475 research outputs found
Approaches in biotechnological applications of natural polymers
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- Publication venue
- 'American Institute of Mathematical Sciences (AIMS)'
- Publication date
- 01/01/2016
- Field of study
Natural polymers, such as gums and mucilage, are biocompatible, cheap, easily available and non-toxic materials of native origin. These polymers are increasingly preferred over synthetic materials for industrial applications due to their intrinsic properties, as well as they are considered alternative sources of raw materials since they present characteristics of sustainability, biodegradability and biosafety. As definition, gums and mucilages are polysaccharides or complex carbohydrates consisting of one or more monosaccharides or their derivatives linked in bewildering variety of linkages and structures. Natural gums are considered polysaccharides naturally occurring in varieties of plant seeds and exudates, tree or shrub exudates, seaweed extracts, fungi, bacteria, and animal sources. Water-soluble gums, also known as hydrocolloids, are considered exudates and are pathological products; therefore, they do not form a part of cell wall. On the other hand, mucilages are part of cell and physiological products. It is important to highlight that gums represent the largest amounts of polymer materials derived from plants. Gums have enormously large and broad applications in both food and non-food industries, being commonly used as thickening, binding, emulsifying, suspending, stabilizing agents and matrices for drug release in pharmaceutical and cosmetic industries. In the food industry, their gelling properties and the ability to mold edible films and coatings are extensively studied. The use of gums depends on the intrinsic properties that they provide, often at costs below those of synthetic polymers. For upgrading the value of gums, they are being processed into various forms, including the most recent nanomaterials, for various biotechnological applications. Thus, the main natural polymers including galactomannans, cellulose, chitin, agar, carrageenan, alginate, cashew gum, pectin and starch, in addition to the current researches about them are reviewed in this article.. }To the Conselho Nacional de Desenvolvimento Cientfíico e Tecnológico (CNPq) for fellowships (LCBBC and MGCC) and the Coordenação de Aperfeiçoamento de Pessoal de Nvíel Superior (CAPES) (PBSA). This study was supported by the Portuguese Foundation for Science and Technology (FCT) under the scope of the strategic funding of UID/BIO/04469/2013 unit, the Project RECI/BBB-EBI/0179/2012 (FCOMP-01-0124-FEDER-027462) and COMPETE 2020 (POCI-01-0145-FEDER-006684) (JAT)
Disrupted Small-World Brain Networks in Moderate Alzheimer's Disease: A Resting-State fMRI Study
- Author
- AF Alexander-Bloch
- AJ Trachtenberg
- AL Bokde
- AR Borenstein
- B Horwitz
- B Horwitz
- BC Dickerson
- BC Dickerson
- Bing Liu
- C Schmidt
- CJ Brainerd
- CJ Stam
- CJ Stam
- CL Grady
- CR Jack Jr
- CY Lo
- D Tomasi
- D Zhang
- DA Wolk
- DA Wolk
- DC Van Essen
- DC Van Essen
- DJ Watts
- E Bullmore
- E Salmon
- EH Corder
- EJ Sanz-Arigita
- ET Bullmore
- G McKhann
- GA Carlesimo
- GE Alexander
- GM Halliday
- H Forstl
- HA Wishart
- Hong Jiang
- J Davignon
- J Lind
- J Sepulcre
- JC Morris
- JR Andrews-Hanna
- K Supekar
- K Wang
- KR Van Dijk
- L Mosconi
- M Di Paola
- M Zarei
- MD Fox
- MD Greicius
- MD Johnson
- ME Raichle
- MG Packard
- MJ de Leon
- MM Adamson
- MM Machulda
- N Filippini
- N Tzourio-Mazoyer
- NP Azari
- O Sporns
- O Sporns
- O Sporns
- O Sporns
- O Sporns
- Olaf Sporns
- Peijun Wang
- PM Thompson
- Qian Xi
- Qihao Guo
- R Adolphs
- R Mayeux
- R Salvador
- R Salvador
- R Salvador
- RA Sperling
- RL Buckner
- RL Buckner
- RL Buckner
- RL Buckner
- RL Buckner
- S Achard
- S Achard
- SH Strogatz
- SJ Broyd
- Tianzi Jiang
- V Latora
- V Stenset
- X Delbeuck
- X Delbeuck
- Xiangbin Wang
- Xiaohu Zhao
- Y He
- Y He
- Y He
- Y Li
- Y Liu
- Y Liu
- Y Liu
- Y Yoneoka
- YD Van der Werf
- Yong Liu
- Z Wang
- Z Yao
- Z Zhang
- Publication venue
- Public Library of Science
- Publication date
- 01/03/2012
- Field of study
The small-world organization has been hypothesized to reflect a balance between local processing and global integration in the human brain. Previous multimodal imaging studies have consistently demonstrated that the topological architecture of the brain network is disrupted in Alzheimer's disease (AD). However, these studies have reported inconsistent results regarding the topological properties of brain alterations in AD. One potential explanation for these inconsistent results lies with the diverse homogeneity and distinct progressive stages of the AD involved in these studies, which are thought to be critical factors that might affect the results. We investigated the topological properties of brain functional networks derived from resting functional magnetic resonance imaging (fMRI) of carefully selected moderate AD patients and normal controls (NCs). Our results showed that the topological properties were found to be disrupted in AD patients, which showing increased local efficiency but decreased global efficiency. We found that the altered brain regions are mainly located in the default mode network, the temporal lobe and certain subcortical regions that are closely associated with the neuropathological changes in AD. Of note, our exploratory study revealed that the ApoE genotype modulates brain network properties, especially in AD patients
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
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- Zakharchuk N
- Zambito S
- Zanzi D
- Zaripovas DR
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
- Zenis T
- Zerwas D
- Zgubic M
- Zhang B
- Zhang DF
- Zhang G
- Zhang H
- Zhang J
- Zhang L
- Zhang M
- Zhang R
- Zhang S
- Zhang X
- Zhang Y
- Zhang Z
- Zhao P
- Zhao Z
- Zhemchugov A
- Zheng Z
- Zhong D
- Zhou B
- Zhou C
- Zhou M
- Zhou MS
- Zhou N
- Zhou Y
- Zhu C
- Zhu CG
- Zhu H
- Zhu HL
- Zhu J
- Zhu Y
- Zhuang X
- Zhukov K
- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zivkovic L
- Zobernig G
- Zoccoli A
- Zoch K
- Zorbas TG
- Zou R
- Zu Theenhausen HM
- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2015
- Field of study
Results of a search for new phenomena in final states with an energetic jet and large missing transverse momentum are reported. The search uses 20.3 fb−1 of √ s = 8 TeV data collected in 2012 with the ATLAS detector at the LHC. Events are required to have at least one jet with pT > 120 GeV and no leptons. Nine signal regions are considered with increasing missing transverse momentum requirements between Emiss T > 150 GeV and Emiss T > 700 GeV. Good agreement is observed between the number of events in data and Standard Model expectations. The results are translated into exclusion limits on models with either large extra spatial dimensions, pair production of weakly interacting dark matter candidates, or production of very light gravitinos in a gauge-mediated supersymmetric model. In addition, limits on the production of an invisibly decaying Higgs-like boson leading to similar topologies in the final state are presente
Search for the neutral Higgs bosons of the minimal supersymmetric standard model in pp collisions at root s=7 TeV with the ATLAS detector
- Author
- Aad G
- Abajyan T
- Abbott B
- Abdallah J
- Abdelalim AA
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- Publication venue
- Publication date
- 01/02/2013
- Field of study
A search for neutral Higgs bosons of the Minimal Supersymmetric Standard Model (MSSM) is reported. The analysis is based on a sample of proton-proton collisions at a centre-of-mass energy of 7TeV recorded with the ATLAS detector at the Large Hadron Collider. The data were recorded in 2011 and correspond to an integrated luminosity of 4.7 fb-1 to 4.8 fb-1. Higgs boson decays into oppositely-charged muon or τ lepton pairs are considered for final states requiring either the presence or absence of b-jets. No statistically significant excess over the expected background is observed and exclusion limits at the 95% confidence level are derived. The exclusion limits are for the production cross-section of a generic neutral Higgs boson, φ, as a function of the Higgs boson mass and for h/A/H production in the MSSM as a function of the parameters mA and tan β in the mhmax scenario for mA in the range of 90GeV to 500 GeV. Copyright CERN
Jet energy measurement with the ATLAS detector in proton-proton collisions at root s=7 TeV
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- Smizanska M
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- Sodomka J
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- Sykora I
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- Taiblum N
- Takahashi Y
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- Torchiani I
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- Tyrvainen H
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- Uhrmacher M
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- Underwood DG
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- Varnes EW
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- Vorobel V
- Vorobiev AP
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- Vos M
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- Vossebeld JH
- Vranjes N
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- Vukotic I
- Wagner P
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- Wiglesworth C
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- Xie Y
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- Yagci KD
- Yamada M
- Yamaguchi H
- Yamamoto A
- Yamamoto K
- Yamamoto S
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- Yamanaka T
- Yamaoka J
- Yamazaki T
- Yamazaki Y
- Yan Z
- Yang H
- Yang UK
- Yang Y
- Yang Y
- Yang Z
- Yanush S
- Yao Y
- Yasu Y
- Ye J
- Ye S
- Yildizb HD
- Yilmaz M
- Yoosootiniya R
- Yorita K
- Yoshida R
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- Youssef S
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- Yu J
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- Yurkewicz A
- Zaets VG
- 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
- Zenonos Z
- Zenz S
- Zerwas D
- Zhan Z
- Zhang D
- Zhang H
- Zhang J
- Zhang Q
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- Zhang Z
- Zhao L
- Zhao T
- Zhao Z
- Zhemchugov A
- Zheng S
- Zhong J
- Zhou B
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- Zhuravlov V
- Zieminska D
- Zimmermann R
- Zimmermann S
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zitoun R
- Zivkovic L
- Zmouchko VV
- Zobernig G
- Zoccoli A
- Zolnierowski Y
- Zsenei A
- Zutshi V
- Zwalinski L
- 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
A second generation human haplotype map of over 3.1 million SNPs
- Author
- Abecasis GR
- Adebamowo CA
- Adewole IF
- Ajayi I
- Altshuler D
- Altshuler D
- Altshuler D
- An D
- Aniagwu T
- Auton A
- Ballinger DG
- Barrett J
- Barry R
- Bellemare G
- Belmont JW
- Belmont JW
- Bentley DR
- Bird CP
- Birren BW
- Blumenstiel B
- Bottolo L
- Boudreau A
- Brooks LD
- Burton J
- Cai D
- Camargo A
- Cardin N
- Cardon LR
- Carter NP
- Chagnon F
- Chakravarti A
- Chee MS
- Chen PE
- Chen Z
- Chretien YR
- Chu X
- Clarke G
- Clayton EW
- Clee CM
- Collins FS
- Cox DR
- Cutler DJ
- Daly MJ
- Daly MJ
- de Bakker PI
- Defelice M
- Delgado M
- Deloukas P
- Dermitzakis ET
- Dixon M
- Donnelly P
- Evans DM
- Eyheramendy S
- Faggart M
- Fan JB
- Feolo M
- Ferretti V
- Foster MW
- Frazer KA
- Freeman C
- Fu H
- Fukushima Y
- Fulton LL
- Gabriel SB
- Gabriel SB
- Galver LM
- Gao Y
- Gibbs RA
- Gibbs RA
- Godbout M
- Goyette M
- Griffiths M
- Guan W
- Gunderson K
- Gupta S
- Guyer MS
- Gwilliam R
- Han H
- Hardenbol P
- He Y
- Hinds DA
- Holden AL
- Hu H
- Hu W
- Huang W
- Hudson TJ
- Hunt S
- Jamieson R
- Jin L
- Jones MC
- Kang L
- Kashuk CS
- Kato K
- Kawaguchi T
- Kennedy K
- Kent A
- Kitamoto T
- Knoppers BM
- Koboldt DC
- Krishnan L
- Kwok PY
- L'Archevêque P
- Leal SM
- Leboeuf M
- Leppert MF
- Li C
- Li Q
- Li Y
- Lin S
- Lin W
- Liu S
- Liu Y
- Macer DR
- Mak W
- Maller J
- Marchini J
- Marshall PA
- Matsuda I
- McCarroll S
- McEwen JE
- McLay K
- McVean G
- Miller RD
- Montpetit A
- Moore J
- Morizono T
- Morris AP
- Morrison J
- Mullikin JC
- Munro HM
- Murray SS
- Muzny D
- Myers S
- Nagashima A
- Nakamura Y
- Nazareth L
- Nguyen H
- Niikawa N
- Nkwodimmah C
- Ohnishi Y
- Oliphant AR
- Olivier JF
- Onofrio RC
- Onofrio RC
- Pan H
- Parkin M
- Pasternak S
- Patterson N
- Pawlikowska L
- Pe'er I
- Peiffer A
- Peterson JL
- Phillips MS
- Plumb RW
- Powell D
- Price A
- Purcell S
- Qin ZS
- Qiu R
- Richter DJ
- Richter DJ
- Rogers J
- Ross MT
- Rotimi CN
- Roumy S
- Roy J
- Royal CD
- Sabeti P
- Saeki K
- Sallée C
- Saxena R
- Schaffner SF
- Sekine A
- Sham PC
- Shen Y
- Shen Y
- Sherry ST
- Shi M
- Sims SK
- Skol A
- Smith AV
- Sodergren E
- Song YQ
- Spencer C
- Spiegel J
- Stahl E
- Stein LD
- Stephens M
- Stewart J
- Stranger BE
- Stuve LL
- Suda E
- Sun W
- Sung LM
- Taillon-Miller P
- Tam PK
- Tanaka T
- Tang X
- Tello-Ruiz MK
- Thomas DJ
- Thorisson GA
- Tsui LC
- Tsui SK
- Tsunoda T
- Tsunoda T
- Varilly P
- Verner A
- Wallenburg JC
- Wang H
- Wang H
- Wang J
- Wang R
- Wang VO
- Wang W
- Wang Y
- Wang Y
- Wang Z
- Watkin J
- Waye MM
- Weinstock GM
- Weir BS
- Wheeler DA
- Wheeler DA
- Whittaker P
- Willey DL
- Willis TD
- Wilson RK
- Winchester E
- Wong JT
- Xiao M
- Xiong X
- Xu L
- Xue H
- Yakub I
- Yang H
- Yao Z
- Yu F
- Yu J
- Zacharia LF
- Zeng C
- Zeng C
- Zhang B
- Zhang H
- Zhang Q
- Zhao H
- Zhao H
- Zhao H
- Zhou J
- Ziaugra L
- Ziaugra L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2007
- Field of study
We describe the Phase II HapMap, which characterizes over 3.1 million human single nucleotide polymorphisms (SNPs) genotyped in 270 individuals from four geographically diverse populations and includes 25-35% of common SNP variation in the populations surveyed. The map is estimated to capture untyped common variation with an average maximum r(2) of between 0.9 and 0.96 depending on population. We demonstrate that the current generation of commercial genome-wide genotyping products captures common Phase II SNPs with an average maximum r(2) of up to 0.8 in African and up to 0.95 in non-African populations, and that potential gains in power in association studies can be obtained through imputation. These data also reveal novel aspects of the structure of linkage disequilibrium. We show that 10-30% of pairs of individuals within a population share at least one region of extended genetic identity arising from recent ancestry and that up to 1% of all common variants are untaggable, primarily because they lie within recombination hotspots. We show that recombination rates vary systematically around genes and between genes of different function. Finally, we demonstrate increased differentiation at non-synonymous, compared to synonymous, SNPs, resulting from systematic differences in the strength or efficacy of natural selection between populations.Peer Reviewedhttp://deepblue.lib.umich.edu/bitstream/2027.42/62863/1/nature06258.pd
Transcriptome 3′end organization by PCF11 links alternative polyadenylation to formation and neuronal differentiation of neuroblastoma
- Author
- A Castello
- A Dobin
- A Meinhart
- A Ogorodnikov
- A Yoda
- AJ Gruber
- AN Brooks
- B Beagle
- B Dichtl
- B Fusby
- B Tian
- C Lavarino
- C Mayr
- C Mayr
- CE Birse
- CP Masamha
- D Kaida
- DD Licatalosi
- DJ Duffy
- EK Maxwell
- ER DeLong
- ET Wang
- FA Bava
- FA McMorris
- FE Kleiman
- G López-Carballo
- GC Vieira
- GM Brodeur
- H Kocak
- I Garcia
- J Brumbaugh
- J Chen
- J Chen
- J Neve
- JB Beckwith
- JH Schulte
- JM Maris
- K Lohmann
- KK Matthay
- M Dutertre
- M Flahaut
- M Hallais
- M Hoque
- M Jenal
- M Müller-McNicoll
- M Selbach
- ME Ritchie
- N Al-Furoukh
- N Barker
- NKV Cheung
- P Carninci
- P Miura
- R Batra
- R Sandberg
- RE Turner
- RT Dorsam
- S Bulashevska
- S Danckwardt
- S Danckwardt
- S Millevoi
- S Vorlova
- SB Turkel
- Si Hino
- T Hashimshony
- TJ Pugh
- W Yao
- WM Oldham
- X Liu
- Y Huang
- Y Jan
- Y Kargapolova
- Y Shi
- Z Su
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2018
- Field of study
In gene regulation, diversification at the transcriptome 3′end is linked to differentiation and dedifferentiation. Here, the authors discover extensive transcriptome 3′end-alterations in neuroblastoma, regulated by PCF11, and provide an interactive data repository of transcriptome-wide alternative polyadenylation
Measurements of differential cross-sections in top-quark pair events with a high transverse momentum top quark and limits on beyond the Standard Model contributions to top-quark pair production with the ATLAS detector at √s = 13 TeV
- Author
- Aad G
- Abbott B
- Abbott DC
- Abeling K
- Abhayasinghe DK
- Abidi SH
- Aboulhorma A
- Abramowicz H
- Abreu H
- Abud AA
- Abulaiti Y
- Acharya BS
- Achkar B
- Adam L
- Adamczyk L
- Adamek L
- Addepalli SV
- Adelman J
- Adiguzel A
- Adorni S
- Adye T
- Affolder AA
- Afik Y
- Agaras MN
- Agarwala J
- Aggarwal A
- Agheorghiesei C
- Aguilar-Saavedra JA
- Agullo PM
- Ahmad A
- Ahmadov F
- Ahmed WS
- Ai X
- Aielli G
- Aizenberg I
- Akbiyik M
- Akesson TPA
- Akimov AV
- Al Khoury K
- Alberghi GL
- Albert J
- Albicocco P
- 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
- Allport PP
- Aloisio A
- Alonso F
- Alpigiani C
- Alves FLL
- Alviggi MG
- Ambler A
- Ambroz L
- Amelung C
- Amidei D
- Amoroso S
- Amos KR
- Amrouche CS
- Ananiev V
- Anastopoulos C
- Andana RYG
- Andari N
- Andeen T
- Anders JK
- Andrean SY
- Andreazza A
- Angelidakis S
- Angerami A
- Anisenkov AV
- Annovi A
- Antel C
- Anthony MT
- Antipov E
- Antonelli M
- Antrim DJA
- Anulli F
- Aoki M
- Aparo MA
- Appelt C
- Aranda CP
- Aranzabal N
- Araya ST
- Arcangeletti C
- Arce ATH
- Arena E
- Arguin JF
- Argyropoulos S
- Arling JH
- Armbruster AJ
- Arnaez O
- Arnold H
- Artoni G
- Asada H
- Asai K
- Asai S
- Asbah NA
- Asimakopoulou EM
- Assahsah J
- Assamagan K
- Astalos R
- Astigarraga MEP
- Atkin RJ
- Atkinson M
- Atlay NB
- Atmani H
- Atmasiddha PA
- Augsten K
- Auricchio S
- Austrup VA
- Avner G
- Avolio G
- Ayoub MK
- Azuelos G
- Babal D
- Bachacou H
- Bachas K
- Bachiu A
- Backman F
- Badea A
- Bagnaia P
- Bahilo JJL
- Bahmani M
- Bailey AJ
- Bailey VR
- Baines JT
- Bakalis C
- Baker OK
- Bakker PJ
- Bakos E
- Balaji S
- Balasubramanian R
- Baldin EM
- Balek P
- Ballabene E
- Balli F
- Baltes LM
- Balunas WK
- Balz J
- Banas E
- Bandieramonte M
- Bandyopadhyay A
- Bansal S
- Barak L
- Barberio EL
- Barberis D
- Barbero M
- Barbour G
- Barends KN
- Barillari T
- Barisits MS
- Barkeloo J
- Barklow T
- Barnett RM
- Baron P
- Baroncelli A
- Barone G
- Barr AJ
- Barreiro F
- Barron U
- Barrue RFC
- Barsov S
- Bartels F
- Bartoldus R
- Bartolini G
- Barton AE
- Bartos P
- Basalaev A
- Basan A
- Baselga M
- Bashta I
- Bassalat A
- Basso MJ
- Basson CR
- Bates RL
- Batlamous S
- Batley JR
- Batool B
- Battaglia M
- Bauce M
- Bauer F
- Bauer P
- Bayirli A
- Beacham JB
- Beau T
- Beauchemin PH
- Becherer F
- Bechtle P
- Beck HP
- Becker K
- Becot C
- Beddall AJ
- Bednyakov VA
- Bee CP
- Beemster LJ
- Beermann TA
- Begalli M
- Begel M
- Behera A
- Behr JK
- Beirer JF
- Beisiegel F
- Belfkir M
- Bella G
- Bella LA
- Bellagamba L
- Bellerive A
- Bellos P
- Beloborodov K
- Belotskiy K
- Belyaev NL
- Benchekroun D
- Benhammou Y
- Benjamin DP
- Benoit M
- Bensinger JR
- Bentvelsen S
- Beresford L
- Beretta M
- Berge D
- Berger N
- Bergmann B
- Beringer J
- Berlendis S
- Berlingen JM
- Bernardi G
- Bernius C
- Bernlochner FU
- Berry T
- Berta P
- Bertram IA
- Bethke S
- Betti A
- Bevan AJ
- Bhatta S
- Bhattacharya DS
- Bhattarai P
- Bhopatkar VS
- Bi R
- Bi R
- Bianchi RM
- Biebel O
- Bielski R
- Biesuz NV
- Biglietti M
- Billoud TRV
- Bindi M
- Bingul A
- Bini C
- Biondi S
- Biondini A
- Birch-sykes CJ
- Bird GA
- Birman M
- Bisanz T
- Biswal JP
- Biswas D
- Bitadze A
- Bjorke K
- Bloch I
- Blocker C
- Blue A
- Blumenschein U
- Blumenthal J
- Bobbink GJ
- Bobrovnikov VS
- Boehler M
- Boeriu OEV
- Bogavac D
- Bogdanchikov AG
- Bohm C
- Boisvert V
- Bokan P
- Bolanos GR
- Bold T
- Bomben M
- Bona M
- Boonekamp M
- Booth CD
- Borbely AG
- Borecka-Bielska HM
- Borgna LS
- Borissov G
- Bortoletto D
- Bosca SR
- Boscherini D
- Bosman M
- Bostanabad MG
- Bouaouda K
- Boudreau J
- Bouhova-Thacker EV
- Boumediene D
- Bouquet R
- Bourdarios CA
- Boveia A
- Boyd J
- Boye D
- Boyko IR
- 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
- Britton D
- Britzger D
- Brock I
- Brooijmans G
- Brooks WK
- Brost E
- Bruers B
- Bruncko D
- Bruni A
- Bruni G
- Bruschi M
- Bruscino N
- Bryngemark L
- Buanes T
- Buat Q
- Buchholz P
- Buckley AG
- Budagov IA
- Bugge MK
- Bulekov O
- Bullard BA
- Burdin S
- Burgard CD
- Burger AM
- Burghgrave B
- Burr JTP
- Burton CD
- Burzynski JC
- Busch EL
- Buscher V
- Bussey PJ
- Butler JM
- Buttar CM
- Butterworth JM
- Buttinger W
- Buzykaev AR
- Bylund OB
- Cabras G
- Caforio D
- Cai H
- Cai Y
- Cairo VMM
- Cakir IT
- Cakir O
- Calace N
- Calafiura P
- Calderini G
- Calfayan P
- Callea G
- Caloba LP
- Calvet D
- Calvet S
- Calvet TP
- Calvetti M
- Camarda S
- Camarri P
- Camelia EA
- Camerlingo MT
- Cameron D
- Camincher C
- Campanelli M
- Camplani A
- Canale V
- Canesse A
- Cantero J
- Cao Y
- Capocasa F
- Capriles FGD
- Capua M
- Carbone A
- Cardarelli R
- Cardenas JCJ
- Cardillo F
- Carducci G
- Carli T
- Carlino G
- Carlson BT
- Carlson EM
- Carlson TI
- Carminati L
- Carnesale M
- Caron S
- Carquin E
- Carra S
- Carratta G
- Carter JWS
- Carter TM
- Casadei D
- Casado MP
- Casha AF
- Castiglia EG
- Castillo FL
- Castillo LRF
- Castro NF
- Catinaccio A
- Catmore JR
- Cavaliere V
- Cavalli N
- Cavasinni V
- Celebi E
- Celli F
- Centonze MS
- Cerny K
- Cerqueira AS
- Cerri A
- Cerrito L
- Cerutti F
- Cervelli A
- Cetin SA
- Chadi Z
- Chakraborty D
- Chala M
- Chan J
- Chan WS
- Chan WY
- Chapman JD
- Chargeishvili B
- Charlton DG
- Charman TP
- Chatterjee M
- Chekanov S
- Chekulaev SV
- Chelkov GA
- Chen A
- Chen B
- Chen B
- Chen C
- Chen H
- Chen H
- Chen J
- Chen J
- Chen S
- Chen SJ
- Chen X
- Chen X
- Chen Y
- Cheng CL
- Cheng HC
- Cheplakov A
- Cheremushkina E
- Cherepanova E
- Cheu E
- Cheung K
- Chevalier L
- Chiarella V
- Chiarelli G
- Chiodini G
- Chisholm AS
- Chitan A
- Chiu YH
- Chizhov MV
- Choi K
- Chomont AR
- Chou Y
- Chow YS
- Chowdhury T
- Christopher LD
- Chu MC
- Chu X
- Chudoba J
- Chwastowski JJ
- Cieri D
- Ciesla KM
- Cindro V
- Ciocio A
- Cirotto F
- Citron ZH
- Citterio M
- Ciubotaru DA
- Ciungu BM
- Clark A
- Clark PJ
- Clawson SE
- Clement C
- Clissa L
- Coadou Y
- Cobal M
- Coccaro A
- Codina EP
- Coelli S
- Cohen H
- Coimbra AEC
- Cole B
- Collot J
- Columbie JMC
- Connell SH
- Connelly IA
- Conroy EI
- Conventi F
- Cooke HG
- Cooper-Sarkar AM
- Cormier F
- Cornell SD
- Corpe LD
- Corradi M
- Correia AMH
- Corrigan EE
- Corriveau F
- Costa MJ
- Costanza F
- Costanzo D
- Cote BM
- Coutinho YA
- Cowan G
- Cowley JW
- Cranmer K
- Crepe-Renaudin S
- Crescioli F
- Cristinziani M
- Cristoforetti M
- Croft V
- Crosetti G
- Cueto A
- Cui H
- Cui Z
- Cukierman AR
- Cunningham WR
- Curcio F
- Czodrowski P
- Czurylo MM
- D'amen G
- D'Amico V
- D'Auria S
- D'Eramo L
- D'onofrio A
- D'Onofrio M
- D'uffizi M
- Da Costa AMMJ
- da Costa JBG
- Da Via C
- Dabrowski W
- Dado T
- Dahbi S
- Dai T
- Dallapiccola C
- Dam M
- Damazio DO
- Damp J
- Dandoy JR
- Daneri MF
- Danninger M
- Dao V
- Darbo G
- Darmora S
- Dattagupta A
- David C
- Davidek T
- Davis DR
- Davis-Purcell B
- Dawson I
- de Andrade LM
- De Araujo MV
- De Asmundis R
- De Beurs M
- De Carvalho ALM
- De Castro S
- De Groot N
- de Jong P
- De K
- de la Hoz SG
- De la Torre H
- De Lima RT
- De Maria A
- De Regie JBD
- de Renstrom PAB
- De Sa RCL
- De Salvo A
- De Sanctis U
- De Santis M
- De Santo A
- De Sousa MJDS
- De Souza EEP
- Dedovich DV
- Degens J
- Deiana AM
- Del Peso J
- Del Rio F
- Delegido AJG
- Deliot F
- Delitzsch CM
- Dell'Acqua A
- Dell'Asta L
- Della Pietra M
- Della Volpe D
- Delmastro M
- Delsart PA
- Demers S
- Demichev M
- Denisov SP
- Derendarz D
- Derue F
- Dervan P
- Desch K
- Dette K
- Deutsch C
- Deviveiros PO
- Di Bello FA
- Di Ciaccio A
- Di Ciaccio L
- Di Domenico A
- Di Donato C
- Di Girolamo A
- Di Gregorio G
- Di Luca A
- Di Micco B
- Di Nardo R
- Diaconu C
- Dias BP
- Dias FA
- Diaz MA
- Didenko M
- Diehl EB
- Dimitriadi C
- Dimitrievska A
- Ding W
- Dingfelder J
- Dinu IM
- Dittmeier SJ
- Dittus F
- Djama F
- Djobava T
- Djuvsland JI
- Do Vale TD
- Dodsworth D
- Doglioni C
- Dolejsi J
- Dolezal Z
- Dominguez LP
- Donadelli M
- Donaldson CP
- Dong B
- Donini J
- Donszelmann TC
- Dopke J
- Doria A
- Dos Santos SPA
- Dova MT
- Doyle AT
- Drechsler E
- Dreyer E
- Drobac AS
- Du D
- du Pree TA
- Dubinin F
- Dubovsky M
- Duchovni E
- Duckeck G
- Ducu OA
- Duda D
- Dudarev A
- Duflot L
- Duhrssen M
- Dulsen C
- Dumitriu AE
- Dunford M
- Dungs S
- Dunne K
- Duperrin A
- Duren M
- Durglishvili A
- Dutta B
- Dwyer BL
- Dyckes GI
- Dyndal M
- Dysch S
- Dziedzic BS
- Eckerova B
- Eggleston MG
- Ehrke LF
- Eigen G
- Einsweiler K
- Ekelof T
- El Ghazali Y
- El Jarrari H
- El Moursli RC
- El Moussaouy A
- Ellajosyula V
- Ellert M
- Ellinghaus F
- Elliot AA
- Ellis N
- Elmsheuser J
- Elsing M
- Emeliyanov D
- Emerman A
- Enari Y
- Ene I
- Erdmann J
- Ereditato A
- Erland PA
- Errenst M
- Escalier M
- Escobar C
- Estabragh MR
- Estevez MA
- Etzion E
- Evans G
- Evans H
- Evans MO
- Ezhilov A
- Ezzarqtouni S
- Fabbri F
- Fabbri L
- Facini G
- Fadeyev V
- Fakhrutdinov RM
- Falciano S
- Falke PJ
- Falke S
- Faltova J
- Fan Y
- Fang Y
- Fanourakis G
- Fanti M
- Faraj M
- Farbin A
- Farilla A
- Farooque T
- Farrington SM
- Fassi F
- Fassouliotis D
- Fawcett WJ
- Fayard L
- Fedin OL
- Fedotov G
- Feickert M
- Feligioni L
- Fell A
- Fellers DE
- Feng C
- Feng M
- Fenton MJ
- Fenyuk AB
- Ferguson SW
- Fernandez SG
- Ferrando J
- Ferrari A
- Ferrari P
- Ferrari R
- Ferraz VA
- Ferrer JAV
- Ferrere D
- Ferretti C
- Fiedler F
- Filmer EK
- Filthaut F
- Fiolhais MCN
- Fiorini L
- Fischer F
- Fisher WC
- Fitschen T
- Fleck I
- Fleischmann P
- Flick T
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- Zhemchugov A
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- Zwalinski L
- Publication venue
- 'Springer Science and Business Media LLC'
- Publication date
- 01/01/2022
- Field of study
Cross-section measurements of top-quark pair production where the hadronically decaying top quark has transverse momentum greater than 355 GeV and the other top quark decays into ℓνb are presented using 139 fb−1 of data collected by the ATLAS experiment during proton-proton collisions at the LHC. The fiducial cross-section at s = 13 TeV is measured to be σ = 1.267 ± 0.005 ± 0.053 pb, where the uncertainties reflect the limited number of data events and the systematic uncertainties, giving a total uncertainty of 4.2%. The cross-section is measured differentially as a function of variables characterising the tt¯ system and additional radiation in the events. The results are compared with various Monte Carlo generators, including comparisons where the generators are reweighted to match a parton-level calculation at next-to-next-to-leading order. The reweighting improves the agreement between data and theory. The measured distribution of the top-quark transverse momentum is used to search for new physics in the context of the effective field theory framework. No significant deviation from the Standard Model is observed and limits are set on the Wilson coefficients of the dimension-six operators OtG and Otq(8), where the limits on the latter are the most stringent to date. [Figure not available: see fulltext.]
Pan-cancer analysis of whole genomes
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- The ICGC/TCGA Pan-Cancer Analysis of Whole Genomes Consortium View Correspondence (jump link)
- Thiessen
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- Y. fv
- Y. gl
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- Y. hq
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- Y. ia
- Y. kq
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- Y. nh
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- Y. rg
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- Y. S. jf
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- Y. vr
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- Yachida
- Yamaguchi
- Yamaguchi T. N. k
- Yamamoto
- Yamaue
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- Yang
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- Yellapantula
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- z ah
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- Z. hv
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- Z. jq
- Z. kt
- Z. oe
- Zaikova
- Zapatka
- zd Gershenwald
- Zenklusen
- Zeps
- zf Ghossein
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang
- Zhang H. b
- Zhao
- Zheng
- Zhou
- Zhou
- Zhu
- Zhu
- zi zj
- zm Jayaseelan
- Zou
- Zou
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- zw Lewis
- Ó. A. th
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- Publication venue
- Publication date
- 11/12/2019
- Field of study
Cancer is driven by genetic change, and the advent of massively parallel sequencing has enabled systematic documentation of this variation at the whole-genome scale(1-3). Here we report the integrative analysis of 2,658 whole-cancer genomes and their matching normal tissues across 38 tumour types from the Pan-Cancer Analysis of Whole Genomes (PCAWG) Consortium of the International Cancer Genome Consortium (ICGC) and The Cancer Genome Atlas (TCGA). We describe the generation of the PCAWG resource, facilitated by international data sharing using compute clouds. On average, cancer genomes contained 4-5 driver mutations when combining coding and non-coding genomic elements; however, in around 5% of cases no drivers were identified, suggesting that cancer driver discovery is not yet complete. Chromothripsis, in which many clustered structural variants arise in a single catastrophic event, is frequently an early event in tumour evolution; in acral melanoma, for example, these events precede most somatic point mutations and affect several cancer-associated genes simultaneously. Cancers with abnormal telomere maintenance often originate from tissues with low replicative activity and show several mechanisms of preventing telomere attrition to critical levels. Common and rare germline variants affect patterns of somatic mutation, including point mutations, structural variants and somatic retrotransposition. A collection of papers from the PCAWG Consortium describes non-coding mutations that drive cancer beyond those in the TERT promoter(4); identifies new signatures of mutational processes that cause base substitutions, small insertions and deletions and structural variation(5,6); analyses timings and patterns of tumour evolution(7); describes the diverse transcriptional consequences of somatic mutation on splicing, expression levels, fusion genes and promoter activity(8,9); and evaluates a range of more-specialized features of cancer genomes(8,10-18).Peer reviewe
Measurements of differential cross-sections in four-lepton events in 13 TeV proton-proton collisions with the ATLAS detector
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- Traeet A
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- Tsopoulou M
- Tsukerman II
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- Yildiz HD
- Yin P
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- Zanzi D
- Zeissner S
- Zeitnitz C
- Zemaityte G
- Zeng JC
- Zenin O
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- Zhemchugov A
- Zheng Z
- Zhong D
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- Zhulanov V
- Zieminska D
- Zimine N
- Zimmermann S
- Zinonos Z
- Ziolkowski M
- Zobernig G
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- Zorbas TG
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- Zwalinski L
- Publication venue
- 'Springer Fachmedien Wiesbaden GmbH'
- Publication date
- 02/07/2021
- Field of study
Measurements of four-lepton differential and integrated fiducial cross-sections in events with two same-flavour, opposite-charge electron or muon pairs are presented. The data correspond to 139 fb−1 of s√ = 13 TeV proton-proton collisions, collected by the ATLAS detector during Run 2 of the Large Hadron Collider (2015–2018). The final state has contributions from a number of interesting Standard Model processes that dominate in different four-lepton invariant mass regions, including single Z boson production, Higgs boson production and on-shell ZZ production, with a complex mix of interference terms, and possible contributions from physics beyond the Standard Model. The differential cross-sections include the four-lepton invariant mass inclusively, in slices of other kinematic variables, and in different lepton flavour categories. Also measured are dilepton invariant masses, transverse momenta, and angular correlation variables, in four regions of four-lepton invariant mass, each dominated by different processes. The measurements are corrected for detector effects and are compared with state-of-the-art Standard Model calculations, which are found to be consistent with the data. The Z → 4ℓ branching fraction is extracted, giving a value of (4.41 ± 0.30) × 10−6. Constraints on effective field theory parameters and a model based on a spontaneously broken B − L gauge symmetry are also evaluated. Further reinterpretations can be performed with the provided information
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