189 research outputs found
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
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Aranda CP
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asner D
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
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- Azuelos G
- Azuma Y
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- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
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- Backhaus M
- Badescu E
- Bagnaia P
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- Bai Y
- Bailey DC
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- Boscherini D
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- Botterill D
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- Budagov IA
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- Bueso XP
- Bugge L
- Buira-Clark D
- Bulekov O
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- Castanheira MTD
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- Castro NF
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- Chapman JD
- Chapman JW
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- Charlton DG
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- Cheatham S
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen S
- Chen T
- Chen X
- Cheng S
- Cheong ALF
- Cheplakov A
- Chepurnov VF
- Chernyatin V
- Cheu E
- Cheung SL
- Chevalier L
- Chiefari G
- Chikovani L
- Childers JT
- Chilingarov A
- Chiodini G
- Chizhov MV
- Choudalakis G
- Chouridou S
- Christidi IA
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- Chromek-Burckhart D
- Chu ML
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- Cioccaa C
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- Collaboration ATLAS
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- Da Costa JBG
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- Damazio DO
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- De la Taille C
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- Degenhardt J
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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
Measurement of the inclusive and dijet cross-sections of b-jets in pp collisions at sqrt(s) = 7 TeV with the ATLAS detector
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- Willocq S
- Wilson A
- Wilson JA
- Wilson MG
- Wingerter-Seez I
- Winkelmann S
- Winklmeier F
- Wittgen M
- Wolter MW
- Wolters H
- Wooden G
- Wosiek BK
- Wotschack J
- Woudstra MJ
- Wraight K
- Wright C
- Wrona B
- Wu SL
- Wu X
- Wu Y
- Wulf E
- Wunstorf R
- Wynne BM
- Xaplanteris L
- Xella S
- Xie S
- Xie Y
- Xu C
- Xu D
- Xu G
- Yabsley B
- Yagci KD
- Yamada M
- Yamamoto A
- Yamamoto K
- Yamamoto S
- Yamamura T
- Yamaoka J
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang S
- Yang UK
- Yang Y
- Yang Y
- Yang Z
- Yanush S
- Yao W-M
- Yao Y
- Yasu Y
- Ye J
- Ye S
- Yildiz HD
- Yilmaz M
- Yoosoofmiya R
- Yorita K
- Yoshida R
- Young C
- Youssef S
- Yu D
- Yu J
- Yu J
- Yuan L
- Yurkewicz A
- Zaets VG
- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zdrazil M
- Zeitnitz C
- Zeller M
- Zema PF
- Zemla A
- Zendler C
- Zenin AV
- Zenin O
- Zenis T
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang X
- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
- Zhou N
- Zhou Y
- Zhu CG
- Zhu H
- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zilka B
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- 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
MEF2C Enhances Dopaminergic Neuron Differentiation of Human Embryonic Stem Cells in a Parkinsonian Rat Model
- Author
- A Brederlau
- A Shalizi
- AC Barbosa
- Alexey Terskikh
- AU Hicks
- B Zhu
- B Zhu
- BE Reubinoff
- Cesario V. Borlongan
- CU Hellen
- D Leifer
- D Leifer
- D Yang
- DW Kim
- E Arenas
- E Hedlund
- Eliezer Masliah
- Eun-Gyung Cho
- F Calon
- GE Lyons
- GI Nistor
- H Li
- HS Keirstead
- J Jankovic
- JC McDermott
- Jeffrey D. Zaremba
- JJ Buzzard
- JY Kim
- JY Li
- L Thompson
- LA Gossett
- LE Allan
- M Amit
- M Hatami
- Maria Talantova
- MJ Potthoff
- MM Daadi
- MS Cho
- MW Pfaffl
- N Flames
- Nobuki Nakanishi
- NS Roy
- PH Schwartz
- QL Ying
- R Nat
- S Chiba
- S De Val
- S Friling
- S Okamoto
- SC Zhang
- Scott R. McKercher
- Shichun Tu
- Shing Fai Chan
- Stuart A. Lipton
- SW Flavell
- T Ben-Hur
- T Perlmann
- T Schallert
- TA McKinsey
- TC Schulz
- Y Elkabetz
- Y Elkabetz
- Y Yan
- Z Li
- Z Mao
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2011
- Field of study
Human embryonic stem cells (hESCs) can potentially differentiate into any cell type, including dopaminergic neurons to treat Parkinson's disease (PD), but hyperproliferation and tumor formation must be avoided. Accordingly, we use myocyte enhancer factor 2C (MEF2C) as a neurogenic and anti-apoptotic transcription factor to generate neurons from hESC-derived neural stem/progenitor cells (NPCs), thus avoiding hyperproliferation. Here, we report that forced expression of constitutively active MEF2C (MEF2CA) generates significantly greater numbers of neurons with dopaminergic properties in vitro. Conversely, RNAi knockdown of MEF2C in NPCs decreases neuronal differentiation and dendritic length. When we inject MEF2CA-programmed NPCs into 6-hydroxydopamine—lesioned Parkinsonian rats in vivo, the transplanted cells survive well, differentiate into tyrosine hydroxylase-positive neurons, and improve behavioral deficits to a significantly greater degree than non-programmed cells. The enriched generation of dopaminergic neuronal lineages from hESCs by forced expression of MEF2CA in the proper context may prove valuable in cell-based therapy for CNS disorders such as PD
An overview of using small punch testing for mechanical characterization of MCrAlY bond coats
- Author
- A Feuerstein
- A Gil
- A Scrivani
- A Vardelle
- AG Evans
- B Ule
- BA Pint
- BJ Kim
- C Mercer
- C Rodríguez
- C Rodríguez
- CU Hardwicke
- D Naumenko
- DT Blagoeva
- E Altstadt
- E Fleury
- F Dobeš
- FM Huang
- G. A. Jackson
- GA Jackson
- GA Jackson
- GE Lucas
- GW Meetham
- H Chen
- H Chen
- H Chen
- H Chen
- H Chen
- H Chen
- H Chen
- H Waki
- H Waki
- H. Chen
- J Chakrabarty
- J Kameda
- J Kameda
- J Kameda
- J Toscano
- J Toscano
- J Yang
- JH Bulloch
- JP Rouse
- JR Nicholls
- JS Cheon
- JZ Chen
- K Guan
- K Matocha
- K Turba
- KJ Hemker
- L Ajdelsztajn
- L Wang
- LY Ni
- M Ahrens
- M Arana Antelo
- M Bruchhausen
- M Eskner
- M Eskner
- M Evans
- M Gupta
- M-C Kim
- MA Contreras
- MC Kim
- MG Hebsur
- MG Hebsur
- MH Enayati
- MP Manahan
- MP Manahan
- MP Taylor
- MP Taylor
- N Curry
- O Kovářík
- P Dymáček
- P Hancock
- R Darolia
- R Musalek
- R Musalek
- R Soltani
- R Soltani
- R Sturm
- RD Jackson
- RD Noebe
- RR Bowman
- RW Smith
- S Bose
- S Dryepondt
- S Haroush
- S Komazaki
- S Rasche
- S Soltysiak
- T Hyde
- T Linse
- TC Totemeier
- TE García
- TH Hyde
- TH Hyde
- TH Hyde
- U Hermosilla
- U Schulz
- W Brindley
- W Tillmann
- W. Sun
- WR Chen
- X Gong
- X Mao
- X Mao
- X Mao
- Y Bai
- Y Liu
- Y Ruan
- Y Tamarin
- Z Yang
- ZX Wang
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 05/07/2017
- Field of study
Considerable work has been carried out on overlay bond coats in the past several decades because of its excellent oxidation resistance and good adhesion between the top coat and superalloy substrate in the thermal barrier coating systems. Previous studies mainly focus on oxidation and diffusion behavior of these coatings. However, the mechanical behavior and the dominant fracture and deformation mechanisms of the overlay bond coats at different temperatures are still under investigation. Direct comparison between individual studies has not yet been achieved due to the fragmentary data on deposition processes, microstructure and, more apparently, the difficulty in accurately measuring the mechanical properties of thin coatings. One of the miniaturized specimen testing methods, small punch testing, appears to have the potential to provide such mechanical property measurements for thin coatings. The purpose of this paper is to give an overview of using small punch testing to evaluate material properties and to summarize the available mechanical properties that include the ductile-to-brittle transition and creep of MCrAlY bond coat alloys, in an attempt to understand the mechanical behavior of MCrAlY coatings over a broad temperature range
Biomarkers in T cell therapy clinical trials
- Author
- A Hoos
- A Varela-Rohena
- AM Leen
- AP Rapoport
- AR Hersperger
- AR Hersperger
- B Jena
- BG Till
- BL Levine
- C Berger
- C Berger
- C Yee
- CF Taylor
- CH June
- CH Lamers
- CJ Turtle
- CM Bollard
- CU Louis
- D Gaucher
- D Hollyman
- D Kalamasz
- DB Kohn
- DC Palmer
- DF Stroncek
- DF Stroncek
- DJ Powell Jr
- DJ Stewart
- DL Porter
- DL Porter
- DR Bandura
- EA Walter
- G Makedonas
- G Makedonas
- H Tahara
- HI Scher
- HP Bonarius
- HS Robins
- HT Maecker
- J van Lunzen
- J Zhou
- JC Siebert
- JD Freeman
- JE Cortes
- JJ Melenhorst
- JL Davis
- JW Gratama
- KQ Tran
- KR Schulz
- L Gattinoni
- L Rowen
- LA Johnson
- LH Butterfield
- LH Butterfield
- LH Finke
- M Kalos
- M Raki
- MA Pule
- MA Suni
- MC Jensen
- ME Dudley
- Michael Kalos
- MJ Besser
- MR Betts
- MV Maus
- OI Ornatsky
- PD Greenberg
- PF Robbins
- PF Robbins
- PJ Amrolia
- PK Chattopadhyay
- R Brentjens
- RA Morgan
- RA Morgan
- RA Morgan
- RA Seder
- RJ O'Reilly
- S Ambs
- S Biswas
- S Gnjatic
- S Janetzki
- S Yang
- SC Chow
- SH Beachy
- SP Perfetto
- T Feuchtinger
- TF Gajewski
- U Petrausch
- W Liu
- WT Rogers
- X Wang
- Y Lin
- Y Zhao
- Y Zhao
- Publication venue
- BioMed Central
- Publication date
- 01/01/2011
- Field of study
T cell therapy represents an emerging and promising modality for the treatment of both infectious disease and cancer. Data from recent clinical trials have highlighted the potential for this therapeutic modality to effect potent anti-tumor activity. Biomarkers, operationally defined as biological parameters measured from patients that provide information about treatment impact, play a central role in the development of novel therapeutic agents. In the absence of information about primary clinical endpoints, biomarkers can provide critical insights that allow investigators to guide the clinical development of the candidate product. In the context of cell therapy trials, the definition of biomarkers can be extended to include a description of parameters of the cell product that are important for product bioactivity
Measurement of the cross-section for b-jets produced in association with a Z boson at root s=7 TeV with the ATLAS detector ATLAS Collaboration
- 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
- Akdogan T
- Akesson TPA
- Akimoto G
- Akimov AV
- Akiyama 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
- Almond J
- Aloisio A
- Alon R
- Alonso A
- Alviggi MG
- Amako K
- Amaral P
- Amelung C
- Ammosov VV
- Amorim A
- Amoros G
- Amram N
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders G
- Anderson KJ
- Andreazza A
- Andrei V
- Andrieux M-L
- Anduaga XS
- Angerami A
- Anghinolfi F
- Anh TV
- Anjos N
- Annovi A
- Antonaki A
- Antonelli M
- Antonov A
- Antos J
- Anulli F
- Aoun S
- Apolle R
- Arabidze G
- Aracena I
- Arai Y
- Arce ATH
- Archambault JP
- Arfaoui S
- Arguin J-F
- Arik E
- Arik M
- Armbruster AJ
- Arnaez O
- Arnault C
- Artamonov A
- Artoni G
- Arutinov D
- Asai S
- Asfandiyarov R
- Ask S
- Asman B
- Asquith L
- Assamagan K
- Astbury A
- Astvatsatourov A
- Atoian G
- Aubert B
- Auge E
- Augsten K
- Aurousseau M
- Austin N
- Avolio G
- Avramidou R
- Axen D
- Ay C
- Azuelos G
- Azuma Y
- Baak MA
- Baccaglioni G
- Bacci C
- Bach AM
- Bachacou H
- Bachas K
- Bachy G
- Backes M
- Backhaus M
- Badescu E
- Bagnaia P
- Bahinipati S
- Bai Y
- Bailey DC
- Bain T
- Baines JT
- Baker MD
- Baker OK
- Baker S
- Banas E
- Banerjee P
- Banerjee S
- Banfi D
- Bangert A
- Bansal V
- Bansil HS
- Barajas CAC
- Barak L
- Baranov SP
- Barashkou A
- Barber T
- Barberio EL
- Barberis D
- Barbero M
- Bardin DY
- Barillari T
- Barisonzi M
- Barklow T
- Barlow N
- Barnett BM
- Barnett RM
- Baroncellia A
- Barone G
- Barr AJ
- Barreiro F
- Barrera CO
- Barrillon P
- Bartoldus R
- Barton AE
- Bartsch D
- Bartsch V
- Bates RL
- Batkovaa L
- Batley JR
- Battaglia A
- Battistin M
- Battistonia G
- Bauer F
- Bawa HS
- Beare B
- Beau T
- Beauchemin PH
- Beccherlea R
- Bechtle R
- Beck HP
- Beckingham M
- Becks KH
- Beddallc A
- Beddallc AJ
- Bedikian S
- Bednyakov VA
- Bee CP
- Begel M
- Behera PK
- Beimforde M
- Belanger-Champagne C
- Belenguer MJ
- Bell PJ
- Bell WH
- Bella G
- Bella LA
- Bellagambaa L
- Bellina F
- Bellomo M
- Belloni A
- Beloborodova O
- Belotskiy K
- Beltramello O
- Ben Ami S
- Benary O
- Benchekrouna D
- Benchouk C
- Bendel M
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Benslama K
- Bentvelsen S
- Berge D
- Berger N
- Berghaus F
- Berglund E
- Beringer J
- Bernardet K
- Bernat P
- Bernhard R
- Bernius C
- Berry T
- Bertina A
- Bertinelli F
- Bertoluccia F
- Besanaa MI
- Besson N
- Bethke S
- Bhimji W
- Bianchi RM
- Biancoa M
- Biebel O
- Bieniek SR
- Bierwagen K
- Biesiada J
- Bigliettia M
- Bilokon H
- Bindia M
- Binet S
- Bingulc A
- Binia C
- Biscarat C
- Bitenc U
- Black KM
- Blair RE
- Blanchard J-B
- Blanchot G
- Blazeka T
- Blocker C
- Blocki J
- Blondel A
- Blum W
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VB
- Bocchetta SS
- Bocci A
- Boddy CR
- Boehler M
- Boek J
- Boelaert N
- Boeriu OEV
- Boeser S
- Bogaerts JA
- Bogdanchikov A
- Bogouch A
- Bohma C
- Boisvert V
- Bold T
- Boldeaa V
- Bolnet NM
- Bona M
- Bondarenko VG
- Bondioli M
- Boonekamp M
- Boorman G
- Booth CN
- Bordoni S
- Borer C
- Borisov A
- Borissov G
- Borjanovica I
- Borronia S
- Bos K
- Boscherinia D
- Bosman M
- Boterenbrood H
- Botterill D
- Bouchami J
- Boudreau J
- Bouhova-Thacker EV
- Bourdarios C
- Bousson N
- Boveia A
- Boyd J
- Boyko IR
- Bozhko NI
- Bozovic-Jelisavcicb I
- Bracinik J
- Braem A
- Branchinia P
- Brandenburg GW
- Brandt A
- Brandt G
- Brandt O
- Bratzler U
- Brau B
- Brau JE
- Braun HM
- Brelier B
- Bremer J
- Brenner R
- Bressler S
- Breton D
- Britton D
- Brochu FM
- Brock I
- Brock R
- Brodbeck TJ
- Brodet E
- Broggia F
- Bromberg C
- Brooijmans G
- Brooksb WK
- Brown G
- Brown H
- Bruckman de Renstrom PA
- Bruncko D
- Bruneliere R
- Brunet S
- Brunia A
- Brunia G
- Bruschia M
- Buanes T
- Bucci F
- Buchanan J
- Buchanan NJ
- Buchholz P
- Buckingham RM
- Buckley AG
- Budaa SI
- Budagov IA
- Budick B
- Buescher V
- Bueso XP
- Bugge L
- Buira-Clark D
- Bulekov O
- Bunse M
- Buran T
- Burckhart H
- Burdin S
- Burgess T
- Burke S
- Busato E
- Bussey P
- Buszello CP
- Butin F
- Butler B
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Byatt T
- Cabrera Urban S
- Caforioa D
- Cakir IT
- Cakira O
- Calafiura P
- Calderini G
- Calfayan P
- Calkins R
- Calobaa LP
- Caloia R
- Calvet D
- Calvet S
- Camarri P
- Cambiaghia M
- Cameron D
- Camillocci ES
- Campana S
- Campanelli M
- Canalea V
- Canelli F
- Canepaa A
- Cantero J
- Capassoa L
- Caprinia I
- Caprinia M
- Capriotti D
- Capuaa M
- Caputo R
- Cardarelli R
- Carli T
- Carlinoa G
- Carminatia L
- Caron S
- Carona B
- Carter AA
- Carter JR
- Carvalhoa J
- Casadei D
- Casado MP
- Cascellaa M
- Casoa C
- Castaneda-Miranda E
- Castanheira MTD
- Castillo Gimenez V
- Castillo LRF
- Castro NF
- Cataldia G
- Cataneo F
- Catinaccio A
- Catmore JR
- Cattai A
- Cattani G
- Caughron S
- Cauza D
- Cavalcanti TP
- Cavalleri P
- Cavalli-Sforza M
- Cavallia D
- Cavasinnia V
- Ceradinia F
- Cerqueiraa AS
- Cerri A
- Cerrito L
- Cerutti F
- Cetinb SA
- Ceveninia F
- Chafaqa A
- Chakraborty D
- Chan K
- Chapleau B
- Chapman JD
- Chapman JW
- Chareyre E
- Charlton DG
- Chavda V
- Cheatham S
- Chekanov S
- Chekulaeva SV
- Chelkov GA
- Chelstowska MA
- Chen C
- Chen H
- Chen X
- Chenc S
- Chenc T
- Chenga S
- Cheong ALF
- Cheplakov A
- Chepurnov VF
- Cherkaoui El Moursli R
- Chernyatin V
- Cheu E
- Cheung SL
- Chevalier L
- Chiefaria G
- Chikovani L
- Childersa JT
- Chilingarov A
- Chiodinia G
- Chizhov MV
- Choudalakis G
- Chouridou S
- Christidi IA
- Christov A
- Chromek-Burckhart D
- Chu ML
- Chudoba J
- Ciapettia G
- Ciba K
- Ciftcia AK
- Ciftcia R
- Cinca D
- Cindro V
- Ciobotaru MD
- Cioccaa C
- Ciocio A
- Cirilli M
- Ciubancana M
- Clark A
- Clark PJ
- Cleland W
- Clemens JC
- Clement B
- Clementa C
- Clifft RW
- Coadou Y
- Cobala M
- Coccaroa A
- Cochran J
- Coe P
- Cogan JG
- Coggeshall J
- Cogneras E
- Cojocaru CD
- Colas J
- Colijn AP
- Collaboration ATLAS
- Collard C
- Collins NJ
- Collins-Tooth C
- Collot J
- Colon G
- Conde Muinoa P
- Coniavitis E
- Conidi MC
- Consonni M
- Consorti V
- Constantinescua S
- Contaa C
- Conventia F
- Cook J
- Cooke M
- Cooper BD
- Cooper-Sarkar AM
- Cooper-Smith NJ
- Copic K
- Cornelissena T
- Corradia M
- Correia AMH
- Corriveau F
- Cortes-Gonzalez A
- Cortiana G
- Costa MJ
- Costaa G
- Costanzo D
- Costin T
- Cote D
- Courneyea L
- Cowan G
- Cowden C
- Cox BE
- Cranmer K
- Crepe-Renaudin S
- Cresciolia F
- Cristinziani M
- Crosettia G
- Crupia R
- Cuciuca C-M
- Curatolo M
- Curtis CJ
- Cwetanski P
- Czirr H
- Czyczula Z
- D'Auria S
- D'Onofrio M
- D'Orazioa A
- da Costa JBG
- Da Costa JGPF
- Da Silvaa PVM
- Da Via C
- Dabrowski W
- Dai T
- Dallapiccola C
- Dam M
- Damazio DO
- Dameria M
- Damiani DS
- Danielsson HO
- Dannheim D
- Dao V
- Darboa G
- Darleab GL
- Daum C
- Dauvergne JP
- Davey W
- Davidek T
- Davidson N
- Davidson R
- Davies E
- Davies M
- Davison AR
- Davygoraa Y
- Dawe E
- Dawson I
- Dawson JW
- Daya RK
- de Asmundis R
- De Castroa S
- De Cecco S
- de Graat J
- De Groot N
- de Jong P
- De La Taille C
- De la Torre H
- de Lima JGR
- De Lottoa B
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- De Nooij L
- De Pedisa D
- De Regie JBDV
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- della Porta GZ
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- Devetak E
- Deviveiros PO
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- Dhaliwal S
- Dhullipudi R
- Di Ciaccio A
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- Di Girolamo A
- Di Girolamo B
- Di Luisea S
- Di Mattia A
- Di Micco B
- Di Nardo R
- Di Simone A
- Di Sipioa R
- Diaza MA
- Diblenc F
- Diehl EB
- Dietrich J
- Dietzscha TA
- Diglio S
- Dingfelder J
- Dionisia C
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- Yilmaz M
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- Zaidan R
- Zaitsev AM
- Zajacova Z
- Zalite YK
- Zanello L
- Zarzhitsky P
- Zaytsev A
- Zeitnitz C
- Zeller M
- Zeman M
- Zemla A
- Zendler C
- Zenin O
- Zenis T
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
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- Zhang Z
- Zhao L
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- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
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- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- zur Nedden M
- Zutshi V
- Zwalinski L
- Publication venue
- 'Elsevier BV'
- Publication date
- 01/01/2011
- Field of study
A measurement is presented of the inclusive cross-section for b-jet production in association with a Z boson in pp collisions at a centre-of-mass energy of root s = 7 TeV. The analysis uses the data sample collected by the ATLAS experiment in 2010, corresponding to an integrated luminosity of approximately 36 pb(-1). The event selection requires a Z boson decaying into high P-T electrons or muons, and at least one b-jet, identified by its displaced vertex, with transverse momentum p(T) > 25 GeV and rapidity vertical bar y vertical bar < 2.1. After subtraction of background processes, the yield is extracted from the vertex mass distribution of the candidate b-jets. The ratio of this cross-section to the inclusive Z cross-section (the average number of b-jets per Z event) is also measured. Both results are found to be in good agreement with perturbative QCD predictions at next-to-leading order
Search for strongly interacting massive particles generating trackless jets in proton-proton collisions at s = 13 TeV
- Author
- Aarrestad TK
- Aarup Petersen H
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams E
- Adams MR
- Adams T
- Adloff C
- Adzic P
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmed A
- Ahuja S
- Aime C
- Akchurin N
- Akgun B
- Akpinar A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Alcaraz Maestre J
- Aldaya Martin M
- Aldá Júnior WL
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
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- Zecchinelli AG
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- Zeuner WD
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- Zorbilmez C
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- Álvarez Fernández A
- Österberg K
- Özçelik Ö
- Široký J
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
A search for dark matter in the form of strongly interacting massive particles (SIMPs) using the CMS detector at the LHC is presented. The SIMPs would be produced in pairs that manifest themselves as pairs of jets without tracks. The energy fraction of jets carried by charged particles is used as a key discriminator to suppress efficiently the large multijet background, and the remaining background is estimated directly from data. The search is performed using proton-proton collision data corresponding to an integrated luminosity of 16.1 fb - 1 , collected with the CMS detector in 2016. No significant excess of events is observed above the expected background. For the simplified dark matter model under consideration, SIMPs with masses up to 100 GeV are excluded and further sensitivity is explored towards higher masses
Search for Higgs Boson Pair Production in the Four b Quark Final State in Proton-Proton Collisions at root s=13 TeV
- Author
- Aarrestad T
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WW
- Abdullin S
- Abercrombie D
- Abreu A
- Acharya H
- Acosta D
- Adam W
- Adamidis K
- Adams E
- Adams M
- Adams T
- Addesa F
- Adloff C
- Adzic P
- Adán DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmad WH
- Ahmed A
- Ahuja S
- Aime` C
- Akchurin N
- Akgun B
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- Yohay R
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- Yuan L
- Yuan S
- Yuldashev B
- Yumiceva F
- Yusli M
- Yzquierdo AP
- Zabi A
- Zacharopoulou A
- Zahid S
- Zaleski S
- Zalewski P
- Zanetti M
- Zarubin A
- Zarucki M
- Zecchinelli A
- Zeinali M
- Zeuner W
- Zghiche A
- Zhang F
- Zhang H
- Zhang J
- Zhang L
- Zhang W
- Zhang Y
- Zhang Z
- Zhao J
- Zhizhin I
- Zhokin A
- Zhu D
- Zhu R
- Ziemons T
- Zoi I
- Zolkapli Z
- Zorbakir I
- Zorbilmez C
- Zotto P
- Zotz A
- Zou D
- Zou R
- Zucchetta A
- Zumerle G
- Zuo X
- Zuolo D
- Zygala L
- Álvarez CR
- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2022
- Field of study
Search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks in proton-proton collisions at root s=13TeV
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
- Abdullah WATW
- Abdullin S
- Abercrombie D
- Acharya H
- Acosta D
- Acosta JG
- Adam W
- Adams E
- Adams MR
- Adams T
- Adloff C
- Adzic P
- Adán DP
- Afanasiev S
- Agapitos A
- Agarwal G
- Aggleton R
- Agram J-L
- Aguilar-Benitez M
- Ahmad A
- Ahmad M
- Ahmad WH
- Ahmed A
- Ahuja S
- Aime' C
- Akchurin N
- Akgun B
- Akpinar A
- Albajar C
- Albergo S
- Albert A
- Albrow M
- Aleksandrov A
- Alexander J
- Alhusseini M
- Alimena J
- Alison J
- Allen B
- Almond J
- Alonso AG
- Alvarez JDR
- Alverson G
- Alves GA
- Aly R
- Alyari M
- Amapane N
- Amaral SMSD
- Amendola C
- Amin N
- Amram O
- Amsler C
- Anagnostou G
- Anampa KH
- Anderson D
- Andrea J
- Andreev V
- Andreev Y
- Andrews MB
- Androsov K
- Angioni GLP
- Antchev G
- Antunovic Z
- Anuar AAB
- Apanasevich L
- Apollinari G
- Appelt E
- Apresyan A
- Apyan A
- Araujo M
- Arbelaez NV
- Arbol PMRD
- Arcaro D
- Arcidiacono R
- Arenton MW
- Argiro S
- Arneodo M
- Aruta C
- Asavapibhop B
- Asawatangtrakuldee C
- Asenov P
- Asghar MI
- Asilar E
- Askew A
- Asmuss P
- Atakisi IO
- Atanasov I
- Ather MW
- Attikis A
- Auffray E
- Aushev T
- Auzinger G
- Avati V
- Avery P
- Avila C
- Awan MIM
- Ayala E
- Ayala G
- Azarkin M
- Azhgirey I
- Aziz T
- Azzi P
- Azzurri P
- Baarmand MM
- Babaev A
- Babounikau I
- Bacchetta N
- Bachiller I
- Bachtis M
- Backhaus M
- Baden A
- Baechler J
- Bagliesi G
- Bahinipati S
- Baillon P
- Bainbridge R
- Bakas G
- Bakhshiansohi H
- Ball AH
- Ban Y
- Band R
- Bandyopadhyay H
- Banerjee S
- Banerjee S
- Banos LIE
- Bansal S
- Barbagli G
- Barberis E
- Bargassa P
- Baringer P
- Barnes VE
- Barney D
- Baron O
- Barrera CB
- Barrera CO
- Bartek R
- Bartosik N
- Bartók M
- Bastos D
- Battilana C
- Baty A
- Bauerdick LAT
- Baur S
- Baxter S
- Bayshev I
- Bean A
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- Beaudette F
- Becerra DAS
- Bechtel J
- Bedoya CF
- Beghin D
- Behera PK
- Behera SC
- Behnke O
- Bein S
- Belforte S
- Bell KW
- Bellan R
- Belloni A
- Bellora A
- Belyaev A
- Belyaev A
- Benaglia A
- Benato L
- Bencze G
- Bendavid J
- Benecke A
- Benelli G
- Beni N
- Benitez JF
- Benussi L
- Beretvas A
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- Özçelik Ö
- Publication venue
- Publication date
- 01/01/2018
- Field of study
A search for dark matter produced in association with a Higgs boson decaying to a pair of bottom quarks is performed in proton-proton collisions at a center-of-mass energy of 13 TeV collected with the CMS detector at the LHC. The analyzed data sample corresponds to an integrated luminosity of 35.9 fb(-1). The signal is characterized by a large missing transverse momentum recoiling against a bottom quark-antiquark system that has a large Lorentz boost. The number of events observed in the data is consistent with the standard model background prediction. Results are interpreted in terms of limits both on parameters of the type-2 two-Higgs doublet model extended by an additional light pseudoscalar boson a (2HDM+a) and on parameters of a baryonic Z simplified model. The 2HDM+a model is tested experimentally for the first time. For the baryonic Z model, the presented results constitute the most stringent constraints to date.Peer reviewe
A Deep Neural Network for Simultaneous Estimation of b Jet Energy and Resolution
- Author
- Aarrestad TK
- Abbaneo D
- Abbiendi G
- Abbrescia M
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- Publication venue
- Publication date
- 01/01/2020
- Field of study
We describe a method to obtain point and dispersion estimates for the energies of jets arising from b quarks produced in proton-proton collisions at an energy of s = 13 TeV at the CERN LHC. The algorithm is trained on a large sample of simulated b jets and validated on data recorded by the CMS detector in 2017 corresponding to an integrated luminosity of 41 fb - 1 . A multivariate regression algorithm based on a deep feed-forward neural network employs jet composition and shape information, and the properties of reconstructed secondary vertices associated with the jet. The results of the algorithm are used to improve the sensitivity of analyses that make use of b jets in the final state, such as the observation of Higgs boson decay to b b ¯
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