312 research outputs found
ES-Cell Derived Hematopoietic Cells Induce Transplantation Tolerance
- Author
- A Weissmann
- AJ Potocnik
- AJ Potocnik
- B Schiedlmeier
- Derya Unutmaz
- F Faendrich
- GR Honig
- J Antonchuk
- J Krosl
- K Chan
- KG Haanstra
- KM Bowles
- KM Chan
- Kun-Ming Chan
- L Wang
- M Kyba
- M Sykes
- N Zavazava
- Nicholas Zavazava
- NJ Robertson
- R Billingham
- R Billingham
- R Corry
- RK Burt
- S Bonde
- S Pilat
- Sabrina Bonde
- TM Schmitt
- TM Schmitt
- U Just
- XB Zhang
- Y Wang
- Publication venue
- Public Library of Science
- Publication date
- 01/01/2008
- Field of study
Background: Bone marrow cells induce stable mixed chimerism under appropriate conditioning of the host, mediating the induction of transplantation tolerance. However, their strong immunogenicity precludes routine use in clinical transplantation due to the need for harsh preconditioning and the requirement for toxic immunosuppression to prevent rejection and graft-versus-host disease. Alternatively, embryonic stem (ES) cells have emerged as a potential source of less immunogenic hematopoietic progenitor cells (HPCs). Up till now, however, it has been difficult to generate stable hematopoietic cells from ES cells. Methodology/Principal Findings: Here, we derived CD45 + HPCs from HOXB4-transduced ES cells and showed that they poorly express MHC antigens. This property allowed their long-term engraftment in sublethally irradiated recipients across MHC barriers without the need for immunosuppressive agents. Although donor cells declined in peripheral blood over 2 months, low level chimerism was maintained in the bone marrow of these mice over 100 days. More importantly, chimeric animals were protected from rejection of donor-type cardiac allografts. Conclusions: Our data show, for the first time, the efficacy of ES-derived CD45 + HPCs to engraft in allogenic recipient
VASCo: computation and visualization of annotated protein surface contacts
- Author
- A Kuglstatter
- A Nicholls
- A Porollo
- A Valencia
- AD Kern
- AG Murzin
- AK Ghose
- AK Ghose
- B Honig
- C Breithaupt
- C Breithaupt
- C Giacovazzo
- C Oubridge
- Christoph Kratky
- DA Pearlman
- E Audry
- F Eisenhaber
- F Eisenhaber
- G Franzot
- Georg Steinkellner
- Gerhard G Thallinger
- GR Smith
- H Berman
- HM Berman
- J Teyra
- K Henrick
- Karl Gruber
- KV Brinda
- M Hall
- M Weisel
- M Zviling
- MA Verdecia
- MF Sanner
- ML Connolly
- N Guex
- OV Tsodikov
- RB Russell
- Robert Rader
- RP Bahadur
- S Albeck
- S De
- S Jones
- S Jones
- S Shazman
- SJ Darnell
- SJ Wodak
- VN Viswanadhan
- W Heiden
- Y Ofran
- Publication venue
- BioMed Central
- Publication date
- 01/01/2009
- Field of study
<p>Abstract</p> <p>Background</p> <p>Structural data from crystallographic analyses contain a vast amount of information on protein-protein contacts. Knowledge on protein-protein interactions is essential for understanding many processes in living cells. The methods to investigate these interactions range from genetics to biophysics, crystallography, bioinformatics and computer modeling. Also crystal contact information can be useful to understand biologically relevant protein oligomerisation as they rely in principle on the same physico-chemical interaction forces. Visualization of crystal and biological contact data including different surface properties can help to analyse protein-protein interactions.</p> <p>Results</p> <p>VASCo is a program package for the calculation of protein surface properties and the visualization of annotated surfaces. Special emphasis is laid on protein-protein interactions, which are calculated based on surface point distances. The same approach is used to compare surfaces of two aligned molecules. Molecular properties such as electrostatic potential or hydrophobicity are mapped onto these surface points. Molecular surfaces and the corresponding properties are calculated using well established programs integrated into the package, as well as using custom developed programs. The modular package can easily be extended to include new properties for annotation. The output of the program is most conveniently displayed in PyMOL using a custom-made plug-in.</p> <p>Conclusion</p> <p>VASCo supplements other available protein contact visualisation tools and provides additional information on biological interactions as well as on crystal contacts. The tool provides a unique feature to compare surfaces of two aligned molecules based on point distances and thereby facilitates the visualization and analysis of surface differences.</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
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov A
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparisi Pozo JA
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya ST
- Arcangeletti C
- Arce ATH
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Artz S
- Asai S
- Asawatavonvanich T
- Asbah N
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Augsten K
- Avolio G
- Ayoub MK
- Azuelos G
- Bachacou H
- Bachas K
- Backes M
- Backman F
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
- Balaji S
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandyopadhyay A
- Banerjee S
- Bannoura AAE
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- Zemaityte G
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- Zhang B
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- Zhang H
- Zhang J
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- 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
α-thalassaemia
- Author
- A Cao
- A Zorai
- AC Kattamis
- AM Michelson
- AO Wilkie
- AO Wilkie
- AO Wilkie
- AO Wilkie
- AR Cohen
- ASC Tan
- AV Hill
- B Bellosillo
- B Eng
- BJ Bain
- C Dame
- C Kattamis
- C Liao
- C Suwanrath-Kengpol
- C Velati
- CL Harteveld
- CL Harteveld
- CL Harteveld
- Cornelis L Harteveld
- CS Richards
- D Todd
- DH Chui
- DH Chui
- DH Chui
- DJ Weatherall
- DJ Weatherall
- DJ Weatherall
- DJ Weatherall
- DJ Weatherall
- DM Hunt
- Douglas R Higgs
- DR Higgs
- DR Higgs
- DR Higgs
- DR Higgs
- DR Higgs
- DR Higgs
- DR Higgs
- DR Higgs
- DR Higgs
- DR Higgs
- DR Higgs
- DW Bianchi
- E Jauniaux
- E Kanavakis
- E Mirabile
- E Whitelaw
- EA Zimmer
- EP Vichinsky
- F Kutlar
- F Lorey
- FE Chen
- G Modiano
- GC Ooi
- GP Patrinos
- GR Honig
- GT Yuregir
- GW Hall
- H Wajcman
- J Flint
- J Flint
- J Lauer
- J Slomp
- J Tan
- J Traeger-Synodinos
- J Traeger-Synodinos
- J Traeger-Synodinos
- JB Clegg
- JB Clegg
- JB Clegg
- JF Hess
- JP Schouten
- JS Waye
- JS Waye
- JS Yi
- KH Nicolaides
- KL McBride
- L Bernini
- L Pressley
- LE Lie-Injo
- LF Bernini
- LL Pan
- M Goossens
- M Petrou
- MA Beaudry
- MA Curuk
- MJ Rugless
- MO Arcasoy
- N Fischel-Ghodsian
- NF Olivieri
- NI Noguera
- P Delft van
- P Moi
- P Tabone
- P Winichagoon
- PC Giordano
- PC Ng
- R Fodde
- R Galanello
- R Galanello
- R Galanello
- R Gibbons
- R Nakayama
- R Origa
- RJ Gibbons
- RJ Gibbons
- RJ Trent
- RJ Trent
- S Fucharoen
- S Fucharoen
- S Henderson
- SH Embury
- SJ White
- SL Schrier
- SL Thein
- SS Chong
- ST Liang
- ST Singer
- SY Lee
- SY Lee
- T Lucke
- T Sanguansermsri
- TB Bradley
- TL Stockley
- TM Ko
- TM Lin
- TP Molchanova
- V Chan
- V Chan
- V Chan
- V Laosombat
- V Viprakasit
- VM Ingram
- W Holzgreve
- WW De Jong
- X Zhou
- YL Lau
- YT Liu
- Publication venue
- BioMed Central
- Publication date
- 01/01/2010
- Field of study
Alpha-thalassaemia is inherited as an autosomal recessive disorder characterised by a microcytic hypochromic anaemia, and a clinical phenotype varying from almost asymptomatic to a lethal haemolytic anaemia
Muon reconstruction and identification efficiency in ATLAS using the full Run 2 pp collision data set at \sqrt{s}=13 TeV
- 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
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agapopoulou C
- Agaras MN
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ahnen JV
- Ai X
- Aielli G
- Akatsuka S
- Akbiyik M
- Akesson TPA
- Akilli E
- Akimov AV
- Alberghi GL
- Albert J
- Alderweireldt S
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexopoulos T
- Alfonsi A
- Alfonsi F
- Alhroob M
- Ali B
- Ali S
- Aliev M
- Alimonti G
- Allaire C
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amrouche CS
- An F
- Anastopoulos C
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Andrei V
- Anelli CR
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparo MA
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arguin J-F
- Argyropoulos S
- Arling J-H
- Armbruster AJ
- Armstrong A
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asawatavonvanich T
- Asbah NA
- Asimakopoulou EM
- Asquith L
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
- Augsten K
- Austrup VA
- Avolio G
- Ayoub MK
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Backman F
- Bagnaia P
- Bahilo JJL
- Bahrasemani H
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
- Bakos E
- Balaji S
- Balasubramanian R
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Balz J
- Banas E
- Bandieramonte M
- Bandyopadhyay A
- Banerjee S
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barillari T
- Barisits M-S
- Barkeloo J
- Barklow T
- Barnea R
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barron U
- Barsov S
- Bartels F
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
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- Batlamous S
- Batley JR
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- Bauce M
- Bauer F
- Bauer P
- Bawa HS
- Bayirli A
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HC
- Beck HP
- Becker K
- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beisiegel F
- Belfkir M
- Bell AS
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev NL
- Benchekroun D
- Benekos N
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Bergmann B
- Bergsten LJ
- Beringer J
- Berlendis S
- Berlingen JM
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Berthold A
- Bertram IA
- Besson N
- Bethke S
- Betti A
- Bevan AJ
- Beyer J
- Bhatta S
- Bhattacharya DS
- Bhattarai P
- Bhopatkar VS
- Bi R
- Bianchi RM
- Biebel O
- Biedermann D
- Bielski R
- Bierwagen K
- Biesuz NV
- Biglietti M
- Billoud TRV
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Birch-sykes CJ
- Birman M
- Bisanz T
- Biswal JP
- Biswas D
- Bitadze A
- Bittrich C
- Bjorke K
- Blazek T
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Boeriu OEV
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bolanos GR
- Bold T
- Bolz AE
- Bomben M
- Bona M
- Bonilla JS
- Boonekamp M
- Booth CD
- Borbely AG
- Borecka-Bielska HM
- Borgna LS
- Borisov A
- Borissov G
- Bortoletto D
- Bosca SR
- Boscherini D
- Bosman M
- Bostanabad MG
- Bouaouda K
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios CA
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- Bozson AJ
- Bracinik J
- Brahimi N
- Brandt G
- Brandt O
- Braren F
- Brau B
- Brau JE
- Brendlinger K
- Brener R
- Brenner L
- Brenner R
- Bressler S
- Bret MC
- Brickwedde B
- Briglin DL
- Britton D
- Britzger D
- Brock I
- Brock R
- Brooijmans G
- Brooks WK
- Brost E
- Brueers B
- Bruncko D
- Bruni A
- Bruni G
- Bruschi M
- Bruscino N
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Buescher V
- Bugge MK
- Bulekov O
- Bullard BA
- Burch TJ
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Buschmann E
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Butti P
- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund OB
- Cabras G
- Caforio D
- Cai H
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Caltabiano A
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camarda S
- Camarri P
- Camelia EA
- Camerlingo MT
- Cameron D
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Canale V
- Canesse A
- Cantero J
- Cao T
- Cao Y
- Capriles FGD
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- Ye S
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- Yexley MR
- Yigitbasi E
- Yildiz HD
- Yin P
- 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
- Zeissner SV
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang DF
- Zhang G
- Zhang J
- Zhang K
- Zhang L
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang X
- Zhang Y
- Zhang Z
- Zhang Z
- Zhao P
- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou H
- Zhou M
- 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 NI
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2021
- Field of study
This article documents the muon reconstruction and identification efficiency obtained by the ATLAS experiment for 139 \hbox {fb}^{-1} of pp collision data at \sqrt{s}=13 TeV collected between 2015 and 2018 during Run 2 of the LHC. The increased instantaneous luminosity delivered by the LHC over this period required a reoptimisation of the criteria for the identification of prompt muons. Improved and newly developed algorithms were deployed to preserve high muon identification efficiency with a low misidentification rate and good momentum resolution. The availability of large samples of Z\rightarrow \mu \mu and J/\psi \rightarrow \mu \mu decays, and the minimisation of systematic uncertainties, allows the efficiencies of criteria for muon identification, primary vertex association, and isolation to be measured with an accuracy at the per-mille level in the bulk of the phase space, and up to the percent level in complex kinematic configurations. Excellent performance is achieved over a range of transverse momenta from 3 GeV to several hundred GeV, and across the full muon detector acceptance of |\eta |<2.7
Search for bottom-squark pair production in pp collision events at √s=13 TeV with hadronically decaying τ-leptons, b-jets, and missing transverse momentum using the ATLAS detector
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- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
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- Zemaityte G
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- Zhao Y
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu Y
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- Zhulanov V
- Zieminska D
- Zimine N
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- Zorbas TG
- Zou R
- Zwalinski L
- Publication venue
- AMER PHYSICAL SOC
- Publication date
- 01/08/2021
- Field of study
A search for pair production of bottom squarks in events with hadronically decaying
τ
-leptons,
b
-tagged jets, and large missing transverse momentum is presented. The analyzed dataset is based on proton-proton collisions at
√
s
=
13
TeV
delivered by the Large Hadron Collider and recorded by the ATLAS detector from 2015 to 2018, and corresponds to an integrated luminosity of
139
fb
−
1
. The observed data are compatible with the expected Standard Model background. Results are interpreted in a simplified model where each bottom squark is assumed to decay into the second-lightest neutralino
˜
χ
0
2
and a bottom quark, with
˜
χ
0
2
decaying into a Higgs boson and the lightest neutralino
˜
χ
0
1
. The search focuses on final states where at least one Higgs boson decays into a pair of hadronically decaying
τ
-leptons. This allows the acceptance and thus the sensitivity to be significantly improved relative to the previous results at low masses of the
˜
χ
0
2
, where bottom-squark masses up to 850 GeV are excluded at the 95% confidence level, assuming a mass difference of 130 GeV between
˜
χ
0
2
and
˜
χ
0
1
. Model-independent upper limits are also set on the cross section of processes beyond the Standard Model
Erratum: Measurement of angular and momentum distributions of charged particles within and around jets in Pb + Pb and pp collisions at √sNN = 5.02 TeV with the ATLAS detector [Phys. Rev. C 100 , 064901 (2019)]
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- Abbott B
- Abbott Dc
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- Abeling K
- Abhayasinghe Dk
- Abidi Sh
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- Black Km
- Blazek T
- Bloch I
- Blocker C
- Blue A
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- Bobbink Gj
- Bobrovnikov Vs
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- Bocci A
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- Bogavac D
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- Boscherini D
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- Bruckman De Renstrom Pa
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- Buat Q
- Buchholz P
- Buckley Ag
- Budagov Ia
- Bugge Mk
- Buhrer F
- Bulekov O
- Burch Tj
- Burdin S
- Burgard Cd
- Burger Am
- Burghgrave B
- Burr Jtp
- Burton Cd
- Burzynski Jc
- Buscher V
- Buschmann E
- Bussey Pj
- Butler Jm
- Buttar Cm
- Butterworth Jm
- Butti P
- Buttinger W
- Buxo Vazquez Cj
- Buzatu A
- Buzykaev Ar
- Cabras G
- Cabrera Urban S
- Caforio D
- Cai H
- Cairo Vmm
- Cakir O
- Calace N
- Calafiura P
- Calandri A
- Calderini G
- Calfayan P
- Callea G
- Caloba Lp
- Calvente Lopez S
- Calvet D
- Calvet S
- Calvet Tp
- Calvetti M
- Camacho Toro R
- Camarda S
- Camarero Munoz D
- Camarri P
- Cameron D
- Caminal Armadans R
- Camincher C
- Campana S
- Campanelli M
- Camplani A
- Campoverde A
- Canale V
- Canesse A
- Cano Bret M
- Cantero J
- Cao T
- Cao Y
- Capeans Garrido Mdm
- Capua M
- Cardarelli R
- Cardillo F
- Carducci G
- Carli I
- Carli T
- Carlino G
- Carlson Bt
- Carminati L
- Carney Rmd
- Caron S
- Carquin E
- Carra S
- Carter Jws
- Casado Mp
- Casha Af
- Casper Dw
- Castelijn R
- Castillo Gimenez V
- Castillo Fl
- Castro Nf
- Catinaccio A
- Catmore Jr
- Cattai A
- Caudron J
- Cavaliere V
- Cavallaro E
- Cavalli-Sforza M
- Cavasinni V
- Celebi E
- Ceradini F
- Cerda Alberich L
- Cerny K
- Cerqueira As
- Cerri A
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- Cervelli A
- Cetin Sa
- Chadi Z
- Chakraborty D
- Chan Sk
- Chan Ws
- Chan Wy
- Chapman Jd
- Chargeishvili B
- Charlton Dg
- Charman Tp
- Chau Cc
- Che S
- Chekanov S
- Chekulaev Sv
- Chelkov Ga
- Chelstowska Ma
- Chen B
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- Chen Ch
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- Chen X
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- Cheng Hc
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- Cheplakov A
- Cheremushkina E
- Cherkaoui El Moursli R
- Cheu E
- Cheung K
- Chevalerias Tja
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm As
- Chitan A
- Chiu I
- Chiu Yh
- Chizhov Mv
- Choi K
- Chomont Ar
- Chouridou S
- Chow Ys
- Chu Mc
- Chu X
- Chudoba J
- Chuinard Aj
- Chwastowski Jj
- Chytka L
- Cieri D
- Ciesla Km
- Cinca D
- Cindro V
- Cioara Ia
- Ciocio A
- Cirotto F
- Citron Zh
- Citterio M
- Ciubotaru Da
- Ciungu Bm
- Clark A
- Clark Mr
- Clark Pj
- Clement C
- Coadou Y
- Cobal M
- Coccaro A
- Cochran J
- Cohen H
- Coimbra Aec
- Colasurdo L
- Cole B
- Colijn Ap
- Collot J
- Conde Muino P
- Coniavitis E
- Connell Sh
- Connelly Ia
- Constantinescu S
- Conventi F
- Cooper-Sarkar Am
- Cormier F
- Cormier Kjr
- Corpe Ld
- Corradi M
- Corrigan Ee
- Corriveau F
- Cortes-Gonzalez A
- Costa Mj
- Costanza F
- Costanzo D
- Cowan G
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- Zheng Z
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- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas Tg
- Zou R
- Zwalinski L
- Publication venue
- American Physical Society
- Publication date
- 01/01/2020
- Field of study
Measurement of the tt¯tt¯ production cross section in pp collisions at √s=13 TeV with the ATLAS detector
- Author
- Aad G
- Abbott B
- Abbott DC
- Abed Abud A
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Abramowicz H
- Abreu H
- Abulaiti Y
- Abusleme Hoffman AC
- Acharya BS
- Achkar B
- Adam Bourdarios C
- Adam L
- Adamczyk L
- Adamek L
- Adelman J
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- Adorni S
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- Afik Y
- Agapopoulou C
- Agaras MN
- Agarwala J
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- Alberghi GL
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- Aleksa M
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- Zeißner SV
- Zemaityte G
- Zeng JC
- Zenin O
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhu HL
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- Zhu Y
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- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine NI
- Zimmermann S
- Ziolkowski M
- Zoccoli A
- Zoch K
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- Zwalinski L
- Åkesson TPA
- Öncel ÖO
- Ženiš T
- Živković L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 16/11/2021
- Field of study
A measurement of four-top-quark production using proton-proton collision data at a centre-of-mass energy of 13 TeV collected by the ATLAS detector at the Large Hadron Collider corresponding to an integrated luminosity of 139 fb−1 is presented. Events are selected if they contain a single lepton (electron or muon) or an opposite-sign lepton pair, in association with multiple jets. The events are categorised according to the number of jets and how likely these are to contain b-hadrons. A multivariate technique is then used to discriminate between signal and background events. The measured four-top-quark production cross section is found to be 26+17−15 fb, with a corresponding observed (expected) significance of 1.9 (1.0) standard deviations over the background-only hypothesis. The result is combined with the previous measurement performed by the ATLAS Collaboration in the multilepton final state. The combined four-top-quark production cross section is measured to be 24+7−6 fb, with a corresponding observed (expected) signal significance of 4.7 (2.6) standard deviations over the background-only predictions. It is consistent within 2.0 standard deviations with the Standard Model expectation of 12.0 ± 2.4 fb
Measurement of single top-quark production in association with a W boson in the single-lepton channel at \sqrt{s} = 8\,\text {TeV} with the ATLAS detector
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zimmermann S
- Zinonos Z
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- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 01/01/2021
- Field of study
The production cross-section of a top quark in association with a W boson is measured using proton–proton collisions at \sqrt{s} = 8\,\text {TeV}. The dataset corresponds to an integrated luminosity of 20.2\,\text {fb}^{-1}, and was collected in 2012 by the ATLAS detector at the Large Hadron Collider at CERN. The analysis is performed in the single-lepton channel. Events are selected by requiring one isolated lepton (electron or muon) and at least three jets. A neural network is trained to separate the tW signal from the dominant t{\bar{t}} background. The cross-section is extracted from a binned profile maximum-likelihood fit to a two-dimensional discriminant built from the neural-network output and the invariant mass of the hadronically decaying W boson. The measured cross-section is \sigma _{tW} = 26 \pm 7\,\text {pb}, in good agreement with the Standard Model expectation
Measurements of Higgs bosons decaying to bottom quarks from vector boson fusion production with the ATLAS experiment at √=13TeV
- Author
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- Abbott B
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- Abhayasinghe DK
- Abidi SH
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- Buttinger W
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- Öncel ÖO
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- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 23/06/2021
- Field of study
The paper presents a measurement of the Standard Model Higgs Boson decaying to b-quark pairs in the vector boson fusion (VBF) production mode. A sample corresponding to 126 fb−1 of s√=13TeV proton–proton collision data, collected with the ATLAS experiment at the Large Hadron Collider, is analyzed utilizing an adversarial neural network for event classification. The signal strength, defined as the ratio of the measured signal yield to that predicted by the Standard Model for VBF Higgs production, is measured to be 0.95+0.38−0.36 , corresponding to an observed (expected) significance of 2.6 (2.8) standard deviations from the background only hypothesis. The results are additionally combined with an analysis of Higgs bosons decaying to b-quarks, produced via VBF in association with a photon
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