337 research outputs found
Tension-Enhanced Hydrogen Evolution Reaction on Vanadium Disulfide Monolayer
- Author
- A Tavangar
- BL Dou
- BY Xia
- C Tsai
- C Tsai
- CG Morales-Guio
- D Voiry
- D Voiry
- FH Saadi
- G Cipriani
- G Kresse
- G Kresse
- H Li
- H Pan
- H Pan
- H Pan
- HJ Monkhorst
- Hui Pan
- J Andrews
- J Gressley
- J Kibsgaard
- J Lin
- J Yang
- JH Lee
- JL Contreras
- JP Perdew
- JP Shi
- K Christopher
- K Xu
- M Carmo
- MA Lukowski
- MA Lukowski
- P Hohenberg
- PE Blöchl
- R Vedarajan
- RY Sun
- T Hisatomi
- TY Chen
- TY Yung
- WF Chen
- XH Lu
- XM Geng
- XN Peng
- XW Zhang
- XX Yuan
- Y Qu
- Y Qu
- Y Yan
- YF Yu
- YH Fang
- YH Fang
- YZ Lu
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
3D extracellular matrix microenvironment in bioengineered tissue models of primary pediatric and adult brain tumors.
- Author
- A Audia
- A Li
- A Rape
- A Varone
- A Wade
- AJ Engler
- B Ananthanarayanan
- B Delpech
- B Hegedus
- BJ Gill
- C Jones
- C Remy
- C Wang
- CA Alonzo
- CG Hubert
- CJ Medberry
- CL Evans
- CM Nelson
- D Guo
- D Sood
- DJ Silver
- DM Cairns
- DM Tiek
- DP Ivanov
- E Stuntz
- EJ Delikatny
- F Geng
- H Xu
- J Cofre
- JJ Phillips
- K Chwalek
- KB Pointer
- KP Quinn
- KP Quinn
- L Yu
- M Snuderl
- MA Digman
- MA Qazi
- MD Tang-Schomer
- MJ Bissell
- N Kawano
- NB Schwartz
- P Yu
- PF Ledur
- Q Ni
- QT Ostrom
- R Chen
- R Reinartz
- RK Nuttall
- S Avram
- S Yadavilli
- SS Patil
- SY Lee
- TE Merchant
- TN Ignatova
- TR Alves
- TT Le
- TY Fan
- VM Tran
- YH Zhou
- Z Liu
- Z Liu
- Publication venue
- The Mouseion at the JAXlibrary
- Publication date
- 04/10/2019
- Field of study
Dynamic alterations in the unique brain extracellular matrix (ECM) are involved in malignant brain tumors. Yet studies of brain ECM roles in tumor cell behavior have been difficult due to lack of access to the human brain. We present a tunable 3D bioengineered brain tissue platform by integrating microenvironmental cues of native brain-derived ECMs and live imaging to systematically evaluate patient-derived brain tumor responses. Using pediatric ependymoma and adult glioblastoma as examples, the 3D brain ECM-containing microenvironment with a balance of cell-cell and cell-matrix interactions supports distinctive phenotypes associated with tumor type-specific and ECM-dependent patterns in the tumor cells\u27 transcriptomic and release profiles. Label-free metabolic imaging of the composite model structure identifies metabolically distinct sub-populations within a tumor type and captures extracellular lipid-containing droplets with potential implications in drug response. The versatile bioengineered 3D tumor tissue system sets the stage for mechanistic studies deciphering microenvironmental role in brain tumor progression
Numerical study of nano-biofilm stagnation flow from a nonlinear stretching/shrinking surface with variable nanofluid and bioconvection transport properties
- Author
- A Javid
- AJ Hillesdon
- AT Brimmo
- AV Kuznetsov
- AV Kuznetsov
- AV Kuznetsov
- AV Kuznetsov
- B Yuan
- BM Morrisand
- C Wang
- DP Bakker
- E Paul
- G Adomian
- H Schlichting
- H Tsuji
- J Buongiorno
- JJ Batteh
- K Zaimi
- M Nasir
- M Nematolahi
- N Begum
- P Desmond
- P Geng
- P Geng
- R Kumar
- R Mehmood
- S Ghorai
- S Yao
- SE Ahmed
- TJ Pedley
- TJ Pedley
- TR Mahapatra
- TY Na
- W Ibrahim
- X Liao
- Y Pechaud
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 10/05/2021
- Field of study
A mathematical model is developed for stagnation point flow toward a stretching or shrinking sheet of liquid nano-biofilm containing spherical nano-particles and bioconvecting gyrotactic micro-organisms. Variable transport properties of the liquid (viscosity, thermal conductivity, nano-particle species diffusivity) and micro-organisms (species diffusivity) are considered. Buongiornoâs two-component nanoscale model is deployed and spherical nanoparticles in a dilute nanofluid considered. Using a similarity transformation, the nonlinear systems of partial differential equations is converted into nonlinear ordinary differential equations. These resulting equations are solved numerically using a central space finite difference method in the CodeBlocks Fortran platform. Graphical plots for the distribution of reduced skin friction coefficient, reduced Nusselt number, reduced Sherwood number and the reduced local density of the motile microorganisms as well as the velocity, temperature, nanoparticle volume fraction and the density of motile microorganisms are presented for the influence of wall velocity power-law index (m), viscosity parameter (c2), thermal conductivity parameter (c4), nano-particle mass diffusivity (c6), micro-organism species diffusivity (c8), thermophoresis parameter (Nt), Brownian motion parameter (Nb), Lewis number (Le), bioconvection Schmidt number (Sc), bioconvection constant (Ï) and bioconvection PĂ©clet number (Pe). Validation of the solutions via comparison related to previous simpler models is included. Further verification of the general model is conducted with the Adomian decomposition method (ADM). Extensive interpretation of the physics is included. Skin friction is elevated with viscosity parameter (c2) whereas it is suppressed with greater Lewis number and thermophoresis parameter. Temperatures are elevated with increasing thermal conductivity parameter (c4) whereas Nusselt numbers are reduced. Nano-particle volume fraction (concentration) is enhanced with increasing nano-particle mass diffusivity parameter (c6) whereas it is markedly reduced with greater Lewis number (Le) and Brownian motion parameter (Nb). With increasing stretching/shrinking velocity power-law exponent (m), skin friction is decreased whereas Nusselt number and Sherwood number are both elevated. Motile microorganism density is boosted strongly with increasing micro-organism diffusivity parameter (c8) and Brownian motion parameter (Nb) but reduced considerably with greater bioconvection Schmidt number (Sc) and bioconvection PĂ©clet number (Pe). The simulations find applications in deposition processes in nano-bio-coating manufacturing processes
Patterns of medical pluralism among adults: results from the 2001 National Health Interview Survey in Taiwan
- Author
- A Burke
- AA Izzo
- AA Izzo
- AM Whelan
- AP Wu
- C Chi
- C Chi
- C Chi
- C Pisinger
- C Wade
- C Wade
- CC Liao
- CC Liu
- CC Shih
- CCL Xue
- CH Shih YT
- Chien-Chang Liao
- Chun-Chuan Shih
- CK Landy
- D Lai
- DK Amre
- DM Eisenberg
- DM Eisenberg
- DW Hosmer
- FL Bishop
- FP Chen
- H MacPherson
- HA Tindle
- I Wolffers
- J Yazdany
- Jaung-Geng Lin
- JT Coon
- JT Kang
- K Roy
- KJ Kemper
- KJ Kemper
- L Pulkki
- LC Chang
- LG Miller
- LL Yeh
- M Daly
- M Kim
- MH Cohen
- MP Davis
- MS Wetzel
- N Huang
- NE Waxler
- NE Waxler-Morrison
- O Gefeller
- PM Barnes
- RA Cooper
- RC Kessler
- RE Graham
- RL Page
- S Demeter
- SF Shih
- SL Gall
- SM Ahmed
- TS Yu
- TY Chan
- V Chung
- VCH Chung
- WC Tsai
- WC Tsai
- Yi-Chang Su
- Publication venue
- BioMed Central
- Publication date
- 01/01/2010
- Field of study
Spatial variability and temporal trends of HCH and DDT in soils around Beijing Guanting Reservoir, China
- Author
- A Covaci
- A Polder
- BG Loganathan
- CH Marvin
- Chunli Chen
- F Borghini
- G Wang
- Guang Wang
- H Hung
- H Zhang
- HY Zhang
- J Li
- JB Wei
- Jing Geng
- John P. Giesy
- K Feng
- KSB Miglioranza
- KSB Miglioranza
- KSB Miglioranza
- M Manz
- MT Wan
- ND Xue
- ND Xue
- P Shegunova
- R Gioia
- S Tao
- S Villa
- SK Gaw
- T Harner
- T Poolpak
- Tieyu Wang
- TY Wang
- TY Wang
- TY Wang
- VD Toan
- W Luo
- Wei Luo
- Wentao Jiao
- Wenyou Hu
- XH Li
- XH Li
- XL Yang
- Y Shi
- Yajuan Shi
- YF Zhu
- Yonglong Lu
- YP Lin
- ZM Gong
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Effect of Paclitaxel-Mesoporous Silica Nanoparticles with a Core-Shell Structure on the Human Lung Cancer Cell Line A549
- Author
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- Field of study
Search for High-Mass Resonances Decaying to ÏÎœ in pp Collisions at âs=13 TeV with the ATLAS Detector
- Author
- Aaboud M
- Aad G
- Abbott B
- Abdinov O
- Abeloos B
- Abidi SH
- AbouZeid OS
- Abraham NL
- Abramowicz H
- Abreu H
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Afik Y
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akesson TPA
- 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
- Aliev M
- 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
- Alvarez Piqueras D
- 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
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antonelli M
- Antrim DJ
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Araujo Ferraz V
- Araujo Pereira R
- Araya S Tapia
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Armadans R Caminal
- Armbruster AJ
- Armitage LJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asimakopoulou EM
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga ME Pozo
- Atkin RJ
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Avramidou R
- Axen B
- Ayoub MK
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Baines JT
- Bajic M
- Baker OK
- Bakker PJ
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Banas E
- Bandyopadhyay A
- Banerjee Sw
- Bannoura AAE
- Barak L
- Barbe WM
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M-S
- Barkeloo JT
- Barklow T
- Barlow N
- Barnea R
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro Guimaraes da Costa J
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
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- Bates RL
- Batista SJ
- Batley JR
- Battaglia M
- Bauce M
- Bauer F
- Bauer KT
- Bawa HS
- Beacham JB
- Beattie MD
- Beau T
- Beauchemin PH
- Bechtle P
- Beck HC
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- Becker K
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- Becot C
- Beddall A
- Beddall AJ
- Bednyakov VA
- Bedognetti M
- Bee CP
- Beermann TA
- Begalli M
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- Behera A
- Behr JK
- Bell AS
- Bella G
- Bella L Aperio
- Bellagamba L
- Bellerive A
- Bellomo M
- Belotskiy K
- Belyaev NL
- Benary O
- Benchekroun D
- Bender M
- Benekos N
- Benhammou Y
- Benitez J
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
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- Berge D
- Berger N
- Bergsten LJ
- Beringer J
- Berlendis S
- Berlingen J Montejo
- Bernard NR
- Bernardi G
- Bernius C
- Bernlochner FU
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- Berta P
- Bertella C
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- Bertram IA
- Bertsche C
- Besjes GJ
- Bessner M
- Besson N
- Bethani A
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- Bianchi RM
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- Biedermann D
- Bielski R
- Bierwagen K
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- Biglietti M
- Billoud TRV
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- Black JE
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- Bobbink GJ
- Bobrovnikov VS
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- Bogdanchikov AG
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- Boldyrev AS
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- Butterworth JM
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- Buttinger W
- Buzatu A
- Buzykaev AR
- Bylund O Bessidskaia
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- Cakir I Turk
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- Chekanov S
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- Cheremushkina E
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- Chevalier L
- Chiarella V
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- Chiodini G
- Chisholm AS
- Chitan A
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- Chiu YH
- Chizhov MV
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- Chomont AR
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- Christodoulou V
- Chu MC
- Chudoba J
- Chuinard AJ
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- Correia AM Henriques
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- Czodrowski P
- D'amen G
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- D'eramo L
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- Da Cunha Sargedas De Sousa MJ
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- Dabrowski W
- Dado T
- Dahbi S
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- Dam M
- Damazio D Oliveira
- Dandoy JR
- Daneri MF
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- de Renstrom PA Bruckman
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- Di Ciaccio A
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- Di Clemente WK
- Di Donato C
- Di Girolamo A
- Di Micco B
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- Di Simone A
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- Diehl EB
- Dietrich J
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- Djuvsland JI
- do Vale MAB
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- Donszelmann T Cuhadar
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- Dubreuil A
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- Ducourthial A
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- Duehrssen M
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- Duffield EM
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- Dulsen C
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- Dumitriu AE
- Duncan AK
- Dunford M
- Duperrin A
- Durglishvili A
- Duschinger D
- Dutta B
- Duvnjak D
- Dyndal M
- Dziedzic BS
- Eckardt C
- Ecker KM
- Edgar RC
- Eifert T
- Eigen G
- Einsweiler K
- Ekelof T
- El Kacimi M
- El Kosseifi R
- El Moursli R Cherkaoui
- Ellajosyula V
- Ellert M
- Ellinghaus F
- Elliot AA
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- Favareto A
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- Fleischmann P
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- Formica A
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- Zhemchugov A
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- Zhou N
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- Zhu CG
- Zhu H
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- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zibell A
- Zieminska D
- 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 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
- Abraham NL
- Abramowicz H
- Abreu H
- Abreu R
- Abulaiti Y
- Acharya BS
- Adachi S
- Adamczyk L
- Adelman J
- Adersberger M
- Adye T
- Affolder AA
- Afik Y
- Agatonovic-Jovin T
- Agheorghiesei C
- Aguilar-Saavedra JA
- Ahlen SP
- Ahmadov F
- Aielli G
- Akatsuka S
- Akerstedt H
- Akesson TPA
- Akilli E
- Akimov AV
- Albergh GL
- Albert J
- Albicocco P
- Alconada Verzini MJ
- Alderweireldt SC
- Aleksa M
- Aleksandrov IN
- Alexa C
- Alexander G
- Alexopoulos T
- Alhroob M
- Ali B
- Aliev M
- Alimonti G
- Alison J
- Alkire SP
- Allbrooke BMM
- Allen BW
- Allport PP
- Aloisio A
- Alonso A
- Alonso F
- Alpigiani C
- Alshehri AA
- Alstaty MI
- Alvarez Piqueras D
- Alviggi MG
- Amadio BT
- Amelung C
- Amidei D
- Amoroso S
- Amundsen G
- Anastopoulos C
- Ancu LS
- Andari N
- Andeen T
- Anders CF
- Anders JK
- Anderson KJ
- Andreazza A
- Andrei V
- Angelidakis S
- Angelozzi I
- Angerami A
- Anisenkov AV
- Anjos N
- Annovi A
- Antel C
- Antonelli M
- Antonov A
- Antrim DJ
- Anulli F
- Aoki M
- Arabidze G
- Arai Y
- Araque JP
- Arce ATH
- Ardell RE
- Arduh FA
- Arguin J-F
- Argyropoulos S
- Arik M
- Armadans R Caminal
- Armbruster AJ
- Armitage LJ
- Arnaez O
- Arnold H
- Arratia M
- Arslan O
- Artamonov A
- Artoni G
- Artz S
- Asai S
- Asbah N
- Ashkenazi A
- Asquith L
- Assamagan K
- Astalos R
- Astigarraga ME Pozo
- Atkinson M
- Atlay NB
- Augsten K
- Avolio G
- Axen B
- Ayoub MK
- Azuelos G
- Baas AE
- Baca MJ
- Bachacou H
- Bachas K
- Backes M
- Bagnaia P
- Bahmani M
- Bahrasemani H
- Baines JT
- Bajic M
- Baker OK
- Baldin EM
- Balek P
- Balli F
- Balunas WK
- Banas E
- Bandyopadhyay A
- Banerjee Sw
- Bannoura AAE
- Barajas CA Chavez
- Barak L
- Barberio EL
- Barberis D
- Barbero M
- Barillari T
- Barisits M-S
- Barkeloo JT
- Barklow T
- Barlow N
- Barnes SL
- Barnett BM
- Barnett RM
- Barnovska-Blenessy Z
- Baroncelli A
- Barone G
- Barr AJ
- Barranco Navarro L
- Barreiro F
- Bartoldus R
- Barton AE
- Bartos P
- Basalaev A
- Bassalat A
- Bates RL
- Batista SJ
- Batley JR
- Battaglia M
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- Bauer F
- Bawa HS
- Beacham JB
- Beattie MD
- Beau T
- Beauchemin PH
- Bechtle P
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- Beddall A
- Beddall AJ
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- Begalli M
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- Behr JK
- Bell AS
- Bella G
- Bella L Aperio
- Bellagamba L
- Bellerive A
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- Beltramello O
- Belyaev NL
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- Benitez J
- Benjamin DP
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- Bensinger JR
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- Beresford L
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- Berge D
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- Berlingen J Montejo
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- Bernardi G
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- Black JE
- Black KM
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- Bloch I
- Blocker C
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- Blum W
- Blumenschein U
- Blunier S
- Bobbink GJ
- Bobrovnikov VS
- Bocchetta SS
- Bocci A
- Bock C
- Boehler M
- Boeriu OE Vickey
- Boerner D
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bold T
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- Bolz AE
- Bomben M
- Bona M
- Boonekamp M
- Borisov A
- Borissov G
- Bortfeldt J
- Bortoletto D
- Bortolotto V
- Boscherini D
- Bosman M
- Bossio Sola JD
- Boudreau J
- Bouffard J
- Bouhova-Thacker EV
- Boumediene D
- Bourdarios C
- Boutle SK
- Boveia A
- Boyd J
- Boyko IR
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- Yigitbasi E
- Yildirim E
- Yildiz H Duran
- Yorita K
- Yoshihara K
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- Yuen SPY
- Yusuff I
- Zabinski B
- Zacharis G
- Zaidan R
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- Zakharchuk N
- Zalieckas J
- Zaman A
- Zambito S
- Zanzi D
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- Zemaityte G
- Zemla A
- Zeng JC
- Zeng Q
- Zenin O
- Zenis T
- Zerwas D
- Zhang D
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- Zhang G
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- Zhang J
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- Zhang M
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- 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
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- Zhou N
- 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
- '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
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
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- Zhemchugov A
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- 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
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