou R
- Axen B
- Ayoub MK
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
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- Bahmani M
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- Baldin EM
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- Zhemchugov A
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- Zibell A
- Zieminska D
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- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zobernig G
- Zoccoli A
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- Zorbas TG
- Zou R
- Zur Nedden M
- Zwalinski L
- Ălvarez Piqueras D
- Ă kesson TPA
- Ć filigoj T
- ĆœeniĆĄ T
- ĆœivkoviÄ 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 fbâ1 of 13 TeV protonâproton collision data produced by the LHC and recorded by the ATLAS detector in 2015 and 2016. Cross sections are obtained from measured Hâγγ and HâZZ*(â4â 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 57.0â5.9 +6.0 (stat.) â3.3 +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
Search for High-Mass Resonances Decaying to ÏÎœ in pp Collisions at âs=13 TeV with the ATLAS Detector
- Author
- Aaboud M
- Aad G
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- Abdinov O
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- 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 ÏÎœ using proton-proton collisions at âs=13 TeV produced by the Large Hadron Collider is presented. Only Ï-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 fbâ1. No statistically significant excess above the standard model expectation is observed; model-independent upper limits are set on the visible ÏÎœ production cross section. Heavy WâČ bosons with masses less than 3.7 TeV in the sequential standard model and masses less than 2.2â3.8 TeV depending on the coupling in the nonuniversal G(221) model are excluded at the 95% credibility level
Search for the direct production of charginos and neutralinos in final states with tau leptons in âs=13 TeV collisions with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2017
- Field of study
A search for the direct production of charginos and neutralinos in final states with at least two hadronically decaying tau leptons is presented. The analysis uses a dataset of pp collisions corresponding to an integrated luminosity of 36.1 fbâ1, recorded with the ATLAS detector at the Large Hadron Collider at a centre-of-mass energy of 13TeV.Nosignificant deviation from the expected Standard Model background is observed. Limits are derived in scenarios of ËÏ+1 ËÏâ1 pair production and of Ëϱ1 ËÏ02 and ËÏ+1 ËÏâ1 production in simplified models where the neutralinos and charginos decay solely via intermediate left-handed staus and tau sneutrinos, and the mass of the Ë ÏL state is set to be halfway between the masses of the Ëϱ1 and the ËÏ01. Chargino masses up to 630 GeV are excluded at 95% confidence level in the scenario of direct production of ËÏ+1 ËÏâ1 for a massless ËÏ01. Common Ëϱ1 and ËÏ02 masses up to 760 GeV are excluded in the case of production of Ëϱ1 ËÏ02 and ËÏ+1 ËÏâ1 assuming a massless ËÏ01. Exclusion limits for additional benchmark scenarios with large and small mass-splitting between the Ëϱ1 and the ËÏ01 are also studied by varying the Ë ÏL mass between the masses of the Ëϱ1 and the ËÏ01
Measurement of differential cross sections and W + /W â cross-section ratios for W boson production in association with jets at âs =8 TeV with the ATLAS detector
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- Zhemchugov A
- Zhou B
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- Zibell A
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- Zimine NI
- Zimmermann C
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- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
This paper presents a measurement of the W boson production cross section and the W + /W â cross-section ratio, both in association with jets, in proton--proton collisions at s â =8 TeV with the ATLAS experiment at the Large Hadron Collider. The measurement is performed in final states containing one electron and missing transverse momentum using data corresponding to an integrated luminosity of 20.2 fb â1 . Differential cross sections for events with one or two jets are presented for a range of observables, including jet transverse momenta and rapidities, the scalar sum of transverse momenta of the visible particles and the missing transverse momentum in the event, and the transverse momentum of the W boson. For a subset of the observables, the differential cross sections of positively and negatively charged W bosons are measured separately. In the cross-section ratio of W + /W â the dominant systematic uncertainties cancel out, improving the measurement precision by up to a factor of nine. The observables and ratios selected for this paper provide valuable input for the up quark, down quark, and gluon parton distribution functions of the proto
Measurement of the cross section for inclusive isolated-photon production in pp collisions at âs=13TeV using the ATLAS detector
- Author
- Aaboud M
- Aad G
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- Abdinov O
- Abeloos B
- Abidi SH
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- Abraham NL
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- Alberghi GL
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- Kozanecki W
- Kozhin AS
- Kramarenko VA
- Kramberger G
- Krasnopevtsev D
- Krasny MW
- Krasznahorkay A
- Krauss D
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- Kuehn S
- Kugel A
- Kuger F
- Kuh T
- Kukhtin V
- Kukla R
- Kulchitsky Y
- Kuleshov S
- Kulinich YP
- Kuna M
- Kunigo T
- Kupco A
- Kupfer T
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- Kurashige H
- Kurchaninov LL
- Kurochkin YA
- Kurth MG
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- Kuwertz ES
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- Lankford AJ
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- Lanza A
- Lapertosa A
- Laplace S
- Laporte JF
- Lari T
- Lassnig M
- Latour BMD
- Lau TS
- Laurelli P
- Lavrijsen W
- Law AT
- Laycock P
- Lazovich T
- Lazzaroni M
- Le Dortz O
- Le Guirriec E
- Le Quilleuc EP
- Le B
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- LeCompte T
- Ledroit-Guillon F
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- Lee GR
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- Leite MAL
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- Liebig W
- Limosani A
- Lin CY
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- Linck RA
- Lindquist BE
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- Lipeles E
- Lipniacka A
- Lisovyi M
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- Lister A
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- Lloyd SL
- Lo Sterzo F
- Lo CY
- Lobodzinska EM
- Loch P
- Loebinger FK
- Loesle A
- Loew KM
- Lohse T
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- Lou X
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- Lukas W
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- Lundberg O
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- Lyu F
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- Ma Y
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- Macchiolo A
- Macdonald CM
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- Maevskiy AS
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- Martyniuk AC
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- Maznas I
- Mazza SM
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- Mc Goldrick G
- Mc Kee SP
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- Yamaguchi Y
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- Yamamoto S
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- Yamatani M
- Yamazaki T
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- Yang Z
- Yao W-M
- Yap YC
- Yasu Y
- Yatsenko E
- Ye J
- Ye S
- Yeletskikh I
- Yigitbasi E
- Yildirim E
- Yildiz HD
- Yorita K
- Yoshihara K
- Young C
- Young CJS
- Yu J
- Yu J
- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
- Zaitsev AM
- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
- Zeitnitz C
- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
- Zhang D
- Zhang F
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang L
- Zhang M
- Zhang P
- Zhang R
- Zhang R
- Zhang X
- Zhang Y
- Zhang Z
- Zhao X
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zhou B
- Zhou C
- Zhou L
- Zhou M
- Zhou M
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zibell A
- Zieminska D
- Zimine NI
- Zimmermann C
- Zimmermann S
- Zinonos Z
- Zinser M
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zou R
- zur Nedden M
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2017
- Field of study
Inclusive isolated-photon production in pp collisions at a centre-of-mass energy of 13TeVis studied with the ATLAS detector at the LHC using a data set with an integrated luminosity of 3.2fbâ1. The cross section is measured as a function of the photon transverse energy above 125GeVin different regions of photon pseudorapidity. Next-to-leading-order perturbative QCD and Monte Carlo event-generator predictions are compared to the cross-section measurements and provide an adequate description of the data
Operation and performance of the ATLAS Tile Calorimeter in Run 1
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abhayasinghe DK
- Abidi SH
- Abouelfadl 
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adiguzel A
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- 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 
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- Amadio BT
- Amaral Coutinho Y
- Ambroz L
- Amelung C
- Amidei D
- Amor 
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- Amrouche CS
- 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
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aperio Bella L
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Arce ATH
- Ardell RE
- Arduh FA
- Argos FC
- Arguin J-
- Argyropoulos S
- Armadans R
- Armbruster AJ
- Armitage LJ
- Armstrong A
- Arnaez O
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- Arslan O
- Artamonov A
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- Asquith L
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- Atkin RJ
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- Atlay NB
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- Calafiura P
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- Canale V
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- Capeans Garrido MDM
- Caprini I
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- Carbone RM
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- Cardillo FC
- Carli I
- Carli T
- Carlino G
- Carlson BT
- Carminati L
- Carney RMD
- Caron S
- Carquin E
- CarraÌ S
- Carrillo-Montoya GD
- Casadei D
- Casado MP
- Casha AF
- Casolino M
- Casper DW
- Castelijn R
- Castillo Gimenez V
- Castillo FL
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- Catinaccio A
- Catmore JR
- Cattai A
- Caudron J
- Cavaliere V
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- Cherkaoui El Moursli R
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- Chevalier L
- Chiarella V
- Chiarelli G
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- Chiu I
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- Christodoulou V
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- Cindro V
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- Cortes-Gonzalez A
- Costa MJ
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- Cottin G
- Cowan G
- Cox BE
- Crane J
- Cranmer K
- Crawley SJ
- Creager RA
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- CreÌpeÌ-Renaudin S
- Cristinziani M
- Croft V
- Crosetti G
- Cueto A
- Cuhadar Donszelmann T
- Cukierman AR
- Cunha 
- Curatolo M
- CuÌth J
- Czekierda S
- Czodrowski P
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- Dado T
- Dahbi S
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- Dam M
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- Dandoy JR
- Daneri MF
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- Dao V
- Darbo G
- Darmora S
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- Dattagupta A
- Daubney T
- Davey W
- David C
- Davidek T
- Davis DR
- Davydov Y
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- Dawson I
- De Asmundis R
- De Benedetti A
- De Castro S
- De Cecco S
- De Groot N
- de Jong P
- De la Torre H
- De Lorenzi F
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- De Moura 
- De Pedis D
- De Salvo A
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- Debenedetti C
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- Zwalinski L
- ZÌenisÌ T
- ZÌivkovicÌ L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
The Tile Calorimeter is the hadron calorimeter covering the central region of the ATLAS experiment at the Large Hadron Collider. Approximately 10,000 photomultipliers collect light from scintillating tiles acting as the active material sandwiched between slabs of steel absorber. This paper gives an overview of the calorimeterâs performance during the years 2008â2012 using cosmic-ray muon events and protonâproton collision data at centre-of-mass energies of 7 and 8TeV with a total integrated luminosity of nearly 30 fbâ1. The signal reconstruction methods, calibration systems as well as the detector operation status are presented. The energy and time calibration methods performed excellently, resulting in good stability of the calorimeter response under varying conditions during the LHC Run 1. Finally, the Tile Calorimeter response to isolated muons and hadrons as well as to jets from protonâproton collisions is presented. The results demonstrate excellent performance in accord with specifications mentioned in the Technical Design Report
Measurement of VH, H â b b ÂŻ production as a function of the vector-boson transverse momentum in 13 TeV pp collisions with the ATLAS detector
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- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
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- Zhu CG
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- Zhu J
- Zhu Y
- Zhuang X
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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
Measurements of integrated and differential cross sections for isolated photon pair production in pp collisions at âs=8 TeV with the ATLAS detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdallah J
- Abdinov O
- Abeloos B
- Abidi SH
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- Publication venue
- 'American Physical Society (APS)'
- Publication date
- 01/01/2017
- Field of study
A measurement of the production cross section for two isolated photons in proton-proton collisions at a center-of-mass energy of âs=8 TeV is presented. The results are based on an integrated luminosity of 20.2 fbâ1 recorded by the ATLAS detector at the Large Hadron Collider. The measurement considers photons with pseudorapidities satisfying |ηγ|40GeV and EÎłT,2>30 GeV for the two leading photons ordered in transverse energy produced in the interaction. The background due to hadronic jets and electrons is subtracted using data-driven techniques. The fiducial cross sections are corrected for detector effects and measured differentially as a function of six kinematic observables. The measured cross section integrated within the fiducial volume is 16.8 ± 0.8â pb . The data are compared to fixed-order QCD calculations at next-to-leading-order and next-to-next-to-leading-order accuracy as well as next-to-leading-order computations including resummation of initial-state gluon radiation at next-to-next-to-leading logarithm or matched to a parton shower, with relative uncertainties varying from 5% to 20%
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